<?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-21-8111-2021</article-id><title-group><article-title>The role of coarse aerosol particles as a sink of HNO<inline-formula><mml:math id="M1" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> in wintertime pollution events in the Salt Lake Valley</article-title><alt-title>The role of coarse aerosol particles as a sink of HNO<inline-formula><mml:math id="M2" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula></alt-title>
      </title-group><?xmltex \runningtitle{The role of coarse aerosol particles as a sink of HNO${}_{{3}}$}?><?xmltex \runningauthor{A. Hrdina et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff6">
          <name><surname>Hrdina</surname><given-names>Amy</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2126-8060</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Murphy</surname><given-names>Jennifer G.</given-names></name>
          <email>jen.murphy@utoronto.ca</email>
        <ext-link>https://orcid.org/0000-0001-8865-5463</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Hallar</surname><given-names>Anna Gannet</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Lin</surname><given-names>John C.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2794-184X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff7">
          <name><surname>Moravek</surname><given-names>Alexander</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-4342-8173</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Bares</surname><given-names>Ryan</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff8">
          <name><surname>Petersen</surname><given-names>Ross C.</given-names></name>
          
        <ext-link>https://orcid.org/0009-0005-6147-7499</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff4">
          <name><surname>Franchin</surname><given-names>Alessandro</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Middlebrook</surname><given-names>Ann M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2984-6304</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5 aff9">
          <name><surname>Goldberger</surname><given-names>Lexie</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1507-6422</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Lee</surname><given-names>Ben H.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Baasandorj</surname><given-names>Munkh</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Brown</surname><given-names>Steven S.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7477-9078</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department of Chemistry, University of Toronto, Toronto, ON, M5S 0A6, Canada</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Atmospheric Sciences, University of Utah, Salt Lake
City, UT 84112, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Chemical Sciences Laboratory, NOAA Earth System Research Laboratories (ESRL), Boulder, CO 80305, USA</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Cooperative Institute for Research in Environmental Sciences (CIRES), University of Colorado, Boulder, CO 80309, USA</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Department of Atmospheric Sciences, University of Washington, Seattle, WA 98195, USA</institution>
        </aff>
        <aff id="aff6"><label>a</label><institution>now at: Department of Civil and Environmental Engineering,
Massachusetts Institute of Technology,<?xmltex \hack{\break}?> Cambridge, MA 02139, USA</institution>
        </aff>
        <aff id="aff7"><label>b</label><institution>now at: Department of Chemistry, York University, Toronto, ON,
M3J 1P3, Canada</institution>
        </aff>
        <aff id="aff8"><label>c</label><institution>now at: Department of Physical Geography and Ecosystem
Science, Lund University, Lund, Sweden</institution>
        </aff>
        <aff id="aff9"><label>d</label><institution>now at: Pacific Northwest National Laboratory, Richland, WA 99352, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Jennifer G. Murphy (jen.murphy@utoronto.ca)</corresp></author-notes><pub-date><day>27</day><month>May</month><year>2021</year></pub-date>
      
      <volume>21</volume>
      <issue>10</issue>
      <fpage>8111</fpage><lpage>8126</lpage>
      <history>
        <date date-type="received"><day>11</day><month>January</month><year>2020</year></date>
           <date date-type="rev-request"><day>29</day><month>January</month><year>2020</year></date>
           <date date-type="rev-recd"><day>16</day><month>March</month><year>2021</year></date>
           <date date-type="accepted"><day>23</day><month>March</month><year>2021</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="d1e266">Wintertime ammonium nitrate (NH<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M4" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>) pollution events
burden urban mountain basins around the globe. In the Salt Lake Valley of
Utah in the United States, such pollution events are often driven by the
formation of persistent cold-air pools (PCAPs) that trap emissions near the
surface for several consecutive days. As a result, secondary pollutants
including fine particulate matter less than 2.5 <inline-formula><mml:math id="M5" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m in diameter
(PM<inline-formula><mml:math id="M6" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>), largely in the form of NH<inline-formula><mml:math id="M7" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M8" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, build up during these
events and lead to severe haze. As part of an extensive measurement campaign
to understand the chemical processes underlying PM<inline-formula><mml:math id="M9" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> formation, the
2017 Utah Winter Fine Particulate Study, water-soluble trace gases and
PM<inline-formula><mml:math id="M10" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> constituents were continuously monitored using the ambient ion
monitoring ion chromatograph (AIM-IC) system at the University of Utah
campus. Gas-phase NH<inline-formula><mml:math id="M11" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, HNO<inline-formula><mml:math id="M12" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, HCl, and SO<inline-formula><mml:math id="M13" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> along with
particulate NH<inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, Na<inline-formula><mml:math id="M15" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, K<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, Mg<inline-formula><mml:math id="M17" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, Ca<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>,
NO<inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, Cl<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>, and SO<inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> were measured from 21 January
to 21 February 2017. During the two PCAP events captured, the fine
particulate matter was dominated by secondary NH<inline-formula><mml:math id="M22" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M23" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>. The
comparison of total nitrate (HNO<inline-formula><mml:math id="M24" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M25" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> PM<inline-formula><mml:math id="M26" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> NO<inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>) and
total NH<inline-formula><mml:math id="M28" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> (NH<inline-formula><mml:math id="M29" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M30" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> PM<inline-formula><mml:math id="M31" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> NH<inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>) showed NH<inline-formula><mml:math id="M33" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> was
in excess during both pollution events. However, chemical composition
analysis of the snowpack during the first PCAP event revealed that the total
concentration of deposited NO<inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> was nearly 3 times greater
than that of deposited NH<inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>. Daily snow composition measurements
showed a strong correlation between NO<inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and Ca<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> in the
snowpack. The presence of non-volatile salts (Na<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, Ca<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and
Mg<inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>), which are frequently associated with coarse-mode dust, was also
detected in PM<inline-formula><mml:math id="M41" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> by the AIM-IC during the two PCAP events,
accounting for roughly 5 % of total mass loading. The presence of a
significant particle mass and surface area in the coarse mode during the
first PCAP event was indicated by size-resolved particle measurements from
an aerodynamic particle sizer. Taken together, these observations imply that
atmospheric measurements of the gas-phase and fine-mode particle nitrate may
not represent the total burden of nitrate in the atmosphere, implying a
potentially significant role for uptake by coarse-mode dust. Using the
NO<inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> : NH<inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> ratio observed in the snowpack to estimate the
proportion of atmospheric nitrate present in the coarse mode, we estimate
that the amount of secondary NH<inline-formula><mml:math id="M44" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M45" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> could double in the absence of
the coarse-mode sink. The underestimation of total nitrate indicates an
incomplete account of the total oxidant<?pagebreak page8112?> production during PCAP events. The
ability of coarse particles to permanently remove HNO<inline-formula><mml:math id="M46" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and influence
PM<inline-formula><mml:math id="M47" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> formation is discussed using information about particle
composition and size distribution.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e733">Episodes with high particulate matter (PM) pollution occur frequently in
urban air basins across the globe during winter months when a stable
boundary layer persists for multiple days, including in the mountain valleys in
the western USA
(Baasandorj
et al., 2017; Bares et al., 2018; Green et al., 2015; Silcox et al., 2012;
Whiteman et al., 2014), the Po Valley in Italy
(Bernardoni
et al., 2017; Vecchi et al., 2018), and the Sichuan
(Tian et al., 2019) and Twin-Hu
(Gao et
al., 2019) basins in China. These mountain basins, including the Salt Lake
Valley (SLV) in northern Utah, experience strong temperature inversions that
develop into persistent cold-air pools (PCAPs), which suppress vertical
mixing and trap emissions within a shallow boundary layer
(Lareau
et al., 2013; Whiteman et al., 2014). Under these conditions, mass loadings
of fine particles smaller than 2.5 <inline-formula><mml:math id="M48" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m (PM<inline-formula><mml:math id="M49" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>) often reach values
of 60–80 <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M51" 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> in the western USA, which are far above the US
National Ambient Air Quality Standard (35 <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M53" 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>, 24 h average)
(Lareau
et al., 2013; Silcox et al., 2012; Whiteman et al., 2014). Along with
environmental impacts such as haze and localized deposition, mass loadings
of PM<inline-formula><mml:math id="M54" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> that exceed this standard have been associated with increased
risk of mortality, especially cardiopulmonary or cardiovascular disease
mortality
(Pope et
al., 2003, 2017). However, despite significant societal concerns about the
impact on human health from these PM<inline-formula><mml:math id="M55" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> pollution episodes and their
common occurrence around the world, the major chemical processes that drive
PM formation in these regions are still uncertain.</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="d1e814">Processes influencing the concentrations of NH<inline-formula><mml:math id="M56" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, NO<inline-formula><mml:math id="M57" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>,
HNO<inline-formula><mml:math id="M58" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, and NH<inline-formula><mml:math id="M59" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M60" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>. Pathways that occur during the day are shown
in dashed grey arrows, while pathways that occur during the night are shown
in black. The rate of uptake of HNO<inline-formula><mml:math id="M61" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> to coarse particles, <inline-formula><mml:math id="M62" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> PM<inline-formula><mml:math id="M63" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>, composed of CaCO<inline-formula><mml:math id="M64" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and/or NaCl is unknown.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/8111/2021/acp-21-8111-2021-f01.png"/>

      </fig>

      <p id="d1e903">Several studies conducted in northern Utah have shown that PM<inline-formula><mml:math id="M65" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> during
these PCAP episodes is predominantly composed of ammonium nitrate
(NH<inline-formula><mml:math id="M66" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M67" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>), accounting for roughly 60 %–80 % of the total dry particle mass (Baasandorj
et al., 2017; Franchin et al., 2018; Hansen et al., 2013; Kelly et al.,
2013; Kuprov et al., 2014; Long et al., 2002, 2003; Mangelson et al., 1997).
NH<inline-formula><mml:math id="M68" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M69" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation is thermodynamically favorable under conditions
with low temperatures and high relative humidity based on equilibrium
partitioning with gas-phase ammonia (NH<inline-formula><mml:math id="M70" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>) and nitric acid (HNO<inline-formula><mml:math id="M71" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>)
(Mozurkewich,
1993; Nowak et al., 2010; Seinfeld and Pandis, 2006), illustrated in the
right-hand portion of Fig. 1.</p>
      <p id="d1e971">NH<inline-formula><mml:math id="M72" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> emissions are often associated with agricultural activities and
waste disposal; however, in recent years automotive emissions and industrial
processes have become increasingly important sources in urban areas
(Behera
et al., 2013; Bishop et al., 2010, 2016; Livingston et al., 2009; Nowak et
al., 2012; Roth et al., 2019; Suarez-Bertoa et al., 2014; Sun et al., 2017).
In contrast, HNO<inline-formula><mml:math id="M73" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> is formed in the atmosphere and is a major sink of
nitrogen oxides, which are emitted primarily through fossil fuel combustion.
The two dominant mechanisms highlighted in Fig. 1 that lead to HNO<inline-formula><mml:math id="M74" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
occur either (1) from oxidation of NO<inline-formula><mml:math id="M75" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> via reaction with OH (in orange),
which is photochemically driven during the day, or (2) through heterogenous
uptake of N<inline-formula><mml:math id="M76" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O<inline-formula><mml:math id="M77" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">5</mml:mn></mml:msub></mml:math></inline-formula> (in black), which typically occurs at night. Gas-phase HNO<inline-formula><mml:math id="M78" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and NH<inline-formula><mml:math id="M79" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and particulate NH<inline-formula><mml:math id="M80" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M81" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> are removed
from the atmosphere through dry and wet deposition under typical atmospheric
conditions. However, under PCAP conditions, the stably stratified boundary
layer reduces convective mixing, which in turn allows pollutants to
accumulate. In addition, HNO<inline-formula><mml:math id="M82" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> can also be lost through heterogenous
reaction with dust and sea salt components, such as CaCO<inline-formula><mml:math id="M83" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and NaCl
(Beichert
and Finlayson-Pitts, 1996; Dasgupta et al., 2007; Fenter et al., 1994; Liu
et al., 2008a). When the loss of HNO<inline-formula><mml:math id="M84" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> to deposition is suppressed under
PCAP conditions, the loss to reactive uptake to airborne dust and sea salt
can potentially become more important.</p>
      <p id="d1e1093">To formulate effective control strategies that reduce wintertime PM<inline-formula><mml:math id="M85" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>
in northern Utah, measurement campaigns have been conducted to improve our
understanding of fine particulate formation during these PCAP episodes (Baasandorj
et al., 2017; Bares et al., 2018; Hansen et al., 2010; Kelly et al., 2013;
Kuprov et al., 2014; Lareau et al., 2013; Malek et al., 2006; Mangelson et
al., 1997; Silcox et al., 2012; Whiteman et al., 2014). Several analyses of
the PM build-up in cold-air pool events in the SLV have been published, all
based on measurements from one or several ground sites
(Baasandorj
et al., 2017; Kuprov et al., 2014; Long et al., 2003; Silcox et al., 2012).
Long-term PM<inline-formula><mml:math id="M86" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> composition measurements in the SLV are made using
filter samples
(Kelly
et al., 2013; Kuprov et al., 2014; Long et al., 2003; Mangelson et al.,
1997; Silcox et al., 2012; Whiteman et al., 2014), with PM<inline-formula><mml:math id="M87" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>
speciation carried out on filter extracts in accordance with the US Environmental
Protection Agency (EPA) Speciation Trends Network (STN) protocol. Kuprov
et al. (2014) were the first to report the gas and PM<inline-formula><mml:math id="M88" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> composition
during pollution events in northern Utah using an ambient ion monitoring ion chromatograph (AIM-IC) system; however, this study only measured
anionic species, providing HNO<inline-formula><mml:math id="M89" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and particle nitrate (<inline-formula><mml:math id="M90" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>)
concentrations at an hourly resolution. Ambient NH<inline-formula><mml:math id="M92" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> concentrations were
monitored using a chemiluminescence-based NH<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> analyzer, but particulate
ammonium (<inline-formula><mml:math id="M94" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NH<inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>) had to be inferred based on the assumption that
both <inline-formula><mml:math id="M96" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and particulate sulfate (<inline-formula><mml:math id="M98" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>SO<inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>) were in the
form of their respective ammonium salts. Particle mass fractions of crustal
and carbonaceous material in PM<inline-formula><mml:math id="M100" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> were calculated on 24 h average
measurements of Al, Si, and elemental and organic carbon in fine particles from
the NCore program (US EPA, 2010).</p>
      <p id="d1e1249">Recent research in the SLV has focused on determining whether ammonium
nitrate mass loading is most sensitive to reductions in NH<inline-formula><mml:math id="M101" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> or
HNO<inline-formula><mml:math id="M102" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> to inform PM<inline-formula><mml:math id="M103" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> reduction<?pagebreak page8113?> strategies
(Kuprov et al.,
2014). Baasandorj et al. (2017) recently proposed that PM<inline-formula><mml:math id="M104" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> forms
overnight in the upper layers of the PCAP and mixes down to the surface,
enhancing the total PM<inline-formula><mml:math id="M105" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> loading experienced in the SLV. This
explanation of stratified particulate nitrate chemistry throughout PCAP
events suggests a complex coupling of a HNO<inline-formula><mml:math id="M106" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-limited surface layer with
a NH<inline-formula><mml:math id="M107" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-limited elevated layer
(Baasandorj et al., 2017).
Aircraft measurements during the 2017 Utah Winter Fine Particulate Study
(UWFPS) provided the first detailed vertically resolved chemical composition
of these PCAP episodes in the SLV. Analysis presented in McDuffie et al. (2019) confirms that the formation of NH<inline-formula><mml:math id="M108" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M109" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> during these
pollution events is largely limited by HNO<inline-formula><mml:math id="M110" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> but with more frequent
periods approaching NH<inline-formula><mml:math id="M111" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-limited conditions in the upper boundary layer
over time
(McDuffie et
al., 2019). Regimes of both NH<inline-formula><mml:math id="M112" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-limited and HNO<inline-formula><mml:math id="M113" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-limited
conditions are also consistent with an aerosol thermodynamic model
sensitivity study of the same data by Franchin et al. (2018), who found
simulations of non-refractory PM<inline-formula><mml:math id="M114" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> mass were sensitive to reductions in
both total ammonium and total nitrate
(Franchin et al., 2018).
Box model studies of the odd oxygen budget during UWFPS by Womack et al. (2019) assumed that NH<inline-formula><mml:math id="M115" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M116" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation during PCAP episodes is
HNO<inline-formula><mml:math id="M117" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-limited, and found full episodes tend to be NO<inline-formula><mml:math id="M118" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>-saturated. In
conditions where <inline-formula><mml:math id="M119" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> production is HNO<inline-formula><mml:math id="M121" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-limited, it is
often assumed that reduction in NO<inline-formula><mml:math id="M122" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> would directly lead to reductions
in HNO<inline-formula><mml:math id="M123" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>. However, Womack et al. (2019) showed the production of
HNO<inline-formula><mml:math id="M124" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, and therefore, NH<inline-formula><mml:math id="M125" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M126" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation, is sensitive to
changes in VOC concentrations emphasizing the complexity of chemical
processes involved in PM formation under these conditions.</p>
      <p id="d1e1491">The balance of factors influencing HNO<inline-formula><mml:math id="M127" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation are still being
understood. Modelling results from both McDuffie et al. (2019) and Womack et
al. (2019) predict that up to <inline-formula><mml:math id="M128" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 50 % of HNO<inline-formula><mml:math id="M129" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
production is from the heterogeneous N<inline-formula><mml:math id="M130" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O<inline-formula><mml:math id="M131" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">5</mml:mn></mml:msub></mml:math></inline-formula> pathway in the residual
layer. This is in line with ground-based measurements of N<inline-formula><mml:math id="M132" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O<inline-formula><mml:math id="M133" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">5</mml:mn></mml:msub></mml:math></inline-formula> by
Baasandorj et al. (2017) highlighting the importance of nighttime pathway
(Baasandorj et al., 2017). Less
attention has been paid to the possibility that alternate sinks for
HNO<inline-formula><mml:math id="M134" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> may also significantly limit the amount of nitrate that can
contribute to PM<inline-formula><mml:math id="M135" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> formation.</p>
      <p id="d1e1574">Here, results are presented from ground site observations in Salt Lake City
from a moderately elevated site at the edge of the SLV during the UWFPS
campaign in January and February 2017. Atmospheric concentrations of
inorganic trace gases and water-soluble PM<inline-formula><mml:math id="M136" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> constituents were
measured by an AIM-IC, equipped with both cation and anion ion
chromatographs. During PCAP episodes, we observed the formation and build-up
of NH<inline-formula><mml:math id="M137" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M138" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> over several days. Between the hours of 08:00 and 18:00 mountain standard time (MST)
on several PCAP days, we also observed the presence of elevated levels of
non-volatile cations in PM<inline-formula><mml:math id="M139" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>. To investigate the role of
mineral–coarse-mode aerosols in limiting the availability of HNO<inline-formula><mml:math id="M140" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> during
these events, the final section presents estimates of HNO<inline-formula><mml:math id="M141" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> lifetime
against reactive uptake onto mineral–coarse-mode dust based on aerodynamic
particle sizer (APS) data and estimates of the total nitrate budget using
the chemical composition of the snowpack measured during UWFPS.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Site description</title>
      <p id="d1e1647">The SLV (1300 km<inline-formula><mml:math id="M142" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) is a mountain basin in northern Utah surrounded by
steep mountain ranges with the Great Salt Lake sitting to the northwest. The
Wasatch Mountains (peak at 3636 m a.s.l.) span the entire eastern border of the
valley with the Oquirrh Mountains (peak at 3235 m a.s.l.) to the west. There is
a narrow passage in the southern Traverse Range (1878 m a.s.l.) that creates a
small opening into<?pagebreak page8114?> the Utah Valley. Salt Lake City sits at the base of the
valley (1288 m a.s.l.), making a vast elevation difference between the
metropolis and the surrounding mountains. Measurements were conducted from
the rooftop of the William Brown Building 33 m above ground level at the
University of Utah (UU) located 40<inline-formula><mml:math id="M143" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>45<inline-formula><mml:math id="M144" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>58.7<inline-formula><mml:math id="M145" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 111<inline-formula><mml:math id="M146" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>50<inline-formula><mml:math id="M147" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>51.6<inline-formula><mml:math id="M148" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> W, in Salt Lake City. The UU site is located 155 m above the valley
floor along the northeast sidewall of the SLV. The site is impacted by local
traffic that enters the university on the north side of campus.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Instrumentation</title>
      <p id="d1e1728">Hourly averages of PM<inline-formula><mml:math id="M149" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> chemical composition and gas-phase precursors
were measured using an online continuous AIM-IC instrument (Model 9000D, URG
Corp, Chapel Hill, NC). Briefly, gases and particles are sampled from the
same airflow by passing through a short inlet with elements for size
selection (PM<inline-formula><mml:math id="M150" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> impactor), gas collection (wet parallel plate
denuder), and particle capture (saturation chamber) at a flow rate of 3 L min<inline-formula><mml:math id="M151" 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>. Aqueous solutions containing analytes originally in the gas and
particle phases are separately transferred through 22 m inlet lines into 5 mL glass syringes that are subsequently analyzed by ion chromatographs (ICs) following hour-long
collection periods. More in-depth details about the AIM-IC system, including
important adaptations from the standard commercial system, can be found in
Markovic et al. (2012). During the UWFPS campaign, the components of the
inlet assembly were housed in a small weatherproof box 2 m above the roof of
the UU site and the IC systems were housed in a laboratory below. Standard
calibrations of the ICs were performed offline using mixed ion standard
solutions before and after the measurement period. Charged species
(Na<inline-formula><mml:math id="M152" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, NH<inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, K<inline-formula><mml:math id="M154" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, Mg<inline-formula><mml:math id="M155" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, Ca<inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, NH<inline-formula><mml:math id="M157" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, amines,
Cl<inline-formula><mml:math id="M158" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>, NO<inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, NO<inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, and SO<inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>) were measured
using a Dionex ICS-2000 equipped with concentrator columns (TCC-ULP1 and
TAC-ULP1), guard columns (CG17 and AG19), and 4 mm analytical columns (CS17
and AS19). Gradient elution methods, using methanesulfonic acid (MSA) and
potassium hydroxide (KOH), were carried out using electrolytically
regenerated suppressors to reduce the influence of the eluent in the
conductivity detection. Carbonate salts are never quantified in the anion IC
due to the natural presence of carbonate in the distilled deionized water
reservoir that sustains the IC systems. Background measurements of the
entire AIM-IC system were conducted by overflowing the sampling inlet using
high-purity zero air to determine the method zero and detection limits of
each species. The limits of detection (LODs), based on 3<inline-formula><mml:math id="M162" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> of the
background, for trace gases were found to be 150, 20, 40, and 10 ppt for NH<inline-formula><mml:math id="M163" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, HCl, HNO<inline-formula><mml:math id="M164" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, and SO<inline-formula><mml:math id="M165" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, respectively. The LODs for
PM<inline-formula><mml:math id="M166" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> chemical constituents were 0.2, 0.1, 0.1, 0.04, and 0.4 <inline-formula><mml:math id="M167" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M168" 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>, for <inline-formula><mml:math id="M169" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NH<inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M171" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M172" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M173" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M174" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M175" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M176" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and
<inline-formula><mml:math id="M177" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M178" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> and 0.03, 0.03, and 0.01 <inline-formula><mml:math id="M179" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M180" 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> for <inline-formula><mml:math id="M181" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Cl<inline-formula><mml:math id="M182" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M183" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M185" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>SO<inline-formula><mml:math id="M186" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>.
Traces gases and PM<inline-formula><mml:math id="M187" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> constituents measured as cations are reported
from 21 January to 21 February 2017. Due to technical difficulties, anionic
constituents measured from 21 January to 8 February were compromised.
Therefore, PM<inline-formula><mml:math id="M188" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> anionic components are only reported from 13 to 21 February and the trace gases measured as anions during the former period may
be less reliable.</p>
      <p id="d1e2125">Continuous measurements of total PM<inline-formula><mml:math id="M189" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass concentrations were also
captured at the site using the Filter Dynamics Measurement System (FDMS) with
a tapered element oscillating microbalance (TEOM) ambient particulate monitor (FDMS
TEOM 1400ab, Thermo Fisher Scientific) provided by the Utah Division of Air
Quality (UDAQ). Ambient air was sampled at <inline-formula><mml:math id="M190" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1.5 m above the
roof through a <inline-formula><mml:math id="M191" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 7 m long <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> o.d. PFA line with a
volumetric flow rate of 20 L min<inline-formula><mml:math id="M193" 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>. A custom-made inertial PM impactor was
connected to the entrance of the sampling inlet to remove coarse PM and
water from the sample flow. A critical orifice was installed downstream of
the PM impactor to restrict the sample flow, maintaining a pressure below 200 mbar. The air sample was sent through an additional filter to remove
particles larger than 2.5 <inline-formula><mml:math id="M194" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m. An aerodynamic particle sizer (APS; TSI
Inc, Model 3321) was operated from 26 January to 10 February to size and
detect particles with an aerodynamic diameter of between 0.54 and 19.81 <inline-formula><mml:math id="M195" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m based on the time of flight of the particle between two (633 nm) He-Ne
lasers. This instrument was attached to an aerosol inlet that included a 2.54 cm diameter stainless-steel tube connected to a stainless-steel rain cap
with approximately a 10 cm diameter. Aerosol mass was calculated using the
Aerosol Instrument Manager (AIM) software for the APS Model 3321. The
particle density used for calculating the aerosol mass concentration was 1.0 g cm<inline-formula><mml:math id="M196" 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 particles were assumed to be spherical. The APS was attached
to this inlet system via a custom-made stainless-steel pickoff. To improve
aerosol transmission through the inlet, an external pump was attached to the
system. The pump pulled at approximately 7.2 L min<inline-formula><mml:math id="M197" 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>. The calculated
transmission shows a 50 % cutoff at approximately 7 <inline-formula><mml:math id="M198" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m for this
inlet system (Skiles et al., 2018).</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Snow sampling and analysis</title>
      <p id="d1e2238">The inorganic chemical composition (Na<inline-formula><mml:math id="M199" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, NH<inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, K<inline-formula><mml:math id="M201" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>,
Mg<inline-formula><mml:math id="M202" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, Ca<inline-formula><mml:math id="M203" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, NH<inline-formula><mml:math id="M204" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, Cl<inline-formula><mml:math id="M205" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>, NO<inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, NO<inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>,
and SO<inline-formula><mml:math id="M208" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>) of the snowpack was monitored throughout the campaign
during periods of snow cover. The snowpack composition and depth were
measured daily within a 2 m radius around the AIM-IC inlet atop UU using a
clean graduated 5 cm diameter beveled snow corer. Samples were collected in
triplicate along with a field blank to account for any contamination during
sampling. Collected samples were melted in sealed containers. The resulting
snowmelt solution was measured for total melt volume and pH (Hach
sensION+ PH1 Portable pH Meter). Snowmelt samples were
then filtered through 0.25 <inline-formula><mml:math id="M209" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m PTFE filters (Whatman, VWR
International) before analysis utilizing ion chromatography.</p>
</sec>
<?pagebreak page8115?><sec id="Ch1.S2.SS4">
  <label>2.4</label><title>Aerosol thermodynamic modelling using ISORROPIA</title>
      <p id="d1e2369">Thermodynamic modelling was used to examine the expected gas and particle
partitioning of semi-volatile constituents based on the local meteorological
conditions and the observed concentrations of gas and particle constituents.
These models carry out bulk calculations to estimate the gas-phase and
particle-phase composition of inorganic species, in which all particles are
assumed to have the same chemical composition. To examine how the presence
of non-volatile particle components observed during this period may affect
nitrate partitioning, ISORROPIA v2.1 (Nenes et al., 1998; Fountoukis and
Nenes, 2007) was used. Model calculations were run in forward mode, with
observed total ammonia (NH<inline-formula><mml:math id="M210" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M211" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M212" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NH<inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>), particulate sulfate
(<inline-formula><mml:math id="M214" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>SO<inline-formula><mml:math id="M215" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>), total nitrate (HNO<inline-formula><mml:math id="M216" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M217" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M218" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M219" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>), total
chloride (HCl <inline-formula><mml:math id="M220" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M221" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Cl<inline-formula><mml:math id="M222" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>), and non-volatile particulate species (<inline-formula><mml:math id="M223" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M224" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>,
<inline-formula><mml:math id="M225" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M226" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M227" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M228" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M229" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M230" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>), along with ambient relative humidity
and temperature, as inputs. Model runs were conducted using the metastable
state option, which prevents solid formation by forcing all particulate
components to remain in an aqueous state.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><?xmltex \opttitle{Trace gas and PM${}_{{2.5}}$ composition in the Salt Lake Valley}?><title>Trace gas and PM<inline-formula><mml:math id="M231" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> composition in the Salt Lake Valley</title>
      <p id="d1e2586">The AIM-IC measurement period included two PCAP pollution episodes, 27 January to 3 February 2017 (episode 1) and 13 to 17 February 2017 (episode 2), defined by the meteorological conditions that stabilize the boundary
layer and by the total observed PM<inline-formula><mml:math id="M232" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass, separated by a relatively
clean period from 5 to 12 February 2017. The PCAP episodes can be clearly
seen in the build-up of PM<inline-formula><mml:math id="M233" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass and the inorganic constituents
measured by the AIM-IC as shown in Fig. 2. Pollution periods with a total 24 h
average PM<inline-formula><mml:math id="M234" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass <inline-formula><mml:math id="M235" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 17.5 <inline-formula><mml:math id="M236" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M237" 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> are deemed PCAP
periods, while periods with a 24 h average PM<inline-formula><mml:math id="M238" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass <inline-formula><mml:math id="M239" display="inline"><mml:mo>≤</mml:mo></mml:math></inline-formula> 2 <inline-formula><mml:math id="M240" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M241" 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> are considered clean periods, as previously defined by Whiteman et al. (2014). The
pollution period from 27 January to 3 February 2017 (episode 1) was the most
persistent and severe during the UWFPS measurement campaign.</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="d1e2682"><bold>(a)</bold> The time series of NH<inline-formula><mml:math id="M242" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M243" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NH<inline-formula><mml:math id="M244" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> observed by the AIM-IC and total PM<inline-formula><mml:math id="M245" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass loading (<inline-formula><mml:math id="M246" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M247" 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>) measured by the TEOM from 23 January to 19 February 2017. <bold>(b)</bold> The AIM-IC observations of inorganic gases HCl, HNO<inline-formula><mml:math id="M248" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, and SO<inline-formula><mml:math id="M249" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M250" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> components <inline-formula><mml:math id="M251" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Cl<inline-formula><mml:math id="M252" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M253" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M255" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M256" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M257" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>SO<inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> present in
PM<inline-formula><mml:math id="M259" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>. <bold>(c)</bold> The AIM-IC observations of the non-volatile inorganic cations <inline-formula><mml:math id="M260" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M261" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M262" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M263" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M264" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M265" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M266" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M267" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> measured in
PM<inline-formula><mml:math id="M268" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> for the entire campaign period. The two PCAP pollution episodes
captured during the campaign are emphasized by the dotted black line. Time
is expressed in mountain standard time (MST).</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/8111/2021/acp-21-8111-2021-f02.png"/>

        </fig>

      <p id="d1e2951">Both pollution events are marked in Fig. 2, while the full suite of
inorganic gases and PM<inline-formula><mml:math id="M269" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> components was measured by the AIM-IC only
from 8 to 19 February 2017. The increase in total PM<inline-formula><mml:math id="M270" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass at the
onset of episode 1 on 27 January coincides with a rise in <inline-formula><mml:math id="M271" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NH<inline-formula><mml:math id="M272" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>,
seen in Fig. 2a, while there is an initial drop in ambient NH<inline-formula><mml:math id="M273" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
concentration before it plateaus at a mixing ratio of <inline-formula><mml:math id="M274" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1 ppb as
the PCAP progresses. The HNO<inline-formula><mml:math id="M275" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M276" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M277" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> data, depicted in Fig. 2b
for the second pollution event, confirm the major water-soluble component of
PM<inline-formula><mml:math id="M278" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> in the SLV is NH<inline-formula><mml:math id="M279" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M280" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, as previously reported
(Hansen
et al., 2010; Kelly et al., 2013; Kuprov et al., 2014; Long et al., 2003).
Compared to the <inline-formula><mml:math id="M281" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Cl<inline-formula><mml:math id="M282" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula> and <inline-formula><mml:math id="M283" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>SO<inline-formula><mml:math id="M284" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> mass loadings measured during
that event, Fig. 2b shows the total mass of <inline-formula><mml:math id="M285" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M286" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> is an order of
magnitude larger. Particularly at midday, the majority of the PM<inline-formula><mml:math id="M287" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>
mass is NH<inline-formula><mml:math id="M288" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M289" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>. It is important to note the organic fraction of
PM<inline-formula><mml:math id="M290" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> was not measured by the AIM-IC. Based on TEOM total mass and
AIM-IC-measured mass fractions, the AIM-IC captured 75 % of the total
PM<inline-formula><mml:math id="M291" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass.</p>
      <p id="d1e3165">The distinction between PCAP episodes 1 and 2 is important to note because
the stability of the cold-air pool and its persistence influences the
intensity of PM<inline-formula><mml:math id="M292" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> build-up in the SLV. Episode 1 was the most severe,
persisting for 9 d and allowing PM<inline-formula><mml:math id="M293" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> daily averages to reach the
highest observed through the measurement period, a maximum hourly average of
60 <inline-formula><mml:math id="M294" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M295" 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 episode occurred a few days after a storm
deposited roughly 22 cm of snow across the SLV and Wasatch front. Ambient
temperatures remained below freezing, between 263 and 273 K, sustaining the
snowpack throughout the event. This in turn increased the surface albedo,
limiting the strength of convection that can disrupt the stable boundary
layer (Whiteman et al., 2014). Winds during this episode were light,
averaging 1 m s<inline-formula><mml:math id="M296" 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>, with gusts under 7 m s<inline-formula><mml:math id="M297" 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> during the most stable
and calm cold pool period from 31 January to 2 February.</p>
      <p id="d1e3231">The second PCAP observed during the campaign was much shorter-lived with
moderate cold pool conditions only present from 13 through 17 February. This
episode was distinctly different than episode 1, having no snow cover and much
warmer conditions, with temperatures ranging from 270 to 284 K. The winter
snowpack in the surrounding mountain range showed signs of spring melt,
which extended the surface area of exposed ground. Winds were slightly
stronger, averaging 1.6 m s<inline-formula><mml:math id="M298" 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> with stronger gusts averaging around 8 m s<inline-formula><mml:math id="M299" 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> caused by stronger convection. The hourly PM<inline-formula><mml:math id="M300" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> average at the
UU site peaked at 28 <inline-formula><mml:math id="M301" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M302" 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 elevated PM levels only persisted for
2 to 3 full days, so the intensity and duration of episode 2 was about half
that of episode 1.</p>
      <p id="d1e3287">The presence of non-volatile cations (<inline-formula><mml:math id="M303" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M304" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M305" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M306" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M307" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M308" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, and
<inline-formula><mml:math id="M309" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M310" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>), seen in Fig. 2c, was also observed during PCAP events. Of all the
non-volatile cations observed, only potassium increases with the same
pattern as the increase in <inline-formula><mml:math id="M311" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NH<inline-formula><mml:math id="M312" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and total PM<inline-formula><mml:math id="M313" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass
measured by the TEOM. Potassium salts are often found in primary aerosols
formed from biomass or biofuel burning
(Pósfai
et al., 2003; Rissler et al., 2006). Wood burning is still a commonly used
source of heat during the winter months in the SLV and could be the source
of <inline-formula><mml:math id="M314" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M315" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> observed during the severe PCAP episode 1. Aerosol mass
spectrometer (AMS) data from Franchin et al. (2018) showed traces of
levoglucosan, a known marker for wood combustion, during the pollution
episode. However, levoglucosan was typically measured at close to background
values. Overall, the data reported from AMS measurements indicated the
organic material from wood combustion is not<?pagebreak page8116?> a dominant mass fraction on
the regional scale
(Franchin et al., 2018).
Recent radiocarbon analysis from ground sites in the SLV indicates that fossil
fuels were the dominant sources of carbonaceous aerosols during winter,
contributing to 88 % (80 % to 98 %) of the black carbon in aerosols and
58 % (48 % to 69 %) of the organic carbon in aerosols
(Mouteva et al., 2017).
Similarly, the AIM-IC data also suggest that <inline-formula><mml:math id="M316" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M317" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> salts generally
compose a small fraction of the total PM<inline-formula><mml:math id="M318" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> mass.</p>
      <?pagebreak page8117?><p id="d1e3431">The alkali and alkaline metal components <inline-formula><mml:math id="M319" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M320" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M321" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M322" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> and
<inline-formula><mml:math id="M323" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M324" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> are commonly found in larger primary particles often emitted from
the lofting of mineral dust and salts. These species are often found in
mineral aerosols, which typically range from 0.1 to more than 10 <inline-formula><mml:math id="M325" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m,
partially contributing to PM<inline-formula><mml:math id="M326" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> (Zender,
2003). The coarse-mode fraction of these primary particles, with diameters
greater than 2.5 <inline-formula><mml:math id="M327" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m, has sufficiently large settling velocities that
the particles have much shorter lifetimes in the atmosphere compared to PM<inline-formula><mml:math id="M328" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>.
If the non-volatile cations observed in PM<inline-formula><mml:math id="M329" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> are present in the
largest fine particles, then their lifetime in the atmosphere is
considerably shorter than NH<inline-formula><mml:math id="M330" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M331" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> found in the accumulation mode.
This may be the explanation for the more pronounced diel pattern of
<inline-formula><mml:math id="M332" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M333" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M334" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M335" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M336" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M337" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> during the PCAP periods. It is also
possible that because vertical mixing is suppressed during PCAP episodes,
the UU site is in contact with air from the mineral dust source region to a
measurable degree only at midday. During the clean periods, the
concentrations of these ions measured by the AIM-IC are very close to their
respective detection limits. <inline-formula><mml:math id="M338" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M339" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M340" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M341" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> and <inline-formula><mml:math id="M342" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M343" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> PM<inline-formula><mml:math id="M344" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>
components peak at midday during pollution events, suggesting similar and/or
co-located sources. Concentrations of <inline-formula><mml:math id="M345" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M346" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, which is an effective
tracer for mineral dust along with <inline-formula><mml:math id="M347" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M348" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>
(Maxwell-Meier et al., 2004),
are present throughout the entire measurement period, averaging 0.02 <inline-formula><mml:math id="M349" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M350" 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 reaching a maximum of 0.15 <inline-formula><mml:math id="M351" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M352" 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>. It is known
that sea salt is the most common source of <inline-formula><mml:math id="M353" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M354" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, so examining the
Ca-to-Na ratios can suggest the predominant source. Particularly for the SLV
region, the Great Salt Lake can also be a source of sea salt. In PCAP
episode 1, Ca-to-Na ratios were below 1, suggesting the presence of sea
salts. In contrast, in episode 2 ratios of Ca-to-Na were above 1, suggesting
the sources of these particulate components differ between the two PCAP
periods. Due to the heavy snowfall during episode 1, road salt was
continuously applied to all major roads and walkways throughout the UU
campus, which may act as a local source of Na salts during periods of heavy
traffic. The lack of snow cover during the latter episode and higher
temperatures may suggest some influence of mineral dust from the surrounding
ground surface areas, where sediments and weathered minerals are often
Ca-rich
(Chesselet
et al., 1972; Kassomenos et al., 2012; Kuo et al., 2005). Recent studies
have found the Great Salt Lake is quickly receding, suggesting the exposed
the lake bed could act as a source of dust and sea salt
(Hahnenberger
and Nicoll, 2012; Skiles et al., 2018; Wurtsbaugh et al., 2017). However,
the bulk PM<inline-formula><mml:math id="M355" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> chemical composition measured by the AIM-IC is not
detailed enough to unambiguously identify the source of non-volatile cations
observed during PCAP events.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><?xmltex \opttitle{Estimating HNO${}_{{3}}$ loss to coarse-mode particles}?><title>Estimating HNO<inline-formula><mml:math id="M356" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> loss to coarse-mode particles</title>
      <p id="d1e3793">Gas-phase HNO<inline-formula><mml:math id="M357" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> exists in equilibrium with semi-volatile nitrate in
PM<inline-formula><mml:math id="M358" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, and the extent of gas-to-particle partitioning depends on
temperature, relative humidity, and NH<inline-formula><mml:math id="M359" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, via the formation of
NH<inline-formula><mml:math id="M360" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M361" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">3</mml:mn><mml:mo>(</mml:mo><mml:mi mathvariant="normal">s</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msub></mml:math></inline-formula> in dry particles or its influence on particle acidity in
deliquesced particles. At the same time, HNO<inline-formula><mml:math id="M362" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> may undergo net uptake by
primary particles when it reacts with their constituents, for example
CaCO<inline-formula><mml:math id="M363" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> or NaCl, to form non-volatile nitrate salts. The rate of
HNO<inline-formula><mml:math id="M364" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> loss can be impacted by the composition of the reactive salt and
the reactive surface area available (Seinfeld and Pandis, 2006).
During the two PCAP episodes, we observed elevated midday concentrations of
<inline-formula><mml:math id="M365" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M366" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M367" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M368" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M369" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M370" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> in PM<inline-formula><mml:math id="M371" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> using the AIM-IC.</p>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title>Inferences from aerodynamic particle sizing</title>
      <p id="d1e3947">Coarse-mode particles (diameters <inline-formula><mml:math id="M372" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> 2.5 <inline-formula><mml:math id="M373" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m) were not
speciated during the UWFPS campaign. There are very few reports of coarse-mode nitrate in winter conditions that could offer an approximation of how
much HNO<inline-formula><mml:math id="M374" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> may have been taken up by coarse-mode particles in the SLV.
The study of Hansen et al. (2010) is the only one commenting on coarse-mode nitrate in
northern Utah region, in Lindon, <inline-formula><mml:math id="M375" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 50 km located south of the SLV,
during January to February 2007. The authors observed high mass loadings, up to 80 <inline-formula><mml:math id="M376" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M377" 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> of coarse aerosols (PM<inline-formula><mml:math id="M378" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>–PM<inline-formula><mml:math id="M379" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>), during PCAP
events, based on measurements from two GRIMM optical particle counters
(Hansen et
al., 2010). The authors did not report any quantification of the chemical
components of the coarse aerosols collected by integrated filter samples,
although they commented that the nitrate levels were relatively low.</p>

      <?xmltex \floatpos{p}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e4022"><bold>(a, b)</bold> The total fine-mode (PM<inline-formula><mml:math id="M380" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>) and coarse-mode (<inline-formula><mml:math id="M381" display="inline"><mml:mo lspace="0mm">&gt;</mml:mo></mml:math></inline-formula> PM<inline-formula><mml:math id="M382" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>) surface area calculated in <inline-formula><mml:math id="M383" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m<inline-formula><mml:math id="M384" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> cm<inline-formula><mml:math id="M385" 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> from APS data. <bold>(c)</bold> The particle size distribution as a function of time, 28 January to 4 February, with particle size displayed along the <inline-formula><mml:math id="M386" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis and color
contours representing mass that is normalized by size bin (<inline-formula><mml:math id="M387" display="inline"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>M</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi>log⁡</mml:mi><mml:mi>D</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></inline-formula>). The
population of particles that the AIM-IC captures is below the labelled
PM<inline-formula><mml:math id="M388" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> line.</p></caption>
            <?xmltex \igopts{width=412.564961pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/8111/2021/acp-21-8111-2021-f03.png"/>

          </fig>

      <?xmltex \floatpos{p}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e4129"><bold>(a)</bold> Wind speed and temperature (<inline-formula><mml:math id="M389" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) measured at UU. The coarse particle (PM<inline-formula><mml:math id="M390" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>–PM<inline-formula><mml:math id="M391" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>) mass loading in <inline-formula><mml:math id="M392" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M393" 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 a function of time, 28 January to 4 February 2017, at three separate ground-based sites: Rose Park <bold>(b)</bold> shown in green and Hawthorne Elementary <bold>(c)</bold> shown in black, which are EPA monitoring sites, and the UU site <bold>(d)</bold> in blue.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/8111/2021/acp-21-8111-2021-f04.png"/>

          </fig>

      <p id="d1e4198">To obtain information about the coarse-mode loadings during PCAP events in
UWFPS, APS data collected during the pollution episode from 28 January to 3 February are displayed in Fig. 3. The particle size bins are colored by mass
normalized to the size bin (<inline-formula><mml:math id="M394" display="inline"><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>M</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi>log⁡</mml:mi><mml:mi>D</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math></inline-formula>), clearly showing elevated midday
burdens of coarse-mode particles, which become more pronounced during the
intensive cold-air pool period from 30 January to 2 February 2017. This is
consistent with the midday increases in coarse-mode mass observed across
the SLV, shown in Fig. 4. The coarse fraction of PM<inline-formula><mml:math id="M395" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> measured at Hawthorne
Elementary (the air quality regulatory site at the base of the SLV operated by UDAQ) shows a similar trend to the APS mass loading of
PM<inline-formula><mml:math id="M396" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>–PM<inline-formula><mml:math id="M397" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> observed at UU. In contrast, the Rose Park site
(another UDAQ site), which is close to Great Salt Lake, exhibits moderate
increases in coarse-mode mass compared to UU and Hawthorne. This difference
is more evident during the calmest period of the pollution event, when the
lowest wind speeds were observed, which suggests the sources of coarse
particles are highly localized during PCAP events. An analysis of coarse
particles by Li et al. (2013) found only moderate correlation between PM<inline-formula><mml:math id="M398" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">10</mml:mn><mml:mtext>–</mml:mtext><mml:mn mathvariant="normal">2.5</mml:mn></mml:mrow></mml:msub></mml:math></inline-formula> mass loadings and wind speed at several sites across the USA
(Li et al., 2013).</p>
      <p id="d1e4262">The time series of the total surface area of PM larger than 2.5 <inline-formula><mml:math id="M399" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m in
<inline-formula><mml:math id="M400" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m<inline-formula><mml:math id="M401" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> cm<inline-formula><mml:math id="M402" 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> (Fig. 3) shows the available coarse-mode surface
area exceeds 1500 <inline-formula><mml:math id="M403" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m<inline-formula><mml:math id="M404" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> cm<inline-formula><mml:math id="M405" 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> for several hours on each of the
3 most severe pollution days, 30 January to 1 February 2017. For
comparison, the total surface area of the fine-mode particles is also shown,
which is roughly 3 times the maximum surface area of the coarse
fraction but with less diurnal variability. However, the fine-mode aerosol
nitrate is assumed to be in equilibrium with gas-phase HNO<inline-formula><mml:math id="M406" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, in
contrast to the coarse-mode surface area, which could be viewed as a
reactive sink allowing net uptake. The midday increases in coarse-particle
surface area, therefore, could represent an important permanent sink for
HNO<inline-formula><mml:math id="M407" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> if the particles are composed of reactive salts such as CaCO<inline-formula><mml:math id="M408" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
or NaCl.</p>
      <?pagebreak page8119?><p id="d1e4359"><?xmltex \hack{\newpage}?>A lower limit to the lifetime of HNO<inline-formula><mml:math id="M409" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> with respect to uptake by the
coarse aerosol surface can be calculated to infer the potential importance
of mineral–coarse aerosol particles during these heavy pollution events. The
approximate first-order removal rate of HNO<inline-formula><mml:math id="M410" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> due to the heterogeneous
reaction with coarse aerosols, <inline-formula><mml:math id="M411" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mi mathvariant="normal">het</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, depends on its average
molecular speed, <inline-formula><mml:math id="M412" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula>; the surface area density of coarse aerosols, <inline-formula><mml:math id="M413" display="inline"><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>; and
the uptake coefficient, <inline-formula><mml:math id="M414" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula>, given in the following expression
(Ammann
et al., 2013; Crowley et al., 2010; Kolb et al., 2010; Tang et al., 2017):
              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M415" display="block"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mi mathvariant="normal">het</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn><mml:mo>⋅</mml:mo><mml:mi>c</mml:mi><mml:mo>⋅</mml:mo><mml:msub><mml:mi>S</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The variation in mineralogy of coarse-mode particles can influence the
efficiency in HNO<inline-formula><mml:math id="M416" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> reactive uptake via the uptake coefficient, <inline-formula><mml:math id="M417" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula>. This is represented in the range of reported uptake coefficients of
HNO<inline-formula><mml:math id="M418" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> to CaCO<inline-formula><mml:math id="M419" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> (<inline-formula><mml:math id="M420" display="inline"><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula> at RH <inline-formula><mml:math id="M421" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 50 %) and NaCl
(<inline-formula><mml:math id="M422" display="inline"><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.11</mml:mn></mml:mrow></mml:math></inline-formula> at RH <inline-formula><mml:math id="M423" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 55 %) (Liu et al., 2008a; Saul et al., 2006).
The average RH at peak coarse-mode loading was 54 %; therefore, the
reported uptake coefficients close to this RH value were used in our
calculations. Literature reports have shown RH significantly enhances the
reaction probability of HNO<inline-formula><mml:math id="M424" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> uptake with mineral dust and sea salts
(Liu
et al., 2008a; Saul et al., 2006; Vlasenko et al., 2006). The detailed
kinetics of HNO<inline-formula><mml:math id="M425" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> reacting with CaCO<inline-formula><mml:math id="M426" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> particles in a flow reactor
by Liu et al. (2008a) found low uptake values of <inline-formula><mml:math id="M427" display="inline"><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>≤</mml:mo><mml:mn mathvariant="normal">0.003</mml:mn></mml:mrow></mml:math></inline-formula> at 10 % RH, while at 80 % RH, <inline-formula><mml:math id="M428" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> can be <inline-formula><mml:math id="M429" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 0.21. This agrees with
reports from Vlasenko et al. (2006), in which HNO<inline-formula><mml:math id="M430" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> uptake on dust
aerosols containing <inline-formula><mml:math id="M431" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 5 % CaCO<inline-formula><mml:math id="M432" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> was also enhanced by an
increase in RH. Saul et al. (2006) also found RH affects the uptake
of HNO<inline-formula><mml:math id="M433" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> onto pure NaCl showing a maximum <inline-formula><mml:math id="M434" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> of 0.12 at 50 %
RH, while at 85 % RH, <inline-formula><mml:math id="M435" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> is 0.05. They also observed an increase in
reactivity with the presence of MgCl<inline-formula><mml:math id="M436" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> in NaCl powder. The greater
reactivity of MgCl<inline-formula><mml:math id="M437" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> is consistent with the hygroscopic character of
magnesium salts that facilitate the increase in adsorbed water at the
particle surface, which can in turn increase the effective uptake of
HNO<inline-formula><mml:math id="M438" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>.</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="d1e4656">Predicted HNO<inline-formula><mml:math id="M439" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> loss rate to coarse-particle surface area
concentration measured by the APS from 28 January to 4 February 2017.</p></caption>
            <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/8111/2021/acp-21-8111-2021-f05.png"/>

          </fig>

      <p id="d1e4674">Because <inline-formula><mml:math id="M440" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M441" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> and <inline-formula><mml:math id="M442" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M443" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> were the dominant non-volatile species that
showed common behavior with the coarse-mode mass loading, the rates of
uptake with respect to NaCl and CaCO<inline-formula><mml:math id="M444" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> were calculated to approximate
how quickly HNO<inline-formula><mml:math id="M445" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> might be sequestered. Literature values for the uptake
coefficients of HNO<inline-formula><mml:math id="M446" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> on NaCl (0.11 at 55 % RH) and CaCO<inline-formula><mml:math id="M447" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> (0.07
at 50 % RH) were used to estimate a lifetime against reactive uptake
based on the measured coarse-mode surface area
(Fenter
et al., 1994; Liu et al., 2008a; Vlasenko et al., 2006). The time series of
<inline-formula><mml:math id="M448" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mi mathvariant="normal">het</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> from 27 January to 4 February 2017 is presented in Fig. 5. The
effective lifetime of HNO<inline-formula><mml:math id="M449" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> against reactive uptake to CaCO<inline-formula><mml:math id="M450" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> during
episode 1 ranges from 2 to 90 min with the shortest lifetimes during
periods of peak coarse-mode loading. The lifetime against NaCl (0.11) ranges
from 1.3 to 57 min. These lifetime calculations assume that the entire
surface is reactive and do not account for any mass transfer limitations
that may occur on the particle surface. Therefore, the time range is an
estimate of the upper limit to the rate of HNO<inline-formula><mml:math id="M451" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> uptake, or how quickly
the reaction could potentially occur.</p>
      <p id="d1e4789">Under high-RH conditions, which often occur during PCAP events, it is also
possible coarse particles may be deliquesced, allowing exchange between
surface and bulk ions within a particle. This would result in an increased
loss of nitrate if uptake were not limited to the surface. If the total mass
of coarse particles measured during episode 1 were assumed to be composed of
Ca(NO<inline-formula><mml:math id="M452" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>)<inline-formula><mml:math id="M453" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, in which carbonate has been completely displaced, that
would amount to an average of 6.2 <inline-formula><mml:math id="M454" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M455" 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> of HNO<inline-formula><mml:math id="M456" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> sequestered
with a maximum of 32 <inline-formula><mml:math id="M457" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M458" 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> during midday. This assumes HNO<inline-formula><mml:math id="M459" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
can react with the bulk particle components, thereby representing an upper
estimate of HNO<inline-formula><mml:math id="M460" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> mass loss to PM<inline-formula><mml:math id="M461" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>. However, due to the size
cutoff of the APS, with significant transmission losses above 10 <inline-formula><mml:math id="M462" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>m,
it is possible that the mass of coarse-mode particles is underestimated
under some conditions.</p>
      <p id="d1e4895">The calculations of the removal rate do not include changes in reactive
uptake associated with the changes in hygroscopicity of the resulting
nitrate salts formed. The presence of calcium or magnesium nitrate salts can
enhance the absorbance of water, which has been shown to increase the
relative uptake of HNO<inline-formula><mml:math id="M463" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> because it is no longer limited to the particle
surface, so the estimation of HNO<inline-formula><mml:math id="M464" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> loss can also be highly variable
(Beichert
and Finlayson-Pitts, 1996; Goodman et al., 2000). This is dependent on the
deliquescence relative humidity (DRH) of the nitrate salt formed, in which
DRH of Ca(NO<inline-formula><mml:math id="M465" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>)<inline-formula><mml:math id="M466" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> is 10 % at 298 K
(Liu
et al., 2008b; Sullivan et al., 2009a, b) and NaNO<inline-formula><mml:math id="M467" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> is 81 % at
273 K (Seinfeld and Pandis, 2006). The DRH is also
temperature-dependent and tends to increase with decreasing temperature. The
temperatures during episode 1 were consistently below 273 K; therefore, it
is assumed DRH would be higher. The inference from the heterogeneous uptake
calculation suggests that the loss of HNO<inline-formula><mml:math id="M468" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> can be very rapid. The
question of how this loss in HNO<inline-formula><mml:math id="M469" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> to coarse aerosols could be shifting
the gas-to-particle equilibrium that exists between HNO<inline-formula><mml:math id="M470" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, NH<inline-formula><mml:math id="M471" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, and
NH<inline-formula><mml:math id="M472" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M473" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> is still unknown. Therefore, further investigation of
time-resolved coarse-aerosol chemical composition, in addition to PM<inline-formula><mml:math id="M474" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>
composition, is needed to better quantify how much coarse aerosols may be
limiting HNO<inline-formula><mml:math id="M475" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> availability during these PCAP pollution events and
elucidate their effect on NH<inline-formula><mml:math id="M476" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M477" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation.</p>
      <p id="d1e5035">Studies from coastal sites provide evidence that the uptake of nitrate to
coarse-model aerosols can be substantial. For example, single particle
measurements of sea salt particles using an aerosol time-of-flight mass spectrometer (ATOFMS) in California found that the
chloride mole fraction could decrease from 0.3 to 0, while the nitrate mole
fraction could increase from 0 to 0.5 following exposure of sea salt to
urban air pollution (Gard et al., 1998). In
coastal Florida, measurements using an online ion chromatographic technique
showed that deliquesced sea salt particles could have more than 50 % of
the chloride content replaced by nitrate
(Dasgupta et al., 2007).
Measurements from a size-resolved<?pagebreak page8120?> integrated sampler showed that nitrate
peaked in the coarse mode, where its concentration was close to that of
chloride (on a molar basis) and half that of sodium. Size-resolved particle
composition measurements near the coast in British Columbia during the
summer showed that during the day, nitrate was only present in coarse-mode
particles (corresponding to a deficiency in chloride), whereas during the
night, nitrate could also be measured in accumulation mode particles
(Anlauf et al., 2006). In
addition, Lee et al. (2018) identify that coarse-mode nitrate particles, formed
from acid displacement, are more important in national park areas in Arizona
and Tennessee. Measurements were taken during spring and summer,
respectively, so did not have competing NH<inline-formula><mml:math id="M478" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M479" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation; however,
they do highlight the fact coarse particle nitrate extends into the
PM<inline-formula><mml:math id="M480" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> regime and not all nitrate in this regime is associated with
NH<inline-formula><mml:math id="M481" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>Evidence from snow analysis</title>
      <p id="d1e5082">During the campaign period, a snow event occurred prior to the first PCAP
episode (21 January), in which the snow remained on the surface until
3 February. This provided a snowpack that was subjected to the first
pollution event, providing a record of chemical composition changes caused
by PCAP exposure. A snow event that happened later in the season occurred
during clean conditions (23 February to 2 March 2017), when no PCAP was
observed, thus providing a representative example of chemical composition
changes in snow not associated with PCAP exposure.</p>
      <p id="d1e5085">Chemical analysis of the snowpack exposed to PCAP episode 1 reflects a
combination of cloud water composition and the atmospheric gas and particle
composition of species scavenged by snowfall or later deposited to the
snow, including particles larger than the PM<inline-formula><mml:math id="M482" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> cutoff monitored by the
AIM-IC. Figure 6 shows a scatter plot of the NH<inline-formula><mml:math id="M483" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> versus
NO<inline-formula><mml:math id="M484" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> measured in the snowpack, where each data point is
representative of the averaged chemical composition of the entire snowpack
(sampling area 0.008 m<inline-formula><mml:math id="M485" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula>) on a single day, and in the atmosphere by the
AIM-IC (gas phase <inline-formula><mml:math id="M486" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> PM<inline-formula><mml:math id="M487" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>), where PM<inline-formula><mml:math id="M488" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> NO<inline-formula><mml:math id="M489" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> is
assumed to be equivalent to 90 % of PM<inline-formula><mml:math id="M490" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> NH<inline-formula><mml:math id="M491" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> on a molar
basis, and by a Twin Otter aircraft (gas phase <inline-formula><mml:math id="M492" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> PM<inline-formula><mml:math id="M493" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula>). Aerosol particle
measurements from the aircraft do not include non-volatile cations and their
associated nitrates, which the AMS does not measure (Franchin et al., 2018).
Gas-phase HNO<inline-formula><mml:math id="M494" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> measurements collected on the aircraft are from the
University of Washington high-resolution time-of-flight chemical ionization mass spectrometer (HR-ToF-CIMS) instrument operated similarly to the method
described in Lee
et al. (2018). Gas-phase NH<inline-formula><mml:math id="M495" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> measurements from the Twin Otter were
taken using a quantum cascade tunable infrared differential absorption spectrometer (QC-TILDAS) instrument (Aerodyne Research Inc, MA, USA) and are described
in Moravek et al. (2019). Based on aircraft data (Franchin et
al., 2018) and AIM-IC measurements at the ground site, the sum of nitrate in
the gas phase and particle phases, or total NO<inline-formula><mml:math id="M496" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> (TNO<inline-formula><mml:math id="M497" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>) per cubic metre
of ambient air, is less than the sum of ammonia in the gas phase and
particle phases, total NH<inline-formula><mml:math id="M498" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> per cubic metre of ambient air. Therefore, we
might expect that there would be more ammonium depositing into the snow
compared to nitrate. However, in Fig. 6, it is clear that the deposition of
NH<inline-formula><mml:math id="M499" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> is less than half that of total NO<inline-formula><mml:math id="M500" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> on a molar basis for the
highest deposition amounts. The average TNO<inline-formula><mml:math id="M501" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> : NH<inline-formula><mml:math id="M502" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> molar ratio of
3 : 1 measured in the snowpack is significantly different compared to what is
observed in the atmospheric measurements. This implies that there could be
another source of nitrate being deposited to the snow that is not reflected
in the atmospheric measurements of the gas-phase and fine-mode particles.
Therefore, there is a missing portion of the overall nitrate budget that is
connected to how much NH<inline-formula><mml:math id="M503" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M504" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> can be formed.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><?xmltex \def\figurename{Figure}?><label>Figure 6</label><caption><p id="d1e5308">Total NO<inline-formula><mml:math id="M505" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> (<inline-formula><mml:math id="M506" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M507" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M508" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> HNO<inline-formula><mml:math id="M509" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>) with respect to total
NH<inline-formula><mml:math id="M510" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> measured and predicted from AIM-IC data (grey circles), aircraft
measurements (open blue circles) per cubic metre of ambient air and snow (red
triangles) within 0.008 m<inline-formula><mml:math id="M511" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> sampling area from 21 January to 3 February
2017.</p></caption>
            <?xmltex \igopts{width=156.490157pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/8111/2021/acp-21-8111-2021-f06.png"/>

          </fig>

      <?pagebreak page8121?><p id="d1e5381">Further investigation into the composition of the snowpack reveals there is
a strong correlation between the amount of NO<inline-formula><mml:math id="M512" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and the amount of
Ca<inline-formula><mml:math id="M513" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> (<inline-formula><mml:math id="M514" display="inline"><mml:mrow><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.836</mml:mn></mml:mrow></mml:math></inline-formula>), seen in Fig. 7. Both Na<inline-formula><mml:math id="M515" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> and Ca<inline-formula><mml:math id="M516" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>
are also found in the snowpack in higher abundances than NH<inline-formula><mml:math id="M517" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>,
despite being present at much lower levels in PM<inline-formula><mml:math id="M518" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>. The larger
concentrations of <inline-formula><mml:math id="M519" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M520" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> relative to <inline-formula><mml:math id="M521" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M522" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> seen in the AIM-IC
PM<inline-formula><mml:math id="M523" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> data are consistent with the larger concentrations of Na<inline-formula><mml:math id="M524" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>
measured in the snowpack relative to Ca<inline-formula><mml:math id="M525" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> concentrations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><?xmltex \currentcnt{7}?><?xmltex \def\figurename{Figure}?><label>Figure 7</label><caption><p id="d1e5534">Daily total micromoles of NH<inline-formula><mml:math id="M526" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>, Ca, and Na vs. NO<inline-formula><mml:math id="M527" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> within
the snow from 21 January to 3 February 2017, leading into the most severe
PCAP period from 27 January to 4 February 2017.</p></caption>
            <?xmltex \igopts{width=142.26378pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/8111/2021/acp-21-8111-2021-f07.png"/>

          </fig>

      <p id="d1e5561">This suggests the coarse-mode aerosols during this PCAP event were Na-rich.
Due to the large excess of micromoles of Na<inline-formula><mml:math id="M528" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> when compared to
NO<inline-formula><mml:math id="M529" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, the amount of Cl<inline-formula><mml:math id="M530" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula> was examined to determine whether
Na-rich particles came in the form of NaCl salt. The snowpack showed the
highest concentrations of Cl<inline-formula><mml:math id="M531" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula> out of all of the inorganic anions measured,
over 10 times more than NO<inline-formula><mml:math id="M532" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and SO<inline-formula><mml:math id="M533" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> combined. The total water-soluble ion balance measured in the snowpack
shows a slight excess of anions, partially due to the high Cl<inline-formula><mml:math id="M534" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula> content.
However, the concentrations of Cl<inline-formula><mml:math id="M535" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula> measured in the snow were
greater than what can be accounted for by observed Na<inline-formula><mml:math id="M536" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>. The low
concentrations of Mg<inline-formula><mml:math id="M537" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> in the snowpack had no noticeable correlation
with Cl<inline-formula><mml:math id="M538" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>. A closer look at the daily inorganic composition changes and
decrease in snowpack height reveals Ca<inline-formula><mml:math id="M539" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> and
NO<inline-formula><mml:math id="M540" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> exhibit similar trends throughout the lifetime of the
snowpack. This is also true for changes in K<inline-formula><mml:math id="M541" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> and Cl<inline-formula><mml:math id="M542" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula> total snow
column concentrations.</p>
      <p id="d1e5722">The proportions of non-volatile cations, where K<inline-formula><mml:math id="M543" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M544" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> Na<inline-formula><mml:math id="M545" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M546" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> Ca<inline-formula><mml:math id="M547" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M548" display="inline"><mml:mo>&gt;</mml:mo></mml:math></inline-formula> Mg<inline-formula><mml:math id="M549" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, found in the snow
exhibit a similar distribution to that observed in PM<inline-formula><mml:math id="M550" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> composition. We infer
that our measurements of these constituents in PM<inline-formula><mml:math id="M551" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> also reflect a
larger unmeasured contribution of these non-volatile cations in the coarse
mode. In addition, the nitrate present in the snow appears to have a strong
correlation with Ca<inline-formula><mml:math id="M552" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, suggesting there could be a significant amount
of particle nitrate in the coarse mode that is not accounted for in
PM<inline-formula><mml:math id="M553" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> measurements. This underestimation of particle nitrate during
peak coarse-mode periods that occur during the day could lead to an
underestimation in the production rate of nitrate due to photochemistry.
This could impact estimates of the sensitivity of PM<inline-formula><mml:math id="M554" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> to NH<inline-formula><mml:math id="M555" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and
NO<inline-formula><mml:math id="M556" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> emissions reductions.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS3">
  <label>3.2.3</label><title>ISORROPIA analysis</title>
      <p id="d1e5865">The comparison of ISORROPIA model runs of predicted NH<inline-formula><mml:math id="M557" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M558" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
(<inline-formula><mml:math id="M559" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M560" 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>) with and without non-volatile components measured by
the AIM-IC are depicted in Fig. 8 through pollution episode 2 from 13 to 19 February 2017 when both anion and cation gas and particle data were
available. ISORROPIA calculates the equilibrium concentrations of the
NH<inline-formula><mml:math id="M561" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>–SO<inline-formula><mml:math id="M562" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>–NO<inline-formula><mml:math id="M563" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>–Na<inline-formula><mml:math id="M564" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>–Cl<inline-formula><mml:math id="M565" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>–K<inline-formula><mml:math id="M566" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>–Mg<inline-formula><mml:math id="M567" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>–Ca<inline-formula><mml:math id="M568" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>–H<inline-formula><mml:math id="M569" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>O
system. Overall, the difference in model outputs for these two input
conditions demonstrates how influential the presence of non-volatiles
(<inline-formula><mml:math id="M570" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M571" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M572" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M573" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M574" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M575" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M576" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M577" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>) is on the thermodynamic
equilibrium between HNO<inline-formula><mml:math id="M578" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and its particulate counterpart
<inline-formula><mml:math id="M579" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M580" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><?xmltex \currentcnt{8}?><?xmltex \def\figurename{Figure}?><label>Figure 8</label><caption><p id="d1e6109">Predicted concentrations (ISORROPIA) with respected to measured (AIM-IC) ambient
concentrations of NH<inline-formula><mml:math id="M581" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M582" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> in <inline-formula><mml:math id="M583" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M584" 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> through the second pollution event from 13 to 19 February 2017. The model was run in
three separate conditions: (1) with (red cross) and (2) without (open black
circle) the addition of <inline-formula><mml:math id="M585" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M586" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M587" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M588" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M589" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M590" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> and (3) with
non-volatiles and the increase in total nitrate based on the ratio of
NH<inline-formula><mml:math id="M591" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> to NO<inline-formula><mml:math id="M592" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> measured in the snow.</p></caption>
            <?xmltex \igopts{width=227.622047pt}?><graphic xlink:href="https://acp.copernicus.org/articles/21/8111/2021/acp-21-8111-2021-f08.png"/>

          </fig>

      <?pagebreak page8122?><p id="d1e6236">Previous studies have shown the inclusion of non-volatile cations in
thermodynamic models can more accurately reproduce gas-particle partitioning
observations by correctly reflecting the ion balance and the
ammonium : sulfate ratio (Guo et al., 2018). With
the addition of <inline-formula><mml:math id="M593" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Cl<inline-formula><mml:math id="M594" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M595" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M596" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M597" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M598" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M599" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M600" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M601" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M602" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula> in
ISORROPIA model runs, the model consistently underpredicts the
concentrations of NH<inline-formula><mml:math id="M603" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M604" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> observed. This underestimation is
expected because the implicit assumption in the ISORROPIA run is that all
the non-volatile cations are associated with particle nitrate, which is
unlikely to be the case. The model also does not accommodate the presence of
carbonate, nor does the AIM-IC measure particulate carbonate, which can also
associate with non-volatile cations. Therefore, the model runs represent an
upper limit of how much nitrate could be permanently trapped in the
particulate phase. The model outputs imply that some non-zero fraction of
the nitrate in the gas <inline-formula><mml:math id="M605" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> PM<inline-formula><mml:math id="M606" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> system is associated with non-volatile
cations. Based on the strong relationship ISORROPIA predicts between
non-volatile cations and particle nitrate, the next step is to determine how
sensitive NH<inline-formula><mml:math id="M607" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M608" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation is to this portion of missing nitrate.
Figure 8 demonstrates how much more NH<inline-formula><mml:math id="M609" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M610" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> could be formed if
HNO<inline-formula><mml:math id="M611" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> was not sequestered by the coarse particles, depicted in blue
squares. Based on measured gas-phase NH<inline-formula><mml:math id="M612" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and <inline-formula><mml:math id="M613" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NH<inline-formula><mml:math id="M614" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, it is
assumed there is a very little coarse-mode NH<inline-formula><mml:math id="M615" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> in the atmosphere.
To estimate the missing nitrate budget associated with coarse particles,
assuming the total concentration of snow nitrate is derived from coarse
particles is unrealistic. Therefore, with ambient NH<inline-formula><mml:math id="M616" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> measurements as a
point of reference, the total NH<inline-formula><mml:math id="M617" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> in the snow was used to
estimate the fraction of snow nitrate potentially from coarse particles, in
the absence of any other direct coarse-mode measurements. The total nitrate
input into ISORROPIA was calculated using the NO<inline-formula><mml:math id="M618" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>-to-NH<inline-formula><mml:math id="M619" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> ratio observed in the snowpack during the first PCAP event.
This serves as an upper limit of the missing nitrate budget and the impact
this HNO<inline-formula><mml:math id="M620" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> loss has on NH<inline-formula><mml:math id="M621" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M622" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation. As seen in Fig. 6,
the TNO<inline-formula><mml:math id="M623" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> concentration was on average 2.5 times greater than the
TNH<inline-formula><mml:math id="M624" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> concentration measured in the snowpack. This ratio is
strictly for the concentrations measured during the PCAP event. When
averaging TNO<inline-formula><mml:math id="M625" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> : TNH<inline-formula><mml:math id="M626" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> molar ratios for the full lifetime
of the snowpack, the average ratio is slightly greater (3). This average
ratio estimates the relative amount of TNO<inline-formula><mml:math id="M627" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> that may come from
coarse particles. This does not account for HNO<inline-formula><mml:math id="M628" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> dry deposition loss;
therefore, the ratio of NO<inline-formula><mml:math id="M629" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> to NH<inline-formula><mml:math id="M630" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> is an overestimate.
However, with the combination of stable PCAP conditions, in which the vertical
mixing is suppressed, and relatively low ambient concentrations of HNO<inline-formula><mml:math id="M631" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
(<inline-formula><mml:math id="M632" display="inline"><mml:mo lspace="0mm">&lt;</mml:mo></mml:math></inline-formula> 1 ppb), the dry deposition velocities would be relatively small.
Therefore, this overestimate is within reason. This average molar ratio of
2.5 measured during the pollution event was applied to the total NH<inline-formula><mml:math id="M633" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>
measured by the AIM-IC and used as the total nitrate input into ISORROPIA
along with <inline-formula><mml:math id="M634" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Cl<inline-formula><mml:math id="M635" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M636" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M637" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M638" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M639" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M640" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M641" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M642" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M643" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>
concentrations observed by the AIM-IC. Overall, the model predicts greater
amounts of NH<inline-formula><mml:math id="M644" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M645" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and, therefore, PM<inline-formula><mml:math id="M646" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> will form. Based on the
upper-limit estimates of the missing nitrate, the increased amounts of
NH<inline-formula><mml:math id="M647" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M648" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> modelled also represent an upper limit of how much more PM
could potentially form. When observed NH<inline-formula><mml:math id="M649" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M650" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> concentrations are
above 10 <inline-formula><mml:math id="M651" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M652" 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 model predicts roughly 2 times more
NH<inline-formula><mml:math id="M653" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M654" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> mass will form when nitrate lost to coarse particles is
accounted for. The additional modelled <inline-formula><mml:math id="M655" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M656" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> mass is on average 6.8 <inline-formula><mml:math id="M657" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M658" 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> with a maximum of 18 <inline-formula><mml:math id="M659" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi></mml:mrow></mml:math></inline-formula>g m<inline-formula><mml:math id="M660" 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>, which is within the upper-limit range of total nitrate loss predicted when assuming uptake to the
entire bulk of the aerosol particle. This simple analysis also shows how
strongly HNO<inline-formula><mml:math id="M661" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-limited the PCAP event in the SLV was, when additional
nitrate led to increases in NH<inline-formula><mml:math id="M662" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M663" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>. This suggests the coarse
particles have the potential to control NH<inline-formula><mml:math id="M664" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M665" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> formation
indirectly by acting as a permanent sink for HNO<inline-formula><mml:math id="M666" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>, thereby reducing the
amount of available HNO<inline-formula><mml:math id="M667" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> to form PM<inline-formula><mml:math id="M668" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>. Therefore, future campaign
studies should also include coarse particle speciation, especially in
systems involving semi-volatile nitrate salts.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusion</title>
      <p id="d1e6971">The AIM-IC measurements confirmed the dominance of NH<inline-formula><mml:math id="M669" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M670" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> in
wintertime PM<inline-formula><mml:math id="M671" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> pollution events in the SLV. The detection of non-volatile
cations (<inline-formula><mml:math id="M672" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Na<inline-formula><mml:math id="M673" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M674" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>K<inline-formula><mml:math id="M675" display="inline"><mml:msup><mml:mi/><mml:mo>+</mml:mo></mml:msup></mml:math></inline-formula>, <inline-formula><mml:math id="M676" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Ca<inline-formula><mml:math id="M677" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>, and <inline-formula><mml:math id="M678" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>Mg<inline-formula><mml:math id="M679" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>) in PM<inline-formula><mml:math id="M680" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> by
the AIM-IC suggests the presence of mineral dust and/or salt during PCAP
pollution events, which can potentially impact the availability of
HNO<inline-formula><mml:math id="M681" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>. This is due to the reactive uptake of HNO<inline-formula><mml:math id="M682" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> onto NaCl- and
CaCO<inline-formula><mml:math id="M683" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>-containing particles, which can be predominantly found in the
coarse mode. This can introduce a permanent sink for HNO<inline-formula><mml:math id="M684" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>. Due to the
lack of coarse-mode speciation, auxiliary data were used to estimate the
amount of HNO<inline-formula><mml:math id="M685" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> potentially lost to reactive uptake. The APS surface
area data were used to calculate a lifetime for HNO<inline-formula><mml:math id="M686" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> with respect to
uptake that was on the order of minutes, depending on the uptake coefficient
used, which is influenced by particle composition (Fenter et al., 1994; Liu
et al., 2008b; Vlasenko et al., 2006). The potential presence of coarse-mode
nitrate was also supported by the strong correlation between total Ca<inline-formula><mml:math id="M687" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula>
and total NO<inline-formula><mml:math id="M688" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> observed in the snowpack. Total NO<inline-formula><mml:math id="M689" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> in
the snowpack was 2.8 times larger than the total NH<inline-formula><mml:math id="M690" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, implying
there is additional NO<inline-formula><mml:math id="M691" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> that is not observed by PM<inline-formula><mml:math id="M692" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>
<inline-formula><mml:math id="M693" display="inline"><mml:mi>p</mml:mi></mml:math></inline-formula>NO<inline-formula><mml:math id="M694" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula> and gas-phase HNO<inline-formula><mml:math id="M695" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> measurements alone.</p>
      <?pagebreak page8123?><p id="d1e7235"><?xmltex \hack{\newpage}?>The equilibrium dynamics were explored by thermodynamic modelling of trace
gas and PM<inline-formula><mml:math id="M696" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> composition, during episode 2. Despite the discrepancies
between observed and modelled NH<inline-formula><mml:math id="M697" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M698" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> concentrations during PCAP
episode 2, the inclusion of coarse nitrate, from snowpack estimates, into
the model shows that coarse particles could be limiting a significant
portion of the HNO<inline-formula><mml:math id="M699" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> being generated, preventing its reaction with NH<inline-formula><mml:math id="M700" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
to form NH<inline-formula><mml:math id="M701" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:math></inline-formula>NO<inline-formula><mml:math id="M702" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>. The extent to which coarse-mode aerosols are
limiting PM<inline-formula><mml:math id="M703" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> formation remains unanswered and warrants further
investigation of coarse-mode composition and the role these particles play
in the atmospheric chemistry during pollution events.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e7317">Ground site and aircraft data from UWFPS can be found here: <uri>https://csl.noaa.gov/groups/csl7/measurements/2017uwfps/</uri> (NOAA, 2017).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e7326">AH performed the measurements and analysis of snowpack and inorganic gas and particles and wrote the paper. JGM provided input at all stages regarding the measurements, analysis, and discussion of the results. AM collected and analyzed aircraft NH<inline-formula><mml:math id="M704" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> data. AF and AMM obtained and analyzed the aircraft-based AMS data. JCL provided TOEM and NO<inline-formula><mml:math id="M705" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> instrumentation. RB collected and processed TEOM data. AGH and RCP collected and processed APS data. LG collected HR-ToF-CIMS aircraft data. BHL provided processed HR-ToF-CIMS data. SSB and MB planned and organized the UWFPS measurement campaign. All authors discussed the results and contributed to the final paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e7350">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e7356">The authors would like to thank all the members of the UWFPS campaign. The authors
would also like to thank many members from the University of Utah in the
Atmospheric Sciences department for their support. We would especially
like to thank Catherine Chachere and Lauren Zuromski for processing the APS
data. The authors acknowledge the funding support from the Michael Smith
Foreign Study Supplements Program awarded by the Natural Sciences and
Engineering Research Council of Canada. NOAA acknowledges support for Twin
Otter flights from the Utah Division of Air Quality under agreement number
16-049696.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e7361">This research has been supported by the Natural Sciences and Engineering Research Council of Canada (Michael Smith Foreign Study Supplements Program) and the Utah Division of Air Quality (agreement no. 16-049696).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e7367">This paper was edited by Ryan Sullivan and reviewed by two anonymous referees.</p>
  </notes><ref-list>
    <title>References</title>

      <ref id="bib1.bib1"><label>1</label><?label 1?><mixed-citation>Ammann, M., Cox, R. A., Crowley, J. N., Jenkin, M. E., Mellouki, A., Rossi, M. J., Troe, J., and Wallington, T. J.: Evaluated kinetic and photochemical data for atmospheric chemistry: Volume VI – heterogeneous reactions with liquid substrates, Atmos. Chem. Phys., 13, 8045–8228, <ext-link xlink:href="https://doi.org/10.5194/acp-13-8045-2013" ext-link-type="DOI">10.5194/acp-13-8045-2013</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib2"><label>2</label><?label 1?><mixed-citation>Anlauf, K., Li, S. M., Leaitch, R., Brook, J., Hayden, K., Toom-Sauntry, D.,
and Wiebe, A.: Ionic composition and size characteristics of particles in
the Lower Fraser Valley: Pacific 2001 field study, Atmos. Environ., 40,
2662–2675, <ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2005.12.027" ext-link-type="DOI">10.1016/j.atmosenv.2005.12.027</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bib3"><label>3</label><?label 1?><mixed-citation>Baasandorj, M., Hoch, S. W., Bares, R., Lin, J. C., Brown, S. S., Millet, D.
B., Martin, R., Kelly, K., Zarzana, K. J., Whiteman, C. D., Dube, W. P.,
Tonnesen, G., Jaramillo, I. C., and Sohl, J.: Coupling between Chemical and
Meteorological Processes under Persistent Cold-Air Pool Conditions:
Evolution of Wintertime PM<inline-formula><mml:math id="M706" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> Pollution Events and N2O5Observations in Utah's
Salt Lake Valley, Environ. Sci. Technol., 51, 5941–5950,
<ext-link xlink:href="https://doi.org/10.1021/acs.est.6b06603" ext-link-type="DOI">10.1021/acs.est.6b06603</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib4"><label>4</label><?label 1?><mixed-citation>Bares, R., Lin, J. C., Hoch, S. W., Baasandorj, M., Mendoza, D. L., Fasoli,
B., Mitchell, L., Catharine, D., and Stephens, B. B.: The Wintertime
Covariation of CO<inline-formula><mml:math id="M707" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and Criteria Pollutants in an Urban Valley of the Western
United States, J. Geophys. Res.-Atmos., 123, 2684–2703,
<ext-link xlink:href="https://doi.org/10.1002/2017JD027917" ext-link-type="DOI">10.1002/2017JD027917</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib5"><label>5</label><?label 1?><mixed-citation>Behera, S. N., Sharma, M., Aneja, V. P., and Balasubramanian, R.: Ammonia in
the atmosphere: A review on emission sources, atmospheric chemistry and
deposition on terrestrial bodies, Environ. Sci. Pollut. Res., 20,
8092–8131, <ext-link xlink:href="https://doi.org/10.1007/s11356-013-2051-9" ext-link-type="DOI">10.1007/s11356-013-2051-9</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib6"><label>6</label><?label 1?><mixed-citation>Beichert, P. and Finlayson-Pitts, B. J.: Knudsen Cell Studies of the Uptake
of Gaseous HNO <inline-formula><mml:math id="M708" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> and Other Oxides of Nitrogen on Solid NaCl: The Role
of Surface-Adsorbed Water, J. Phys. Chem., 100, 15218–15228,
<ext-link xlink:href="https://doi.org/10.1021/jp960925u" ext-link-type="DOI">10.1021/jp960925u</ext-link>, 1996.</mixed-citation></ref>
      <ref id="bib1.bib7"><label>7</label><?label 1?><mixed-citation>Bernardoni, V., Elser, M., Valli, G., Valentini, S., Bigi, A., Fermo, P.,
Piazzalunga, A., and Vecchi, R.: Size-segregated aerosol in a hot-spot
pollution urban area: Chemical composition and three-way source
apportionment, Environ. Pollut., 231, 601–611,
<ext-link xlink:href="https://doi.org/10.1016/j.envpol.2017.08.040" ext-link-type="DOI">10.1016/j.envpol.2017.08.040</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib8"><label>8</label><?label 1?><mixed-citation>
Bishop, G. A., Peddle, A. M., Stedman, D. H., Air, C., Board, R., Street, I., and Box, P. O.: On-Road Emission Measurements of Reactive Nitrogen Compounds
from Three California Cities, Environ. Sci. Technol., 44, 3616–3620, 2010.</mixed-citation></ref>
      <ref id="bib1.bib9"><label>9</label><?label 1?><mixed-citation>Bishop, G. A., Stedman, D. H., Burgard, D. A., and Atkinson, O.: High-Mileage
Light-Duty Fleet Vehicle Emissions: Their Potentially Overlooked Importance,
Environ. Sci. Technol., 50, 5405–5411, <ext-link xlink:href="https://doi.org/10.1021/acs.est.6b00717" ext-link-type="DOI">10.1021/acs.est.6b00717</ext-link>,
2016.</mixed-citation></ref>
      <ref id="bib1.bib10"><label>10</label><?label 1?><mixed-citation>Chesselet, R., Morelli, J., and Buat-Menard, P.: Variations in ionic ratios
between reference sea water and marine aerosols, J. Geophys. Res., 77,
5116–5131, <ext-link xlink:href="https://doi.org/10.1029/JC077i027p05116" ext-link-type="DOI">10.1029/JC077i027p05116</ext-link>, 1972.</mixed-citation></ref>
      <ref id="bib1.bib11"><label>11</label><?label 1?><mixed-citation>Crowley, J. N., Ammann, M., Cox, R. A., Hynes, R. G., Jenkin, M. E., Mellouki, A., Rossi, M. J., Troe, J., and Wallington, T. J.: Evaluated kinetic and photochemical data for atmospheric chemistry: Volume V – heterogeneous reactions on solid substrates, Atmos. Chem. Phys., 10, 9059–9223, <ext-link xlink:href="https://doi.org/10.5194/acp-10-9059-2010" ext-link-type="DOI">10.5194/acp-10-9059-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib12"><label>12</label><?label 1?><mixed-citation>Dasgupta, P. K., Campbell, S. W., Al-Horr, R. S., Ullah, S. M. R., Li, J.,
Amalfitano, C., and Poor, N. D.: Conversion of sea salt aerosol to NaNO3and
the production of HCl: Analysis of temporal behavior of aerosol
chloride/nitrate and gaseous HCl/HNO<inline-formula><mml:math id="M709" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> concentrations with AIM, Atmos.
Environ., 41, 4242–4257, <ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2006.09.054" ext-link-type="DOI">10.1016/j.atmosenv.2006.09.054</ext-link>, 2007.</mixed-citation></ref>
      <ref id="bib1.bib13"><label>13</label><?label 1?><mixed-citation>Fenter, F. F., Caloz, F., and Rossi, M. J.: Kinetics of nitric acid uptake by
salt, J. Phys. Chem., 98, 9801–9810, <ext-link xlink:href="https://doi.org/10.1021/j100090a014" ext-link-type="DOI">10.1021/j100090a014</ext-link>, 1994.</mixed-citation></ref>
      <ref id="bib1.bib14"><label>14</label><?label 1?><mixed-citation>Fountoukis, C. and Nenes, A.: ISORROPIA II: a computationally efficient
thermodynamic equilibrium model for
<inline-formula><mml:math id="M710" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">K</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M711" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Ca</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M712" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Mg</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M713" display="inline"><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mo>+</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M714" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Na</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M715" display="inline"><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M716" display="inline"><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M717" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>–<inline-formula><mml:math id="M718" 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>
aerosols, Atmos. Chem. Phys., 7, 4639–4659,
<ext-link xlink:href="https://doi.org/10.5194/acp-7-4639-2007" ext-link-type="DOI">10.5194/acp-7-4639-2007</ext-link>, 2007.</mixed-citation></ref>
      <ref id="bib1.bib15"><label>15</label><?label 1?><mixed-citation>Franchin, A., Fibiger, D. L., Goldberger, L., McDuffie, E. E., Moravek, A., Womack, C. C., Crosman, E. T., Docherty, K. S., Dube, W. P., Hoch, S. W., Lee, B. H., Long, R., Murphy, J. G., Thornton, J. A., Brown, S. S., Baasandorj, M., and Middlebrook, A. M.: Airborne and ground-based observations of ammonium-nitrate-dominated aerosols in a shallow boundary layer during intense winter pollution episodes in northern Utah, Atmos. Chem. Phys., 18, 17259–17276, <ext-link xlink:href="https://doi.org/10.5194/acp-18-17259-2018" ext-link-type="DOI">10.5194/acp-18-17259-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib16"><label>16</label><?label 1?><mixed-citation>Gao, Z., Wang, X., Shen, L., Xiang, H., and Wang, H.: Observation and Source
Apportionment of Trace Gases, Water-Soluble Ions and Carbonaceous Aerosol
During a Haze Episode in Wuhan, Atmosphere, 10, 397,
<ext-link xlink:href="https://doi.org/10.3390/atmos10070397" ext-link-type="DOI">10.3390/atmos10070397</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib17"><label>17</label><?label 1?><mixed-citation>Gard, E. E., Kleeman, M. J., Gross, D. S., Hughes, L. S., Allen, J. O.,
Morrical, B. D., Fergenson, D. P., Dienes, T., Gälli, M. E., Johnson, R.
J., Cass, G. R., and Prather, K. A.: Direct observation of heterogeneous
chemistry in the atmosphere, Science, 279, 1184–1187,
<ext-link xlink:href="https://doi.org/10.1126/science.279.5354.1184" ext-link-type="DOI">10.1126/science.279.5354.1184</ext-link>, 1998.</mixed-citation></ref>
      <ref id="bib1.bib18"><label>18</label><?label 1?><mixed-citation>
Goodman, A. L., Underwood, G. M., and Grassian, V. H.: A laboratory study of
the heterogeneous reaction of nitric acid on calcium carbonate particles, J.
Geophys. Res., 105, 29053–29064, 2000.</mixed-citation></ref>
      <ref id="bib1.bib19"><label>19</label><?label 1?><mixed-citation>Green, M. C., Chow, J. C., Watson, J. G., Dick, K., and Inouye, D.: Effects
of snow cover and atmospheric stability on winter PM<inline-formula><mml:math id="M719" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>concentrations in
western U.S. Valleys, J. Appl. Meteorol. Climatol., 54, 1191–1201,
<ext-link xlink:href="https://doi.org/10.1175/JAMC-D-14-0191.1" ext-link-type="DOI">10.1175/JAMC-D-14-0191.1</ext-link>, 2015.</mixed-citation></ref>
      <ref id="bib1.bib20"><label>20</label><?label 1?><mixed-citation>Guo, H., Nenes, A., and Weber, R. J.: The underappreciated role of nonvolatile cations in aerosol ammonium-sulfate molar ratios, Atmos. Chem. Phys., 18, 17307–17323, <ext-link xlink:href="https://doi.org/10.5194/acp-18-17307-2018" ext-link-type="DOI">10.5194/acp-18-17307-2018</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib21"><label>21</label><?label 1?><mixed-citation>Hahnenberger, M. and Nicoll, K.: Meteorological characteristics of dust
storm events in the eastern Great Basin of Utah, U.S.A., Atmos. Environ.,
60, 601–612, <ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2012.06.029" ext-link-type="DOI">10.1016/j.atmosenv.2012.06.029</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib22"><label>22</label><?label 1?><mixed-citation>Hansen, J. C., Woolwine, W. R., Bates, B. L., Clark, J. M., Kuprov, R. Y.,
Mukherjee, P., Murray, J. A., Simmons, M. A., Waite, M. F., Eatough, N. L.,
Eatough, D. J., Long, R., and Grover, B. D.: Semicontinuous PM<inline-formula><mml:math id="M720" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and PM<inline-formula><mml:math id="M721" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula> mass
and composition measurements in Lindon, Utah, during winter 2007, J. Air
Waste Manag. Assoc., 60, 346–355, <ext-link xlink:href="https://doi.org/10.3155/1047-3289.60.3.346" ext-link-type="DOI">10.3155/1047-3289.60.3.346</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib23"><label>23</label><?label 1?><mixed-citation>Hansen, K., Sørensen, L. L., Hertel, O., Geels, C., Skjøth, C. A., Jensen, B., and Boegh, E.: Ammonia emissions from deciduous forest after leaf fall, Biogeosciences, 10, 4577–4589, <ext-link xlink:href="https://doi.org/10.5194/bg-10-4577-2013" ext-link-type="DOI">10.5194/bg-10-4577-2013</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib24"><label>24</label><?label 1?><mixed-citation>Kassomenos, P., Vardoulakis, S., Chaloulakou, A., Grivas, G., Borge, R., and
Lumbreras, J.: Levels, sources and seasonality of coarse particles (PM<inline-formula><mml:math id="M722" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:math></inline-formula>–PM<inline-formula><mml:math id="M723" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>) in three European capitals – Implications for particulate pollution
control, Atmos. Environ., 54, 337–347, <ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2012.02.051" ext-link-type="DOI">10.1016/j.atmosenv.2012.02.051</ext-link>,
2012.</mixed-citation></ref>
      <ref id="bib1.bib25"><label>25</label><?label 1?><mixed-citation>Kelly, K. E., Kotchenruther, R., Kuprov, R., and Silcox, G. D.: Receptor
model source attributions for Utah's Salt Lake City airshed and the impacts
of wintertime secondary ammonium nitrate and ammonium chloride aerosol, J.
Air Waste Manag. Assoc., 63, 575–590, <ext-link xlink:href="https://doi.org/10.1080/10962247.2013.774819" ext-link-type="DOI">10.1080/10962247.2013.774819</ext-link>,
2013.</mixed-citation></ref>
      <ref id="bib1.bib26"><label>26</label><?label 1?><mixed-citation>Kolb, C. E., Cox, R. A., Abbatt, J. P. D., Ammann, M., Davis, E. J., Donaldson, D. J., Garrett, B. C., George, C., Griffiths, P. T., Hanson, D. R., Kulmala, M., McFiggans, G., Pöschl, U., Riipinen, I., Rossi, M. J., Rudich, Y., Wagner, P. E., Winkler, P. M., Worsnop, D. R., and O' Dowd, C. D.: An overview of current issues in the uptake of atmospheric trace gases by aerosols and clouds, Atmos. Chem. Phys., 10, 10561–10605, <ext-link xlink:href="https://doi.org/10.5194/acp-10-10561-2010" ext-link-type="DOI">10.5194/acp-10-10561-2010</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib27"><label>27</label><?label 1?><mixed-citation>Kuo, C. Y., Chen, H. H., Shih, J. F., and Wong, R. H.: Variations of nitrate
and sulfate in the atmosphere on days of high and low particulate matters,
Environ. Toxicol. Chem., 24, 846–851, <ext-link xlink:href="https://doi.org/10.1897/04-198R.1" ext-link-type="DOI">10.1897/04-198R.1</ext-link>, 2005.</mixed-citation></ref>
      <ref id="bib1.bib28"><label>28</label><?label 1?><mixed-citation>Kuprov, R., Eatough, D. J., Cruickshank, T., Olson, N., Cropper, P. M., and
Hansen, J. C.: Composition and secondary formation of fine particulate
matter in the Salt Lake Valley: Winter 2009, J. Air Waste Manag. Assoc.,
64, 957–969, <ext-link xlink:href="https://doi.org/10.1080/10962247.2014.903878" ext-link-type="DOI">10.1080/10962247.2014.903878</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib29"><label>29</label><?label 1?><mixed-citation>Lareau, N. P., Crosman, E., Whiteman, C. D., Horel, J. D., Hoch, S. W.,
Brown, W. O. J., and Horst, T. W.: The persistent cold-air pool study, Bull.
Am. Meteorol. Soc., 94, 51–63, <ext-link xlink:href="https://doi.org/10.1175/BAMS-D-11-00255.1" ext-link-type="DOI">10.1175/BAMS-D-11-00255.1</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib30"><label>30</label><?label 1?><mixed-citation>Lee, B. H., Lopez-Hilfiker, F. D., Veres, P. R., McDuffie, E. E., Fibiger,
D. L., Sparks, T. L., Ebben, C. J., Green, J. R., Schroder, J. C.,
Campuzano-Jost, P., Iyer, S., D'Ambro, E. L., Schobesberger, S., Brown, S.
S., Wooldridge, P. J., Cohen, R. C., Fiddler, M. N., Bililign, S., Jimenez,
J. L., Kurtén, T., Weinheimer, A. J., Jaegle, L., and Thornton, J. A.:
Flight Deployment of a High-Resolution Time-of-Flight Chemical Ionization
Mass Spectrometer: Observations of Reactive Halogen and Nitrogen Oxide
Species, J. Geophys. Res.-Atmos., 123, 7670–7686,
<ext-link xlink:href="https://doi.org/10.1029/2017JD028082" ext-link-type="DOI">10.1029/2017JD028082</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib31"><label>31</label><?label 1?><mixed-citation>Li, R., Wiedinmyer, C., Baker, K. R., and Hannigan, M. P.: Characterization of coarse particulate matter in the western United States: a comparison between observation and modeling, Atmos. Chem. Phys., 13, 1311–1327, <ext-link xlink:href="https://doi.org/10.5194/acp-13-1311-2013" ext-link-type="DOI">10.5194/acp-13-1311-2013</ext-link>, 2013.</mixed-citation></ref>
      <ref id="bib1.bib32"><label>32</label><?label 1?><mixed-citation>Liu, Y., Gibson, E. R., Cain, J. P., Wang, H., Grassian, V. H., and Laskin,
A.: Kinetics of heterogeneous reaction of CaCO<inline-formula><mml:math id="M724" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> particles with gaseous HNO<inline-formula><mml:math id="M725" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>
over a wide range of humidity, J. Phys. Chem. A, 112, 1561–1571,
<ext-link xlink:href="https://doi.org/10.1021/jp076169h" ext-link-type="DOI">10.1021/jp076169h</ext-link>, 2008a.</mixed-citation></ref>
      <ref id="bib1.bib33"><label>33</label><?label 1?><mixed-citation>Liu, Y. J., Zhu, T., Zhao, D. F., and Zhang, Z. F.: Investigation of the hygroscopic properties of Ca(NO3)2 and internally mixed Ca(NO<inline-formula><mml:math id="M726" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula>)<inline-formula><mml:math id="M727" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> <inline-formula><mml:math id="M728" display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> CaCO<inline-formula><mml:math id="M729" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> particles by micro-Raman spectrometry, Atmos. Chem. Phys., 8, 7205–7215, <ext-link xlink:href="https://doi.org/10.5194/acp-8-7205-2008" ext-link-type="DOI">10.5194/acp-8-7205-2008</ext-link>, 2008b.</mixed-citation></ref>
      <?pagebreak page8125?><ref id="bib1.bib34"><label>34</label><?label 1?><mixed-citation>Livingston, C., Rieger, P., and Winer, A.: Ammonia emissions from a
representative in-use fleet of light and medium-duty vehicles in the
California South Coast Air Basin, Atmos. Environ., 43, 3326–3333,
<ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2009.04.009" ext-link-type="DOI">10.1016/j.atmosenv.2009.04.009</ext-link>, 2009.</mixed-citation></ref>
      <ref id="bib1.bib35"><label>35</label><?label 1?><mixed-citation>Long, R. W., Smith, R., Smith, S., Eatough, N. L., Mangelson, N. F.,
Eatough, D. J., Pope, C. A., and Wilson, W. E.: Sources of fine particulate
material along the wasatch front, Energ. Fuel., 16, 282–293,
<ext-link xlink:href="https://doi.org/10.1021/ef010168l" ext-link-type="DOI">10.1021/ef010168l</ext-link>, 2002.</mixed-citation></ref>
      <ref id="bib1.bib36"><label>36</label><?label 1?><mixed-citation>Long, R. W., Eatough, N. L., Mangelson, N. F., Thompson, W., Fiet, K.,
Smith, S., Smith, R., Eatough, D. J., Pope, C. A., and Wilson, W. E.: The
measurement of PM<inline-formula><mml:math id="M730" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, including semi-volatile components, in the EMPACT
program: results from the Salt Lake City Study, Atmos. Environ., 37,
4407–4417, <ext-link xlink:href="https://doi.org/10.1016/s1352-2310(03)00585-5" ext-link-type="DOI">10.1016/s1352-2310(03)00585-5</ext-link>, 2003.</mixed-citation></ref>
      <ref id="bib1.bib37"><label>37</label><?label 1?><mixed-citation>Malek, E., Davis, T., Martin, R. S., and Silva, P. J.: Meteorological and
environmental aspects of one of the worst national air pollution episodes
(January, 2004) in Logan, Cache Valley, Utah, USA, Atmos. Res., 79,
108–122, <ext-link xlink:href="https://doi.org/10.1016/j.atmosres.2005.05.003" ext-link-type="DOI">10.1016/j.atmosres.2005.05.003</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bib38"><label>38</label><?label 1?><mixed-citation>Mangelson, N. F., Lewis, L., Joseph, J. M., Cui, W., Machir, J., Eatough, D.
J., Rees, L. B., Wilkerson, T., and Jensen, D. T.: The contribution of
sulfate and nitrate to atmospheric fine particles during winter inversion
fogs in cache valley, utah, J. Air Waste Manag. Assoc., 47, 167–175,
<ext-link xlink:href="https://doi.org/10.1080/10473289.1997.10464429" ext-link-type="DOI">10.1080/10473289.1997.10464429</ext-link>, 1997.</mixed-citation></ref>
      <ref id="bib1.bib39"><label>39</label><?label 1?><mixed-citation>Markovic, M. Z., VandenBoer, T. C., and Murphy, J. G.: Characterization and
optimization of an online system for the simultaneous measurement of
atmospheric water-soluble constituents in the gas and particle phases, J.
Environ. Monit., 14, 1872–84, <ext-link xlink:href="https://doi.org/10.1039/c2em00004k" ext-link-type="DOI">10.1039/c2em00004k</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib40"><label>40</label><?label 1?><mixed-citation>Maxwell-Meier, K., Weber, R., Song, C., Orsini, D., Ma, Y., Carmichael, G.
R., and Streets, D. G.: Inorganic composition of fine particles in mixed
mineral dust-pollution plumes observed from airborne measurements during
ACE-Asia, J. Geophys. Res.-Atmos., 109, 1–20,
<ext-link xlink:href="https://doi.org/10.1029/2003JD004464" ext-link-type="DOI">10.1029/2003JD004464</ext-link>, 2004.</mixed-citation></ref>
      <ref id="bib1.bib41"><label>41</label><?label 1?><mixed-citation>McDuffie, E. E., Womack, C. C., Fibiger, D. L., Dube, W. P., Franchin, A., Middlebrook, A. M., Goldberger, L., Lee, B. H., Thornton, J. A., Moravek, A., Murphy, J. G., Baasandorj, M., and Brown, S. S.: On the contribution of nocturnal heterogeneous reactive nitrogen chemistry to particulate matter formation during wintertime pollution events in Northern Utah, Atmos. Chem. Phys., 19, 9287–9308, <ext-link xlink:href="https://doi.org/10.5194/acp-19-9287-2019" ext-link-type="DOI">10.5194/acp-19-9287-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib42"><label>42</label><?label 1?><mixed-citation>Moravek, A., Murphy, J. G., Hrdina, A., Lin, J. C., Pennell, C., Franchin, A., Middlebrook, A. M., Fibiger, D. L., Womack, C. C., McDuffie, E. E., Martin, R., Moore, K., Baasandorj, M., and Brown, S. S.: Wintertime spatial distribution of ammonia and its emission sources in the Great Salt Lake region, Atmos. Chem. Phys., 19, 15691–15709, <ext-link xlink:href="https://doi.org/10.5194/acp-19-15691-2019" ext-link-type="DOI">10.5194/acp-19-15691-2019</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib43"><label>43</label><?label 1?><mixed-citation>Mouteva, G. O., Randerson, J. T., Fahrni, S. M., Bush, S. E., Ehleringer, J.
R., Xu, X., Santos, G. M., Kuprov, R., Schichtel, B. A., and Czimczik, C. I.:
Using radiocarbon to constrain black and organic carbon aerosol sources in
Salt Lake City, J. Geophys. Res.-Atmos., 122, 9843–9857,
<ext-link xlink:href="https://doi.org/10.1002/2017JD026519" ext-link-type="DOI">10.1002/2017JD026519</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib44"><label>44</label><?label 1?><mixed-citation>Mozurkewich, M.: The dissociation constant of ammonium nitrate and its
dependence on temperature, relative humidity and particle size, Atmos.
Environ. Part A, Gen. Top., 27, 261–270,
<ext-link xlink:href="https://doi.org/10.1016/0960-1686(93)90356-4" ext-link-type="DOI">10.1016/0960-1686(93)90356-4</ext-link>, 1993.</mixed-citation></ref>
      <ref id="bib1.bib45"><label>45</label><?label 1?><mixed-citation>National Oceanic and Atmospheric Administration (NOAA): Utah Winter Fine Particulate Study 2017, available at: <uri>https://csl.noaa.gov/groups/csl7/measurements/2017uwfps/</uri> (last access: 5 October 2019), 2017.</mixed-citation></ref>
      <ref id="bib1.bib46"><label>46</label><?label 1?><mixed-citation>Nenes, A., Pandis, S. N., and Pilinis, C.: ISORROPIA: A new thermodynamic equilibrium model for multiphase multicomponent inorganic aerosols, Aquat. Geoch., 4, 123–152, <ext-link xlink:href="https://doi.org/10.1023/A:1009604003981" ext-link-type="DOI">10.1023/A:1009604003981</ext-link>, 1998.</mixed-citation></ref>
      <ref id="bib1.bib47"><label>47</label><?label 1?><mixed-citation>Nowak, J. B., Neuman, J. A., Bahreini, R., Brock, C. A., Middlebrook, A. M.,
Wollny, A. G., Holloway, J. S., Peischl, J., Ryerson, T. B., and Fehsenfeld,
F. C.: Airborne observations of ammonia and ammonium nitrate formation over
Houston, Texas, J. Geophys. Res.-Atmos., 115, 1–12,
<ext-link xlink:href="https://doi.org/10.1029/2010JD014195" ext-link-type="DOI">10.1029/2010JD014195</ext-link>, 2010.</mixed-citation></ref>
      <ref id="bib1.bib48"><label>48</label><?label 1?><mixed-citation>Nowak, J. B., Neuman, J. A., Bahreini, R., Middlebrook, A. M., Holloway, J.
S., McKeen, S. A., Parrish, D. D., Ryerson, T. B., and Trainer, M.: Ammonia
sources in the California South Coast Air Basin and their impact on ammonium
nitrate formation, Geophys. Res. Lett., 39, 6–11,
<ext-link xlink:href="https://doi.org/10.1029/2012GL051197" ext-link-type="DOI">10.1029/2012GL051197</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib49"><label>49</label><?label 1?><mixed-citation>Pope, C. A., Hansen, M. L., Long, R. W., Nielsen, K. R., Eatough, N. L.,
Wilson, W. E., and Eatough, D. J.: Ambient Particulate Air Pollution, Heart
Rate Variability, and Blood Markers of Inflammation in a Panel of Elderly
Subjects, Environ. Health Perspect., 112, 339–345, <ext-link xlink:href="https://doi.org/10.1289/ehp.6588" ext-link-type="DOI">10.1289/ehp.6588</ext-link>,
2003.</mixed-citation></ref>
      <ref id="bib1.bib50"><label>50</label><?label 1?><mixed-citation>Pope, C. A., Krewski, D., Gapstur, S. M., Turner, M. C., Jerrett, M., and
Burnett, R. T.: Fine Particulate Air Pollution and Mortality: Response to
Enstrom's Reanalysis of the American Cancer Society Cancer Prevention Study
II Cohort, Dose-Response, 15, 1–5, <ext-link xlink:href="https://doi.org/10.1177/1559325817746303" ext-link-type="DOI">10.1177/1559325817746303</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib51"><label>51</label><?label 1?><mixed-citation>Pósfai, M., Simonics, R., Li, J., Hobbs, P. V., and Buseck, P. R.:
Individual aerosol particles from biomass burning in southern Africa: 1.
Compositions and size distributions of carbonaceous particles, J. Geophys. Res.-Atmos., 108, 1–13, <ext-link xlink:href="https://doi.org/10.1029/2002jd002291" ext-link-type="DOI">10.1029/2002jd002291</ext-link>, 2003.</mixed-citation></ref>
      <ref id="bib1.bib52"><label>52</label><?label 1?><mixed-citation>Rissler, J., Vestin, A., Swietlicki, E., Fisch, G., Zhou, J., Artaxo, P., and Andreae, M. O.: Size distribution and hygroscopic properties of aerosol particles from dry-season biomass burning in Amazonia, Atmos. Chem. Phys., 6, 471–491, <ext-link xlink:href="https://doi.org/10.5194/acp-6-471-2006" ext-link-type="DOI">10.5194/acp-6-471-2006</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bib53"><label>53</label><?label 1?><mixed-citation>Roth, P., Yang, J., Fofie, E., Cocker, D. R., Durbin, T. D., Brezny, R.,
Geller, M., Asa-Awuku, A., and Karavalakis, G.: Catalyzed Gasoline
Particulate Filters Reduce Secondary Organic Aerosol Production from
Gasoline Direct Injection Vehicles, Environ. Sci. Technol., 53,
3037–3047, <ext-link xlink:href="https://doi.org/10.1021/acs.est.8b06418" ext-link-type="DOI">10.1021/acs.est.8b06418</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib54"><label>54</label><?label 1?><mixed-citation>Saul, T. D., Tolocka, M. P., and Johnston, M. V.: Reactive uptake of nitric
acid onto sodium chloride aerosols across a wide range of relative
humidities, J. Phys. Chem. A, 110, 7614–7620, <ext-link xlink:href="https://doi.org/10.1021/jp060639a" ext-link-type="DOI">10.1021/jp060639a</ext-link>,
2006.</mixed-citation></ref>
      <ref id="bib1.bib55"><label>55</label><?label 1?><mixed-citation>
Seinfeld, J. H. and Pandis, S. N.: Atmospheric Chemistry and Physics: From
Air Pollution to Climate Change, 2nd edn., Wile-Interscience, Hoboken, New Jersey, USA, 2006.</mixed-citation></ref>
      <?pagebreak page8126?><ref id="bib1.bib56"><label>56</label><?label 1?><mixed-citation>Silcox, G. D., Kelly, K. E., Crosman, E. T., Whiteman, C. D., and Allen, B.
L.: Wintertime PM<inline-formula><mml:math id="M731" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> concentrations during persistent, multi-day cold-air
pools in a mountain valley, Atmos. Environ., 46, 17–24,
<ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2011.10.041" ext-link-type="DOI">10.1016/j.atmosenv.2011.10.041</ext-link>, 2012.</mixed-citation></ref>
      <ref id="bib1.bib57"><label>57</label><?label 1?><mixed-citation>Skiles, S. M. K., Mallia, D. V., Hallar, A. G., Lin, J. C., Lambert, A.,
Petersen, R., and Clark, S.: Implications of a shrinking Great Salt Lake for
dust on snow deposition in the Wasatch Mountains, UT, as informed by a
source to sink case study from the 13-14 April 2017 dust event, Environ.
Res. Lett., 13, 1–9, <ext-link xlink:href="https://doi.org/10.1088/1748-9326/aaefd8" ext-link-type="DOI">10.1088/1748-9326/aaefd8</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib58"><label>58</label><?label 1?><mixed-citation>Suarez-Bertoa, R., Zardini, A. A., and Astorga, C.: Ammonia exhaust emissions
from spark ignition vehicles over the New European Driving Cycle, Atmos.
Environ., 97, 43–53, <ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2014.07.050" ext-link-type="DOI">10.1016/j.atmosenv.2014.07.050</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib59"><label>59</label><?label 1?><mixed-citation>Sullivan, R. C., Moore, M. J. K., Petters, M. D., Kreidenweis, S. M., Roberts, G. C., and Prather, K. A.: Effect of chemical mixing state on the hygroscopicity and cloud nucleation properties of calcium mineral dust particles, Atmos. Chem. Phys., 9, 3303–3316, <ext-link xlink:href="https://doi.org/10.5194/acp-9-3303-2009" ext-link-type="DOI">10.5194/acp-9-3303-2009</ext-link>, 2009a.</mixed-citation></ref>
      <ref id="bib1.bib60"><label>60</label><?label 1?><mixed-citation>Sullivan, R. C., Moore, M. J. K., Petters, M. D., Kreidenweis, S. M.,
Roberts, G. C., and Prather, K. A.: Timescale for hygroscopic conversion of
calcite mineral particles through heterogeneous reaction with nitric acid,
Phys. Chem. Chem. Phys., 11, 7759, <ext-link xlink:href="https://doi.org/10.1039/b916865f" ext-link-type="DOI">10.1039/b916865f</ext-link>, 2009b.</mixed-citation></ref>
      <ref id="bib1.bib61"><label>61</label><?label 1?><mixed-citation>Sun, K., Tao, L., Miller, D. J., Pan, D., Golston, L. M., Zondlo, M. A.,
Griffin, R. J., Wallace, H. W., Leong, Y. J., Yang, M. M., Zhang, Y.,
Mauzerall, D. L., and Zhu, T.: Vehicle Emissions as an Important Urban
Ammonia Source in the United States and China, Environ. Sci. Technol.,
51, 2472–2481, <ext-link xlink:href="https://doi.org/10.1021/acs.est.6b02805" ext-link-type="DOI">10.1021/acs.est.6b02805</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib62"><label>62</label><?label 1?><mixed-citation>Tang, M., Huang, X., Lu, K., Ge, M., Li, Y., Cheng, P., Zhu, T., Ding, A., Zhang, Y., Gligorovski, S., Song, W., Ding, X., Bi, X., and Wang, X.: Heterogeneous reactions of mineral dust aerosol: implications for tropospheric oxidation capacity, Atmos. Chem. Phys., 17, 11727–11777, <ext-link xlink:href="https://doi.org/10.5194/acp-17-11727-2017" ext-link-type="DOI">10.5194/acp-17-11727-2017</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib63"><label>63</label><?label 1?><mixed-citation>Tian, M., Liu, Y., Yang, F., Zhang, L., Peng, C., Chen, Y., Shi, G., Wang,
H., Luo, B., Jiang, C., Li, B., Takeda, N., and Koizumi, K.: Increasing
importance of nitrate formation for heavy aerosol pollution in two
megacities in Sichuan Basin, southwest China, Environ. Pollut., 250,
898–905, <ext-link xlink:href="https://doi.org/10.1016/j.envpol.2019.04.098" ext-link-type="DOI">10.1016/j.envpol.2019.04.098</ext-link>, 2019.
</mixed-citation></ref><?xmltex \hack{\newpage}?>
      <ref id="bib1.bib64"><label>64</label><?label 1?><mixed-citation>United States Environmental Protection Agency (US EPA): NCore multipollutant monitoring network, available at: <uri>https://www3.epa.gov/ttn/amtic/ncore.html</uri> (last access: 19 November 2018), 2010.</mixed-citation></ref>
      <ref id="bib1.bib65"><label>65</label><?label 1?><mixed-citation>Vecchi, R., Bernardoni, V., Valentini, S., Piazzalunga, A., Fermo, P., and
Valli, G.: Assessment of light extinction at a European polluted urban area
during wintertime: Impact of PM<inline-formula><mml:math id="M732" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:math></inline-formula> composition and sources, Environ. Pollut.,
233, 679–689, <ext-link xlink:href="https://doi.org/10.1016/j.envpol.2017.10.059" ext-link-type="DOI">10.1016/j.envpol.2017.10.059</ext-link>, 2018.</mixed-citation></ref>
      <ref id="bib1.bib66"><label>66</label><?label 1?><mixed-citation>Vlasenko, A., Sjogren, S., Weingartner, E., Stemmler, K., Gäggeler, H. W., and Ammann, M.: Effect of humidity on nitric acid uptake to mineral dust aerosol particles, Atmos. Chem. Phys., 6, 2147–2160, <ext-link xlink:href="https://doi.org/10.5194/acp-6-2147-2006" ext-link-type="DOI">10.5194/acp-6-2147-2006</ext-link>, 2006.</mixed-citation></ref>
      <ref id="bib1.bib67"><label>67</label><?label 1?><mixed-citation>Whiteman, C. D., Hoch, S. W., Horel, J. D., and Charland, A.: Relationship
between particulate air pollution and meteorological variables in Utah's
Salt Lake Valley, Atmos. Environ., 94, 742–753,
<ext-link xlink:href="https://doi.org/10.1016/j.atmosenv.2014.06.012" ext-link-type="DOI">10.1016/j.atmosenv.2014.06.012</ext-link>, 2014.</mixed-citation></ref>
      <ref id="bib1.bib68"><label>68</label><?label 1?><mixed-citation>Womack, C. C., McDuffie, E. E., Edwards, P. M., Bares, R., Gouw, J. A. A., Docherty, K. S., Dubé, W. P., Fibiger, D. L., Franchin, A., Gilman, J. B., Goldberger, L., Lee, B. H., Lin, J. C., Long, R., Middlebrook, A. M., Millet, D. B., Moravek, A., Murphy, J. G., Quinn, P. K., Riedel, T. P., Roberts, J. M., Thornton, J. A., Valin, L. C., Veres, P. R., Whitehill, A. R., Wild, R. J., Warneke, C., Yuan, B., Baasandorj, M., and Brown, S. S.: An Odd Oxygen Framework for Wintertime Ammonium Nitrate Aerosol Pollution in Urban Areas: NO<inline-formula><mml:math id="M733" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> and VOC Control as Mitigation Strategies, Geophys. Res. Lett., 46, 4971–4979, <ext-link xlink:href="https://doi.org/10.1029/2019GL082028" ext-link-type="DOI">10.1029/2019GL082028</ext-link>, 2019.</mixed-citation></ref>
      <ref id="bib1.bib69"><label>69</label><?label 1?><mixed-citation>Wurtsbaugh, W. A., Miller, C., Null, S. E., Justin De Rose, R., Wilcock, P.,
Hahnenberger, M., Howe, F., and Moore, J.: Decline of the world's saline
lakes, Nat. Geosci., 10, 816–821, <ext-link xlink:href="https://doi.org/10.1038/NGEO3052" ext-link-type="DOI">10.1038/NGEO3052</ext-link>, 2017.</mixed-citation></ref>
      <ref id="bib1.bib70"><label>70</label><?label 1?><mixed-citation>Zender, C. S.: Mineral Dust Entrainment and Deposition (DEAD) model:
Description and 1990s dust climatology, J. Geophys. Res., 108, 1–19,
<ext-link xlink:href="https://doi.org/10.1029/2002jd002775" ext-link-type="DOI">10.1029/2002jd002775</ext-link>, 2003.</mixed-citation></ref>

  </ref-list></back>
    <!--<article-title-html>The role of coarse aerosol particles as a sink of HNO<sub>3</sub> in wintertime pollution events in the Salt Lake Valley</article-title-html>
<abstract-html><p>Wintertime ammonium nitrate (NH<sub>4</sub>NO<sub>3</sub>) pollution events
burden urban mountain basins around the globe. In the Salt Lake Valley of
Utah in the United States, such pollution events are often driven by the
formation of persistent cold-air pools (PCAPs) that trap emissions near the
surface for several consecutive days. As a result, secondary pollutants
including fine particulate matter less than 2.5&thinsp;µm in diameter
(PM<sub>2.5</sub>), largely in the form of NH<sub>4</sub>NO<sub>3</sub>, build up during these
events and lead to severe haze. As part of an extensive measurement campaign
to understand the chemical processes underlying PM<sub>2.5</sub> formation, the
2017 Utah Winter Fine Particulate Study, water-soluble trace gases and
PM<sub>2.5</sub> constituents were continuously monitored using the ambient ion
monitoring ion chromatograph (AIM-IC) system at the University of Utah
campus. Gas-phase NH<sub>3</sub>, HNO<sub>3</sub>, HCl, and SO<sub>2</sub> along with
particulate NH<sub>4</sub><sup>+</sup>, Na<sup>+</sup>, K<sup>+</sup>, Mg<sup>2+</sup>, Ca<sup>2+</sup>,
NO<sub>3</sub><sup>−</sup>, Cl<sup>−</sup>, and SO<sub>4</sub><sup>2−</sup> were measured from 21 January
to 21 February 2017. During the two PCAP events captured, the fine
particulate matter was dominated by secondary NH<sub>4</sub>NO<sub>3</sub>. The
comparison of total nitrate (HNO<sub>3</sub>&thinsp;+&thinsp;PM<sub>2.5</sub> NO<sub>3</sub><sup>−</sup>) and
total NH<sub><i>x</i></sub> (NH<sub>3</sub>&thinsp;+&thinsp;PM<sub>2.5</sub> NH<sub>4</sub><sup>+</sup>) showed NH<sub><i>x</i></sub> was
in excess during both pollution events. However, chemical composition
analysis of the snowpack during the first PCAP event revealed that the total
concentration of deposited NO<sub>3</sub><sup>−</sup> was nearly 3 times greater
than that of deposited NH<sub>4</sub><sup>+</sup>. Daily snow composition measurements
showed a strong correlation between NO<sub>3</sub><sup>−</sup> and Ca<sup>2+</sup> in the
snowpack. The presence of non-volatile salts (Na<sup>+</sup>, Ca<sup>2+</sup>, and
Mg<sup>2+</sup>), which are frequently associated with coarse-mode dust, was also
detected in PM<sub>2.5</sub> by the AIM-IC during the two PCAP events,
accounting for roughly 5&thinsp;% of total mass loading. The presence of a
significant particle mass and surface area in the coarse mode during the
first PCAP event was indicated by size-resolved particle measurements from
an aerodynamic particle sizer. Taken together, these observations imply that
atmospheric measurements of the gas-phase and fine-mode particle nitrate may
not represent the total burden of nitrate in the atmosphere, implying a
potentially significant role for uptake by coarse-mode dust. Using the
NO<sub>3</sub><sup>−</sup>&thinsp;:&thinsp;NH<sub>4</sub><sup>+</sup> ratio observed in the snowpack to estimate the
proportion of atmospheric nitrate present in the coarse mode, we estimate
that the amount of secondary NH<sub>4</sub>NO<sub>3</sub> could double in the absence of
the coarse-mode sink. The underestimation of total nitrate indicates an
incomplete account of the total oxidant production during PCAP events. The
ability of coarse particles to permanently remove HNO<sub>3</sub> and influence
PM<sub>2.5</sub> formation is discussed using information about particle
composition and size distribution.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
Ammann, M., Cox, R. A., Crowley, J. N., Jenkin, M. E., Mellouki, A., Rossi, M. J., Troe, J., and Wallington, T. J.: Evaluated kinetic and photochemical data for atmospheric chemistry: Volume VI – heterogeneous reactions with liquid substrates, Atmos. Chem. Phys., 13, 8045–8228, <a href="https://doi.org/10.5194/acp-13-8045-2013" target="_blank">https://doi.org/10.5194/acp-13-8045-2013</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
Anlauf, K., Li, S. M., Leaitch, R., Brook, J., Hayden, K., Toom-Sauntry, D.,
and Wiebe, A.: Ionic composition and size characteristics of particles in
the Lower Fraser Valley: Pacific 2001 field study, Atmos. Environ., 40,
2662–2675, <a href="https://doi.org/10.1016/j.atmosenv.2005.12.027" target="_blank">https://doi.org/10.1016/j.atmosenv.2005.12.027</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
Baasandorj, M., Hoch, S. W., Bares, R., Lin, J. C., Brown, S. S., Millet, D.
B., Martin, R., Kelly, K., Zarzana, K. J., Whiteman, C. D., Dube, W. P.,
Tonnesen, G., Jaramillo, I. C., and Sohl, J.: Coupling between Chemical and
Meteorological Processes under Persistent Cold-Air Pool Conditions:
Evolution of Wintertime PM<sub>2.5</sub> Pollution Events and N2O5Observations in Utah's
Salt Lake Valley, Environ. Sci. Technol., 51, 5941–5950,
<a href="https://doi.org/10.1021/acs.est.6b06603" target="_blank">https://doi.org/10.1021/acs.est.6b06603</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>
Bares, R., Lin, J. C., Hoch, S. W., Baasandorj, M., Mendoza, D. L., Fasoli,
B., Mitchell, L., Catharine, D., and Stephens, B. B.: The Wintertime
Covariation of CO<sub>2</sub> and Criteria Pollutants in an Urban Valley of the Western
United States, J. Geophys. Res.-Atmos., 123, 2684–2703,
<a href="https://doi.org/10.1002/2017JD027917" target="_blank">https://doi.org/10.1002/2017JD027917</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>
Behera, S. N., Sharma, M., Aneja, V. P., and Balasubramanian, R.: Ammonia in
the atmosphere: A review on emission sources, atmospheric chemistry and
deposition on terrestrial bodies, Environ. Sci. Pollut. Res., 20,
8092–8131, <a href="https://doi.org/10.1007/s11356-013-2051-9" target="_blank">https://doi.org/10.1007/s11356-013-2051-9</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>
Beichert, P. and Finlayson-Pitts, B. J.: Knudsen Cell Studies of the Uptake
of Gaseous HNO <sub>3</sub> and Other Oxides of Nitrogen on Solid NaCl: The Role
of Surface-Adsorbed Water, J. Phys. Chem., 100, 15218–15228,
<a href="https://doi.org/10.1021/jp960925u" target="_blank">https://doi.org/10.1021/jp960925u</a>, 1996.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>
Bernardoni, V., Elser, M., Valli, G., Valentini, S., Bigi, A., Fermo, P.,
Piazzalunga, A., and Vecchi, R.: Size-segregated aerosol in a hot-spot
pollution urban area: Chemical composition and three-way source
apportionment, Environ. Pollut., 231, 601–611,
<a href="https://doi.org/10.1016/j.envpol.2017.08.040" target="_blank">https://doi.org/10.1016/j.envpol.2017.08.040</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation>
Bishop, G. A., Peddle, A. M., Stedman, D. H., Air, C., Board, R., Street, I., and Box, P. O.: On-Road Emission Measurements of Reactive Nitrogen Compounds
from Three California Cities, Environ. Sci. Technol., 44, 3616–3620, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>
Bishop, G. A., Stedman, D. H., Burgard, D. A., and Atkinson, O.: High-Mileage
Light-Duty Fleet Vehicle Emissions: Their Potentially Overlooked Importance,
Environ. Sci. Technol., 50, 5405–5411, <a href="https://doi.org/10.1021/acs.est.6b00717" target="_blank">https://doi.org/10.1021/acs.est.6b00717</a>,
2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>
Chesselet, R., Morelli, J., and Buat-Menard, P.: Variations in ionic ratios
between reference sea water and marine aerosols, J. Geophys. Res., 77,
5116–5131, <a href="https://doi.org/10.1029/JC077i027p05116" target="_blank">https://doi.org/10.1029/JC077i027p05116</a>, 1972.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation>
Crowley, J. N., Ammann, M., Cox, R. A., Hynes, R. G., Jenkin, M. E., Mellouki, A., Rossi, M. J., Troe, J., and Wallington, T. J.: Evaluated kinetic and photochemical data for atmospheric chemistry: Volume V – heterogeneous reactions on solid substrates, Atmos. Chem. Phys., 10, 9059–9223, <a href="https://doi.org/10.5194/acp-10-9059-2010" target="_blank">https://doi.org/10.5194/acp-10-9059-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib12"><label>12</label><mixed-citation>
Dasgupta, P. K., Campbell, S. W., Al-Horr, R. S., Ullah, S. M. R., Li, J.,
Amalfitano, C., and Poor, N. D.: Conversion of sea salt aerosol to NaNO3and
the production of HCl: Analysis of temporal behavior of aerosol
chloride/nitrate and gaseous HCl/HNO<sub>3</sub> concentrations with AIM, Atmos.
Environ., 41, 4242–4257, <a href="https://doi.org/10.1016/j.atmosenv.2006.09.054" target="_blank">https://doi.org/10.1016/j.atmosenv.2006.09.054</a>, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib13"><label>13</label><mixed-citation>
Fenter, F. F., Caloz, F., and Rossi, M. J.: Kinetics of nitric acid uptake by
salt, J. Phys. Chem., 98, 9801–9810, <a href="https://doi.org/10.1021/j100090a014" target="_blank">https://doi.org/10.1021/j100090a014</a>, 1994.
</mixed-citation></ref-html>
<ref-html id="bib1.bib14"><label>14</label><mixed-citation>
Fountoukis, C. and Nenes, A.: ISORROPIA II: a computationally efficient
thermodynamic equilibrium model for
K<sup>+</sup>–Ca<sup>2+</sup>–Mg<sup>2+</sup>–NH<sub>4</sub><sup>+</sup>–Na<sup>+</sup>–SO<sub>4</sub><sup>2−</sup>–NO<sub>3</sub><sup>−</sup>–Cl<sup>−</sup>–H<sub>2</sub>O
aerosols, Atmos. Chem. Phys., 7, 4639–4659,
<a href="https://doi.org/10.5194/acp-7-4639-2007" target="_blank">https://doi.org/10.5194/acp-7-4639-2007</a>, 2007.
</mixed-citation></ref-html>
<ref-html id="bib1.bib15"><label>15</label><mixed-citation>
Franchin, A., Fibiger, D. L., Goldberger, L., McDuffie, E. E., Moravek, A., Womack, C. C., Crosman, E. T., Docherty, K. S., Dube, W. P., Hoch, S. W., Lee, B. H., Long, R., Murphy, J. G., Thornton, J. A., Brown, S. S., Baasandorj, M., and Middlebrook, A. M.: Airborne and ground-based observations of ammonium-nitrate-dominated aerosols in a shallow boundary layer during intense winter pollution episodes in northern Utah, Atmos. Chem. Phys., 18, 17259–17276, <a href="https://doi.org/10.5194/acp-18-17259-2018" target="_blank">https://doi.org/10.5194/acp-18-17259-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib16"><label>16</label><mixed-citation>
Gao, Z., Wang, X., Shen, L., Xiang, H., and Wang, H.: Observation and Source
Apportionment of Trace Gases, Water-Soluble Ions and Carbonaceous Aerosol
During a Haze Episode in Wuhan, Atmosphere, 10, 397,
<a href="https://doi.org/10.3390/atmos10070397" target="_blank">https://doi.org/10.3390/atmos10070397</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib17"><label>17</label><mixed-citation>
Gard, E. E., Kleeman, M. J., Gross, D. S., Hughes, L. S., Allen, J. O.,
Morrical, B. D., Fergenson, D. P., Dienes, T., Gälli, M. E., Johnson, R.
J., Cass, G. R., and Prather, K. A.: Direct observation of heterogeneous
chemistry in the atmosphere, Science, 279, 1184–1187,
<a href="https://doi.org/10.1126/science.279.5354.1184" target="_blank">https://doi.org/10.1126/science.279.5354.1184</a>, 1998.
</mixed-citation></ref-html>
<ref-html id="bib1.bib18"><label>18</label><mixed-citation>
Goodman, A. L., Underwood, G. M., and Grassian, V. H.: A laboratory study of
the heterogeneous reaction of nitric acid on calcium carbonate particles, J.
Geophys. Res., 105, 29053–29064, 2000.
</mixed-citation></ref-html>
<ref-html id="bib1.bib19"><label>19</label><mixed-citation>
Green, M. C., Chow, J. C., Watson, J. G., Dick, K., and Inouye, D.: Effects
of snow cover and atmospheric stability on winter PM<sub>2.5</sub>concentrations in
western U.S. Valleys, J. Appl. Meteorol. Climatol., 54, 1191–1201,
<a href="https://doi.org/10.1175/JAMC-D-14-0191.1" target="_blank">https://doi.org/10.1175/JAMC-D-14-0191.1</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib20"><label>20</label><mixed-citation>
Guo, H., Nenes, A., and Weber, R. J.: The underappreciated role of nonvolatile cations in aerosol ammonium-sulfate molar ratios, Atmos. Chem. Phys., 18, 17307–17323, <a href="https://doi.org/10.5194/acp-18-17307-2018" target="_blank">https://doi.org/10.5194/acp-18-17307-2018</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib21"><label>21</label><mixed-citation>
Hahnenberger, M. and Nicoll, K.: Meteorological characteristics of dust
storm events in the eastern Great Basin of Utah, U.S.A., Atmos. Environ.,
60, 601–612, <a href="https://doi.org/10.1016/j.atmosenv.2012.06.029" target="_blank">https://doi.org/10.1016/j.atmosenv.2012.06.029</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib22"><label>22</label><mixed-citation>
Hansen, J. C., Woolwine, W. R., Bates, B. L., Clark, J. M., Kuprov, R. Y.,
Mukherjee, P., Murray, J. A., Simmons, M. A., Waite, M. F., Eatough, N. L.,
Eatough, D. J., Long, R., and Grover, B. D.: Semicontinuous PM<sub>2.5</sub> and PM<sub>10</sub> mass
and composition measurements in Lindon, Utah, during winter 2007, J. Air
Waste Manag. Assoc., 60, 346–355, <a href="https://doi.org/10.3155/1047-3289.60.3.346" target="_blank">https://doi.org/10.3155/1047-3289.60.3.346</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib23"><label>23</label><mixed-citation>
Hansen, K., Sørensen, L. L., Hertel, O., Geels, C., Skjøth, C. A., Jensen, B., and Boegh, E.: Ammonia emissions from deciduous forest after leaf fall, Biogeosciences, 10, 4577–4589, <a href="https://doi.org/10.5194/bg-10-4577-2013" target="_blank">https://doi.org/10.5194/bg-10-4577-2013</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib24"><label>24</label><mixed-citation>
Kassomenos, P., Vardoulakis, S., Chaloulakou, A., Grivas, G., Borge, R., and
Lumbreras, J.: Levels, sources and seasonality of coarse particles (PM<sub>10</sub>–PM<sub>2.5</sub>) in three European capitals – Implications for particulate pollution
control, Atmos. Environ., 54, 337–347, <a href="https://doi.org/10.1016/j.atmosenv.2012.02.051" target="_blank">https://doi.org/10.1016/j.atmosenv.2012.02.051</a>,
2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib25"><label>25</label><mixed-citation>
Kelly, K. E., Kotchenruther, R., Kuprov, R., and Silcox, G. D.: Receptor
model source attributions for Utah's Salt Lake City airshed and the impacts
of wintertime secondary ammonium nitrate and ammonium chloride aerosol, J.
Air Waste Manag. Assoc., 63, 575–590, <a href="https://doi.org/10.1080/10962247.2013.774819" target="_blank">https://doi.org/10.1080/10962247.2013.774819</a>,
2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib26"><label>26</label><mixed-citation>
Kolb, C. E., Cox, R. A., Abbatt, J. P. D., Ammann, M., Davis, E. J., Donaldson, D. J., Garrett, B. C., George, C., Griffiths, P. T., Hanson, D. R., Kulmala, M., McFiggans, G., Pöschl, U., Riipinen, I., Rossi, M. J., Rudich, Y., Wagner, P. E., Winkler, P. M., Worsnop, D. R., and O' Dowd, C. D.: An overview of current issues in the uptake of atmospheric trace gases by aerosols and clouds, Atmos. Chem. Phys., 10, 10561–10605, <a href="https://doi.org/10.5194/acp-10-10561-2010" target="_blank">https://doi.org/10.5194/acp-10-10561-2010</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib27"><label>27</label><mixed-citation>
Kuo, C. Y., Chen, H. H., Shih, J. F., and Wong, R. H.: Variations of nitrate
and sulfate in the atmosphere on days of high and low particulate matters,
Environ. Toxicol. Chem., 24, 846–851, <a href="https://doi.org/10.1897/04-198R.1" target="_blank">https://doi.org/10.1897/04-198R.1</a>, 2005.
</mixed-citation></ref-html>
<ref-html id="bib1.bib28"><label>28</label><mixed-citation>
Kuprov, R., Eatough, D. J., Cruickshank, T., Olson, N., Cropper, P. M., and
Hansen, J. C.: Composition and secondary formation of fine particulate
matter in the Salt Lake Valley: Winter 2009, J. Air Waste Manag. Assoc.,
64, 957–969, <a href="https://doi.org/10.1080/10962247.2014.903878" target="_blank">https://doi.org/10.1080/10962247.2014.903878</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib29"><label>29</label><mixed-citation>
Lareau, N. P., Crosman, E., Whiteman, C. D., Horel, J. D., Hoch, S. W.,
Brown, W. O. J., and Horst, T. W.: The persistent cold-air pool study, Bull.
Am. Meteorol. Soc., 94, 51–63, <a href="https://doi.org/10.1175/BAMS-D-11-00255.1" target="_blank">https://doi.org/10.1175/BAMS-D-11-00255.1</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib30"><label>30</label><mixed-citation>
Lee, B. H., Lopez-Hilfiker, F. D., Veres, P. R., McDuffie, E. E., Fibiger,
D. L., Sparks, T. L., Ebben, C. J., Green, J. R., Schroder, J. C.,
Campuzano-Jost, P., Iyer, S., D'Ambro, E. L., Schobesberger, S., Brown, S.
S., Wooldridge, P. J., Cohen, R. C., Fiddler, M. N., Bililign, S., Jimenez,
J. L., Kurtén, T., Weinheimer, A. J., Jaegle, L., and Thornton, J. A.:
Flight Deployment of a High-Resolution Time-of-Flight Chemical Ionization
Mass Spectrometer: Observations of Reactive Halogen and Nitrogen Oxide
Species, J. Geophys. Res.-Atmos., 123, 7670–7686,
<a href="https://doi.org/10.1029/2017JD028082" target="_blank">https://doi.org/10.1029/2017JD028082</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib31"><label>31</label><mixed-citation>
Li, R., Wiedinmyer, C., Baker, K. R., and Hannigan, M. P.: Characterization of coarse particulate matter in the western United States: a comparison between observation and modeling, Atmos. Chem. Phys., 13, 1311–1327, <a href="https://doi.org/10.5194/acp-13-1311-2013" target="_blank">https://doi.org/10.5194/acp-13-1311-2013</a>, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib32"><label>32</label><mixed-citation>
Liu, Y., Gibson, E. R., Cain, J. P., Wang, H., Grassian, V. H., and Laskin,
A.: Kinetics of heterogeneous reaction of CaCO<sub>3</sub> particles with gaseous HNO<sub>3</sub>
over a wide range of humidity, J. Phys. Chem. A, 112, 1561–1571,
<a href="https://doi.org/10.1021/jp076169h" target="_blank">https://doi.org/10.1021/jp076169h</a>, 2008a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib33"><label>33</label><mixed-citation>
Liu, Y. J., Zhu, T., Zhao, D. F., and Zhang, Z. F.: Investigation of the hygroscopic properties of Ca(NO3)2 and internally mixed Ca(NO<sub>3</sub>)<sub>2</sub>&thinsp;∕&thinsp;CaCO<sub>3</sub> particles by micro-Raman spectrometry, Atmos. Chem. Phys., 8, 7205–7215, <a href="https://doi.org/10.5194/acp-8-7205-2008" target="_blank">https://doi.org/10.5194/acp-8-7205-2008</a>, 2008b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib34"><label>34</label><mixed-citation>
Livingston, C., Rieger, P., and Winer, A.: Ammonia emissions from a
representative in-use fleet of light and medium-duty vehicles in the
California South Coast Air Basin, Atmos. Environ., 43, 3326–3333,
<a href="https://doi.org/10.1016/j.atmosenv.2009.04.009" target="_blank">https://doi.org/10.1016/j.atmosenv.2009.04.009</a>, 2009.
</mixed-citation></ref-html>
<ref-html id="bib1.bib35"><label>35</label><mixed-citation>
Long, R. W., Smith, R., Smith, S., Eatough, N. L., Mangelson, N. F.,
Eatough, D. J., Pope, C. A., and Wilson, W. E.: Sources of fine particulate
material along the wasatch front, Energ. Fuel., 16, 282–293,
<a href="https://doi.org/10.1021/ef010168l" target="_blank">https://doi.org/10.1021/ef010168l</a>, 2002.
</mixed-citation></ref-html>
<ref-html id="bib1.bib36"><label>36</label><mixed-citation>
Long, R. W., Eatough, N. L., Mangelson, N. F., Thompson, W., Fiet, K.,
Smith, S., Smith, R., Eatough, D. J., Pope, C. A., and Wilson, W. E.: The
measurement of PM<sub>2.5</sub>, including semi-volatile components, in the EMPACT
program: results from the Salt Lake City Study, Atmos. Environ., 37,
4407–4417, <a href="https://doi.org/10.1016/s1352-2310(03)00585-5" target="_blank">https://doi.org/10.1016/s1352-2310(03)00585-5</a>, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib37"><label>37</label><mixed-citation>
Malek, E., Davis, T., Martin, R. S., and Silva, P. J.: Meteorological and
environmental aspects of one of the worst national air pollution episodes
(January, 2004) in Logan, Cache Valley, Utah, USA, Atmos. Res., 79,
108–122, <a href="https://doi.org/10.1016/j.atmosres.2005.05.003" target="_blank">https://doi.org/10.1016/j.atmosres.2005.05.003</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib38"><label>38</label><mixed-citation>
Mangelson, N. F., Lewis, L., Joseph, J. M., Cui, W., Machir, J., Eatough, D.
J., Rees, L. B., Wilkerson, T., and Jensen, D. T.: The contribution of
sulfate and nitrate to atmospheric fine particles during winter inversion
fogs in cache valley, utah, J. Air Waste Manag. Assoc., 47, 167–175,
<a href="https://doi.org/10.1080/10473289.1997.10464429" target="_blank">https://doi.org/10.1080/10473289.1997.10464429</a>, 1997.
</mixed-citation></ref-html>
<ref-html id="bib1.bib39"><label>39</label><mixed-citation>
Markovic, M. Z., VandenBoer, T. C., and Murphy, J. G.: Characterization and
optimization of an online system for the simultaneous measurement of
atmospheric water-soluble constituents in the gas and particle phases, J.
Environ. Monit., 14, 1872–84, <a href="https://doi.org/10.1039/c2em00004k" target="_blank">https://doi.org/10.1039/c2em00004k</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib40"><label>40</label><mixed-citation>
Maxwell-Meier, K., Weber, R., Song, C., Orsini, D., Ma, Y., Carmichael, G.
R., and Streets, D. G.: Inorganic composition of fine particles in mixed
mineral dust-pollution plumes observed from airborne measurements during
ACE-Asia, J. Geophys. Res.-Atmos., 109, 1–20,
<a href="https://doi.org/10.1029/2003JD004464" target="_blank">https://doi.org/10.1029/2003JD004464</a>, 2004.
</mixed-citation></ref-html>
<ref-html id="bib1.bib41"><label>41</label><mixed-citation>
McDuffie, E. E., Womack, C. C., Fibiger, D. L., Dube, W. P., Franchin, A., Middlebrook, A. M., Goldberger, L., Lee, B. H., Thornton, J. A., Moravek, A., Murphy, J. G., Baasandorj, M., and Brown, S. S.: On the contribution of nocturnal heterogeneous reactive nitrogen chemistry to particulate matter formation during wintertime pollution events in Northern Utah, Atmos. Chem. Phys., 19, 9287–9308, <a href="https://doi.org/10.5194/acp-19-9287-2019" target="_blank">https://doi.org/10.5194/acp-19-9287-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib42"><label>42</label><mixed-citation>
Moravek, A., Murphy, J. G., Hrdina, A., Lin, J. C., Pennell, C., Franchin, A., Middlebrook, A. M., Fibiger, D. L., Womack, C. C., McDuffie, E. E., Martin, R., Moore, K., Baasandorj, M., and Brown, S. S.: Wintertime spatial distribution of ammonia and its emission sources in the Great Salt Lake region, Atmos. Chem. Phys., 19, 15691–15709, <a href="https://doi.org/10.5194/acp-19-15691-2019" target="_blank">https://doi.org/10.5194/acp-19-15691-2019</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib43"><label>43</label><mixed-citation>
Mouteva, G. O., Randerson, J. T., Fahrni, S. M., Bush, S. E., Ehleringer, J.
R., Xu, X., Santos, G. M., Kuprov, R., Schichtel, B. A., and Czimczik, C. I.:
Using radiocarbon to constrain black and organic carbon aerosol sources in
Salt Lake City, J. Geophys. Res.-Atmos., 122, 9843–9857,
<a href="https://doi.org/10.1002/2017JD026519" target="_blank">https://doi.org/10.1002/2017JD026519</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib44"><label>44</label><mixed-citation>
Mozurkewich, M.: The dissociation constant of ammonium nitrate and its
dependence on temperature, relative humidity and particle size, Atmos.
Environ. Part A, Gen. Top., 27, 261–270,
<a href="https://doi.org/10.1016/0960-1686(93)90356-4" target="_blank">https://doi.org/10.1016/0960-1686(93)90356-4</a>, 1993.
</mixed-citation></ref-html>
<ref-html id="bib1.bib45"><label>45</label><mixed-citation>
National Oceanic and Atmospheric Administration (NOAA): Utah Winter Fine Particulate Study 2017, available at: <a href="https://csl.noaa.gov/groups/csl7/measurements/2017uwfps/" target="_blank"/> (last access: 5 October 2019), 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib46"><label>46</label><mixed-citation>
Nenes, A., Pandis, S. N., and Pilinis, C.: ISORROPIA: A new thermodynamic equilibrium model for multiphase multicomponent inorganic aerosols, Aquat. Geoch., 4, 123–152, <a href="https://doi.org/10.1023/A:1009604003981" target="_blank">https://doi.org/10.1023/A:1009604003981</a>, 1998.
</mixed-citation></ref-html>
<ref-html id="bib1.bib47"><label>47</label><mixed-citation>
Nowak, J. B., Neuman, J. A., Bahreini, R., Brock, C. A., Middlebrook, A. M.,
Wollny, A. G., Holloway, J. S., Peischl, J., Ryerson, T. B., and Fehsenfeld,
F. C.: Airborne observations of ammonia and ammonium nitrate formation over
Houston, Texas, J. Geophys. Res.-Atmos., 115, 1–12,
<a href="https://doi.org/10.1029/2010JD014195" target="_blank">https://doi.org/10.1029/2010JD014195</a>, 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib48"><label>48</label><mixed-citation>
Nowak, J. B., Neuman, J. A., Bahreini, R., Middlebrook, A. M., Holloway, J.
S., McKeen, S. A., Parrish, D. D., Ryerson, T. B., and Trainer, M.: Ammonia
sources in the California South Coast Air Basin and their impact on ammonium
nitrate formation, Geophys. Res. Lett., 39, 6–11,
<a href="https://doi.org/10.1029/2012GL051197" target="_blank">https://doi.org/10.1029/2012GL051197</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib49"><label>49</label><mixed-citation>
Pope, C. A., Hansen, M. L., Long, R. W., Nielsen, K. R., Eatough, N. L.,
Wilson, W. E., and Eatough, D. J.: Ambient Particulate Air Pollution, Heart
Rate Variability, and Blood Markers of Inflammation in a Panel of Elderly
Subjects, Environ. Health Perspect., 112, 339–345, <a href="https://doi.org/10.1289/ehp.6588" target="_blank">https://doi.org/10.1289/ehp.6588</a>,
2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib50"><label>50</label><mixed-citation>
Pope, C. A., Krewski, D., Gapstur, S. M., Turner, M. C., Jerrett, M., and
Burnett, R. T.: Fine Particulate Air Pollution and Mortality: Response to
Enstrom's Reanalysis of the American Cancer Society Cancer Prevention Study
II Cohort, Dose-Response, 15, 1–5, <a href="https://doi.org/10.1177/1559325817746303" target="_blank">https://doi.org/10.1177/1559325817746303</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib51"><label>51</label><mixed-citation>
Pósfai, M., Simonics, R., Li, J., Hobbs, P. V., and Buseck, P. R.:
Individual aerosol particles from biomass burning in southern Africa: 1.
Compositions and size distributions of carbonaceous particles, J. Geophys. Res.-Atmos., 108, 1–13, <a href="https://doi.org/10.1029/2002jd002291" target="_blank">https://doi.org/10.1029/2002jd002291</a>, 2003.
</mixed-citation></ref-html>
<ref-html id="bib1.bib52"><label>52</label><mixed-citation>
Rissler, J., Vestin, A., Swietlicki, E., Fisch, G., Zhou, J., Artaxo, P., and Andreae, M. O.: Size distribution and hygroscopic properties of aerosol particles from dry-season biomass burning in Amazonia, Atmos. Chem. Phys., 6, 471–491, <a href="https://doi.org/10.5194/acp-6-471-2006" target="_blank">https://doi.org/10.5194/acp-6-471-2006</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib53"><label>53</label><mixed-citation>
Roth, P., Yang, J., Fofie, E., Cocker, D. R., Durbin, T. D., Brezny, R.,
Geller, M., Asa-Awuku, A., and Karavalakis, G.: Catalyzed Gasoline
Particulate Filters Reduce Secondary Organic Aerosol Production from
Gasoline Direct Injection Vehicles, Environ. Sci. Technol., 53,
3037–3047, <a href="https://doi.org/10.1021/acs.est.8b06418" target="_blank">https://doi.org/10.1021/acs.est.8b06418</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib54"><label>54</label><mixed-citation>
Saul, T. D., Tolocka, M. P., and Johnston, M. V.: Reactive uptake of nitric
acid onto sodium chloride aerosols across a wide range of relative
humidities, J. Phys. Chem. A, 110, 7614–7620, <a href="https://doi.org/10.1021/jp060639a" target="_blank">https://doi.org/10.1021/jp060639a</a>,
2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib55"><label>55</label><mixed-citation>
Seinfeld, J. H. and Pandis, S. N.: Atmospheric Chemistry and Physics: From
Air Pollution to Climate Change, 2nd edn., Wile-Interscience, Hoboken, New Jersey, USA, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib56"><label>56</label><mixed-citation>
Silcox, G. D., Kelly, K. E., Crosman, E. T., Whiteman, C. D., and Allen, B.
L.: Wintertime PM<sub>2.5</sub> concentrations during persistent, multi-day cold-air
pools in a mountain valley, Atmos. Environ., 46, 17–24,
<a href="https://doi.org/10.1016/j.atmosenv.2011.10.041" target="_blank">https://doi.org/10.1016/j.atmosenv.2011.10.041</a>, 2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib57"><label>57</label><mixed-citation>
Skiles, S. M. K., Mallia, D. V., Hallar, A. G., Lin, J. C., Lambert, A.,
Petersen, R., and Clark, S.: Implications of a shrinking Great Salt Lake for
dust on snow deposition in the Wasatch Mountains, UT, as informed by a
source to sink case study from the 13-14 April 2017 dust event, Environ.
Res. Lett., 13, 1–9, <a href="https://doi.org/10.1088/1748-9326/aaefd8" target="_blank">https://doi.org/10.1088/1748-9326/aaefd8</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib58"><label>58</label><mixed-citation>
Suarez-Bertoa, R., Zardini, A. A., and Astorga, C.: Ammonia exhaust emissions
from spark ignition vehicles over the New European Driving Cycle, Atmos.
Environ., 97, 43–53, <a href="https://doi.org/10.1016/j.atmosenv.2014.07.050" target="_blank">https://doi.org/10.1016/j.atmosenv.2014.07.050</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib59"><label>59</label><mixed-citation>
Sullivan, R. C., Moore, M. J. K., Petters, M. D., Kreidenweis, S. M., Roberts, G. C., and Prather, K. A.: Effect of chemical mixing state on the hygroscopicity and cloud nucleation properties of calcium mineral dust particles, Atmos. Chem. Phys., 9, 3303–3316, <a href="https://doi.org/10.5194/acp-9-3303-2009" target="_blank">https://doi.org/10.5194/acp-9-3303-2009</a>, 2009a.
</mixed-citation></ref-html>
<ref-html id="bib1.bib60"><label>60</label><mixed-citation>
Sullivan, R. C., Moore, M. J. K., Petters, M. D., Kreidenweis, S. M.,
Roberts, G. C., and Prather, K. A.: Timescale for hygroscopic conversion of
calcite mineral particles through heterogeneous reaction with nitric acid,
Phys. Chem. Chem. Phys., 11, 7759, <a href="https://doi.org/10.1039/b916865f" target="_blank">https://doi.org/10.1039/b916865f</a>, 2009b.
</mixed-citation></ref-html>
<ref-html id="bib1.bib61"><label>61</label><mixed-citation>
Sun, K., Tao, L., Miller, D. J., Pan, D., Golston, L. M., Zondlo, M. A.,
Griffin, R. J., Wallace, H. W., Leong, Y. J., Yang, M. M., Zhang, Y.,
Mauzerall, D. L., and Zhu, T.: Vehicle Emissions as an Important Urban
Ammonia Source in the United States and China, Environ. Sci. Technol.,
51, 2472–2481, <a href="https://doi.org/10.1021/acs.est.6b02805" target="_blank">https://doi.org/10.1021/acs.est.6b02805</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib62"><label>62</label><mixed-citation>
Tang, M., Huang, X., Lu, K., Ge, M., Li, Y., Cheng, P., Zhu, T., Ding, A., Zhang, Y., Gligorovski, S., Song, W., Ding, X., Bi, X., and Wang, X.: Heterogeneous reactions of mineral dust aerosol: implications for tropospheric oxidation capacity, Atmos. Chem. Phys., 17, 11727–11777, <a href="https://doi.org/10.5194/acp-17-11727-2017" target="_blank">https://doi.org/10.5194/acp-17-11727-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib63"><label>63</label><mixed-citation>
Tian, M., Liu, Y., Yang, F., Zhang, L., Peng, C., Chen, Y., Shi, G., Wang,
H., Luo, B., Jiang, C., Li, B., Takeda, N., and Koizumi, K.: Increasing
importance of nitrate formation for heavy aerosol pollution in two
megacities in Sichuan Basin, southwest China, Environ. Pollut., 250,
898–905, <a href="https://doi.org/10.1016/j.envpol.2019.04.098" target="_blank">https://doi.org/10.1016/j.envpol.2019.04.098</a>, 2019.

</mixed-citation></ref-html>
<ref-html id="bib1.bib64"><label>64</label><mixed-citation>
United States Environmental Protection Agency (US EPA): NCore multipollutant monitoring network, available at: <a href="https://www3.epa.gov/ttn/amtic/ncore.html" target="_blank"/> (last access: 19 November 2018), 2010.
</mixed-citation></ref-html>
<ref-html id="bib1.bib65"><label>65</label><mixed-citation>
Vecchi, R., Bernardoni, V., Valentini, S., Piazzalunga, A., Fermo, P., and
Valli, G.: Assessment of light extinction at a European polluted urban area
during wintertime: Impact of PM<sub>1</sub> composition and sources, Environ. Pollut.,
233, 679–689, <a href="https://doi.org/10.1016/j.envpol.2017.10.059" target="_blank">https://doi.org/10.1016/j.envpol.2017.10.059</a>, 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib66"><label>66</label><mixed-citation>
Vlasenko, A., Sjogren, S., Weingartner, E., Stemmler, K., Gäggeler, H. W., and Ammann, M.: Effect of humidity on nitric acid uptake to mineral dust aerosol particles, Atmos. Chem. Phys., 6, 2147–2160, <a href="https://doi.org/10.5194/acp-6-2147-2006" target="_blank">https://doi.org/10.5194/acp-6-2147-2006</a>, 2006.
</mixed-citation></ref-html>
<ref-html id="bib1.bib67"><label>67</label><mixed-citation>
Whiteman, C. D., Hoch, S. W., Horel, J. D., and Charland, A.: Relationship
between particulate air pollution and meteorological variables in Utah's
Salt Lake Valley, Atmos. Environ., 94, 742–753,
<a href="https://doi.org/10.1016/j.atmosenv.2014.06.012" target="_blank">https://doi.org/10.1016/j.atmosenv.2014.06.012</a>, 2014.
</mixed-citation></ref-html>
<ref-html id="bib1.bib68"><label>68</label><mixed-citation>
Womack, C. C., McDuffie, E. E., Edwards, P. M., Bares, R., Gouw, J. A. A., Docherty, K. S., Dubé, W. P., Fibiger, D. L., Franchin, A., Gilman, J. B., Goldberger, L., Lee, B. H., Lin, J. C., Long, R., Middlebrook, A. M., Millet, D. B., Moravek, A., Murphy, J. G., Quinn, P. K., Riedel, T. P., Roberts, J. M., Thornton, J. A., Valin, L. C., Veres, P. R., Whitehill, A. R., Wild, R. J., Warneke, C., Yuan, B., Baasandorj, M., and Brown, S. S.: An Odd Oxygen Framework for Wintertime Ammonium Nitrate Aerosol Pollution in Urban Areas: NO<sub><i>x</i></sub> and VOC Control as Mitigation Strategies, Geophys. Res. Lett., 46, 4971–4979, <a href="https://doi.org/10.1029/2019GL082028" target="_blank">https://doi.org/10.1029/2019GL082028</a>, 2019.
</mixed-citation></ref-html>
<ref-html id="bib1.bib69"><label>69</label><mixed-citation>
Wurtsbaugh, W. A., Miller, C., Null, S. E., Justin De Rose, R., Wilcock, P.,
Hahnenberger, M., Howe, F., and Moore, J.: Decline of the world's saline
lakes, Nat. Geosci., 10, 816–821, <a href="https://doi.org/10.1038/NGEO3052" target="_blank">https://doi.org/10.1038/NGEO3052</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib70"><label>70</label><mixed-citation>
Zender, C. S.: Mineral Dust Entrainment and Deposition (DEAD) model:
Description and 1990s dust climatology, J. Geophys. Res., 108, 1–19,
<a href="https://doi.org/10.1029/2002jd002775" target="_blank">https://doi.org/10.1029/2002jd002775</a>, 2003.
</mixed-citation></ref-html>--></article>
