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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 GmbH</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>

    <article-meta>
      <article-id pub-id-type="doi">10.5194/acp-15-7537-2015</article-id><title-group><article-title>The role of blowing snow in the activation of bromine over first-year Antarctic sea ice</article-title>
      </title-group><?xmltex \runningtitle{Blowing snow and bromine activation}?><?xmltex \runningauthor{R.~M.~Lieb-Lappen and R.~W.~Obbard}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Lieb-Lappen</surname><given-names>R. M.</given-names></name>
          <email>ross.lieb-lappen@dartmouth.edu</email>
        <ext-link>https://orcid.org/0000-0002-5840-7538</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Obbard</surname><given-names>R. W.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2532-5648</ext-link></contrib>
        <aff id="aff1"><institution>14 Engineering Drive, Thayer School of Engineering, Dartmouth College, Hanover, NH, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">R. M. Lieb-Lappen (ross.lieb-lappen@dartmouth.edu)</corresp></author-notes><pub-date><day>13</day><month>July</month><year>2015</year></pub-date>
      
      <volume>15</volume>
      <issue>13</issue>
      <fpage>7537</fpage><lpage>7545</lpage>
      <history>
        <date date-type="received"><day>06</day><month>March</month><year>2015</year></date>
           <date date-type="rev-request"><day>22</day><month>April</month><year>2015</year></date>
           <date date-type="rev-recd"><day>18</day><month>June</month><year>2015</year></date>
           <date date-type="accepted"><day>30</day><month>June</month><year>2015</year></date>
      </history>
      <permissions>
<license license-type="open-access">
<license-p>This work is licensed under a Creative Commons Attribution 3.0 Unported License. To view a copy of this license, visit <ext-link ext-link-type="uri" xlink:href="http://creativecommons.org/licenses/by/3.0/">http://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions><self-uri xlink:href="https://acp.copernicus.org/articles/.html">This article is available from https://acp.copernicus.org/articles/.html</self-uri>
<self-uri xlink:href="https://acp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/.pdf</self-uri>


      <abstract>
    <p>It is well known that during polar springtime halide sea salt ions, in
particular Br<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>, are photochemically activated into reactive halogen
species (e.g., Br and BrO), where they break down tropospheric ozone. This
research investigated the role of blowing snow in transporting salts from the
sea ice/snow surface into reactive bromine species in the air. At two
different locations over first-year ice in the Ross Sea, Antarctica,
collection baskets captured blowing snow at different heights. In addition,
sea ice cores and surface snow samples were collected throughout the
month-long campaign. Over this time, sea ice and surface snow
Br<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mo>/</mml:mo></mml:math></inline-formula> Cl<inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula> mass ratios remained constant and equivalent to
seawater, and only in lofted snow did bromide become depleted relative to
chloride. This suggests that replenishment of bromide in the snowpack occurs
faster than bromine activation in mid-strength wind conditions (approximately
<inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula> m s<inline-formula><mml:math 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>) or that blowing snow represents only a small portion of
the surface snowpack. Additionally, lofted snow was found to be depleted in
sulfate and enriched in nitrate relative to surface snow.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p>The polar springtime is a season of change, most notably in temperature, sea
ice coverage, and weather, but it also signals the onset of many
photochemically driven atmospheric chemical reactions, such as tropospheric
ozone depletion events (ODEs) <xref ref-type="bibr" rid="bib1.bibx5" id="paren.1"><named-content content-type="pre">e.g.,</named-content></xref>. Boundary layer
ozone in polar regions has been observed to fall dramatically periodically in
the spring in both the Arctic <xref ref-type="bibr" rid="bib1.bibx5" id="paren.2"/> and Antarctic
<xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx51" id="paren.3"/>. These tropospheric ODEs are initiated by
increased concentrations of reactive bromine gases (BrO and Br) resulting in
a catalytic removal of ozone <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx29 bib1.bibx11" id="paren.4"/>;
however the mechanism by which Br enters the atmosphere is not well
understood <xref ref-type="bibr" rid="bib1.bibx1" id="paren.5"/>. The heterogeneous reaction producing bromine
gas and hypothesized to explain the “bromine explosion” is given by
<xref ref-type="bibr" rid="bib1.bibx10" id="text.6"/>:

              <disp-formula id="Ch1.E1" content-type="numbered"><mml:math display="block"><mml:mrow><mml:mrow class="chem"><mml:mi mathvariant="normal">HOBr</mml:mi></mml:mrow><mml:mo>+</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>+</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">H</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow><mml:mo>→</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">Br</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

        Proposed surfaces on which this reaction may occur have included sea spray
<xref ref-type="bibr" rid="bib1.bibx43" id="normal.7"/>, frost flowers <xref ref-type="bibr" rid="bib1.bibx40 bib1.bibx22" id="paren.8"/>, surface
snow <xref ref-type="bibr" rid="bib1.bibx44" id="paren.9"/>, aerosols <xref ref-type="bibr" rid="bib1.bibx49 bib1.bibx11" id="paren.10"/>, and blowing
snow <xref ref-type="bibr" rid="bib1.bibx54" id="paren.11"/>.</p>
      <p>Although some bromide may arrive via sea spray produced aerosol
<xref ref-type="bibr" rid="bib1.bibx43" id="paren.12"/>, this mechanism is relatively less efficient and does not
produce aerosol with the observed sulfate depletion <xref ref-type="bibr" rid="bib1.bibx50" id="paren.13"/>. As
seawater freezes, salt rejection leads to an increasingly saline brine
<xref ref-type="bibr" rid="bib1.bibx47" id="paren.14"/>. Specific salts precipitate out of solution when
solubility limits are reached below <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C <xref ref-type="bibr" rid="bib1.bibx27" id="paren.15"/>,
producing brine with different ion ratios than those found in seawater. The
brine is expelled to the ice/snow or ice/atmosphere surface, where it forms
a fractionated surface skim and slush <xref ref-type="bibr" rid="bib1.bibx41" id="paren.16"/>. This reservoir of
bromide and other sea salts can be incorporated into frost flowers by
wicking, or into the snow lying on sea ice by upward migration through
capillary forces <xref ref-type="bibr" rid="bib1.bibx35" id="paren.17"/>. It may be transported by the lofting
of snow from sea ice with subsequent sublimation and return of the aerosol to
the snowpack <xref ref-type="bibr" rid="bib1.bibx54 bib1.bibx20" id="paren.18"/>. However, the physical surface at
which bromide activation occurs remains a subject of some debate.</p>
      <p>It has been shown that brine is wicked upward by frost flowers that form on
fresh sea ice, yielding a highly saline surface with the aforementioned
sulfate depletion, and that the dendritic nature of frost flowers magnifies
the surface area available for atmospheric interactions <xref ref-type="bibr" rid="bib1.bibx41" id="paren.19"/>.
However, studies have shown that frost flowers do not significantly increase
the surface area available for heterogeneous reactions <xref ref-type="bibr" rid="bib1.bibx7 bib1.bibx33" id="paren.20"/> and that frost flowers are not easily broken and lofted
<xref ref-type="bibr" rid="bib1.bibx33" id="paren.21"/>. Instead, they accumulate snow on their windward side in
strong winds and when broken, fall where they are <xref ref-type="bibr" rid="bib1.bibx33" id="paren.22"/>.
Laboratory studies of frost flowers have also shown that frost flowers are
quite stable in winds up to <inline-formula><mml:math display="inline"><mml:mn>12</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, and aerosol production is
not observed under these conditions <xref ref-type="bibr" rid="bib1.bibx42" id="paren.23"/>. Further,
<xref ref-type="bibr" rid="bib1.bibx44" id="text.24"/> and <xref ref-type="bibr" rid="bib1.bibx33" id="text.25"/> found that frost flowers are not
depleted in bromide relative to sodium and chloride, indicating they are not
the immediate source of bromine-depleted snow nor the location of the
heterogeneous reactions activating bromine. It has also been shown that
first-year sea ice contact better correlates to increased BrO concentrations
than does contact with potential frost flower regions <xref ref-type="bibr" rid="bib1.bibx45" id="paren.26"/>.</p>
      <p>In <xref ref-type="bibr" rid="bib1.bibx44" id="text.27"/> however, the snowpack did have
<inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Na</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> ratio fluctuations by 2 orders of magnitude
with bromide depletions of up to <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>90</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>, suggesting bromine was released
in the aerosol phase or in the snowpack itself. Sea salts can migrate upwards
through the snowpack as high as <inline-formula><mml:math display="inline"><mml:mn>17</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula>, even in cold conditions
where slush is not present <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx6" id="paren.28"/>. However, in thicker
snowpacks, the surface snow is more readily acidified and influenced by
atmospheric processes, and thus, more likely to play a role in halogen
activation. Bromine activation is more efficient in acidic conditions and in
environments with a higher <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> ratio
<xref ref-type="bibr" rid="bib1.bibx38" id="paren.29"/>. <xref ref-type="bibr" rid="bib1.bibx38" id="text.30"/> further hypothesized that the snowpack
interstitial air is the primary location for the heterogeneous reactions,
with wind pumping providing a vehicle to release the bromine into the
boundary layer.</p>
      <p><xref ref-type="bibr" rid="bib1.bibx54" id="text.31"/> proposed a fourth mechanism for bromine activation that
involves the lofting of snow from sea ice with subsequent sublimation and
either direct bromine release or return of the aerosol to the snowpack. In
the model, lofted snow particles were allowed to sublimate to a particle size
of <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn>10</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, whereby the particles instantaneously released
bromine or were potentially scoured by more blowing snow particles. Snow
salinity was found to have a nonlinear relationship with bromine production,
and the reaction rate varied with dry aerosol particle size. It was shown
that <inline-formula><mml:math display="inline"><mml:mn>1.3</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> particles yielded the most efficient release of
bromine since the smaller aerosol could be lofted further and longer
<xref ref-type="bibr" rid="bib1.bibx54" id="paren.32"/>. Further work showed that snow in the sea ice zone may
contain enough salt when lofted by wind to produce the necessary aerosol to
explain the observed Antarctic ODEs <xref ref-type="bibr" rid="bib1.bibx55" id="paren.33"/>. While it may be
difficult for saturated snow lying on surface skim to become lofted, snow in
the upper layers could wick up salts yet remain mobile, providing enormous
capacity for transporting bromide into the boundary layer. <xref ref-type="bibr" rid="bib1.bibx54" id="text.34"/>
provides the theoretical framework and model-based data for the physical
measurements observed and presented in this manuscript.</p>
      <p>ODEs have been found to occur at a range of wind speeds, something that has
made agreement upon a mechanism difficult. Some have observed that ODEs
require low winds, a stable boundary layer, and a relatively clear sky, or
the movement of air masses from such regions <xref ref-type="bibr" rid="bib1.bibx46" id="paren.35"/>. Using
measurements and modeling, <xref ref-type="bibr" rid="bib1.bibx3" id="text.36"/> found rapid ozone depletion in
the top <inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula> of the snowpack due to diffusion and ventilation in
moderate winds. More recently, ODEs have been recorded during high winds
(<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn>12</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), which increase the snow surface area exposed via
blowing snow, and thus, the probability of contact between the gaseous and
condensed phases required to initiate bromine release <xref ref-type="bibr" rid="bib1.bibx20" id="paren.37"/>.
During the 2009 OASIS campaign in Barrow, AK, high winds were observed to
correspond with increased BrO concentrations <xref ref-type="bibr" rid="bib1.bibx12" id="paren.38"/>. This was
accompanied by decreased HOBr, suggesting that blowing snow likely provided
additional surfaces for heterogeneous HOBr loss <xref ref-type="bibr" rid="bib1.bibx26" id="paren.39"/>. These high
wind halogen activation events may have a more widespread role when
considering the impact of ODEs on regional tropospheric chemistry
<xref ref-type="bibr" rid="bib1.bibx21" id="paren.40"/>. Additionally, higher winds may enhance the availability of
radical bromine precursors in the snowpack, accelerating bromine activation
<xref ref-type="bibr" rid="bib1.bibx48" id="paren.41"/>. On the contrary, others <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx16" id="paren.42"><named-content content-type="pre">e.g.,</named-content></xref> have found no correlation between ODEs and wind speed. However,
the lack of low ozone observations at high wind speed may be a result of
enhanced mixing <xref ref-type="bibr" rid="bib1.bibx17" id="paren.43"/>. Although the chemistry of snow has been
well studied <xref ref-type="bibr" rid="bib1.bibx28 bib1.bibx6 bib1.bibx15" id="paren.44"/>, there has been no
attempt until now at segregating snow capable of wind transport or snow
actually blown by wind.</p>
      <p>It is noted that both <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">Cl</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and BrCl play a role in halide boundary
layer chemistry and ODEs <xref ref-type="bibr" rid="bib1.bibx1" id="paren.45"/>, but the focus of this work is on
bromine because it is a far more efficient catalyst of ozone loss. As the
main constituents of seawater, both chloride and sodium have been used as sea
salt tracers, and thus chloride was used here to both determine snow and ice
salinity and relative activity of other anions. Previous work has shown that
sulfate is influenced both by mirabilite precipitation and atmospheric
interactions, while nitrate is uncorrelated with sea salt and is deposited as
a byproduct of other reactions <xref ref-type="bibr" rid="bib1.bibx25" id="paren.46"/>.</p>

      <fig id="Ch1.F1" specific-use="star"><caption><p>Map of the Ross Sea region showing the two field sites Butter
Point and Iceberg. Basemap is Landsat image.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/15/7537/2015/acp-15-7537-2015-f01.png"/>

      </fig>

</sec>
<sec id="Ch1.S2">
  <title>Methods</title>
      <p>Two field sites on first-year sea ice in the Ross Sea, Antarctica, were
chosen, based upon prevailing wind direction, to maximize contact of the
blowing snow with the first-year sea ice. Their locations are shown in
Fig. <xref ref-type="fig" rid="Ch1.F1"/>. Butter Point Site was located <inline-formula><mml:math display="inline"><mml:mn>6.5</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> from the open
ocean and <inline-formula><mml:math display="inline"><mml:mn>35</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> north of the Ross Ice Shelf. Iceberg Site was
located <inline-formula><mml:math display="inline"><mml:mn>55</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> northwest of Butter Point, and since the ice edge
located to the east follows the shore, the distance to open water here was
also <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula>. Iceberg Site was chosen based upon the presence of
a <inline-formula><mml:math display="inline"><mml:mn>740</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> long and <inline-formula><mml:math display="inline"><mml:mn>35</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> high iceberg located
<inline-formula><mml:math display="inline"><mml:mn>250</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> to the west that would block winds sourced over land,
maximizing blowing snow collection from over sea ice. At each site,
a <inline-formula><mml:math display="inline"><mml:mn>5.5</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> blowing snow collection tower was erected for the time
period of <inline-formula><mml:math display="inline"><mml:mn>11</mml:mn></mml:math></inline-formula> October–<inline-formula><mml:math display="inline"><mml:mn>08</mml:mn></mml:math></inline-formula> November <inline-formula><mml:math display="inline"><mml:mn>2012</mml:mn></mml:math></inline-formula>. Collection baskets made out of
<inline-formula><mml:math display="inline"><mml:mn>150</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> nylon monofilament mesh and <inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mn mathvariant="normal">7</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> diameter by <inline-formula><mml:math display="inline"><mml:mrow><mml:msup><mml:mn>14</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> long
(Midwest Filter Corporation, Lake Forest, IL) were placed at four different
heights: 0.3, 2.0, 3.0, and <inline-formula><mml:math display="inline"><mml:mn>5.5</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> above the snow surface.</p>
      <p>The sites were visited approximately every other day, and collection baskets
were switched even if no snow was collected. Baskets were triple rinsed with
DI water between uses. Surface snow samples were collected each of the <inline-formula><mml:math display="inline"><mml:mn>12</mml:mn></mml:math></inline-formula>
days the sites were visited. In addition, <inline-formula><mml:math display="inline"><mml:mn>1.78</mml:mn></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mn>1.89</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula> ice
cores were extracted from Butter Point and Iceberg sites, respectively. Snow
samples and sea ice cores were transported at a constant temperature of
<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>20</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C back to Thayer School of Engineering's Ice Research
Laboratory at Dartmouth College and stored in a <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>33</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C cold room.</p>
      <p>Winds during the field campaign were generally mild, only surpassing
<inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> on a few occasions. Site visits were not feasible
during stormy weather, and much of the blowing snow captured during those
periods sublimated in the baskets prior to collection as observed by
a webcam. Thus, only on <inline-formula><mml:math display="inline"><mml:mn>25</mml:mn></mml:math></inline-formula> October were blowing snow samples collected at
both sites and all four heights. The collected snow was the result of
approximately <inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> southerly winds on <inline-formula><mml:math display="inline"><mml:mn>24</mml:mn></mml:math></inline-formula> October.
Visibility at McMurdo station during this blowing snow event dropped below
<inline-formula><mml:math display="inline"><mml:mn>0.5</mml:mn></mml:math></inline-formula> miles for about <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">4</mml:mn></mml:math></inline-formula> h. Temperatures ranged from <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>20.5</mml:mn></mml:mrow></mml:math></inline-formula>
to <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>11.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C with an average relative humidity of <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>69</mml:mn><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> on
<inline-formula><mml:math display="inline"><mml:mn>24</mml:mn></mml:math></inline-formula> October and <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>17.5</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>13.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C with an average
relative humidity of <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>61</mml:mn><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> on <inline-formula><mml:math display="inline"><mml:mn>25</mml:mn></mml:math></inline-formula> October. These temperatures were a couple
of degrees warmer than the average for the rest of the field campaign.</p>
      <p>All surface snow and blowing snow samples were melted into acid-rinsed HDPE
vials, and diluted by a factor of <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula> with DI water. Those samples falling
outside of the calibration standard concentrations were further diluted to
fall within the desired range. Each ice core was sub-sampled every
<inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula>, melted, and diluted by a factor of <inline-formula><mml:math display="inline"><mml:mn>50</mml:mn></mml:math></inline-formula>, except for the
bottom-most sample that was diluted by a factor of <inline-formula><mml:math display="inline"><mml:mn>100</mml:mn></mml:math></inline-formula>. A <inline-formula><mml:math display="inline"><mml:mn>0.5</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">mL</mml:mi></mml:math></inline-formula>
aliquot of each diluted snow and ice sample was then analyzed for anion
concentrations.</p>
      <p>Anion chromatography was completed using a Dionex-<inline-formula><mml:math display="inline"><mml:mn>600</mml:mn></mml:math></inline-formula> IC system, equipped
with a LC <inline-formula><mml:math display="inline"><mml:mn>25</mml:mn></mml:math></inline-formula> chromatogram oven set at <inline-formula><mml:math display="inline"><mml:mn>30</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C, GD <inline-formula><mml:math display="inline"><mml:mn>50</mml:mn></mml:math></inline-formula> gradient
pump, CD <inline-formula><mml:math display="inline"><mml:mn>25</mml:mn></mml:math></inline-formula> conductivity detector, AS15 anion column with a AG15 guard
column, and an auto-sampler. A <inline-formula><mml:math display="inline"><mml:mn>38</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">mM</mml:mi></mml:math></inline-formula> NaOH eluent was used at a flow
rate of <inline-formula><mml:math display="inline"><mml:mn>1.2</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">mL</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">min</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and the SRS current was set to
<inline-formula><mml:math display="inline"><mml:mn>100</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:mrow></mml:math></inline-formula>. Pressure in the column was 1600 psi and the signal
noise was approximately <inline-formula><mml:math display="inline"><mml:mn>0.003</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:mrow></mml:math></inline-formula>. Peak analysis was performed
using Chromeleon <inline-formula><mml:math display="inline"><mml:mn>6.8</mml:mn></mml:math></inline-formula> software with a <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula> point standard calibration curve.
IC detection limits were <inline-formula><mml:math display="inline"><mml:mn>0.6</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mn>0.1</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mn>0.04</mml:mn></mml:math></inline-formula>, and <inline-formula><mml:math display="inline"><mml:mn>0.03</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>,
yielding limits of quantification of <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">2</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mn>0.3</mml:mn></mml:math></inline-formula>, <inline-formula><mml:math display="inline"><mml:mn>0.1</mml:mn></mml:math></inline-formula>, and
<inline-formula><mml:math display="inline"><mml:mn>0.1</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for chloride, sulfate, bromide, and nitrate,
respectively.</p>

      <fig id="Ch1.F2" specific-use="star"><caption><p>Anion concentrations for sea ice cores. Butter Point Site
samples are shown in red filled-in squares and red lines, while
Iceberg Site samples are shown in blue open circles and blue lines.</p></caption>
        <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/15/7537/2015/acp-15-7537-2015-f02.pdf"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <title>Results</title>
      <p>Raw anion concentrations for sea ice, surface snow, and blowing snow samples
are provided in the Supplement. Sea ice anion concentrations
had nearly identical profiles for Butter Point and Iceberg cores, with both
showing the expected C-shape profile (see Fig. <xref ref-type="fig" rid="Ch1.F2"/>)
<xref ref-type="bibr" rid="bib1.bibx9" id="paren.47"/>. Note that the deepest sample for Iceberg Site was
directly at the base of the core, while the deepest sample for Butter Point
was <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">8</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula> above the base, due to a mushy, poorly defined basal
layer, and thus missed the saltiest portion. Chloride concentrations ranged
from 2000–8000 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, while bromide concentrations ranged
from 5–35 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Sulfate concentrations ranged from 2–3000 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, with increased variation observed over the top
<inline-formula><mml:math display="inline"><mml:mn>40</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula> of both cores. Nitrate concentrations were below detection
limits for all sea ice core samples.</p>
      <p>Surface snow anion concentrations varied greatly, but were of similar
magnitude at the two sites and showed no noticeable trend with time over the
field campaign. Concentrations ranged from 200–5000 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
chloride, 1.0–16 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> bromide, 20–2300 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
sulfate, and 0–1.2 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> nitrate, though the majority of
samples were below detection limits in nitrate. If we assume Cl
concentrations to be a good proxy to estimate salinity using sea water ion
ratios, this corresponds to a mean surface snow salinity of <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">3</mml:mn></mml:math></inline-formula> PSU, with a
range of 0.4–9 PSU. There was little snow cover at Butter Point with the
surface varying from completely wind scoured to several cm of snow. Iceberg
Site had a more variable snowpack, with prevalent rafted ice and sastrugi,
resulting in snow depths varying from tens of cm to over <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">1</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>.
A <inline-formula><mml:math display="inline"><mml:mn>21</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">cm</mml:mi></mml:math></inline-formula> snow pit was dug <inline-formula><mml:math display="inline"><mml:mn>15</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">km</mml:mi></mml:math></inline-formula> from Butter Point Site to
study a more consistent snowpack that is representative of the greater
first-year sea ice of the region. In this snow pit, both chloride and bromide
concentrations increased steadily from the snow surface to the snow/ice
interface, with concentrations ranging from 500–1600 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
chloride and 1.5–6 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> bromide. Sulfate concentrations
ranged from 30–50 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, but showed a C-shaped profile with
highest concentrations found near the top and bottom of the snow pit.
A second snow pit located slightly closer to the open ocean showed similar
trends.</p>
      <p>Anion concentrations from the blowing snow samples collected on <inline-formula><mml:math display="inline"><mml:mn>25</mml:mn></mml:math></inline-formula> October
in both towers varied greatly, including separate samples from the same
collection baskets, indicating that blown snow can be quite varied in its
salt concentration. Concentrations ranged from 50–6800 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
chloride, 0.2–18.5 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> bromide, 3–240 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>
sulfate, and 0.4–23 <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> nitrate. Using chloride
concentrations to derive an estimate of salinity, blowing snow samples ranged
from <inline-formula><mml:math display="inline"><mml:mn>0.1</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math display="inline"><mml:mn>12</mml:mn></mml:math></inline-formula> PSU. Comparing the <inline-formula><mml:math display="inline"><mml:mn>0.3</mml:mn></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mn>5.5</mml:mn></mml:math></inline-formula> m baskets at both
sites suggests a <inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula>-fold increase in salinity from <inline-formula><mml:math display="inline"><mml:mn>0.6</mml:mn></mml:math></inline-formula> to <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">6</mml:mn></mml:math></inline-formula> PSU.
However, when all blowing snow samples are considered, there is not a
statistically significant trend of increasing salt concentration with basket
height, except for nitrate where concentrations increased with height above
the snow surface.</p>

      <fig id="Ch1.F3"><caption><p><inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios for sea ice (negative
heights), surface snow (height of <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula>), and blowing snow (height
above snow surface).  Blowing snow lines connect averages for each
basket height.  Butter Point Site samples are shown in red filled-in
squares and red lines, while Iceberg Site samples are shown in blue
open circles and blue lines.  The standard ocean
<inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratio is shown as a black dashed
line <xref ref-type="bibr" rid="bib1.bibx31" id="paren.48"/>.</p></caption>
        <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://acp.copernicus.org/articles/15/7537/2015/acp-15-7537-2015-f03.pdf"/>

      </fig>

      <p>Anion concentrations can provide a general understanding of the overall
salinity of the snow and ice, but in order to understand chemical reaction
activity, it is instructive to calculate anion concentration ratios. The
<inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratio has long been used as a metric for
analyzing both frozen and liquid saline water samples, and comparing measured
values to the well established <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>290</mml:mn></mml:mrow></mml:math></inline-formula> ratio observed in seawater
<xref ref-type="bibr" rid="bib1.bibx31" id="paren.49"/>. This ratio is plotted in Fig. <xref ref-type="fig" rid="Ch1.F3"/> for all
samples at both sites. <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios were
relatively constant for all sea ice samples (<inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>281</mml:mn><mml:mo>±</mml:mo><mml:mn>24</mml:mn></mml:mrow></mml:math></inline-formula>) and all surface
snow samples (<inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>296</mml:mn><mml:mo>±</mml:mo><mml:mn>22</mml:mn></mml:mrow></mml:math></inline-formula>). However, there was a linear correlation
between <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios for blowing snow relative to
height at both Butter Point (<inline-formula><mml:math 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>0.89</mml:mn></mml:mrow></mml:math></inline-formula>) and Iceberg Site (<inline-formula><mml:math 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>0.93</mml:mn></mml:mrow></mml:math></inline-formula>).
Sulfate mass ratios in sea ice, surface snow, and blowing snow did not show
as clear a trend (Fig. <xref ref-type="fig" rid="Ch1.F4"/>). In sea ice, the
<inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratio was roughly <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:math></inline-formula> in the bottom
half of the cores, consistent with what is generally observed in seawater
<xref ref-type="bibr" rid="bib1.bibx31" id="paren.50"/>, but varied from approximately <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>12</mml:mn></mml:mrow></mml:math></inline-formula> in the
upper halves of the cores. Surface snow mass ratios also were quite variable
ranging from <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>19</mml:mn></mml:mrow></mml:math></inline-formula> with no clear correlations. Collected lofted
snow was quite depleted in sulfate with mass ratios reaching <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>20</mml:mn></mml:mrow></mml:math></inline-formula> to
<inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>40</mml:mn></mml:mrow></mml:math></inline-formula>, but did not show the linear trend with height observed with bromide.</p>

      <fig id="Ch1.F4"><caption><p><inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios for sea ice
(negative heights), surface snow (height of <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">0</mml:mn></mml:math></inline-formula>), and blowing snow
(height above snow surface).  Butter Point Site samples are shown in
red filled-in squares (snow samples) and a red line (sea ice), while
Iceberg Site samples are shown in blue open circles (snow samples)
and a blue line (sea ice). The standard ocean
<inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratio is shown as a black dashed
line <xref ref-type="bibr" rid="bib1.bibx31" id="paren.51"/>.</p></caption>
        <?xmltex \igopts{width=199.169291pt}?><graphic xlink:href="https://acp.copernicus.org/articles/15/7537/2015/acp-15-7537-2015-f04.pdf"/>

      </fig>

</sec>
<sec id="Ch1.S4">
  <title>Discussion</title>
      <p>Observation of bromide depletion relative to other salts is an indication of
heterogeneous atmospheric chemical reactions and bromine activation
<xref ref-type="bibr" rid="bib1.bibx2 bib1.bibx18 bib1.bibx44" id="paren.52"/>. Although there was some variability
in <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios for sea ice and surface snow,
these ratios were remarkably constant, just over <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>300</mml:mn></mml:mrow></mml:math></inline-formula>. As shown in
Fig. <xref ref-type="fig" rid="Ch1.F3"/>, signs of bromide depletion occur above the snowpack,
with greater depletion occurring at greater heights, reaching mass ratios of
nearly <inline-formula><mml:math display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn>1000</mml:mn></mml:mrow></mml:math></inline-formula> at heights of <inline-formula><mml:math display="inline"><mml:mn>5.5</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>. This is consistent with
aerosol observations by <xref ref-type="bibr" rid="bib1.bibx8" id="text.53"/> that measured increased bromide
depletion with height, albeit at tropical latitudes. They noted a strong
particle size dependence with increased bromide depletion corresponding to
mid-sized aerosol particles. Further studies have shown that particle size
influences the mode of transport and it may not be realistic to differentiate
snow saltation and suspension based solely on wind speed and height
<xref ref-type="bibr" rid="bib1.bibx32" id="paren.54"/>. Nevertheless, both processes greatly increase the snow
surface area exposed for gas-phase reactions by as much as <inline-formula><mml:math display="inline"><mml:mn>3000</mml:mn></mml:math></inline-formula> times that
of surface snow <xref ref-type="bibr" rid="bib1.bibx37" id="paren.55"/>. It is noted that snow blowing at the
windspeed will have no relative motion compared to the gases and gas-phase
diffusion becomes an important consideration, especially for large grain
particles. Local turbulence however, will help to overcome some of these
diffusion limitations <xref ref-type="bibr" rid="bib1.bibx32" id="paren.56"/>. We also note that sublimation of
blowing snow particles likely has a strong effect on anion concentrations.
Consistent with the mechanism suggested by <xref ref-type="bibr" rid="bib1.bibx54" id="text.57"/>, lighter
particles would remain airborne for longer periods of time, leading to
suspension at greater heights and more time for photochemical reactions.
However, since particle sizes were not measured in this study, we solely
mention the potential sublimation may have on increasing bromine release
through this pathway.</p>
      <p>A depletion factor (DF) was defined such that DF <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> signifies no bromine
depletion in particles, and DF<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> signifies complete depletion
<xref ref-type="bibr" rid="bib1.bibx53" id="paren.58"/>. We note that a negative value for DF indicates bromine
enrichment. Averaging the <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios at each
height for Butter Point yields DF <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mn>0.04</mml:mn><mml:mo>,</mml:mo><mml:mn>0.11</mml:mn><mml:mo>,</mml:mo><mml:mn>0.41</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mn>0.68</mml:mn></mml:math></inline-formula> for heights
of 0.3, 2.0, 3.0, and <inline-formula><mml:math display="inline"><mml:mn>5.5</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mi mathvariant="normal">m</mml:mi></mml:math></inline-formula>, respectively. At Iceberg Site,
DF <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn>0.08</mml:mn></mml:mrow></mml:math></inline-formula>, 0.20, 0.33, and <inline-formula><mml:math display="inline"><mml:mn>0.64</mml:mn></mml:math></inline-formula> for the four heights, respectively.
Depletion factors were relatively small for both surface snow and ice core
samples, with values ranging from <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.20</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math display="inline"><mml:mn>0.13</mml:mn></mml:math></inline-formula> and <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn>0.13</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math display="inline"><mml:mn>0.17</mml:mn></mml:math></inline-formula>,
respectively. These values are consistent with previously reported values and
currently used in some models <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx53" id="paren.59"/>. Previously,
<xref ref-type="bibr" rid="bib1.bibx44" id="text.60"/> observed up to <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>90</mml:mn><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> bromide depletion in surface snow,
while <xref ref-type="bibr" rid="bib1.bibx19" id="text.61"/> observed up to <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>70</mml:mn><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula> depletion in snow mobilized
<inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula> cm above the surface. The latter study also noted that during a blowing
snow event, there was first bromide enrichment in the snow during the initial
part of the storm followed by later bromide depletion <xref ref-type="bibr" rid="bib1.bibx19" id="paren.62"/>. An
increased depletion factor can either signify bromide depletion due to
bromine release or chloride enrichment from, for example, gaseous HCL uptake.
If the latter hypothesis were true, one would expect to observe increased
chloride concentrations in higher baskets. The lack of an observed chloride
trend with height leads to our interpretation that the decreased mass ratio
is a clear indicator of bromine activation. Interestingly, lower
<inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> ratios have also been found to correspond with a
decrease in chlorine release <xref ref-type="bibr" rid="bib1.bibx52" id="paren.63"/>. This is due to the fact that
BrCl plays a critical role in chlorine production. BrCl is initially formed
from the reaction between HOBr and <inline-formula><mml:math display="inline"><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>, and then upon later
photolysis, can lead to chlorine release <xref ref-type="bibr" rid="bib1.bibx52" id="paren.64"/>.</p>
      <p>Previously, bromine activation and ODEs were observed in both low
(<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) and high (<inline-formula><mml:math display="inline"><mml:mrow><mml:mo>&gt;</mml:mo><mml:mn>12</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) winds
<xref ref-type="bibr" rid="bib1.bibx20" id="paren.65"/>. Here, the blowing snow event occurred during moderate
winds of approximately <inline-formula><mml:math display="inline"><mml:mn>10</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Since the wind was from the
south and there was no new precipitation, it is safe to assume that the snow
originated from the surface of first-year sea ice. It is noted that the
blowing snow event lasted approximately 4–6 h, and that snow samples
from the baskets were not collected until 10–12 h later. During this
time, wind speeds dropped to less than <inline-formula><mml:math display="inline"><mml:mn mathvariant="normal">5</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, and it is
possible that the collected snow was exposed to further wind scouring.
However, all baskets would have experienced a similar degree of scouring in
these minimal winds and the effect would be minor over the short time period
prior to collection. Further, the collected snow was mostly windpacked,
suggesting it was unlikely the wind penetrated both the <inline-formula><mml:math display="inline"><mml:mn>150</mml:mn></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>
nylon monofilament mesh of the basket and the interior bulk of the snow.
Future studies, however, may attempt to better seal off collected blown snow.</p>
      <p>The surface snow <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios at both sites showed
little variation and no observed trend with date or meteorology over the
month-long campaign. If there was a significant amount of lofted snow being
depleted in bromide and then falling back to the snow surface, one might
expect to detect a signal in the surface snow chemistry. The lack of recorded
bromide depletion in the surface snow may indicate that either surface snow
bromide concentration is quickly replenished or that blowing snow represents
only a small portion of the surface snowpack. Surface snow will be
replenished in bromide through interaction with saline brine
<xref ref-type="bibr" rid="bib1.bibx34" id="paren.66"/>, deposition of HOBr as a byproduct of the reaction
between BrO and HO<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, deposition of HBr, and deposition of aerosol-phase
bromine. In cold ambient environments, frost flowers, surface snow, and the
sea ice surface have been shown to be bromide enriched sources, likely due to
the precipitation of NaCl <xref ref-type="bibr" rid="bib1.bibx23 bib1.bibx30" id="paren.67"/>. Additionally,
recycling of deposited bromine plays a critical role with as much as <inline-formula><mml:math display="inline"><mml:mrow><mml:mn>75</mml:mn><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></inline-formula>
of deposited bromine being re-emitted into the gas phase as Br<inline-formula><mml:math display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> or BrCl
<xref ref-type="bibr" rid="bib1.bibx36" id="paren.68"/>. In future work, it would be informative to collect both
surface and blowing snow during stronger wind events.</p>
      <p>The sulfate depletion observed in lofted snow is consistent with the
observations of others, most likely a product of mirabilite precipitation
occurring at temperatures below <inline-formula><mml:math display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C <xref ref-type="bibr" rid="bib1.bibx40" id="paren.69"/>. The
range of <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios measured in surface snow
and the upper halves of the ice cores is also likely due to similar
interactions. Sulfate depletion can result from a wide variety of processes
involving brine and mirabilite formation as brine constantly moves through
sea ice and is also wicked up by surface snow <xref ref-type="bibr" rid="bib1.bibx25" id="paren.70"/>. In
addition, non-sea salt sourced sulfate may provide additional sulfate to the
surface snowpack <xref ref-type="bibr" rid="bib1.bibx39 bib1.bibx25" id="paren.71"/>.</p>
      <p>Nitrate concentration in seawater is highly dependent upon phytoplankton
blooms, and therefore varies greatly from single digit <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> to
less than one <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx14 bib1.bibx4" id="paren.72"><named-content content-type="pre">e.g.,</named-content></xref>. Thus,
it was not surprising that sea ice samples were below the quantification
limit for nitrate. Surface snow samples also were generally below nitrate
detection limits, and those with quantifiable concentrations showed no
noticeable trend. Nitrate snow photochemistry is quite complex, with many
processes both adding and subtracting nitrate from the snowpack
<xref ref-type="bibr" rid="bib1.bibx15 bib1.bibx25" id="paren.73"/>. Nitrate sources include biomass burning,
lightning production, soil exhalation, and anthropogenic pollutants that can
be carried long distances through atmospheric transport <xref ref-type="bibr" rid="bib1.bibx13 bib1.bibx25" id="paren.74"/>. The increase in nitrate concentration observed with basket
height may be attributed to increased atmospheric interactions higher above
the snowpack. Additionally, basket nitrate concentration may also be
influenced by interactions occurring while the snow was sitting in the basket
but prior to collection, as cycling of different nitrogen-containing
compounds is relatively fast and can vary greatly during a day
<xref ref-type="bibr" rid="bib1.bibx15" id="paren.75"/>. Considering the number of competing reactions, more data
points would be needed to make conclusive statements regarding the cycling of
nitrate in the polar boundary layer.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p>In summary, this work examined the mass ratio of <inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula>
in blowing snow during mid-strength winds to better understand mechanisms
leading to bromine activation. It was found that while
<inline-formula><mml:math display="inline"><mml:mrow><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Br</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow><mml:mo>/</mml:mo><mml:mrow class="chem"><mml:msup><mml:mi mathvariant="normal">Cl</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:mrow></mml:math></inline-formula> mass ratios remained relatively constant for sea
ice and surface snow, bromide becomes strongly depleted relative to chloride
in lofted snow. Thus, we conclude the blowing snow particles provide a very
viable surface for the initial heterogeneous reactions initializing ODEs to
occur. The findings of this study are consistent with previous modeling
results <xref ref-type="bibr" rid="bib1.bibx55" id="paren.76"/>, suggesting that blowing snow has the capacity to
explain the occurrence of ODEs in the polar springtime.</p>
</sec>

      
      </body>
    <back><app-group>
        <supplementary-material position="anchor"><p><bold>The Supplement related to this article is available online at <inline-supplementary-material xlink:href="http://dx.doi.org/10.5194/acp-15-7537-2015-supplement" xlink:title="pdf">doi:10.5194/acp-15-7537-2015-supplement</inline-supplementary-material>.</bold></p></supplementary-material>
        </app-group><ack><title>Acknowledgements</title><p>This research was supported by a National Science Foundation (NSF) Grant
# <inline-formula><mml:math display="inline"><mml:mn>1043145</mml:mn></mml:math></inline-formula>. The authors would like to thank Anthony Faia, Josh Landis,
Dave Ferris, Howard Roscoe, and the two referees for guidance with IC and
insightful suggestions in preparing this manuscript.</p><p><?xmltex \hack{\noindent}?>All data is available online at
<uri>http://engineering.dartmouth.edu/materials/bromide/data.html</uri>.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: R. Sander</p></ack><ref-list>
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