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  <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-18-15451-2018</article-id><title-group><article-title>Primary emissions of glyoxal and methylglyoxal from laboratory measurements of open biomass burning</article-title><alt-title>Glyoxal from biomass burning</alt-title>
      </title-group><?xmltex \runningtitle{Glyoxal from biomass burning}?><?xmltex \runningauthor{K.~J.~Zarzana et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff6">
          <name><surname>Zarzana</surname><given-names>Kyle J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1581-6419</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Selimovic</surname><given-names>Vanessa</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff4 aff7">
          <name><surname>Koss</surname><given-names>Abigail R.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff5">
          <name><surname>Sekimoto</surname><given-names>Kanako</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Coggon</surname><given-names>Matthew M.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff8">
          <name><surname>Yuan</surname><given-names>Bin</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3041-0329</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Dubé</surname><given-names>William P.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Yokelson</surname><given-names>Robert J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8415-6808</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Warneke</surname><given-names>Carsten</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff4">
          <name><surname>de Gouw</surname><given-names>Joost A.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-0385-1826</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Roberts</surname><given-names>James M.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-8485-8172</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff4">
          <name><surname>Brown</surname><given-names>Steven S.</given-names></name>
          <email>steven.s.brown@noaa.gov</email>
        </contrib>
        <aff id="aff1"><label>1</label><institution>NOAA Earth System Research Laboratory (ESRL) Chemical Sciences Division, Boulder, CO 80305, USA</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Cooperative Institute for Research in Environmental Sciences, University of Colorado Boulder, Boulder, CO 80309, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Chemistry and Biochemistry, University of Montana, Missoula, MT 59812, USA</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Department of Chemistry and Biochemistry, University of Colorado Boulder, Boulder, CO 80309, USA</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Graduate School of Nanobioscience, Yokohama City University, Yokohama, Kanagawa 236-0027, Japan</institution>
        </aff>
        <aff id="aff6"><label>a</label><institution>now at: Department of Chemistry and Biochemistry, University of Colorado Boulder, Boulder, CO 80309, USA</institution>
        </aff>
        <aff id="aff7"><label>b</label><institution>now at: Department of Civil and Environmental Engineering, Massachusetts Institute of Technology,<?xmltex \hack{\break}?> Cambridge, MA 02142, USA</institution>
        </aff>
        <aff id="aff8"><label>c</label><institution>now at: Institute of Environment and Climate Research, Jinan University, Guangzhou 510632, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Steven S. Brown (steven.s.brown@noaa.gov)</corresp></author-notes><pub-date><day>26</day><month>October</month><year>2018</year></pub-date>
      
      <volume>18</volume>
      <issue>20</issue>
      <fpage>15451</fpage><lpage>15470</lpage>
      <history>
        <date date-type="received"><day>24</day><month>May</month><year>2018</year></date>
           <date date-type="rev-request"><day>13</day><month>June</month><year>2018</year></date>
           <date date-type="rev-recd"><day>26</day><month>September</month><year>2018</year></date>
           <date date-type="accepted"><day>27</day><month>September</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <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/18/15451/2018/acp-18-15451-2018.html">This article is available from https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018.pdf</self-uri>
      <abstract>
    <p id="d1e231">We report the emissions of glyoxal and methylglyoxal from the open burning of
biomass during the NOAA-led 2016 FIREX intensive at the Fire Sciences
Laboratory in Missoula, MT. Both compounds were measured using cavity-enhanced spectroscopy, which is both more sensitive and more selective than
methods previously used to determine emissions of these two compounds. A
total of 75 burns were conducted, using 33 different fuels in 8 different
categories, providing a far more comprehensive dataset for emissions than was
previously available. Measurements of methylglyoxal using our instrument
suffer from spectral interferences from several other species, and the values
reported here are likely underestimates, possibly by as much as 70 %.
Methylglyoxal emissions were 2–3 times higher than glyoxal emissions on a
molar basis, in contrast to previous studies that report methylglyoxal
emissions lower than glyoxal emissions. Methylglyoxal emission ratios for all
fuels averaged <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">2.4</mml:mn></mml:mrow></mml:math></inline-formula> ppbv methylglyoxal (ppmv <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>)<inline-formula><mml:math id="M3" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, while emission
factors averaged <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.66</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.50</mml:mn></mml:mrow></mml:math></inline-formula> g methylglyoxal (kg fuel burned)<inline-formula><mml:math id="M5" 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>. Primary
emissions of glyoxal from biomass burning were much lower than previous
laboratory measurements but consistent with recent measurements from
aircraft. Glyoxal emission ratios for all fuels averaged <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula> ppbv glyoxal (ppmv <inline-formula><mml:math id="M7" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>)<inline-formula><mml:math id="M8" 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>, while
emission factors averaged <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.20</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.12</mml:mn></mml:mrow></mml:math></inline-formula> g glyoxal (kg fuel burned)<inline-formula><mml:math id="M10" 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>, values that are at least a factor of 4 lower than
assumed in previous estimates of the global glyoxal budget. While there was
significant variability in the glyoxal emission ratios and factors between
the different fuel groups, glyoxal and formaldehyde were highly correlated
during the course of any given fire, and the ratio of glyoxal to
formaldehyde, <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, was consistent across many different fuel
types, with an average value of <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.068</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.018</mml:mn></mml:mrow></mml:math></inline-formula>. While <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values
for fresh emissions were consistent across many fuel types, further work is
required to determine how this value changes as the emissions age.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e389">In addition to the large primary emissions of gases and particulate matter,
the secondary chemistry that occurs downwind of fires can play an important
role in numerous atmospheric processes. Ozone (<inline-formula><mml:math id="M14" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), peroxy nitrates
such as acetyl peroxynitrate (PAN), and organic aerosol are frequently
enhanced in downwind fire plumes <xref ref-type="bibr" rid="bib1.bibx79 bib1.bibx3 bib1.bibx6 bib1.bibx41" id="paren.1"><named-content content-type="pre">e.g.,</named-content></xref>, and in<?pagebreak page15452?> urban areas influenced by biomass burning,
emissions from fires have been shown to increase <inline-formula><mml:math id="M15" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> above the 70
ppbv standard set by the EPA <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx23" id="paren.2"/>. Modeling of
the chemistry of biomass burning plumes has found that carbonyls such as
formaldehyde, methylglyoxal, and 2,3-butanedione play a large role in the
formation of both <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and PAN <xref ref-type="bibr" rid="bib1.bibx42 bib1.bibx48" id="paren.3"/>, either
through reactions with hydroxyl radicals or photolysis. Carbonyl photolysis
leading to <inline-formula><mml:math id="M17" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> production has also been observed in other regions,
such as oil and natural gas producing basins <xref ref-type="bibr" rid="bib1.bibx17" id="paren.4"/>. In addition
to contributing to <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> formation, photolysis of carbonyls such as
acetone and methylglyoxal can lead to the formation of PAN
<xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx48" id="paren.5"/>. Understanding the impact of carbonyls on
fire plume chemistry requires accurate measurements of emissions of these
compounds, but those data are lacking for several carbonyl species,
particularly small <inline-formula><mml:math id="M19" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-dicarbonyls such as glyoxal and methylglyoxal.</p>
      <p id="d1e472">Along with glyoxal and methylglyoxal, numerous other carbonyl species such as
formaldehyde have been detected in fire plumes <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx62 bib1.bibx34" id="paren.6"><named-content content-type="pre">e.g.,</named-content></xref>. While methylglyoxal's absorption cross
section is relatively weak and unstructured, the cross sections of glyoxal
and formaldehyde in the visible and ultraviolet respectively are large and
structured, enabling the detection of those two molecules from space using
remote sensing instruments such as the Scanning Imaging Absorption
Spectrometer for Atmospheric Cartography <xref ref-type="bibr" rid="bib1.bibx76 bib1.bibx49" id="paren.7"><named-content content-type="pre">SCIAMACHY,</named-content></xref>, the Global Ozone Monitoring Experiment-2
<xref ref-type="bibr" rid="bib1.bibx39" id="paren.8"><named-content content-type="pre">GOME-2,</named-content></xref>, the Ozone Monitoring Instrument
<xref ref-type="bibr" rid="bib1.bibx5 bib1.bibx12" id="paren.9"><named-content content-type="pre">OMI,</named-content></xref>, or the Tropospheric Emissions:
Monitoring Pollution Instrument <xref ref-type="bibr" rid="bib1.bibx83" id="paren.10"><named-content content-type="pre">TEMPO,</named-content></xref>.</p>
      <p id="d1e500">The column abundances of glyoxal and formaldehyde are enhanced in regions
influenced by biomass burning <xref ref-type="bibr" rid="bib1.bibx12" id="paren.11"/>, but the main source of
both molecules globally is oxidation of larger volatile organic compounds (VOCs)
<xref ref-type="bibr" rid="bib1.bibx57 bib1.bibx21 bib1.bibx20" id="paren.12"/>. The relative yields of
glyoxal and formaldehyde depend in part on the precursor VOC, and the ratio
of glyoxal to formaldehyde, <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, is higher in regions dominated
by emissions of aromatic VOCs than it is in regions dominated by emissions of
isoprene <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx31" id="paren.13"/>. <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> has been
proposed as a metric for examining VOC chemistry from space
<xref ref-type="bibr" rid="bib1.bibx72 bib1.bibx12 bib1.bibx31" id="paren.14"/>, as glyoxal and
formaldehyde have similar atmospheric lifetimes with respect to photolysis
and OH (<inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:math></inline-formula> h), but they have different yields from VOC oxidation.
However, doing so requires both accurate yields from oxidation reactions and
a thorough understanding of direct emissions from sources producing both
compounds, such as biomass burning.</p>
      <p id="d1e548">Together, direct emissions from biomass burning and biofuel (biomass used as
an energy source) have been estimated to contribute 20 % of the glyoxal
budget but only 3.5 % of the methylglyoxal budget <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx58" id="paren.15"/>. While there have been numerous measurements of
formaldehyde emissions from biomass burning both in the laboratory and the
field, glyoxal and methylglyoxal emissions in current models are based on
only two laboratory studies <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx27" id="paren.16"/>. These studies
examined only a limited number of fuels, and the method used in those studies
to quantify carbonyl emissions is now known to be prone to interferences
<xref ref-type="bibr" rid="bib1.bibx33 bib1.bibx1" id="paren.17"/>. The reported emissions of glyoxal and
methylglyoxal from those studies are contradicted by field measurements from
aircraft that find significantly less glyoxal but more methylglyoxal in fresh
biomass burning plumes than was measured in the lab <xref ref-type="bibr" rid="bib1.bibx82" id="paren.18"/>.
Additionally, the laboratory studies reported that glyoxal and formaldehyde
are emitted at a molar ratio of 1, roughly an order of magnitude higher than
what was observed in the field <xref ref-type="bibr" rid="bib1.bibx82" id="paren.19"/> and from remote sensing
platforms over regions dominated by biomass burning <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx60" id="paren.20"/>.</p>
      <p id="d1e571">Models have generally been able to reproduce the formaldehyde columns
observed by satellites <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx8" id="paren.21"/> but have had
varying success reproducing glyoxal columns. Several studies comparing model
outputs to satellite columns retrieved by SCIAMACHY and GOME-2 have found
that the models underestimate global glyoxal emissions
<xref ref-type="bibr" rid="bib1.bibx49 bib1.bibx58 bib1.bibx39" id="paren.22"/>. A more recent
study by <xref ref-type="bibr" rid="bib1.bibx60" id="text.23"/> examined emissions from crop residue fires in
the North China Plain using data from OMI. The column <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
measured by OMI (<inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula>–0.05) was comparable to the <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
values observed by <xref ref-type="bibr" rid="bib1.bibx82" id="text.24"/>, and a model was able to reproduce the
measured formaldehyde columns and the glyoxal enhancements observed during
the height of the burning season. However, <xref ref-type="bibr" rid="bib1.bibx60" id="text.25"/> used glyoxal
emissions from the two previous laboratory studies, which are both higher
than recent field data and imply that <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> should be close to 1.
Better measurements of emissions of glyoxal and methylglyoxal from biomass
burning from a wider range of fuels, and subsequent chemistry following
emission, are needed to resolve these discrepancies and provide better inputs
to models.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><caption><p id="d1e635">Setup of ACES, the OP-FTIR, and the PTR-ToF at the FSL during the
2016 campaign (diagram not to scale). <bold>(a)</bold> Installation of ACES and the
OP-FTIR on the platform. The inlet for ACES was located immediately above the
OP-FTIR. <bold>(b)</bold> View from the platform looking down to the burn chamber floor
showing the stack and the window of the control room, where the PTR-ToF was
located. <bold>(c)</bold> View of the stack and platform from the burn chamber floor.
<bold>(d)</bold> View of the stack and control room from the burn chamber floor, showing the
PTR-ToF transfer line.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f01.pdf"/>

      </fig>

      <p id="d1e656">In this work we use cavity-enhanced spectroscopy (CES) to measure primary
emissions of glyoxal and methylglyoxal from open burns conducted in a
laboratory setting. These experiments were conducted as part of the NOAA-led
Fire Influence on Regional and Global Environments Experiment (FIREX), which
took place from October to November 2016 at the US Forest Service Fire
Sciences Laboratory (FSL) in Missoula, MT. CES measurements of glyoxal and
methylglyoxal are faster, more sensitive, and more specific than the methods
used in previous studies. Over 30 different fuel types were burned during
the 2016 FIREX campaign, and, combined with the other<?pagebreak page15453?> instrumentation
deployed at the FSL, our data provide the most detailed look to date at
direct emissions of glyoxal and methylglyoxal from biomass burning.</p><?xmltex \hack{\vspace{-3mm}}?>
</sec>
<sec id="Ch1.S2">
  <title>Methods</title>
<sec id="Ch1.S2.SS1">
  <title>FSL facility</title>
      <p id="d1e671">Burns were conducted at the FSL during the 2016 FIREX intensive
(<uri>https://www.esrl.noaa.gov/csd/projects/firex/firelab/</uri>, last access: 23 May 2018). Details on the FSL
facility <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx16 bib1.bibx11" id="paren.26"/> and the FIREX
campaign <xref ref-type="bibr" rid="bib1.bibx56" id="paren.27"/> are given elsewhere. The data presented here
were collected during the 75 stack burns conducted during the first three
weeks of the campaign and primarily come from three instruments: the NOAA
Airborne Cavity Enhanced Spectrometer (ACES), the NOAA
proton-transfer-reaction time-of-flight mass spectrometer (PTR-ToF), and the
University of Montana open-path Fourier transform infrared spectrometer
(OP-FTIR). The setup of the three instruments during the stack burns is shown
in Fig. <xref ref-type="fig" rid="Ch1.F1"/>. The fuel bed is located in the center of
the burn chamber, which during burns was pressurized to push smoke out the
ceiling through a 1.6 m diameter stack past a sampling platform 17 m above
the fuel bed. The flow through the stack was well mixed, with a residence
time of roughly 5 s. All three instruments had sampling ports on the
platform, though the PTR-ToF was not mounted on the platform
itself.</p>
      <p id="d1e685">A total of 33 different fuels were used, including numerous burns of
coniferous fuels and chaparral species. For the conifers, burns were
conducted either using only one component (e.g., litter, canopy) or with
realistic mixes of several components. A full list of fuels in given in the
Table S1 in the Supplement and in <xref ref-type="bibr" rid="bib1.bibx56" id="text.28"/>.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p id="d1e694">Details of the measurements and instruments used in this work. All
three instruments can measure additional species not used in this analysis.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="150.799606pt"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="119.501575pt"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="85.358268pt"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Instrument</oasis:entry>
         <oasis:entry colname="col2">Measured species used in this analysis</oasis:entry>
         <oasis:entry colname="col3">Uncertainty</oasis:entry>
         <oasis:entry colname="col4">Reference</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">ACES</oasis:entry>
         <oasis:entry colname="col2">glyoxal, methylglyoxal</oasis:entry>
         <oasis:entry colname="col3">glyoxal: <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula> %, <?xmltex \hack{\hfill\break}?>methylglyoxal: <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> %/<inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">70</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>
         <oasis:entry colname="col4">
                      <xref ref-type="bibr" rid="bib1.bibx47" id="text.29"/>
                    </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">OP-FTIR</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M30" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M31" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, formaldehyde</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M33" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M35" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: <inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mo>∼</mml:mo></mml:mrow></mml:math></inline-formula>2 %,<?xmltex \hack{\hfill\break}?>formaldehyde: <inline-formula><mml:math id="M37" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>10 %</oasis:entry>
         <oasis:entry colname="col4">
                      <xref ref-type="bibr" rid="bib1.bibx61 bib1.bibx56" id="text.30"/>
                    </oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PTR-ToF</oasis:entry>
         <oasis:entry colname="col2">formaldehyde, acetaldehyde, acetone, glycolaldehyde, methylglyoxal, hydroxyacetone, 2,3-butanedione, 2,3-pentanedione</oasis:entry>
         <oasis:entry colname="col3">formaldehyde, acetaldehyde,<?xmltex \hack{\hfill\break}?>acetone, glycolaldehyde: <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula> % <?xmltex \hack{\hfill\break}?>all others: <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> %</oasis:entry>
         <oasis:entry colname="col4"><xref ref-type="bibr" rid="bib1.bibx81" id="text.31"/>;<?xmltex \hack{\hfill\break}?> <xref ref-type="bibr" rid="bib1.bibx34" id="text.32"/></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2.SS2">
  <title>Instruments used</title>
      <p id="d1e928">All the instruments used here have been described previously, so only brief
descriptions will be provided. The species-specific uncertainties for each
instrument are given in Table <xref ref-type="table" rid="Ch1.T1"/>. Concentrations of all
species were significantly higher than the instrument detection limits, with
concentrations of glyoxal and formaldehyde during the fires ranging from 10
to either 600 (glyoxal) or 5000 ppbv (formaldehyde),<?pagebreak page15454?> and concentrations of
carbon monoxide at the peak of the fire exceeded 100 ppmv.</p>
<sec id="Ch1.S2.SS2.SSS1">
  <title>ACES</title>
      <p id="d1e938">Glyoxal and methylglyoxal were measured using the ACES instrument
<xref ref-type="bibr" rid="bib1.bibx47" id="paren.33"/>. Light from an LED with a center wavelength of 455 nm was
introduced into a 45 cm long cavity capped with highly reflective
(<inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mi>R</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.99995</mml:mn></mml:mrow></mml:math></inline-formula> at 455 nm) mirrors, enabling the light to make multiple passes and resulting
in an effective pathlength of 10–12 km. The light exiting the cavity entered
a grating spectrometer and was imaged onto a charge-coupled device (CCD)
array. The overlap between the mirror reflectivity and the LED output
resulted in a useful spectral range between 438 and 468 nm. The measured CCD
counts were then converted into extinction (the sum of scattering and
absorption) <xref ref-type="bibr" rid="bib1.bibx73" id="paren.34"/>. The wavelength-dependent extinction,
<inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, is due to absorption and Rayleigh scattering by gas-phase
molecules and scattering and absorption by aerosol particles. The particles
were removed with a filter (see below), and Rayleigh scattering was accounted
for by measuring the number density in the cell. The measured extinction is
then
              <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M42" display="block"><mml:mrow><mml:mi mathvariant="italic">α</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:msub><mml:mo>)</mml:mo><mml:mi mathvariant="normal">measured</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:msub><mml:mo>)</mml:mo><mml:mi>i</mml:mi></mml:msub><mml:msub><mml:mi>N</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">λ</mml:mi><mml:msub><mml:mo>)</mml:mo><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are respectively the absorption cross
section and number density of a given species. The measured spectra were fit
using the DOAS fitting routines in the DOASIS software package
<xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx52" id="paren.35"/>, which took as inputs the absorption cross
sections of the species of interest convolved to the resolution of the
instrument (here, nitrogen dioxide (<inline-formula><mml:math id="M45" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), glyoxal, and
methylglyoxal). For each spectrum, DOASIS then determined the number density
for each species that resulted in the best agreement between the measured and
calculated spectrum. Data for ACES are reported at 1 Hz.</p>
      <p id="d1e1066">ACES has a second channel centered at 375 nm measuring nitrous acid (HONO)
and <inline-formula><mml:math id="M46" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> that is imaged onto the CCD using the same spectrometer.
Imaging two channels separated by 80 nm with the same spectrometer requires a
relatively coarse grating, resulting in a resolution for both channels of
<inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> nm full width half maximum (FWHM). Even at this resolution, the
glyoxal cross section in the ACES retrieval window is highly structured and
distinct from the cross sections of other molecules absorbing in the same
region such as <inline-formula><mml:math id="M48" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and methylglyoxal. This method therefore
provides a robust and direct measurement of glyoxal with a minimal need for
corrections. The methylglyoxal cross section is less structured than the
glyoxal cross section, and at our resolution suffers from spectral
interferences from other substituted <inline-formula><mml:math id="M49" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-dicarbonyls such as
2,3-butanedione and 2,3-pentanedione, which have cross sections with similar
structure but lower intensity.</p>
      <p id="d1e1108">ACES was installed on the platform (see Fig. <xref ref-type="fig" rid="Ch1.F1"/>) and
sampled from the stack using a 0.4 cm (5/32 in.) inner diameter, 1 m long
fluorinated ethylene propylene (FEP) line that extended approximately 30 cm into the stack. Two polytetrafluoroethylene (PTFE) filters (1 <inline-formula><mml:math id="M50" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m pore
size) were mounted in series to remove aerosol particles and were changed
after every burn. The sampling line contained a restriction consisting of a
short section of 0.16 cm (1/16 in.) inner diameter tubing installed in between
the stack and the filters that lowered the pressure from <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">900</mml:mn></mml:mrow></mml:math></inline-formula> to
<inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">600</mml:mn></mml:mrow></mml:math></inline-formula> hPa in order to reduce the relative humidity. The residence time in
the sampling line was less than 1 s. Additionally, a glyoxal source
consisting of a bubbler containing a 40 wt % solution of glyoxal in water was
used to periodically add glyoxal to the instrument above both the restriction
and the filters to determine any potential losses of glyoxal on the filters.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <title>OP-FTIR</title>
      <p id="d1e1146">The OP-FTIR measured carbon monoxide (<inline-formula><mml:math id="M53" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>), carbon dioxide
(<inline-formula><mml:math id="M54" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), methane (<inline-formula><mml:math id="M55" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), and formaldehyde (<inline-formula><mml:math id="M56" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">HCHO</mml:mi></mml:mrow></mml:math></inline-formula>), as
well as a variety of other species <xref ref-type="bibr" rid="bib1.bibx61 bib1.bibx56" id="paren.36"/>. The
OP-FTIR was mounted on the platform and measured across the diameter of the
stack, with a time resolution of <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.73</mml:mn></mml:mrow></mml:math></inline-formula> Hz. Reference spectra were taken
from both the High-resolution Transmission (HITRAN) spectral database and
spectra previously recorded at Pacific Northwest National Laboratory (PNNL).
The<?pagebreak page15455?> collected IR spectra were then fit using the reference spectra to
determine the mixing ratios of the various species <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx25" id="paren.37"/>.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <title>PTR-ToF</title>
      <p id="d1e1210">The PTR-ToF was used to measure VOCs with a proton affinity greater than that
of water, including formaldehyde, 2,3-butanedione, 2,3-pentanedione, and
several other carbonyl species, with a time resolution of 1 Hz
<xref ref-type="bibr" rid="bib1.bibx81 bib1.bibx34" id="paren.38"/>. For some species, such as
formaldehyde and acetaldehyde, calibration factors were determined via the
addition of standards, but for other compounds such as 2,3-butanedione the
calibration factors were calculated using the method of <xref ref-type="bibr" rid="bib1.bibx54" id="text.39"/>.
PTR instruments generally cannot detect glyoxal since the majority of the
glyoxal molecules fragment following protonation to make formaldehyde
<xref ref-type="bibr" rid="bib1.bibx65" id="paren.40"/>, but glyoxal concentrations at the FSL were high enough
for the PTR-ToF to observe some glyoxal, although the agreement with ACES was
poor <xref ref-type="bibr" rid="bib1.bibx34" id="paren.41"/>. Additionally, the detection of methylglyoxal
by PTR suffers from an interference from propenoic (acrylic) acid, which has
the same formula (<inline-formula><mml:math id="M58" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">C</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and therefore the same exact mass
as methylglyoxal, but does not absorb in the visible. Glycolaldehyde has a
similar interference from acetic acid, while 2,3-pentanedione has an
interference from methyl methacrylate. The other carbonyls discussed in this
work (e.g., 2,3-butanedione) generally are not affected by species with the
same masses. While the PTR-ToF had an inlet on the platform, the instrument
itself was not mounted on the platform and instead sampled through a 16 m heated transfer line with a residence time of roughly 1 s. Data from the
OP-FTIR and ACES are available for all 75 stack burns, but due to different
sampling strategies PTR-ToF data are only available for 58 burns.</p>
</sec>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Data analysis</title>
      <p id="d1e1253">Fire-integrated emission ratios relative to <inline-formula><mml:math id="M59" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> (ERs, ppbv glyoxal or
methylglyoxal per ppmv <inline-formula><mml:math id="M60" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>) were calculated using
            <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M61" display="block"><mml:mrow><mml:mi mathvariant="normal">ER</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>X</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">start</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">stop</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">fire</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mi mathvariant="normal">bkgd</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">start</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">stop</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:mo>(</mml:mo><mml:msub><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow><mml:mi mathvariant="normal">fire</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow><mml:mi mathvariant="normal">bkgd</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>X</mml:mi></mml:mrow></mml:math></inline-formula> are the background-corrected,
fire-integrated mixing ratios of <inline-formula><mml:math id="M64" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> and the species of interest, <inline-formula><mml:math id="M65" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>.
Fire-integrated emission factors (EFs, grams of compound <inline-formula><mml:math id="M66" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula> emitted per kilogram of
fuel burned on a dry mass basis) were calculated using the carbon mass
balance method by the following equation:
            <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M67" display="block"><mml:mrow><mml:mi mathvariant="normal">EF</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1000</mml:mn><mml:mo>×</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="normal">MM</mml:mi><mml:mi>X</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="normal">AM</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>×</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>X</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:mrow></mml:mfrac></mml:mstyle><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NC</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">C</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the mass fraction of carbon in the fuel, MM<inline-formula><mml:math id="M69" display="inline"><mml:msub><mml:mi/><mml:mi>X</mml:mi></mml:msub></mml:math></inline-formula> is the
molecular mass of species <inline-formula><mml:math id="M70" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>, AM<inline-formula><mml:math id="M71" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">C</mml:mi></mml:msub></mml:math></inline-formula> is the atomic mass of carbon, <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>X</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> is the emission ratio relative to <inline-formula><mml:math id="M73" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> for species
<inline-formula><mml:math id="M74" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>, NC<inline-formula><mml:math id="M75" display="inline"><mml:msub><mml:mi/><mml:mi>i</mml:mi></mml:msub></mml:math></inline-formula> is the number of carbon atoms in a given species <inline-formula><mml:math id="M76" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, and <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:mrow></mml:math></inline-formula> is the emission ratio relative to <inline-formula><mml:math id="M78" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> for that
species. For the 58 burns where the PTR-ToF was sampling from the stack, the
total carbon mass was calculated using either only OP-FTIR data or by
combining the data from both the OP-FTIR and the PTR-ToF. The addition of the
VOCs measured by the PTR-ToF decreased the glyoxal emission factors by only
3 % on average. This is consistent with previous results from the FSL
<xref ref-type="bibr" rid="bib1.bibx62" id="paren.42"/> and with past field studies <xref ref-type="bibr" rid="bib1.bibx7 bib1.bibx44 bib1.bibx2" id="paren.43"><named-content content-type="pre">e.g.,</named-content></xref>, which have found that <inline-formula><mml:math id="M79" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M80" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>,
and methane generally make up at least 95 % of the total emitted carbon mass.
We report EFs based on the combined datasets when PTR-ToF data were available
and just OP-FTIR data when PTR-ToF data were not available.</p>
      <p id="d1e1655">The glyoxal to formaldehyde ratio (<inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, moles of glyoxal per
moles of formaldehyde) was calculated using
            <disp-formula id="Ch1.E4" content-type="numbered"><mml:math id="M82" display="block"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">Glyoxal</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">Formaldehyde</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">Glyoxal</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="normal">Formaldehyde</mml:mi></mml:mrow></mml:math></inline-formula> are the
background-corrected, fire-integrated concentrations of those two species.
<inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was calculated using formaldehyde from either the PTR-ToF and
the OP-FTIR, but since the two instruments generally agreed well and since
the OP-FTIR sampled more burns than the PTR-ToF, unless otherwise stated, all
<inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values discussed in the text used OP-FTIR formaldehyde data.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><caption><p id="d1e1741">Data from a filter transmission experiment conducted in Boulder,
Colorado,
prior to the FIREX campaign. Shown are the retrieved glyoxal (green) and
<inline-formula><mml:math id="M87" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (blue) concentrations from the three fire periods (orange
shading) and the additions using the bubbler (green shading). The filter was
not changed during the experiment.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f02.pdf"/>

        </fig>

      <?pagebreak page15456?><p id="d1e1761">The modified combustion efficiency, MCE, was calculated using
            <disp-formula id="Ch1.E5" content-type="numbered"><mml:math id="M88" display="block"><mml:mrow><mml:mi mathvariant="normal">MCE</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          MCE values can be calculated either as a fire-integrated value, where the
integrals of <inline-formula><mml:math id="M89" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M90" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> over the course of the fire are used
in Eq. (<xref ref-type="disp-formula" rid="Ch1.E5"/>), or as an instantaneous value. Unless otherwise
noted, all MCE values here are fire integrated. A higher MCE indicates a
greater proportion of flaming during the fire, with a value of 0.9 indicating
that the fire was roughly half flaming and half smoldering <xref ref-type="bibr" rid="bib1.bibx2" id="paren.44"/>.
Fuel moisture content, defined as
            <disp-formula id="Ch1.E6" content-type="numbered"><mml:math id="M91" display="block"><mml:mrow><mml:mi mathvariant="normal">moisture</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">content</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">wet</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">weight</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">dry</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">weight</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">dry</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="normal">weight</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>
          and fuel elemental composition were also measured for all 75 burns. Moisture
contents are given in the Supplement (Table S1), and elemental compositions
can be found in <xref ref-type="bibr" rid="bib1.bibx56" id="text.45"/>.<?xmltex \hack{\newpage}?></p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <title>Carbonyl filter transmission</title>
      <p id="d1e1882">Previous work has shown that glyoxal loss to filters and any aerosol
particles collected on the filters is low <xref ref-type="bibr" rid="bib1.bibx66 bib1.bibx74" id="paren.46"/>. Glyoxal uptake onto aerosol particles is driven by liquid
water content <xref ref-type="bibr" rid="bib1.bibx37 bib1.bibx71 bib1.bibx50" id="paren.47"/>. Biomass burning
particles generally are not very hygroscopic <xref ref-type="bibr" rid="bib1.bibx79 bib1.bibx2 bib1.bibx36" id="paren.48"/>, and during the 2016 campaign, the ambient relative humidity
in the burn chamber was low (25 %–40 %). Additionally, the inlet restriction
before the filter further reduced the relative humidity. Flow through the
filter holder was fast (10 L min<inline-formula><mml:math id="M92" 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>) to keep the residence time
(<inline-formula><mml:math id="M93" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula>0.3 s) to a minimum. However, the aerosol loadings during these
experiments were high and resulted in large accumulations of mass on the
filters, even for short burns. A fresh filter was used for each burn, but it
is possible that the buildup of material on the filters caused losses of
glyoxal and methylglyoxal.</p>
      <p id="d1e1913">Prior to the deployment to the FSL, filter transmission tests were conducted
in Boulder, Colorado, by burning dried pine needles and branches in a small wood-burning stove and then adding glyoxal to the inlet using the bubbler. The
data from one of these tests are shown in Fig. <xref ref-type="fig" rid="Ch1.F2"/>. The filter was not changed during this
experiment, and glyoxal was added before and after each fire to assess
potential losses. No glyoxal losses to the filter were observed during these
tests.</p>
      <p id="d1e1918">Unfortunately, during the FIREX campaign, the bubbler output frequently was
unstable, even over short (20 min) timescales. During times when the bubbler
was reasonably stable, the maximum observed loss was only 10 %, but the
instabilities in the bubbler output made it difficult to fully constrain this
number. Since we did not observe losses during the tests prior to FIREX and
given the uncertainty in the transmission measurements made during FIREX, we
have not corrected our data for filter loss, and note that our glyoxal
emissions might be up to 10 % low. Methylglyoxal is even less reactive than
glyoxal with respect to aerosol uptake <xref ref-type="bibr" rid="bib1.bibx37" id="paren.49"/>, so any loss of
methylglyoxal to the filters should be smaller.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Glyoxal emissions</title>
<sec id="Ch1.S3.SS2.SSS1">
  <title>Glyoxal emission ratios and factors</title>
      <p id="d1e1935">Glyoxal emission ratios and factors for all 75 burns are shown graphically in
Fig. <xref ref-type="fig" rid="Ch1.F3"/>a and b, and values can be found
in Table S2 in the Supplement. Burns from the 33 fuel types have been grouped into
eight general categories: chaparrals; realistic coniferous mixes; separate
canopy, litter, duff, and rotten logs from coniferous ecosystems; artificial;
and other. Duff is organic material that is denser than litter and has
undergone more decomposition. The artificial fuels were untreated lumber and
excelsior (wood wool), fuels that are unlikely to be major components of
biomass burning. We use the term “artificial” in the sense that these fuels
have been processed to some degree, and the biomass is not in its natural
state. The “other” category consists of fuels that do not fall into one of
the previous seven categories, and it includes several important fuels such as
peat, rice straw, and yak dung. Bar graphs of the average emission ratios and
factors for the first five groups and select other fuels are shown in
Fig. S1 in the Supplement.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p id="d1e1942"><bold>(a)</bold> Glyoxal emission ratios in units of ppbv glyoxal (ppmv <inline-formula><mml:math id="M94" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>)<inline-formula><mml:math id="M95" 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>
for the different fuel types. The number in the label denotes the number of
replicate burns for a given fuel type, while each marker represents the value
for an individual fire. <bold>(b)</bold> Glyoxal emission factors in units of g glyoxal (kg fuel)<inline-formula><mml:math id="M96" 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>. <bold>(c)</bold> The glyoxal to formaldehyde ratio, <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, calculated
using formaldehyde data from the OP-FTIR. For the first five groups, the
average and standard deviation of all the burns in that group are shown. For
the last three groups, averages are not provided due to the small number of
samples and because the fuels in “other” are unrelated.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f03.pdf"/>

          </fig>

      <p id="d1e2003">Glyoxal emission ratios for realistic mix burns averaged <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.71</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.22</mml:mn></mml:mrow></mml:math></inline-formula> ppbv glyoxal (ppmv <inline-formula><mml:math id="M99" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>)<inline-formula><mml:math id="M100" 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>, nearly a factor of 4 lower than the emission ratio
used in the global glyoxal budget by <xref ref-type="bibr" rid="bib1.bibx21" id="text.50"/>. The other categories
have similarly<?pagebreak page15457?> low average emission ratios, and the highest emission ratio,
3.67 ppbv glyoxal (ppmv <inline-formula><mml:math id="M101" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>)<inline-formula><mml:math id="M102" 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> from burning rice straw, was 40 % lower than the
value from <xref ref-type="bibr" rid="bib1.bibx21" id="text.51"/>. However, the emission ratios measured here are
consistent with the glyoxal enhancements from aircraft intercepts of fresh
(<inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> h old) biomass burning plumes, which averaged <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula> ppbv glyoxal (ppmv <inline-formula><mml:math id="M105" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula>)<inline-formula><mml:math id="M106" 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> <xref ref-type="bibr" rid="bib1.bibx82" id="paren.52"/>. Glyoxal emission factors from
other laboratory experiments have been reported by <xref ref-type="bibr" rid="bib1.bibx43" id="text.53"/> and
<xref ref-type="bibr" rid="bib1.bibx27" id="text.54"/>, but only two of the fuels used in those studies, ponderosa
pine and loblolly pine, overlapped with fuels used here. <xref ref-type="bibr" rid="bib1.bibx27" id="text.55"/>
burned fresh ponderosa pine needles and reported emission factors 5 times
higher than our fresh ponderosa pine canopy emission factor.
<xref ref-type="bibr" rid="bib1.bibx43" id="text.56"/> averaged emissions from both ponderosa and pinion pine
burns and report a value that is roughly a factor of 2 higher than ours.
Emission factors from burning dry loblolly pine needles were reported by
<xref ref-type="bibr" rid="bib1.bibx27" id="text.57"/> and are over 12 times higher than the emission factor for
our loblolly pine needle litter burns.</p>
      <p id="d1e2126">These discrepancies in emission factors between the two laboratory studies
and the burns conducted at the FSL could be due to systematic differences in
the MCE between the two studies <xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx78 bib1.bibx80 bib1.bibx61" id="paren.58"/>. However, due to differences in the ratio of
glyoxal to other carbonyls such as formaldehyde (see Sect. <xref ref-type="sec" rid="Ch1.S3.SS2.SSS2"/>), a more
likely explanation is that the method used by the two previous laboratory
studies for detecting carbonyls suffers from interferences. In those studies,
carbonyls were detected through derivatization followed by separation using
high-performance liquid chromatography and detection by ultraviolet
absorption measurements. It is now known that measurements of formaldehyde
using this method have interferences from unrelated species such as
<inline-formula><mml:math id="M107" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> that react with the derivatizing agent to form products with
similar retention times and absorbances <xref ref-type="bibr" rid="bib1.bibx33" id="paren.59"/>. ACES also measures
<inline-formula><mml:math id="M108" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and the <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations were comparable to those
of formaldehyde for many burns. The species that could cause interferences
for glyoxal are not known, but given the complexity of fire emissions and the
lack of<?pagebreak page15458?> specificity for the derivatization technique, glyoxal measurement
from fires using that technique should be treated with caution. More recent
work detects the derivatized product using electrospray ionization coupled to
tandem mass spectrometry <xref ref-type="bibr" rid="bib1.bibx32" id="paren.60"><named-content content-type="pre">e.g.,</named-content></xref>, which should provide a
greater degree of specificity. The optical method used here relies on the
unique differential structure in the visible absorption cross section of
glyoxal, reducing the potential for interferences.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p id="d1e2179">Glyoxal emission factors <bold>(a, b)</bold> and <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values
<bold>(c, d)</bold>
for each fire as a function of either MCE <bold>(a, c)</bold> or fuel moisture content
<bold>(b, d)</bold>.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f04.pdf"/>

          </fig>

      <p id="d1e2211">Examining emissions from individual fuels, peat had the lowest emission ratio
by a factor of 5, while rice straw and bear grass had the highest, consistent
with past results for emissions of larger oxygenated aliphatic compounds
<xref ref-type="bibr" rid="bib1.bibx26" id="paren.61"/>. For the conifer-derived fuels, the duff burns had the
lowest emission ratios, while the canopy and realistic mix burns were the
highest. Emission ratios depended more on the fuel component (e.g., canopy or
duff) than on the dominant tree species and generally were consistent within
each fuel component group. Chaparral emission ratios were low and in between
the duff and litter emission ratios. For the emission factors (grams of
glyoxal emitted per kilogram of fuel burned), peat again had the lowest value,
followed by the chaparrals. Duff and litter were again lower than the canopy
and realistic mix burns, but the emission factors for these four groups were
much closer than the emission ratios. Fuel component again mattered more than
species, but there was more variability in the emission factors than in the
emission ratios, especially for the canopy burns.</p>
      <p id="d1e2217">We examined the relationship between EF and either MCE or fuel moisture
content to see if this could explain the variability in the observed EFs.
Emission factors as a function of MCE and moisture content are shown in
Fig. <xref ref-type="fig" rid="Ch1.F4"/>a and b. Generally, burns
with higher MCEs had lower glyoxal emissions. This is unsurprising, as a
higher MCE means that a greater fraction of the carbon in the fuel was
converted to <inline-formula><mml:math id="M111" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Duff and peat did not follow this trend and,
despite having MCEs below 0.9, generally had low glyoxal emission factors.
Both duff and peat have undergone some amount of decomposition, and for the
duff burns this results in a unique VOC emission profile
<xref ref-type="bibr" rid="bib1.bibx55" id="paren.62"/>, so it is not surprising that these two fuels behave
differently. However, of the other four main groups (chaparrals, realistic
mixes, canopy, and litter), only the canopy burns covered a wide range of MCE
values, and those burns drive most of the observed trend in emission factors.
There appears to be a higher correlation between the fuel moisture content
and the glyoxal emission factor, with the wetter fuels having higher glyoxal
emissions. Peat is again an outlier, with low emissions despite a high
moisture content. However, the canopy burns again were the only group with a
large range of moisture content values. Additionally, moisture content and
MCE generally were inversely correlated, making it difficult to determine
which parameter had the greater effect on emission factor.</p>
      <p id="d1e2236">Within certain fuel groups, some of the variability in the emission factors
did appear to be driven by differences in the moisture content and MCE. The
canopy burns of Engelmann spruce and subalpine fir with the highest emission
factors also had moisture contents higher and MCE values lower than the other
burns of that material. For most of the other fuel groups, the moisture
content within the group did not vary significantly, making it difficult to
fully constrain the relationship between glyoxal emissions and moisture
content. Additionally, for some of the burns, there was significant
variability in the emission factors despite similar conditions. For example,
the two ponderosa pine litter burns were both dry (moisture contents of 0.11
and 0.07) and had similar MCEs, but the emission factors differed by a factor
of 3. While moisture content and MCE can affect emissions, clearly there are
other factors that also play a role.</p>
      <p id="d1e2239">Multiple burns of chaparral and coniferous fuels were conducted in 2016,
allowing for some investigation of the variability in emissions for those
fuels. However, there were several important fuels that were only burned
once, such as peat and rice straw. During El Niño years, peat fires can
emit almost as much non-methane organic carbon as all other biomass burning
combined and can negatively impact local-regional air quality
<xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx64" id="paren.63"/>. Crop residue burning is also
significant on a<?pagebreak page15459?> global scale and can strongly impact local-regional air
quality, and crop residue may be used as biofuel <xref ref-type="bibr" rid="bib1.bibx77 bib1.bibx2 bib1.bibx60" id="paren.64"/>. Since only one burn each of peat and rice straw
were conducted in 2016, it is difficult to assess the effect of fire to fire
variability and fuel differences (e.g., peat from different regions) on the
glyoxal emission factors. However, while glyoxal emissions have rarely been
measured, emissions of other small carbonyls from peat and various crop
residues have been measured in laboratory studies, such as the fourth Fire
Lab at Missoula Experiment (FLAME-4) conducted at the FSL in 2012
<xref ref-type="bibr" rid="bib1.bibx62" id="paren.65"/>, and field projects, such as 2015 Nepal Ambient
Monitoring and Source Testing Experiment (NAMaSTE)
<xref ref-type="bibr" rid="bib1.bibx63" id="paren.66"/> and a 2015 study conducted in the fall of 2015 in
Indonesia <xref ref-type="bibr" rid="bib1.bibx64" id="paren.67"/>. These studies measured carbonyls such
as formaldehyde and glycolaldehyde using the same techniques and sometimes
the same instruments as the 2016 study, and emission factors from previous
work for the small carbonyls were within a factor of 2 of the emission
factors measured in 2016 <xref ref-type="bibr" rid="bib1.bibx34 bib1.bibx56" id="paren.68"/>. Since
emissions of glyoxal are generally very well correlated with the emissions of
these other small carbonyls (see Sect. <xref ref-type="sec" rid="Ch1.S3.SS2.SSS3"/>), particularly
formaldehyde, the good agreement with the previous work gives us confidence
that our results from single burns of peat and rice straw are broadly
representative of emissions from those fuels.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <?xmltex \opttitle{Glyoxal to formaldehyde ratio, $R_{{\mathrm{GF}}}$
}?><title>Glyoxal to formaldehyde ratio, <inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
</title>
      <p id="d1e2281">Glyoxal to formaldehyde ratios, <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, for all the burns using
OP-FTIR formaldehyde are shown in Fig. <xref ref-type="fig" rid="Ch1.F3"/>c, and bar graphs of <inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for certain
fuels are shown in Fig. S2 in the Supplement. <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values for each
fire using either OP-FTIR or PTR-ToF data are available in Table S2 in the Supplement. Formaldehyde measurements from the two instruments agreed to within 10 %
(campaign average) <xref ref-type="bibr" rid="bib1.bibx34" id="paren.69"/>, and <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> generally
was not significantly affected by the choice of instrument. The main
exceptions were several of the litter burns and the rice straw burn, where
<inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> calculated with OP-FTIR data was higher than <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
from PTR-ToF data (e.g., for the rice straw burn <inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> calculated
using OP-FTIR data is 0.11, compared to an <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of 0.08 when using
PTR-ToF data). <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> across all fuels averaged <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.068</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.018</mml:mn></mml:mrow></mml:math></inline-formula> when
using OP-FTIR formaldehyde and <inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.060</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.025</mml:mn></mml:mrow></mml:math></inline-formula> when using formaldehyde from
the PTR-ToF.</p>
      <p id="d1e2414">These values are at least an order of magnitude lower than those reported
from previous laboratory burns <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx27" id="paren.70"/>, but they are
comparable to column measurements by satellites of <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
(0.05–0.08) over regions dominated by biomass burning <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx60" id="paren.71"/>. <xref ref-type="bibr" rid="bib1.bibx82" id="text.72"/> measured <inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in nighttime
plumes that were roughly several hours old and in daytime plumes less than
an hour old. While <inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values in the fresh daytime plumes were
comparable to those measured at the FSL (0.06–0.11), <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values
in the nighttime plumes were roughly 40 % lower (0.009–0.04). With the
exception of one daytime plume that mostly likely came from burning sugarcane
fields, the fuels being burned were not known, so whether the lower nighttime
<inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values observed by <xref ref-type="bibr" rid="bib1.bibx82" id="text.73"/> were due to different
chemistry in the fire plumes or different fuel types cannot be determined at
this time.</p>
      <p id="d1e2485">Unlike the glyoxal emission ratios and factors, <inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was
consistent across many of the burns, even for unrelated fuels such as
chaparral and conifers that had distinct glyoxal emission ratios and factors.
The main exceptions were the fuels that had undergone some form of
decomposition, such as duff and peat, which have <inline-formula><mml:math id="M130" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values 2 to
4 times lower than the others. Given the uniqueness of the duff VOC profiles
<xref ref-type="bibr" rid="bib1.bibx55" id="paren.74"/>, the different <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for these fuels is not
surprising.</p>
      <p id="d1e2524">Unlike the emission ratios and factors, <inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> showed little
dependence on moisture content and MCE (Fig. <xref ref-type="fig" rid="Ch1.F4"/>c–d). Figure <xref ref-type="fig" rid="Ch1.F4"/>c
has an apparent positive correlation between <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and MCE, but
this is driven entirely by the low <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and MCE values from the
duff and peat burns. For the other burns, <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> showed little
dependence on MCE. The only conifer burns that were conducted at low (<inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.9</mml:mn></mml:mrow></mml:math></inline-formula>)
MCE were the duff burns, so it is hard to draw conclusions based on the fire-averaged MCE values (see below for discussion of instantaneous MCE values).
Duff and peat were outliers in the plot of <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> versus moisture
content, but in general no trend was observed between those two parameters.
In particular, the canopy burns had a wide range of moisture contents but
only a very narrow range of <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p id="d1e2611"><bold>(a)</bold> Glyoxal as a function of <inline-formula><mml:math id="M139" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> for Fire 016 (ponderosa pine
litter). <bold>(b)</bold> Glyoxal as a function of formaldehyde for the same burn. Glyoxal
as a function of <inline-formula><mml:math id="M140" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> <bold>(c)</bold> and formaldehyde <bold>(d)</bold> for Fire 073 (ponderosa
pine rotten log). The markers in all plots are colored by the instantaneous
MCE.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f05.pdf"/>

          </fig>

      <p id="d1e2647">In addition to fire-averaged <inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values, we examined the
correlation between glyoxal and formaldehyde emissions at each point in the
fire. For most of the fuels, glyoxal emissions were well correlated with
formaldehyde emissions in real time but were not well correlated with
real-time <inline-formula><mml:math id="M142" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> measurements. Additionally, there was not a consistent
and strong relation between glyoxal emissions and instantaneous MCE. This is
shown in Fig. <xref ref-type="fig" rid="Ch1.F5"/>. Figure <xref ref-type="fig" rid="Ch1.F5"/>a and b display glyoxal versus
<inline-formula><mml:math id="M143" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> and formaldehyde respectively for Fire 016, a ponderosa pine litter
burn. The markers are colored by the instantaneous MCE. Glyoxal and
formaldehyde are highly correlated (<inline-formula><mml:math id="M144" 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">0.94</mml:mn></mml:mrow></mml:math></inline-formula>), but the correlations with
either <inline-formula><mml:math id="M145" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> or MCE are poor (<inline-formula><mml:math id="M146" 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">0.3</mml:mn></mml:mrow></mml:math></inline-formula> for both). Instantaneous
<inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was constant over the entire burn, despite the changes in
instantaneous MCE. The other burn of ponderosa pine litter (Fire 038, not
shown) had a similar fire-integrated MCE and fuel moisture content, but it had a
glyoxal emission factor 3 times higher than the emission factor in Fire 016
(0.189 versus 0.063 g glyoxal (kg fuel burned)<inline-formula><mml:math id="M148" 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 Fire 016,
additional fuel was added several times to increase the length of burn, while
no additional fuel was added for Fire 038. Despite the different glyoxal
emission factors and fire behavior, these fires had similar <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
values (0.080 for Fire 038 versus 0.062 for Fire 016).</p>
      <?pagebreak page15460?><p id="d1e2754">Figure <xref ref-type="fig" rid="Ch1.F5"/>c and d show the same plots, but for Fire 073, a ponderosa pine rotten
log. There are two distinct glyoxal to <inline-formula><mml:math id="M150" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> emission ratios, one
corresponding to the start of the burn when no flames were present, and the
second from the end of the burn when there were flames. For Fire 073, the
emission ratios during the non-flaming period at the start and the flaming
period at the end of the burn differed by a factor of 20, but despite this,
<inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was constant during the entire duration of the fire and
consistent with the ratio from other fuels (0.06 compared to the average of
<inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.068</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.018</mml:mn></mml:mrow></mml:math></inline-formula>). While for Fire 073 it does appear that there is a
correlation between instantaneous MCE and glyoxal emission ratio, with the
lower MCE corresponding to higher glyoxal emissions, this trend was not
observed for many other burns, such as Fire 016, where the highest MCE and
emission ratio both occurred at the start of the fire.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS3">
  <title>Correlations with other carbonyls
</title>
      <p id="d1e2796">In addition to formaldehyde, we compared emissions of glyoxal to several
other carbonyl species measured by the PTR-ToF: acetaldehyde, acetone,
2,3-butanedione, hydroxyacetone, and glycolaldehyde. The latter two of these
species are also measured by the OP-FTIR, but the PTR-ToF data were at the
same time resolution as the ACES data, so we chose to use those data here.
There is good overall agreement between the PTR-ToF and the OP-FTIR for these
species <xref ref-type="bibr" rid="bib1.bibx34" id="paren.75"/>, so the results using OP-FTIR data should be
similar.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p id="d1e2804">Correlation plots for glyoxal relative to four other carbonyls for
Fire 027 (chamise chaparral). Shown are the plots for glyoxal versus
formaldehyde <bold>(a)</bold>, acetaldehyde <bold>(b)</bold>, glycolaldehyde <bold>(c)</bold>, and 2,3-butanedione <bold>(d)</bold>. The markers are colored by instantaneous MCE. Correlation plots for
acetone and hydroxyacetone are similar to the plots for glycolaldehyde and
2,3-butanedione.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f06.pdf"/>

          </fig>

      <?pagebreak page15461?><p id="d1e2825">Formaldehyde had the best correlation, with an average <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of 0.91,
followed by acetaldehyde with an <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> of 0.85. For the other carbonyls,
<inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula> values were between 0.75 and 0.79. While glyoxal emissions were only
6 %–7 % of those of formaldehyde, this ratio was higher for the other
carbonyls, with glyoxal emissions being roughly 20 % of those of acetaldehyde
and approximately equal to emissions of 2,3-butanedione and hydroxyacetone.
Correlation plots of glyoxal versus four of the other carbonyls for Fire 027, a chamise chaparral fire, are shown in Fig. <xref ref-type="fig" rid="Ch1.F6"/>.
Glyoxal to formaldehyde plots for the other
fires are generally similar, with well correlated and linearly related
emissions for the two species. For acetaldehyde, while many fires resemble
Fire 027, in other fires the emissions of glyoxal and acetaldehyde are less
well correlated. The other four carbonyl species behave similarly to each
other, and the correlations generally decrease as the carbonyl size
increases.<?xmltex \hack{\newpage}?></p>
</sec>
</sec>
<sec id="Ch1.S3.SS3">
  <title>Methylglyoxal emissions</title>
<sec id="Ch1.S3.SS3.SSS1">
  <title>Spectral retrieval</title>
      <p id="d1e2876">While the <inline-formula><mml:math id="M156" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and glyoxal cross sections are highly structured, the
methylglyoxal cross section is not, particularly at the ACES instrument
resolution of 1 nm FWHM. This can be seen in Fig. <xref ref-type="fig" rid="Ch1.F7"/>a, which shows the absorption cross sections of
three of the main absorbers in the ACES retrieval window: <inline-formula><mml:math id="M157" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>;
glyoxal; and methylglyoxal. In addition to methylglyoxal, there are several
other substituted <inline-formula><mml:math id="M158" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-dicarbonyls such as 2,3-butanedione and
2,3-pentanedione that have absorption cross sections similar to that of
methylglyoxal, albeit with lower magnitudes. The 2,3-butanedione and
2,3-pentanedione cross sections are also shown in Fig. <xref ref-type="fig" rid="Ch1.F7"/>a, and the lack of structure in cross sections of
the three substituted <inline-formula><mml:math id="M159" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-dicarbonyls, especially compared to the
structure present in the <inline-formula><mml:math id="M160" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and glyoxal cross sections, can be
clearly seen.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p id="d1e2933"><bold>(a)</bold> Absorption cross sections for <inline-formula><mml:math id="M161" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
<xref ref-type="bibr" rid="bib1.bibx68" id="paren.76"/>, glyoxal <xref ref-type="bibr" rid="bib1.bibx70" id="paren.77"/>, methylglyoxal
<xref ref-type="bibr" rid="bib1.bibx45" id="paren.78"/>, 2,3-butanedione <xref ref-type="bibr" rid="bib1.bibx28" id="paren.79"/>, and
2,3-pentanedione <xref ref-type="bibr" rid="bib1.bibx46" id="paren.80"/> in the ACES fit window. <bold>(b)</bold> Absorption
cross sections of methylglyoxal, 2,3-butanedione, and 2,3-pentanedione (solid
lines), and the absorption cross section of 2,3-butanedione scaled by a
factor of 1.8 (dashed line) to better show the similarity in the shape of
that cross section with the methylglyoxal cross section. All the cross
sections shown are convolved to the instrument resolution of 1 nm (FWHM).</p></caption>
            <?xmltex \igopts{width=184.942913pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f07.pdf"/>

          </fig>

      <p id="d1e2974">Figure <xref ref-type="fig" rid="Ch1.F7"/>b shows the methylglyoxal, 2,3-butanedione,
and 2,3-pentanedione cross sections. While the methylglyoxal cross section
has several features between 440 and 450 nm that are not present in the other
two cross sections, these features are usually too small to be observed in
the measured spectra, except at high concentrations. The fit results from the
peak of emissions during Fire 060 (rice straw) are shown in Fig. <xref ref-type="fig" rid="Ch1.F8"/>, and at these methylglyoxal concentrations the
small features can be resolved, indicating that at least part of the signal
attributed to methylglyoxal is indeed from that molecule. However, previous
work has shown that the other substituted <inline-formula><mml:math id="M162" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-dicarbonyls are emitted
from biomass burning in amounts comparable to the methylglyoxal emissions we
measured at the FSL <xref ref-type="bibr" rid="bib1.bibx22 bib1.bibx62 bib1.bibx34" id="paren.81"/>,
and the contribution of these species to the measured extinction needs to be
taken into account to properly retrieve the methylglyoxal concentrations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p id="d1e2994">Fit results from the peak of emissions from Fire 060 (rice straw).
<bold>(a)</bold> The measured spectrum (blue), the fitted spectrum (red), and the residual
(green). Fits for <inline-formula><mml:math id="M163" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <bold>(b)</bold>, glyoxal <bold>(c)</bold>, and methylglyoxal <bold>(d)</bold>. At
these concentrations, the small features in the methylglyoxal cross section
can be resolved. The methylglyoxal concentration given in the figure is the
retrieved concentration, and has not been corrected for the interference from
2,3-butanedione.</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f08.pdf"/>

          </fig>

      <?pagebreak page15462?><p id="d1e3026">Other techniques for the measurement of methylglyoxal also suffer from
interferences. Methylglyoxal measurements by PTR-ToF are complicated by the
presence of an isomer, propenoic (acrylic) acid, which has been measured in
fire emissions at the FSL in 2009 using negative-ion proton-transfer
chemical-ionization mass spectrometry <xref ref-type="bibr" rid="bib1.bibx69" id="paren.82"/> and in 2016
using iodide chemical ionization mass spectrometry (<inline-formula><mml:math id="M164" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">I</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> CIMS)
<xref ref-type="bibr" rid="bib1.bibx34" id="paren.83"/>. For the 2016 campaign, the calibration factor for
propenoic acid on the <inline-formula><mml:math id="M165" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">I</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> CIMS was directly measured by additions of
propenoic acid using a liquid calibration unit, while the
methylglyoxal/propenoic acid calibration factor for the PTR-ToF was estimated
using the method of <xref ref-type="bibr" rid="bib1.bibx54" id="text.84"/>. The sum of methylglyoxal and
propenoic acid measured by the PTR-ToF was 30 % lower than propenoic acid
measured by the <inline-formula><mml:math id="M166" display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">I</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> CIMS and 50 % lower than the methylglyoxal
measured by ACES (even after applying the corrections to the ACES data
discussed below), indicating that the PTR-ToF is substantially
underestimating the sum of these compounds. However, a previous study used
PTR instruments and CES instruments similar to ACES to measure methylglyoxal
either directly injected into a chamber or formed in situ by VOC
oxidation, and  it found agreement within 25 % <xref ref-type="bibr" rid="bib1.bibx67" id="paren.85"/>.</p>
      <p id="d1e3075">Emissions at the FSL have also been analyzed using two-dimensional gas-chromatography time-of-flight mass spectrometry <xref ref-type="bibr" rid="bib1.bibx26" id="paren.86"/>.
Unfortunately, methylglyoxal is too sticky to elute on the GC column used for
light compounds and too light for the column used for polar compounds
(Lindsay Hatch, personal communication, 2017), so the relative contribution of
methylglyoxal and propenoic acid to the PTR-ToF signal at <inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula> 73.0284 cannot
be quantified at this time. However, it is clear that, at least in fresh
emissions, both compounds are present in appreciable amounts, and the signal
at that mass should be interpreted as the sum of both compounds.</p>
      <p id="d1e3093">ACES data from the FSL were analyzed in several ways to try to account for
the optical interference on the retrieved methylglyoxal concentrations. While
2,3-butanedione emissions are comparable to methylglyoxal emissions,
emissions of larger <inline-formula><mml:math id="M168" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-dicarbonyls such as 2,3-pentanedione are at
least an order of magnitude lower (based on the GC-PTR-ToF results, less than
a third of the signal at <inline-formula><mml:math id="M169" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula> 101.06, <inline-formula><mml:math id="M170" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">C</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">8</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msup><mml:mi mathvariant="normal">H</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>, is due to
2,3-pentanedione) <xref ref-type="bibr" rid="bib1.bibx62 bib1.bibx34" id="paren.87"/>, so the only
optical interference that we will consider is that from 2,3-butanedione.</p>
      <p id="d1e3144">In previous work, a third- or fourth-order polynomial was included in the fit
to account for drift in the instrument zero signal counts <xref ref-type="bibr" rid="bib1.bibx47" id="paren.88"/>,
but given the high peak signal at the FSL (several orders of magnitude
greater than ambient), any changes in the background were small relative to
the signal from gas phase absorbers. Due to the lack of structure in the
methylglyoxal cross section, the DOASIS fitting software tended to assign a
large portion of the signal to the polynomial, rather than to methylglyoxal.
The polynomial was therefore excluded from the fits. This did not change the
retrieved concentrations of the structured absorbers (glyoxal and
<inline-formula><mml:math id="M171" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), but it did increase the retrieved methylglyoxal concentrations
by roughly 30 %.</p>
      <p id="d1e3161">When running the DOASIS fits without accounting for the other substituted
<inline-formula><mml:math id="M172" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-dicarbonyls, the extinction attributed to methylglyoxal,
<inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, is the product of the methylglyoxal cross section,
<inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and the apparent methylglyoxal concentration, <inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:msubsup><mml:mi>N</mml:mi><mml:mi mathvariant="normal">MG</mml:mi><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>.
Since 2,3-butanedione is present, the extinction is rather
              <disp-formula id="Ch1.E7" content-type="numbered"><mml:math id="M176" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msubsup><mml:mi>N</mml:mi><mml:mi mathvariant="normal">MG</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">BD</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">BD</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">BD</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">BD</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the concentration and absorption cross
section of 2,3-butanedione respectively. There are two ways to account for
the interference from 2,3-butanedione: include 2,3-butanedione in the DOASIS
fits and attempt to simultaneously retrieve both methylglyoxal and
2,3-butanedione; or only include methylglyoxal in the DOASIS fit and correct
the retrieved methylglyoxal using the 2,3-butanedione concentrations measured
by the PTR-ToF:
              <disp-formula id="Ch1.E8" content-type="numbered"><mml:math id="M179" display="block"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>N</mml:mi><mml:mi mathvariant="normal">MG</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">BD</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">BD</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="normal">MG</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:msubsup><mml:mi>N</mml:mi><mml:mi mathvariant="normal">MG</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>-</mml:mo><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">BD</mml:mi></mml:msub><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">BD</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">MG</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mrow><mml:mi mathvariant="normal">BD</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">MG</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> is the average ratio of the two cross sections in the ACES
fit window (<inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.55</mml:mn></mml:mrow></mml:math></inline-formula>).</p>
      <p id="d1e3381">PTR-ToF data were only available for 58 burns, so all further discussion of
the methylglyoxal emissions will be limited to results from those fires. All
33 fuel groups are still represented in this subset of fires.</p>
      <p id="d1e3384">The DOASIS software in principle can simultaneously retrieve the absolute
amounts of methylglyoxal and 2,3-butanedione, but this is complicated by the
similarities in the two cross sections and their lack of structure,
particularly at the low resolution (<inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> nm FWHM) of the ACES instrument.
Including 2,3-butanedione in the DOASIS fits lowered the methylglyoxal
emission ratios by <inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:mn mathvariant="normal">41</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">17</mml:mn></mml:mrow></mml:math></inline-formula> %. However, there are many periods when there
were rapid fluctuations in the retrieved concentrations of the two species,
caused by the similarity between the two cross sections. Additionally, there
were numerous periods when either the retrieved methylglyoxal or
2,3-butanedione concentration was negative. These two behaviors do not give
us confidence that DOASIS is correctly dividing the measured extinction
between methylglyoxal and 2,3-butanedione. While we cannot rule out changes
in the ratio of emitted methylglyoxal to 2,3-butanedione as the cause of the
variability in the correction, at least part of the variability also appears
to be due to fit instabilities.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p id="d1e3411">Methylglyoxal emission ratios <bold>(a)</bold>, emission factors <bold>(b)</bold>, and the
molar ratio of methylglyoxal to glyoxal <bold>(c)</bold>. Note the split axes for the
emission ratio and methylglyoxal to glyoxal plots. Average values for the
first five fuel groups and values for certain individual fuels are also
shown.</p></caption>
            <?xmltex \igopts{width=497.923228pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/15451/2018/acp-18-15451-2018-f09.pdf"/>

          </fig>

      <p id="d1e3429">Using the 2,3-butanedione concentrations measured by the PTR-ToF to correct
the methylglyoxal data could be complicated by the presence of other species
at the same mass. However, during FIREX, the contribution of different
species to the signal at the 2,3-butanedione mass of <inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula> 87.0441 was well
characterized by putting a GC column in front of the PTR-ToF, allowing for
the separation and quantification of isomeric compounds. 2,3-butanedione
contributed 87 % of the signal, while methyl acrylate (5 %) and several
minor, unidentified compounds (8 %) made up the balance of the signal. These
fractions were consistent across the nine fires analyzed with this method
<xref ref-type="bibr" rid="bib1.bibx34" id="paren.89"/>. However, the calibration factor necessary to
convert the counts measured by the PTR-ToF into 2,3-butanedione
concentrations was not measured but rather calculated using the method of
<xref ref-type="bibr" rid="bib1.bibx54" id="text.90"/> and has an uncertainty of 50 %. This method is<?pagebreak page15463?> likely to
produce calibration factors that result in an underestimation of the
2,3-butanedione concentration, and thus using those concentrations to correct
the methylglyoxal will result in methylglyoxal emissions higher than the
actual values.</p>
      <p id="d1e3450">Using 2,3-butanedione from the PTR-ToF to correct the ACES methylglyoxal did
not result in undesirable and unphysical behavior and reduced the
methylglyoxal emission ratios by <inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:mn mathvariant="normal">17</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:math></inline-formula> % for the 57 non-peat burns and by
52 % for the peat burn (Fire 055), which was the only burn where
2,3-butanedione concentrations were comparable to methylglyoxal
concentrations. Due to the issues with simultaneously fitting two diffuse
cross sections in DOASIS, we have chosen to fit the ACES data using only the
methylglyoxal cross section (in addition to the <inline-formula><mml:math id="M186" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and glyoxal
cross sections) and then correct the apparent methylglyoxal concentrations
using Eq. <xref ref-type="disp-formula" rid="Ch1.E8"/> and 2,3-butanedione concentrations from the
PTR-ToF. Due to the uncertainties associated with the calibration factor for
2,3-butanedione, we increased the 2,3-butanedione reported by the PTR-ToF by
50 %, so the methylglyoxal emissions we report are likely lower than the true
values and have an estimated uncertainty of <inline-formula><mml:math id="M187" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">30</mml:mn></mml:mrow></mml:math></inline-formula> %/<inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">70</mml:mn></mml:mrow></mml:math></inline-formula> %. We note that there
is still considerable uncertainty in the methylglyoxal emissions, and
reducing this uncertainty will require instruments with greater specificity
and sensitivity for methylglyoxal.</p>
</sec>
<sec id="Ch1.S3.SS3.SSS2">
  <title>Methylglyoxal emission ratios and factors</title>
      <?pagebreak page15464?><p id="d1e3504">Shown in Fig. <xref ref-type="fig" rid="Ch1.F9"/> are emission ratios, emission
factors, and the molar ratio of emitted methylglyoxal to glyoxal. Bar graphs
of average values for certain fuel groups are also given in
Figs. S1 and S2 in the Supplement. Values for the 58 fires where PTR-ToF data were available
are given in Table S3 in the Supplement. The chaparral burns had some of the
lowest methylglyoxal emission factors and ratios, similar to the results for
glyoxal. However, litter and duff emitted considerable amounts of
methylglyoxal, with the duff burns emitting roughly 50 % more methylglyoxal
than the canopy and realistic mix burns. This is quite different from the
glyoxal results, where duff and litter emitted little glyoxal compared to the
canopy burns. As with glyoxal, peat had the lowest methylglyoxal emissions,
while rice straw had some of the highest.<?xmltex \hack{\newpage}?></p>
      <p id="d1e3510">Emissions of methylglyoxal from fresh ponderosa pine needles and dead
loblolly pine needles have been previously reported by <xref ref-type="bibr" rid="bib1.bibx27" id="text.91"/>.
While that study reported glyoxal emission factors several times higher than
ours, the methylglyoxal emission factors are at most only 30 % higher than
the ones reported here. Emissions for the signal at <inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>/</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula> 73.0284 have been
reported previously by <xref ref-type="bibr" rid="bib1.bibx62" id="text.92"/> and <xref ref-type="bibr" rid="bib1.bibx34" id="text.93"/>. As
noted above, the signal at this mass is due to a combination of methylglyoxal
and propenoic acid, with calculated, not measured, calibration factors, so
the comparisons between this work and those studies should be treated with
caution. Generally, the emission factors from <xref ref-type="bibr" rid="bib1.bibx62" id="text.94"/> for
chaparrals and ponderosa pine are comparable to ours, although we see higher
methylglyoxal emissions from rice straw. Our emission factors are higher than
those from <xref ref-type="bibr" rid="bib1.bibx34" id="text.95"/>, with better agreement for the conifers
(30 % difference) than for the chaparrals and rice straw (factor of 2).</p>
      <p id="d1e3541">For all the burns, molar emissions of methylglyoxal exceeded those of
glyoxal, generally by a factor of 2 and by a factor of 15 for the duff burns.
This is consistent with the limited field data, which also found
methylglyoxal emissions to be higher than glyoxal emissions
<xref ref-type="bibr" rid="bib1.bibx82" id="paren.96"/>, but is in contrast to the results of <xref ref-type="bibr" rid="bib1.bibx27" id="text.97"/>,
who reported glyoxal emissions that were twice as high as methylglyoxal
emissions. While the glyoxal and methylglyoxal budgets from <xref ref-type="bibr" rid="bib1.bibx21" id="text.98"/>
also predict that biomass burning emits more glyoxal than methylglyoxal, this
is due to the high glyoxal emissions used, as the methylglyoxal emissions
used in that study are comparable to those observed here.
<?xmltex \hack{\vspace{-3mm}}?></p>
</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Implications</title>
      <p id="d1e3562">Budgets for glyoxal and methylglyoxal predict that the largest global source
for both compounds is VOC oxidation <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx49 bib1.bibx58" id="paren.99"/>. However, on local scales emissions of glyoxal and
methylglyoxal from biomass burning are expected to dominate over other
sources, even with our lower glyoxal emission factors. For example, during
the Southeast Nexus (SENEX) campaign in the summer of 2013 in the
southeastern United States, the large regional emissions of isoprene resulted
in ambient glyoxal mixing ratios of roughly 100 pptv, 10 times lower than
what was measured in biomass burning plumes <xref ref-type="bibr" rid="bib1.bibx31 bib1.bibx82" id="paren.100"/>.</p>
      <p id="d1e3571">The effects of our revised emission factors on the global budgets for these
two compounds are harder to quantify. <xref ref-type="bibr" rid="bib1.bibx60" id="text.101"/> analyzed
emissions from crop residue fires (mainly wheat and maize) in the North China
Plain measured by the OMI instrument and were able to model formaldehyde and
<inline-formula><mml:math id="M190" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> columns using literature emission factors for those compounds.
The glyoxal column measurements were also compared to the model, and the
observed column enhancements were best reproduced using a glyoxal emission
factor of 1.12 g glyoxal (kg fuel)<inline-formula><mml:math id="M191" 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>, over a factor of 3 higher than our rice
straw emission factor (0.34 g glyoxal (kg fuel)<inline-formula><mml:math id="M192" 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>). Several studies have examined
the impact of post-harvest practices on crop-burning emission factors and
found that when the crop residue is piled (mostly commonly in Asia), the fuel
tends to smolder for long periods, resulting in lower MCEs and emission
factors at the lowest MCEs 2–3 times higher than those at the
highest MCE <xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx29 bib1.bibx38" id="paren.102"/>. Our rice straw burn
was an open burn, where the fuel was not piled, and had a high MCE
(<inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula>), so crop residue burns where the fuel is wetter and piled may
have higher emission factors. However, aircraft intercepts of fresh biomass
burning plumes that likely originated from crop residue fires in the
southeastern United States have found glyoxal enhancements relative to
<inline-formula><mml:math id="M194" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> similar to those observed at the FSL <xref ref-type="bibr" rid="bib1.bibx82" id="paren.103"/>, in
accordance with the tendency not to pile residues for burning in developed
countries <xref ref-type="bibr" rid="bib1.bibx2" id="paren.104"/>.</p>
      <p id="d1e3640"><xref ref-type="bibr" rid="bib1.bibx60" id="text.105"/> speculated that some of the glyoxal observed from the
satellites could be due to secondary production in the biomass burning
plumes. Many of the plumes studied by <xref ref-type="bibr" rid="bib1.bibx82" id="text.106"/> were emitted at
dusk, and two of the daytime plumes were less than an hour old, limiting any
secondary photochemistry leading to glyoxal production in those plumes. While
to date there have been no measurements of glyoxal production (or loss) in
aged fire plumes, in numerous studies, formaldehyde has been observed to
increase relative to <inline-formula><mml:math id="M195" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow></mml:math></inline-formula> downwind of fires <xref ref-type="bibr" rid="bib1.bibx79 bib1.bibx3 bib1.bibx4 bib1.bibx48" id="paren.107"/>. Our measurements of the glyoxal to
formaldehyde ratio for fresh emissions are similar to the ratio of total
column glyoxal to formaldehyde retrieved by satellites <xref ref-type="bibr" rid="bib1.bibx12 bib1.bibx60" id="paren.108"/>, but they are higher than those observed by <xref ref-type="bibr" rid="bib1.bibx82" id="text.109"/>.
Glyoxal and formaldehyde have similar lifetimes with respect to photolysis
<xref ref-type="bibr" rid="bib1.bibx70 bib1.bibx53" id="paren.110"/> and oxidation by OH <xref ref-type="bibr" rid="bib1.bibx18 bib1.bibx10" id="paren.111"/>, and if formaldehyde is increasing downwind of fires, then glyoxal
must also be increasing if <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> remains roughly constant.
<xref ref-type="bibr" rid="bib1.bibx82" id="text.112"/> observed <inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values 40 % lower than the ones
we observed at the FSL, so it is possible that the timing of the increases in
these two compounds is different. Unfortunately, there have been no
measurements of changes in glyoxal as a fire plume ages, and these
measurements are crucial to constraining secondary glyoxal chemistry downwind
of fires.</p>
      <p id="d1e3697">The global glyoxal and methylglyoxal budgets by <xref ref-type="bibr" rid="bib1.bibx21" id="text.113"/> predict that
oxidation of isoprene by OH is the dominant source of both compounds
(<inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> % for glyoxal and <inline-formula><mml:math id="M199" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">78</mml:mn></mml:mrow></mml:math></inline-formula> % for methylglyoxal). However, since
that study, the mechanism and products of the oxidation of isoprene by OH
have been examined in much greater detail both theoretically and
experimentally <xref ref-type="bibr" rid="bib1.bibx75" id="paren.114"><named-content content-type="pre">e.g</named-content><named-content content-type="post">and references therein</named-content></xref>. Despite
this, there is still disagreement in models as to the effect of <inline-formula><mml:math id="M200" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
on glyoxal yields. The latest<?pagebreak page15465?> version of the Master Chemical Mechanism (MCM
v3.3.1) predicts that glyoxal yields will increase as <inline-formula><mml:math id="M201" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> increases
<xref ref-type="bibr" rid="bib1.bibx30" id="paren.115"/>. Two studies examined glyoxal measurements from SENEX
using different mechanisms and chemical transport models. Both <xref ref-type="bibr" rid="bib1.bibx40" id="text.116"/>
and <xref ref-type="bibr" rid="bib1.bibx14" id="text.117"/> found that the best agreement between the
measurements and their respective models came from isoprene oxidation
mechanisms where the glyoxal yield decreases with increasing <inline-formula><mml:math id="M202" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.
In particular, the mechanism used by <xref ref-type="bibr" rid="bib1.bibx14" id="text.118"/> showed no
dependence on <inline-formula><mml:math id="M203" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> over short (30 min) timescales. Unfortunately,
laboratory measurements of glyoxal and methylglyoxal yields from isoprene
oxidation under low <inline-formula><mml:math id="M204" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> conditions are lacking and will be
required to better constrain the global budgets of both compounds.
Additionally, the secondary production of glyoxal and methylglyoxal in fire
plumes, and the potential <inline-formula><mml:math id="M205" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> dependence of that chemistry, has not
been measured in either a field or laboratory setting.</p>
      <p id="d1e3811">Since <inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be measured from satellites, several studies have
examined its utility as a tracer for VOC oxidation. In areas where isoprene
is the main VOC being oxidized, <inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was less than 0.025
<xref ref-type="bibr" rid="bib1.bibx31" id="paren.119"/>, while in areas where aromatics are the dominant VOCs,
<inline-formula><mml:math id="M208" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is higher (<inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula>) <xref ref-type="bibr" rid="bib1.bibx13" id="paren.120"/>. <inline-formula><mml:math id="M210" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
from fresh biomass burning is the same for many different fuel types and
unaffected by parameters such as MCE and fuel moisture content. While the
<inline-formula><mml:math id="M211" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values from fresh biomass burning are distinct from
<inline-formula><mml:math id="M212" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values from isoprene oxidation, further work to determine if
<inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> remains constant during aging of BB VOC will be an important
next step in defining the utility of this metric for investigations of VOC
sources from remote sensing instruments.
<?xmltex \hack{\vspace{-3mm}}?></p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e3916">Emissions of glyoxal and methylglyoxal from biomass burning have been
determined for a number of different fuels, including peat, rice straw,
chaparrals, and numerous conifers. Both compounds were measured using cavity-enhanced spectroscopy, which for glyoxal provides a highly sensitive
measurement with minimal interferences. The detection of methylglyoxal using
this method suffers from interferences from structurally similar compounds,
but due to the high concentrations present, methylglyoxal emissions could be
constrained to within a factor of 2. Methylglyoxal emissions were higher
than glyoxal emissions, and some fuels that emitted little glyoxal emitted
large amounts of methylglyoxal. Primary emissions of glyoxal were
significantly lower than those reported in previous laboratory work, but they were
consistent with field measurements in fresh plumes. Glyoxal emissions showed
variability between fuel groups but in nearly all cases were well correlated
with emissions of formaldehyde. The ratio of glyoxal to formaldehyde was
consistent at 0.06–0.07 for many of the fuels, with the notable exceptions of
duff and peat, which had <inline-formula><mml:math id="M214" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi mathvariant="normal">GF</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values at least a factor of 2 lower.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p id="d1e3934">Data from all instruments are publicly
available at
<uri>https://esrl.noaa.gov/csd/groups/csd7/measurements/2016firex/FireLab/DataDownload/</uri> (last access: 23 May 2018) <xref ref-type="bibr" rid="bib1.bibx51" id="paren.121"/>.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e3943">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-18-15451-2018-supplement" xlink:title="zip">https://doi.org/10.5194/acp-18-15451-2018-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution">

      <p id="d1e3952">KJZ, SSB, RJY, and JMR designed the research. KJZ, VS, ARK, KS, MMC, BY, WPD, CW,
JAdG, and SSB performed the measurements, contributed to the data analysis,
or both. All authors participated in the discussion of the results and the
writing of the paper.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e3958">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e3964">The authors thank Ryan Thalman (Snow College, UT) and Theodore Koenig
(University of Colorado Boulder) for useful discussion. The authors also
thank all those who helped organize and participated in the 2016 FIREX
intensive, particularly Edward O'Donnell and Maegan Dills for lighting the
fires, Ted Christian, Roger Ottmar, David Weise, Mark Cochrane, Kevin Ryan,
and Robert Keane for assistance with the fuels, and Shawn Urbanski and Thomas
Dzomba for logistical support. Support for Vanessa Selimovic and Robert J. Yokelson was
provided by NOAA-CPO grant NA16OAR4310100. Abigail R. Koss was supported by funding
from the NSF Graduate Fellowship Program. Kanako Sekimoto acknowledges funding
from the Postdoctoral Fellowships for Research Abroad from Japan Society for
the Promotion of Science (JSPS) and a Grant-in-Aid for Young Scientists
(B)
(15K16117) from the Ministry of Education, Culture, Sports, Science and
Technology of Japan. Matthew Coggon was supported by a CIRES Visiting
Postdoctoral Fellowship. This work was also supported by NOAA's Climate
Research and Health of the Atmosphere initiative.
<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Frank Keutsch<?xmltex \hack{\newline}?>
Reviewed by: two anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>Primary emissions of glyoxal and methylglyoxal from laboratory measurements of open biomass burning</article-title-html>
<abstract-html><p>We report the emissions of glyoxal and methylglyoxal from the open burning of
biomass during the NOAA-led 2016 FIREX intensive at the Fire Sciences
Laboratory in Missoula, MT. Both compounds were measured using cavity-enhanced spectroscopy, which is both more sensitive and more selective than
methods previously used to determine emissions of these two compounds. A
total of 75 burns were conducted, using 33 different fuels in 8 different
categories, providing a far more comprehensive dataset for emissions than was
previously available. Measurements of methylglyoxal using our instrument
suffer from spectral interferences from several other species, and the values
reported here are likely underestimates, possibly by as much as 70&thinsp;%.
Methylglyoxal emissions were 2–3 times higher than glyoxal emissions on a
molar basis, in contrast to previous studies that report methylglyoxal
emissions lower than glyoxal emissions. Methylglyoxal emission ratios for all
fuels averaged 3.6±2.4&thinsp;ppbv methylglyoxal&thinsp;(ppmv CO)<sup>−1</sup>, while emission
factors averaged 0.66±0.50&thinsp;g methylglyoxal&thinsp;(kg fuel burned)<sup>−1</sup>. Primary
emissions of glyoxal from biomass burning were much lower than previous
laboratory measurements but consistent with recent measurements from
aircraft. Glyoxal emission ratios for all fuels averaged 1.4±0.7&thinsp;ppbv glyoxal&thinsp;(ppmv CO)<sup>−1</sup>, while
emission factors averaged 0.20±0.12&thinsp;g glyoxal&thinsp;(kg fuel burned)<sup>−1</sup>, values that are at least a factor of 4 lower than
assumed in previous estimates of the global glyoxal budget. While there was
significant variability in the glyoxal emission ratios and factors between
the different fuel groups, glyoxal and formaldehyde were highly correlated
during the course of any given fire, and the ratio of glyoxal to
formaldehyde, <i>R</i><sub>GF</sub>, was consistent across many different fuel
types, with an average value of 0.068±0.018. While <i>R</i><sub>GF</sub> values
for fresh emissions were consistent across many fuel types, further work is
required to determine how this value changes as the emissions age.</p></abstract-html>
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