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<article language="en">
	<journal>
		<journal_title>Atmospheric Chemistry and Physics</journal_title>
		<journal_url>www.atmos-chem-phys.net</journal_url>
		<issn>1680-7316</issn>
		<eissn>1680-7324</eissn>
		<volume_number>1</volume_number>
		<issue_number>1</issue_number>
		<publication_year>2001</publication_year>
	</journal>
	<doi>10.5194/acp-1-73-2001</doi>
	<article_url>http://www.atmos-chem-phys.net/1/73/2001/</article_url>
	<abstract_html>http://www.atmos-chem-phys.net/1/73/2001/acp-1-73-2001.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys.net/1/73/2001/acp-1-73-2001.pdf</fulltext_pdf>
	<start_page>73</start_page>
	<end_page>78</end_page>
	<publication_date>2001-12-28</publication_date>
	<article_title content_type="html">Oxidation of SO&lt;sub&gt;2&lt;/sub&gt; by H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt; on ice surfaces at 228 K: a sink for SO&lt;sub&gt;2&lt;/sub&gt; in ice clouds</article_title>
	<authors>
		<author numeration="1" affiliations="1,2">
			<name>S. M. Clegg</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>J. P. D. Abbatt</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Department of Chemistry, University of Toronto, 80 St. George St., Toronto, M5S 3H6 Ontario, Canada</affiliation>
		<affiliation numeration="2" content_type="html">now at: Combustion Research Facility, Sandia National Laboratory, Livermore, CA 94551-0969, USA</affiliation>
	</affiliations>
	<abstract content_type="html">The heterogeneous reaction
      SO&lt;sub&gt;2&lt;/sub&gt; + H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt; &lt;img border=&quot;0&quot; src=&quot;http://www.atmos-chem-phys.net/1/73/2001//img/rarrow.gif&quot; width=&quot;24&quot; height=&quot;9&quot;&gt;&amp;nbsp;
      H&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt; on ice at
      228 K has been studied in a low temperature coated-wall flow tube.  With H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt; in excess of
      SO&lt;sub&gt;2&lt;/sub&gt;, the loss of SO&lt;sub&gt;2&lt;/sub&gt; on an ice surface is time dependent with the reaction most efficient on a freshly exposed surface. The deactivation of the
      surface arises because the protons formed in the reaction inhibit the dissociation of adsorbed
      SO&lt;sub&gt;2&lt;/sub&gt;.  This lowers the surface concentrations of HSO&lt;sub&gt;3&lt;/sub&gt;&lt;sup&gt;-&lt;/sup&gt;, a participant in the rate-determining step of the oxidation
      mechanism. For a fixed SO&lt;sub&gt;2&lt;/sub&gt; partial pressure of 1.4 x 10&lt;sup&gt;-4&lt;/sup&gt;
      Pa, the reaction probabilities for SO&lt;sub&gt;2&lt;/sub&gt; loss on a freshly exposed surface scale linearly with
      H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt; partial pressures between 2.7 x 10&lt;sup&gt;-3&lt;/sup&gt; and 2.7
      x 10&lt;sup&gt;-2&lt;/sup&gt; Pa because the H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt; surface coverage is unsaturated in this regime. Conversely, the reaction probabilities
      decrease as the partial pressure of SO&lt;sub&gt;2&lt;/sub&gt; is raised from 2.7 x 10&lt;sup&gt;-5&lt;/sup&gt; to 1.3
      x 10&lt;sup&gt;-3&lt;/sup&gt; Pa, for a fixed H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt; partial pressure of 8.7
      x 10&lt;sup&gt;-3 &lt;/sup&gt;Pa. This is expected if the rate determining step for the mechanism involves
      HSO&lt;sub&gt;3&lt;/sub&gt;&lt;sup&gt;-&lt;/sup&gt; rather than SO&lt;sub&gt;2&lt;/sub&gt;.  It may also arise to some degree if there is competition between gas phase
      SO&lt;sub&gt;2&lt;/sub&gt; and H&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;2&lt;/sub&gt; for adsorption sites. The reaction is sufficiently fast that the lifetime of
      SO&lt;sub&gt;2&lt;/sub&gt; within ice clouds could be controlled by this heterogeneous reaction and not by the gas-phase reaction with OH.</abstract>
	<references>
	</references>
</article>

