<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0">
  <front>
    <journal-meta><journal-id journal-id-type="publisher">ACP</journal-id><journal-title-group>
    <journal-title>Atmospheric Chemistry and Physics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ACP</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1680-7324</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/acp-21-1507-2021</article-id><title-group><article-title>An overview of the ORACLES (ObseRvations of Aerosols above CLouds and their
intEractionS) project: aerosol–cloud–radiation interactions in the southeast
Atlantic basin</article-title><alt-title>An overview of the ORACLES project</alt-title>
      </title-group><?xmltex \runningtitle{An overview of the ORACLES project}?><?xmltex \runningauthor{J.~Redemann et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Redemann</surname><given-names>Jens</given-names></name>
          <email>jredemann@ou.edu</email>
        <ext-link>https://orcid.org/0000-0002-2404-7984</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Wood</surname><given-names>Robert</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1401-3828</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Zuidema</surname><given-names>Paquita</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4719-372X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Doherty</surname><given-names>Sarah J.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Luna</surname><given-names>Bernadette</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5 aff4">
          <name><surname>LeBlanc</surname><given-names>Samuel E.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0173-3890</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Diamond</surname><given-names>Michael S.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2147-5921</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff7">
          <name><surname>Shinozuka</surname><given-names>Yohei</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Chang</surname><given-names>Ian Y.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0815-275X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Ueyama</surname><given-names>Rei</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Pfister</surname><given-names>Leonhard</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4 aff36">
          <name><surname>Ryoo</surname><given-names>Ju-Mee</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Dobracki</surname><given-names>Amie N.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>da Silva</surname><given-names>Arlindo M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3381-4030</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6 aff7">
          <name><surname>Longo</surname><given-names>Karla M.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Kacenelenbogen</surname><given-names>Meloë S.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Flynn</surname><given-names>Connor J.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5 aff4">
          <name><surname>Pistone</surname><given-names>Kristina</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6130-0192</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff8">
          <name><surname>Knox</surname><given-names>Nichola M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4637-0811</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff9">
          <name><surname>Piketh</surname><given-names>Stuart J.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff10">
          <name><surname>Haywood</surname><given-names>James M.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff11">
          <name><surname>Formenti</surname><given-names>Paola</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0372-1351</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff12">
          <name><surname>Mallet</surname><given-names>Marc</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff13">
          <name><surname>Stier</surname><given-names>Philip</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1191-0128</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff14">
          <name><surname>Ackerman</surname><given-names>Andrew S.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0254-6253</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff14">
          <name><surname>Bauer</surname><given-names>Susanne E.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7823-8690</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff14">
          <name><surname>Fridlind</surname><given-names>Ann M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-9020-0852</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff15">
          <name><surname>Carmichael</surname><given-names>Gregory R.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff16 aff17">
          <name><surname>Saide</surname><given-names>Pablo E.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3879-7962</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff15">
          <name><surname>Ferrada</surname><given-names>Gonzalo A.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7502-9439</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff18">
          <name><surname>Howell</surname><given-names>Steven G.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff18">
          <name><surname>Freitag</surname><given-names>Steffen</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1951-5576</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff14">
          <name><surname>Cairns</surname><given-names>Brian</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Holben</surname><given-names>Brent N.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1251-9809</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Knobelspiesse</surname><given-names>Kirk D.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5986-1751</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff20">
          <name><surname>Tanelli</surname><given-names>Simone</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff20">
          <name><surname>L'Ecuyer</surname><given-names>Tristan S.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-7584-4836</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff20">
          <name><surname>Dzambo</surname><given-names>Andrew M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3789-8435</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff19">
          <name><surname>Sy</surname><given-names>Ousmane O.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff39">
          <name><surname>McFarquhar</surname><given-names>Greg M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0950-0135</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff21">
          <name><surname>Poellot</surname><given-names>Michael R.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Gupta</surname><given-names>Siddhant</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0663-4595</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff21">
          <name><surname>O'Brien</surname><given-names>Joseph R.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff22 aff37 aff38">
          <name><surname>Nenes</surname><given-names>Athanasios</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3873-9970</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff22">
          <name><surname>Kacarab</surname><given-names>Mary</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff22 aff23">
          <name><surname>Wong</surname><given-names>Jenny P. S.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff24">
          <name><surname>Small-Griswold</surname><given-names>Jennifer D.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4563-8596</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff25 aff34">
          <name><surname>Thornhill</surname><given-names>Kenneth L.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff26 aff35">
          <name><surname>Noone</surname><given-names>David</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8642-7843</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Podolske</surname><given-names>James R.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff27">
          <name><surname>Schmidt</surname><given-names>K. Sebastian</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3899-228X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff27">
          <name><surname>Pilewskie</surname><given-names>Peter</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff27">
          <name><surname>Chen</surname><given-names>Hong</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7427-2031</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff27">
          <name><surname>Cochrane</surname><given-names>Sabrina P.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff28">
          <name><surname>Sedlacek</surname><given-names>Arthur J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9595-3653</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff29">
          <name><surname>Lang</surname><given-names>Timothy J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1576-572X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff30">
          <name><surname>Stith</surname><given-names>Eric</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4 aff5 aff31">
          <name><surname>Segal-Rozenhaimer</surname><given-names>Michal</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff25">
          <name><surname>Ferrare</surname><given-names>Richard A.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff25">
          <name><surname>Burton</surname><given-names>Sharon P.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff25">
          <name><surname>Hostetler</surname><given-names>Chris A.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff19">
          <name><surname>Diner</surname><given-names>David J.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff19">
          <name><surname>Seidel</surname><given-names>Felix C.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4282-2198</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Platnick</surname><given-names>Steven E.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff32">
          <name><surname>Myers</surname><given-names>Jeffrey S.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Meyer</surname><given-names>Kerry G.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff34">
          <name><surname>Spangenberg</surname><given-names>Douglas A.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff33">
          <name><surname>Maring</surname><given-names>Hal</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Gao</surname><given-names>Lan</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>School of Meteorology, University of Oklahoma, Norman, OK, USA</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Atmospheric Sciences, University of Washington, Seattle, WA, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Atmospheric Sciences, University of Miami, Miami, FL, USA</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>NASA Ames Research Center, Moffett Field, CA, USA</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Bay Area Environmental Research Institute, Moffett Field, CA, USA</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>NASA Goddard Space Flight Center, Greenbelt, MD, USA</institution>
        </aff>
        <aff id="aff7"><label>7</label><institution>Universities Space Research Association, Columbia, MD, USA</institution>
        </aff>
        <aff id="aff8"><label>8</label><institution>Department of Geo-Spatial Sciences and Technology, Namibia University
of Science and Technology, Windhoek, Namibia</institution>
        </aff>
        <aff id="aff9"><label>9</label><institution>Unit for Environmental Science and Management, North-West University, Potchefstroom, North-West, South Africa</institution>
        </aff>
        <aff id="aff10"><label>10</label><institution>College of Engineering, Mathematics and Physical Science, University of Exeter, Exeter, EX4 4QE, UK</institution>
        </aff>
        <aff id="aff11"><label>11</label><institution>Laboratoire Interuniversitaire des Systèmes Atmosphériques
(LISA), UMR CNRS 7583, Université Paris-Est-Créteil, Université
de Paris, Institut Pierre Simon Laplace, Créteil, France</institution>
        </aff>
        <aff id="aff12"><label>12</label><institution>Centre National de Recherches Météorologiques,
Météo-France-CNRS, Toulouse, France</institution>
        </aff>
        <aff id="aff13"><label>13</label><institution>Atmospheric, Oceanic and Planetary Physics, Department of Physics,
University of Oxford, Oxford, UK</institution>
        </aff>
        <aff id="aff14"><label>14</label><institution>NASA Goddard Institute for Space Studies, New York, NY, USA</institution>
        </aff>
        <aff id="aff15"><label>15</label><institution>Center for Global and Regional Environmental Research, University of Iowa, Iowa City, IA, USA</institution>
        </aff>
        <aff id="aff16"><label>16</label><institution>Department of Atmospheric and Oceanic Sciences, University of California, Los Angeles, CA,
USA</institution>
        </aff>
        <aff id="aff17"><label>17</label><institution>Institute of the
Environment and Sustainability, University of California, Los Angeles, CA,
USA</institution>
        </aff>
        <aff id="aff18"><label>18</label><institution>Department of Oceanography, University of Hawai`i at Mānoa, Honolulu,
HI, USA</institution>
        </aff>
        <aff id="aff19"><label>19</label><institution>Jet Propulsion Laboratory, California Institute of Technology,
Pasadena, CA, USA</institution>
        </aff>
        <aff id="aff20"><label>20</label><institution>Department of Atmospheric and Oceanic Sciences, University of
Wisconsin–Madison, Madison, WI, USA</institution>
        </aff>
        <aff id="aff21"><label>21</label><institution>Department of Atmospheric Sciences, University of North Dakota, Grand Forks, ND, USA</institution>
        </aff>
        <aff id="aff22"><label>22</label><institution>Georgia Institute of Technology, Atlanta, GA, USA</institution>
        </aff>
        <aff id="aff23"><label>23</label><institution>Department of Chemistry and Biochemistry, Mount Allison University,
Sackville, Canada</institution>
        </aff>
        <aff id="aff24"><label>24</label><institution>Department of Atmospheric Sciences, University of Hawai`i at Mānoa,
Honolulu, HI, USA</institution>
        </aff>
        <aff id="aff25"><label>25</label><institution>NASA Langley Research Center, Hampton, VA, USA</institution>
        </aff>
        <aff id="aff26"><label>26</label><institution>College of Earth, Ocean, and Atmospheric Sciences, Oregon State
University, Corvallis, OR, USA</institution>
        </aff>
        <aff id="aff27"><label>27</label><institution>Department of Atmospheric and Oceanic Sciences, University of Colorado, Boulder, CO, USA</institution>
        </aff>
        <aff id="aff28"><label>28</label><institution>Brookhaven National Laboratory, Upton, NY, USA</institution>
        </aff>
        <aff id="aff29"><label>29</label><institution>NASA Marshall Space Flight Center, Huntsville, AL, USA</institution>
        </aff>
        <aff id="aff30"><label>30</label><institution>National Suborbital Research Center, Moffett Field, CA, USA</institution>
        </aff>
        <aff id="aff31"><label>31</label><institution>Department of Geophysics and Planetary Sciences, Porter School of the
Environment and Earth Sciences, <?xmltex \hack{\break}?>Tel Aviv University, Tel Aviv, Israel</institution>
        </aff>
        <aff id="aff32"><label>32</label><institution>University of California Santa Cruz, Santa Cruz, CA, USA</institution>
        </aff>
        <aff id="aff33"><label>33</label><institution>NASA Headquarters, Washington, D.C., USA</institution>
        </aff>
        <aff id="aff34"><label>34</label><institution>Science Systems and Applications, Inc., Hampton, VA, USA</institution>
        </aff>
        <aff id="aff35"><label>35</label><institution>Department of Physics, University of Auckland, Auckland, New Zealand</institution>
        </aff>
        <aff id="aff36"><label>36</label><institution>Science and Technology Corporation, Moffett Field, CA, USA</institution>
        </aff>
        <aff id="aff37"><label>37</label><institution>Ecole Polytechnique Federale de Lausanne, Lausanne, Switzerland</institution>
        </aff>
        <aff id="aff38"><label>38</label><institution>Foundation for Research and Technology – Hellas, Heraklion, Greece</institution>
        </aff>
        <aff id="aff39"><label>39</label><institution>Cooperative Institute for Mesoscale Meteorological Studies (CIMMS)
and School of Meteorology, <?xmltex \hack{\break}?>University of Oklahoma, Norman, OK, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Jens Redemann (jredemann@ou.edu)</corresp></author-notes><pub-date><day>4</day><month>February</month><year>2021</year></pub-date>
      
      <volume>21</volume>
      <issue>3</issue>
      <fpage>1507</fpage><lpage>1563</lpage>
      <history>
        <date date-type="received"><day>8</day><month>May</month><year>2020</year></date>
           <date date-type="rev-request"><day>16</day><month>June</month><year>2020</year></date>
           <date date-type="rev-recd"><day>9</day><month>October</month><year>2020</year></date>
           <date date-type="accepted"><day>1</day><month>November</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2021 </copyright-statement>
        <copyright-year>2021</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://acp.copernicus.org/articles/.html">This article is available from https://acp.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e976">Southern Africa produces almost a third of the Earth's biomass
burning (BB) aerosol particles, yet the fate of these particles and their
influence on regional and global climate is poorly understood. ORACLES
(ObseRvations of Aerosols above CLouds and their intEractionS) is a
5-year NASA EVS-2 (Earth Venture Suborbital-2) investigation with three intensive observation periods designed to study key atmospheric processes
that determine the climate impacts of these aerosols. During the Southern Hemisphere winter and spring (June–October), aerosol particles reaching 3–5 km in altitude are transported westward over the southeast Atlantic, where
they interact with one of the largest subtropical stratocumulus  (Sc) cloud decks in the world. The representation of these
interactions in climate models remains highly uncertain in part due to a
scarcity of observational constraints on aerosol and cloud properties, as well as due to the parameterized treatment of physical processes. Three ORACLES
deployments by the NASA P-3 aircraft in September 2016, August 2017, and
October 2018 (totaling <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">350</mml:mn></mml:mrow></mml:math></inline-formula> science flight hours), augmented
by the deployment of the NASA ER-2 aircraft for remote sensing in September
2016 (totaling <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> science flight hours), were intended to
help fill this observational gap. ORACLES focuses on three fundamental
science themes centered on the climate effects of African BB aerosols: (a) direct aerosol radiative effects, (b) effects of aerosol absorption on
atmospheric circulation and clouds, and (c) aerosol–cloud microphysical
interactions. This paper summarizes the ORACLES science objectives,
describes the project implementation, provides an overview of the flights
and measurements in each deployment, and highlights the integrative modeling
efforts from cloud to global scales to address science objectives.
Significant new findings on the vertical structure of BB aerosol physical
and chemical properties, chemical aging, cloud condensation nuclei, rain and
precipitation statistics, and aerosol indirect effects are emphasized, but
their detailed descriptions are the subject of separate publications. The
main purpose of this paper is to familiarize the broader scientific
community with the ORACLES project and the dataset it produced.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<?pagebreak page1508?><sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e1008">The radiative and cloud-altering impacts of anthropogenic aerosol particles
constitute the largest source of uncertainty in anthropogenic climate
forcing (IPCC, 2013). Aerosol particles interact directly with solar
radiation through scattering and absorption of radiation, which leads to a
direct radiative forcing whose sign depends on the ratio of the absorption
to the total aerosol extinction and on the albedo of the underlying
surface–atmosphere system (Coakley and Chylek, 1975). Heating of the
atmosphere by aerosol absorption can induce changes in atmospheric
circulation and mixing that can either enhance or decrease cloudiness
(Ackerman et al., 2000; Koch and Del Genio, 2010). Aerosol particles also
serve as cloud condensation nuclei (CCN), which can enhance cloud albedo by
increasing the concentration of cloud droplets and reducing their size when
aerosol concentrations increase at fixed liquid water content (Twomey,
1974), and also potentially drive changes in cloud condensate or cloud cover
by altering cloud lifetimes (Simpson and Wiggert, 1969; Albrecht, 1989;
Ackerman et al., 2004; Wood, 2007). The magnitudes of all effects and even the
sign of the latter two aerosol<?pagebreak page1509?> effects are not well quantified globally
(IPCC, 2013) and are expected to be geographically and seasonally
heterogeneous because the total aerosol forcing is dependent upon the nature
and amount of different aerosol species, cloud type and cover, and surface
albedo, all of which vary on such scales.</p>
      <p id="d1e1011">Biomass burning (BB) is one of the largest sources of absorbing aerosol
globally (Bond et al., 2013). BB aerosol particles contain black carbon, the
most strongly absorbing of all aerosol constituents found in the atmosphere.
The sign of the direct aerosol forcing is highly dependent upon the relative
vertical locations of aerosol and clouds, with forcing changing from
negative to positive when BB aerosol layers overlie low clouds rather than a
dark ocean surface (Chand et al., 2009). BB aerosols also contain oxidized
organic carbon and other soluble inorganic species that can act as effective
CCN if transported into clouds.</p>
      <p id="d1e1014">The southeast Atlantic (SEA) region has some of the highest optical depths
of BB aerosol on the planet. It is also the location of large inter-model
differences in aerosol forcing assessments (Schulz et al., 2006; Stier et al.,
2013; Zuidema et al., 2016). The neighboring southern African biomass
burning (BB) source regions account for almost one third of the Earth's BB
emissions (550 Tg C yr<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; van der Werf et al., 2010), producing optically
thick BB aerosol layers that are routinely transported across much of the
South Atlantic basin (Chand et al., 2009; Zuidema et al., 2016). While
burned areas are decreasing in size globally, burned areas in Africa are
increasing, raising interesting questions about BB aerosol interactions with
climate in that region in the future (Andela et al., 2017).</p>
      <p id="d1e1029">The SE Atlantic is also home to one of the Earth's largest subtropical
stratocumulus (Sc) cloud decks, which plays a key role in the energetic
balance of the region. The physical processes governing the feedbacks
between sea surface temperature (SST) and cloud properties in these Sc decks
are poorly represented in climate models (Bony and Dufresne, 2005). In the
Austral spring (July to October), the Sc deck interacts with the African BB
aerosols that have been transported westward by prevailing mid-tropospheric
tropical easterly winds. These aspects of the SE Atlantic attracted several
international field experiments on aerosol–cloud–climate interactions in the
region. These projects were based out of deployment sites distributed
throughout the SE Atlantic (Fig. 1) and were scheduled between 2016 and
2018 to allow for collaborative science. These experiments include the NASA
ORACLES project described in this paper, deploying from Walvis Bay, Namibia,
in 2016 and São Tomé in 2017 and 2018; the UK CLARIFY
(Clouds and Aerosol Radiative Impacts and Forcing), deploying from Ascension
Island in 2017; the French AEROCLO-sA (Aerosol, Radiation and Clouds in
southern Africa) project, deploying from Walvis Bay, Namibia, in 2017; and the
DOE Atmospheric Radiation Measurement mobile facility LASIC (Layered
Atlantic Smoke Interactions with Clouds) deployment to Ascension Island in
2016–2017, all described in more detail in Sect. 3.4.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e1035">Deployment sites for the 2016–2018 ORACLES field experiments and
collaborative international deployment activities (see text), along with
CALIOP curtain data visualized by Charles Trepte (NASA Langley), adapted
from © Google Maps 2020. The ovals with the letter A indicate new
or refurbished AERONET sites (Holben et al., 2018).</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f01.jpg"/>

      </fig>

      <p id="d1e1044">The southern and central African fires producing BB aerosol occur during the
warm, dry season over the continent, so emissions are lofted in the
convective boundary layer to an altitude of several kilometers. As they
advect offshore, the BB aerosol layers form a plume that initially overlays
the cloud deck over the Atlantic (Fig. 2; see also Adebiyi and Zuidema, 2016;
Zuidema et al., 2016; Deaconu et al., 2019) and exerts a direct radiative
forcing (RF) whose sign and magnitude depend upon the reflectance and
coverage of the clouds below and on the absorptivity of the aerosols (Keil
and Haywood, 2003; Chand et al., 2009). Depending on the relative vertical
location of the aerosols and the cloud deck, cloud condensate may increase
or decrease in response to aerosol absorption and subsequent changes in
atmospheric stability, relative humidity, and subsidence (semi-direct
forcing). Cloud optical thickness and areal coverage may also be influenced
by aerosol-induced changes in cloud microphysics (forcing from aerosol–cloud
interactions) when BB aerosols are mixed into the marine boundary layer
(MBL). This is expected to occur more frequently offshore as the MBL deepens
in response to warming sea surface temperatures (e.g., Eastman et al., 2017),
raising cloud top heights (Zuidema et al., 2009) and easing entrainment of
the overlying aerosol, and as BB aerosol layers descend in response to
prevailing large-scale subsidence (Fig. 2).</p>
      <p id="d1e1047">Satellite- and model-based assessments of aerosol–cloud–climate interactions
in this region (e.g., Chand et al., 2009; Wilcox, 2012; Stier et al., 2013; De
Graaf et al., 2014; Zhang et al., 2016; Adebiyi and Zuidema, 2018; Zhang and Zuidema, 2019;
Kacenelenbogen et al., 2019; Sayer et al., 2019) indicate that improved
observations of aerosol properties and loading, cloud fraction, albedo,
and liquid water path (LWP) are needed to constrain the local aerosol
radiative impacts. Such studies are hampered by problematic aerosol
retrievals in regions of extensive low clouds and difficulties retrieving
cloud microphysical properties underneath dense aerosol layers (Haywood et
al., 2004; Coddington et al., 2010; Deaconu et al., 2017). The observations
used in these studies often have severe limitations and require significant
assumptions about aerosol and cloud properties (Yu et al., 2012; Yu and
Zhang, 2013; Jethva et al., 2014; Knobelspiesse et al., 2015; Meyer et al.,
2015; Sayer et al., 2016).</p>
      <p id="d1e1050">An example of a satellite-based retrieval of both aerosols and clouds is
given in Fig. 2, which shows the altitude of aerosol and cloud layers during
3 months as a function of longitude, as operationally retrieved from the
Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) space-based lidar.
Multiple filters have been applied for quality assurance of these data.
However, the simple message this figure conveys, of an elevated aerosol
layer that is typically far above the low cloud, is somewhat misleading
because (i) there could be multiple aerosol layers above the uppermost cloud
and (ii) the CALIOP-derived aerosol layer base<?pagebreak page1510?> height has been found to be
biased high, based on airborne measurements made during ORACLES as well as
CALIOP retrievals that have been constrained by above-cloud aerosol optical
thickness derived from the CALIOP data. The latter results from the fact
that, especially for the daytime retrievals from CALIOP, there is a
significant reduction in the signal-to-noise ratio in the presence of optically thick
aerosol layers. Hence, the separation between clouds and overlying aerosols
(Fig. 2, yellow bars) is also likely biased high (see also Rajapakshe et
al., 2017). Such observational uncertainty and the differing conclusions one
may draw based on the separation between the BB aerosol layer and the
underlying Sc clouds in this region were a significant contributing impetus
for the ORACLES project. We include the CALIOP-derived Fig. 2 here to
provide the scientific information available at the ORACLES proposal stage,
which partially motivated the project in the first place and greatly
influenced its design (Watson-Parris et al., 2018).</p>
      <p id="d1e1053">Surface-based measurements also have limitations. AERONET (Aerosol Robotic
Network) sky radiance observations (Holben et al., 1998) are used frequently
to tune global model estimates of aerosol absorption (Bond et al., 2013) but can be routinely performed only from land and in the absence of clouds.
Although historically a number of AERONET stations existed near the main
African BB sources, just prior to ORACLES, there were no operational AERONET
stations in the main BB region, with the exception of Ascension Island far
downwind.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e1059">Distributions of aerosol top height (red), cloud top height (blue),
and the separation between clouds and overlying aerosols (yellow) as a
function of longitude, between 10–22.5<inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Observations are taken
from the Cloud-Aerosol Lidar with Orthogonal Polarization (CALIOP) version 3
aerosol profile product from 2006 to 2012 (7 years).</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f02.png"/>

      </fig>

      <p id="d1e1077">Airborne instruments provide measurements of aerosols and clouds under
co-varying meteorological conditions that are currently impossible to obtain
from space. High-resolution airborne observations, over scales that resolve
processes of interest, provide critical constraints for<?pagebreak page1511?> parameterizing
aerosol–cloud–climate interactions in models. They can also be used to
enhance satellite-based remote sensing, by resolving in situ characteristics
and variability within a particular scene, by providing a direct test of
retrieved properties, and in the long term by guiding the development of new
and improved remote-sensing techniques. Because previous efforts to study BB
emissions in South Africa (e.g., SAFARI-2K, Swap et al., 2003; TRACE-A, Fishman et al., 1996) were focused over land or in close proximity to the
coastal zone (e.g., Haywood et al., 2003), prior to ORACLES, there was a
dearth of measurements over the SE Atlantic Ocean, where the major radiative
impacts of BB aerosols are taking place.</p>
      <p id="d1e1080">In response to the need for new measurement constraints, in 2014 NASA funded
the ORACLES project as one of the Earth Venture Suborbital-2 investigations.
The goal of ORACLES is to provide a process-level understanding of the role
of aerosols in climate by providing observations of all relevant aerosol
effects over the SE Atlantic, a region with some of the largest aerosol
loadings on the planet that is readily accessible with airborne platforms.
The overarching ORACLES science goals, which encompass the specific science
themes and questions in the abstract and Table 1 below, are as follows.
<list list-type="order"><list-item>
      <p id="d1e1085">Determine the impact of African BB aerosol on cloud properties and the
radiation balance over the South Atlantic, using state-of-the-art in situ
and remote-sensing instruments to generate datasets that can also be used
to verify and refine current and future observation methods, including
instrument concepts with potential for deployment to space.</p></list-item><list-item>
      <p id="d1e1089">Acquire a process-level understanding of aerosol–cloud–radiation
interactions and resulting cloud adjustments that can be applied in global
models.</p></list-item></list>
In this paper, we provide an overview of all three ORACLES deployments,
highlighting aerosol absorptive and cloud-nucleating properties, their
vertical distribution relative to clouds, the locations and degree of
aerosol mixing into clouds, and cloud changes in response to such mixing. We
make an initial assessment of the differences and similarities of the BB
plume and cloud properties as observed from the 2016 deployment site (Walvis
Bay, Namibia) at the plume's southern edge and from the 2017 and 2018
deployment site (São Tomé and Príncipe) near the plume's
northern edge. We conclude with an outlook for the integrative work we
envision to address the overarching science questions regarding
aerosol–radiation–climate interactions in the SE Atlantic and how these
suborbital observations will aid long-term modeling and satellite remote-sensing efforts.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Project background</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Motivation for 3-year field deployment</title>
      <p id="d1e1108">Prior to the ORACLES implementation stage, an analysis of satellite data in
the study area had revealed pronounced shifts in aerosol altitude,
concentration, and optical properties through the July to October BB season.
That<?pagebreak page1512?> combined body of work suggested that aerosol loadings peak in September
(Fig. 3, see also Adebiyi et al., 2015), whereas single-scattering albedo
(SSA) increases over the season, reflecting either a change in BB aerosol
composition (Eck et al., 2013) or the mix of aerosol types present (Bond et
al., 2013). Another striking seasonal change is that, on average, the gap
between cloud top and the aerosol layer increases dramatically (Fig. 2),
primarily due to higher aerosol layers.</p>
      <p id="d1e1111">The closer vertical proximity of BB aerosol layers to clouds early in the
season (shown in Fig. 2) suggested that studies of aerosol–cloud
interactions would be most feasible then, while larger gaps later in the
season would suggest weaker indirect effects. Observing and quantifying
these seasonal changes and the changing importance of the aerosol
semi-direct and indirect effects over the BB season required either an
impractically extended deployment or separate deployments spread across the
season. The ORACLES team decided on separate deployments in September 2016,
August 2017, and October 2018, a decision that was aided by a relative lack
of interannual variability in meteorology. This variability was
predominantly linked to SST variations known as Benguela Niños that
mainly occur in boreal spring, not fall, and are much less frequent than the
better-known Pacific El Niños (Rouault, 2012). Interannual variability
in fire emissions was expected to be low as well (van der Werf et al., 2010). As a result, aerosol loading in the ORACLES region was expected to be repeatable,
with Moderate Resolution Imaging Spectroradiometer (MODIS) clear-sky aerosol
optical depth (AOD) retrievals implying year-to-year variability through the
burning season of only 20 % of the mean. In reality, recently developed
above-cloud AOD retrievals reveal a significant interannual variability in
the properties of the above-cloud aerosol plume (see Sect. 4.2–4.3 below);
investigations into the particular reasons are ongoing. Finally, a practical
consideration for the attempt to cover the BB seasonal cycle with three
separate deployments was based on the fact that airborne instrument
performance has a tendency to significantly decrease as mission durations
extend beyond 4 weeks.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e1116">Aerosol optical depth at 440/441 nm <bold>(a)</bold> from AERONET sites in southern Africa peaks in early September, while SSA at 440/441 nm <bold>(b)</bold>
shows a significant increase between August and November. Red circles in the
inset indicate the few stations operating between 2011 and 2013. Both panels
contain data from 1995 to 2013 to represent the state of knowledge prior to
the ORACLES deployments.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f03.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Science questions and objectives</title>
      <p id="d1e1139">ORACLES science questions and related objectives are generally focused on
direct, semi-direct, and indirect aerosol effects on climate. Table 1
summarizes science questions and objectives as originally posed. The general
approach for developing these objectives was to include goals that were
highly achievable first and to increase the complexity of objectives
gradually. The objectives related to science questions 1 and 2, i.e., direct
and semi-direct effects, constituted the “threshold” (for success) science
mission. The science objectives associated with question 3, i.e., indirect
effect assessments, were part of the “baseline” science mission, which in
NASA terminology indicates the full mission scope.</p><?xmltex \hack{\newpage}?><?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Table}?><label>Table 1</label><caption><p id="d1e1145">A summary of ORACLES science questions and related objectives.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="5cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="10cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Science questions</oasis:entry>
         <oasis:entry colname="col2">Related science objectives</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Q1: what is the direct radiative effect of the African biomass burning (BB) aerosol layer in clear- and cloudy-sky conditions over the SE Atlantic?</oasis:entry>
         <oasis:entry colname="col2">O1-1 (aerosol spatial evolution): determine the evolution of the BB aerosol microphysical and spectral radiative properties as the aerosol is transported across the South Atlantic. <?xmltex \hack{\hfill\break}?>O1-2 (aerosol-induced radiative fluxes): measure aerosol-induced spectral radiative fluxes as a function of cloud albedo and aerosol properties. <?xmltex \hack{\hfill\break}?>O1-3 (seasonal aerosol variation): assess the key factors that control the seasonal variation in aerosol direct effects.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Q2: how does absorption of solar radiation by African biomass burning (BB) aerosol change atmospheric stability, circulation, and ultimately cloud properties?</oasis:entry>
         <oasis:entry colname="col2">O2-1 (relative vertical distribution): determine the seasonally varying relative vertical distributions of aerosol and cloud properties as a function of distance from shore. <?xmltex \hack{\hfill\break}?>O2-2 (aerosol–cloud heating rates): constrain aerosol-induced heating rates for aerosol layers above, within, and below cloud. <?xmltex \hack{\hfill\break}?>O2-3 (cloud changes due to aerosol-induced heating): investigate the sensitivity of cloud structure and condensate to aerosol-induced heating rates.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Q3: how do BB aerosols affect cloud droplet size distributions, precipitation, and the persistence of clouds over the SE Atlantic?</oasis:entry>
         <oasis:entry colname="col2">O3-1 (mixing survey): survey the location and extent of aerosol mixing into the boundary layer (BL) and its seasonal variation. <?xmltex \hack{\hfill\break}?>O3-2 (cloud changes due to aerosol mixing): measure changes in cloud microphysical properties, albedo, and precipitation as a function of aerosol mixing into the BL. <?xmltex \hack{\hfill\break}?>O3-3 (cloud changes due to aerosol-suppressed precipitation): investigate the sensitivity of cloud structure and condensate to aerosol-induced suppression in precipitation.</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Project implementation</title>
<sec id="Ch1.S2.SS3.SSS1">
  <label>2.3.1</label><title>Logistics and deployment details</title>
      <p id="d1e1226">The Walvis Bay airport in western Namibia was originally considered the
ideal location for ORACLES due to its proximity to the ocean and cloud deck,
runway length and hangar size for the ER-2, and due to its use during the
SAFARI-2K campaign by the University of Washington CV-580 aircraft. The
runway had been extended to <inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3350</mml:mn></mml:mrow></mml:math></inline-formula> m, but certification of
the extension was still in progress as ORACLES began. It was our intention
to deploy only one aircraft in the first year and grow the activity after
acclimating to the locality and airspace. However, during the ORACLES-2016
deployment planning, the UK CLARIFY team announced plans to fly its airborne
assets in 2016 as well. In response, leadership re-ordered ORACLES
deployments to bring both aircraft to Walvis Bay in 2016, so as to maximize
their impact in a concerted effort with the international partners.</p>
      <p id="d1e1239">In the event that the facilities were found to be inadequate or unready or
unavailable, alternate airfields were investigated. Specifically, Upington
(FAUP), South Africa, and São Tomé (FPST) were pursued with due
diligence until country approval was obtained from Namibia. Upington had no
usable hangar but an extremely long runway, little competing traffic, and
the benefit of a long-standing collaborative relationship with the USA and
NASA. São Tomé's runway length and hangars could not accommodate the
ER-2 requirements, but officials were very enthusiastic about a NASA
collaboration. Both locations could support a P-3-only deployment. A
temporary hangar in Upington, South Africa, or Windhoek, Namibia, might have supported
the ER-2. Ascension Island also had no hangar and posed significant
constraints to the commercial import/transport of people and equipment. In
later years, Ascension Island was subject to runway construction, but it did serve
as an overnight transit stop for the P-3 in 2016 and 2017 and as the target for suitcase (overnight stay) flights in 2017.</p>
      <p id="d1e1242">ORACLES experiment requirements dictated deployment of up to 80 people (110
in 2016) for three 5-week periods, centered on the months of September 2016,
August 2017, and October 2018.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS2">
  <label>2.3.2</label><title>Choice of measurement platforms: envisioned versus realized
capabilities</title>
      <p id="d1e1253">The revised ORACLES project implementation plan called for the operation of
two aircraft in 2016 and the operation of only one aircraft in 2017 and
2018. The choice to deploy the ER-2 aircraft in 1 year only was solely
based on funding considerations, as its operations are considerably more
complicated and costly.</p>
      <p id="d1e1256">The ORACLES platforms and instruments were selected to efficiently and quantitatively address the science questions outlined above through measurements of radiative fluxes, derivation of heating rates,
observations of aerosol and cloud microphysical and radiative properties,
atmospheric thermodynamics, and chemistry. The desired flight plans were
driven by expected aerosol–cloud features and their interactions within the
region, by regional model forecasts, and by recent (same-flight or
previous-flight) observations. When the P-3 was the sole NASA aircraft
deployed (August 2017 and October 2018), Research Scanning Polarimeter (RSP)
and High Spectral Resolution Lidar (HSRL-2) instruments (Table A4) were
added to its payload to capture relevant<?pagebreak page1514?> science data by flying above, within, and below aerosol layers and clouds. When both the P-3 and ER-2 were
present (September 2016), the ER-2 served in a remote-sensing role,
obviating the need for the P-3 to fly above both cloud and aerosol layers.</p>
      <p id="d1e1259">It was known from the planning stage that the range of the P-3 aircraft was
dependent on payload and flight pattern flown; spirals and low-altitude flight reduce flight time. Based on DISCOVER-AQ's successful inclusion of
spirals from 1000 to 5000 ft (305 to 1525 m) during 8 h flights, ORACLES flights were
expected to be similar in duration and character. From Walvis Bay, Namibia,
this covered the target science zone (5 to 35<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S,
westward from the coast to approximately the prime meridian), transit to
Ascension Island for suitcase flights and for coordination with the UK's
CLARIFY team, and transit to São Tomé Island, located near the
northern edge of the climatological BB plume, with margins for headwinds,
profiles, and low-altitude flight.</p>
      <p id="d1e1271">During the 2016 deployment, it became obvious that there was merit in P-3
flights that extended beyond the originally estimated 8 h duration. The
NASA P-3 crew accommodated this request as far as crew rest considerations
permitted; the average flight duration for local P-3 science flights
(excluding transits) in 2016 was 8.3 h (see Sect. 4.4). In 2017 and
2018, while flying from São Tomé, a larger P-3 flight crew was able
to average 9.1 and 8.3 flight hours respectively for similar flights, with
the 2018 average affected by increased safety margins due to expected
inclement weather.</p>
      <p id="d1e1275">For ORACLES, ER-2 flights were envisioned to be up to 8 h in duration,
similar to the prior Studies of Emissions and Atmospheric Composition,
Clouds and Climate Coupling by Regional Surveys (SEAC4RS) campaign. Due to
the 2 h pre-flight hands-off period and pilot 12 h duty day, there
were concerns that weather delays (e.g., low ceilings) would result in
flight duration limitations and therefore limitations in the final
geographical coverage. The ER-2 deployed only once for ORACLES, to Walvis
Bay, Namibia, during September 2016. The payload consisted of the Enhanced MODIS
Airborne Simulator (eMAS), Airborne Multiangle SpectroPolarimetric Imager
(AirMSPI), RSP, and HSRL-2 (Table B2) for various aspects of cloud
composition, aerosol properties, and the overall cloud/aerosol morphology, as well as
the Solar Spectral Flux Radiometer (SSFR) for radiative flux measurements.
The aircraft operated as expected, and the average flight duration from
Walvis Bay was 8.1 h. Especially during the second half of the campaign,
the ER-2 pilots were extremely accommodating, frequently extending
individual flight duration to 9 h.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS3">
  <label>2.3.3</label><title>Choice of instrumentation</title>
      <p id="d1e1286">In this section, we discuss the choice of instrumentation for each platform
and deployment. Depending on ORACLES deployment year, the P-3 carried 8 to
11 instruments or instrument suites, with the following included for all
deployments: cloud suite (UND/OU); phase Doppler interferometer (PDI);
Hawaii Group for Environmental Aerosol Research (HiGEAR) in situ measurement
suite for aerosols; SSFR/CG-4 for radiative fluxes; Spectrometer for Sky-Scanning, Sun-Tracking Atmospheric Research (4STAR) for aerosol
optical depth, cloud, and sky radiances; Airborne Third Generation
Precipitation Radar (APR-3) for cloud and precipitation observations;
Research Scanning Polarimeter (RSP); CO Measurements and Analysis (COMA)
for CO, CO<inline-formula><mml:math id="M7" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, and H<inline-formula><mml:math id="M8" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O mixing ratios; CCN spectrometer for cloud
condensation nuclei; and Water Isotope System for Precipitation and
Entrainment Research (WISPER) for water isotope measurements. In certain
years there were targeted additions/deletions, listed as follows.
<list list-type="bullet"><list-item>
      <p id="d1e1309">The HSRL-2 was added to the P-3 payload for deployments without the ER-2,
i.e., 2017 and 2018.</p></list-item><list-item>
      <p id="d1e1313">Advanced Microwave Precipitation Radiometer (AMPR) was included in the first
deployment year only (2016), when the ER-2 also carried the HSRL-2 and RSP.</p></list-item><list-item>
      <p id="d1e1317">The PTI (photothermal interferometer) was included in the 2016 and 2018
deployments only, as it suffered a failure before the 2017 deployment.</p></list-item><list-item>
      <p id="d1e1321">The counterflow virtual impactor (CVI) was added for 2017 and 2018 as part
of WISPER to enable cloud residual aerosol and droplet water isotope ratio
measurements.</p></list-item><list-item>
      <p id="d1e1325">An aerosol filter system (AFS) for trapping aerosol particles for
post-flight analysis was added in 2017 and 2018.</p></list-item><list-item>
      <p id="d1e1329">In 2017 and 2018, a duplicate cloud droplet probe (CDP) was mounted in a
position more forward relative to the leading edge of the wing, in an
attempt to determine whether proximity to the leading edge affected cloud
particle measurements.</p></list-item><list-item>
      <p id="d1e1333">In 2018, two customized versions of the sunshine pyranometer (Badosa et al.,
2014) were added to the P-3, as was a nadir-viewing geo-referenced and
radiometrically calibrated fish-eye camera.</p></list-item></list>
As part of ORACLES, two new AERONET stations were established, i.e., the
“Namibe” site in Namibe, Angola, and the “SEGC_Lope_ Gabon” site near Libreville, Gabon. Many other sites in
the region were revamped or established with separate funding and are shown
in Fig. 1 (see <uri>https://aeronet.gsfc.nasa.gov/cgi-bin/site_info_v3</uri>, last access: December 2019, for a list of sites).</p>
      <p id="d1e1340">Tables B1 to B3 in Appendix B provide full payload tables, including
instrument names, instrument descriptions, primary measurements, and derived
geophysical observables for each instrument.</p>
</sec>
<?pagebreak page1515?><sec id="Ch1.S2.SS3.SSS4">
  <label>2.3.4</label><title>Experiment strategy: dry-run exercise</title>
      <p id="d1e1351">ORACLES conducted a 2-week “dry-run” activity from 14–28 September 2015,
prior to its first deployment in 2016. Project meteorologists, platform
scientists, pilots, and the leadership team met by phone and Cisco Webex to
examine daily weather forecasts, chemical weather predictions, and flight
conditions. In response to these forecasts, detailed flight plans were
developed for the upcoming 1 or 2 possible flight days, using a flight
planning tool that was specifically designed for multi-aircraft flight
operations (LeBlanc, 2018). Longer-range forecasts up to 5 d were used to
plan for extended flight strategies relative to overarching flight
objectives. Satellite data, primarily Meteosat-10 Spinning Enhanced Visible
and Infrared Imager (SEVIRI) visible imagery and Cloud-Aerosol-Transport
System (CATS) and CALIPSO vertical feature mask and attenuated backscatter
profiles, were used to evaluate the likely success of a given flight plan for
a given day. The process familiarized the science team with items that
impacted real flight planning: aircraft limitations, staff fatigue limits
(e.g., down days, crew rest), aviation authority coordination timelines, the
availability and latency of meteorological forecasts, and the use of the
flight planning tool. This practice time made ORACLES actual deployments
more efficient, although the complexity and scope of actual chemical and
meteorological forecasts in the field ended up being well beyond the scope
of the dry-run exercise. This increased complexity was undoubtedly the
result of lessons learned during the dry-run exercise itself.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS5">
  <label>2.3.5</label><title>Experiment strategy: forecasting and flight planning</title>
      <p id="d1e1363">The forecasting effort for ORACLES deployments in the field entailed both
meteorological and chemical weather predictions. The meteorological
forecasting effort for the ORACLES mission consisted of three components:
(i) forecasting for flight planning, (ii) nowcasting during flights for
real-time flight direction, and (iii) forecasting local weather for flight
operations. Each of the three ORACLES deployments featured daily planning
meetings. On non-flight days, the flight planning team met at 08:00 local
time to discuss the weather and chemical weather forecasts for a period of
up to 5 d, with special emphasis on the upcoming 1 or 2 flight
days. On flight days, the team would assemble at 05:00 local time to assess
whether the latest forecasts warranted any changes to flight plans made the
day prior. Also on flight days, the forecast team would provide in-flight
nowcasting that often led to significant adjustments of flight plans,
usually to respond to actual cloud conditions that materialized on a given
flight day or in response to changing local conditions.</p>
      <p id="d1e1366">Clouds were the primary focus of the meteorological forecasting effort for
both flight planning and nowcasting. Low clouds (i.e., stratocumulus at the
inversion) were of primary scientific interest for their interaction with
the African smoke plume. However, middle and high clouds were also important
since the presence of these clouds complicated the radiation measurements of
some instruments (e.g., 4STAR, SSFR). Verification studies prior to the
ORACLES deployments showed that the European Centre for Medium Range Weather
Forecasts (ECMWF; Pappenberger et al., 2008; ECMWF Newsletter, 2012; Ye et
al., 2014) and United Kingdom Meteorological Office (UKMO; Ran et al., 2018)
global forecast models provided the best performance for cloud forecasts.
ECMWF digital data were available at 0.125<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> longitude <inline-formula><mml:math id="M10" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> latitude
resolution and included the primary meteorological variables (relative
humidity and horizontal winds at 925, 850, 800, 700, 600, 500, 400, 300,
150, and 100 hPa levels; 1000–500 hPa layer thickness; surface wind speed;
mean sea level pressure; boundary layer height; precipitation; convective
available potential energy) as well as 3-D ice and liquid water mass. We
also used the 2-D ECMWF products of cloud fraction and cloud base for the
low, middle, and high clouds, which were found to be adequate for our
forecasting requirements. The ECMWF cloud forecasts were supplemented by
low, middle, and high cloud distribution forecasts from the UKMO global
forecast model. In order to forecast the overall circulation over the
southeast Atlantic, with an emphasis on wind and relative humidity
distributions from the surface to 500 hPa, we used a suite of forecast
products from ECMWF, UKMO, Global Forecasting System (GFS) from the National
Centers for Environmental Prediction (Environmental Modeling Center, 2003),
and the NASA Goddard Earth Observing System, Version 5 (GEOS-5) model (Molod
et al., 2012).</p>
      <p id="d1e1385">Our primary nowcasting tool during the flights was the geostationary
satellite imagery from the SEVIRI instrument aboard Meteosat-10 and
Meteosat-11. Raw imagery from the infrared and visible channels was useful
for establishing the evolution and distribution of clouds during flight.
Satellite cloud properties described by Minnis et al. (2008, 2020) were
calculated from SEVIRI raw radiances by NASA Langley, including cloud
altitude, water path, and effective radius, and were also used in real-time
flight direction. For forecasting local weather for flight operations,
particularly during the October 2018 deployment in São Tomé, we
primarily relied on satellite imagery over the past 12–24 h for a
short-term (i.e., a day or less) outlook of heavy precipitation at the
airport, as precipitation forecasts from the models were largely unreliable.</p>
      <p id="d1e1388">Chemical forecasts were done using both global and regional models, with the
regional models providing a lot of the detail required for flight planning
on a daily basis. We used three global systems: GEOS5 (<uri>https://gmao.gsfc.nasa.gov/GEOS/</uri>, last access: May 2020), the Copernicus Atmosphere Monitoring
Service (CAMS, <uri>https://atmosphere.copernicus.eu/</uri>, last access: May 2020), and a bespoke three-component aerosol (carbonaceous, mineral dust, and industrial
pollution) modeling system developed by the UK Met Office for their CLARIFY
deployment in 2017. Five-day aerosol<?pagebreak page1516?> forecasts provided the expected spatial
and vertical location of the main smoke coming from the African continent.
These models were also useful in identifying times when the smoke was
expected to be mixed with dust aerosols, especially during the 2016
deployment from Walvis Bay.</p>
      <p id="d1e1398">For regional model forecasts, two configurations of the Weather Research and
Forecasting Model (WRF; Skamarock et al., 2008) were employed. One of them
used WRF coupled to chemistry (WRF-Chem, Grell et al., 2005) using the
physics package from the Community Atmosphere Model version 5 (CAM5, Ma et
al., 2014), run by a team from the University of Iowa (WRF-CAM5, PI: Gregory Carmichael). This model provided daily 72 h aerosol forecasts for similar
purposes as for the global models by using a full chemistry suite with
hundreds of chemical species considered. WRF was also configured using an
aerosol-aware microphysics (AAM) scheme (Saide et al., 2016) maintained by a
team from NCAR/UCLA (PI: Pablo E. Saide). The Weather Research and Forecasting
aerosol-aware microphysics (WRF-AAM) model provided forecasts for lead times
of up to 4 d at 12 km resolution. The system included a near-real-time
emission constraint using satellite-based aerosol optical depth (Saide et
al., 2016), which to our knowledge corresponds to the first near-real-time
system to perform such tasks. Two simulations were performed per forecasting
cycle turning smoke emissions on and off in the model. Since WRF-AAM
resolves aerosol–cloud–radiation interactions, these simulations allowed
assessment of the effects of smoke on weather in forecasting mode by taking
the difference between the two forecasts. The forecasts also included
tracers tagged to each day of smoke emissions from the African continent,
which were used to provide a distribution of smoke age based on the tracer
concentrations and the days since emissions. Statistics such as mean and
mode were extracted from the age distribution and used for flight planning
to target plumes with different ages to explore the temporal evolution of
aerosol properties.</p>
      <p id="d1e1401">Another task performed during the planning meetings was near-real-time
evaluation of the forecasts. These were focused on assessing forecast
performance in predicting clouds and the aerosol plume location, and relied
mostly on the latest SEVIRI cloud retrievals, and clear-sky and above-cloud
AOD from MODIS. This exercise allowed the team to track forecast failures
and successes and provided a sense of reliability when making decisions
based on forecasts.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS6">
  <label>2.3.6</label><title>Routine flights vs. target-of-opportunity flights</title>
      <p id="d1e1412">The ORACLES investigation concept featured a combination of routine flights
to facilitate comparisons with climate models and to ensure sampling of a
wide range of aerosol loadings and cloud conditions, with other flights
addressing “targets of opportunity”. The “routine” flights all took
place along a fixed latitude–longitude line with sampling at a range of
altitudes and remote sensing of the full column. In 2016, the routine flight
track was along a diagonal with endpoints of 20<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/10<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E
and 10<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/0<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; in 2017 and 2018 the routine flight
track extended from the Equator to <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S along
5<inline-formula><mml:math id="M17" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. See Fig. 11 in Sect. 4.4 for a complete set of flight
tracks.</p>
      <p id="d1e1479">In situ observations of aerosol microphysical and optical properties during
the routine flights were envisioned to map the evolution of BB aerosol
radiative properties during transport. HSRL-2 (High Spectral Resolution
Lidar) observations from the P-3 or ER-2 helped map the spatial extent of
the layers, while SSFR (Solar Spectral Flux Radiometer) and 4STAR
(Spectrometer for Sky-Scanning, Sun-Tracking Atmospheric Research)
observations provided additional insights into the in situ-derived aerosol
properties via optical and radiative closure experiments. Measurements to
address seasonal variations in direct aerosol radiative effects and their
controlling factors were derived from the routine flights. The routine
flight requirements were derived based on the assumption that the statistics
of important observed aerosol and cloud properties, given sampling and
measurement uncertainties, are sufficiently constrained to distinguish
between climate model estimates. For this, we assumed that the variability
in aerosol properties at model-relevant scales (100 km<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) can be
extrapolated from the analysis of Shinozuka and Redemann (2011) to be less
than 20 % and that such variability is well below the inter-model
differences on such scales.</p>
      <p id="d1e1491">Another motivation for the routine flights was to ensure sampling of a wide
range of aerosol loadings and cloud conditions. The five to six envisioned
routine flights (equaling <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">40</mml:mn></mml:mrow></mml:math></inline-formula>–50 flight hours per deployment)
that comprise the ORACLES threshold science objectives were intended to
yield aerosol and cloud data in about 200 100 km<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> climate model grid
boxes. Prior to the start of the campaign, we investigated probability density functions (PDFs) of MODIS
daily <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> averaged AOD between 10–20<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and
5<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W–5<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E for September 2001 derived from the
then-available dark target algorithm. We randomly subsampled the roughly
3000 <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> MODIS AOD boxes with the planned 200 airborne observations and
found that the resulting PDFs were a good representation of the parent
population of MODIS AOD. We concluded that the number of threshold science
flight hours was adequate to compile probability density functions of
aerosol properties that allow assessments of climate model differences at
these spatial scales. This was confirmed by analysis after the first
deployment (Shinozuka et al., 2020).</p>
      <p id="d1e1581">About half of the flight hours in each campaign focused on targets of
opportunity, as detailed in Tables A1–A3 in Appendix A. These flights
targeted specific science goals (e.g., capturing a range of aerosol ages, or
contrasting conditions in terms of aerosol–cloud interactions). Flight
patterns (e.g., “radiation walls”, square spirals) were optimized to
leverage the measurement capabilities of the range of instruments on board
the P-3 and to allow for later comparison of different methods of measuring
a common parameter (e.g., aerosol SSA). During the 2017 and 2018
deployments, the<?pagebreak page1517?> target-of-opportunity flights were planned to be near the
routine flight track whenever possible to improve sampling statistics.</p>
</sec>
<sec id="Ch1.S2.SS3.SSS7">
  <label>2.3.7</label><title>Considerations for 2016 deployment with ER-2 and P-3</title>
      <p id="d1e1592">The planning for the 2016 field deployment in Namibia started in early 2015,
with multiple site visits to the Walvis Bay airport, logistics and hotel
providers, Namibian science partners, and representatives of various Namibian
government organizations. This planning started early because the unexpected
change to deploy both ORACLES aircraft in 2016 brought along a significant
set of challenges due to the large contingency of scientific and aircraft
support equipment needed, with this being the first of the three ORACLES
deployments. The ORACLES team gratefully acknowledges the help provided by
the Honorable Thomas F. Daughton, US Ambassador to Namibia from 2014 to
2017, and the support by the US embassy staff led by John Kowalski. The
US embassy proved instrumental in receiving flight permissions and in
arranging the student program in August 2016. The ORACLES team also received
invaluable feedback and support from the Namibia University of Science and
Technology (NUST), led by its rector, Tjama Tjivikua, and Dean Lameck
Mwewa. In addition to NUST, the Gobabeb Training and Research Center led by
Gillian Maggs-Kolling, the University of Namibia represented by
Martin Hipondoka and Michael Backes as well as North-West University (South
Africa) represented by Stuart Piketh provided information and logistics
support throughout the 2016 campaign. As we describe in Sect. 3.5 below,
these contacts were the springboard for the outreach efforts that led to the
deployment of seven graduate students in the 2016 field campaign, including five
students from NUST and the University of Namibia. In their totality, we hope
that the efforts expended by the Namibian government and the Namibian and
South African science community, as well as the reciprocating efforts by the
ORACLES science team, can be considered a transformational effort in the
context of science diplomacy (Annegarn and Swap, 2012), at least in so far
as the experience for the individual students that participated in the
outreach efforts are concerned.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Linkage with international deployment efforts (LASIC, CLARIFY,
AEROCLO-sA)</title>
      <p id="d1e1604">ORACLES was not the only recent experimental investigation in the southeast
Atlantic (see Fig. 1). The UK CLARIFY project, which deployed their BAe-146
plane from Ascension Island in August–September 2017 (Haywood et al., 2020),
and the French AEROCLO-sA project, which deployed a Falcon-20 plane from
Walvis Bay, Namibia, in August 2017 (Formenti et al., 2019), shared similar
science objectives with ORACLES, as did the DOE Atmospheric Radiation
Measurement mobile facility deployment to Ascension Island from June 2016
through October 2017 for the LASIC project (Zuidema et al., 2015). All four
campaigns were active in August–September 2017, and a “suitcase” flight to
Ascension Island by the NASA P-3 plane included a direct instrument
intercomparison flight with the CLARIFY BAe-146 on 18 August 2017.
Collaboration between all four campaigns continued through a joint data
workshop held in Paris in April 2019, prior to a joint session at the annual
meeting of the European Geophysical Union. The excitement generated from
sharing insights and points of view, some similar and some not, from the
individual campaigns led to a decision to hold another joint workshop in May 2020, planned for the United States but held virtually due to the COVID-19
pandemic. In one example, a different view of the relationship of the single-scattering albedo to aerosol aging was noted, with ORACLES scientists
focusing more on the vertical structure (Fig. 12) and CLARIFY scientists
interested in investigating the change in SSA with distance from the
continent. The latter is an excellent example of the synergism afforded
between the two campaigns, with ORACLES sampling air closer to the
continent and the CLARIFY campaign sampling <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1700</mml:mn></mml:mrow></mml:math></inline-formula> km
offshore.</p>
</sec>
<sec id="Ch1.S2.SS5">
  <label>2.5</label><title>Outreach efforts</title>
<sec id="Ch1.S2.SS5.SSS1">
  <label>2.5.1</label><title>Namibia – 2016</title>
      <p id="d1e1633">During the field campaign held in Namibia in 2016, the gathering of science
data not only benefited the scientists directly involved in the project;
through an outreach program the science was extended to the Namibian
population (and to some extent the broader southern African region). The
outreach effort was multi-tiered and aimed to inform the public, develop
young scientists, and encourage children to enter into STEM fields of study.
Outreach activities included public lectures, interviews with local radio
and newspapers, and open days at the airfield. In addition, ORACLES
scientists traveled to northern Namibia for several days to participate in
the Ongwediva Annual Trade Fair (OATF) together with students, staff, and
faculty from the University of Namibia (UNAM), the Namibia University of
Science and Technology (NUST), and the Gobabeb Research and Training Center.
The OATF showcased collaborative environmental research from participating
research institutes and was attended by Ongwediva-area students, business
leaders, and local dignitaries.</p>
      <p id="d1e1636">In addition to these broader public engagement outreach activities, a
targeted science development program was initiated with support from the US
Embassy in Namibia and NUST. This 3-week full immersion outreach program was
developed to provide promising local and regional young scientists with an
opportunity to experience different components of a large complex airborne
research field campaign. In total, seven post-graduate students (master's and PhD level), from Namibia (five students) and South Africa (two students),
participated in the student guest program (Fig. 4).<?pagebreak page1518?> Student guests were
exposed to the planning, modeling, and instrumentation used within the
ORACLES field campaign. In addition to these broad field campaign skills,
they received a solid foundation in basic atmospheric science through
tutorials from the participating campaign scientists, some introductory
programming tutorials, and an opportunity to interact with scientists
aligned with their field of research. Within the duration of the program
they also all had an opportunity to join a science flight. Further regional
expansion of this student guest program was planned for the 2017 and 2018
field campaigns in collaboration with the CLARIFY and AEROCLO-sA campaigns,
but with the move of the ORACLES field campaigns to São Tomé this
expansion outreach effort could not be implemented.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e1641">The ORACLES guest students, together with ER-2 pilot, James Gregory Nelson, at the Walvis Bay airport.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f04.jpg"/>

          </fig>

</sec>
<sec id="Ch1.S2.SS5.SSS2">
  <label>2.5.2</label><?xmltex \opttitle{S\~{a}o Tom\'{e} and Pr\'{\i}ncipe (STP) -- 2017 and 2018}?><title>São Tomé and Príncipe (STP) – 2017 and 2018</title>
      <p id="d1e1659">To understand the challenges of implementing an outreach program as part of
a scientific project like ORACLES in São Tomé and Príncipe
(STP), one needs to know a little about the history of this young country of
just over 200 000 inhabitants. Previously uninhabited, the STP Archipelago
was colonized by Portugal throughout the 16th century, when it served as a
warehouse for the slave trade and established itself as a producer of
sugarcane, coffee, and cocoa. STP independence from Portugal came in 1975,
keeping Portuguese as its official language, although minority groups also
speak at least four other dialects.</p>
      <p id="d1e1662">During an initial exploratory visit in 2015, built on a previous
NSF-sponsored site visit, the ORACLES team contacted the Instituto Nacional de Meteorologia (INM) to establish
collaborations. The INM operates at STP airport facilities and showed great
initial enthusiasm for ORACLES deployments from STP. During the 2 years of
ORACLES operations in 2017 and 2018, INM kindly issued daily weather reports
tailored to ORACLES needs. There were several visits from the ORACLES team
to INM, and Aristómenes Amadeu do Nascimento of INM attended various
ORACLES weather briefings.</p>
      <p id="d1e1665">The only public university in STP and the most important one, the University
of STP (USTP), was established only in 2014. The creation of USTP came to
address fundamental and emergency problems of the country, which included
training of personnel for the health and education sectors, agriculture, and
food production. When the ORACLES team deployed to STP in 2017, USTP had, in
its current format, only 2 years of existence, still consolidating its
vocations and priorities. Nevertheless, the institution represented by
Aires Bruzaca (dean), João Pontífice (vice dean), and
Manuel do Sacramento Ramos Penhor was enthusiastic about establishing
scientific collaborations with NASA.</p>
      <p id="d1e1669">The ORACLES team organized a series of seminars about ORACLES scientific
objectives for the USTP and INM communities. The seminar themes also
included the AERONET (Aerosol Robotic Network) and Pandora NASA projects,
global networks of spectrometers designed to retrieve, respectively, aerosol
optical depth and microphysical parameters (Holben et al., 1998; Dubovik and
King, 2000), and total columns of ozone and other trace gases in the
atmosphere from direct-Sun measurements (Herman et al., 2009, 2015;
Tzortziou et al., 2012). All lectures were presented by ORACLES science team
members in Portuguese to address potential language barriers.</p>
      <p id="d1e1672">A Pandora Spectrometer Instrument (PSI) and an AERONET instrument were
brought to STP as part of the ORACLES deployment. The main goal, especially
for the PSI deployment, was to assess whether mutual goodwill, interest,
and capabilities exist for NASA, USTP, and INM to collaborate scientifically
long term. The team was successful in training professors of the USTP to
operate the PSI and the AERONET instruments (Fig. 5), and this resulted in
additional aerosol measurements beyond the campaign periods. Moreover, it
laid the foundation to have STP as one of the sites of the Pandora network,
with an official agreement between NASA and the USTP signed in 2018.</p>
      <p id="d1e1675">The ORACLES team found in STP a community open to and eager for the
establishment of a fruitful scientific cooperation. Our experience points
out that involvement with the local community is of extreme importance, not
only for the dissemination of scientific knowledge but also to facilitate
engagement between the young scientists from both communities. Collaboration
with local scientific communities during field deployments such as ORACLES
has the dual benefits of enhancing local scientific capabilities in
under-resourced areas of the world and producing tangible benefits for this
and future missions in the region.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><?xmltex \def\figurename{Figure}?><label>Figure 5</label><caption><p id="d1e1680">A picture of the STP Instituto Nacional de Meteorologia (INM),
with an inset of the Pandora and AERONET instruments temporarily installed
on the rooftop. Photo credit: James Podolske.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f05.jpg"/>

          </fig>

</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Description of deployments</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Meteorological context</title>
      <p id="d1e1706">The key feature of the circulation that transports fire emissions from the
African continent over the southeast Atlantic is the easterly flow above
about 2 km. Figure 6 shows the 4 km flow and relative humidity (RH) from the
ERA-Interim reanalysis, along with the southerly limit of significant
rainfall from the monthly 0.25<inline-formula><mml:math id="M29" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> satellite-based 3B43 dataset
(Huffman et al., 2007) for the 19-year September mean (2000–2018). The
easterly flow maximizes around 8<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, reaching minima near 4<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N
and 18<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. This flow is maintained by the thermally direct
circulation over the continent, which is driven by heating of the elevated
African plateau south of 10<inline-formula><mml:math id="M33" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S (Adebiyi and Zuidema, 2016). The
moister regions to the north are cooler, consistent with the thermal wind
relation and the easterly shear below the jet. The jet is similar in
character to the northern African Easterly Jet (NAEJ;
consistent with the temperature gradient between the hot Sahara desert and
the cooler equatorial region), if not as pronounced. Since there is no
heating source over<?pagebreak page1519?> the southeast Atlantic, the jet decreases in intensity
as soon as the winds leave the continent. The mean 4 km flow then curls
anticyclonically near 10–20<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W and merges with the midlatitude jet,
most pronounced in September–October. Smoke associated with this flow has
been observed as far away as the South Pacific (Chatfield et al., 2002).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e1766">September-mean relative humidity (RH – color fill) and horizontal
winds at 4 km (averaged over 600–650 hPa – red contours and white arrows),
and the southerly limit of significant rainfall averaged over 19 years
(2000–2018 – blue contour). Heavy solid and dashed red contours indicate
elevated wind speeds (7 <inline-formula><mml:math id="M35" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> – solid; 8 and 9 m s<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> – dashed). The white
rectangle encompasses 8–16<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and 14–3<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. The cyan lines refer to 9.75<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and 9.75<inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E,
respectively (see Fig. 7). RH and winds are from the ERA-Interim analyses,
and the rainfall is from the monthly 0.25<inline-formula><mml:math id="M41" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> satellite-based 3B43
dataset.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f06.png"/>

        </fig>

      <p id="d1e1850">The RH at 4 km altitude provides a useful qualitative indicator of the
effects of upward vertical motion (Fig. 6). North of about 3<inline-formula><mml:math id="M42" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S,
rainfall is substantial (averaging 0.25 mm h<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), and the enhanced RH
is almost certainly due to moist convection. The 4 km RH decreases south of
3<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, with a secondary maximum near 10–11<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. This
feature is present in other analyses as well (e.g., Modern Era-Retrospective
Analysis for Research and Applications, MERRA-2, not shown) and occurs at
the boundary between the Congo River basin (about 300 m) and the elevated
African plateau (up to 1500 m). Though moist convection is present in this
region, most of the vertical mixing is probably due to dry convection. The
effects of this dry convection on the temperature and RH profile have been
seen in the occasional radiosondes over south central Africa and downstream
over St. Helena Island.</p>
      <p id="d1e1893">Figure7a and b show latitudinal and longitudinal cross sections along
the lines indicated in cyan in Fig. 6, also for the 19-year September mean.
Figure 7a clearly shows the southern African Easterly Jet (SAEJ) near 4 km
and 8<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, just offshore at 9.75<inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. The enhanced RH extends up to
about 5–6 km between 10 and 20<inline-formula><mml:math id="M48" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, at times moist enough to support
mid-level clouds (Adebiyi et al., 2020). Notably, even though the flow is
easterly (though weaker) above 6 km, the air is dry, indicating that
convection is not reaching those levels on a consistent basis. Farther
north, moist convection is maintaining RH exceeding 80 % up to 7 km (and
higher, not shown). Another notable feature is the dry tongue extending to
10–15<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S at 1–2 km, just above the moist boundary layer. At low
levels, there is a strong southerly jet associated with the St. Helena high-pressure system. Potential temperature surfaces slope downward and northward
to about 15<inline-formula><mml:math id="M50" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, implying subsidence and drying of the northward flow
(Fig. 6a).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e1943">September-mean <bold>(a)</bold> meridional and <bold>(b)</bold> zonal cross sections of RH
(shading), potential temperature (black contours), and horizontal winds
(white barbs), with wind speeds exceeding 7 <inline-formula><mml:math id="M51" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> outlined in magenta contours
(7 m s<inline-formula><mml:math id="M52" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> – solid; 8 and 9 m s<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> – dashed), at <bold>(a)</bold> 9.75<inline-formula><mml:math id="M54" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E
and <bold>(b)</bold> 9.75<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, respectively, averaged over 19 years (2000–2018). <bold>(c)</bold> Strength of the SAEJ averaged over the volume defined by the white
rectangles in panels <bold>(a)</bold> and <bold>(b)</bold>. The solid lines represent the individual and
19-year (2000–2018) means; the dashed lines represent the standard deviation
during the 19-year period.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f07.png"/>

        </fig>

      <p id="d1e2034">The longitudinal cross section at 9.75<inline-formula><mml:math id="M56" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, the approximate meridional
center of the SAEJ, indicates that the SAEJ is strongest at the coastline.
The top of the moist layer is roughly consistent with the top of the daytime
boundary layer over the continent near 16<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E (Fig. 6b). The RH
decreases<?pagebreak page1520?> in the mean as the air flows westward, consistent with the overall
subsidence over the SE Atlantic. This subsidence is consistent with modest
radiative cooling in this region.</p>
      <p id="d1e2055">An analysis of the SAEJ (averaged over a volume the white rectangle in Fig. 6 and the upper left panels in Fig. 7a and b) shown in Fig. 7c reveals that
some months during deployment years deviated substantially from the average
(such as October 2016). The actual deployment months varied – the SAEJ
strength in September 2016 is <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M59" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> weaker than the
climatological mean, the SAEJ strength in August 2017 is weaker than the
climatological mean, and the SAEJ strength in October 2018 is very similar to
the climatological jet intensity. The individual August–October months of
the three ORACLES deployment years are compared to the climatological means
of RH and winds at 4 km altitude (represented as the SAEJ) in Fig. 8.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e2087">The same as Fig. 6 except for the 19-year mean (2000–2018) and 3 years of the ORACLES deployment (2016, 2017, and 2018). The boxes with
magenta frames indicate the ORACLES deployment months. The white rectangle
represents the area over 8–16<inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and 14–3<inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f08.png"/>

        </fig>

      <p id="d1e2115">Clearly apparent is the southward progression of the regions of significant
rainfall as the seasons change and the strengthening of the SAEJ. Note
that the basic westward circulation at 4 km is present for all 3 months
but is only about half as strong in August as in the other 2 months. The
other rows represent the three ORACLES years (2016–2018), with the relevant
deployment months outlined in magenta. A<?pagebreak page1521?> number of features are apparent.
Rainfall in September 2016 was greater in the SAEJ region than typical, and
RH values were higher. The strength of the SAEJ in 2016 was about average.
The August SAEJ strength was about average during the 2017 deployment year,
though RH values were lower than climatology. The October 2018 SAEJ
strength was also about average, rainfall was about typical, and RH values
were lower than the climatology.</p>
      <p id="d1e2118">Similar to the SAEJ feature, the southeasterly low-level jet and boundary
layer flow intensity during deployment years are within the range of
climatological mean, even though some months deviated substantially from the
average. The most important feature of the boundary layer height (BLH) over
the area that ORACLES sampled is an overall decrease in BLH from August to
October (not shown), consistent with climatological monthly-mean radiosonde
profiles at St. Helena Island (Adebiyi et al., 2015).</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Aerosol and cloud context</title>
      <p id="d1e2129">As pointed out above, the interannual variability in fire emissions in
southern Africa was expected to be low (van der Werf et al., 2010), and as a result,
aerosol loading in the ORACLES region was expected to be repeatable, with
analyses of MODIS clear-sky AOD retrievals in the project planning stage
implying year-to-year variability through the burning season of only 20 %
of the mean. Since the beginning of the ORACLES project, a number of MODIS-
and SEVIRI-based retrieval algorithms for above-cloud aerosol optical depth
(ACAOD) have been developed (Meyer et al., 2015; Jethva et al., 2016, 2018; Peers
et al., 2019; Sayer et al., 2019), allowing a study of the interannual
variability of the aerosol loading above clouds, which is more relevant for
ORACLES science objectives than clear-sky AOD. In this section, we describe
the interannual variability of MODIS-detected fire counts, ACAOD, and Sc
cloud fractions in August, September, and October for the three ORACLES
flights years, i.e., 2016–2018. We compare them to the climatologies of the
same quantities for the period of 2003 to 2018 for context (Fig. 9). MODIS
data are a composite of Terra and Aqua, where available.</p>
      <p id="d1e2132">Within each panel, Fig. 9 shows monthly averages of fire counts as
blue-to-red shading over land, ACAOD as yellow-to-red shading over ocean
(Meyer et al., 2015), and low cloud fractions as black contours over ocean,
for August, September, and October. The top row of panels shows the 2003 to
2018 climatological means, while the second, third, and fourth row of plots
provide the August, September, and October means for the 3 deployment
years, i.e., 2016 to 2018.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><?xmltex \def\figurename{Figure}?><label>Figure 9</label><caption><p id="d1e2137">Combined Terra–Aqua data for August, September, and October,
aggregated at 0.1<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. Yellow to red shading over water indicates
above-cloud AOD, black open contours indicate low-level (cloud top below
2.5 km) cloud fraction of 0.8 and 0.9, and color shading over land indicates
MODIS fire frequency for fires with detection confidence above 70 %. Top
row: climatologies computed over 2003–2018 (coinciding with the Aqua
record). Second through fourth row: monthly averages for August through
October 2016, 2017, and 2018, respectively. ST and WB stand for São
Tomé and Walvis Bay. Bold black frames indicate ORACLES deployment
months.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f09.png"/>

        </fig>

      <p id="d1e2156">Overall, Fig. 9 corroborates the initial assumption that the interannual
variability in fire locations and fire counts is relatively small. While
there are differences from month to month, both in a given year and in the
climatology, the fire counts in the three deployment years are very similar
to the climatologies, with minor differences discussed below. We attribute
this to the interannual consistency in agricultural practices in the various
burning regions. The extent of the Sc cloud deck exhibits some interannual
variability. The August Sc cloud distributions in 2016 to 2018 appear quite
similar to the August climatologies, while some of the September and October
distributions appear to extend slightly farther south or west. The largest
interannual differences of any of the quantities shown in Fig. 9 are in the
ACAOD. The August 2016 and 2018 plumes appear stronger than the
climatological plume, while the August 2017 plume appears weaker than the
climatology; the September 2016 and 2018 plumes appear slightly weaker than
the climatologies, while the September 2017 plume appears slightly stronger
than the climatological plume; the October plumes in 2016 to 2018 are
somewhat reproducible year to year, but they all appear slightly stronger
than the October climatology. Overall, this supports the conclusion of an
earlier and possibly prolonged presence of the BB plume over the SE Atlantic
in recent years, relative to the 2003 to 2018 climatology.</p>
      <p id="d1e2159">As far as the specific ORACLES deployment months are concerned (black
outlined panels in Fig. 9), September 2016 shows a slightly weaker ACAOD
plume than the climatology. We attribute this mainly to slightly weaker free
troposphere (FT) winds in the SAEJ and slightly lower RH at plume level (see
RH contours, and 7 <inline-formula><mml:math id="M63" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> contours not extending as far westward in Fig. 8). August
2017 also has a slightly weaker ACAOD plume than the climatology; since
fires are as strong<?pagebreak page1522?> or even stronger than the climatology, we again
attribute this to a slightly weaker SAEJ than the climatological mean.
October 2018 has a slightly stronger plume than the climatology: the SAEJ
winds are very similar to the climatology, but fires in southern Angola
appear to be slightly stronger and a more expansive area of elevated RH is
present by comparison to the climatology, likely giving rise to the more
expansive BB plume in this month.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Cloud droplet number concentrations and boundary layer winds</title>
      <p id="d1e2187">As ORACLES science objectives encompassed direct, semi-direct, and indirect
effects, we were keenly aware of the interannual variability of marine
boundary layer pollution levels, as well as boundary layer wind strengths
and directions. In analogy to Sect. 4.2, this section summarizes our current
assessment of the interannual variability of boundary layer winds and of
cloud droplet number concentrations, <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the latter as a proxy for BL
pollution.</p>
      <p id="d1e2201">Cloud droplet number concentrations are derived following Painemal and
Zuidema (2011) as
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M65" display="block"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.4067</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mo>[</mml:mo><mml:mrow class="unit"><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>]</mml:mo><mml:mo>×</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>(</mml:mo><mml:mtext>COD</mml:mtext><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mtext>CER</mml:mtext><mml:msup><mml:mo>)</mml:mo><mml:mrow><mml:mn mathvariant="normal">5</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where COD is the cloud optical depth and CER is the cloud droplet effective
radius near cloud top. Equation (1) assumes an adiabatic liquid water
content profile and a vertically uniform <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (Szczodrak et al., 2001).
<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is computed from COD and CER products that have accounted for the
above-cloud AOD (Meyer et al., 2015). These products are used instead of
those from the MODIS standard product (i.e., MXD06) where CODs are typically
underestimated in the retrievals due to the top of atmosphere (TOA)
shortwave reflectance absorption by overlying smoke aerosols (Haywood et
al., 2004; Coddington et al., 2010; Meyer et al., 2013).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><?xmltex \def\figurename{Figure}?><label>Figure 10</label><caption><p id="d1e2308">As in Fig. 9, but for <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> from combined Terra–Aqua
retrievals for August, September, and October, aggregated at 0.1<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>.
Black arrows denote 925 mb wind vectors with 8 <inline-formula><mml:math id="M70" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> wind vector scale shown in
the black box. The bold black frames indicate ORACLES deployment months.</p></caption>
          <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f10.png"/>

        </fig>

      <p id="d1e2355">Within each panel, Fig. 10 shows monthly averages of <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> calculated from
MODIS Aqua and Terra cloud optical depth (COD) and effective radius (CER)
retrievals as yellow-to-red shaded contours, along with 925 mb wind data from the National Centers for Environmental Prediction (NCEP) reanalysis. As in Fig. 9, the top row of plots shows the climatological mean from 2003 to 2018 for
August, September, and October, while the second, third, and fourth row show
the monthly means for the same months in 2016, 2017, and 2018, respectively.
Overall, there are striking deviations in the <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> averages in every year
relative to the climatological mean. August 2016 and August 2017 show
significantly larger <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, while August 2018 shows a lower <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
relative to climatology. By contrast, the September <inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values in 2016
to 2018 resemble the climatological mean quite closely. October 2016 and
October 2017 are again quite similar to the October climatology while the
October 2018 <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values are significantly elevated relative to
climatology. MBL winds in most months were similar to the climatological
means, with the notable exception of the 2018 October ORACLES deployment,
when the MBL winds were somewhat weaker than the climatological means.</p>
      <p id="d1e2425">To summarize our findings regarding the general plume and MBL pollution
levels during the ORACLES deployment months (September 2016, August 2017,
and October 2018), we note that the September 2016 FT plume and boundary
layer <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values were quite similar to the climatologies of these
quantities. August 2017 featured a FT BB plume with notably lower ACAOD but
an MBL with significantly elevated <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> relative to the climatologies.
October 2018 featured a markedly more expansive FT ACAOD plume and a
simultaneously more polluted MBL with significantly elevated <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.
Detailed explanations for these interannual variations are currently the
subject of at least one ORACLES-related investigation. Taking all 3 years together, mean ACAOD values were slightly lower than their
climatological mean values for August–October and <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values slightly
higher than climatology. These deviations are substantially smaller than the
day-to-day variability sampled in the three campaigns, and we therefore
consider the ORACLES measurements to have captured representative conditions
overall. Detailed assessment of the representativeness of the actual
aircraft observations, which only sampled a fraction of the days within each
of the three measurement months, has been undertaken in the
model–observation intercomparison studies (Shinozuka et al., 2020). This
assessment indicates that the airborne sampling provides averages
sufficiently representative of the monthly means to be able to characterize
and test model<?pagebreak page1524?> skill at representing geographical gradients in
climatological mean plume structure. The wide range of varying aerosol–cloud
vertical structures sampled are sufficient for addressing all of the
originally postulated objectives.</p>
</sec>
<sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Description of flights and links to data</title>
      <p id="d1e2480">In total, the P-3 aircraft flew 350.6 flight hours in 44 flights for science
operations between September 2016 and October 2018, while the ER-2 flew 97.3
flight hours in 12 science flights in 2016. Both tallies include transit
flights with science data collections into and out of the deployment sites,
because on many occasions valuable science data were collected during these
flights. The P-3 flight hours and flight counts exclude an attempt at a
transit flight from Ascension Island in 2017, which had to be aborted due to
an aircraft malfunction.</p>
      <?pagebreak page1525?><p id="d1e2483">Figure 11 shows the flight tracks of the three P-3 ORACLES deployments in
2016 (light blue), 2017 (orange), and 2018 (dark blue) and the ER-2 flights
in 2016 (green). In each of the flight years, about half of the P-3 flights
lie on top of each other along the routine flight track as described above.
For clarity, the 2018 P-3 flight tracks have been offset by 0.1<inline-formula><mml:math id="M81" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in
longitude to allow distinction from 2017 P-3 flight tracks. In their
totality, these flight tracks cover a vast portion of the climatological SE
Atlantic Sc cloud deck and the overlying BB plume.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><?xmltex \def\figurename{Figure}?><label>Figure 11</label><caption><p id="d1e2497">Flight tracks of the ORACLES aircraft in 2016 to 2018, overlain
on a MODIS-Aqua True Color Image acquired on 13 September 2018. ER-2 flight
tracks in 2016 (only deployment year) are shown in green, adapted from
© Google Maps 2020. P-3 flight tracks in 2016, 2017, and 2018 are
shown in red, orange, and blue, respectively. The 2018 P-3 flight tracks are
offset by 0.1<inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in longitude to allow distinction from 2017 flight
tracks.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f11.jpg"/>

        </fig>

      <p id="d1e2516">Table 2 summarizes eight types of flight maneuvers conducted during research
flights and briefly describes the purpose for each maneuver. Figure 12
provides a schematic representation of each of these flight maneuvers.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Table}?><label>Table 2</label><caption><p id="d1e2522">P-3 flight maneuvers conducted during research flights, and their
primary purpose.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="8cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Flight maneuver</oasis:entry>
         <oasis:entry colname="col2">Primary purpose</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">1. Ramp – RA</oasis:entry>
         <oasis:entry colname="col2">Continuous profile of thermodynamic state variables, aerosol, and cloud properties from in situ measurements, often conducted to maximize the geographic extent of a given flight, while also sampling vertical gradients.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">2. Square spiral - SS</oasis:entry>
         <oasis:entry colname="col2">A spiral descent (or ascent) for localized radiation and in situ profile measurements, modified to include four 20–30 s level segments every 90<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> heading for radiation measurements, giving the pattern the appearance of a box with rounded edges.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">3. MBL leg – ML</oasis:entry>
         <oasis:entry colname="col2">A constant-altitude leg in the MBL to assess aerosol properties and trace gas concentrations, usually below cloud.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">4. In-cloud leg – ICL</oasis:entry>
         <oasis:entry colname="col2">A nearly-constant-altitude leg, deliberately placed at an altitude of specific cloud interest, e.g., in the thickest part of the cloud or near cloud top for remote-sensing validation.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">5. Above-cloud Leg – ACL</oasis:entry>
         <oasis:entry colname="col2">A constant-altitude leg, usually just above cloud top, to ascertain the presence of a clear slot and to measure full-column above-cloud aerosol plume with remote-sensing/radiation instruments. Sometimes this leg was optimized in altitude to provide sufficient standoff for radar observations.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">6. Sawtooth leg – STL</oasis:entry>
         <oasis:entry colname="col2">A flight segment that continuously profiles from just above cloud top to just below cloud base, to ascertain the cloud vertical structure; also useful for quick above-cloud aerosol assessments at the top of each sawtooth.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">7. In-plume leg – IPL</oasis:entry>
         <oasis:entry colname="col2">A constant-altitude leg deliberately placed at a specific altitude to assess aerosol properties with in situ measurements; frequently in the heaviest aerosol loading to provide the largest signal-to-noise ratio.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">8. Above-plume leg - APL</oasis:entry>
         <oasis:entry colname="col2">A constant-altitude leg above the BB aerosol layer, usually intended for full-column lidar assessments with HSRL-2.</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12"><?xmltex \currentcnt{12}?><?xmltex \def\figurename{Figure}?><label>Figure 12</label><caption><p id="d1e2633">Schematic of flight maneuvers during research flight linked to
descriptions in Table 2 and flight synopses in Tables A1–A3.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f12.png"/>

        </fig>

      <p id="d1e2642">Tables A1–A3 in Appendix A summarize the flights of both ORACLES aircraft in
2016, 2017, and 2018. They include a brief flight synopsis and the number of
each of the eight flight maneuvers described in Table 2 for every flight.
Detailed flight reports for each of the flights listed in Tables A1–A3 can
be found at the project web page: <uri>https://espo.nasa.gov/oracles/mission-flight-docs</uri> (last<?pagebreak page1526?> access: May 2020). ORACLES data are
archived permanently with separate digital objective identifiers (DOIs) for
each deployment year and separate DOI for the two aircraft participating in
the 2016 deployment (see references for ORACLES Science Team, 2020–2016 P-3
data, 2016 ER2 data, 2017 P-3 data, and 2018 P-3 data). A link to images and
KMZ files for flight tracks, data from ground-based instruments, and other
auxiliary information can be found at <uri>https://espo.nasa.gov/home/oracles/content/ORACLES_Science</uri> (last access: May 2020).
Video footage from the P-3 front and nadir cameras is available at
<uri>https://asp-archive.arc.nasa.gov/Oracles/N426NA/Video/</uri> (last access: May 2020).</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Preliminary science findings and implications</title>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>List of golden days for various objectives</title>
      <p id="d1e2670">The target-of-opportunity flights, described in Sect. 4.4, usually were
designed to address more focused scientific objectives within the context of
the general science objectives. Broadly, these objectives can be
characterized as pertaining to (i) the radiative interactions of aerosols
and clouds (radiation flights); (ii) the microphysical interactions of
aerosols and clouds as they are affected by vertical mixing, drizzle
suppression, etc. (cloud microphysics flights); and (iii) the spatiotemporal
evolution of aerosol microphysics in the BB plume (plume evolution flights).
In addition, a number of<?pagebreak page1527?> flights provided an excellent dataset for the
evaluation of remote-sensing concepts (see Sect. 5.3.7), often on the basis
of successful coordination of the P-3 with the ER-2 in 2016 or with
satellite assets in 2017 and 2018. Table 3 provides a list of “golden
days” for each observational focus, to be interpreted as the likely best
start of exploration of the ORACLES dataset for an uninitiated science
user. The ordering of flights within each category is based on a preliminary
assessment of the utility and quality of the data to address the
observational objective. Flights with coordinated P-3 and ER-2 sampling in
2016 are postulated to provide superior data and hence appear before any
single-aircraft flights. Future analyses are likely to provide a revised
list of useful flight days in the context of detailed and overarching
ORACLES objectives.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Table}?><label>Table 3</label><caption><p id="d1e2676">ORACLES golden flight days by observational focus.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="2">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">

         <oasis:entry colname="col1">Observational focus</oasis:entry>

         <oasis:entry colname="col2">Dates (mm/dd/yyyy) – P-3/ER-2 flight number</oasis:entry>

       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="7">Radiation</oasis:entry>

         <oasis:entry colname="col2">09/20/2016 – PRF11Y16/ERF06Y16</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">09/14/2016 – PRF09Y16/ERF03Y16</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">09/27/2016 – ERF10Y16</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">09/02/2016 – PRF03Y16</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">08/13/2017 – PRF02Y17</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">08/26/2017 – PRF09Y17</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">09/30/2018 – PRF02Y18</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">10/05/2018 – PRF05Y18</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="10">Cloud microphysics</oasis:entry>

         <oasis:entry colname="col2">09/20/2016 – PRF11Y16/ERF06Y16</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">09/14/2016 – PRF09Y16/ERF03Y16</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">09/06/2016 – PRF05Y16</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">09/25/2016 - PRF13Y16</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">08/28/2017 – PRF10Y17</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">08/13/2017 – PRF02Y17</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">09/02/2017 – PRF13Y17</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">10/03/2018 – PRF04Y18</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">10/02/2018 – PRF03Y18</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">10/23/2018 – PRF13Y18</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">10/12/2018 – PRF08Y18</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry rowsep="1" colname="col1" morerows="7">Plume evolution</oasis:entry>

         <oasis:entry colname="col2">09/18/2016 – PRF10Y16/ERF05Y16</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">09/24/2016 – PRF12Y16/ERF08Y16</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">09/06/2016 – PRF05Y16</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">08/17/2017 – PRF04Y17</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">08/21/2017 – PRF07Y17</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">08/31/2017 – PRF12Y17</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col2">10/17/2018 – PRF10Y18</oasis:entry>

       </oasis:row>
       <oasis:row rowsep="1">

         <oasis:entry colname="col2">10/19/2018 – PRF11Y18</oasis:entry>

       </oasis:row>
       <oasis:row>

         <oasis:entry colname="col1">Remote-sensing test bed data</oasis:entry>

         <oasis:entry colname="col2">09/20/2016 – PRF11Y16/ERF06Y16</oasis:entry>

       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Examples of significant findings</title>
<sec id="Ch1.S4.SS2.SSS1">
  <label>4.2.1</label><title>HSRL-2 statistics on contact of plume and cloud tops</title>
      <p id="d1e2902">An important line of inquiry and indeed a major motivation for the ORACLES
project was the question of how frequently Sc clouds in the SE Atlantic MBL
are in physical contact with the BB plume emanating from the southern
African continent. The only prior work in the area using in situ aircraft
measurements (Haywood et al., 2003) found frequent separation between cloud
and aerosol close to the coast of Namibia and Angola but potential
interactions between cloud and aerosol in the vicinity of Ascension Island.
However, the statistical relevance of those findings is impossible to
establish given the scarcity of the available in situ data. For a large
number of coincident CALIOP and MODIS aerosol and cloud retrievals in the SE
Atlantic region, Costantino and Bréon (2013) found that more than half of
the vertical profiles they studied indicated “well-separated” aerosol<?pagebreak page1528?> and
cloud layers, i.e., an “aerosol-free gap” above cloud top. They went on to
attribute the differences in cloud effective radii between separated and
unseparated cases to the probable paucity of aerosols in the MBL in the
separated cases. ORACLES observations show that the separation of aerosol
and cloud layers in an instantaneous profile is a poor indicator for the
concentration of aerosol in the MBL, because there are many other pathways
for the aerosol to reach the MBL at a given location. However, the physical
contact of the BB plume and Sc cloud tops is indicative of active
entrainment of BB aerosol into the MBL and is often associated with
significant BB aerosol in the MBL. The relatively low signal-to-noise ratio (SNR)
in CALIOP vertical profiles after traversing a BB plume with significant
optical attenuation, also alluded to in Sect. 2.1, raises the question of
how accurate the CALIOP-indicated frequent separation between the BB plume
and Sc cloud tops (shown in Fig. 2) really is.</p>
      <p id="d1e2905">To help address this question, we investigate here how frequently the HSRL-2
aerosol extinction profiles in the three ORACLES deployments indicate
separation or lack thereof between the BB plume base and the Sc cloud tops.
The left panel of Fig. 13 shows mean aerosol extinction profiles at 532 nm
for each ORACLES deployment year, along with mean cloud top heights as
horizontal solid lines. Because ORACLES-2016 had a somewhat different
geographic focus from ORACLES-2017 and ORACLES-2018, Fig. 13 only shows data
for the geographic box bounded by 5–15<inline-formula><mml:math id="M84" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and 2.5–7.5<inline-formula><mml:math id="M85" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, where
there are data present in all 3 flight years.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13" specific-use="star"><?xmltex \currentcnt{13}?><?xmltex \def\figurename{Figure}?><label>Figure 13</label><caption><p id="d1e2928"><bold>(a)</bold> A composite of vertical profiles of aerosol
extinction at 532 nm, derived from HSRL-2 measurements for each of the
deployment months bounded by 5–15<inline-formula><mml:math id="M86" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and 2.5–7.5<inline-formula><mml:math id="M87" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. Shaded regions
represent 1 standard deviation of extinction measurements. Solid
horizontal lines indicate the mean cloud top heights for each dataset.
<bold>(b)</bold> Cumulative distribution function for mean aerosol
backscattering in the 300 m layer above cloud top.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f13.png"/>

          </fig>

      <p id="d1e2961">The mean extinction profiles show that the BB plume in ORACLES-2017 (August)
has a local maximum of aerosol extinction at altitudes between 2–3 km, while
the ORACLES-2016 (September) and ORACLES-2018 (October) mean profiles have
maximum aerosol loading between 3.0 and 4.5 km in altitude, albeit with
somewhat lower values. In all 3 years, there is a relative minimum in
aerosol loading near the location of the mean cloud tops. This suggests that
the air mass just above cloud top may indeed be significantly older, more
processed, and scavenged than the<?pagebreak page1529?> FT above and possibly even the BL below,
which may have been subject to entrainment of FT air upstream of the BL
flow, to the south of the bounding box.</p>
      <p id="d1e2964">The separation between the BB plume base and the cloud tops for each year is
indicated in the right hand panel in Fig. 13. It shows the cumulative
distribution of HSRL-derived aerosol backscattering coefficient at 532 nm in
the 300 m layer just above cloud top for the same geographic region as the
left panel. The cumulative distribution of aerosol backscatter values near
the cloud top varies sigmoidally, without any discontinuity that would
indicate an unambiguous lower edge to the aerosol layer. Instead, it is
apparent that the assessment of an aerosol-free gap depends entirely on
the definition of the aerosol loading. For example, the August 2017 and
October 2018 deployments featured a relatively low fraction of profiles with
less than 0.25 M m<inline-formula><mml:math id="M88" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> Sr<inline-formula><mml:math id="M89" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> aerosol backscatter coefficient in the
first 300 m above cloud, i.e., 3 % and 15 % for 2017 and 2018,
respectively. The September 2016 profiles in this region on the other hand
show less than 0.25 M m<inline-formula><mml:math id="M90" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> Sr<inline-formula><mml:math id="M91" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> aerosol backscatter coefficient, and
hence an aerosol-free gap, almost 50 % of the time. Regardless of the
exact threshold chosen, September 2016 showed by far the highest frequency
of aerosol-free gaps above clouds when compared to the 2017 and 2018
deployments. The representativeness of this September maximum in
aerosol-free gaps above clouds is unknown and will need to be explored with
future satellite lidar observations of sufficient accuracy. Overall, we
found significant spatial and temporal variability in the degree of contact
between BB aerosol and Sc clouds in the SEA region and that the frequency
of occurrence of aerosol-free gaps is likely much lower than previously
assumed (Costantino and Bréon, 2013). These findings need to be considered
when interpreting previous results on aerosol–cloud interactions in the
region.</p>
      <p id="d1e3015">ORACLES data provide a useful test bed for algorithm development in support
of future satellite missions, for example NASA's ACCP (Aerosols, Clouds,
Convection and Precipitation) mission. For instance, ORACLES observations
are currently being used to develop joint polarimeter–lidar retrievals of
aerosol and cloud properties. Whether such observations will successfully
detect features such as the clear-air layers in the SEA will depend on
specific instrument characteristics, but the ORACLES measurements should
provide useful benchmarks for the testing of candidate observing concepts.</p>
</sec>
<sec id="Ch1.S4.SS2.SSS2">
  <label>4.2.2</label><title>Vertical plume structure and chemical composition</title>
      <p id="d1e3026">The lidar-derived increase in extinction with height for September (2016) in
Fig. 13 is accompanied by a similar increase with height of the mean in situ
SSA (derived from the in situ PSAP absorption paired with nephelometer
scattering at 530 nm) from 0.84 to 0.87 (Fig. 14, middle of top row). The
SSA values are in reasonable agreement with values of <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.83</mml:mn></mml:mrow></mml:math></inline-formula>
for dry conditions in Davies et al. (2019) derived using state-of-the-art
photoacoustic and cavity ring-down instrumentation. Pistone et al. (2019)
compare the ORACLES absorption–scattering measurements with SSA derived by
several different airborne remote-sensing methods at wavelengths between 400
and 995 nm and found reasonable agreement both for specific case studies and
for the range of measured spectral SSA over the full ORACLES-2016
deployment.</p>
      <p id="d1e3039">Black carbon is the primary absorber of sunlight within BB aerosol (e.g.,
Bond et al., 2013). Although a<?pagebreak page1530?> corresponding decrease with height of the
refractory black carbon (BC) mass concentration relative to the mean organic
aerosol (OA) mass concentration is not clearly apparent in Fig. 14, (middle
of middle row), an example from an individual profile from the 24 September 2016 flight indicates more nitrate and organic aerosol above 3.5 km than
below it, relative to the black carbon mass concentration (Fig. 14, middle
of bottom row). This is consistent with an increase in SSA with height.
Examples of individual profiles are shown from each year, broken down by
aerosol species – black carbon, organic aerosol, nitrate (NO<inline-formula><mml:math id="M93" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>), ammonium
(NH<inline-formula><mml:math id="M94" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>) and sulfates (SO<inline-formula><mml:math id="M95" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>), indicate distinct vertical structures
(Fig. 14 bottom row).</p>
      <p id="d1e3069">Profiles from August 2017 also indicate some vertical structure to the SSA
without a clear mapping to the <inline-formula><mml:math id="M96" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">BC</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">OA</mml:mi></mml:mrow></mml:math></inline-formula> ratio, while the mean SSA from the
October 2018 deployment increases even more sharply with altitude than does
the mean SSA from September (2016). For October 2018, the increase of SSA
with height is clearly consistent with the proportional increase in organic
aerosol relative to black carbon. Work is ongoing to attribute changes in
SSA to both thermodynamically driven changes in gas–particle phase
partitioning (e.g., Wu et al., 2020) and more irreversibly driven changes
related to forms of photodegradation in this near-equatorial, sun-exposed
environment. Overall the SSA values are less than has been previously
assumed, with that implication further explored within the modeling study of
Mallet et al. (2020).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F14" specific-use="star"><?xmltex \currentcnt{14}?><?xmltex \def\figurename{Figure}?><label>Figure 14</label><caption><p id="d1e3087"><bold>(a–c)</bold> Deployment-mean 530 nm SSA vertical profiles for each
year for the August (2017), September (2016), and October (2018)
deployments. <bold>(d–f)</bold> The corresponding mean black carbon to organic
aerosol ratio (<inline-formula><mml:math id="M97" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">BC</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">OA</mml:mi></mml:mrow></mml:math></inline-formula>) profiles. <bold>(g–i)</bold> Example profiles of individual
aerosol species, from left to right: 30 August 2017, 12:40–13:00 UTC,
8<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/<inline-formula><mml:math id="M99" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; 24 September 2016, 12:45–13:00 UTC, 12.34<inline-formula><mml:math id="M100" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/11<inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; and 4 October 2018, 13:00–13:15 UTC,
4.6<inline-formula><mml:math id="M102" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/5<inline-formula><mml:math id="M103" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. A blue line connects mean values, with
box–whisker plots indicating the 10th, 25th, 50th, 75th, and 90th percentile values.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f14.png"/>

          </fig>

      <p id="d1e3171">Some of the differences between the individual profiles in Fig. 14, bottom
row, can be related to differences in the prevailing meteorology shown in
Fig. 8. The distinctive two-layer aerosol structure profiled on 24 September 2016 reflects the ability of strong winds at 4 km (see also Fig. 6) to disperse aerosol westward, with the aerosol lower down, at 2–3 km,
resulting from an anticyclonic circulation (Fig. 8). The strong 4 km zonal
winds are much less apparent in August, consistent with a lower-lying, less
layered aerosol vertical structure. The free-tropospheric winds remain
strong into October, but by then the fire emissions have reduced
considerably and less aerosol appears to reach the altitude at which the
zonal winds are strongest.</p>
</sec>
<sec id="Ch1.S4.SS2.SSS3">
  <label>4.2.3</label><title>Chemical aging</title>
      <p id="d1e3182">Ongoing analysis of the ORACLES dataset is relating the observed vertical
structure in aerosol composition and optical properties to aerosol aging.
Rather than using an aircraft to track the evolution of a smoke plume as it
advects, or using an aerosol chemical component as a “chemical clock” to
determine aerosol age, an alternative approach links a model-derived mean
aerosol age to in situ aerosol characteristics. Particles, including at fire
emission sources, are marked at the time of the model initialization and
tracked in time thereafter (Saide et al., 2016), with the particle ages
subsequently extracted along the flight legs and these modeled ages
combined with the in situ datasets. An example is shown in Fig. 15 for 24 September 2016 (a profile from this flight is also shown in Fig. 14), using
aerosol age derived from one of the ORACLES in-field aerosol forecasting
models, WRF-AAM (see Sect. 3.3.5). The model-derived mean aerosol age
height–latitude cross section is overlaid with measurements of f44, the mass-to-charge ratio <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula> 44 relative to total organics. Higher fractions of f44
reflect the formation of carboxylic acids, which coincide with older aerosol
ages up to approximately 10 d. The ORACLES f44 values shown here are on
par with those reported for Siberian biomass burning aerosol after
trans-Pacific transport to Alaska. Notable is that younger aerosol overlies
older aerosol on this day, coinciding with the altitude range of strong
zonal winds (not shown, but consistent with Fig. 6). This figure also
highlights the wide range of aerosol ages beyond 4 d that ORACLES sampled
during its flights, marking another unique contribution by the ORACLES
campaign. Ongoing work is relating the model-derived aerosol aging to a
continuous depletion of non-black-carbon aerosols.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F15" specific-use="star"><?xmltex \currentcnt{15}?><?xmltex \def\figurename{Figure}?><label>Figure 15</label><caption><p id="d1e3199">The WRF-AAM model-derived mean aerosol age along the P-3 flight
track for 24 September 2016, overlain with a measure of aerosol oxidation
derived from in situ f44 measurements on the P-3 aircraft.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f15.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS2.SSS4">
  <label>4.2.4</label><title>Boundary layer clouds – CCN, cloud, and rain statistics</title>
      <p id="d1e3216">ORACLES scientific objective 3 (Table 1) seeks to understand the extent to
which smoke aerosol from southern Africa mixes into the MBL and impacts
marine low cloud microphysical processes. Smoke may enhance the population
of cloud condensation nuclei (CCN), which can lead to increases in cloud
droplet concentration and smaller droplet sizes. It can also potentially
induce changes in cloud condensate through suppressing precipitation rates,
enhancing cloud top entrainment, and otherwise influencing cloud
macrophysical properties. These indirect effects lead to significant
increases in albedo in global models, but little in situ data are available
over the SE Atlantic to test these models.</p>
      <?pagebreak page1532?><p id="d1e3219">According to HSRL-2 observations (Fig. 13), a denser, more frequent smoke
layer in the FT occurred in 2017 than in 2016 or 2018. CCN measurements made
on all three ORACLES deployments (Kacarab et al., 2020) provide evidence that
FT CCN concentrations were also higher in 2017 (Fig. 16a). Despite the
frequent contact of the smoke with the sub-cloud planetary boundary layer
(PBL) top, concentrations of CCN in the PBL are much lower than those in the
FT (compare panels a and b in Fig. 16). Also, despite very similar FT CCN
concentrations in 2016 and 2018, PBL CCN levels were actually significantly
higher in 2018 than in 2016 (Fig. 16b), suggesting that the FT CCN
concentration alone is not a unique determinant of microphysical properties
in the PBL. As noted in Diamond et al. (2018), it is the history of
subsidence and entrainment of smoke into the PBL, rather than the
instantaneous presence of aerosol immediately above clouds, that sets the
MBL CCN level and therefore cloud droplet concentration (<inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>).
Seasonally, satellite evidence (Fig. 10) indicates that the highest <inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
values offshore occurred in 2017, and this is consistent with the highest
measured PBL CCN concentrations (at supersaturations <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula> %)
occurring during 2017. October 2018 also showed high <inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values offshore
consistent with the higher measured CCN concentrations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F16"><?xmltex \currentcnt{16}?><?xmltex \def\figurename{Figure}?><label>Figure 16</label><caption><p id="d1e3267">Composite CCN supersaturation spectra (concentration of CCN as a
function of the applied supersaturation, SS) for <bold>(a)</bold> the free-tropospheric
BB plume and <bold>(b)</bold> the MBL within a region (5–15<inline-formula><mml:math id="M109" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and 2.5–7.5<inline-formula><mml:math id="M110" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) sampled during all three deployments.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f16.png"/>

          </fig>

      <p id="d1e3301">In addition to entrainment of smoke from the FT, the concentration of CCN
and resulting droplet concentrations in the marine PBL are also modulated
strongly by coalescence scavenging by light precipitation (Wood et al.,
2012). In addition, evidence suggests that precipitation can be suppressed
in clouds with high CCN and <inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (e.g., Sorooshian et al., 2009). The
APR-3 radar on the P-3 is sufficiently sensitive to detect this light
precipitation. Measurements of precipitation from the APR-3 indicated
significant differences in precipitation during the three campaigns (Fig. 17). Comparing the two campaigns flown out of São Tomé (2017 and
2018), precipitation was significantly lighter in 2017 (Fig. 17), which may
indicate suppression due to higher droplet concentrations, but additional
analysis of cloud thickness and liquid water path differences between the
campaigns is underway to quantify these impacts (see also Dzambo et al.,
2020).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F17" specific-use="star"><?xmltex \currentcnt{17}?><?xmltex \def\figurename{Figure}?><label>Figure 17</label><caption><p id="d1e3317">The fraction of clouds in which rain is possible, probable, and
certain, for the ORACLES research flights in 2016 <bold>(a)</bold>, 2017 <bold>(b)</bold>, and
2018 <bold>(c)</bold> as detected using the APR-3 radar. Certain rain (dark green),
probable rain (medium green), and possible rain or drizzle (light green) are
shown left to right for each research flight, which are determined by each
cloudy profile's maximum reflectivity being greater than 0, <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7.5</mml:mn></mml:mrow></mml:math></inline-formula>, and
<inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula> dBZ respectively (see Haynes et al., 2009, for more information).</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f17.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS2.SSS5">
  <label>4.2.5</label><title>Evidence of aerosol indirect effects</title>
      <p id="d1e3364">Observations obtained by in situ probes installed on the NASA P-3 are being
used to investigate cloud–aerosol interactions. Over the 3-year period of
ORACLES, 397 vertical profiles were flown through clouds during either
sawtooth profiles (see Fig. 11) or in individual cloud profiles isolated in
time–space from other profiles. The vertical dependence of cloud properties
in a common reference frame is examined using a normalized altitude
<inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, defined as (<inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mi>Z</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>/</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math id="M116" display="inline"><mml:mi>Z</mml:mi></mml:math></inline-formula> is altitude, <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">t</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> cloud
top altitude and <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">b</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> cloud base altitude. This allows us to composite the
vertical microphysical structure of cloud decks from many different clouds.</p>
      <p id="d1e3442">We select 397 vertical profiles through the cloud layer when
accumulation-mode (<inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.1</mml:mn><mml:mo>&lt;</mml:mo><mml:mi>D</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M120" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>) aerosol
concentration (<inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) was measured at least 100 m above and below cloud
using the Passive Cavity Aerosol Spectrometer Probe (PCASP). Each profile
was classified as “Contact” or “Separated” based on whether the layer of
enhanced above-cloud aerosol concentration (defined as PCASP <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) was in contact with cloud top or separated from
it by at least 100 m. Each of the “Contact” and “Separated” profiles was
further classified based on whether the average PCASP <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> within the 100 m layer below cloud base was greater than or less than 250 cm<inline-formula><mml:math id="M125" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Four
different regimes were thus defined based on the below-cloud boundary layer
<inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and by whether or not the cloud layer was in contact with an
overlying biomass burning aerosol (BBA) plume or separated from it.</p>
      <p id="d1e3544">Figure 18 shows the mean cloud droplet concentration <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as a function
of <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the four regimes. The average boundary layer <inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values for the
regimes are as follows: Contact/<inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula>, 184 cm<inline-formula><mml:math id="M131" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; Contact/<inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula>, 507 cm<inline-formula><mml:math id="M133" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>;
Separated/<inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula>, 113 cm<inline-formula><mml:math id="M135" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; Separated/<inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula>, 318 cm<inline-formula><mml:math id="M137" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The average boundary layer
<inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is a good predictor of the vertical mean <inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> across the four
regimes, consistent with the primary source for droplets being aerosols
ingested into cloud base (Diamond et al., 2018). Although <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is
approximately constant with height for the two Separated regimes and the
Contact/<inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M142" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> regime, consistent with many
previous studies (Nicholls and Leighton, 1986; Martin et al., 1994; Miles et
al., 2000; Painemal and Zuidema, 2011; Wood, 2012), it experiences a
significant and unexpected increase with <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the
Contact/<inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M145" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> case. The highest <inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values
occur where the MBL has both high <inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and is in contact with overlying
BB aerosol layers. The lowest boundary layer <inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is found where there is
separation from the overlying aerosol. It is perhaps surprising that clouds
within boundary layers with higher <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> but not overlain by aerosol, or
clouds within boundary layers with lower <inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> but overlain by aerosol,
possess very similar <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. This further suggests that clouds' history of
interacting with aerosol within the prior days (Mauger and Norris, 2007;
Diamond et al., 2018) can have an impact on <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> but that aerosols
entrained from above cloud top also have an impact on <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. These
findings are further described by Gupta et al. (2020).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F18"><?xmltex \currentcnt{18}?><?xmltex \def\figurename{Figure}?><label>Figure 18</label><caption><p id="d1e3881">Mean cloud droplet number concentration (<inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) as a function
of normalized cloud depth (<inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mi>Z</mml:mi><mml:mi mathvariant="normal">N</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), where the mean is computed for 397
vertical profiles flown during the three ORACLES campaigns. Different colors
correspond to whether the boundary layer below cloud has average aerosol
concentration <inline-formula><mml:math id="M156" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M157" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> or <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">250</mml:mn></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M159" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> as measured by PCASP and according to whether a layer of BB
aerosol is in contact with (<inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M161" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> within 100 m
of cloud top) or separated from cloud top (no layer with <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">500</mml:mn></mml:mrow></mml:math></inline-formula> cm<inline-formula><mml:math id="M163" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> within 100 m of cloud top). Uncertainties
indicated by horizontal error bars represent the 95 % confidence
intervals. Numbers in parentheses represent the number of 1 s data points
included in each of the profiles. See text for details.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f18.png"/>

          </fig>

</sec>
<?pagebreak page1533?><sec id="Ch1.S4.SS2.SSS6">
  <label>4.2.6</label><title>Comparisons of models and observations</title>
      <?pagebreak page1534?><p id="d1e4029">Approximately one-half of all of the flights were devoted to a routine path,
motivated by a desire to facilitate model improvement through an unbiased
sampling performed frequently enough to adequately capture the monthly mean
(see Sect. 3.3.6). An a priori evaluation based on the random sampling of
clear-sky aerosol optical depths rationalized the decision to allocate six to eight flights to a routinely sampled flight line, on random days during the
deployment. The initial model–observation comparison (Shinozuka et al.,
2020), which is based on the 2016 measurements only, includes model versions
similar to those used for the aerosol forecasts in the field (WRF-CAM5
(Weather Research and Forecasting – Community Atmosphere Model 5) and GEOS-5
(Goddard Earth Observing System, Version 5)), as well as the UK
Meteorological Office Unified Model (UM), the French ALADIN-Climate (Aire
Limitée Adaptation dynamique Développement InterNational – Climate,
Mallet et al., 2019), the global GEOS-Chem (Goddard Earth Observing System –
Chemistry) model, and the E3SM (Energy Exascale Earth System Model)
Atmosphere Model (EAM). Measured variables which are compared include the
aerosol layer top/bottom boundaries (as determined from lidar and in situ),
aerosol extinction (lidar and in situ), black carbon and organic aerosol
mass concentrations (SP2 and AMS), carbon monoxide, scattering and
absorption Ångström exponents, and the single-scattering albedo
(in situ). The new datasets allow an extension beyond previous assessments
emphasizing the aerosol layer boundaries only (Das et al., 2017; Koffi et
al., 2012). Not all of the models include all of these variables, and no
effort is made to standardize model features such as the emissions databases
and frequency of initialization. The project confronted the issue of how
best to compare infrequently sampled but detailed measurements to
frequently sampled but coarsely resolved model output, through aggregating
both measured and model data into approximately 2 by 2<inline-formula><mml:math id="M164" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid boxes
centered on the routine flight track (see Fig. 19 for an example). This
approach is similar to that applied within the AeroCom community (e.g.,
Katich et al., 2018; Myhre et al., 2013). The smaller grid spacings applied
within a larger domain also clarify the ability of models to transport
aerosol further offshore. A further study will apply a similar approach to
model–observation comparisons based on the 2017 and 2018 deployments.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F19" specific-use="star"><?xmltex \currentcnt{19}?><?xmltex \def\figurename{Figure}?><label>Figure 19</label><caption><p id="d1e4043">Vertical distribution of mid-visible ambient aerosol extinction
from four models compared to dry ORACLES observations in <inline-formula><mml:math id="M165" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M166" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> grid
boxes (locations indicated) along the 2016 routine flight track.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f19.png"/>

          </fig>

      <p id="d1e4072">Shinozuka et al. (2020) assessed modeled aerosol properties through
examining three separate layers and concluded that the upper 3–6 km layer
generally contains less aerosol in the models than is observed, primarily
because the aerosol layer tops are placed too low. Another approach, applied
within Doherty et al. (2021) is examining the vertical distribution of
aerosol (as in Fig. 19) and those cloud properties (cloud fraction and
optical depth) important for quantifying the direct aerosol radiative
effect. For example, they find significant differences in both the absolute
value and vertical structure of SSA in the observations versus in the
models, as well as significant differences between models. Consistent with
Shinozuka et al. (2020), the model bias has an altitude dependence that
results from the models generally placing the plume at too low an altitude.
The covariance in the model bias in extinction and SSA with altitude affects
the column SSA – the parameter of interest for determining plume aerosol
direct radiative effect. Therefore Doherty et al. (2021) also compare observed to
modeled extinction-weighted (or column-aerosol) SSA for the smoke plume.
This and related analyses in the paper lay the groundwork for determining
which modeled parameters are contributing most to biases in modeled aerosol
direct radiative effect of the smoke.</p>
</sec>
<sec id="Ch1.S4.SS2.SSS7">
  <label>4.2.7</label><title>Illustration of remote-sensing test bed</title>
      <p id="d1e4083">As alluded to in Sect. 2.1, a subordinate, yet important objective for
ORACLES was the acquisition of data that can be used for the refinement and
testing of retrieval capabilities for instrument concepts that have a
potential for deployment to space. Among the remote-sensing instruments
participating in ORACLES, the following have a link to space-based
instrument concepts: HSRL-2 (future HSRL in space), APR-3 (CloudSat's CPR,
GPM's DPR, RainCube's radar, EarthCARE's CPR, and candidate radars for
future missions targeting clouds, convection, and precipitation), RSP (APS
on Glory), AirMSPI (MAIA), and eMAS (MODIS). Examples of algorithm
developments using ORACLES data include Xu et al. (2018), Segal-Rozenhaimer
et al. (2018), and Miller et al. (2020), who created new cloud retrieval
algorithms for the AirMSPI and RSP instruments. Additionally, the NASA Ames
4STAR instrument was used to provide AERONET-like retrievals of aerosol
microphysics on the basis of sky radiance measurements from an airborne
platform (Pistone et al., 2019), the SSFR instrument provided
within-atmosphere spectral radiative flux observations for direct
measurements of scene and cloud albedos both from the P-3 and from the ER-2
in 2016 (Cochrane et al., 2019), and HSRL-2 successfully deployed a very
stable and accurate density-tuned interferometer as a prototype for
spaceborne instrumentation and leveraged the resulting high accuracy in
the measurements to infer aerosol microphysical properties (Burton et al.,
2018). In combination, these instruments provide a powerful and
unprecedented toolset for retrieving atmospheric trace gases, aerosol, and
cloud properties, with simultaneous closure opportunities against the
spectral radiative flux observations (see Fig. 20). The resulting dataset
will be used in the testing of instrument and algorithm concepts for future
satellite missions, such as the NASA Aerosol, Clouds-Convection and
Precipitation (ACCP) mission, recommended by the 2018 Decadal Survey for
Earth Observations from Space (National Academies of Sciences, Engineering,
and Medicine, 2018) and the NASA Plankton, Aerosol, Cloud, Ocean Ecosystem
(PACE) mission (Werdell et al., 2019), due for launch in 2023.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F20" specific-use="star"><?xmltex \currentcnt{20}?><?xmltex \def\figurename{Figure}?><label>Figure 20</label><caption><p id="d1e4088">Illustrative remote-sensing observations in ORACLES-2016. <bold>(a)</bold> Vertical structure of aerosol backscatter and W-band reflectivity from
HSRL-2 and APR-3, respectively. <bold>(b)</bold> Degree of linear polarization (DoLP) and RGB imagery from AirMSPI
(bow-tie patterns) and eMAS, respectively. <bold>(c)</bold> Above-cloud AOD (ACAOD)
retrievals from various P-3, ER-2, and satellite instruments. <bold>(d)</bold> COD
retrievals from various P-3, ER-2, and satellite instruments.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f20.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S4.SS3">
  <label>4.3</label><title>A revised schematic view of the system</title>
      <p id="d1e4118">Based on the knowledge acquired thus far from ORACLES analysis, we present a
revised schematic of the system (Fig. 21) compared with what was described
in Sect. 2 as the state of knowledge during ORACLES conception and planning.
Smoke from biomass burning over the southern African continent in Austral
winter and spring (July–October) is emitted into a continental boundary
layer that is potentially warmer, and therefore more buoyant, than the cold
marine PBL to the west. As this smoke moves westward over the SEA, it must
first cool to allow it to subside and be entrained into the PBL. In the free
troposphere, clear-sky longwave cooling by emission to space helps drive
large-scale subsidence. This process is slow, with typical
radiatively driven subsidence rates of 200 400 <inline-formula><mml:math id="M167" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">d</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (Betts and Ridgway,
1988). Solar heating by absorbing aerosol may significantly slow down this
process (Sakaeda et al., 2011). As the smoke moves initially westward over
the SEA, it typically takes 6–10 d to subside from the jet core to the
top<?pagebreak page1536?> of the marine PBL. Typical free-tropospheric wind speeds over the SEA in
the southern African Easterly Jet (SAEJ) can reach 5 <inline-formula><mml:math id="M168" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, so smoke can
travel hundreds to a few thousand kilometers offshore in the time taken to descend
from the main smoke outflow altitude of 4–5 km. However, FT wind speeds over
the SEA are quite variable (see Fig. 15 in Adebiyi and Zuidema, 2016) and are
modulated by tropical wave disturbances and by incursions of midlatitude
systems into the tropics over the Southern Ocean. Depending upon winds in
the FT, smoke trajectories may result in only modest horizontal
displacement or may (as in the case shown in the schematic Fig. 21) be
advected as far south as 30<inline-formula><mml:math id="M169" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, especially when midlatitude
systems result in re-circulating trajectories that move air back toward the
African continent after initial outflow. Thus, smoke aerosol may be
entrained into the PBL over a relatively wide geographical region.</p>
      <p id="d1e4164">Because subsidence is strongest off the coast of Namibia and southern
Angola, this makes it a favored region for entrainment of smoke into the
marine PBL, especially from recirculating trajectories like the one shown in
Fig. 21. This setup results in a typical (September) vertical plume
structure in the ORACLES sampling region comprising relatively young aerosol
aloft, more aged aerosol immediately above cloud, and the oldest aerosol
typically in the marine PBL itself. However, the extensive lateral
displacement of the core, and a wind structure with significant vertical
shear, means that the presence of smoke immediately above cloud top is
intermittent. The PBL over the SEA therefore entrains a considerable volume
of clean air, especially from the Southern Ocean. Thus, mean CO levels in
the PBL are lower than 100 ppm, while FT plume mean values are typically
150–200 ppm (Shinozuka et al., 2020). With typical unpolluted background
levels of 50–70 ppm, this suggests that the majority of the air in the PBL
has origins in regions other than those affected by biomass burning.
Although this is the case, smoke plumes in the FT have very high aerosol
levels (mass, concentration) compared with those in the pristine marine PBL
(see Shinozuka et al., 2020), so even quite small mean elevations of CO in
the PBL are associated with large aerosol perturbations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F21"><?xmltex \currentcnt{21}?><?xmltex \def\figurename{Figure}?><label>Figure 21</label><caption><p id="d1e4169">A schematic showing an example of a commonly occurring trajectory
pathway into the marine PBL for smoke aerosol ejected from southern Africa
in the core (3–5 km altitude) of the southern African Easterly Jet  (SAEJ).
This is overlaid onto an August–October mean climatology of cloud droplet
concentration (colors) derived using MODIS (Bennartz and Rausch, 2017).
Trajectories over the SEA are variable. Depending upon the winds in the FT,
the trajectory may remain relatively static or may (as in the case shown
here) be advected as far south as 30<inline-formula><mml:math id="M170" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and back toward the
African continent by the incursion of midlatitude disturbances that lead to
westerly lower tropospheric winds extending into tropical latitudes.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f21.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Discussion</title>
      <p id="d1e4197">As with any significant suborbital field deployment, we expect substantial
data analysis efforts to extend well beyond the nominal project end date. In
this section, we describe ongoing analyses not previously mentioned. Future
work that may be facilitated by ORACLES data is captured in Sect. 7.</p>
      <p id="d1e4200">Science objective 1 on direct aerosol radiative effects (DAREs) is being
pursued with a number of different approaches. At the finest spatiotemporal scale, these approaches entail instantaneous assessments of DAREs on the
basis of very complete measurements of aerosol and cloud radiative
properties from designated flight maneuvers on a particular flight day. On
the larger scales, these approaches combine geostationary satellite
observations of diurnally varying cloud properties and above-cloud AOD, both
adjusted for aerosol radiative properties measured in situ and possibly
nudged by chemical transport model outputs, with campaign-average models of
aerosol intensive properties. A designated group of ORACLES scientists meets
routinely to discuss the results of the DARE assessment efforts and to avoid
duplication of research efforts. Participation in these teleconferences can be
requested through email to the corresponding authors of this paper.</p>
      <p id="d1e4203">Current work on science objective 2, the semi-direct aerosol effect, focuses
on understanding how the vertical structure in the SSA depicted in Fig. 14
relates to aerosol aging versus source composition (fuel type and
flaming/smoldering conditions) and how the aging relates to aerosol
transport patterns. Such work is primarily aimed at developing an
understanding of the processes affecting the aerosol SSA and is
crosscutting across the different campaigns. Other work is examining how
clouds adapt to variations in the absorbing aerosol vertical structure. The
discrimination between cloud adaptations to the aerosol shortwave
absorption, cloud-nucleating properties, and variability in the large-scale
circulation is inherently complex. While this work will assuredly require
focused modeling activities that can control more easily for cause–effect
relationships, ongoing analysis of ORACLES datasets will frame<?pagebreak page1537?> the modeling
activities. In one example, the multiple routine flights along 5<inline-formula><mml:math id="M171" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, conducted in both August 2017 and October 2018, are being analyzed to
determine the dominant thermodynamic, dynamic, and aerosol features. In
another example, remote-sensing data from the ER-2 platform in September 2016 on the aerosol vertical structure and cloud properties are being
constrained by sea surface temperature and location to assess liquid water
path responses to aerosol loading and vertical structure.</p>
      <p id="d1e4215">Science objective 3 focuses on effects of smoke CCN on the microphysical
properties of clouds and precipitation. Concentrations of CCN in the PBL are
much lower than those in the FT smoke plume because (a) subsidence and
entrainment of smoke into the PBL is relatively slow and (b) there are
significant losses in the PBL from both dry and wet deposition. Work is
currently underway to understand the transport pathways from the FT into the
PBL using a combination of measurements of water vapor, tracers such as
carbon monoxide (CO), and the isotopic composition of both water vapor and
liquid water to understand the smoke contribution to the PBL CCN budget.
Cloud droplet concentration closure is being used to quantify the efficacy
with which smoke aerosols serve as nuclei for cloud droplet activation.
Remote-sensing and in situ measurements are being used to understand both how
smoke suppresses precipitation and the extent to which precipitation is
a removal process for CCN. The airborne polarimeter and in situ observations
are being used to provide constraints to correct satellite estimates of
cloud droplet concentrations that may be affected by overlying smoke.
Analyses to assess the Lagrangian evolution of clouds will help quantify how
entrainment of smoke aerosol can impact Nd and change liquid water path and
cloudiness. One such Lagrangian case, observed by both the P-3 and the UK
BAe-146 aircraft over several days, involved a major smoke entrainment
event and is currently being used to constrain large eddy simulations to
evaluate both semi-direct and indirect aerosol effects.</p>
      <p id="d1e4219">All of the ongoing analyses on the overarching science objectives depend
critically on the comparisons of observations and models described in Sect. 5.3.6. This dependence is manifested in two separate ways. The first, and
more obvious way, is that the models are being evaluated for their ability
to fill in missing pieces of information required for the assessment of
direct, semi-direct, or indirect aerosol radiative effects in the SE
Atlantic. If models are shown to provide reasonable predictions of relevant
parts of the aerosol–cloud system, the predictions of these parts can be
used to extrapolate aerosol and cloud properties beyond the available
spatial and temporal domains. The second, and slightly less obvious way, is
that the models can be used to study the representativeness of the airborne
and even some of the satellite observations. In the case of the airborne
measurements, for example, the comparison of a model output averaged over
all time steps coincident with the measurements to the model averaged over
all times in a given month may provide an assessment of how representative
the relatively sparse airborne observations are for a monthly mean. If the
two averages vary significantly, then we may conclude that the airborne
observations should not be used directly but instead should be adjusted by
the model results, for the purpose of calculating monthly mean aerosol
effects. Relatedly, the in situ-measured aerosol properties should only be
used to evaluate model results if both the monthly average model output and
the output subsampled to the airborne observations show the same discrepancy
to the model, as such a consistent discrepancy is attributable to a model
deficiency rather than a sampling error.</p>
      <p id="d1e4222">Radiative closure studies will be equally important for progress on the
overarching science questions. In a broad sense, these closure studies
relate the aerosol and cloud properties measured in situ on the P-3 to
remotely measured radiances or irradiances, either from the ER-2 (in 2016),
from satellites, or from radiation measurements on the P-3 itself. They may
be as ambitious as exploring the connection between the measured aerosol
chemical composition, aerosol and cloud radiative properties, and the
radiation field or as simply comparing the aerosol radiative properties
measured in situ to those measured from remote-sensing instruments. Either
way, the knowledge gained from these closure studies will be crucial for
assessing large-scale aerosol–cloud–radiation interactions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F22" specific-use="star"><?xmltex \currentcnt{22}?><?xmltex \def\figurename{Figure}?><label>Figure 22</label><caption><p id="d1e4227">Longitudinal cross section of the HSRL-2 scattering ratio curtain
collected during the ER-2 transit from Recife, Brazil, to Walvis Bay,
Namibia, on 26 August 2016.</p></caption>
        <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f22.png"/>

      </fig>

</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions and future work</title>
      <p id="d1e4244">The ORACLES project is a highly successful NASA EVS-2 project that had well
surpassed its Level-1 baseline science requirements upon the conclusion of
its last field deployment in October 2018. We conducted a total of three
flight deployments totaling 350.6 science flight hours with the NASA P-3
aircraft and one flight deployment with the NASA ER-2 totaling 97.3 science
flight hours, surveying, probing, and exploring the various features of the
SE Atlantic aerosol–cloud–climate system. The ORACLES dataset permits the
study of aerosol radiative and cloud-nucleating properties, their vertical
distribution relative to clouds, the locations and degree of aerosol mixing
into clouds, and cloud changes in response to such mixing. Here, we have
only touched upon some of the key findings, leaving the detailed exploration
of the various factors determining aerosol–cloud–climate interactions in the
SE Atlantic to the individual investigations being conducted as part of, or
spawned by, the ORACLES project. A high-level summary of some of the main
scientific findings and conclusions from our project includes the following:
<list list-type="bullet"><list-item>
      <p id="d1e4249">the marine boundary layer of the SE Atlantic is more frequently affected by
BB aerosol than previously thought, with the variety of pathways by which BB
aerosol reach the BL complex not yet fully explored (Zuidema et al., 2018);
the transport and climate models<?pagebreak page1538?> used in ORACLES flight planning had limited
success in forecasting the locations and levels of MBL aerosol pollution;</p></list-item><list-item>
      <p id="d1e4253">BB aerosol layers appear to be in much more frequent contact with the Sc
cloud deck underneath than previously estimated, but the correlation of
cloud droplet number concentrations with above-cloud smoke properties is weak
(Diamond et al., 2018); in situ data from August 2017 suggest that cloud
droplet number and above-cloud aerosol can be anticorrelated, owing to the
anticorrelation of MBL aerosol with above-cloud aerosol amount (Kacarab et
al., 2020);</p></list-item><list-item>
      <p id="d1e4257">cloud vertical velocity tends to correlate positively with MBL aerosol
number; this covariance tends to enhance cloud droplet number considerably
beyond what is expected from aerosol changes alone (Kacarab et al., 2020);
most of the observed droplet variability in clouds in polluted boundary
layers during the August 2017 deployment appears driven by vertical
velocity and its variability (Kacarab et al., 2020);</p></list-item><list-item>
      <p id="d1e4261">interannual variations in the seasonal evolution of aerosol loading in the
FT and cloud droplet number concentrations in the MBL over the SE Atlantic
during the BB season are greater than previously appreciated (see Sect. 4.2 and 4.3); they are affected by interannual variations in BB location and
strength and possibly by variations in the SAEJ (see Sect. 4.1);</p></list-item><list-item>
      <p id="d1e4265">direct airborne measurements of the above-cloud AOD have shown a slight
overestimation by current remote-sensing techniques from spaceborne
instruments (MOD06ACAERO, Deep Blue MODIS, and VIIRS) and some potential
difficulties in cloud masking (LeBlanc et al., 2020; Sayer et al., 2019)
but a generally consistent meridionally distribution between the airborne
and orbital observations;</p></list-item><list-item>
      <p id="d1e4269">aerosol radiative properties, such as the single-scattering albedo and
asymmetry parameter, especially in column-integrated values, show
reproducible spectral dependence and a fairly-well-constrained range of
absolute values in each deployment year (Pistone et al., 2019; Cochrane et
al., 2020); their vertical dependence appears to be reproducible as well
(see Sect. 5.2.6); overall these highlight that the aerosol is more
absorbing than previously thought;</p></list-item><list-item>
      <p id="d1e4273">aerosol radiative properties can correlate well to the relative proportion
of BC and organics during plume aging (see Sect. 5.2.2 and 5.2.3), a
process not previously investigated by suborbital means as it requires the
sampling of smoke well beyond the near-field fire environment – this
sampling of smoke properties up to 2 weeks after emission is a unique
accomplishment of ORACLES;</p></list-item><list-item>
      <p id="d1e4277">despite the large aerosol loadings, water vapor also contributes
significantly to the total heating rate at most altitudes (Mallet et al.,
2019; Cochrane et al., 2020), if less to the range in total heating rates;</p></list-item><list-item>
      <p id="d1e4281">there was ample evidence for aerosol-induced modifications of Sc cloud
properties (Fig. 18) and those of mid-level clouds (Adebiyi et al., 2020);</p></list-item><list-item>
      <?pagebreak page1539?><p id="d1e4285">a new cloud/rain dataset produced by a joint multi-wavelength cloud radar
and multi-angle/multi-wavelength polarimeter will allow for further
investigation for the suppression of drizzle by aerosol (Dzambo et al., 2019,
2020);</p></list-item><list-item>
      <p id="d1e4289">chemical transport models and climate models exhibit a fairly systematic
underestimation of aerosol loadings in the SE Atlantic (Shinozuka et al.,
2020).</p></list-item></list>
An analogous summary of lessons learned for logistics and planning of large
field campaigns to address aerosol–cloud–climate interactions includes the
following:
<list list-type="bullet"><list-item>
      <p id="d1e4295">the ORACLES science objectives and questions provided crucial guidance for
flight execution in each of the deployment years;</p></list-item><list-item>
      <p id="d1e4299">progress towards achieving science objectives was facilitated by the
bookkeeping of flight maneuvers that relate directly to the various
detailed science objectives, although such bookkeeping proved challenging
in the field;</p></list-item><list-item>
      <p id="d1e4303">the joint efforts in developing flight plans by scientists with nominally
different flight objectives (e.g., cloud microphysics and radiation)
revealed that relatively minor adjustments to flight maneuvers often
resulted in datasets that are conducive to addressing a broad range of
science questions, well beyond the benefits of flight plans that were
developed by any one focused group in isolation;</p></list-item><list-item>
      <p id="d1e4307">the scientific connection to international deployment efforts conducted by
the CLARIFY and AEROCLO-sA teams in the same region and timeframe as
ORACLES-2017 proved a worthy investment of time – while the connecting
science is ongoing, there are already measurable outcomes from the
international scientific collaborations in terms of the geographic extension
of datasets and related publications (e.g., Mallet et al., 2019; Formenti
et al., 2019; Haywood et al., 2020);</p></list-item><list-item>
      <p id="d1e4311">the routine sampling strategy for about half of the ORACLES flights allowed
for a statistical assessment of climate and chemical transport models,
unprecedented for suborbital efforts in this field of study;</p></list-item><list-item>
      <p id="d1e4315">the involvement of the modeling community in the conception and development
of the ORACLES project in general, and its flight planning specifically,
proved to be invaluable for collecting a dataset that can be used for
addressing model deficiencies that hamper our ability to accurately simulate
aerosol–cloud–climate interactions.</p></list-item></list>
Future work will likely need to focus on aspects of the science that remain
poorly understood and/or physics that is well understood but not well
represented in models. Such topics will likely include long-term changes in
biomass burning activity, convection and FT transport in the BB source
region, the location and degree of mixing of BB aerosols into the SE
Atlantic MBL, and the separation of synoptic-scale variations in the
meteorological environment from aerosol-induced changes in Sc cloud
properties, to name a few.</p>
      <p id="d1e4319">We conclude this paper with a figure that represents the complexity of the
SE Atlantic aerosol–cloud system well. Figure 22 shows the longitudinal
transect of the HSRL-2 scattering ratio curtain collected during the ER-2
transit from Recife, Brazil, to Walvis Bay, Namibia, on 26 August 2016. In
addition to expected features, such as an increasing MBL height with
increasing distance from southern Africa, and the general dilution of the BB
plume with distance from shore, the high signal-to-noise ratio in the HSRL-2 data
also reveals a complexity of the layering structure within the BB plume that
was previously not appreciated. The layering includes horizontal and
vertical gradients in loading, and likely in microphysics, with small-scale
features that bear explanation. Future studies of the SE Atlantic climate
system are well advised to embrace this complexity.</p><?xmltex \hack{\clearpage}?>
</sec>

      
      </body>
    <back><app-group>

<?pagebreak page1540?><app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title>Description of flights</title>
      <p id="d1e4334">Tables A1a and A1b summarize the P-3 and ER-2 flights in 2016, respectively,
while Tables A2 and A3 summarize the P-3 flights in 2017 and 2018,
respectively. The entries for each flight are comprised of the flight date
and identifiers (format xRFnnYyy, where x is the platform indicator – P for
the P-3 or E for the ER-2; RF is static and stands for research flight; yy
is the flight number for this platform and year; Y is static and stands for
year, nn is the numerical year – 16, 17, or 18) in the first column. Column 2
indicates the total flight time. Column 3 contains a brief flight synopsis
and numbers that indicate the number of specific flight maneuvers indicated
in each flight.</p>

<?xmltex \floatpos{p}?><table-wrap id="App1.Ch1.S1.T4" specific-use="star"><?xmltex \currentcnt{A1}?><?xmltex \def\figurename{Table}?><label>Table A1</label><caption><p id="d1e4340"><bold>(a)</bold> The 2016 flight summary for the P-3 aircraft. The number of each type
of flight maneuver (as given in the table header) is shown in parentheses
for each flight. Flight synopsis indicates whether the flight was a
designated routine or target-of-opportunity flight. <bold>(b)</bold> The 2016 flight summary for the ER-2 aircraft.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="1.5cm"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="14cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3" align="left"><bold>(a)</bold></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Date <?xmltex \hack{\hfill\break}?>P-3 flight no.</oasis:entry>
         <oasis:entry colname="col2">h</oasis:entry>
         <oasis:entry colname="col3">Flight synopsis <?xmltex \hack{\hfill\break}?>(ramps, RA; square spirals, SS; MBL legs, ML; in-cloud legs, ICL; above-cloud legs, ACL; sawtooth legs, STL; in-plume legs, IPL; above-plume legs, APL)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/27 <?xmltex \hack{\hfill\break}?>PRF00Y16</oasis:entry>
         <oasis:entry colname="col2">6.8</oasis:entry>
         <oasis:entry colname="col3">Transit: Ascension Island to Walvis Bay <?xmltex \hack{\hfill\break}?>(RA 2/SS 0/ML 1/ICL 0/ACL 0/STL 0/IPL 0/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/30 <?xmltex \hack{\hfill\break}?>PRF01Y16</oasis:entry>
         <oasis:entry colname="col2">1.6</oasis:entry>
         <oasis:entry colname="col3">Routine (aborted): upon takeoff, P-3 climbed through overcast stratocumulus; aircraft hydraulic issue was identified during takeoff and the mission aborted. Some useful science measurements just offshore within the BB plume at approximately 3500 m alt. <?xmltex \hack{\hfill\break}?>(RA 1/SS 0/ML 0/ICL 0/ACL 0/STL 0/IPL 2/APL 0)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/31 <?xmltex \hack{\hfill\break}?>PRF02Y16</oasis:entry>
         <oasis:entry colname="col2">8.1</oasis:entry>
         <oasis:entry colname="col3">Routine: the goal was to provide routine mapping along the NW–SE routine flight track from 23<inline-formula><mml:math id="M172" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/13<inline-formula><mml:math id="M173" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E to as far NW as possible given flight time constraints; clouds were present along the entire routine track on the outbound leg, but by the return the clouds had a clear southern edge around 22<inline-formula><mml:math id="M174" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S; typically, an aerosol-free gap was present between the elevated BB layer and the cloud, corroborated by low RH values associated with clean air just above cloud top. <?xmltex \hack{\hfill\break}?>(RA 7/SS 2/ML 4/ICL 3/ACL 4/STL 1/IPL 9/APL 3)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/02 <?xmltex \hack{\hfill\break}?>PRF03Y16</oasis:entry>
         <oasis:entry colname="col2">8.1</oasis:entry>
         <oasis:entry colname="col3">Target: the objective was to sample aerosol radiative effects above clouds at 20<inline-formula><mml:math id="M175" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/10<inline-formula><mml:math id="M176" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, where the aerosol plume concentration and low-cloud fraction are increasing towards the north, and capture a case with 100 % cloud fraction (CF). Significant in situ aerosol and cloud sampling, connection to remote sensing through Terra overpass. Required no cirrus or mid-level clouds, high AOD, and solid Sc deck (all met). Performed two radiation walls near 16S because cloud conditions were optimal. <?xmltex \hack{\hfill\break}?>(RA 9/SS 2/ML 2/ICL 2/ACL 7/STL 0/IPL 7/APL 3)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/04 <?xmltex \hack{\hfill\break}?>PRF04Y16</oasis:entry>
         <oasis:entry colname="col2">8.0</oasis:entry>
         <oasis:entry colname="col3">Routine: the objective was to reach 10<inline-formula><mml:math id="M177" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/0<inline-formula><mml:math id="M178" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E along routine track with two profiles outgoing and returning, offset from each other. Reached 10<inline-formula><mml:math id="M179" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S with two boundary layer profiles along the way. Second BL profile at 13<inline-formula><mml:math id="M180" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S sampled a decoupled boundary layer reaching 1.5 km altitude with high organic/BC mass. The transit back sampled a thick mid-level cloud lying above the smoke layer, with similar aerosol/black carbon concentrations. <?xmltex \hack{\hfill\break}?>(RA 4/SS 0/ML 2/ICL 2/ACL 2/STL 0/IPL 8/APL 8)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/06 <?xmltex \hack{\hfill\break}?>PRF05Y16</oasis:entry>
         <oasis:entry colname="col2">8.0</oasis:entry>
         <oasis:entry colname="col3">Target: the goal was to sample clouds and aerosols along a N–S line in what <?xmltex \hack{\hfill\break}?>was anticipated to be three different aerosol conditions (aged aerosols on southern end, break in aerosols in the middle of the track, and fresher aerosols towards the northern end of the track). Several in- and above-cloud legs provided some evidence of forecast conditions. Drizzle evident in APR-3 data. <?xmltex \hack{\hfill\break}?>(RA 9/SS 0/ML 6/ICL 4/ACL 6/STL 4/IPL 4/APL 4)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/08 <?xmltex \hack{\hfill\break}?>PRF06Y16</oasis:entry>
         <oasis:entry colname="col2">8.1</oasis:entry>
         <oasis:entry colname="col3">Routine: the plan was to reach 10<inline-formula><mml:math id="M181" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S along routine track with a single profile out midway, and then on return at least two profiles were planned, followed by stepped ascents. The main objective was to quantify discrepancy in amount and vertical location of aerosol plumes between WRF and GEOS. Succeeded in doing three profiles. The aerosol layers were more complicated than modeled; clear slot between aerosol layers, with different aerosol composition in different layers. Some cloud work but mostly over scattered and few cloud areas. <?xmltex \hack{\hfill\break}?>(RA 9/SS 0/ML 3/ICL 1/ACL 4/STL 1/IPL 4/APL 6)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/10 <?xmltex \hack{\hfill\break}?>PRF07Y16</oasis:entry>
         <oasis:entry colname="col2">8.1</oasis:entry>
         <oasis:entry colname="col3">Routine: the goal was a routine flight to 10<inline-formula><mml:math id="M182" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/0<inline-formula><mml:math id="M183" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, with planned profiling legs (below, within, above cloud, sawtooths through cloud and profiling tropospheric aerosols). Coordination with the ER-2 on the inbound leg. Some predicted Sc clouds did not materialize and some planned cloud work needed to be aborted. Aerosol conditions were cleaner than predicted. Coordination between aircraft at 11:30 UTC, with P-3 in cloud at exact ER-2 overpass time. <?xmltex \hack{\hfill\break}?>(RA 6/SS 2/ML 4/ICL 4/ACL 4/STL 1/IPL 6/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">09/12 <?xmltex \hack{\hfill\break}?>PRF08Y16</oasis:entry>
         <oasis:entry colname="col2">8.4</oasis:entry>
         <oasis:entry colname="col3">Routine: the plan was to transit to north and west at high altitude and then to conduct profiling on the return as time permitted. Loose coordination with the ER-2 on the inbound leg was envisioned. Almost reached 10<inline-formula><mml:math id="M184" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/0<inline-formula><mml:math id="M185" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and performed cloud work after descent. ER-2 coordination attempted at 18<inline-formula><mml:math id="M186" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/8<inline-formula><mml:math id="M187" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. In general, boundary layer profiles were quite clean, and clouds and precipitation were observed to reach the ground (APR-3 and in situ) towards the northern end of the track. The biomass burning plume was not being entrained into the Sc clouds. <?xmltex \hack{\hfill\break}?>(RA 6/SS 0/ML 3/ICL 2/ACL 2/STL 1/IPL 2/APL 6)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{p}?><table-wrap id="App1.Ch1.S1.T5" specific-use="star"><?xmltex \currentcnt{A1}?><?xmltex \def\figurename{Table}?><label>Table A1</label><caption><p id="d1e4682">Continued.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="1.5cm"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="14cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3" align="left"><bold>(a)</bold></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Date <?xmltex \hack{\hfill\break}?>P-3 flight no.</oasis:entry>
         <oasis:entry colname="col2">h</oasis:entry>
         <oasis:entry colname="col3">Flight synopsis <?xmltex \hack{\hfill\break}?>(ramps, RA; square spirals, SS; MBL legs, ML; in-cloud legs, ICL; above-cloud legs, ACL; sawtooth legs, STL; in-plume legs, IPL; above-plume legs, APL)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/14 <?xmltex \hack{\hfill\break}?>PRF09Y16</oasis:entry>
         <oasis:entry colname="col2">8.1</oasis:entry>
         <oasis:entry colname="col3">Target: radiation focus – radiation walls at two points with contrasting cloud/aerosol conditions; achieved multiple overflights by ER-2 during two radiation wall segments on N–S legs near 16–17<inline-formula><mml:math id="M188" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, but with moderate AOD (0.4). Clouds were generally quite homogeneous and similar between radiation wall locations. Ultra-clean layers just above cloud top. Full square radiation spirals on leg A – preliminary results indicating significant albedo differences within the spiral itself. <?xmltex \hack{\hfill\break}?>(RA 11/SS 1/ML 4/ICL 5/ACL 7/STL 0/IPL 5/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/18 <?xmltex \hack{\hfill\break}?>PRF10Y16</oasis:entry>
         <oasis:entry colname="col2">8.2</oasis:entry>
         <oasis:entry colname="col3">Target: the goal was to study young, dense plumes. Increased likelihood of cirrus in study region near 12–14<inline-formula><mml:math id="M189" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/11<inline-formula><mml:math id="M190" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. Predicted plume at about 4 km, only a few days old, was substantiated; lower parts of the plume were predicted to be older. Flew one extensive radiation wall, with three in-plume legs, two legs just above cloud, an extended cloud leg, an MBL leg, and one deep profile. Three ER-2 overpasses captured. Mostly polluted but not decoupled MBL. <?xmltex \hack{\hfill\break}?>(RA 3/SS 1/ML 2/ICL 2/ACL 2/STL 0/IPL 5/APL 4)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/20 <?xmltex \hack{\hfill\break}?>PRF11Y16</oasis:entry>
         <oasis:entry colname="col2">8.4</oasis:entry>
         <oasis:entry colname="col3">Target: radiation flight – the objective was to sample aerosol radiative effect and aerosol and cloud properties for two different types of cloud fields (in terms of albedo and/or cloud fraction) in coordination with the ER-2. Very successful flight – two almost complete radiation/microphysics walls at 10.5 and 9<inline-formula><mml:math id="M191" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E; mid-level clouds on 9E leg; BB plume reached highest altitudes so far (21 kft/6.4 km) and largest AOD (<inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.8</mml:mn></mml:mrow></mml:math></inline-formula>); apparently fresh aerosol, absorption Ångström exponent higher than on other flights; plume more stratified than on other days; patches of drizzle found in radar and cloud probes. <?xmltex \hack{\hfill\break}?>(RA 6/SS 4/ML 4/ICL 3/ACL 5/STL 1/IPL 2/APL 4)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/24 <?xmltex \hack{\hfill\break}?>PRF12Y16</oasis:entry>
         <oasis:entry colname="col2">9.2</oasis:entry>
         <oasis:entry colname="col3">Target: the objective was another attempt to find the youngest, densest plume. Went farther north than any other flight, found very polluted layers at altitude. HSRL-2 data exceedingly useful for finding layers. Penetrated a couple of intermediate level clouds, able to get droplet size distributions. Confirmed the high altitude of smoke plume, as predicted by WRF; GEOS-5 showed low-altitude plumes that were not there – excellent model testing! One ER-2 overpass. Spent about 30 min in clouds of various sorts. AOD up to 0.9. <?xmltex \hack{\hfill\break}?>(RA 5/SS 3/ML 4/ICL 3/ACL 3/STL 0/IPL 5/APL 5)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/25 <?xmltex \hack{\hfill\break}?>PRF13Y16</oasis:entry>
         <oasis:entry colname="col2">8.8</oasis:entry>
         <oasis:entry colname="col3">Routine: the objective was to extend routine flight to 9 h and to coordinate with ER-2 at 10<inline-formula><mml:math id="M193" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/0<inline-formula><mml:math id="M194" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. Sampled BB layer at 14 and 18 kft (4.3 and 5.5 km) on outbound leg; profiles on outbound legs flown as planned, with extended low-level legs. AOD 0.3–0.4, with the exception of 0.6 near turnaround point. Coordination with ER-2 at 13:45 UTC, with P-3 in cloud (after a below-cloud leg and before above-cloud legs). Very clean layer above cloud top near 20<inline-formula><mml:math id="M195" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S on return leg. <?xmltex \hack{\hfill\break}?>(RA 7/SS 0/ML 2/ICL 2/ACL 5/STL 1/IPL 8/APL 5)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/27 <?xmltex \hack{\hfill\break}?>PRF14Y16</oasis:entry>
         <oasis:entry colname="col2">7.3</oasis:entry>
         <oasis:entry colname="col3">Transit: Walvis Bay to Ascension Island; mostly high-altitude flight, with some in situ MBL observations and combined radar–in situ observations of precipitating clouds near Ascension Island starting at 11<inline-formula><mml:math id="M196" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/10<inline-formula><mml:math id="M197" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W. <?xmltex \hack{\hfill\break}?>(RA 1/SS 3/ML 1/ICL 0/ACL 2/STL 0/IPL 1/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">15</oasis:entry>
         <oasis:entry namest="col2" nameend="col3" align="center">115.2 </oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{p}?><table-wrap id="App1.Ch1.S1.T6" specific-use="star"><?xmltex \currentcnt{A1}?><?xmltex \def\figurename{Table}?><label>Table A1</label><caption><p id="d1e4926">Continued.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="1.5cm"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="14cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3" align="left"><bold>(b)</bold></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Date <?xmltex \hack{\hfill\break}?>ER-2 flight no.</oasis:entry>
         <oasis:entry colname="col2">h</oasis:entry>
         <oasis:entry colname="col3">Flight synopsis <?xmltex \hack{\hfill\break}?>(ramps, RA; square spirals, SS; MBL legs, ML; in-cloud legs, ICL; above-cloud legs, ACL; sawtooth legs, STL; in-plume legs, IPL; above-plume legs, APL)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/26 <?xmltex \hack{\hfill\break}?>ERF00Y16</oasis:entry>
         <oasis:entry colname="col2">7.9</oasis:entry>
         <oasis:entry colname="col3">Transit: from Recife directly to Walvis Bay, very extensive longitudinal cross section with HSRL; RSP without SWIR, eMAS collected no data as plate installed over aperture; RSP, SSFR, AirMSPI, and HSRL-2 worked well.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col3" align="center">08/27–09/09: waiting for ER-2 fuel to arrive </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/10 <?xmltex \hack{\hfill\break}?>ERF01Y16<inline-formula><mml:math id="M199" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">6.3</oasis:entry>
         <oasis:entry colname="col3">Mapping routine – planned 9 h flight to survey smoke transport; high-level clouds in target area prevented original plan to work with P-3; RSP, AirMSPI, eMAS, and SSFR worked well; HSRL-2 did not operate due to tripped ER-2 circuit breaker/faulty ER-2 coolant pump; flight shortened to attempt coordination with P-3 and allow problem troubleshooting; RSP, AirMSPI, and eMAS (including SWIR) data for cloud retrievals.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/12 <?xmltex \hack{\hfill\break}?>ERF02Y16<inline-formula><mml:math id="M200" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">8.7</oasis:entry>
         <oasis:entry colname="col3">Routine: planned 9 h flight to survey smoke transport (“big triangle”); mid-level clouds in target area prevented original plan to work with P-3; HSRL-2, RSP, AirMSPI, eMAS, and SSFR worked well.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/14 <?xmltex \hack{\hfill\break}?>ERF03Y16<inline-formula><mml:math id="M201" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">8.1</oasis:entry>
         <oasis:entry colname="col3">Target: planned 8 h flight with P-3 coordination along two N–S legs; RSP, AirMSPI, and SSFR worked well; eMAS-VIS/NIR/SWIR worked well – LWIR compromised due to Sterling cooler's active balancer failing during flight. HSRL-2 did not operate due to tripped aircraft circuit breaker. Troubleshooting found faulty aircraft coolant pump which was subsequently replaced; very good Terra overpass; good flight for polarimeter cloud retrievals and intercomparison with P-3 RSP and in situ.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/16 <?xmltex \hack{\hfill\break}?>ERF04Y16</oasis:entry>
         <oasis:entry colname="col2">7.7</oasis:entry>
         <oasis:entry colname="col3">Routine: mapping/survey flight “little triangle”; HSRL-2 operational again after ER-2 coolant pump replaced; HSRL-2, RSP, AirMSPI, and SSFR worked well; eMAS – good data in Vis-SWIR, no LWIR data available.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/18 <?xmltex \hack{\hfill\break}?>ERF05Y16<inline-formula><mml:math id="M202" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">8.5</oasis:entry>
         <oasis:entry colname="col3">Target: mapping plume and CALIPSO underflight; S–N leg near the coast (along 11<inline-formula><mml:math id="M203" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) to look at smoke properties close to coast. Northern part of S–N leg (between 10–12<inline-formula><mml:math id="M204" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 11.5<inline-formula><mml:math id="M205" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E) included a portion that was coordinated with the P-3. Western part of plan included CALIPSO leg (overpass <inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">13</mml:mn></mml:mrow></mml:math></inline-formula>:35 UT); HSRL, RSP, AirMSPI, SSFR, and eMAS worked well.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/20 <?xmltex \hack{\hfill\break}?>ERF06Y16<inline-formula><mml:math id="M207" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">7.7</oasis:entry>
         <oasis:entry colname="col3">Target: P-3 coordination, CALIPSO underflight; coordinated S–N legs with P-3 along 10.5<inline-formula><mml:math id="M208" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and 9<inline-formula><mml:math id="M209" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E between 14–18<inline-formula><mml:math id="M210" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Western part of plan included CALIPSO leg; HSRL, RSP, AirMSPI, SSFR, and eMAS worked well (eMAS – no 13.9 <inline-formula><mml:math id="M211" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> band data)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/22 <?xmltex \hack{\hfill\break}?>ERF07Y16</oasis:entry>
         <oasis:entry colname="col2">7.9</oasis:entry>
         <oasis:entry colname="col3">Routine and mapping: southern survey, St. Helena overflight; RSP, AirMSPI, SSFR, and HSRL-2 worked well; eMAS–not operational (data system failure); southern mapping triangle; flyover of St. Helena – clouds prevented AERONET aerosol measurements; ER-2 overflight nearly coincident with St. Helena radiosonde launch.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/24 <?xmltex \hack{\hfill\break}?>ERF08Y16<inline-formula><mml:math id="M212" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">8.0</oasis:entry>
         <oasis:entry colname="col3">Target: RSP, AirMSPI, SSFR, and HSRL-2 worked well; eMAS – good data in Vis-SWIR. No LWIR data (bands 26–38) – aircraft pod heater failure toward end of flight. ER-2 leg along 11<inline-formula><mml:math id="M213" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E between 8–20<inline-formula><mml:math id="M214" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S along P-3 leg; ER-2 legs between 8–12<inline-formula><mml:math id="M215" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S can be used to study smoke evolution between 11 and 3<inline-formula><mml:math id="M216" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/25 <?xmltex \hack{\hfill\break}?>ERF09Y16<inline-formula><mml:math id="M217" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">8.7</oasis:entry>
         <oasis:entry colname="col3">Routine: RSP, AirMSPI, and SSFR worked well; HSRL-2 no science data due to laser problem; eMAS – good data in Vis-SWIR, no LWIR data (bands 26–38); aircraft pod heater failed. Flew “big triangle” and met P-3 on return leg.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/27 <?xmltex \hack{\hfill\break}?>ERF10Y16<inline-formula><mml:math id="M218" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">9.2</oasis:entry>
         <oasis:entry colname="col3">Routine: RSP, AirMSPI, and SSFR worked well; HSRL-2 did not collect science data due to laser problem; eMAS – good data in Vis-SWIR. No LWIR data (bands 26–38) – aircraft pod heater failed. Short (10–15 min leg) on return leg for Aqua overpass for eMAS. Flew “big triangle” again.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/29 <?xmltex \hack{\hfill\break}?>ERF11Y16</oasis:entry>
         <oasis:entry colname="col2">8.6</oasis:entry>
         <oasis:entry colname="col3">Transit: Walvis Bay to Recife; initial leg NW over standard leg to 0<inline-formula><mml:math id="M219" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N/10<inline-formula><mml:math id="M220" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, then over Ascension Island, before continuing to Recife. eMAS collected no data as plate installed over aperture; HSRL-2 did not collect science data due to laser problem. RSP, SSFR, and AirMSPI worked well.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">12</oasis:entry>
         <oasis:entry namest="col2" nameend="col3" align="center">97.3 </oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d1e4929"><inline-formula><mml:math id="M198" display="inline"><mml:msup><mml:mi/><mml:mo>∗</mml:mo></mml:msup></mml:math></inline-formula> ER-2 flights that were closely coordinated with P-3 aircraft
operations.</p></table-wrap-foot></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{p}?><table-wrap id="App1.Ch1.S1.T7" specific-use="star"><?xmltex \currentcnt{A2}?><?xmltex \def\figurename{Table}?><label>Table A2</label><caption><p id="d1e5361">The 2017 flight summary for the P-3 aircraft.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="2cm"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="14cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Date <?xmltex \hack{\hfill\break}?>P-3 flight no.</oasis:entry>
         <oasis:entry colname="col2">h</oasis:entry>
         <oasis:entry colname="col3">Flight synopsis <?xmltex \hack{\hfill\break}?>(ramps, RA; square spirals, SS; MBL legs, ML; in-cloud legs, ICL; above-cloud legs, ACL; sawtooth legs, STL; in-plume legs, IPL; above-plume legs, APL)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/09 <?xmltex \hack{\hfill\break}?>PRF00Y17</oasis:entry>
         <oasis:entry colname="col2">7.8</oasis:entry>
         <oasis:entry colname="col3">Transit: to São Tomé with science en route. Three square spirals, with backtracking at low altitudes. Two of the three with sawtooth cloud sampling, one in clear air with largest aerosol loading of flight. Most instruments worked well, highest AOD of 0.6, above-cloud AOD about 0.46. Polluted MBL both below clouds and in cloud-free columns. No aerosol above clouds at Ascension Island. Interesting overall gradients. <?xmltex \hack{\hfill\break}?>(RA 7/SS 0/ML 3/ ICL 0/ACL 2/STL 2/IPL 8/APL 0)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/12 <?xmltex \hack{\hfill\break}?>PRF01Y17</oasis:entry>
         <oasis:entry colname="col2">8.5</oasis:entry>
         <oasis:entry colname="col3">Routine: the plan was to reach 13<inline-formula><mml:math id="M221" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Multiple layers near São Tomé; highest ACAOD of flight at <inline-formula><mml:math id="M222" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.45</mml:mn></mml:mrow></mml:math></inline-formula>. During southbound transit, aerosol layer resting on cloud top and then decreasing cloud tops with separation from aerosol at about 2<inline-formula><mml:math id="M223" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. At <inline-formula><mml:math id="M224" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M225" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S – “soft” cloud break and then solid deck of small closed cell clouds topped by aerosol layer right on cloud tops. Two sets of spiral descents, cloud sawtooth patterns, sets of backtracking level legs for additional cloud sampling. <?xmltex \hack{\hfill\break}?>(RA 3/SS 3/ML 3/ICL 1/ACL 2/STL 2/IPL 5/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/13 <?xmltex \hack{\hfill\break}?>PRF02Y17</oasis:entry>
         <oasis:entry colname="col2">9.1</oasis:entry>
         <oasis:entry colname="col3">Target: the objective was a joint cloud–radiation flight, sampling gradient of overcast and broken clouds along the CALIPSO satellite track, aerosol radiative effects in the presence of broken clouds, and mixing of aerosols into clouds. Transition between overcast and broken clouds was found along the 7–9<inline-formula><mml:math id="M226" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S line oriented along A-train track. Line was oriented nearly parallel with surface winds. This allowed both the radiation and microphysics objectives to be addressed. Transition between homogeneous and broken clouds, and some gradient in the mixing mechanism into cloud and the boundary layer. Final part involved sampling at 20 kft (6.1 km) during A-train overpass to get HSRL-2/RSP curtain/comparison. <?xmltex \hack{\hfill\break}?>(RA 4/SS 2/ML 3/ICL 2/ACL 3/STL 1/IPL 2/APL 3)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/15 <?xmltex \hack{\hfill\break}?>PRF03Y17</oasis:entry>
         <oasis:entry colname="col2">9.2</oasis:entry>
         <oasis:entry colname="col3">Routine: flight to 15<inline-formula><mml:math id="M227" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, with main objective to sample Lagrangian start points. Flight altitude first limited due to the heavy fuel load. On way back, after waypoint 18, the 2.5 km level leg was backtracked and a 3 km level leg stacked on top of that. This was done because of concern about the low-altitude level legs disappearing into the boundary layer before they could be sampled on subsequent flight. <?xmltex \hack{\hfill\break}?>(RA 2/SS 3/ML 3/ICL 1/ACL 0/STL 2/IPL 9/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/17 <?xmltex \hack{\hfill\break}?>PRF04Y17</oasis:entry>
         <oasis:entry colname="col2">9.1</oasis:entry>
         <oasis:entry colname="col3">Target: suitcase flight São Tomé to Ascension Island; the objective was to resample air masses from four horizontal legs in flight PRF03Y17. Flight path connected midpoints of legs sampled in PRF03Y17 on their 48 h trajectories – first, overflight of parcels for lidar sampling, then re-trace of track at projected parcel height after transport, then forward run along the same track near cloud top. Low clouds had largely cleared in the region between WPs 3 and 5, precluding cloud sampling. Due to significant interest in the BL Cu near ASI, the P-3 headed west at 8<inline-formula><mml:math id="M228" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S (rather than planned 9.7<inline-formula><mml:math id="M229" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S). Plan was to sample scattered Cu along 8<inline-formula><mml:math id="M230" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S between <inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M232" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W and Ascension Island. P-3 sampled the BB plume to 7.5<inline-formula><mml:math id="M233" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W and then descended into the MBL. Sawtooths through the boundary layer. Clouds were seen but time in cloud was insufficient for sampling. On approach to Ascension Island we overflew the ARM site. <?xmltex \hack{\hfill\break}?>(RA 6/SS 2/ML 4/ICL 1/ACL 1/STL 2/IPL 8/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/18 <?xmltex \hack{\hfill\break}?>PRF05Y17</oasis:entry>
         <oasis:entry colname="col2">5.5</oasis:entry>
         <oasis:entry colname="col3">Target: Ascension Island local; the goal was a coordinated flight with CLARIFY Bae146 to compare aerosol and cloud in situ and radiation measurements. A highly successful coordinated flight, given the difficult cloud and aerosol forecasts. Bae146 assumed formation during initial climb-out to WP 2. Cloud conditions were very broken except for the leg between WP 4 and 5, making cloud comparisons limited. Lots of full boundary layer profiling between WP 10 and 11. Extended HSRL run over the ARM site <?xmltex \hack{\hfill\break}?>(RA 2/SS 0/ML 2/ICL 2/ACL 0/STL 1/IPL 0/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/19 <?xmltex \hack{\hfill\break}?>PRF06Y17</oasis:entry>
         <oasis:entry colname="col2">2.0</oasis:entry>
         <oasis:entry colname="col3">Transit: Ascension Island to São Tomé – aborted transit flight, limited set of instrumentation operated. <?xmltex \hack{\hfill\break}?>(RA 0/SS 0/ML 0/ICL 0/ACL 0/STL 0/IPL 1/APL 0)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">08/21 <?xmltex \hack{\hfill\break}?>PRF07Y17</oasis:entry>
         <oasis:entry colname="col2">8.3</oasis:entry>
         <oasis:entry colname="col3">Target: return suitcase flight, Ascension Island to São Tomé; the objective was to measure the west-to-east transition mostly in the boundary layer. Ranging from “clean above” to “heavier free troposphere pollution above (and mixing into) low cloud” to the east. Also, sampling on routine flight track. Aircraft maintenance issue reduced possible flight time to <inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula> h. Science focus was on three different plume and cloud regimes along 8<inline-formula><mml:math id="M235" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S and the routine track (along 5<inline-formula><mml:math id="M236" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E). Flight featured profiles in very different conditions; low clouds were more broken than forecast. Cirrus (Ci) on the 8S track (near 1<inline-formula><mml:math id="M237" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E). A blob of mid-level clouds and high ACAOD (0.73) at <inline-formula><mml:math id="M238" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M239" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/0<inline-formula><mml:math id="M240" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. <?xmltex \hack{\hfill\break}?>(RA 3/SS 3/ML 3/ICL 2/ACL 4/STL 1/IPL 6/APL 3)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{p}?><table-wrap id="App1.Ch1.S1.T8" specific-use="star"><?xmltex \currentcnt{A2}?><?xmltex \def\figurename{Table}?><label>Table A2</label><caption><p id="d1e5712">Continued.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="2cm"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="14cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Date <?xmltex \hack{\hfill\break}?>P-3 flight no.</oasis:entry>
         <oasis:entry colname="col2">h</oasis:entry>
         <oasis:entry colname="col3">Flight synopsis <?xmltex \hack{\hfill\break}?>(ramps, RA; square spirals, SS; MBL legs, ML; in-cloud legs, ICL; above-cloud legs, ACL; sawtooth legs, STL; in-plume legs, IPL; above-plume legs, APL)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/24 <?xmltex \hack{\hfill\break}?>PRF08Y17</oasis:entry>
         <oasis:entry colname="col2">9.4</oasis:entry>
         <oasis:entry colname="col3">Routine: flight to 15<inline-formula><mml:math id="M241" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S along 5<inline-formula><mml:math id="M242" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and back with some sampling of initial trajectory lines. High cloud contamination of remote sensing on the northern part of the track. Solid deck at 15–10<inline-formula><mml:math id="M243" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, then small popcorn Cu to 5<inline-formula><mml:math id="M244" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, and then Sc followed by mid-level cloud. Lightly polluted BL. SDI inlet froze. <?xmltex \hack{\hfill\break}?>(RA 5/SS 2/ML 3/ICL 3/ACL 3/STL 1/IPL 7/APL 3)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/26 <?xmltex \hack{\hfill\break}?>PRF09Y17</oasis:entry>
         <oasis:entry colname="col2">9.7</oasis:entry>
         <oasis:entry colname="col3">Target: the focus was on radiation walls over broken cloud decks of varying albedos and relatively invariant aerosol. Targeted a region with broken low clouds, significant aerosol loading, and free of high clouds. Adjusted target area based on morning forecasts and satellite imagery high Ci north of 5<inline-formula><mml:math id="M245" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Two successful radiation wall modules. Long transit prevented the third planned radiation wall. Many adjustments in flight for cloud conditions. During first radiation wall, low clouds were scattered to broken, no Ci. During the second wall module, significant Ci contamination for the center part of the legs. Good low clouds for most of the wall. In-plume legs near 2<inline-formula><mml:math id="M246" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S along the routine track. <?xmltex \hack{\hfill\break}?>(RA 2/SS 4/ML 2/ICL 2/ACL 3/STL 0/IPL 5/APL 3)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/28 <?xmltex \hack{\hfill\break}?>PRF10Y17</oasis:entry>
         <oasis:entry colname="col2">9.5</oasis:entry>
         <oasis:entry colname="col3">Routine: flight to 15<inline-formula><mml:math id="M247" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, with a simplified radiation wall, followed by cloud work and stacked aerosol sampling. Absence of Ci at 11<inline-formula><mml:math id="M248" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S allowed good square spiral maneuver over mostly solid cloud. Max ACAOD of 0.76. Extensive cloud sampling. <?xmltex \hack{\hfill\break}?>(RA 3/SS 1/ML 1/ICL 2/ACL 3/STL 2/IPL 4/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/30 <?xmltex \hack{\hfill\break}?>PRF11Y17</oasis:entry>
         <oasis:entry colname="col2">8.9</oasis:entry>
         <oasis:entry colname="col3">Routine: the objective was routine flight, but not reaching as far south and allowing for a full radiation wall (less cloud work and more above-cloud legs than on 28 August flight), and includes sampling of fresh aerosol and trajectory initialization points. HSRL-2 failure removed need for initial high-altitude leg; instead, sampled within the aerosol plume to 13<inline-formula><mml:math id="M249" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Because of Ci, performed radiation wall at 8S. Sampled the plume southbound between 4 and 10<inline-formula><mml:math id="M250" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S at 3.5 km altitude and northbound between 7 and 3<inline-formula><mml:math id="M251" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S at 3.0 km altitude. <?xmltex \hack{\hfill\break}?>(RA 2/SS 3/ML 1/ICL 1/ACL 1/STL 0/IPL 8/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">08/31 <?xmltex \hack{\hfill\break}?>PRF12Y17</oasis:entry>
         <oasis:entry colname="col2">8.3</oasis:entry>
         <oasis:entry colname="col3">Target: the objective was to resample plume sampled on previous day at 3.5 and 3.0 km between 4 and 10<inline-formula><mml:math id="M252" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S along routine track. Plume was projected to be lower than 3 km, but at 2.6 km the aircraft was below the bottom of the plume. Got remote-sensing measurements and cloud measurements in coordination with the A-train overpass. At the northern end of the in situ plume leg (corresponding to air masses sampled at 3–5<inline-formula><mml:math id="M253" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S on 30 August), performed a series of stacked legs at 2.7, 2.9, and 3.0 km to check for vertical variations in aerosol properties. <?xmltex \hack{\hfill\break}?>(RA 2/SS 2/ML 1/ICL 1/ACL 1/STL 0/IPL 12/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/02 <?xmltex \hack{\hfill\break}?>PRF13Y17</oasis:entry>
         <oasis:entry colname="col2">8.7</oasis:entry>
         <oasis:entry colname="col3">Transit: São Tomé to Ascension Island – the objective was to measure BB aerosol at the northern end of the study area, possibly affected by wet convection; get AERONET-like retrieval from 4STAR in a mix of biomass burning smoke and dust, supplemented with in situ and HSRL measurements. Also, sample near ASI where previously sampled air masses may be present. Got one radiation spiral each without and with some dust present. Near ASI, high-altitude HSRL legs, plume leg, and above-cloud leg. Series of legs to study cloudy region just to NE of ASI. <?xmltex \hack{\hfill\break}?>(RA 4/SS 6/ML 1/ICL 1/ACL 5/STL 1/IPL 6/APL 4)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">14</oasis:entry>
         <oasis:entry namest="col2" nameend="col3">114.0 </oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{t}?><table-wrap id="App1.Ch1.S1.T9" specific-use="star"><?xmltex \currentcnt{A3}?><?xmltex \def\figurename{Table}?><label>Table A3</label><caption><p id="d1e5976">The 2018 flight summary for the P-3 aircraft.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="2cm"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="14cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Date <?xmltex \hack{\hfill\break}?>P-3 no.</oasis:entry>
         <oasis:entry colname="col2">h</oasis:entry>
         <oasis:entry colname="col3">Flight synopsis <?xmltex \hack{\hfill\break}?>(ramps, RA; square spirals, SS; MBL legs, ML; in-cloud legs, ICL; above-cloud legs, ACL; sawtooth legs, STL; in-plume legs, IPL; above-plume legs, APL)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/24 <?xmltex \hack{\hfill\break}?>PRF00Y18</oasis:entry>
         <oasis:entry colname="col2">9.3</oasis:entry>
         <oasis:entry colname="col3">Transit: Cabo Verde to São Tomé; mostly transit flight at high altitude, but some in situ sampling near São Tomé. <?xmltex \hack{\hfill\break}?>(RA 0/SS 2/ML 1/ICL 1/ACL 1/STL 0/IPL 1/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/27 <?xmltex \hack{\hfill\break}?>PRF01Y18</oasis:entry>
         <oasis:entry colname="col2">8.0</oasis:entry>
         <oasis:entry colname="col3">Routine: flight along 5<inline-formula><mml:math id="M254" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E to 13<inline-formula><mml:math id="M255" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. High-altitude transit out, square spiral down at 13<inline-formula><mml:math id="M256" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, followed by three samples of the cloudy boundary layer on the way back north, with the most northern one being at <inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M258" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Strong aerosol layering south of 5<inline-formula><mml:math id="M259" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, fairly clean to the north. Little aerosol right above cloud top. <?xmltex \hack{\hfill\break}?>(RA 3/SS 2/ML 2/ICL 1/ACL 1/STL 3/IPL 4/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">09/30 <?xmltex \hack{\hfill\break}?>PRF02Y18</oasis:entry>
         <oasis:entry colname="col2">7.7</oasis:entry>
         <oasis:entry colname="col3">Target: the objective was radiation work near 7–9<inline-formula><mml:math id="M260" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S in radiation wall patterns over broken cloud decks of varying albedos and (nominally) relatively invariant aerosol. Coordinated with MISR local mode. Square spiral near 7.5<inline-formula><mml:math id="M261" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, well coordinated with MISR overpass, in an area of solid low cloud cover. Hit CALIPSO overpass for RSP; got on their track <inline-formula><mml:math id="M262" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula> min after satellite overpass. <?xmltex \hack{\hfill\break}?>(RA 4/SS 1/ML 3/ICL 0/ACL 1/STL 2/IPL 5/APL 4)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/02 <?xmltex \hack{\hfill\break}?>PRF03Y18</oasis:entry>
         <oasis:entry colname="col2">8.5</oasis:entry>
         <oasis:entry colname="col3">Routine: the goal was a flight to 10<inline-formula><mml:math id="M263" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, with setup of BL Lagrangian sampling in PRF04. At approximately 6.7<inline-formula><mml:math id="M264" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, found a transition from closed cells to pockets of open cells (POCs). AOD <inline-formula><mml:math id="M265" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.45</mml:mn></mml:mrow></mml:math></inline-formula>. Square spiral at 10.5<inline-formula><mml:math id="M266" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Boundary layer quite clean with a few big particles, low CN, CO <inline-formula><mml:math id="M267" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">70</mml:mn></mml:mrow></mml:math></inline-formula> ppb, and <inline-formula><mml:math id="M268" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> ppb. A series of 2.5 dull sawtooths, with a clean slot right above the cloud (<inline-formula><mml:math id="M270" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">200</mml:mn></mml:mrow></mml:math></inline-formula> ft/0.06 km). Several constant-altitude legs with high CCN. <?xmltex \hack{\hfill\break}?>(RA 3/SS 3/ML 2/ICL 1/ACL 3/STL 2/IPL 3/APL 4)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/03 <?xmltex \hack{\hfill\break}?>PRF04Y18</oasis:entry>
         <oasis:entry colname="col2">8.5</oasis:entry>
         <oasis:entry colname="col3">Target: Lagrangian resampling of POCs sampled on PRF03; closed cells present on the transit from São Tomé to 5<inline-formula><mml:math id="M271" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 7.5<inline-formula><mml:math id="M272" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. East of 6<inline-formula><mml:math id="M273" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E along 7.5<inline-formula><mml:math id="M274" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, a large region of open cells with significantly lower cloud fraction; FT plume was extensive aloft above both the POC and the surrounding closed cells. Clear evidence of smoke aerosol being present immediately above clouds in closed and open cell regions. <?xmltex \hack{\hfill\break}?>(RA 4/SS 4/ML 2/ICL 1/ACL 2/STL 2/IPL 4/APL 2)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/05 <?xmltex \hack{\hfill\break}?>PRF05Y18</oasis:entry>
         <oasis:entry colname="col2">9.0</oasis:entry>
         <oasis:entry colname="col3">Target: the objective was radiation work at high solar zenith; radiation wall between 5.5<inline-formula><mml:math id="M275" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E and 7<inline-formula><mml:math id="M276" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W on 9.5<inline-formula><mml:math id="M277" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S; incl. high-altitude overpass; square spiral from <inline-formula><mml:math id="M278" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula> km to surface in mostly cloudy conditions; above-cloud, in-cloud, below-cloud leg; three vertically stacked in situ sampling legs in the plume. Second similar maneuver in almost clear conditions. Boundary layer most polluted so far in ORACLES 2018. Cloud droplet number concentrations accordingly elevated. Appeared to be a more aged plume than other days in ORACLES 2018. Good case for radiative closure: two square spirals in different <?xmltex \hack{\hfill\break}?>conditions, the full radiation wall, moderate RH in the plume. <?xmltex \hack{\hfill\break}?>(RA 4/SS 3/ML 4/ICL 2/ACL 3/STL 0/IPL 5/APL 5)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/07 <?xmltex \hack{\hfill\break}?>PRF06Y18</oasis:entry>
         <oasis:entry colname="col2">8.4</oasis:entry>
         <oasis:entry colname="col3">Routine: flight to 15<inline-formula><mml:math id="M279" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. During transit to 15<inline-formula><mml:math id="M280" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S north–south slope in Sc cloud top heights from 2 to 7<inline-formula><mml:math id="M281" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S with sloping aerosol layers above. From 10 to 15<inline-formula><mml:math id="M282" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S mid-level clouds at the top of the outflow plume, embedded in the plume. Boundary layer work between 12 and 9.5<inline-formula><mml:math id="M283" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S – fairly polluted BL. Extended run at 8 kft (2.4 km), clear slot at 9<inline-formula><mml:math id="M284" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S for square spiral and radiation work. This spiral happened in the most cloud-free conditions encountered in ORACLES-2018. Extended leg (1 h<inline-formula><mml:math id="M285" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>) at 8 kft (2.4 km), during transit home. <?xmltex \hack{\hfill\break}?>(RA 6/SS 2/ML 3/ICL 1/ACL 2/STL 1/IPL 4/APL 5)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/10 <?xmltex \hack{\hfill\break}?>PRF07Y18</oasis:entry>
         <oasis:entry colname="col2">8.3</oasis:entry>
         <oasis:entry colname="col3">Routine: the plan was for a flight to 13<inline-formula><mml:math id="M286" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S along 5<inline-formula><mml:math id="M287" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. Three samples of polluted boundary layer allow for the possibility of Lagrangian sampling on 12 October. Square spiral nearly to surface at 13<inline-formula><mml:math id="M288" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Cloud sampling south of 10<inline-formula><mml:math id="M289" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Sampling aerosol layer at 13 kft (4.0 km) between 9 and 10<inline-formula><mml:math id="M290" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Long boundary layer sequence, starting at 7.5<inline-formula><mml:math id="M291" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Aerosol and boundary layer work near 4.5<inline-formula><mml:math id="M292" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Aerosol at southern end of track up to 19.5 kft (5.9 km). <?xmltex \hack{\hfill\break}?>(RA 6/SS 3/ML 4/ICL 2/ACL 3/STL 2/IPL 4/APL 3)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">10/12 <?xmltex \hack{\hfill\break}?>PRF08Y18</oasis:entry>
         <oasis:entry colname="col2">5.3</oasis:entry>
         <oasis:entry colname="col3">Target: the objective was Lagrangian follow-up and cloud profiling. Engine issue delayed departure; flight duration shortened by <inline-formula><mml:math id="M293" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> h. Outbound transit straight south of São Tomé to initial point at 2.5<inline-formula><mml:math id="M294" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 6.5<inline-formula><mml:math id="M295" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E where trajectory indicated resampling of boundary layer air. Square spiral at 2<inline-formula><mml:math id="M296" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/5.75<inline-formula><mml:math id="M297" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. Boundary layer sampling, followed by sawtooth sampling through decoupled cloud layers (stratus above Cu). Cloud patch thicker and precipitating at the north end of the runs. Quite clean conditions just above cloud. More cloud work at 4.5<inline-formula><mml:math id="M298" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, 5.5<inline-formula><mml:math id="M299" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. Ensuing run northbound crossed distinct boundary between clear and polluted air, with corresponding changes in cloud properties. <?xmltex \hack{\hfill\break}?>(RA 2/SS 2/ML 3/ICL 1/ACL 5/STL 2/IPL 2/APL 1)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{t}?><table-wrap id="App1.Ch1.S1.T10" specific-use="star"><?xmltex \currentcnt{A3}?><?xmltex \def\figurename{Table}?><label>Table A3</label><caption><p id="d1e6588">Continued.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="2cm"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="14cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Date <?xmltex \hack{\hfill\break}?>P-3 no.</oasis:entry>
         <oasis:entry colname="col2">h</oasis:entry>
         <oasis:entry colname="col3">Flight synopsis <?xmltex \hack{\hfill\break}?>(ramps, RA; square spirals, SS; MBL legs, ML; in-cloud legs, ICL; above-cloud legs, ACL; sawtooth legs, STL; in-plume legs, IPL; above-plume legs, APL)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/15 <?xmltex \hack{\hfill\break}?>PRF09Y18</oasis:entry>
         <oasis:entry colname="col2">7.8</oasis:entry>
         <oasis:entry colname="col3">Routine: the plan was for a flight to 14<inline-formula><mml:math id="M300" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. During southbound transit, minimal direct contact between smoke and Sc at 3–9<inline-formula><mml:math id="M301" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Heavily precipitating Sc clouds at 5<inline-formula><mml:math id="M302" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Two regions with plume bottom/cloud top gap (8.5<inline-formula><mml:math id="M303" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) and no gap (9.5<inline-formula><mml:math id="M304" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S) in relative close proximity. Significant drizzle between 11 and 13<inline-formula><mml:math id="M305" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Square spiral at 14<inline-formula><mml:math id="M306" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S; geometrically thin high smoke loading layer at 13 kft (4.0 km), broken Sc. Very clean BL, low cloud bases 500 ft (0.15 km). During sawtooth northbound, clouds thickening, peak above-cloud smoke at 12.4<inline-formula><mml:math id="M307" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, dropping to the N. Second set of sawtooth patterns contrasting 9.5 and 8.5<inline-formula><mml:math id="M308" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S – smoke near cloud top at 9.5 and gap at 8.5<inline-formula><mml:math id="M309" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Circular spiral descent at 5.5<inline-formula><mml:math id="M310" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. <?xmltex \hack{\hfill\break}?>(RA 1/SS 2/ML 2/ICL 0/ ACL 3/STL 2/IPL 4/APL 4)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/17 <?xmltex \hack{\hfill\break}?>PRF10Y18</oasis:entry>
         <oasis:entry colname="col2">8.5</oasis:entry>
         <oasis:entry colname="col3">Target: young plume near 7<inline-formula><mml:math id="M311" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/10<inline-formula><mml:math id="M312" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. At 10.5<inline-formula><mml:math id="M313" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E, 7<inline-formula><mml:math id="M314" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S still featured mid-level clouds. Opted to change order radiation wall/spiral module, aerosol in situ legs first (highest altitude layer to lowest altitude layer); then below, in- and above-cloud legs; then square spiral up. Highest aerosol concentrations encountered yet, found in the lower free troposphere. <?xmltex \hack{\hfill\break}?>(RA 0/SS 5/ML 1/ ICL 1/ACL 2/STL 0/IPL 9/APL 5)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/19 <?xmltex \hack{\hfill\break}?>PRF11Y18</oasis:entry>
         <oasis:entry colname="col2">8.0</oasis:entry>
         <oasis:entry colname="col3">Target: the objective was to sample young plume near the coast 7<inline-formula><mml:math id="M315" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S/10<inline-formula><mml:math id="M316" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. Moved north–south sampling further north and west to avoid high cirrus. Evidence of very clean air directly above clouds. Did not find fresh plume near Bight of Angola, ACAOD only <inline-formula><mml:math id="M317" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.27</mml:mn></mml:mrow></mml:math></inline-formula>. Two square spirals near each other, one over clear skies, the other over partially cloudy. The bottom of one square spiral had a ship and its plume. Clean MBL, and ultra-clean above clouds. Underflight of partial cloudy skies – high potential of 3D cloud–aerosol radiative effect. Good in situ sampling, while in cloud (TDMA <inline-formula><mml:math id="M318" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> CVI), indication of large aerosols. High cloud droplet number concentrations were observed near cloud bases (opposite of what has been observed in the past). <?xmltex \hack{\hfill\break}?>(RA 5/SS 4/ML 3/ICL 1/ACL 5/STL 1/IPL 7/APL 6)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/21 <?xmltex \hack{\hfill\break}?>PRF12Y18</oasis:entry>
         <oasis:entry colname="col2">8.2</oasis:entry>
         <oasis:entry colname="col3">Routine: the plan was to reach as far south as possible again; during southbound transit, FT BB aerosol plume tendril-like structure with numerous layers overlapping; interesting wave-like structure in low clouds from 1.9–3<inline-formula><mml:math id="M319" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, with wavelength of <inline-formula><mml:math id="M320" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> km; evidence of N–S mesoscale banding in Sc cloud layer below; at 13.5<inline-formula><mml:math id="M321" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S – square spiral to 200 ft (0.06 km). Plume concentrations all around half of typical values. Ultra-large particles detected on descent. Aerosol well aged in lower part of plume. Multiple sawtooth patterns for cloud work and level legs in plume. <?xmltex \hack{\hfill\break}?>(RA 8/SS 1/ML 6/ICL 2/ACL 2/STL 2/ IPL 6/APL 5)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/23 <?xmltex \hack{\hfill\break}?>PRF13Y18</oasis:entry>
         <oasis:entry colname="col2">8.1</oasis:entry>
         <oasis:entry colname="col3">Target: the plan was for a survey flight going west along 5<inline-formula><mml:math id="M322" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Only flight with significant boundary layer cloud sampling to the west of 5<inline-formula><mml:math id="M323" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E. Four sawtooths through double-layered stratocumulus in which the lower layer cloud droplet number concentrations exceeded those in the upper layer. Generally low ACAOD of 0.19 max. <?xmltex \hack{\hfill\break}?>(RA 2/SS 2/ML 3/ICL 0/ACL 4/STL 3/IPL 4/APL 3)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">10/25 <?xmltex \hack{\hfill\break}?>PRF14Y18</oasis:entry>
         <oasis:entry colname="col2">7.8</oasis:entry>
         <oasis:entry colname="col3">Transit: São Tomé to Cabo Verde; survey flight going west. High-altitude along 5<inline-formula><mml:math id="M324" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> E to 5<inline-formula><mml:math id="M325" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S, then turn west, out to 3<inline-formula><mml:math id="M326" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W along 5<inline-formula><mml:math id="M327" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> S. Three samples of the cloudy boundary layer on the way back. Four sawtooths through double-layered stratocumulus; lower layer cloud droplet number concentrations exceeded those in the upper layer. Square spiral at 3<inline-formula><mml:math id="M328" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W. <?xmltex \hack{\hfill\break}?>(RA 1/SS 1/ML 1/ICL 0/ACL 0/STL 0/IPL 0/APL 3)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">15/15</oasis:entry>
         <oasis:entry namest="col2" nameend="col3">121.4 </oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e6992"><?xmltex \hack{\clearpage}?>Figure A1 shows the distribution of flight times dedicated to the various
flight maneuvers described in Table 5 in each of the three ORACLES
deployments. While broadly similar, there are a few notable distinctions:
2017 and 2018 featured significantly fewer ramp descents, relatively less
time just above cloud top, and more time dedicated to square spiral
descents. Also, 2017 and 2018 entailed more sawtooth profiling through
clouds than time spent in level legs within clouds. These changes represent
an evolution in the thinking regarding the best flight maneuvers to address
various cloud- and radiation-related science objectives from the first to
the second and third deployment.</p>

      <?xmltex \floatpos{h!}?><fig id="App1.Ch1.S1.F23"><?xmltex \currentcnt{A1}?><?xmltex \def\figurename{Figure}?><label>Figure A1</label><caption><p id="d1e6998">Distribution of flight time between flight maneuvers for each
ORACLES deployment year.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/1507/2021/acp-21-1507-2021-f23.png"/>

      </fig>

<?xmltex \hack{\clearpage}?>
</app>

<?pagebreak page1549?><app id="App1.Ch1.S2">
  <?xmltex \currentcnt{B}?><label>Appendix B</label><title>Choice of instrumentation</title>

<?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S2.T11"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{B1}?><?xmltex \def\figurename{Table}?><label>Table B1</label><caption><p id="d1e7021">P-3 instrumentation in ORACLES (bold entries indicate quantities
submitted to the ORACLES archive; see ORACLES Science Team, 2020a–d, in the
list of references).</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.85}[.85]?><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="4cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="6cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="6cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Instrument name/operating <?xmltex \hack{\hfill\break}?>organization</oasis:entry>
         <oasis:entry colname="col2"><?xmltex \hack{\mbox\bgroup}?>Instrument description<?xmltex \hack{\egroup}?>/key specification</oasis:entry>
         <oasis:entry colname="col3">Primary measurement</oasis:entry>
         <oasis:entry colname="col4">Measurements/<?xmltex \hack{\mbox\bgroup}?>derived quantities<?xmltex \hack{\egroup}?>/inversion products</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="left">Remote sensing </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">4STAR/NASA ARC</oasis:entry>
         <oasis:entry colname="col2">Hyperspectral sun/sky photometer (400–1600 nm, <inline-formula><mml:math id="M329" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> nm res.)</oasis:entry>
         <oasis:entry colname="col3">1. Direct solar beam hyperspectral transmittance</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">1. Spectral AOD</oasis:entry>
       <?xmltex \interline{[-19.916929pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" colname="col3"/>
         <oasis:entry rowsep="1" colname="col4">2. Column O<inline-formula><mml:math id="M330" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, H<inline-formula><mml:math id="M331" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O, NO<inline-formula><mml:math id="M332" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" colname="col3">2. Sky radiance</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">3. Aerosol microphysics (e.g., size distribution, refr. index, absorption, scattering phase function)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">3. Hyperspectral cloud zenith transmittance</oasis:entry>
         <oasis:entry colname="col4">4. Cloud optical depth, <inline-formula><mml:math id="M333" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, liquid water path, thermodynamic phase</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">RSP/NASA GISS</oasis:entry>
         <oasis:entry colname="col2">Measurements at 410, 470, 555, 670, 865, 960, 1590, 1880, and 2260 nm with polarimetric accuracy of <inline-formula><mml:math id="M334" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.15</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Stokes parameters <inline-formula><mml:math id="M335" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M336" display="inline"><mml:mi>Q</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M337" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> of reflected light</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">1. Aerosol microphysics, layer height, and AOD</oasis:entry>
       <?xmltex \interline{[-31.298031pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" colname="col3">Measurements are over <inline-formula><mml:math id="M338" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M339" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> from nadir</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">2. Water COD, droplet size distribution at cloud top, bulk effective radius, top height, physical thickness, <inline-formula><mml:math id="M340" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">3. Chl, CDOM conc. and backscatter coeff.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">AMPR/NASA MSFC</oasis:entry>
         <oasis:entry colname="col2">Advanced Microwave Precipitation Radiometer <?xmltex \hack{\hfill\break}?>four-frequency (10.7, 19.35, 37.1, and 85.5 GHz), cross-track scanning, polarization-variable microwave radiometer</oasis:entry>
         <oasis:entry colname="col3">Polarized brightness temperatures</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">1. Precipitation rate</oasis:entry>
       <?xmltex \interline{[-28.452756pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry rowsep="1" colname="col4">2. Liquid water path</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">3. Ocean SST, winds</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">SSFR, CG-4 <?xmltex \hack{\hfill\break}?>/NASA ARC, CU LASP</oasis:entry>
         <oasis:entry colname="col2">Solar Spectral Flux Radiometer (350–2100 nm shortwave irradiance, spectral sampling 4–8 nm) <?xmltex \hack{\hfill\break}?>CG-4 (longwave irradiance 4–40 <inline-formula><mml:math id="M341" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">Spectral solar irradiance</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">1. Cloud and aerosol radiative effects</oasis:entry>
       <?xmltex \interline{[-48.369685pt]}?></oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry rowsep="1" colname="col4">2. Spectral and broadband absorption and heating rate, aerosol SSA from flux divergence</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">3. Cloud phase, OD, <inline-formula><mml:math id="M342" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (from albedo and transmittance)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">APR3</oasis:entry>
         <oasis:entry colname="col2">Three-frequency cloud and precipitation Doppler scanning radar (Ku, Ka, and W band)</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">1. Cloud and precipitation backscatter</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">Rain water content and precipitation rate</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" colname="col3">2. Cloud and precipitation differential backscatter</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">Hydrometeor size (precipitation class)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" colname="col3">3. Cloud and precipitation Doppler velocity</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">Hydrometeor classification (dominant)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">4. Path-integrated attenuation</oasis:entry>
         <oasis:entry colname="col4">Vertical air velocity in precipitation</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S2.T12"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{B1}?><?xmltex \def\figurename{Table}?><label>Table B1</label><caption><p id="d1e7440">Continued.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.85}[.85]?><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="4cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="6cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="6cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Instrument name/operating <?xmltex \hack{\hfill\break}?>organization</oasis:entry>
         <oasis:entry colname="col2"><?xmltex \hack{\mbox\bgroup}?>Instrument description<?xmltex \hack{\egroup}?>/key specification</oasis:entry>
         <oasis:entry colname="col3">Primary measurement</oasis:entry>
         <oasis:entry colname="col4">Measurements/<?xmltex \hack{\mbox\bgroup}?>derived quantities<?xmltex \hack{\egroup}?>/inversion products</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="left">Cloud in situ </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">CAPS/UND</oasis:entry>
         <oasis:entry rowsep="1" colname="col2">1. Cloud imaging probe – optical array probe (25–1600 <inline-formula><mml:math id="M343" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, 25 <inline-formula><mml:math id="M344" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> res.)</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Cloud particle images</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">Number distribution function, nominally between 25–1600 <inline-formula><mml:math id="M345" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, particle images from which other parameters can be derived: total concentration, liquid water content, etc.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" colname="col2">2. Cloud and Aerosol Spectrometer (CAS, forward scattering) (0.53–50 <inline-formula><mml:math id="M346" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, 1 <inline-formula><mml:math id="M347" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> nominal res.)</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Number size distribution</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">Number distribution function between 0.53 and 50 <inline-formula><mml:math id="M348" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, from which liquid water content, effective radius, and other parameters can be derived</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">3. Liquid water content (LWC) sensor (0–3 <inline-formula><mml:math id="M349" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), not operational</oasis:entry>
         <oasis:entry colname="col3">Liquid water content</oasis:entry>
         <oasis:entry colname="col4">Bulk liquid water content</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry rowsep="1" colname="col1">CDP/UND</oasis:entry>
         <oasis:entry rowsep="1" colname="col2">Forward scattering (2–50 <inline-formula><mml:math id="M350" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M351" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M352" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> res.)</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Number size distribution</oasis:entry>
         <oasis:entry colname="col4">Number distribution function between 3 and 50 <inline-formula><mml:math id="M353" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, from which liquid water content, effective radius, and other parameters can be derived</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry rowsep="1" colname="col1">CDP/LARC</oasis:entry>
         <oasis:entry rowsep="1" colname="col2">Cloud droplet probe <?xmltex \hack{\hfill\break}?>forward scattering (2–50 <inline-formula><mml:math id="M354" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M355" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M356" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> res.)</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Number size distribution</oasis:entry>
         <oasis:entry colname="col4"/>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">CDP/HiGEAR</oasis:entry>
         <oasis:entry colname="col2">Cloud droplet probe <?xmltex \hack{\hfill\break}?>forward scattering (2–50 <inline-formula><mml:math id="M357" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M358" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M359" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> res.)</oasis:entry>
         <oasis:entry colname="col3">Number size distribution</oasis:entry>
         <oasis:entry colname="col4"/>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">King/UND</oasis:entry>
         <oasis:entry colname="col2">Hot wire liquid water (0–5 <inline-formula><mml:math id="M360" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3">Liquid water content</oasis:entry>
         <oasis:entry colname="col4">Bulk liquid water content</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">2-DS/ UND</oasis:entry>
         <oasis:entry colname="col2">Two-dimensional stereo probe <?xmltex \hack{\hfill\break}?>optical array probe (10–1280 <inline-formula><mml:math id="M361" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, 10 <inline-formula><mml:math id="M362" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> res.)</oasis:entry>
         <oasis:entry colname="col3">Cloud particle images</oasis:entry>
         <oasis:entry colname="col4">Number distribution function, nominally between 10–1280 <inline-formula><mml:math id="M363" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, and particle images from which other parameters can be derived (total concentration, liquid water content, etc.)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">HVPS-3/ UND</oasis:entry>
         <oasis:entry colname="col2">High Volume Precipitation Spectrometer <?xmltex \hack{\hfill\break}?>optical array probe (150–19 200 <inline-formula><mml:math id="M364" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, 150 <inline-formula><mml:math id="M365" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> res.)</oasis:entry>
         <oasis:entry colname="col3">Cloud particle images</oasis:entry>
         <oasis:entry colname="col4">Number distribution function, nominally between 150–19 200 <inline-formula><mml:math id="M366" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, and particle images from which total concentration and rain water content can be derived</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">FPDR-PDI/Univ. Hawaii</oasis:entry>
         <oasis:entry colname="col2">Cloud droplet size and velocity measurements</oasis:entry>
         <oasis:entry colname="col3">Droplet size and arrival time</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">1. Droplet size (<inline-formula><mml:math id="M367" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>) and arrival time (<inline-formula><mml:math id="M368" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry rowsep="1" colname="col4">2. <inline-formula><mml:math id="M369" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (# cm<inline-formula><mml:math id="M370" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry rowsep="1" colname="col4">3. Derived LWC (<inline-formula><mml:math id="M371" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">4. Droplet velocity (<inline-formula><mml:math id="M372" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S2.T13"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{B1}?><?xmltex \def\figurename{Table}?><label>Table B1</label><caption><p id="d1e8022">Continued.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.85}[.85]?><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="4cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="6cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="6cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Instrument name/operating <?xmltex \hack{\hfill\break}?>organization</oasis:entry>
         <oasis:entry colname="col2"><?xmltex \hack{\mbox\bgroup}?>Instrument description<?xmltex \hack{\egroup}?>/key specification</oasis:entry>
         <oasis:entry colname="col3">Primary measurement</oasis:entry>
         <oasis:entry colname="col4">Measurements/<?xmltex \hack{\mbox\bgroup}?>derived quantities<?xmltex \hack{\egroup}?>/inversion products</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="left">Aerosol in situ </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">HiGEAR/Univ. Hawaii</oasis:entry>
         <oasis:entry rowsep="1" colname="col2">TSI 3321 APS (0.8 to 5 <inline-formula><mml:math id="M373" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> aerodynamic) <?xmltex \hack{\hfill\break}?>DMT UHSAS (70 to 1000 nm optical) <?xmltex \hack{\hfill\break}?>Modified TSI long SMPS (10–550 nm) <?xmltex \hack{\hfill\break}?>Custom TSI thermal tandem SMPS (10 to 200 nm)</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Dry number size distributions <?xmltex \hack{\hfill\break}?>Particle volatility</oasis:entry>
         <oasis:entry colname="col4">Number, area, volume distributions, CCN concentration (indirect)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" colname="col2">TSI 3025A ultrafine CN counter (1–3000 nm)</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Total particle concentration</oasis:entry>
         <oasis:entry rowsep="1" colname="col4"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" colname="col2">TSI 3010 CN counters (3–3000 nm, ambient and denuded to 400 <inline-formula><mml:math id="M374" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C)</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Total particle concentration</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">Internal/external mixing</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" colname="col2">TSI 3563 three-wavelength nephelometers <?xmltex \hack{\hfill\break}?>Paired Radiance Research M901 nephelometers, one with humidity-controlled inlet <?xmltex \hack{\hfill\break}?>Two Radiance Research three-wavelength PSAPs</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Dry particle scattering coefficient, backscattering @ 450, 550, 700 nm <?xmltex \hack{\hfill\break}?>Wet vs. dry scattering @ 550 nm <?xmltex \hack{\hfill\break}?>Particle light absorption</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">SSA, scat. Ångstr. exp., abs. Ångstr. exp., extinction (@ 470, 530, 660 nm)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">DMT SP2 (Single Particle Soot Photometer, four-channel, 90–500 nm) 2016 only</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Refractory black carbon concentration,</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">BC concentration</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry rowsep="1" colname="col2"/>
         <oasis:entry rowsep="1" colname="col3">Refractory black carbon mass</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">BC mass distribution, BB tracer</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Aerodyne HR-ToF-aerosol mass spectrometer (AMS)</oasis:entry>
         <oasis:entry colname="col3">Non-refractory aerosol composition</oasis:entry>
         <oasis:entry colname="col4">Sulfates, nitrates, organics, chloride, BB tracer, pollution tracer</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">PCASP/UND</oasis:entry>
         <oasis:entry colname="col2">Passive Cavity Aerosol Spectrometer Probe</oasis:entry>
         <oasis:entry colname="col3">Forward scattering (0.1–3 <inline-formula><mml:math id="M375" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M376" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.1</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M377" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> res.)</oasis:entry>
         <oasis:entry colname="col4">Aerosol number distribution function between 0.1 and 3 <inline-formula><mml:math id="M378" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, from which total concentration can be derived</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">AFS/NASA ARC</oasis:entry>
         <oasis:entry colname="col2">Aerosol filter system, collecting various filters for offline analysis (2017–2018)</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">TEM-EDX/SEM-EDX analysis for single particle size, mixing state and elemental composition, bulk BrC, and bulk soluble ions</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PTI/BNL</oasis:entry>
         <oasis:entry colname="col2">2016, 2018: photothermal interferometer (532 nm) <?xmltex \hack{\hfill\break}?>2017–2018: DMT Single Particle Soot Photometer (SP2; eight-channel, refractory black carbon particle mass 80–500 nm, mass equivalent diameter)</oasis:entry>
         <oasis:entry colname="col3">Aerosol light absorption at 532 nm; <?xmltex \hack{\hfill\break}?>refractory black carbon (rBC) particle mass</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">1. Absorption coefficient (M m<inline-formula><mml:math id="M379" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>)</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">2. Refractory black carbon (rBC) mass loading (ng m<inline-formula><mml:math id="M380" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) and number size distributions</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">GIT CCN instrument</oasis:entry>
         <oasis:entry colname="col2">CCN concentrations/spectra at cloud-relevant supersaturation</oasis:entry>
         <oasis:entry colname="col3">CCN concentration (0.15 %–0.6 %) water vapor supersaturation</oasis:entry>
         <oasis:entry colname="col4">CCN spectra, cloud effective supersaturation, aerosol hygroscopicity, droplet growth kinetics</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S2.T14"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{B1}?><?xmltex \def\figurename{Table}?><label>Table B1</label><caption><p id="d1e8353">Continued.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.85}[.85]?><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="4cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="6cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="6cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Instrument name/operating <?xmltex \hack{\hfill\break}?>organization</oasis:entry>
         <oasis:entry colname="col2"><?xmltex \hack{\mbox\bgroup}?>Instrument description<?xmltex \hack{\egroup}?>/key specification</oasis:entry>
         <oasis:entry colname="col3">Primary measurement</oasis:entry>
         <oasis:entry colname="col4">Measurements/<?xmltex \hack{\mbox\bgroup}?>derived quantities<?xmltex \hack{\egroup}?>/inversion products</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="left">Gases in situ </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">COMA/NASA ARC</oasis:entry>
         <oasis:entry colname="col2">Trace gas detector</oasis:entry>
         <oasis:entry colname="col3">In situ measurement of gas-phase CO and <inline-formula><mml:math id="M381" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">1. CO mixing ratio <?xmltex \hack{\hfill\break}?>2. <inline-formula><mml:math id="M382" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> mixing ratio</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">WISPER/OSU water isotopes</oasis:entry>
         <oasis:entry colname="col2">In situ gas-phase cavity ring-down water vapor isotopic analyzers (Picarro model L2120-fi) coupled to isokinetic and CVI inlets.</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">1. Total H<inline-formula><mml:math id="M383" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O mixing ratio, <inline-formula><mml:math id="M384" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">18</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>O, and <inline-formula><mml:math id="M385" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula>D</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">1. Cloud droplet and rain evaporation proportion</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" colname="col3">2. Condensed water content (liquid <inline-formula><mml:math id="M386" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> ice) (g m<inline-formula><mml:math id="M387" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), <inline-formula><mml:math id="M388" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">18</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>O, and <inline-formula><mml:math id="M389" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula>D</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">2. Bulk air mass mixing state and entrainment rate.</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">3. CVI enhancement for residual aerosol</oasis:entry>
         <oasis:entry colname="col4">3. Cloud base and cloud top water mass flux when combined with winds</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="left">Winds </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Vertical winds/NASA Langley</oasis:entry>
         <oasis:entry colname="col2">Vertical winds calculated from five hole flush port radome system/aircraft inertial navigation system</oasis:entry>
         <oasis:entry colname="col3">1. Fast response (20 Hz) vertical winds</oasis:entry>
         <oasis:entry colname="col4">1. If combined with another fast response measurement, can provide vertical fluxes of that species</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S2.T15"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{B2}?><?xmltex \def\figurename{Table}?><label>Table B2</label><caption><p id="d1e8580">ER-2 instruments in ORACLES 2016.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="5cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="5cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Instrument name/operating <?xmltex \hack{\hfill\break}?>organization</oasis:entry>
         <oasis:entry colname="col2"><?xmltex \hack{\mbox\bgroup}?>Instrument description<?xmltex \hack{\egroup}?>/key specification</oasis:entry>
         <oasis:entry colname="col3">Primary measurement</oasis:entry>
         <oasis:entry colname="col4">Measurements/derived quantities</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4" align="left">Remote sensing </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">eMAS (Enhanced MODIS Airborne Simulator)</oasis:entry>
         <oasis:entry colname="col2">38-channel multi-spectral line scanner</oasis:entry>
         <oasis:entry colname="col3">Solar reflective and thermal emissive energy in the 0.46–14 <inline-formula><mml:math id="M392" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> range</oasis:entry>
         <oasis:entry colname="col4">Cloud optical properties (phase, optical thickness, effective radius, and water path); cloud top properties (temperature, pressure, height, and infrared phase)<inline-formula><mml:math id="M393" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula> above-cloud AOD</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">RSP/NASA GISS</oasis:entry>
         <oasis:entry colname="col2">Measurements at 410, 470, 555, 670, 865, 960, 1590, 1880, and 2260 nm with polarimetric accuracy of <inline-formula><mml:math id="M394" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.15</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>
         <oasis:entry colname="col3">Stokes parameters <inline-formula><mml:math id="M395" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M396" display="inline"><mml:mi>Q</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M397" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> of reflected light <?xmltex \hack{\hfill\break}?>Measurements are over <inline-formula><mml:math id="M398" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">60</mml:mn></mml:mrow></mml:math></inline-formula><inline-formula><mml:math id="M399" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> from nadir</oasis:entry>
         <oasis:entry rowsep="1" colname="col4">1. Aerosol microphysics, layer height, and AOD from inversion</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry rowsep="1" colname="col4">2. Water COD, droplet size distribution at top, bulk effective radius, top height, physical thickness, <inline-formula><mml:math id="M400" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">3. Chl, CDOM conc. and backscatter coeff.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">AirMSPI/JPL</oasis:entry>
         <oasis:entry colname="col2">Multiangle radiometric/polarimetric imager with bands centered at 355, 380, 445, 470*, 555, 660*, 865*, and 935 nm (* polarimetric).</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">1. Upwelling radiances (multispectral, multiangle, spatial)</oasis:entry>
         <oasis:entry colname="col4">Liquid cloud droplet effective radius and COD<inline-formula><mml:math id="M401" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?>Aerosol optical depth, particle size distribution, single-scattering albedo, refractive index</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">2. Stokes polarization components (<inline-formula><mml:math id="M402" display="inline"><mml:mi>Q</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M403" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula>) (multispectral, multiangle, spatial)</oasis:entry>
         <oasis:entry colname="col4"/>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">SSFR/ NASA ARC, CU LASP</oasis:entry>
         <oasis:entry colname="col2">Solar Spectral Flux Radiometer (350–2150 nm, spectral sampling 4–8 nm)</oasis:entry>
         <oasis:entry colname="col3">1. Spectral solar irradiance</oasis:entry>
         <oasis:entry colname="col4">1a. TOA aerosol radiative effect (BB only) <?xmltex \hack{\hfill\break}?>1b. Aerosol heating rate (w/P-3, BB only) <?xmltex \hack{\hfill\break}?>1c. TOA cloud-aerosol radiative effect <?xmltex \hack{\hfill\break}?>1d. Scene incident irradiance</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">HSRL-2/NASA LaRC</oasis:entry>
         <oasis:entry colname="col2">Multi-wavelength High Spectral Resolution Lidar</oasis:entry>
         <oasis:entry rowsep="1" colname="col3">Particulate extinction (355, 532 nm)</oasis:entry>
         <oasis:entry colname="col4">Aerosol classification, aerosol mixing layer height (<inline-formula><mml:math id="M404" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> PBL height), AOD <?xmltex \hack{\hfill\break}?>Aerosol microphysics from inversion (e.g., N, S, V concentrations, effective radius)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" colname="col3">Particulate backscatter (355, 532, 1064 nm)</oasis:entry>
         <oasis:entry colname="col4"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">Particulate depolarization (355, 532, 1064 nm)</oasis:entry>
         <oasis:entry colname="col4"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table><table-wrap-foot><p id="d1e8583"><inline-formula><mml:math id="M390" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula> eMAS-derived quantities, along with L1B data, are archived and
publicly available at the LAADS DAAC (<uri>https://ladsweb.modaps.eosdis.nasa.gov/</uri>, last access: December 2020), not the ORACLES archive.<?xmltex \hack{\\}?><inline-formula><mml:math id="M391" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula> RSP-derived quantities are publicly available at
<uri>https://asdc.larc.nasa.gov</uri> (last access: December 2020).</p></table-wrap-foot></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S2.T16"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{B3}?><?xmltex \def\figurename{Table}?><label>Table B3</label><caption><p id="d1e8918">Ground-based observations supported by ORACLES.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="3cm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="3cm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry namest="col1" nameend="col4">Ground-based </oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">AERONET</oasis:entry>
         <oasis:entry colname="col2">Spectral sun and sky ground-based radiometer (340 to 1640 nm)</oasis:entry>
         <oasis:entry colname="col3">1. Direct solar beam transmittance <?xmltex \hack{\hfill\break}?>2. Sky radiance; cloud zenith transmittance</oasis:entry>
         <oasis:entry colname="col4">1. Spectral AOD, column <inline-formula><mml:math id="M405" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?>2. Aerosol microphysics from inversion (e.g., size distribution, refr. index, absorption) <?xmltex \hack{\hfill\break}?>3. Cloud phase, OD, <inline-formula><mml:math id="M406" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi mathvariant="normal">eff</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (inversion)</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?>
</app>

<?pagebreak page1555?><app id="App1.Ch1.S3">
  <?xmltex \currentcnt{C}?><label>Appendix C</label><title>Acknowledgement of all participants</title>

<?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S3.T17"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{C1}?><?xmltex \def\figurename{Table}?><label>Table C1</label><caption><p id="d1e9006">Participants in the ORACLES project, 2014–2019, not co-authoring
this paper.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.98}[.98]?><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Last name</oasis:entry>
         <oasis:entry colname="col2">First middle</oasis:entry>
         <oasis:entry colname="col3">Organization</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Adebiyi</oasis:entry>
         <oasis:entry colname="col2">Adeyemi A.</oasis:entry>
         <oasis:entry colname="col3">University of Miami</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Alexandrov</oasis:entry>
         <oasis:entry colname="col2">Mikhail</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Institute for Space Studies, Columbia University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Allison</oasis:entry>
         <oasis:entry colname="col2">Quincy</oasis:entry>
         <oasis:entry colname="col3">Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Alugodhi</oasis:entry>
         <oasis:entry colname="col2">Mercy-Thea</oasis:entry>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Anderson</oasis:entry>
         <oasis:entry colname="col2">Bruce Eldon</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Arnold</oasis:entry>
         <oasis:entry colname="col2">George Thomas</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center, Science Systems and Applications, Inc.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Barrett</oasis:entry>
         <oasis:entry colname="col2">Paul Alan</oasis:entry>
         <oasis:entry colname="col3">UK Met Office</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Barrick</oasis:entry>
         <oasis:entry colname="col2">John</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Bauer</oasis:entry>
         <oasis:entry colname="col2">Susanne</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Institute for Space Studies, Columbia University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Beach Jr.</oasis:entry>
         <oasis:entry colname="col2">Harry Lee</oasis:entry>
         <oasis:entry colname="col3">AMA Inc</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Bennett</oasis:entry>
         <oasis:entry colname="col2">Joseph Ryan</oasis:entry>
         <oasis:entry colname="col3">National Suborbital Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Biswas</oasis:entry>
         <oasis:entry colname="col2">Sayak Krishna</oasis:entry>
         <oasis:entry colname="col3">Aerospace Corporation, NASA Marshall Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Broccardo</oasis:entry>
         <oasis:entry colname="col2">Stephen Paul</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Cantrell</oasis:entry>
         <oasis:entry colname="col2">Alvin Eric</oasis:entry>
         <oasis:entry colname="col3">NASA Marshall Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Carnes</oasis:entry>
         <oasis:entry colname="col2">Steve Raymond</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Chirica</oasis:entry>
         <oasis:entry colname="col2">Dan C.</oasis:entry>
         <oasis:entry colname="col3">Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Chowdhary</oasis:entry>
         <oasis:entry colname="col2">Jacek</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Institute for Space Studies, Columbia University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Chun</oasis:entry>
         <oasis:entry colname="col2">William</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Clarke</oasis:entry>
         <oasis:entry colname="col2">Antony David</oasis:entry>
         <oasis:entry colname="col3">University of Hawai`i at Mānoa</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Colarco</oasis:entry>
         <oasis:entry colname="col2">Peter Richard</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Cook</oasis:entry>
         <oasis:entry colname="col2">Anthony L</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Dahlgren</oasis:entry>
         <oasis:entry colname="col2">Robert Paul</oasis:entry>
         <oasis:entry colname="col3">California State University, Monterey Bay</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Das</oasis:entry>
         <oasis:entry colname="col2">Sampa</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Delaney Jr.</oasis:entry>
         <oasis:entry colname="col2">Michael McFadyen</oasis:entry>
         <oasis:entry colname="col3">National Suborbital Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Delene</oasis:entry>
         <oasis:entry colname="col2">David</oasis:entry>
         <oasis:entry colname="col3">University of North Dakota</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Dobrowalski</oasis:entry>
         <oasis:entry colname="col2">Gregg Charles</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Dominguez</oasis:entry>
         <oasis:entry colname="col2">Roseanne</oasis:entry>
         <oasis:entry colname="col3">University of California, Santa Cruz</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Drouet</oasis:entry>
         <oasis:entry colname="col2">Jeffrey Thomas</oasis:entry>
         <oasis:entry colname="col3">University of Colorado, Boulder</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Dunagan</oasis:entry>
         <oasis:entry colname="col2">Stephen</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Dunwoody</oasis:entry>
         <oasis:entry colname="col2">Kent Nelson</oasis:entry>
         <oasis:entry colname="col3">NASA Armstrong Flight Research Center, USRA</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Durden</oasis:entry>
         <oasis:entry colname="col2">Stephen L.</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Eck</oasis:entry>
         <oasis:entry colname="col2">Thomas Frank</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ellis</oasis:entry>
         <oasis:entry colname="col2">Thomas Ashly</oasis:entry>
         <oasis:entry colname="col3">University of California, Santa Cruz</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Everson</oasis:entry>
         <oasis:entry colname="col2">Chad Michael</oasis:entry>
         <oasis:entry colname="col3">University of North Dakota</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Fenn</oasis:entry>
         <oasis:entry colname="col2">Marta Angeline</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center, Science Systems and Applications, Inc.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Finch</oasis:entry>
         <oasis:entry colname="col2">Patrick Eugene</oasis:entry>
         <oasis:entry colname="col3">Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Fraim</oasis:entry>
         <oasis:entry colname="col2">Eric</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center, Universities Space Research Association</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Garay</oasis:entry>
         <oasis:entry colname="col2">Michael Joseph</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Garland Jr.</oasis:entry>
         <oasis:entry colname="col2">Rebecca Maureen</oasis:entry>
         <oasis:entry colname="col3">Council for Scientific and Industrial Research</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Geogdzhayev</oasis:entry>
         <oasis:entry colname="col2">Igor</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Institute for Space Studies, Columbia University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Giles</oasis:entry>
         <oasis:entry colname="col2">David Matthew</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center, Science Systems and Applications, Inc.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Grant</oasis:entry>
         <oasis:entry colname="col2">Patrick Steven</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center, University of California, Santa Cruz</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Gray</oasis:entry>
         <oasis:entry colname="col2">Ellen Theresa</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Hambloch</oasis:entry>
         <oasis:entry colname="col2">Patrick</oasis:entry>
         <oasis:entry colname="col3">University of Alabama in Huntsville</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Harper</oasis:entry>
         <oasis:entry colname="col2">David B.</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Heikkila</oasis:entry>
         <oasis:entry colname="col2">Ashley Creta</oasis:entry>
         <oasis:entry colname="col3">University of Hawai`i at Mānoa</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Henze</oasis:entry>
         <oasis:entry colname="col2">Dean</oasis:entry>
         <oasis:entry colname="col3">Oregon State University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Hildum</oasis:entry>
         <oasis:entry colname="col2">Edward Ames</oasis:entry>
         <oasis:entry colname="col3">Universities Space Research Association</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Howes</oasis:entry>
         <oasis:entry colname="col2">Calvin Tucker</oasis:entry>
         <oasis:entry colname="col3">University of California, Los Angeles</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ibrahim</oasis:entry>
         <oasis:entry colname="col2">Hani Halim</oasis:entry>
         <oasis:entry colname="col3">SpecTIR LLC</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">James</oasis:entry>
         <oasis:entry colname="col2">Mark W.</oasis:entry>
         <oasis:entry colname="col3">NASA Marshall Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Johnson</oasis:entry>
         <oasis:entry colname="col2">Roy Robert</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Johnson</oasis:entry>
         <oasis:entry colname="col2">Matthew</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?><?xmltex \floatpos{h!}?><table-wrap id="App1.Ch1.S3.T18"><?xmltex \hack{\hsize\textwidth}?><?xmltex \currentcnt{C1}?><?xmltex \def\figurename{Table}?><label>Table C1</label><caption><p id="d1e9686">Continued.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Last name</oasis:entry>
         <oasis:entry colname="col2">First middle</oasis:entry>
         <oasis:entry colname="col3">Organization</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Jordan</oasis:entry>
         <oasis:entry colname="col2">David Everet</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kangueehi</oasis:entry>
         <oasis:entry colname="col2">Ismael</oasis:entry>
         <oasis:entry colname="col3">Stellenbosch University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Karol</oasis:entry>
         <oasis:entry colname="col2">Yana</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kindel</oasis:entry>
         <oasis:entry colname="col2">Bruce</oasis:entry>
         <oasis:entry colname="col3">University of Colorado, Boulder</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kittelman</oasis:entry>
         <oasis:entry colname="col2">Alan Scott</oasis:entry>
         <oasis:entry colname="col3">University of Colorado, Boulder</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Kraft</oasis:entry>
         <oasis:entry colname="col2">Jason Michael</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Klopper</oasis:entry>
         <oasis:entry colname="col2">Danitza</oasis:entry>
         <oasis:entry colname="col3">North-West University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Lebsock</oasis:entry>
         <oasis:entry colname="col2">Matthew David</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Lee</oasis:entry>
         <oasis:entry colname="col2">Joseph William</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Lightbourn</oasis:entry>
         <oasis:entry colname="col2">Frank</oasis:entry>
         <oasis:entry colname="col3">NASA Armstrong (Dryden) Flight Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Mace Jr.</oasis:entry>
         <oasis:entry colname="col2">Gerald Grant</oasis:entry>
         <oasis:entry colname="col3">University of Utah</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Yang Martin</oasis:entry>
         <oasis:entry colname="col2">Meiying Melissa</oasis:entry>
         <oasis:entry colname="col3">National Suborbital Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">McFadden</oasis:entry>
         <oasis:entry colname="col2">Susan Kimi</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center, Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">McIlhattan</oasis:entry>
         <oasis:entry colname="col2">Elin Arwen</oasis:entry>
         <oasis:entry colname="col3">University of Wisconsin–Madison</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Miller</oasis:entry>
         <oasis:entry colname="col2">Rose Marie</oasis:entry>
         <oasis:entry colname="col3">University of Illinois at Urbana–Champaign</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Miller</oasis:entry>
         <oasis:entry colname="col2">Daniel John</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center/UMBC Joint Center for Earth Systems Technology</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Mohrmann</oasis:entry>
         <oasis:entry colname="col2">Johannes</oasis:entry>
         <oasis:entry colname="col3">University of Washington</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Nathanael</oasis:entry>
         <oasis:entry colname="col2">Benjamin</oasis:entry>
         <oasis:entry colname="col3">National Commission on Research, Science and Technology (Namibia)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Nghiyalwa</oasis:entry>
         <oasis:entry colname="col2">Hilma</oasis:entry>
         <oasis:entry colname="col3">Geography Department, University of Namibia</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Nicholas</oasis:entry>
         <oasis:entry colname="col2">Sommer Lynne</oasis:entry>
         <oasis:entry colname="col3">Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Olson</oasis:entry>
         <oasis:entry colname="col2">Jennifer</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ottaviani</oasis:entry>
         <oasis:entry colname="col2">Matteo</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Institute for Space Studies, Terra Research Inc</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Purdue</oasis:entry>
         <oasis:entry colname="col2">Sara Kisa</oasis:entry>
         <oasis:entry colname="col3">University of Miami</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Quigley</oasis:entry>
         <oasis:entry colname="col2">Emmett</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Rheingans</oasis:entry>
         <oasis:entry colname="col2">Brian Eugene</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Rodriguez Monje</oasis:entry>
         <oasis:entry colname="col2">Raquel</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Schafer</oasis:entry>
         <oasis:entry colname="col2">Joel Shannon</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Schaller</oasis:entry>
         <oasis:entry colname="col2">Emily Lauren</oasis:entry>
         <oasis:entry colname="col3">National Suborbital Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Seidel Caprez</oasis:entry>
         <oasis:entry colname="col2">Felix Clemens</oasis:entry>
         <oasis:entry colname="col3">NASA Headquarters, now JPL</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Shimhanda</oasis:entry>
         <oasis:entry colname="col2">Senior</oasis:entry>
         <oasis:entry colname="col3">Kiyushu Institute of Technology, Japan</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Shingler</oasis:entry>
         <oasis:entry colname="col2">Taylor</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center, Science Systems and Applications, Inc.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Shipepe</oasis:entry>
         <oasis:entry colname="col2">David Michael</oasis:entry>
         <oasis:entry colname="col3">Namibia University of Science and Technology</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Simmons</oasis:entry>
         <oasis:entry colname="col2">David Earl</oasis:entry>
         <oasis:entry colname="col3">University of Alabama in Huntsville</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sims</oasis:entry>
         <oasis:entry colname="col2">W. Herb</oasis:entry>
         <oasis:entry colname="col3">University of Alabama in Huntsville</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sinclair</oasis:entry>
         <oasis:entry colname="col2">Kenneth Allan</oasis:entry>
         <oasis:entry colname="col3">Columbia University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sinyuk III</oasis:entry>
         <oasis:entry colname="col2">Aliaksandr</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Slutsker</oasis:entry>
         <oasis:entry colname="col2">Ilya</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Smirnov</oasis:entry>
         <oasis:entry colname="col2">Alexander</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center, Science Systems and Applications, Inc.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Smirnow</oasis:entry>
         <oasis:entry colname="col2">Nikolai Brown</oasis:entry>
         <oasis:entry colname="col3">University of Hawai`i at Mānoa</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Sorokin</oasis:entry>
         <oasis:entry colname="col2">Mikhail Grigorievich</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Space Flight Center, Science Systems and Applications, Inc.</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Stamnes</oasis:entry>
         <oasis:entry colname="col2">Snorre</oasis:entry>
         <oasis:entry colname="col3">NASA Langley Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Swap</oasis:entry>
         <oasis:entry colname="col2">Robert John</oasis:entry>
         <oasis:entry colname="col3">University of Virginia, NASA Headquarters</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Tan</oasis:entry>
         <oasis:entry colname="col2">Qian</oasis:entry>
         <oasis:entry colname="col3">Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Thompson</oasis:entry>
         <oasis:entry colname="col2">Andrew</oasis:entry>
         <oasis:entry colname="col3">Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Tosca</oasis:entry>
         <oasis:entry colname="col2">Mika</oasis:entry>
         <oasis:entry colname="col3">School of the Art Institute of Chicago</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">van Diedenhoven</oasis:entry>
         <oasis:entry colname="col2">Bastiaan</oasis:entry>
         <oasis:entry colname="col3">NASA Goddard Institute for Space Studies, Columbia University</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Van Gilst</oasis:entry>
         <oasis:entry colname="col2">David Patrick</oasis:entry>
         <oasis:entry colname="col3">National Suborbital Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">van Harten</oasis:entry>
         <oasis:entry colname="col2">Gerrit</oasis:entry>
         <oasis:entry colname="col3">Jet Propulsion Laboratory</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Vasques</oasis:entry>
         <oasis:entry colname="col2">Marilyn</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Wasilewski</oasis:entry>
         <oasis:entry colname="col2">Andrzej Piotr</oasis:entry>
         <oasis:entry colname="col3">SciSpace, NASA Goddard Institute for Space Studies</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Williams</oasis:entry>
         <oasis:entry colname="col2">Brent Allan</oasis:entry>
         <oasis:entry colname="col3">Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Winchester</oasis:entry>
         <oasis:entry colname="col2">Cody</oasis:entry>
         <oasis:entry colname="col3">University of Hawai`i at Mānoa</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Xu</oasis:entry>
         <oasis:entry colname="col2">Feng</oasis:entry>
         <oasis:entry colname="col3">JPL, now University of Oklahoma</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Yates</oasis:entry>
         <oasis:entry colname="col2">Brian Avery</oasis:entry>
         <oasis:entry colname="col3">NASA GSFC Wallops Flight Facility, Pinnacle/AMOC</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Zavaleta</oasis:entry>
         <oasis:entry colname="col2">Jhony Ronald</oasis:entry>
         <oasis:entry colname="col3">NASA Ames Research Center</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Zhang</oasis:entry>
         <oasis:entry colname="col2">Jianhao</oasis:entry>
         <oasis:entry colname="col3">University of Miami</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Zhang</oasis:entry>
         <oasis:entry colname="col2">Qin</oasis:entry>
         <oasis:entry colname="col3">Bay Area Environmental Research Institute</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \hack{\clearpage}?>
</app>
  </app-group><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e10417">All ORACLES data are accessible via the digital object identifiers (DOIs) provided under ORACLES Science Team (2020a–d) references: <ext-link xlink:href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2018_V2" ext-link-type="DOI">10.5067/Suborbital/ORACLES/P3/2018_V2</ext-link> (ORACLES Science Team, 2020a), <ext-link xlink:href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2017_V2" ext-link-type="DOI">10.5067/Suborbital/ORACLES/P3/2017_V2</ext-link> (ORACLES Science Team, 2020b), <ext-link xlink:href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2016_V2" ext-link-type="DOI">10.5067/Suborbital/ORACLES/P3/2016_V2</ext-link> (ORACLES Science Team, 2020c), and <ext-link xlink:href="https://doi.org/10.5067/Suborbital/ORACLES/ER2/2016_V2" ext-link-type="DOI">10.5067/Suborbital/ORACLES/ER2/2016_V2</ext-link> (ORACLES Science Team, 2020d). The only exceptions are noted as footnotes to Table B2.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e10435">JR, RW, and PZ, designed the original ORACLES observational concept and
co-led the 5-year investigation. SJD was instrumental in conducting the
ORACLES investigation. BL coordinated all project management. JMH and PF led
the CLARIFY and AEROCLO-sA field experiments, respectively, and their
coordination with ORACLES deployments. SEL, MSD, YS, RU, JMR, AND, AMdS,
KML, MSK, CJF, KP, ASA, SEB, AMF, GRC, PES, GAF, SF, BC, BNH, KDK, ST, TSL,
AMD, OOS, GMM, MRP, SG, JRO, AN, MK, JPSW, JDSG, KLT, DN, JRP, KSS, PP, HC,
SPC, AJS, TJL, ES, MSR, RAF, SPB, CAH, DJD, FCS, SEP, JSM, KGM, and DAS made
critical contributions to the field deployments and post-campaign data
analyses. SGH made vital contributions to the experimental design and
execution. MM and PS led formal modeling analyses in the post-campaign
stage. NMK and SJP coordinated the outreach and scientific efforts by
Namibian and South African partner institutions. IYC and LG created and
visualized results for portions of this paper. HM provided
crucial administrative support to enable ORACLES field operations.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e10441">Paquita Zuidema, Paola Formenti, and James M. Haywood are guest editors for the ACP Special Issue “New
observations and related modeling studies of the aerosol–cloud–climate
system in the Southeast Atlantic and southern Africa regions”, to which this
paper has been submitted. The remaining authors declare that they have no
conflicts of interest.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e10447">This article is part of the special issue “New observations and related modeling studies of the aerosol–cloud–climate system in the Southeast Atlantic and southern Africa regions (ACP/AMT inter-journal SI)”. It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e10453">ORACLES is a NASA Earth Venture Suborbital-2 investigation managed through the Earth System Science Pathfinder Office. The team is equally grateful for the tireless
contributions by the NASA Wallops and NASA Johnson P-3 and NASA Armstrong
ER-2 pilots, flight crews, and their management, as well as air traffic
control at Walvis Bay airport (Namibia) and the airport in São Tomé.
Local authorities in Namibia and São Tomé beyond the ones mentioned
in Sect. 3.3.7 and 3.5 played important roles as well, for which the project
would like to express their gratitude. Philip Stier acknowledges funding from the UK
NERC project CLARIFY (NE/L013479/1) and the European Research Council (ERC)
project RECAP under the European Union's Horizon 2020 research and
innovation program with grant agreement 724602. Part of this work was
performed at the Jet Propulsion Laboratory, California Institute of
Technology, under a contract with the National Aeronautics and Space
Administration (80NM0018D0004).</p><p id="d1e10455">The ORACLES project, in spirit and execution, was very much a collaborative
effort. It entailed contributions small and large, with many of the smaller
and short-term contributions equally crucial to the execution of the
project. In Table C1 in Appendix C we list all participants in the ORACLES
project that are not co-authors of this paper. The ORACLES leadership, and
indeed NASA as a whole, owe sincere gratitude to any and all of the
participants listed there.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e10460">This research has been supported by NASA through the Earth Venture Suborbital-2 (EVS-2) program (grant no. 13-EVS2-13-0028).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e10467">This paper was edited by Frank Eckardt and reviewed by Armin Sorooshian and one anonymous referee.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bib1"><label>1</label><?label 1?><mixed-citation>
Ackerman, A. S., Toon, O. B., Stevens, D. E., Heymsfield, A. J., Ramanathan,
V., and Welton, E. J.: Reduction of tropical cloudiness by soot, Science,
288, 1042–1047, 2000.</mixed-citation></ref>
      <ref id="bib1.bib2"><label>2</label><?label 1?><mixed-citation>Ackerman, A. S., Kirkpatrick, M. P., Stevens, D. E., and Toon, O. B.: The impact of humidity above stratiform clouds on indirect aerosol climate forcing, Nature, 432, 1014–1017, <ext-link xlink:href="https://doi.org/10.1038/nature03174" ext-link-type="DOI">10.1038/nature03174</ext-link>, 2004.</mixed-citation></ref>
      <ref id="bib1.bib3"><label>3</label><?label 1?><mixed-citation>Adebiyi, A. and Zuidema, P.: The Role of the Southern African Easterly Jet
in Modifying the Southeast Atlantic Aerosol and Cloud Environments,
Q. J. Roy. Meteor. Soc., 697, 1574–89,
<ext-link xlink:href="https://doi.org/10.1002/qj.2765" ext-link-type="DOI">10.1002/qj.2765</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib4"><label>4</label><?label 1?><mixed-citation>
Adebiyi, A. A. and Zuidema, P.: Low Cloud Cover Sensitivity to
Biomass-Burning Aerosols and Meteorology over the Southeast Atlantic,
J. Climate, 31, 4329–4346, 2018.</mixed-citation></ref>
      <ref id="bib1.bib5"><label>5</label><?label 1?><mixed-citation>Adebiyi, A., Zuidema, P., and Abel, S.: The convolution of dynamics and
moisture with the presence of shortwave absorbing aerosols over the
southeast Atlantic, J. Climate, 28, 1997–2024,
<ext-link xlink:href="https://doi.org/10.1175/JCLI-D-14-00352.1" ext-link-type="DOI">10.1175/JCLI-D-14-00352.1</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib6"><label>6</label><?label 1?><mixed-citation>Adebiyi, A. A., Zuidema, P., Chang, I., Burton, S. P., and Cairns, B.: Mid-level clouds are frequent above the southeast Atlantic stratocumulus clouds, Atmos. Chem. Phys., 20, 11025–11043, <ext-link xlink:href="https://doi.org/10.5194/acp-20-11025-2020" ext-link-type="DOI">10.5194/acp-20-11025-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib7"><label>7</label><?label 1?><mixed-citation>
Albrecht, B. A.: Aerosols, cloud microphysics, and fractional cloudiness,
Science, 245, 1227–1230, 1989.</mixed-citation></ref>
      <ref id="bib1.bib8"><label>8</label><?label 1?><mixed-citation>
Andela, N., Morton, D. C., Giglio, L., Chen, Y., van der Werf, G. R., Kasibhatla, P. S., DeFries, R. S., Collatz, G. L., Hantson, S., Kloster, S., Bachelet, D., Forrest, M., Lasslop, G., Li, F., Mangeon, S., Melton, J. R., Yue, C., and Randerson, J. T.: A human-driven decline in global burned area, Science, 356,
1356–1362, 2017.</mixed-citation></ref>
      <ref id="bib1.bib9"><label>9</label><?label 1?><mixed-citation>
Annegarn, H. J. and Swap, R. J.: SAFARI 2000: A Southern African Example of
Science Diplomacy, Science and Diplomacy, 1, 4,
2012.</mixed-citation></ref>
      <ref id="bib1.bib10"><label>10</label><?label 1?><mixed-citation>Bennartz, R. and Rausch, J.: Global and regional estimates of warm cloud droplet number concentration based on 13 years of AQUA-MODIS observations, Atmos. Chem. Phys., 17, 9815–9836, <ext-link xlink:href="https://doi.org/10.5194/acp-17-9815-2017" ext-link-type="DOI">10.5194/acp-17-9815-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib11"><label>11</label><?label 1?><mixed-citation>Betts, A. K. and Ridgway, W.: Coupling of the Radiative, Convective, and
Surface Fluxes over the Equatorial Pacific, J. Atmos.
Sci., 45, 522–36, <ext-link xlink:href="https://doi.org/10.1175/1520-0469(1988)045%3C0522:COTRCA%3E2.0.CO;2" ext-link-type="DOI">10.1175/1520-0469(1988)045%3C0522:COTRCA%3E2.0.CO;2</ext-link>, 1988.</mixed-citation></ref>
      <ref id="bib1.bib12"><label>12</label><?label 1?><mixed-citation>Bond, T. C., Doherty, S. J., Fahey, D. W., Forster, P. M.  Berntsen, T., DeAngelo,  B. J.,  Flanner, M. G.,  Ghan, S., Kärcher, B., Koch, D., Kinne, S., Kondo, Y.,  Quinn, P. K., Sarofim, M. C.,  Schultz, M. G.,  Schulz, M., Venkataraman, C., Zhang, H., Zhang S., Bellouin, N., Guttikunda, S. K.,  Hopke, P. K., Jacobson, M. Z., Kaiser, J. W.,  Klimont, Z., Lohmann,  U.,  Schwarz, J. P., Shindell, D., Storelvmo, T., Warren, S. G., and  Zender, C. S.: Bounding the role of black carbon in the climate
system: A scientific assessment, J. Geophys. Res.-Atmos., 118, 5380–5552,
<ext-link xlink:href="https://doi.org/10.1002/jgrd.50171" ext-link-type="DOI">10.1002/jgrd.50171</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib13"><label>13</label><?label 1?><mixed-citation>Bony, S. and Dufresne, J. L.: Marine boundary layer clouds at the heart of
tropical cloud feedback uncertainties in climate models, Geophys. Res.
Lett., 32, L20806, <ext-link xlink:href="https://doi.org/10.1029/2005GL023851" ext-link-type="DOI">10.1029/2005GL023851</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bib14"><label>14</label><?label 1?><mixed-citation>Burton, S., Hostetler, C., Cook, A., Hair, J., Seaman, S., Scola, S.,
Harper, D., Smith, J., Fenn, M., Ferrare, R., Saide, P. E., Chemyakin, E. V., and Müller, D.: Calibration of
a high spectral resolution lidar using a Michelson interferometer, with data
examples from ORACLES, Appl. Optics, 57, 6061, <ext-link xlink:href="https://doi.org/10.1364/AO.57.006061" ext-link-type="DOI">10.1364/AO.57.006061</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib15"><label>15</label><?label 1?><mixed-citation>
Chand, D., Wood, R., Anderson, T., Satheesh, S. K., and Charlson, R. J.:
Satellite-derived direct radiative effect of aerosols dependent on cloud
cover, Nat. Geosci., 2, 181–184, 2009.</mixed-citation></ref>
      <ref id="bib1.bib16"><label>16</label><?label 1?><mixed-citation>Chatfield, R. B., Guo, Z., Sachse, G. W., Blake, D. R., and Blake, N. J.:
The subtropical global plume in the Pacific Exploratory Mission-Tropics A
(PEM-Tropics A), PEM-Tropics B, and the Global Atmospheric Sampling Program
(GASP): How tropical emissions affect the remote Pacific, J. Geophys. Res., 107,
4278, <ext-link xlink:href="https://doi.org/10.1029/2001JD000497" ext-link-type="DOI">10.1029/2001JD000497</ext-link>, 2002.</mixed-citation></ref>
      <ref id="bib1.bib17"><label>17</label><?label 1?><mixed-citation>
Coakley, J. and Chylek, P.: The two-stream approximation in radiative
transfer including the angle of the incident radiation, J. Atmos. Sci., 32,
409–418, 1975.</mixed-citation></ref>
      <ref id="bib1.bib18"><label>18</label><?label 1?><mixed-citation>Cochrane, S. P., Schmidt, K. S., Chen, H., Pilewskie, P., Kittelman, S., Redemann, J., LeBlanc, S., Pistone, K., Kacenelenbogen, M., Segal Rozenhaimer, M., Shinozuka, Y., Flynn, C., Platnick, S., Meyer, K., Ferrare, R., Burton, S., Hostetler, C., Howell, S., Freitag, S., Dobracki, A., and Doherty, S.: Above-cloud aerosol radiative effects based on ORACLES 2016 and ORACLES 2017 aircraft experiments, Atmos. Meas. Tech., 12, 6505–6528, <ext-link xlink:href="https://doi.org/10.5194/amt-12-6505-2019" ext-link-type="DOI">10.5194/amt-12-6505-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib19"><label>19</label><?label 1?><mixed-citation>Coddington, O. M., Pilewskie, P., Redemann, J., Platnick, S., Russell, S. P. B.,
Schmidt, K. S., Gore, W. J., Livingston, J., Wind, G., and Vukicevic, T.:
Examining the impact of overlying aerosols on the retrieval of cloud optical
properties from passive remote sensing, J. Geophys. Res., 115, D10211,
<ext-link xlink:href="https://doi.org/10.1029/2009JD012829" ext-link-type="DOI">10.1029/2009JD012829</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib20"><label>20</label><?label 1?><mixed-citation>Costantino, L. and Bréon, F.-M.: Satellite-based estimate of aerosol direct radiative effect over the South-East Atlantic, Atmos. Chem. Phys. Discuss., 13, 23295–23324, <ext-link xlink:href="https://doi.org/10.5194/acpd-13-23295-2013" ext-link-type="DOI">10.5194/acpd-13-23295-2013</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib21"><label>21</label><?label 1?><mixed-citation>Das, S., Harshvardhan, H., Bian, H., Chin, M., Curci, G., Protonotariou, A.
P. T., Mielonen, K., Zhang, H., Wang, H., and Liu, X.: Biomass burning aerosol
transport and vertical distribution over the South African-Atlantic region,
J. Geophys. Res.-Atmos., 122, 6391–6415, <ext-link xlink:href="https://doi.org/10.1002/2016JD026421" ext-link-type="DOI">10.1002/2016JD026421</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib22"><label>22</label><?label 1?><mixed-citation>Davies, N. W., Fox, C., Szpek, K., Cotterell, M. I., Taylor, J. W., Allan, J. D., Williams, P. I., Trembath, J., Haywood, J. M., and Langridge, J. M.: Evaluating biases in filter-based aerosol absorption measurements using photoacoustic spectroscopy, Atmos. Meas. Tech., 12, 3417–3434, <ext-link xlink:href="https://doi.org/10.5194/amt-12-3417-2019" ext-link-type="DOI">10.5194/amt-12-3417-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib23"><label>23</label><?label 1?><mixed-citation>Deaconu, L. T., Waquet, F., Josset, D., Ferlay, N., Peers, F., Thieuleux, F., Ducos, F., Pascal, N., Tanré, D., Pelon, J., and Goloub, P.: Consistency of aerosols above clouds characterization from A-Train active and passive measurements, Atmos. Meas. Tech., 10, 3499–3523, <ext-link xlink:href="https://doi.org/10.5194/amt-10-3499-2017" ext-link-type="DOI">10.5194/amt-10-3499-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib24"><label>24</label><?label 1?><mixed-citation>Deaconu, L. T., Ferlay, N., Waquet, F., Peers, F., Thieuleux, F., and Goloub, P.: Satellite inference of water vapour and above-cloud aerosol combined effect on radiative budget and cloud-top processes in the southeastern Atlantic Ocean, Atmos. Chem. Phys., 19, 11613–11634, <ext-link xlink:href="https://doi.org/10.5194/acp-19-11613-2019" ext-link-type="DOI">10.5194/acp-19-11613-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib25"><label>25</label><?label 1?><mixed-citation>De Graaf, M., Bellouin, N., Tilstra, L. G., Haywood, J., and Stammes, P.:
Aerosol direct radiative effect of smoke over clouds over the southeast
Atlantic Ocean from 2006 to 2009, Geophys. Res. Lett., 41, 7723–7730,
<ext-link xlink:href="https://doi.org/10.1002/2014GL061103" ext-link-type="DOI">10.1002/2014GL061103</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib26"><label>26</label><?label 1?><mixed-citation>Diamond, M. S., Dobracki, A., Freitag, S., Small Griswold, J. D., Heikkila, A., Howell, S. G., Kacarab, M. E., Podolske, J. R., Saide, P. E., and Wood, R.: Time-dependent entrainment of smoke presents an observational challenge for assessing aerosol–cloud interactions over the southeast Atlantic Ocean, Atmos. Chem. Phys., 18, 14623–14636, <ext-link xlink:href="https://doi.org/10.5194/acp-18-14623-2018" ext-link-type="DOI">10.5194/acp-18-14623-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib27"><label>27</label><?label 1?><mixed-citation>
Doherty, S. J., Saide, P., Zuidema, P., Shinozuka, Y., Ferrada, G., Mallet, M., Meyer, K., Painemal, D., Howell, S. G., Freitag, S., Smirnow, N.,Dobracki, A., Podolske, J., Ferrare, R., Burton, S., Nabat, P., Wood, R., and Redemann, J.: Modeled and observed vertically-resolved aerosol and cloud properties related to the direct aerosol radiative effect in the Southeast Atlantic, in preparation, 2021.</mixed-citation></ref>
      <ref id="bib1.bib28"><label>28</label><?label 1?><mixed-citation>
Dubovik, O. and King, M. D.: A flexible inversion algorithm for retrieval
of aerosol optical properties from sun and sky radiance measurements, J.
Geophys. Res., 105, 20673–20696, 2000.</mixed-citation></ref>
      <ref id="bib1.bib29"><label>29</label><?label 1?><mixed-citation>Dzambo, A. M., L'Ecuyer, T., Sy, O. O., and Tanelli, S.: The Observed
Structure and Precipitation Characteristics of Southeast Atlantic
Stratocumulus from Airborne Radar During ORACLES 2016-17, J. Appl.
Meteorol. Clim., 58, 2197–2215, <ext-link xlink:href="https://doi.org/10.1175/jamc-d-19-0032.1" ext-link-type="DOI">10.1175/jamc-d-19-0032.1</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib30"><label>30</label><?label 1?><mixed-citation>Dzambo, A. M., L'Ecuyer, T., Sinclair, K., van Diedenhoven, B., Gupta, S., McFarquhar, G., O'Brien, J. R., Cairns, B., Wasilewski, A. P., and Alexandrov, M.: Joint Cloud Water Path and Rain Water Path Retrievals from ORACLES Observations, Atmos. Chem. Phys. Discuss., <ext-link xlink:href="https://doi.org/10.5194/acp-2020-849" ext-link-type="DOI">10.5194/acp-2020-849</ext-link>, in review, 2020.</mixed-citation></ref>
      <?pagebreak page1559?><ref id="bib1.bib31"><label>31</label><?label 1?><mixed-citation>Eastman, R. and Wood, R. K. T. O: The subtropical stratocumulus-topped
planetary boundary layer: A climatology and the Lagrangian evolution, J.
Atmos. Sci., 74, 2633–2656, <ext-link xlink:href="https://doi.org/10.1175/JAS-D-16-0336.1" ext-link-type="DOI">10.1175/JAS-D-16-0336.1</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib32"><label>32</label><?label 1?><mixed-citation>Eck, T. F., Holben, B. N., Reid, J. S., Mukelabai, M. M., Piketh, S. J., Torres, O., Jethva, H. T., Hyer, E. J.,  Ward, D. E., Dubovik, O., Sinyuk, A., Schafer,  J. S.,  Giles, D. M., Sorokin, M., Smirnov, A., and Slutsker, I.: A seasonal trend of single scattering albedo in southern
African biomass-burning particles: Implications for satellite products and
estimates of emissions for the world's largest biomass-burning source, J.
Geophys. Res. Atmos., 118, 6414–6432, <ext-link xlink:href="https://doi.org/10.1002/jgrd.50500" ext-link-type="DOI">10.1002/jgrd.50500</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib33"><label>33</label><?label 1?><mixed-citation>ECMWF: Describing ECMWF's forecasts and forecasting system,
Newsletter Feature Article, ECMWF, availabel at:
<uri>https://www.ecmwf.int/sites/default/files/elibrary/2012/17412-describing-ecmwfs-forecasts-and-forecasting-system.pdf</uri>
(last access: December 2013),
2012.</mixed-citation></ref>
      <ref id="bib1.bib34"><label>34</label><?label 1?><mixed-citation>
Fishman, J., Hoell, J. M., Bendura, R. D., McNeal, R. J., and Kirchhoff, V.
W. J. H.: NASA GTE TRACE-A Experiment (September–October 1992), Overview,
J. Geophys. Res., 101, 23865–23880, 1996.</mixed-citation></ref>
      <ref id="bib1.bib35"><label>35</label><?label 1?><mixed-citation>Formenti, P., D'Anna, B., Flamant, C., Mallet, M., Piketh, S. J., Schepanski, K., Waquet, F., Auriol, F., Brogniez, G., Burnet, F., Chaboureau, J., Chauvigné, A., Chazette, P., Denjean, C., Desboeufs, K., Doussin, J., Elguindi, N., Feuerstein, S., Gaetani, M., Giorio, C., Klopper, D., Mallet, M. D., Nabat, P., Monod, A., Solmon, F., Namwoonde, A., Chikwililwa, C., Mushi, R., Welton, E. J., and Holben, B.: The Aerosols, Radiation and Clouds in Southern Africa
Field Campaign in Namibia: Overview, illustrative observations, and way
forward, B. Am. Meteor. Soc., 100, 1277–1298, <ext-link xlink:href="https://doi.org/10.1175/BAMS-D-17-0278.1" ext-link-type="DOI">10.1175/BAMS-D-17-0278.1</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib36"><label>36</label><?label 1?><mixed-citation>Grell, G. A., Peckham, S. E., Schmitz, R., McKeen, S. A., Frost, G., Skamarock,
W. C., and Eder, B.: Fully coupled “online” chemistry within the WRF model, Atmos. Environ., 39, 6957–6975, <ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2005.04.027" ext-link-type="DOI">10.1016/j.atmosenv.2005.04.027</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bib37"><label>37</label><?label 1?><mixed-citation>Gupta, S., McFarquhar, G. M., O'Brien, J. R., Delene, D. J., Poellot, M. R., Dobracki, A., Podolske, J. R., Redemann, J., LeBlanc, S. E., Segal-Rozenhaimer, M., and Pistone, K.: Impact of the Variability in Vertical Separation between Biomass-Burning Aerosols and Marine Stratocumulus on Cloud Microphysical Properties over the Southeast Atlantic, Atmos. Chem. Phys. Discuss. [preprint], <ext-link xlink:href="https://doi.org/10.5194/acp-2020-1039" ext-link-type="DOI">10.5194/acp-2020-1039</ext-link>, in review, 2020.</mixed-citation></ref>
      <ref id="bib1.bib38"><label>38</label><?label 1?><mixed-citation>Haynes, J. M., L'Ecuyer, T. S., Stephens, G. L., Miller, S. D., Mitrescu, C., Wood, N. B., and Tanelli, S.: Rainfall retrieval over the ocean with spaceborne W‐band radar, J. Geophys. Res., 114, D00A22, <ext-link xlink:href="https://doi.org/10.1029/2008JD009973" ext-link-type="DOI">10.1029/2008JD009973</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib39"><label>39</label><?label 1?><mixed-citation>Haywood, J., Francis, P., Dubovik, O., Glew, M., and Holben, B.: Comparison
of aerosol size distributions, radiative properties, and optical depths
determined by aircraft observations and Sun photometers during SAFARI 2000,
J. Geophys. Res., 108, 8471, <ext-link xlink:href="https://doi.org/10.1029/2002JD002250" ext-link-type="DOI">10.1029/2002JD002250</ext-link>, 2003.</mixed-citation></ref>
      <ref id="bib1.bib40"><label>40</label><?label 1?><mixed-citation>
Haywood, J. M., Osborne, S. R., and Abel, S. J.: The effect of overlying
absorbing aerosol layers on remote sensing retrievals of cloud effective
radius and cloud optical depth, Q. J. Roy. Meteor. Soc., 130, 779–800, 2004.</mixed-citation></ref>
      <ref id="bib1.bib41"><label>41</label><?label 1?><mixed-citation>Haywood, J. M., Abel, S. J., Barrett, P. A., Bellouin, N., Blyth, A., Bower, K. N., Brooks, M., Carslaw, K., Che, H., Coe, H., Cotterell, M. I., Crawford, I., Cui, Z., Davies, N., Dingley, B., Field, P., Formenti, P., Gordon, H., de Graaf, M., Herbert, R., Johnson, B., Jones, A. C., Langridge, J. M., Malavelle, F., Partridge, D. G., Peers, F., Redemann, J., Stier, P., Szpek, K., Taylor, J. W., Watson-Parris, D., Wood, R., Wu, H., and Zuidema, P.: Overview: The CLoud-Aerosol-Radiation Interaction and Forcing: Year-2017 (CLARIFY-2017) measurement campaign, Atmos. Chem. Phys. Discuss., <ext-link xlink:href="https://doi.org/10.5194/acp-2020-729" ext-link-type="DOI">10.5194/acp-2020-729</ext-link>, in review, 2020.</mixed-citation></ref>
      <ref id="bib1.bib42"><label>42</label><?label 1?><mixed-citation>Herman, J., Cede, A., Spinei, E., Mount, G., Tzortziou, M., and Abuhassan,
N.: NO<inline-formula><mml:math id="M407" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> column amounts from ground-based Pandora and MFDOAS spectrometers
using the direct-sun DOAS technique: Intercomparisons and application to
OMIvalidation, J. Geophys. Res., 114, D13307, <ext-link xlink:href="https://doi.org/10.1029/2009JD011848" ext-link-type="DOI">10.1029/2009JD011848</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib43"><label>43</label><?label 1?><mixed-citation>Herman, J., Evans, R., Cede, A., Abuhassan, N., Petropavlovskikh, I., and McConville, G.: Comparison of ozone retrievals from the Pandora spectrometer system and Dobson spectrophotometer in Boulder, Colorado, Atmos. Meas. Tech., 8, 3407–3418, <ext-link xlink:href="https://doi.org/10.5194/amt-8-3407-2015" ext-link-type="DOI">10.5194/amt-8-3407-2015</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib44"><label>44</label><?label 1?><mixed-citation>
Holben, B. N., Eck, T. F., Slutsker, I., Tanre, D., Buis, J. P., Setzer, A.,
Vermote, E., Reagan, J. A., Kaufman, Y., Nakajima, T., Lavenu, F.,
Jankowiak, I., and Smirnov, A.: AERONET – A federated instrument network
and data archive for aerosol characterization, Remote Sens. Environ., 66,
1–16, 1998.</mixed-citation></ref>
      <ref id="bib1.bib45"><label>45</label><?label 1?><mixed-citation>Holben, B. N., Kim, J., Sano, I., Mukai, S., Eck, T. F., Giles, D. M., Schafer, J. S., Sinyuk, A., Slutsker, I., Smirnov, A., Sorokin, M., Anderson, B. E., Che, H., Choi, M., Crawford, J. H., Ferrare, R. A., Garay, M. J., Jeong, U., Kim, M., Kim, W., Knox, N., Li, Z., Lim, H. S., Liu, Y., Maring, H., Nakata, M., Pickering, K. E., Piketh, S., Redemann, J., Reid, J. S., Salinas, S., Seo, S., Tan, F., Tripathi, S. N., Toon, O. B., and Xiao, Q.: An overview of mesoscale aerosol processes, comparisons, and validation studies from DRAGON networks, Atmos. Chem. Phys., 18, 655–671, <ext-link xlink:href="https://doi.org/10.5194/acp-18-655-2018" ext-link-type="DOI">10.5194/acp-18-655-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib46"><label>46</label><?label 1?><mixed-citation>
Huffman, G. J., Adler, R. F., Bolvin, D. T., Gu, G., Nelkin, E. J., Bowman, K. P., Hong, Y., Stocker, E. F.,  Wolff, D. B.: The TRMM Multi-satellite Precipitation
Analysis: Quasi-Global, Multi-Year, Combined-Sensor Precipitation Estimates
at Fine Scale, J.Hydrometeor., 8, 38–55, 2007.</mixed-citation></ref>
      <ref id="bib1.bib47"><label>47</label><?label 1?><mixed-citation>
IPCC: Climate Change 2013: The Physical Science Basis. Contribution of
Working Group I to the Fifth Assessment Report of the Intergovernmental
Panel on Climate Change, edited by:
Stocker, T. F., Qin, D., Plattner, G.-K., Tignor,
M., Allen, S. K., Boschung, J., Nauels, A., Xia, Y., Bex, V. and Midgley, P.
M., Cambridge University Press, Cambridge, UK and New
York, USA, 2013.</mixed-citation></ref>
      <ref id="bib1.bib48"><label>48</label><?label 1?><mixed-citation>Jethva, H., Torres, O., Waquet, F., Chand, D., and Hu, Y.: How do A-train
sensors intercompare in the retrieval of above-cloud aerosol optical depth?
A case study-based assessment, Geophys. Res. Lett., 41, 186–192,
<ext-link xlink:href="https://doi.org/10.1002/2013GL058405" ext-link-type="DOI">10.1002/2013GL058405</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib49"><label>49</label><?label 1?><mixed-citation>Jethva, H., Torres, O., Remer, L., Redemann, J., Livingston, J., Dunagan, S., Shinozuka, Y., Kacenelenbogen, M., Rosenheimer, M. S., and Spurr, R.: Validating MODIS above-cloud aerosol optical depth retrieved from “color ratio” algorithm using direct measurements made by NASA's airborne AATS and 4STAR sensors, Atmos. Meas. Tech., 9, 5053–5062, <ext-link xlink:href="https://doi.org/10.5194/amt-9-5053-2016" ext-link-type="DOI">10.5194/amt-9-5053-2016</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib50"><label>50</label><?label 1?><mixed-citation>Jethva, H., Torres, O., and Ahn, C.: A 12-year long global record of optical depth of absorbing aerosols above the cloud<?pagebreak page1560?>s derived from the OMI/OMACA algorithm, Atmos. Meas. Tech., 11, 5837–5864, <ext-link xlink:href="https://doi.org/10.5194/amt-11-5837-2018" ext-link-type="DOI">10.5194/amt-11-5837-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib51"><label>51</label><?label 1?><mixed-citation>Kacarab, M., Thornhill, K. L., Dobracki, A., Howell, S. G., O'Brien, J. R., Freitag, S., Poellot, M. R., Wood, R., Zuidema, P., Redemann, J., and Nenes, A.: Biomass burning aerosol as a modulator of the droplet number in the southeast Atlantic region, Atmos. Chem. Phys., 20, 3029–3040, <ext-link xlink:href="https://doi.org/10.5194/acp-20-3029-2020" ext-link-type="DOI">10.5194/acp-20-3029-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib52"><label>52</label><?label 1?><mixed-citation>Kacenelenbogen, M. S., Vaughan, M. A., Redemann, J., Young, S. A., Liu, Z., Hu, Y., Omar, A. H., LeBlanc, S., Shinozuka, Y., Livingston, J., Zhang, Q., and Powell, K. A.: Estimations of global shortwave direct aerosol radiative effects above opaque water clouds using a combination of A-Train satellite sensors, Atmos. Chem. Phys., 19, 4933–4962, <ext-link xlink:href="https://doi.org/10.5194/acp-19-4933-2019" ext-link-type="DOI">10.5194/acp-19-4933-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib53"><label>53</label><?label 1?><mixed-citation>Katich, J. M., Samset, B. H., Bui, T. P., Dollner, M., Froyd, K. D.,
Campuzano-Jost, P., Nault, B. A., Schroder,  J. C.,  Weinzierl, B., and Schwarz, J. P.: Strong contrast in remote black carbon aerosol
loadings between the Atlantic and Pacific basins, J. Geophys.
Res.-Atmos.,123, 13386–13395,
<ext-link xlink:href="https://doi.org/10.1029/2018JD029206" ext-link-type="DOI">10.1029/2018JD029206</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib54"><label>54</label><?label 1?><mixed-citation>Keil, A. and Haywood, J. M.: Solar radiative forcing by BB aerosol
particles during SAFARI 2000: A case study based on measured aerosol and
cloud properties, J. Geophys. Res., 108, 8467,
<ext-link xlink:href="https://doi.org/10.1029/2002JD002315" ext-link-type="DOI">10.1029/2002JD002315</ext-link>, 2003.</mixed-citation></ref>
      <ref id="bib1.bib55"><label>55</label><?label 1?><mixed-citation>Knobelspiesse, K., Cairns, B., Jethva, H., Kacenelenbogen, M., Segal-Rosenheimer, M., and Torres, O.: Remote sensing of above cloud aerosols, in: Light Scattering Reviews 9, edited by: Kokhanovsky, A., Springer Praxis Books, Springer, Berlin, Heidelberg, <ext-link xlink:href="https://doi.org/10.1007/978-3-642-37985-7_5" ext-link-type="DOI">10.1007/978-3-642-37985-7_5</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib56"><label>56</label><?label 1?><mixed-citation>Koch, D. and Del Genio, A. D.: Black carbon semi-direct effects on cloud cover: review and synthesis, Atmos. Chem. Phys., 10, 7685–7696, <ext-link xlink:href="https://doi.org/10.5194/acp-10-7685-2010" ext-link-type="DOI">10.5194/acp-10-7685-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib57"><label>57</label><?label 1?><mixed-citation>Koffi, B., Schulz, M.,  Bréon, F., Griesfeller, J.,  Winker, D., Balkanski, Y., Bauer, S., Berntsen, T., Chin, M.,  Collins, W. D., Dentener, F., Diehl, T., Easter, R., Ghan, S., Ginoux, P., Gong, S., Horowitz, L. W., Iversen, T.,  Kirkevåg, A., Koch, D., Krol, M., Myhre, G., Stier, P., and Takemura, T.: Application of the CALIOP layer product to evaluate the
vertical distribution of aerosols estimated by global models: AeroCom phase
I results, J. Geophys. Res., 117, D10201, <ext-link xlink:href="https://doi.org/10.1029/2011JD016858" ext-link-type="DOI">10.1029/2011JD016858</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib58"><label>58</label><?label 1?><mixed-citation>LeBlanc, S.: Moving Lines: NASA airborne research flight
planning tool release (Version v1.21), Zenodo, <ext-link xlink:href="https://doi.org/10.5281/zenodo.1478126" ext-link-type="DOI">10.5281/zenodo.1478126</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib59"><label>59</label><?label 1?><mixed-citation>LeBlanc, S. E., Redemann, J., Flynn, C., Pistone, K., Kacenelenbogen, M., Segal-Rosenheimer, M., Shinozuka, Y., Dunagan, S., Dahlgren, R. P., Meyer, K., Podolske, J., Howell, S. G., Freitag, S., Small-Griswold, J., Holben, B., Diamond, M., Wood, R., Formenti, P., Piketh, S., Maggs-Kölling, G., Gerber, M., and Namwoonde, A.: Above-cloud aerosol optical depth from airborne observations in the southeast Atlantic, Atmos. Chem. Phys., 20, 1565–1590, <ext-link xlink:href="https://doi.org/10.5194/acp-20-1565-2020" ext-link-type="DOI">10.5194/acp-20-1565-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib60"><label>60</label><?label 1?><mixed-citation>Ma, P.-L., Rasch, P. J., Fast, J. D., Easter, R. C., Gustafson Jr., W. I., Liu, X., Ghan, S. J., and Singh, B.: Assessing the CAM5 physics suite in the WRF-Chem model: implementation, resolution sensitivity, and a first evaluation for a regional case study, Geosci. Model Dev., 7, 755–778, <ext-link xlink:href="https://doi.org/10.5194/gmd-7-755-2014" ext-link-type="DOI">10.5194/gmd-7-755-2014</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib61"><label>61</label><?label 1?><mixed-citation>Mallet, M., Nabat, P., Zuidema, P., Redemann, J., Sayer, A. M., Stengel, M., Schmidt, S., Cochrane, S., Burton, S., Ferrare, R., Meyer, K., Saide, P., Jethva, H., Torres, O., Wood, R., Saint Martin, D., Roehrig, R., Hsu, C., and Formenti, P.: Simulation of the transport, vertical distribution, optical properties and radiative impact of smoke aerosols with the ALADIN regional climate model during the ORACLES-2016 and LASIC experiments, Atmos. Chem. Phys., 19, 4963–4990, <ext-link xlink:href="https://doi.org/10.5194/acp-19-4963-2019" ext-link-type="DOI">10.5194/acp-19-4963-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib62"><label>62</label><?label 1?><mixed-citation>Mallet, M., Solmon, F., Nabat, P., Elguindi, N., Waquet, F., Bouniol, D., Sayer, A. M., Meyer, K., Roehrig, R., Michou, M., Zuidema, P., Flamant, C., Redemann, J., and Formenti, P.: Direct and semi-direct radiative forcing of biomass-burning aerosols over the southeast Atlantic (SEA) and its sensitivity to absorbing properties: a regional climate modeling study, Atmos. Chem. Phys., 20, 13191–13216, <ext-link xlink:href="https://doi.org/10.5194/acp-20-13191-2020" ext-link-type="DOI">10.5194/acp-20-13191-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib63"><label>63</label><?label 1?><mixed-citation>
Martin, G. M., Johnson, D. W., and Spice, A.: The measurement and parameterization of effective radius of droplets in warm stratiform clouds, J. Atmos. Sci., 51, 1823–1842, 1994.</mixed-citation></ref>
      <ref id="bib1.bib64"><label>64</label><?label 1?><mixed-citation>Mauger, G. and Norris, J.: Meteorological bias in satellite estimates of
aerosol-cloud relationships, Geophys. Res. Lett., 34,
<ext-link xlink:href="https://doi.org/10.1029/2007GL029952" ext-link-type="DOI">10.1029/2007GL029952</ext-link>, 2007.</mixed-citation></ref>
      <ref id="bib1.bib65"><label>65</label><?label 1?><mixed-citation>Meyer, K., Platnick, S., Oreopoulos, L., and Lee, D.: Estimating the direct
radiative effect of absorbing aerosols overlying marine boundary layer
clouds in the southeast Atlantic using MODIS and CALIOP, J. Geophys. Res.-Atmos., 118, 4801–4815, <ext-link xlink:href="https://doi.org/10.1002/jgrd.50449" ext-link-type="DOI">10.1002/jgrd.50449</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib66"><label>66</label><?label 1?><mixed-citation>Meyer, K., Platnick, S., and Zhang, Z.: Simultaneously inferring above-cloud
absorbing aerosol optical thickness and underlying liquid phase cloud
optical and microphysical properties using MODIS, J. Geophys. Res.-Atmos.,
120, 2015JD023128, <ext-link xlink:href="https://doi.org/10.1002/2015JD023128" ext-link-type="DOI">10.1002/2015JD023128</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib67"><label>67</label><?label 1?><mixed-citation>
Miles, N. L., Verlinde, J., and Clothiaux, E. E.: Cloud droplet size distributions in low-level stratiform clouds, J. Atmos. Sci., 57, 295–311, 2000.</mixed-citation></ref>
      <ref id="bib1.bib68"><label>68</label><?label 1?><mixed-citation>Miller, D. J., Segal-Rozenhaimer, M., Knobelspiesse, K., Redemann, J., Cairns, B., Alexandrov, M., van Diedenhoven, B., and Wasilewski, A.: Low-level liquid cloud properties during ORACLES retrieved using airborne polarimetric measurements and a neural network algorithm, Atmos. Meas. Tech., 13, 3447–3470, <ext-link xlink:href="https://doi.org/10.5194/amt-13-3447-2020" ext-link-type="DOI">10.5194/amt-13-3447-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib69"><label>69</label><?label 1?><mixed-citation>
Minnis, P., Nguyen, L., Palikonda, R., Heck, P. W., Spangenberg, D. A., Doelling, D. R., Ayers, J. K., Smith Jr., W. L., Khaiyer, M. M., Trepte, Q. Z., Avey, L. A., Chang, F.-L., Yost, C. R., Chee, T. L., and Sun-Mack, S.: Near-real
time cloud retrievals from operational and research meteorological
satellites, Proceedings of the SPIE Europe Remote Sens., Cardiff, UK, 15–18
September 2008, 7107-2, 2008.</mixed-citation></ref>
      <ref id="bib1.bib70"><label>70</label><?label 1?><mixed-citation>Minnis, P., Sun-Mack, S., Chen, Y., Chang, F.-L., Yost, C. R., Smith Jr., W. L., Heck, P. W., Arduini, R. F., Bedka, S. T., Yi, Y., Hong, G., Jin, Z.,
Painemal, D., Palikonda, R., Scarino, B., Spangenberg, D. A., Smith, R. A.,
Trepte, Q. Z., Yang, P., and Xie, Y.: CERES MODIS cloud product
retrievals for Edition 4, Part I: Algorithm changes, IEEE Trans. Geosci.
Remote Sens., <ext-link xlink:href="https://doi.org/10.1109/TGRS.2020.3008866" ext-link-type="DOI">10.1109/TGRS.2020.3008866</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib71"><label>71</label><?label 1?><mixed-citation>
Molod, A., Takacs, L., Suarez, M., Bacmeister, J., Song, I.-S., and
Eichmann, A.: The GEOS-5 Atmospheric General Circulation Model: Mean Climate
and Development from MERRA t<?pagebreak page1561?>o Fortuna, Technical Report Series on Global
Modeling and Data Assimilation, NASA, Washington, D.C., USA, 28, 124 pp., 2012.</mixed-citation></ref>
      <ref id="bib1.bib72"><label>72</label><?label 1?><mixed-citation>Myhre, G., Samset, B. H., Schulz, M., Balkanski, Y., Bauer, S., Berntsen, T. K., Bian, H., Bellouin, N., Chin, M., Diehl, T., Easter, R. C., Feichter, J., Ghan, S. J., Hauglustaine, D., Iversen, T., Kinne, S., Kirkevåg, A., Lamarque, J.-F., Lin, G., Liu, X., Lund, M. T., Luo, G., Ma, X., van Noije, T., Penner, J. E., Rasch, P. J., Ruiz, A., Seland, Ø., Skeie, R. B., Stier, P., Takemura, T., Tsigaridis, K., Wang, P., Wang, Z., Xu, L., Yu, H., Yu, F., Yoon, J.-H., Zhang, K., Zhang, H., and Zhou, C.: Radiative forcing of the direct aerosol effect from AeroCom Phase II simulations, Atmos. Chem. Phys., 13, 1853–1877, <ext-link xlink:href="https://doi.org/10.5194/acp-13-1853-2013" ext-link-type="DOI">10.5194/acp-13-1853-2013</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib73"><label>73</label><?label 1?><mixed-citation>National Academies of Sciences, Engineering, and Medicine: Thriving on Our
Changing Planet: A Decadal Strategy for Earth Observation from Space,
The National Academies Press,
Washington, DC, USA,
<ext-link xlink:href="https://doi.org/10.17226/24938" ext-link-type="DOI">10.17226/24938</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib74"><label>74</label><?label 1?><mixed-citation>
Nicholls, S. and Leighton, J.: An observational study of the structure of stratiform cloud sheets, Part I: Structure, Q. J. Roy. Meteor. Soc., 112, 431–460, 1986.</mixed-citation></ref>
      <ref id="bib1.bib75"><label>75</label><?label 1?><mixed-citation>ORACLES Science Team: Suite of Aerosol, Cloud, and Related Data Acquired
Aboard P3 During ORACLES 2018, Version 2, NASA Ames Earth Science Project
Office,
<ext-link xlink:href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2018_V2" ext-link-type="DOI">10.5067/Suborbital/ORACLES/P3/2018_V2</ext-link>, 2020a.</mixed-citation></ref>
      <ref id="bib1.bib76"><label>76</label><?label 1?><mixed-citation>ORACLES Science Team: Suite of Aerosol, Cloud, and Related Data Acquired
Aboard P3 During ORACLES 2017, Version 2, NASA Ames Earth Science Project
Office, <ext-link xlink:href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2017_V2" ext-link-type="DOI">10.5067/Suborbital/ORACLES/P3/2017_V2</ext-link>, 2020b.</mixed-citation></ref>
      <ref id="bib1.bib77"><label>77</label><?label 1?><mixed-citation>ORACLES Science Team: Suite of Aerosol, Cloud, and Related Data Acquired
Aboard P3 During ORACLES 2016, Version 2, NASA Ames Earth Science Project
Office, <ext-link xlink:href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2016_V2" ext-link-type="DOI">10.5067/Suborbital/ORACLES/P3/2016_V2</ext-link>, 2020c.</mixed-citation></ref>
      <ref id="bib1.bib78"><label>78</label><?label 1?><mixed-citation>ORACLES Science Team: Suite of Aerosol, Cloud, and Related Data Acquired
Aboard ER2 During ORACLES 2016, Version 2, NASA Ames Earth Science Project
Office, <ext-link xlink:href="https://doi.org/10.5067/Suborbital/ORACLES/ER2/2016_V2" ext-link-type="DOI">10.5067/Suborbital/ORACLES/ER2/2016_V2</ext-link>, 2020d.</mixed-citation></ref>
      <ref id="bib1.bib79"><label>79</label><?label 1?><mixed-citation>Painemal, D. and Zuidema, P.: Microphysical variability in southeast Pacific Stratocumulus clouds: synoptic conditions and radiative response, Atmos. Chem. Phys., 10, 6255–6269, <ext-link xlink:href="https://doi.org/10.5194/acp-10-6255-2010" ext-link-type="DOI">10.5194/acp-10-6255-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib80"><label>80</label><?label 1?><mixed-citation>Painemal, D. and Zuidema, P.: Assessment of MODIS cloud effective radius
and optical thickness retrievals over the Southeast Pacific with VOCALS-REx
in situ measurements, J. Geophys. Res., 116, D24206,
<ext-link xlink:href="https://doi.org/10.1029/2011JD016155" ext-link-type="DOI">10.1029/2011JD016155</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib81"><label>81</label><?label 1?><mixed-citation>
Pappenberger, F., Scipal, K., and Buizza, R.: Hydrological aspects of
meteorological verification, Atmospheric Sci. Lett., 9, 43–52, 2008.</mixed-citation></ref>
      <ref id="bib1.bib82"><label>82</label><?label 1?><mixed-citation>Peers, F., Francis, P., Fox, C., Abel, S. J., Szpek, K., Cotterell, M. I., Davies, N. W., Langridge, J. M., Meyer, K. G., Platnick, S. E., and Haywood, J. M.: Observation of absorbing aerosols above clouds over the south-east Atlantic Ocean from the geostationary satellite SEVIRI – Part 1: Method description and sensitivity, Atmos. Chem. Phys., 19, 9595–9611, <ext-link xlink:href="https://doi.org/10.5194/acp-19-9595-2019" ext-link-type="DOI">10.5194/acp-19-9595-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib83"><label>83</label><?label 1?><mixed-citation>Pistone, K., Redemann, J., Doherty, S., Zuidema, P., Burton, S., Cairns, B., Cochrane, S., Ferrare, R., Flynn, C., Freitag, S., Howell, S. G., Kacenelenbogen, M., LeBlanc, S., Liu, X., Schmidt, K. S., Sedlacek III, A. J., Segal-Rozenhaimer, M., Shinozuka, Y., Stamnes, S., van Diedenhoven, B., Van Harten, G., and Xu, F.: Intercomparison of biomass burning aerosol optical properties from in situ and remote-sensing instruments in ORACLES-2016, Atmos. Chem. Phys., 19, 9181–9208, <ext-link xlink:href="https://doi.org/10.5194/acp-19-9181-2019" ext-link-type="DOI">10.5194/acp-19-9181-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib84"><label>84</label><?label 1?><mixed-citation>Rajapakshe, C., Zhang, Z., Yorks, J. E., Yu, H., Tan, Q., Meyer, K.,
Platnick, S., and Winker, D. M.: Seasonally transported aerosol layers over
southeast Atlantic are closer to underlying clouds than previously reported,
Geophys. Res. Lett., 44, 5818–5825, <ext-link xlink:href="https://doi.org/10.1002/2017GL073559" ext-link-type="DOI">10.1002/2017GL073559</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib85"><label>85</label><?label 1?><mixed-citation>Ran, Q., Fu, W., Liu, Y., Li, T. Shi, K., and Sivakumar, B.: Evaluation of
Quantitative Precipitation Predictions by ECMWF, CMA, and UKMO for Flood
Forecasting: Application to Two Basins in China, Nat. Hazards Rev.,
19, 05018003, <ext-link xlink:href="https://doi.org/10.1061/(ASCE)NH.1527-6996.0000282" ext-link-type="DOI">10.1061/(ASCE)NH.1527-6996.0000282</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib86"><label>86</label><?label 1?><mixed-citation>Rouault, M.: Bi-annual intrusion of tropical water in the northern Benguela
upwelling, Geophys. Res. Lett., 39, L12606, <ext-link xlink:href="https://doi.org/10.1029/GL052099" ext-link-type="DOI">10.1029/GL052099</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib87"><label>87</label><?label 1?><mixed-citation>Saide, P. E., Thompson, G., Eidhammer, T., da Silva, A. M., Pierce, R. B.,
and Carmichael, G. R.: Assessment of biomass burning smoke influence on
environmental conditions for multi-year tornado outbreaks by combining
aerosol-aware microphysics and fire emission constraints, J. Geophys. Res.-Atmos., 121, 10294–10311, <ext-link xlink:href="https://doi.org/10.1002/2016JD025056" ext-link-type="DOI">10.1002/2016JD025056</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib88"><label>88</label><?label 1?><mixed-citation>Sakaeda, N., Wood, R., and Rasch, P. J.: Direct and semidirect aerosol effects of southern African biomass burning aerosol, J. Geophys. Res.-Atmos., 116, D12205,
<ext-link xlink:href="https://doi.org/10.1029/2010JD015540" ext-link-type="DOI">10.1029/2010JD015540</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib89"><label>89</label><?label 1?><mixed-citation>
Sayer, A. M., Hsu, N. C., Bettenhausen, C., Lee, J., Redemann, J., Schmid,
B., and Shinozuka, Y.: Extending “Deep Blue” aerosol retrieval coverage
to cases of absorbing aerosols above clouds: Sensitivity analysis and first
case studies, J. Geophys. Res.-Atmos., 121, 4830–4854, 2016.</mixed-citation></ref>
      <ref id="bib1.bib90"><label>90</label><?label 1?><mixed-citation>Sayer, A. M., Hsu, N. C., Lee, J., Kim, W. V., Burton, S., Fenn, M. A., Ferrare, R. A., Kacenelenbogen, M., LeBlanc, S., Pistone, K., Redemann, J., Segal-Rozenhaimer, M., Shinozuka, Y., and Tsay, S.-C.: Two decades observing smoke above clouds in the south-eastern Atlantic Ocean: Deep Blue algorithm updates and validation with ORACLES field campaign data, Atmos. Meas. Tech., 12, 3595–3627, <ext-link xlink:href="https://doi.org/10.5194/amt-12-3595-2019" ext-link-type="DOI">10.5194/amt-12-3595-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib91"><label>91</label><?label 1?><mixed-citation>Schulz, M., Textor, C., Kinne, S., Balkanski, Y., Bauer, S., Berntsen, T., Berglen, T., Boucher, O., Dentener, F., Guibert, S., Isaksen, I. S. A., Iversen, T., Koch, D., Kirkevåg, A., Liu, X., Montanaro, V., Myhre, G., Penner, J. E., Pitari, G., Reddy, S., Seland, Ø., Stier, P., and Takemura, T.: Radiative forcing by aerosols as derived from the AeroCom present-day and pre-industrial simulations, Atmos. Chem. Phys., 6, 5225–5246, <ext-link xlink:href="https://doi.org/10.5194/acp-6-5225-2006" ext-link-type="DOI">10.5194/acp-6-5225-2006</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bib92"><label>92</label><?label 1?><mixed-citation>
Segal-Rozenhaimer, M., Miller, D., Knobelspiesse, K., Redemann, J., Cairns,
B., and Alexandrov, M.: Development of neural network retrievals of liquid cloud
properties from multi-angle polarimetric observations, J.
Quant. Spectrosc. Ra., 220, 39–51, 2018.</mixed-citation></ref>
      <?pagebreak page1562?><ref id="bib1.bib93"><label>93</label><?label 1?><mixed-citation>Shinozuka, Y. and Redemann, J.: Horizontal variability of aerosol optical depth observed during the ARCTAS airborne experiment, Atmos. Chem. Phys., 11, 8489–8495, <ext-link xlink:href="https://doi.org/10.5194/acp-11-8489-2011" ext-link-type="DOI">10.5194/acp-11-8489-2011</ext-link>, 2011.</mixed-citation></ref>
      <ref id="bib1.bib94"><label>94</label><?label 1?><mixed-citation>Shinozuka, Y., Saide, P. E., Ferrada, G. A., Burton, S. P., Ferrare, R., Doherty, S. J., Gordon, H., Longo, K., Mallet, M., Feng, Y., Wang, Q., Cheng, Y., Dobracki, A., Freitag, S., Howell, S. G., LeBlanc, S., Flynn, C., Segal-Rosenhaimer, M., Pistone, K., Podolske, J. R., Stith, E. J., Bennett, J. R., Carmichael, G. R., da Silva, A., Govindaraju, R., Leung, R., Zhang, Y., Pfister, L., Ryoo, J.-M., Redemann, J., Wood, R., and Zuidema, P.: Modeling the smoky troposphere of the southeast Atlantic: a comparison to ORACLES airborne observations from September of 2016, Atmos. Chem. Phys., 20, 11491–11526, <ext-link xlink:href="https://doi.org/10.5194/acp-20-11491-2020" ext-link-type="DOI">10.5194/acp-20-11491-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib95"><label>95</label><?label 1?><mixed-citation>
Simpson, J. and Wiggert, V.: Models of precipitating cumulus towers, Mon. Weather Rev., 97, 471–489, 1969.</mixed-citation></ref>
      <ref id="bib1.bib96"><label>96</label><?label 1?><mixed-citation>Skamarock, W. C., Klemp, J., Dudhia, J., Gill, D. O., Barker, D., Wang,
W., and Powers, J. G.: A Description of the Advanced Research, WRF, Version 3.27.3-27, NCAR Technical Notes, NCAR/TN-4751STR, available at: <uri>https://opensky.ucar.edu/islandora/object/technotes:500/datastream/PDF/view</uri> (last access: December 2020), 2008.</mixed-citation></ref>
      <ref id="bib1.bib97"><label>97</label><?label 1?><mixed-citation>Sorooshian, A., Feingold, G., Lebsock, M. D., Jiang, H., and Stephens, G. L.:
On the Precipitation Susceptibility of Clouds to Aerosol Perturbations,
Geophys. Res. Lett., 36, 13, <ext-link xlink:href="https://doi.org/10.1029/2009GL038993" ext-link-type="DOI">10.1029/2009GL038993</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib98"><label>98</label><?label 1?><mixed-citation>Stier, P., Schutgens, N. A. J., Bellouin, N., Bian, H., Boucher, O., Chin, M., Ghan, S., Huneeus, N., Kinne, S., Lin, G., Ma, X., Myhre, G., Penner, J. E., Randles, C. A., Samset, B., Schulz, M., Takemura, T., Yu, F., Yu, H., and Zhou, C.: Host model uncertainties in aerosol radiative forcing estimates: results from the AeroCom Prescribed intercomparison study, Atmos. Chem. Phys., 13, 3245–3270, <ext-link xlink:href="https://doi.org/10.5194/acp-13-3245-2013" ext-link-type="DOI">10.5194/acp-13-3245-2013</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib99"><label>99</label><?label 1?><mixed-citation>Swap, R. J., Annegarn, H. J., Suttles, J. T., King, M. D., Platnick, S.,
Privette, J. L., and Scholes, R. J.: Africa burning: A thematic analysis of
the Southern African Regional Science Initiative (SAFARI 2000), J. Geophys.
Res., 108, 8465, <ext-link xlink:href="https://doi.org/10.1029/2003JD003747" ext-link-type="DOI">10.1029/2003JD003747</ext-link>, 2003.</mixed-citation></ref>
      <ref id="bib1.bib100"><label>100</label><?label 1?><mixed-citation>Szczodrak, M., Austin, P. H., and Krummel, P. B.: Variability of Optical
Depth and Effective Radius in Marine Stratocumulus Clouds, J. Atmos. Sci.,
58, 2912–2926, <ext-link xlink:href="https://doi.org/10.1175/1520-0469(2001)058&lt;2912:VOODAE&gt;2.0.CO;2" ext-link-type="DOI">10.1175/1520-0469(2001)058&lt;2912:VOODAE&gt;2.0.CO;2</ext-link>, 2001.</mixed-citation></ref>
      <ref id="bib1.bib101"><label>101</label><?label 1?><mixed-citation>
Twomey, S.: Pollution and the planetary albedo, Atmos. Environ., 8,
1251–1256, 1974.</mixed-citation></ref>
      <ref id="bib1.bib102"><label>102</label><?label 1?><mixed-citation>Tzortziou, M., Herman, J. R., Cede, A., and Abuhassan, N.: High precision,
absolute total column ozone measurements from the Pandora spectrometer
system: Comparisons with data from a Brewer double monochromator and
AuraOMI, J. Geophys. Res., 117, D16303, <ext-link xlink:href="https://doi.org/10.1029/2012JD017814" ext-link-type="DOI">10.1029/2012JD017814</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib103"><label>103</label><?label 1?><mixed-citation>van der Werf, G. R., Randerson, J. T., Giglio, L., Collatz, G. J., Mu, M., Kasibhatla, P. S., Morton, D. C., DeFries, R. S., Jin, Y., and van Leeuwen, T. T.: Global fire emissions and the contribution of deforestation, savanna, forest, agricultural, and peat fires (1997–2009), Atmos. Chem. Phys., 10, 11707–11735, <ext-link xlink:href="https://doi.org/10.5194/acp-10-11707-2010" ext-link-type="DOI">10.5194/acp-10-11707-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib104"><label>104</label><?label 1?><mixed-citation>
Watson-Parris, D., Schutgens, N., Winker, D., Burton, S., Ferrare, R.,
Stier, P.: On the Limits of CALIOP for Constraining Modeled Free Tropospheric
Aerosol, Geophys. Res. Lett., 45, 9260–9266, 2018.</mixed-citation></ref>
      <ref id="bib1.bib105"><label>105</label><?label 1?><mixed-citation>Werdell, P. J., Behrenfeld, M. J., Bontempi, P. S., Boss, E., Cairns, B.,
Davis, G. T., Franz, B. A., Gliese, U. B., Gorman, E. T., Hasekamp, O.,
Knobelspiesse, K. D., Mannino, A., Martins, J. V., McClain, C. R., Meister,
G., and Remer, L. A.: The Plankton, Aerosol, Cloud, ocean Ecosystem (PACE)
mission: Status, science, advances, B. Am. Meteorol.
Soc., 100, 1775–1794 <ext-link xlink:href="https://doi.org/10.1175/bams-d-18-0056.1" ext-link-type="DOI">10.1175/bams-d-18-0056.1</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib106"><label>106</label><?label 1?><mixed-citation>Wilcox, E. M.: Direct and semi-direct radiative forcing of smoke aerosols over clouds, Atmos. Chem. Phys., 12, 139–149, <ext-link xlink:href="https://doi.org/10.5194/acp-12-139-2012" ext-link-type="DOI">10.5194/acp-12-139-2012</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib107"><label>107</label><?label 1?><mixed-citation>
Wood, R.: Cancellation of aerosol indirect effects in marine stratocumulus through cloud thinning, J. Atmos. Sci., 64, 2657–2669, 2007.</mixed-citation></ref>
      <ref id="bib1.bib108"><label>108</label><?label 1?><mixed-citation>Wood, R.: Stratocumulus clouds, Mon. Weather Rev., 140, 2373–2423, <ext-link xlink:href="https://doi.org/10.1175/MWR-D-11-00121.1" ext-link-type="DOI">10.1175/MWR-D-11-00121.1</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib109"><label>109</label><?label 1?><mixed-citation>Wood, R., Leon, D., Lebsock, M., Snider, J., and Clarke, A. D.:
Precipitation Driving of Droplet Concentration Variability in Marine Low
Clouds: PRECIPITATION DRIVING OF DROP CONC, J. Geophys. Res.-Atmos., 117, D19,  <ext-link xlink:href="https://doi.org/10.1029/2012JD018305" ext-link-type="DOI">10.1029/2012JD018305</ext-link>,
2012.</mixed-citation></ref>
      <ref id="bib1.bib110"><label>110</label><?label 1?><mixed-citation>Wu, H., Taylor, J. W., Szpek, K., Langridge, J. M., Williams, P. I., Flynn, M., Allan, J. D., Abel, S. J., Pitt, J., Cotterell, M. I., Fox, C., Davies, N. W., Haywood, J., and Coe, H.: Vertical variability of the properties of highly aged biomass burning aerosol transported over the southeast Atlantic during CLARIFY-2017, Atmos. Chem. Phys., 20, 12697–12719, <ext-link xlink:href="https://doi.org/10.5194/acp-20-12697-2020" ext-link-type="DOI">10.5194/acp-20-12697-2020</ext-link>, 2020.</mixed-citation></ref>
      <ref id="bib1.bib111"><label>111</label><?label 1?><mixed-citation>
Xu, F., van Harten, G., Diner, D., Davis, A., Seidel, F., Rheingans, B.,
Tosca, M., Alexandrov, M., Cairns, B., Ferrare, R., Burton, S., Fenn, M. A., Hostetler, C. A., Wood, R., and Redemann, J.:
Coupled Retrieval of Liquid Water Cloud and Above-Cloud Aerosol Properties
using the Airborne Multiangle SpectroPolarimetric Imager (AirMSPI), J.
Geophys. Res.-Atmos., 123, 3175–3204, 2018.</mixed-citation></ref>
      <ref id="bib1.bib112"><label>112</label><?label 1?><mixed-citation>
Ye, J., He, Y., Pappenberger, F., Cloke, H. L., Manful, D. Y., and Li, Z.:
Evaluation of ECMWF medium-range ensemble forecasts of precipitation for
river basins, Q. J. R. Meteor. Soc., 140, 1615–1628, 2014.</mixed-citation></ref>
      <ref id="bib1.bib113"><label>113</label><?label 1?><mixed-citation>
Yu, H. and Zhang, Z.: New Directions: Emerging satellite observations of
above-cloud aerosols and direct radiative forcing, Atmos. Environ.,
72, 36–40, 2013.</mixed-citation></ref>
      <ref id="bib1.bib114"><label>114</label><?label 1?><mixed-citation>Yu, H., Zhang, Y., Chin, M., Liu, Z., Omar, A., Remer, L. A., Yang, Y., Yuan,
T., and Zhang, J.: An Integrated Analysis of Aerosol above Clouds from
A-Train Multi-sensor Measurements, Rem. Sens. Environ., 121, 125–131,
<ext-link xlink:href="https://doi.org/10.1016/j.rse.2012.01.011" ext-link-type="DOI">10.1016/j.rse.2012.01.011</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib115"><label>115</label><?label 1?><mixed-citation>Zhang, J. and Zuidema, P.: The diurnal cycle of the smoky marine boundary layer observed during August in the remote southeast Atlantic, Atmos. Chem. Phys., 19, 14493–14516, <ext-link xlink:href="https://doi.org/10.5194/acp-19-14493-2019" ext-link-type="DOI">10.5194/acp-19-14493-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib116"><label>116</label><?label 1?><mixed-citation>Zhang, Z., Meyer, K., Yu, H., Platnick, S., Colarco, P., Liu, Z., and Oreopoulos, L.: Shortwave direct radiative effects of above-cloud aerosols over global oceans derived from 8 years of CALIOP and MODIS observations, Atmos. Chem. Phys., 16, 2877–2900, <ext-link xlink:href="https://doi.org/10.5194/acp-16-2877-2016" ext-link-type="DOI">10.5194/acp-16-2877-2016</ext-link>, 2016.</mixed-citation></ref>
      <?pagebreak page1563?><ref id="bib1.bib117"><label>117</label><?label 1?><mixed-citation>Zuidema, P., Painemal, D., deSzoeke, S., and Fairall, C.: Stratocumulus cloud
top height estimates and their climatic implications, J. Climate, 22,
4652–4666, <ext-link xlink:href="https://doi.org/10.1175/2009JCLI2708.1" ext-link-type="DOI">10.1175/2009JCLI2708.1</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib118"><label>118</label><?label 1?><mixed-citation>Zuidema, P., Chiu, C., Fairall, C. W., Ghan, S. J., Kollias, P., McFarguhar,
G. M., Mechem, D. B., Romps, D. M., Wong, H., Yuter, S. E., Alvarado, M. J.,
DeSzoeke, S. P., Feingold, G.,
Haywood, J. M.,
Lewis, E. R., McComiskey, A.,
Redemann, J., Turner, D. D., Wood, R., and Zhu, P.: Layered Atlantic Smoke
Interactions with Clouds (LASIC) Science Plan, DOE/SC-ARM-14-037, availabe at:
<uri>http://www.osti.gov/scitech/servlets/purl/1232658</uri> (last access: December 2018), 2015.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bib119"><label>119</label><?label 1?><mixed-citation>Zuidema, P., Redemann, J., Haywood, J., Wood, R., Piketh, S., Hipondoka, M., and
Formenti, P.: Smoke and Clouds above the Southeast Atlantic: Upcoming Field
Campaigns Probe Absorbing Aerosol's Impact on Climate, B.
Am. Meteorol. Soc., 97, 1131–1135, <ext-link xlink:href="https://doi.org/10.1175/BAMS-D-15-00082.1" ext-link-type="DOI">10.1175/BAMS-D-15-00082.1</ext-link>, 2016.</mixed-citation></ref>
      <ref id="bib1.bib120"><label>120</label><?label 1?><mixed-citation>Zuidema, P., Sedlacek III, A. J., Flynn, C., Springston, S., Delgadillo, R.,
Zhang, J., Aiken, A. C., Koontz, A., and Muradyan, P.: The Ascension Island boundary layer in the remote
southeast Atlantic is often smoky, Geophys. Res. Lett., 45,
4456–4465, <ext-link xlink:href="https://doi.org/10.1002/2017GL076926" ext-link-type="DOI">10.1002/2017GL076926</ext-link>, 2018.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>An overview of the ORACLES (ObseRvations of Aerosols above CLouds and their intEractionS) project: aerosol–cloud–radiation interactions in the southeast Atlantic basin</article-title-html>
<abstract-html><p>Southern Africa produces almost a third of the Earth's biomass
burning (BB) aerosol particles, yet the fate of these particles and their
influence on regional and global climate is poorly understood. ORACLES
(ObseRvations of Aerosols above CLouds and their intEractionS) is a
5-year NASA EVS-2 (Earth Venture Suborbital-2) investigation with three intensive observation periods designed to study key atmospheric processes
that determine the climate impacts of these aerosols. During the Southern Hemisphere winter and spring (June–October), aerosol particles reaching 3–5&thinsp;km in altitude are transported westward over the southeast Atlantic, where
they interact with one of the largest subtropical stratocumulus  (Sc) cloud decks in the world. The representation of these
interactions in climate models remains highly uncertain in part due to a
scarcity of observational constraints on aerosol and cloud properties, as well as due to the parameterized treatment of physical processes. Three ORACLES
deployments by the NASA P-3 aircraft in September 2016, August 2017, and
October 2018 (totaling  ∼ 350 science flight hours), augmented
by the deployment of the NASA ER-2 aircraft for remote sensing in September
2016 (totaling  ∼ 100 science flight hours), were intended to
help fill this observational gap. ORACLES focuses on three fundamental
science themes centered on the climate effects of African BB aerosols: (a) direct aerosol radiative effects, (b) effects of aerosol absorption on
atmospheric circulation and clouds, and (c) aerosol–cloud microphysical
interactions. This paper summarizes the ORACLES science objectives,
describes the project implementation, provides an overview of the flights
and measurements in each deployment, and highlights the integrative modeling
efforts from cloud to global scales to address science objectives.
Significant new findings on the vertical structure of BB aerosol physical
and chemical properties, chemical aging, cloud condensation nuclei, rain and
precipitation statistics, and aerosol indirect effects are emphasized, but
their detailed descriptions are the subject of separate publications. The
main purpose of this paper is to familiarize the broader scientific
community with the ORACLES project and the dataset it produced.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Ackerman, A. S., Toon, O. B., Stevens, D. E., Heymsfield, A. J., Ramanathan,
V., and Welton, E. J.: Reduction of tropical cloudiness by soot, Science,
288, 1042–1047, 2000.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
Ackerman, A. S., Kirkpatrick, M. P., Stevens, D. E., and Toon, O. B.: The impact of humidity above stratiform clouds on indirect aerosol climate forcing, Nature, 432, 1014–1017, <a href="https://doi.org/10.1038/nature03174" target="_blank">https://doi.org/10.1038/nature03174</a>, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
Adebiyi, A. and Zuidema, P.: The Role of the Southern African Easterly Jet
in Modifying the Southeast Atlantic Aerosol and Cloud Environments,
Q. J. Roy. Meteor. Soc., 697, 1574–89,
<a href="https://doi.org/10.1002/qj.2765" target="_blank">https://doi.org/10.1002/qj.2765</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>
Adebiyi, A. A. and Zuidema, P.: Low Cloud Cover Sensitivity to
Biomass-Burning Aerosols and Meteorology over the Southeast Atlantic,
J. Climate, 31, 4329–4346, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>
Adebiyi, A., Zuidema, P., and Abel, S.: The convolution of dynamics and
moisture with the presence of shortwave absorbing aerosols over the
southeast Atlantic, J. Climate, 28, 1997–2024,
<a href="https://doi.org/10.1175/JCLI-D-14-00352.1" target="_blank">https://doi.org/10.1175/JCLI-D-14-00352.1</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>
Adebiyi, A. A., Zuidema, P., Chang, I., Burton, S. P., and Cairns, B.: Mid-level clouds are frequent above the southeast Atlantic stratocumulus clouds, Atmos. Chem. Phys., 20, 11025–11043, <a href="https://doi.org/10.5194/acp-20-11025-2020" target="_blank">https://doi.org/10.5194/acp-20-11025-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>
Albrecht, B. A.: Aerosols, cloud microphysics, and fractional cloudiness,
Science, 245, 1227–1230, 1989.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation>
Andela, N., Morton, D. C., Giglio, L., Chen, Y., van der Werf, G. R., Kasibhatla, P. S., DeFries, R. S., Collatz, G. L., Hantson, S., Kloster, S., Bachelet, D., Forrest, M., Lasslop, G., Li, F., Mangeon, S., Melton, J. R., Yue, C., and Randerson, J. T.: A human-driven decline in global burned area, Science, 356,
1356–1362, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>
Annegarn, H. J. and Swap, R. J.: SAFARI 2000: A Southern African Example of
Science Diplomacy, Science and Diplomacy, 1, 4,
2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>
Bennartz, R. and Rausch, J.: Global and regional estimates of warm cloud droplet number concentration based on 13 years of AQUA-MODIS observations, Atmos. Chem. Phys., 17, 9815–9836, <a href="https://doi.org/10.5194/acp-17-9815-2017" target="_blank">https://doi.org/10.5194/acp-17-9815-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation>
Betts, A. K. and Ridgway, W.: Coupling of the Radiative, Convective, and
Surface Fluxes over the Equatorial Pacific, J. Atmos.
Sci., 45, 522–36, <a href="https://doi.org/10.1175/1520-0469(1988)045%3C0522:COTRCA%3E2.0.CO;2" target="_blank">https://doi.org/10.1175/1520-0469(1988)045%3C0522:COTRCA%3E2.0.CO;2</a>, 1988.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>12</label><mixed-citation>
Bond, T. C., Doherty, S. J., Fahey, D. W., Forster, P. M.  Berntsen, T., DeAngelo,  B. J.,  Flanner, M. G.,  Ghan, S., Kärcher, B., Koch, D., Kinne, S., Kondo, Y.,  Quinn, P. K., Sarofim, M. C.,  Schultz, M. G.,  Schulz, M., Venkataraman, C., Zhang, H., Zhang S., Bellouin, N., Guttikunda, S. K.,  Hopke, P. K., Jacobson, M. Z., Kaiser, J. W.,  Klimont, Z., Lohmann,  U.,  Schwarz, J. P., Shindell, D., Storelvmo, T., Warren, S. G., and  Zender, C. S.: Bounding the role of black carbon in the climate
system: A scientific assessment, J. Geophys. Res.-Atmos., 118, 5380–5552,
<a href="https://doi.org/10.1002/jgrd.50171" target="_blank">https://doi.org/10.1002/jgrd.50171</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation>
Bony, S. and Dufresne, J. L.: Marine boundary layer clouds at the heart of
tropical cloud feedback uncertainties in climate models, Geophys. Res.
Lett., 32, L20806, <a href="https://doi.org/10.1029/2005GL023851" target="_blank">https://doi.org/10.1029/2005GL023851</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>14</label><mixed-citation>
Burton, S., Hostetler, C., Cook, A., Hair, J., Seaman, S., Scola, S.,
Harper, D., Smith, J., Fenn, M., Ferrare, R., Saide, P. E., Chemyakin, E. V., and Müller, D.: Calibration of
a high spectral resolution lidar using a Michelson interferometer, with data
examples from ORACLES, Appl. Optics, 57, 6061, <a href="https://doi.org/10.1364/AO.57.006061" target="_blank">https://doi.org/10.1364/AO.57.006061</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>15</label><mixed-citation>
Chand, D., Wood, R., Anderson, T., Satheesh, S. K., and Charlson, R. J.:
Satellite-derived direct radiative effect of aerosols dependent on cloud
cover, Nat. Geosci., 2, 181–184, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>16</label><mixed-citation>
Chatfield, R. B., Guo, Z., Sachse, G. W., Blake, D. R., and Blake, N. J.:
The subtropical global plume in the Pacific Exploratory Mission-Tropics A
(PEM-Tropics A), PEM-Tropics B, and the Global Atmospheric Sampling Program
(GASP): How tropical emissions affect the remote Pacific, J. Geophys. Res., 107,
4278, <a href="https://doi.org/10.1029/2001JD000497" target="_blank">https://doi.org/10.1029/2001JD000497</a>, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>17</label><mixed-citation>
Coakley, J. and Chylek, P.: The two-stream approximation in radiative
transfer including the angle of the incident radiation, J. Atmos. Sci., 32,
409–418, 1975.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>18</label><mixed-citation>
Cochrane, S. P., Schmidt, K. S., Chen, H., Pilewskie, P., Kittelman, S., Redemann, J., LeBlanc, S., Pistone, K., Kacenelenbogen, M., Segal Rozenhaimer, M., Shinozuka, Y., Flynn, C., Platnick, S., Meyer, K., Ferrare, R., Burton, S., Hostetler, C., Howell, S., Freitag, S., Dobracki, A., and Doherty, S.: Above-cloud aerosol radiative effects based on ORACLES 2016 and ORACLES 2017 aircraft experiments, Atmos. Meas. Tech., 12, 6505–6528, <a href="https://doi.org/10.5194/amt-12-6505-2019" target="_blank">https://doi.org/10.5194/amt-12-6505-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>19</label><mixed-citation>
Coddington, O. M., Pilewskie, P., Redemann, J., Platnick, S., Russell, S. P. B.,
Schmidt, K. S., Gore, W. J., Livingston, J., Wind, G., and Vukicevic, T.:
Examining the impact of overlying aerosols on the retrieval of cloud optical
properties from passive remote sensing, J. Geophys. Res., 115, D10211,
<a href="https://doi.org/10.1029/2009JD012829" target="_blank">https://doi.org/10.1029/2009JD012829</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>20</label><mixed-citation>
Costantino, L. and Bréon, F.-M.: Satellite-based estimate of aerosol direct radiative effect over the South-East Atlantic, Atmos. Chem. Phys. Discuss., 13, 23295–23324, <a href="https://doi.org/10.5194/acpd-13-23295-2013" target="_blank">https://doi.org/10.5194/acpd-13-23295-2013</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>21</label><mixed-citation>
Das, S., Harshvardhan, H., Bian, H., Chin, M., Curci, G., Protonotariou, A.
P. T., Mielonen, K., Zhang, H., Wang, H., and Liu, X.: Biomass burning aerosol
transport and vertical distribution over the South African-Atlantic region,
J. Geophys. Res.-Atmos., 122, 6391–6415, <a href="https://doi.org/10.1002/2016JD026421" target="_blank">https://doi.org/10.1002/2016JD026421</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>22</label><mixed-citation>
Davies, N. W., Fox, C., Szpek, K., Cotterell, M. I., Taylor, J. W., Allan, J. D., Williams, P. I., Trembath, J., Haywood, J. M., and Langridge, J. M.: Evaluating biases in filter-based aerosol absorption measurements using photoacoustic spectroscopy, Atmos. Meas. Tech., 12, 3417–3434, <a href="https://doi.org/10.5194/amt-12-3417-2019" target="_blank">https://doi.org/10.5194/amt-12-3417-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>23</label><mixed-citation>
Deaconu, L. T., Waquet, F., Josset, D., Ferlay, N., Peers, F., Thieuleux, F., Ducos, F., Pascal, N., Tanré, D., Pelon, J., and Goloub, P.: Consistency of aerosols above clouds characterization from A-Train active and passive measurements, Atmos. Meas. Tech., 10, 3499–3523, <a href="https://doi.org/10.5194/amt-10-3499-2017" target="_blank">https://doi.org/10.5194/amt-10-3499-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>24</label><mixed-citation>
Deaconu, L. T., Ferlay, N., Waquet, F., Peers, F., Thieuleux, F., and Goloub, P.: Satellite inference of water vapour and above-cloud aerosol combined effect on radiative budget and cloud-top processes in the southeastern Atlantic Ocean, Atmos. Chem. Phys., 19, 11613–11634, <a href="https://doi.org/10.5194/acp-19-11613-2019" target="_blank">https://doi.org/10.5194/acp-19-11613-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>25</label><mixed-citation>
De Graaf, M., Bellouin, N., Tilstra, L. G., Haywood, J., and Stammes, P.:
Aerosol direct radiative effect of smoke over clouds over the southeast
Atlantic Ocean from 2006 to 2009, Geophys. Res. Lett., 41, 7723–7730,
<a href="https://doi.org/10.1002/2014GL061103" target="_blank">https://doi.org/10.1002/2014GL061103</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>26</label><mixed-citation>
Diamond, M. S., Dobracki, A., Freitag, S., Small Griswold, J. D., Heikkila, A., Howell, S. G., Kacarab, M. E., Podolske, J. R., Saide, P. E., and Wood, R.: Time-dependent entrainment of smoke presents an observational challenge for assessing aerosol–cloud interactions over the southeast Atlantic Ocean, Atmos. Chem. Phys., 18, 14623–14636, <a href="https://doi.org/10.5194/acp-18-14623-2018" target="_blank">https://doi.org/10.5194/acp-18-14623-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>27</label><mixed-citation>
Doherty, S. J., Saide, P., Zuidema, P., Shinozuka, Y., Ferrada, G., Mallet, M., Meyer, K., Painemal, D., Howell, S. G., Freitag, S., Smirnow, N.,Dobracki, A., Podolske, J., Ferrare, R., Burton, S., Nabat, P., Wood, R., and Redemann, J.: Modeled and observed vertically-resolved aerosol and cloud properties related to the direct aerosol radiative effect in the Southeast Atlantic, in preparation, 2021.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>28</label><mixed-citation>
Dubovik, O. and King, M. D.: A flexible inversion algorithm for retrieval
of aerosol optical properties from sun and sky radiance measurements, J.
Geophys. Res., 105, 20673–20696, 2000.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>29</label><mixed-citation>
Dzambo, A. M., L'Ecuyer, T., Sy, O. O., and Tanelli, S.: The Observed
Structure and Precipitation Characteristics of Southeast Atlantic
Stratocumulus from Airborne Radar During ORACLES 2016-17, J. Appl.
Meteorol. Clim., 58, 2197–2215, <a href="https://doi.org/10.1175/jamc-d-19-0032.1" target="_blank">https://doi.org/10.1175/jamc-d-19-0032.1</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>30</label><mixed-citation>
Dzambo, A. M., L'Ecuyer, T., Sinclair, K., van Diedenhoven, B., Gupta, S., McFarquhar, G., O'Brien, J. R., Cairns, B., Wasilewski, A. P., and Alexandrov, M.: Joint Cloud Water Path and Rain Water Path Retrievals from ORACLES Observations, Atmos. Chem. Phys. Discuss., <a href="https://doi.org/10.5194/acp-2020-849" target="_blank">https://doi.org/10.5194/acp-2020-849</a>, in review, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>31</label><mixed-citation>
Eastman, R. and Wood, R. K. T. O: The subtropical stratocumulus-topped
planetary boundary layer: A climatology and the Lagrangian evolution, J.
Atmos. Sci., 74, 2633–2656, <a href="https://doi.org/10.1175/JAS-D-16-0336.1" target="_blank">https://doi.org/10.1175/JAS-D-16-0336.1</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>32</label><mixed-citation>
Eck, T. F., Holben, B. N., Reid, J. S., Mukelabai, M. M., Piketh, S. J., Torres, O., Jethva, H. T., Hyer, E. J.,  Ward, D. E., Dubovik, O., Sinyuk, A., Schafer,  J. S.,  Giles, D. M., Sorokin, M., Smirnov, A., and Slutsker, I.: A seasonal trend of single scattering albedo in southern
African biomass-burning particles: Implications for satellite products and
estimates of emissions for the world's largest biomass-burning source, J.
Geophys. Res. Atmos., 118, 6414–6432, <a href="https://doi.org/10.1002/jgrd.50500" target="_blank">https://doi.org/10.1002/jgrd.50500</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>33</label><mixed-citation>
ECMWF: Describing ECMWF's forecasts and forecasting system,
Newsletter Feature Article, ECMWF, availabel at:
<a href="https://www.ecmwf.int/sites/default/files/elibrary/2012/17412-describing-ecmwfs-forecasts-and-forecasting-system.pdf" target="_blank"/>
(last access: December 2013),
2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>34</label><mixed-citation>
Fishman, J., Hoell, J. M., Bendura, R. D., McNeal, R. J., and Kirchhoff, V.
W. J. H.: NASA GTE TRACE-A Experiment (September–October 1992), Overview,
J. Geophys. Res., 101, 23865–23880, 1996.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>35</label><mixed-citation>
Formenti, P., D'Anna, B., Flamant, C., Mallet, M., Piketh, S. J., Schepanski, K., Waquet, F., Auriol, F., Brogniez, G., Burnet, F., Chaboureau, J., Chauvigné, A., Chazette, P., Denjean, C., Desboeufs, K., Doussin, J., Elguindi, N., Feuerstein, S., Gaetani, M., Giorio, C., Klopper, D., Mallet, M. D., Nabat, P., Monod, A., Solmon, F., Namwoonde, A., Chikwililwa, C., Mushi, R., Welton, E. J., and Holben, B.: The Aerosols, Radiation and Clouds in Southern Africa
Field Campaign in Namibia: Overview, illustrative observations, and way
forward, B. Am. Meteor. Soc., 100, 1277–1298, <a href="https://doi.org/10.1175/BAMS-D-17-0278.1" target="_blank">https://doi.org/10.1175/BAMS-D-17-0278.1</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>36</label><mixed-citation>
Grell, G. A., Peckham, S. E., Schmitz, R., McKeen, S. A., Frost, G., Skamarock,
W. C., and Eder, B.: Fully coupled “online” chemistry within the WRF model, Atmos. Environ., 39, 6957–6975, <a href="https://doi.org/10.1016/j.atmosenv.2005.04.027" target="_blank">https://doi.org/10.1016/j.atmosenv.2005.04.027</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>37</label><mixed-citation>
Gupta, S., McFarquhar, G. M., O'Brien, J. R., Delene, D. J., Poellot, M. R., Dobracki, A., Podolske, J. R., Redemann, J., LeBlanc, S. E., Segal-Rozenhaimer, M., and Pistone, K.: Impact of the Variability in Vertical Separation between Biomass-Burning Aerosols and Marine Stratocumulus on Cloud Microphysical Properties over the Southeast Atlantic, Atmos. Chem. Phys. Discuss. [preprint], <a href="https://doi.org/10.5194/acp-2020-1039" target="_blank">https://doi.org/10.5194/acp-2020-1039</a>, in review, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>38</label><mixed-citation>
Haynes, J. M., L'Ecuyer, T. S., Stephens, G. L., Miller, S. D., Mitrescu, C., Wood, N. B., and Tanelli, S.: Rainfall retrieval over the ocean with spaceborne W‐band radar, J. Geophys. Res., 114, D00A22, <a href="https://doi.org/10.1029/2008JD009973" target="_blank">https://doi.org/10.1029/2008JD009973</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>39</label><mixed-citation>
Haywood, J., Francis, P., Dubovik, O., Glew, M., and Holben, B.: Comparison
of aerosol size distributions, radiative properties, and optical depths
determined by aircraft observations and Sun photometers during SAFARI 2000,
J. Geophys. Res., 108, 8471, <a href="https://doi.org/10.1029/2002JD002250" target="_blank">https://doi.org/10.1029/2002JD002250</a>, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>40</label><mixed-citation>
Haywood, J. M., Osborne, S. R., and Abel, S. J.: The effect of overlying
absorbing aerosol layers on remote sensing retrievals of cloud effective
radius and cloud optical depth, Q. J. Roy. Meteor. Soc., 130, 779–800, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>41</label><mixed-citation>
Haywood, J. M., Abel, S. J., Barrett, P. A., Bellouin, N., Blyth, A., Bower, K. N., Brooks, M., Carslaw, K., Che, H., Coe, H., Cotterell, M. I., Crawford, I., Cui, Z., Davies, N., Dingley, B., Field, P., Formenti, P., Gordon, H., de Graaf, M., Herbert, R., Johnson, B., Jones, A. C., Langridge, J. M., Malavelle, F., Partridge, D. G., Peers, F., Redemann, J., Stier, P., Szpek, K., Taylor, J. W., Watson-Parris, D., Wood, R., Wu, H., and Zuidema, P.: Overview: The CLoud-Aerosol-Radiation Interaction and Forcing: Year-2017 (CLARIFY-2017) measurement campaign, Atmos. Chem. Phys. Discuss., <a href="https://doi.org/10.5194/acp-2020-729" target="_blank">https://doi.org/10.5194/acp-2020-729</a>, in review, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>42</label><mixed-citation>
Herman, J., Cede, A., Spinei, E., Mount, G., Tzortziou, M., and Abuhassan,
N.: NO<sub>2</sub> column amounts from ground-based Pandora and MFDOAS spectrometers
using the direct-sun DOAS technique: Intercomparisons and application to
OMIvalidation, J. Geophys. Res., 114, D13307, <a href="https://doi.org/10.1029/2009JD011848" target="_blank">https://doi.org/10.1029/2009JD011848</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>43</label><mixed-citation>
Herman, J., Evans, R., Cede, A., Abuhassan, N., Petropavlovskikh, I., and McConville, G.: Comparison of ozone retrievals from the Pandora spectrometer system and Dobson spectrophotometer in Boulder, Colorado, Atmos. Meas. Tech., 8, 3407–3418, <a href="https://doi.org/10.5194/amt-8-3407-2015" target="_blank">https://doi.org/10.5194/amt-8-3407-2015</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>44</label><mixed-citation>
Holben, B. N., Eck, T. F., Slutsker, I., Tanre, D., Buis, J. P., Setzer, A.,
Vermote, E., Reagan, J. A., Kaufman, Y., Nakajima, T., Lavenu, F.,
Jankowiak, I., and Smirnov, A.: AERONET – A federated instrument network
and data archive for aerosol characterization, Remote Sens. Environ., 66,
1–16, 1998.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>45</label><mixed-citation>
Holben, B. N., Kim, J., Sano, I., Mukai, S., Eck, T. F., Giles, D. M., Schafer, J. S., Sinyuk, A., Slutsker, I., Smirnov, A., Sorokin, M., Anderson, B. E., Che, H., Choi, M., Crawford, J. H., Ferrare, R. A., Garay, M. J., Jeong, U., Kim, M., Kim, W., Knox, N., Li, Z., Lim, H. S., Liu, Y., Maring, H., Nakata, M., Pickering, K. E., Piketh, S., Redemann, J., Reid, J. S., Salinas, S., Seo, S., Tan, F., Tripathi, S. N., Toon, O. B., and Xiao, Q.: An overview of mesoscale aerosol processes, comparisons, and validation studies from DRAGON networks, Atmos. Chem. Phys., 18, 655–671, <a href="https://doi.org/10.5194/acp-18-655-2018" target="_blank">https://doi.org/10.5194/acp-18-655-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>46</label><mixed-citation>
Huffman, G. J., Adler, R. F., Bolvin, D. T., Gu, G., Nelkin, E. J., Bowman, K. P., Hong, Y., Stocker, E. F.,  Wolff, D. B.: The TRMM Multi-satellite Precipitation
Analysis: Quasi-Global, Multi-Year, Combined-Sensor Precipitation Estimates
at Fine Scale, J.Hydrometeor., 8, 38–55, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>47</label><mixed-citation>
IPCC: Climate Change 2013: The Physical Science Basis. Contribution of
Working Group I to the Fifth Assessment Report of the Intergovernmental
Panel on Climate Change, edited by:
Stocker, T. F., Qin, D., Plattner, G.-K., Tignor,
M., Allen, S. K., Boschung, J., Nauels, A., Xia, Y., Bex, V. and Midgley, P.
M., Cambridge University Press, Cambridge, UK and New
York, USA, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>48</label><mixed-citation>
Jethva, H., Torres, O., Waquet, F., Chand, D., and Hu, Y.: How do A-train
sensors intercompare in the retrieval of above-cloud aerosol optical depth?
A case study-based assessment, Geophys. Res. Lett., 41, 186–192,
<a href="https://doi.org/10.1002/2013GL058405" target="_blank">https://doi.org/10.1002/2013GL058405</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>49</label><mixed-citation>
Jethva, H., Torres, O., Remer, L., Redemann, J., Livingston, J., Dunagan, S., Shinozuka, Y., Kacenelenbogen, M., Rosenheimer, M. S., and Spurr, R.: Validating MODIS above-cloud aerosol optical depth retrieved from “color ratio” algorithm using direct measurements made by NASA's airborne AATS and 4STAR sensors, Atmos. Meas. Tech., 9, 5053–5062, <a href="https://doi.org/10.5194/amt-9-5053-2016" target="_blank">https://doi.org/10.5194/amt-9-5053-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>50</label><mixed-citation>
Jethva, H., Torres, O., and Ahn, C.: A 12-year long global record of optical depth of absorbing aerosols above the clouds derived from the OMI/OMACA algorithm, Atmos. Meas. Tech., 11, 5837–5864, <a href="https://doi.org/10.5194/amt-11-5837-2018" target="_blank">https://doi.org/10.5194/amt-11-5837-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>51</label><mixed-citation>
Kacarab, M., Thornhill, K. L., Dobracki, A., Howell, S. G., O'Brien, J. R., Freitag, S., Poellot, M. R., Wood, R., Zuidema, P., Redemann, J., and Nenes, A.: Biomass burning aerosol as a modulator of the droplet number in the southeast Atlantic region, Atmos. Chem. Phys., 20, 3029–3040, <a href="https://doi.org/10.5194/acp-20-3029-2020" target="_blank">https://doi.org/10.5194/acp-20-3029-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>52</label><mixed-citation>
Kacenelenbogen, M. S., Vaughan, M. A., Redemann, J., Young, S. A., Liu, Z., Hu, Y., Omar, A. H., LeBlanc, S., Shinozuka, Y., Livingston, J., Zhang, Q., and Powell, K. A.: Estimations of global shortwave direct aerosol radiative effects above opaque water clouds using a combination of A-Train satellite sensors, Atmos. Chem. Phys., 19, 4933–4962, <a href="https://doi.org/10.5194/acp-19-4933-2019" target="_blank">https://doi.org/10.5194/acp-19-4933-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>53</label><mixed-citation>
Katich, J. M., Samset, B. H., Bui, T. P., Dollner, M., Froyd, K. D.,
Campuzano-Jost, P., Nault, B. A., Schroder,  J. C.,  Weinzierl, B., and Schwarz, J. P.: Strong contrast in remote black carbon aerosol
loadings between the Atlantic and Pacific basins, J. Geophys.
Res.-Atmos.,123, 13386–13395,
<a href="https://doi.org/10.1029/2018JD029206" target="_blank">https://doi.org/10.1029/2018JD029206</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib54"><label>54</label><mixed-citation>
Keil, A. and Haywood, J. M.: Solar radiative forcing by BB aerosol
particles during SAFARI 2000: A case study based on measured aerosol and
cloud properties, J. Geophys. Res., 108, 8467,
<a href="https://doi.org/10.1029/2002JD002315" target="_blank">https://doi.org/10.1029/2002JD002315</a>, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib55"><label>55</label><mixed-citation>
Knobelspiesse, K., Cairns, B., Jethva, H., Kacenelenbogen, M., Segal-Rosenheimer, M., and Torres, O.: Remote sensing of above cloud aerosols, in: Light Scattering Reviews 9, edited by: Kokhanovsky, A., Springer Praxis Books, Springer, Berlin, Heidelberg, <a href="https://doi.org/10.1007/978-3-642-37985-7_5" target="_blank">https://doi.org/10.1007/978-3-642-37985-7_5</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib56"><label>56</label><mixed-citation>
Koch, D. and Del Genio, A. D.: Black carbon semi-direct effects on cloud cover: review and synthesis, Atmos. Chem. Phys., 10, 7685–7696, <a href="https://doi.org/10.5194/acp-10-7685-2010" target="_blank">https://doi.org/10.5194/acp-10-7685-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib57"><label>57</label><mixed-citation>
Koffi, B., Schulz, M.,  Bréon, F., Griesfeller, J.,  Winker, D., Balkanski, Y., Bauer, S., Berntsen, T., Chin, M.,  Collins, W. D., Dentener, F., Diehl, T., Easter, R., Ghan, S., Ginoux, P., Gong, S., Horowitz, L. W., Iversen, T.,  Kirkevåg, A., Koch, D., Krol, M., Myhre, G., Stier, P., and Takemura, T.: Application of the CALIOP layer product to evaluate the
vertical distribution of aerosols estimated by global models: AeroCom phase
I results, J. Geophys. Res., 117, D10201, <a href="https://doi.org/10.1029/2011JD016858" target="_blank">https://doi.org/10.1029/2011JD016858</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib58"><label>58</label><mixed-citation>
LeBlanc, S.: Moving Lines: NASA airborne research flight
planning tool release (Version v1.21), Zenodo, <a href="https://doi.org/10.5281/zenodo.1478126" target="_blank">https://doi.org/10.5281/zenodo.1478126</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib59"><label>59</label><mixed-citation>
LeBlanc, S. E., Redemann, J., Flynn, C., Pistone, K., Kacenelenbogen, M., Segal-Rosenheimer, M., Shinozuka, Y., Dunagan, S., Dahlgren, R. P., Meyer, K., Podolske, J., Howell, S. G., Freitag, S., Small-Griswold, J., Holben, B., Diamond, M., Wood, R., Formenti, P., Piketh, S., Maggs-Kölling, G., Gerber, M., and Namwoonde, A.: Above-cloud aerosol optical depth from airborne observations in the southeast Atlantic, Atmos. Chem. Phys., 20, 1565–1590, <a href="https://doi.org/10.5194/acp-20-1565-2020" target="_blank">https://doi.org/10.5194/acp-20-1565-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib60"><label>60</label><mixed-citation>
Ma, P.-L., Rasch, P. J., Fast, J. D., Easter, R. C., Gustafson Jr., W. I., Liu, X., Ghan, S. J., and Singh, B.: Assessing the CAM5 physics suite in the WRF-Chem model: implementation, resolution sensitivity, and a first evaluation for a regional case study, Geosci. Model Dev., 7, 755–778, <a href="https://doi.org/10.5194/gmd-7-755-2014" target="_blank">https://doi.org/10.5194/gmd-7-755-2014</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib61"><label>61</label><mixed-citation>
Mallet, M., Nabat, P., Zuidema, P., Redemann, J., Sayer, A. M., Stengel, M., Schmidt, S., Cochrane, S., Burton, S., Ferrare, R., Meyer, K., Saide, P., Jethva, H., Torres, O., Wood, R., Saint Martin, D., Roehrig, R., Hsu, C., and Formenti, P.: Simulation of the transport, vertical distribution, optical properties and radiative impact of smoke aerosols with the ALADIN regional climate model during the ORACLES-2016 and LASIC experiments, Atmos. Chem. Phys., 19, 4963–4990, <a href="https://doi.org/10.5194/acp-19-4963-2019" target="_blank">https://doi.org/10.5194/acp-19-4963-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib62"><label>62</label><mixed-citation>
Mallet, M., Solmon, F., Nabat, P., Elguindi, N., Waquet, F., Bouniol, D., Sayer, A. M., Meyer, K., Roehrig, R., Michou, M., Zuidema, P., Flamant, C., Redemann, J., and Formenti, P.: Direct and semi-direct radiative forcing of biomass-burning aerosols over the southeast Atlantic (SEA) and its sensitivity to absorbing properties: a regional climate modeling study, Atmos. Chem. Phys., 20, 13191–13216, <a href="https://doi.org/10.5194/acp-20-13191-2020" target="_blank">https://doi.org/10.5194/acp-20-13191-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib63"><label>63</label><mixed-citation>
Martin, G. M., Johnson, D. W., and Spice, A.: The measurement and parameterization of effective radius of droplets in warm stratiform clouds, J. Atmos. Sci., 51, 1823–1842, 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib64"><label>64</label><mixed-citation>
Mauger, G. and Norris, J.: Meteorological bias in satellite estimates of
aerosol-cloud relationships, Geophys. Res. Lett., 34,
<a href="https://doi.org/10.1029/2007GL029952" target="_blank">https://doi.org/10.1029/2007GL029952</a>, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib65"><label>65</label><mixed-citation>
Meyer, K., Platnick, S., Oreopoulos, L., and Lee, D.: Estimating the direct
radiative effect of absorbing aerosols overlying marine boundary layer
clouds in the southeast Atlantic using MODIS and CALIOP, J. Geophys. Res.-Atmos., 118, 4801–4815, <a href="https://doi.org/10.1002/jgrd.50449" target="_blank">https://doi.org/10.1002/jgrd.50449</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib66"><label>66</label><mixed-citation>
Meyer, K., Platnick, S., and Zhang, Z.: Simultaneously inferring above-cloud
absorbing aerosol optical thickness and underlying liquid phase cloud
optical and microphysical properties using MODIS, J. Geophys. Res.-Atmos.,
120, 2015JD023128, <a href="https://doi.org/10.1002/2015JD023128" target="_blank">https://doi.org/10.1002/2015JD023128</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib67"><label>67</label><mixed-citation>
Miles, N. L., Verlinde, J., and Clothiaux, E. E.: Cloud droplet size distributions in low-level stratiform clouds, J. Atmos. Sci., 57, 295–311, 2000.
</mixed-citation></ref-html>
<ref-html id="bib1.bib68"><label>68</label><mixed-citation>
Miller, D. J., Segal-Rozenhaimer, M., Knobelspiesse, K., Redemann, J., Cairns, B., Alexandrov, M., van Diedenhoven, B., and Wasilewski, A.: Low-level liquid cloud properties during ORACLES retrieved using airborne polarimetric measurements and a neural network algorithm, Atmos. Meas. Tech., 13, 3447–3470, <a href="https://doi.org/10.5194/amt-13-3447-2020" target="_blank">https://doi.org/10.5194/amt-13-3447-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib69"><label>69</label><mixed-citation>
Minnis, P., Nguyen, L., Palikonda, R., Heck, P. W., Spangenberg, D. A., Doelling, D. R., Ayers, J. K., Smith Jr., W. L., Khaiyer, M. M., Trepte, Q. Z., Avey, L. A., Chang, F.-L., Yost, C. R., Chee, T. L., and Sun-Mack, S.: Near-real
time cloud retrievals from operational and research meteorological
satellites, Proceedings of the SPIE Europe Remote Sens., Cardiff, UK, 15–18
September 2008, 7107-2, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib70"><label>70</label><mixed-citation>
Minnis, P., Sun-Mack, S., Chen, Y., Chang, F.-L., Yost, C. R., Smith Jr., W. L., Heck, P. W., Arduini, R. F., Bedka, S. T., Yi, Y., Hong, G., Jin, Z.,
Painemal, D., Palikonda, R., Scarino, B., Spangenberg, D. A., Smith, R. A.,
Trepte, Q. Z., Yang, P., and Xie, Y.: CERES MODIS cloud product
retrievals for Edition 4, Part I: Algorithm changes, IEEE Trans. Geosci.
Remote Sens., <a href="https://doi.org/10.1109/TGRS.2020.3008866" target="_blank">https://doi.org/10.1109/TGRS.2020.3008866</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib71"><label>71</label><mixed-citation>
Molod, A., Takacs, L., Suarez, M., Bacmeister, J., Song, I.-S., and
Eichmann, A.: The GEOS-5 Atmospheric General Circulation Model: Mean Climate
and Development from MERRA to Fortuna, Technical Report Series on Global
Modeling and Data Assimilation, NASA, Washington, D.C., USA, 28, 124 pp., 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib72"><label>72</label><mixed-citation>
Myhre, G., Samset, B. H., Schulz, M., Balkanski, Y., Bauer, S., Berntsen, T. K., Bian, H., Bellouin, N., Chin, M., Diehl, T., Easter, R. C., Feichter, J., Ghan, S. J., Hauglustaine, D., Iversen, T., Kinne, S., Kirkevåg, A., Lamarque, J.-F., Lin, G., Liu, X., Lund, M. T., Luo, G., Ma, X., van Noije, T., Penner, J. E., Rasch, P. J., Ruiz, A., Seland, Ø., Skeie, R. B., Stier, P., Takemura, T., Tsigaridis, K., Wang, P., Wang, Z., Xu, L., Yu, H., Yu, F., Yoon, J.-H., Zhang, K., Zhang, H., and Zhou, C.: Radiative forcing of the direct aerosol effect from AeroCom Phase II simulations, Atmos. Chem. Phys., 13, 1853–1877, <a href="https://doi.org/10.5194/acp-13-1853-2013" target="_blank">https://doi.org/10.5194/acp-13-1853-2013</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib73"><label>73</label><mixed-citation>
National Academies of Sciences, Engineering, and Medicine: Thriving on Our
Changing Planet: A Decadal Strategy for Earth Observation from Space,
The National Academies Press,
Washington, DC, USA,
<a href="https://doi.org/10.17226/24938" target="_blank">https://doi.org/10.17226/24938</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib74"><label>74</label><mixed-citation>
Nicholls, S. and Leighton, J.: An observational study of the structure of stratiform cloud sheets, Part I: Structure, Q. J. Roy. Meteor. Soc., 112, 431–460, 1986.
</mixed-citation></ref-html>
<ref-html id="bib1.bib75"><label>75</label><mixed-citation>
ORACLES Science Team: Suite of Aerosol, Cloud, and Related Data Acquired
Aboard P3 During ORACLES 2018, Version 2, NASA Ames Earth Science Project
Office,
<a href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2018_V2" target="_blank">https://doi.org/10.5067/Suborbital/ORACLES/P3/2018_V2</a>, 2020a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib76"><label>76</label><mixed-citation>
ORACLES Science Team: Suite of Aerosol, Cloud, and Related Data Acquired
Aboard P3 During ORACLES 2017, Version 2, NASA Ames Earth Science Project
Office, <a href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2017_V2" target="_blank">https://doi.org/10.5067/Suborbital/ORACLES/P3/2017_V2</a>, 2020b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib77"><label>77</label><mixed-citation>
ORACLES Science Team: Suite of Aerosol, Cloud, and Related Data Acquired
Aboard P3 During ORACLES 2016, Version 2, NASA Ames Earth Science Project
Office, <a href="https://doi.org/10.5067/Suborbital/ORACLES/P3/2016_V2" target="_blank">https://doi.org/10.5067/Suborbital/ORACLES/P3/2016_V2</a>, 2020c.
</mixed-citation></ref-html>
<ref-html id="bib1.bib78"><label>78</label><mixed-citation>
ORACLES Science Team: Suite of Aerosol, Cloud, and Related Data Acquired
Aboard ER2 During ORACLES 2016, Version 2, NASA Ames Earth Science Project
Office, <a href="https://doi.org/10.5067/Suborbital/ORACLES/ER2/2016_V2" target="_blank">https://doi.org/10.5067/Suborbital/ORACLES/ER2/2016_V2</a>, 2020d.
</mixed-citation></ref-html>
<ref-html id="bib1.bib79"><label>79</label><mixed-citation>
Painemal, D. and Zuidema, P.: Microphysical variability in southeast Pacific Stratocumulus clouds: synoptic conditions and radiative response, Atmos. Chem. Phys., 10, 6255–6269, <a href="https://doi.org/10.5194/acp-10-6255-2010" target="_blank">https://doi.org/10.5194/acp-10-6255-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib80"><label>80</label><mixed-citation>
Painemal, D. and Zuidema, P.: Assessment of MODIS cloud effective radius
and optical thickness retrievals over the Southeast Pacific with VOCALS-REx
in situ measurements, J. Geophys. Res., 116, D24206,
<a href="https://doi.org/10.1029/2011JD016155" target="_blank">https://doi.org/10.1029/2011JD016155</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib81"><label>81</label><mixed-citation>
Pappenberger, F., Scipal, K., and Buizza, R.: Hydrological aspects of
meteorological verification, Atmospheric Sci. Lett., 9, 43–52, 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib82"><label>82</label><mixed-citation>
Peers, F., Francis, P., Fox, C., Abel, S. J., Szpek, K., Cotterell, M. I., Davies, N. W., Langridge, J. M., Meyer, K. G., Platnick, S. E., and Haywood, J. M.: Observation of absorbing aerosols above clouds over the south-east Atlantic Ocean from the geostationary satellite SEVIRI – Part 1: Method description and sensitivity, Atmos. Chem. Phys., 19, 9595–9611, <a href="https://doi.org/10.5194/acp-19-9595-2019" target="_blank">https://doi.org/10.5194/acp-19-9595-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib83"><label>83</label><mixed-citation>
Pistone, K., Redemann, J., Doherty, S., Zuidema, P., Burton, S., Cairns, B., Cochrane, S., Ferrare, R., Flynn, C., Freitag, S., Howell, S. G., Kacenelenbogen, M., LeBlanc, S., Liu, X., Schmidt, K. S., Sedlacek III, A. J., Segal-Rozenhaimer, M., Shinozuka, Y., Stamnes, S., van Diedenhoven, B., Van Harten, G., and Xu, F.: Intercomparison of biomass burning aerosol optical properties from in situ and remote-sensing instruments in ORACLES-2016, Atmos. Chem. Phys., 19, 9181–9208, <a href="https://doi.org/10.5194/acp-19-9181-2019" target="_blank">https://doi.org/10.5194/acp-19-9181-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib84"><label>84</label><mixed-citation>
Rajapakshe, C., Zhang, Z., Yorks, J. E., Yu, H., Tan, Q., Meyer, K.,
Platnick, S., and Winker, D. M.: Seasonally transported aerosol layers over
southeast Atlantic are closer to underlying clouds than previously reported,
Geophys. Res. Lett., 44, 5818–5825, <a href="https://doi.org/10.1002/2017GL073559" target="_blank">https://doi.org/10.1002/2017GL073559</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib85"><label>85</label><mixed-citation>
Ran, Q., Fu, W., Liu, Y., Li, T. Shi, K., and Sivakumar, B.: Evaluation of
Quantitative Precipitation Predictions by ECMWF, CMA, and UKMO for Flood
Forecasting: Application to Two Basins in China, Nat. Hazards Rev.,
19, 05018003, <a href="https://doi.org/10.1061/(ASCE)NH.1527-6996.0000282" target="_blank">https://doi.org/10.1061/(ASCE)NH.1527-6996.0000282</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib86"><label>86</label><mixed-citation>
Rouault, M.: Bi-annual intrusion of tropical water in the northern Benguela
upwelling, Geophys. Res. Lett., 39, L12606, <a href="https://doi.org/10.1029/GL052099" target="_blank">https://doi.org/10.1029/GL052099</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib87"><label>87</label><mixed-citation>
Saide, P. E., Thompson, G., Eidhammer, T., da Silva, A. M., Pierce, R. B.,
and Carmichael, G. R.: Assessment of biomass burning smoke influence on
environmental conditions for multi-year tornado outbreaks by combining
aerosol-aware microphysics and fire emission constraints, J. Geophys. Res.-Atmos., 121, 10294–10311, <a href="https://doi.org/10.1002/2016JD025056" target="_blank">https://doi.org/10.1002/2016JD025056</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib88"><label>88</label><mixed-citation>
Sakaeda, N., Wood, R., and Rasch, P. J.: Direct and semidirect aerosol effects of southern African biomass burning aerosol, J. Geophys. Res.-Atmos., 116, D12205,
<a href="https://doi.org/10.1029/2010JD015540" target="_blank">https://doi.org/10.1029/2010JD015540</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib89"><label>89</label><mixed-citation>
Sayer, A. M., Hsu, N. C., Bettenhausen, C., Lee, J., Redemann, J., Schmid,
B., and Shinozuka, Y.: Extending “Deep Blue” aerosol retrieval coverage
to cases of absorbing aerosols above clouds: Sensitivity analysis and first
case studies, J. Geophys. Res.-Atmos., 121, 4830–4854, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib90"><label>90</label><mixed-citation>
Sayer, A. M., Hsu, N. C., Lee, J., Kim, W. V., Burton, S., Fenn, M. A., Ferrare, R. A., Kacenelenbogen, M., LeBlanc, S., Pistone, K., Redemann, J., Segal-Rozenhaimer, M., Shinozuka, Y., and Tsay, S.-C.: Two decades observing smoke above clouds in the south-eastern Atlantic Ocean: Deep Blue algorithm updates and validation with ORACLES field campaign data, Atmos. Meas. Tech., 12, 3595–3627, <a href="https://doi.org/10.5194/amt-12-3595-2019" target="_blank">https://doi.org/10.5194/amt-12-3595-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib91"><label>91</label><mixed-citation>
Schulz, M., Textor, C., Kinne, S., Balkanski, Y., Bauer, S., Berntsen, T., Berglen, T., Boucher, O., Dentener, F., Guibert, S., Isaksen, I. S. A., Iversen, T., Koch, D., Kirkevåg, A., Liu, X., Montanaro, V., Myhre, G., Penner, J. E., Pitari, G., Reddy, S., Seland, Ø., Stier, P., and Takemura, T.: Radiative forcing by aerosols as derived from the AeroCom present-day and pre-industrial simulations, Atmos. Chem. Phys., 6, 5225–5246, <a href="https://doi.org/10.5194/acp-6-5225-2006" target="_blank">https://doi.org/10.5194/acp-6-5225-2006</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib92"><label>92</label><mixed-citation>
Segal-Rozenhaimer, M., Miller, D., Knobelspiesse, K., Redemann, J., Cairns,
B., and Alexandrov, M.: Development of neural network retrievals of liquid cloud
properties from multi-angle polarimetric observations, J.
Quant. Spectrosc. Ra., 220, 39–51, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib93"><label>93</label><mixed-citation>
Shinozuka, Y. and Redemann, J.: Horizontal variability of aerosol optical depth observed during the ARCTAS airborne experiment, Atmos. Chem. Phys., 11, 8489–8495, <a href="https://doi.org/10.5194/acp-11-8489-2011" target="_blank">https://doi.org/10.5194/acp-11-8489-2011</a>, 2011.
</mixed-citation></ref-html>
<ref-html id="bib1.bib94"><label>94</label><mixed-citation>
Shinozuka, Y., Saide, P. E., Ferrada, G. A., Burton, S. P., Ferrare, R., Doherty, S. J., Gordon, H., Longo, K., Mallet, M., Feng, Y., Wang, Q., Cheng, Y., Dobracki, A., Freitag, S., Howell, S. G., LeBlanc, S., Flynn, C., Segal-Rosenhaimer, M., Pistone, K., Podolske, J. R., Stith, E. J., Bennett, J. R., Carmichael, G. R., da Silva, A., Govindaraju, R., Leung, R., Zhang, Y., Pfister, L., Ryoo, J.-M., Redemann, J., Wood, R., and Zuidema, P.: Modeling the smoky troposphere of the southeast Atlantic: a comparison to ORACLES airborne observations from September of 2016, Atmos. Chem. Phys., 20, 11491–11526, <a href="https://doi.org/10.5194/acp-20-11491-2020" target="_blank">https://doi.org/10.5194/acp-20-11491-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib95"><label>95</label><mixed-citation>
Simpson, J. and Wiggert, V.: Models of precipitating cumulus towers, Mon. Weather Rev., 97, 471–489, 1969.
</mixed-citation></ref-html>
<ref-html id="bib1.bib96"><label>96</label><mixed-citation>
Skamarock, W. C., Klemp, J., Dudhia, J., Gill, D. O., Barker, D., Wang,
W., and Powers, J. G.: A Description of the Advanced Research, WRF, Version 3.27.3-27, NCAR Technical Notes, NCAR/TN-4751STR, available at: <a href="https://opensky.ucar.edu/islandora/object/technotes:500/datastream/PDF/view" target="_blank"/> (last access: December 2020), 2008.
</mixed-citation></ref-html>
<ref-html id="bib1.bib97"><label>97</label><mixed-citation>
Sorooshian, A., Feingold, G., Lebsock, M. D., Jiang, H., and Stephens, G. L.:
On the Precipitation Susceptibility of Clouds to Aerosol Perturbations,
Geophys. Res. Lett., 36, 13, <a href="https://doi.org/10.1029/2009GL038993" target="_blank">https://doi.org/10.1029/2009GL038993</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib98"><label>98</label><mixed-citation>
Stier, P., Schutgens, N. A. J., Bellouin, N., Bian, H., Boucher, O., Chin, M., Ghan, S., Huneeus, N., Kinne, S., Lin, G., Ma, X., Myhre, G., Penner, J. E., Randles, C. A., Samset, B., Schulz, M., Takemura, T., Yu, F., Yu, H., and Zhou, C.: Host model uncertainties in aerosol radiative forcing estimates: results from the AeroCom Prescribed intercomparison study, Atmos. Chem. Phys., 13, 3245–3270, <a href="https://doi.org/10.5194/acp-13-3245-2013" target="_blank">https://doi.org/10.5194/acp-13-3245-2013</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib99"><label>99</label><mixed-citation>
Swap, R. J., Annegarn, H. J., Suttles, J. T., King, M. D., Platnick, S.,
Privette, J. L., and Scholes, R. J.: Africa burning: A thematic analysis of
the Southern African Regional Science Initiative (SAFARI 2000), J. Geophys.
Res., 108, 8465, <a href="https://doi.org/10.1029/2003JD003747" target="_blank">https://doi.org/10.1029/2003JD003747</a>, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib100"><label>100</label><mixed-citation>
Szczodrak, M., Austin, P. H., and Krummel, P. B.: Variability of Optical
Depth and Effective Radius in Marine Stratocumulus Clouds, J. Atmos. Sci.,
58, 2912–2926, <a href="https://doi.org/10.1175/1520-0469(2001)058&lt;2912:VOODAE&gt;2.0.CO;2" target="_blank">https://doi.org/10.1175/1520-0469(2001)058&lt;2912:VOODAE&gt;2.0.CO;2</a>, 2001.
</mixed-citation></ref-html>
<ref-html id="bib1.bib101"><label>101</label><mixed-citation>
Twomey, S.: Pollution and the planetary albedo, Atmos. Environ., 8,
1251–1256, 1974.
</mixed-citation></ref-html>
<ref-html id="bib1.bib102"><label>102</label><mixed-citation>
Tzortziou, M., Herman, J. R., Cede, A., and Abuhassan, N.: High precision,
absolute total column ozone measurements from the Pandora spectrometer
system: Comparisons with data from a Brewer double monochromator and
AuraOMI, J. Geophys. Res., 117, D16303, <a href="https://doi.org/10.1029/2012JD017814" target="_blank">https://doi.org/10.1029/2012JD017814</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib103"><label>103</label><mixed-citation>
van der Werf, G. R., Randerson, J. T., Giglio, L., Collatz, G. J., Mu, M., Kasibhatla, P. S., Morton, D. C., DeFries, R. S., Jin, Y., and van Leeuwen, T. T.: Global fire emissions and the contribution of deforestation, savanna, forest, agricultural, and peat fires (1997–2009), Atmos. Chem. Phys., 10, 11707–11735, <a href="https://doi.org/10.5194/acp-10-11707-2010" target="_blank">https://doi.org/10.5194/acp-10-11707-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib104"><label>104</label><mixed-citation>
Watson-Parris, D., Schutgens, N., Winker, D., Burton, S., Ferrare, R.,
Stier, P.: On the Limits of CALIOP for Constraining Modeled Free Tropospheric
Aerosol, Geophys. Res. Lett., 45, 9260–9266, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib105"><label>105</label><mixed-citation>
Werdell, P. J., Behrenfeld, M. J., Bontempi, P. S., Boss, E., Cairns, B.,
Davis, G. T., Franz, B. A., Gliese, U. B., Gorman, E. T., Hasekamp, O.,
Knobelspiesse, K. D., Mannino, A., Martins, J. V., McClain, C. R., Meister,
G., and Remer, L. A.: The Plankton, Aerosol, Cloud, ocean Ecosystem (PACE)
mission: Status, science, advances, B. Am. Meteorol.
Soc., 100, 1775–1794 <a href="https://doi.org/10.1175/bams-d-18-0056.1" target="_blank">https://doi.org/10.1175/bams-d-18-0056.1</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib106"><label>106</label><mixed-citation>
Wilcox, E. M.: Direct and semi-direct radiative forcing of smoke aerosols over clouds, Atmos. Chem. Phys., 12, 139–149, <a href="https://doi.org/10.5194/acp-12-139-2012" target="_blank">https://doi.org/10.5194/acp-12-139-2012</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib107"><label>107</label><mixed-citation>
Wood, R.: Cancellation of aerosol indirect effects in marine stratocumulus through cloud thinning, J. Atmos. Sci., 64, 2657–2669, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib108"><label>108</label><mixed-citation>
Wood, R.: Stratocumulus clouds, Mon. Weather Rev., 140, 2373–2423, <a href="https://doi.org/10.1175/MWR-D-11-00121.1" target="_blank">https://doi.org/10.1175/MWR-D-11-00121.1</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib109"><label>109</label><mixed-citation>
Wood, R., Leon, D., Lebsock, M., Snider, J., and Clarke, A. D.:
Precipitation Driving of Droplet Concentration Variability in Marine Low
Clouds: PRECIPITATION DRIVING OF DROP CONC, J. Geophys. Res.-Atmos., 117, D19,  <a href="https://doi.org/10.1029/2012JD018305" target="_blank">https://doi.org/10.1029/2012JD018305</a>,
2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib110"><label>110</label><mixed-citation>
Wu, H., Taylor, J. W., Szpek, K., Langridge, J. M., Williams, P. I., Flynn, M., Allan, J. D., Abel, S. J., Pitt, J., Cotterell, M. I., Fox, C., Davies, N. W., Haywood, J., and Coe, H.: Vertical variability of the properties of highly aged biomass burning aerosol transported over the southeast Atlantic during CLARIFY-2017, Atmos. Chem. Phys., 20, 12697–12719, <a href="https://doi.org/10.5194/acp-20-12697-2020" target="_blank">https://doi.org/10.5194/acp-20-12697-2020</a>, 2020.
</mixed-citation></ref-html>
<ref-html id="bib1.bib111"><label>111</label><mixed-citation>
Xu, F., van Harten, G., Diner, D., Davis, A., Seidel, F., Rheingans, B.,
Tosca, M., Alexandrov, M., Cairns, B., Ferrare, R., Burton, S., Fenn, M. A., Hostetler, C. A., Wood, R., and Redemann, J.:
Coupled Retrieval of Liquid Water Cloud and Above-Cloud Aerosol Properties
using the Airborne Multiangle SpectroPolarimetric Imager (AirMSPI), J.
Geophys. Res.-Atmos., 123, 3175–3204, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib112"><label>112</label><mixed-citation>
Ye, J., He, Y., Pappenberger, F., Cloke, H. L., Manful, D. Y., and Li, Z.:
Evaluation of ECMWF medium-range ensemble forecasts of precipitation for
river basins, Q. J. R. Meteor. Soc., 140, 1615–1628, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib113"><label>113</label><mixed-citation>
Yu, H. and Zhang, Z.: New Directions: Emerging satellite observations of
above-cloud aerosols and direct radiative forcing, Atmos. Environ.,
72, 36–40, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib114"><label>114</label><mixed-citation>
Yu, H., Zhang, Y., Chin, M., Liu, Z., Omar, A., Remer, L. A., Yang, Y., Yuan,
T., and Zhang, J.: An Integrated Analysis of Aerosol above Clouds from
A-Train Multi-sensor Measurements, Rem. Sens. Environ., 121, 125–131,
<a href="https://doi.org/10.1016/j.rse.2012.01.011" target="_blank">https://doi.org/10.1016/j.rse.2012.01.011</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib115"><label>115</label><mixed-citation>
Zhang, J. and Zuidema, P.: The diurnal cycle of the smoky marine boundary layer observed during August in the remote southeast Atlantic, Atmos. Chem. Phys., 19, 14493–14516, <a href="https://doi.org/10.5194/acp-19-14493-2019" target="_blank">https://doi.org/10.5194/acp-19-14493-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib116"><label>116</label><mixed-citation>
Zhang, Z., Meyer, K., Yu, H., Platnick, S., Colarco, P., Liu, Z., and Oreopoulos, L.: Shortwave direct radiative effects of above-cloud aerosols over global oceans derived from 8 years of CALIOP and MODIS observations, Atmos. Chem. Phys., 16, 2877–2900, <a href="https://doi.org/10.5194/acp-16-2877-2016" target="_blank">https://doi.org/10.5194/acp-16-2877-2016</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib117"><label>117</label><mixed-citation>
Zuidema, P., Painemal, D., deSzoeke, S., and Fairall, C.: Stratocumulus cloud
top height estimates and their climatic implications, J. Climate, 22,
4652–4666, <a href="https://doi.org/10.1175/2009JCLI2708.1" target="_blank">https://doi.org/10.1175/2009JCLI2708.1</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib118"><label>118</label><mixed-citation>
Zuidema, P., Chiu, C., Fairall, C. W., Ghan, S. J., Kollias, P., McFarguhar,
G. M., Mechem, D. B., Romps, D. M., Wong, H., Yuter, S. E., Alvarado, M. J.,
DeSzoeke, S. P., Feingold, G.,
Haywood, J. M.,
Lewis, E. R., McComiskey, A.,
Redemann, J., Turner, D. D., Wood, R., and Zhu, P.: Layered Atlantic Smoke
Interactions with Clouds (LASIC) Science Plan, DOE/SC-ARM-14-037, availabe at:
<a href="http://www.osti.gov/scitech/servlets/purl/1232658" target="_blank"/> (last access: December 2018), 2015.

</mixed-citation></ref-html>
<ref-html id="bib1.bib119"><label>119</label><mixed-citation>
Zuidema, P., Redemann, J., Haywood, J., Wood, R., Piketh, S., Hipondoka, M., and
Formenti, P.: Smoke and Clouds above the Southeast Atlantic: Upcoming Field
Campaigns Probe Absorbing Aerosol's Impact on Climate, B.
Am. Meteorol. Soc., 97, 1131–1135, <a href="https://doi.org/10.1175/BAMS-D-15-00082.1" target="_blank">https://doi.org/10.1175/BAMS-D-15-00082.1</a>, 2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib120"><label>120</label><mixed-citation>
Zuidema, P., Sedlacek III, A. J., Flynn, C., Springston, S., Delgadillo, R.,
Zhang, J., Aiken, A. C., Koontz, A., and Muradyan, P.: The Ascension Island boundary layer in the remote
southeast Atlantic is often smoky, Geophys. Res. Lett., 45,
4456–4465, <a href="https://doi.org/10.1002/2017GL076926" target="_blank">https://doi.org/10.1002/2017GL076926</a>, 2018.
</mixed-citation></ref-html>--></article>
