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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-3-1131-2003</article-id>
<title-group>
<article-title>The rate of water vapor evaporation from ice substrates in the presence of HCl and HBr: implications for the lifetime of atmospheric ice particles</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Delval</surname>
<given-names>C.</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>Fluckiger</surname>
<given-names>B.</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>Rossi</surname>
<given-names>M. J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Laboratory of Air and Soil Pollution Studies (LPAS), Swiss Federal Institute of Technology (EPFL), CH-1015 Lausanne, Switzerland</addr-line>
</aff>
<pub-date pub-type="epub">
<day>01</day>
<month>08</month>
<year>2003</year>
</pub-date>
<volume>3</volume>
<issue>4</issue>
<fpage>1131</fpage>
<lpage>1145</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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<self-uri xlink:href="http://www.atmos-chem-phys.net/3/1131/2003/acp-3-1131-2003.pdf">The full text article is available as a PDF file from http://www.atmos-chem-phys.net/3/1131/2003/acp-3-1131-2003.pdf</self-uri>
<abstract>
<p>Using a
      multidiagnostic approach the rate Rev [ molec cm&lt;sup&gt;-3&lt;/sup&gt; s&lt;sup&gt;-1&lt;/sup&gt;]
      or flux J&lt;sub&gt;ev&lt;/sub&gt; [ molec cm&lt;sup&gt;-2&lt;/sup&gt; s&lt;sup&gt;-1&lt;/sup&gt;] of
      evaporation of H&lt;sub&gt;2&lt;/sub&gt;O and its corresponding rate constant for
      condensation, k&lt;sub&gt;cond&lt;/sub&gt; [s&lt;sup&gt;-1&lt;/sup&gt; ], on a 1 µm thick ice
      film have been studied in the temperature range 190 to 240 K as well as in
      the presence of small amounts of HCl and HBr that left the vapor pressure
      of H&lt;sub&gt;2&lt;/sub&gt;O on ice unchanged. The resulting Arrhenius expressions
      for pure ice are J&lt;sub&gt;ev&lt;/sub&gt; = 1.6 · 10 &lt;sup&gt;28 ± 1&lt;/sup&gt; ·
      exp&amp;nbsp; (- 10.3 ± 1.2/ RT)&amp;nbsp; [ molec cm&lt;sup&gt;-2&lt;/sup&gt; s&lt;sup&gt;-1&lt;/sup&gt;]
      , k&lt;sub&gt;cond&lt;/sub&gt; = 1.7 · 10 &lt;sup&gt;- 2 ± 1&lt;/sup&gt; · exp&amp;nbsp; (+ 1.6 ±
      1.5/ RT ) [s &lt;sup&gt;-1&lt;/sup&gt;], in the presence of a HCl mole fraction in the
      range 3.2 · 10 &lt;sup&gt;- 5&lt;/sup&gt; - 6.4 · 10 &lt;sup&gt;- 3&lt;/sup&gt; : J&lt;sub&gt;ev&lt;/sub&gt;
      = 6.4 · 10 &lt;sup&gt;26 ± 1&lt;/sup&gt; · exp&amp;nbsp; (- 9.7 ± 1.2/ RT)&amp;nbsp; [
      molec cm&lt;sup&gt;-2&lt;/sup&gt; s&lt;sup&gt;-1&lt;/sup&gt;] , k&lt;sub&gt;cond&lt;/sub&gt; = 2.8 · 10 &lt;sup&gt;-
      2 ± 1&lt;/sup&gt; · exp ( + 1.5 ± 1.6 /RT)&amp;nbsp; [s &lt;sup&gt;-1&lt;/sup&gt;], and a HBr
      mole fraction smaller than 6.4 · 10 &lt;sup&gt;- 3&lt;/sup&gt; : J&lt;sub&gt;ev&lt;/sub&gt; = 7.4
      · 10 &lt;sup&gt;25 ± 1&lt;/sup&gt; · exp ( - 9.1 ± 1.2 /RT)&amp;nbsp; [ molec cm&lt;sup&gt;-2&lt;/sup&gt;
      s&lt;sup&gt;-1&lt;/sup&gt;] , k&lt;sub&gt;cond&lt;/sub&gt; = 7.1 · 10 &lt;sup&gt;- 5 ± 1&lt;/sup&gt; · exp
      (+ 2.6 ± 1.5/ RT) [s &lt;sup&gt;-1&lt;/sup&gt;]. The small negative activation energy
      for H&lt;sub&gt;2&lt;/sub&gt;O condensation on ice points to a precursor mechanism.
      The corresponding enthalpy of sublimation is &lt;font face=&quot;Symbol&quot;&gt;D&lt;/font&gt;H&lt;sub&gt;subl&lt;/sub&gt;
      = E&lt;sub&gt;ev&lt;/sub&gt; - E&lt;sub&gt;cond&lt;/sub&gt; = 11.9 ± 2.7 kcal mol&lt;sup&gt;-1&lt;/sup&gt; , &lt;font face=&quot;Symbol&quot;&gt;D&lt;/font&gt;H&lt;sub&gt;subl&lt;/sub&gt;
      = 11.2 ± 2.8 kcal mol&lt;sup&gt;-1&lt;/sup&gt;, and &lt;font face=&quot;Symbol&quot;&gt;D&lt;/font&gt;H&lt;sub&gt;subl&lt;/sub&gt;
      = 11.7 ± 2.8 kcal mol&lt;sup&gt;-1&lt;/sup&gt; whose values are identical within
      experimental uncertainty to the accepted literature value of 12.3 kcal mol&lt;sup&gt;-1&lt;/sup&gt;
      . Interferometric data at 633 nm and FTIR absorption spectra in
      transmission support the kinetic results. The data are consistent with a
      significant lifetime enhancement for HCl- and HBr-contaminated ice
      particles by a factor of 3–6 and 10–20, respectively, for submonolayer
      coverages of HX once the fraction of the ice not contaminated by HX has
      evaporated.</p>
</abstract>
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