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<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" article-type="research-article" dtd-version="3.0" xml:lang="en">
<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>
</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-8-1547-2008</article-id>
<title-group>
<article-title>The atmospheric chemistry of sulphuryl fluoride, SO&lt;sub&gt;2&lt;/sub&gt;F&lt;sub&gt;2&lt;/sub&gt;</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Dillon</surname>
<given-names>T. J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Horowitz</surname>
<given-names>A.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Crowley</surname>
<given-names>J. N.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Max Planck Institute for Chemistry, Mainz, Germany</addr-line>
</aff>
<pub-date pub-type="epub">
<day>13</day>
<month>03</month>
<year>2008</year>
</pub-date>
<volume>8</volume>
<issue>6</issue>
<fpage>1547</fpage>
<lpage>1557</lpage>
<permissions>
<license xlink:type="simple">
<license-p>This is an open-access article ditributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.</license-p>
</license>
</permissions>
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<abstract>
<p>The atmospheric chemistry of sulphuryl fluoride, SO&lt;sub&gt;2&lt;/sub&gt;F&lt;sub&gt;2&lt;/sub&gt;, was
investigated in a series of laboratory studies. A competitive rate method,
using pulsed laser photolysis (PLP) to generate O(&lt;sup&gt;1&lt;/sup&gt;D) coupled to
detection of OH by laser induced fluorescence (LIF), was used to determine
the overall rate coefficient for the reaction O(&lt;sup&gt;1&lt;/sup&gt;D) + SO&lt;sub&gt;2&lt;/sub&gt;F&lt;sub&gt;2&lt;/sub&gt; &amp;rarr; products (R1) of &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;1&lt;/sub&gt;
(220&amp;ndash;300 K) = (1.3 &amp;plusmn; 0.2) &amp;times; 10&lt;sup&gt;&amp;minus;10&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt; molecule&lt;sup&gt;&amp;minus;1&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. Monitoring the O(&lt;sup&gt;3&lt;/sup&gt;P)
product (R1a) enabled the contribution (α) of the physical quenching
process (in which SO&lt;sub&gt;2&lt;/sub&gt;F&lt;sub&gt;2&lt;/sub&gt; is not consumed) to be determined as
α (225&amp;ndash;296 K)=(0.55 &amp;plusmn; 0.04). Separate, relative rate
measurements at 298 K provided a rate coefficient for reactive loss of
O(&lt;sup&gt;1&lt;/sup&gt;D), &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;1b&lt;/sub&gt;, of (5.8 &amp;plusmn; 0.8) &amp;times; 10&lt;sup&gt;&amp;minus;11&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt; molecule&lt;sup&gt;&amp;minus;1&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;
in good agreement with the value calculated from
(1&amp;minus;&amp;alpha;) &amp;times; &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;1&lt;/sub&gt;=(5.9 &amp;plusmn; 1.0) &amp;times; 10&lt;sup&gt;&amp;minus;11&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt; molecule&lt;sup&gt;&amp;minus;1&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. Upper limits for the rate coefficients
for reaction of SO&lt;sub&gt;2&lt;/sub&gt;F&lt;sub&gt;2&lt;/sub&gt; with OH (R2, using PLP-LIF), and with
O&lt;sub&gt;3&lt;/sub&gt; (R3, static reactor) were determined as &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;2&lt;/sub&gt; (294 K)&amp;lt;1 &amp;times; 10&lt;sup&gt;&amp;minus;15&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt; molecule&lt;sup&gt;&amp;minus;1&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;
and &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;3&lt;/sub&gt; (294 K)&amp;lt;1 &amp;times; 10&lt;sup&gt;&amp;minus;23&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt; molecule&lt;sup&gt;&amp;minus;1&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;. In experiments using
the wetted-wall flow tube technique, no loss of SO&lt;sub&gt;2&lt;/sub&gt;F&lt;sub&gt;2&lt;/sub&gt; onto aqueous
surfaces was observed, allowing an upper limit for the uptake coefficient of
γ(pH 2&amp;ndash;12)&amp;lt;1 &amp;times; 10&lt;sup&gt;&amp;minus;7&lt;/sup&gt; to be determined. These results
indicate that SO&lt;sub&gt;2&lt;/sub&gt;F&lt;sub&gt;2&lt;/sub&gt; has no significant loss processes in the
troposphere, and a very long stratospheric lifetime. Integrated band
intensities for SO&lt;sub&gt;2&lt;/sub&gt;F&lt;sub&gt;2&lt;/sub&gt; infrared absorption features between 6 and
19 μm were obtained, and indicate a significant global warming
potential for this molecule. In the course of this work, ambient temperature
rate coefficients for the reactions O(&lt;sup&gt;1&lt;/sup&gt;D) with several important
atmospheric species were determined. The results (in units of
10&lt;sup&gt;&amp;minus;10&lt;/sup&gt; cm&lt;sup&gt;3&lt;/sup&gt; molecule&lt;sup&gt;&amp;minus;1&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;,
&lt;i&gt;k&lt;/i&gt;&lt;sub&gt;(O&lt;sup&gt;1&lt;/sup&gt;D + N&lt;sub&gt;2&lt;/sub&gt;)&lt;/sub&gt;=(0.33 &amp;plusmn; 0.06);
&lt;i&gt;k&lt;/i&gt;&lt;sub&gt;(O&lt;sup&gt;1&lt;/sup&gt;D + N&lt;sub&gt;2&lt;/sub&gt;O)&lt;/sub&gt;=(1.47 &amp;plusmn; 0.2) and &lt;i&gt;k&lt;/i&gt;&lt;sub&gt;(O&lt;sup&gt;1&lt;/sup&gt;D + H&lt;sub&gt;2&lt;/sub&gt;O)&lt;/sub&gt;=(1.94 &amp;plusmn; 0.5)
were in good agreement with other recent determinations.</p>
</abstract>
<counts><page-count count="11"/></counts>
</article-meta>
</front>
<body/>
<back>
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</article>