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<article language="en">
	<journal>
		<journal_title>Atmospheric Chemistry and Physics Discussions</journal_title>
		<journal_url>www.atmos-chem-phys-discuss.net</journal_url>
		<issn>1680-7367</issn>
		<eissn>1680-7375</eissn>
		<volume_number>3</volume_number>
		<issue_number>2</issue_number>
		<publication_year>2003</publication_year>
	</journal>
	<doi>10.5194/acpd-3-1949-2003</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/3/1949/2003/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/3/1949/2003/acpd-3-1949-2003.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/3/1949/2003/acpd-3-1949-2003.pdf</fulltext_pdf>
	<start_page>1949</start_page>
	<end_page>1971</end_page>
	<publication_date>2003-04-14</publication_date>
	<article_title content_type="html">Study of the heterogeneous reaction of O&lt;sub&gt;3&lt;/sub&gt; with CH&lt;sub&gt;3&lt;/sub&gt;SCH&lt;sub&gt;3&lt;/sub&gt; using the wetted-wall flowtube technique</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>M. Barcellos da Rosa</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>W. Behnke</name>
		</author>
		<author numeration="3" affiliations="1">
			<name>C. Zetzsch</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Fraunhofer-Institut für Toxikologie und Experimentelle Medizin Nikolai-Fuchs-Str. 1, 30625 Hannover, Germany</affiliation>
	</affiliations>
	<abstract content_type="html">This work presents the heterogeneous kinetics of the reaction of
      CH&lt;sub&gt;3&lt;/sub&gt;SCH&lt;sub&gt;3&lt;/sub&gt; (dimethyl sulphide, DMS) with O&lt;sub&gt;3&lt;/sub&gt; (ozone) in aqueous solution at different ionic strengths (0,
      0.1 and 1.0 M NaCl) using the wetted-wall flowtube (WWFT) technique. Henry&apos;s law
      coefficients of DMS were determined on pure water and on different concentrations of
      NaCl (0.1 M&amp;ndash;4.0 M) in the WWFT from UV spectrophotometric measurements of DMS in the gas phase using a numerical transport model of phase exchange to be  H (M
      atm&lt;sup&gt;&amp;minus;1&lt;/sup&gt;) = 2.16&amp;plusmn;0.5 at 274.4 K, 1.47&amp;plusmn;0.3 at 283.4 K, 0.72&amp;plusmn;0.2 at
      291 K, 0.57&amp;plusmn;0.1 at 303.4 K and 0.33±0.1 at 313.4K on water, on 1.0M NaCl to be H =
      1.57&amp;plusmn;0.4 at 275.7 K, 0.8&amp;plusmn;0.2 at 291 K and on 4.0 M NaCl to be H = 0.44&amp;plusmn;0.1 at
      275.7 K and 0.16±0.04 at 29 K, showing a significant effect of ionic strength,
      mu, on the solubility of DMS according to the equation   ln H  = &amp;minus;4061 T&lt;sup&gt;&amp;minus;1&lt;/sup&gt; + 0.052
      mu&lt;sup&gt;2&lt;/sup&gt; + 50.9 &amp;mu; T&lt;sup&gt;&amp;minus;1&lt;/sup&gt; + 14.0. At concentrations ofDMS&lt;sub&gt;(liq)&lt;/sub&gt; above
      50 &amp;mu; M, UV spectrophotometry of both O&lt;sub&gt;3(gas)&lt;/sub&gt; and DMS&lt;sub&gt;(gas)&lt;/sub&gt; enables us to observe simultaneously the reactive uptake of
      O&lt;sub&gt;3&lt;/sub&gt; on DMS solution and the gas-liquid equilibration of DMS along  the flowtube. The uptake
      coefficient, gamma, of O&lt;sub&gt;3&lt;/sub&gt; on aqueous solutions of DMS, varying between 1 and
      15&amp;times;10&lt;sup&gt;&amp;minus;6&lt;/sup&gt;, showed a square root-dependence on the aqueous DMS concentration (as expected for
      diffusive penetration into the surface film, where the reaction takes place in aqueous
      solution). It was smaller on NaCl solution in accord with the lower solubility of
      O&lt;sub&gt;3&lt;/sub&gt;. The heterogeneous reaction of O&lt;sub&gt;3(gas)&lt;/sub&gt; with DMS&lt;sub&gt;(liq)&lt;/sub&gt; was evaluated from the observations of
      the second order rate constant (k&lt;sup&gt;II&lt;/sup&gt;) for the homogeneous aqueous reaction
      O&lt;sub&gt;3(liq)&lt;/sub&gt; + DMS&lt;sub&gt;(liq)&lt;/sub&gt; using a numerical model of radial diffusion and reactive penetration and
      leading to k&lt;sup&gt;II&lt;/sup&gt; (in units of 10&lt;sup&gt;&amp;minus;8&lt;/sup&gt;M&lt;sup&gt;-1&lt;/sup&gt; s&lt;sup&gt;-1&lt;/sup&gt;) =
      4.1&amp;plusmn;1.2 at 291.0 K, 2.15&amp;plusmn;0.65 at 283.4 K and 1.8&amp;plusmn;0.5 at 274.4 K. Aside from the expected influence on solubility and aqueous-phase
      diffusion coefficient of both gases there was no significant  effect of ionic strength on
      k&lt;sup&gt;II&lt;/sup&gt;, that was determined for 0.1M NaCl, leading to k&lt;sup&gt;II&lt;/sup&gt;
      (10&lt;sup&gt;8&lt;/sup&gt;M&lt;sup&gt;-1&lt;/sup&gt; s&lt;sup&gt;-1&lt;/sup&gt;) = 3.2&amp;plusmn;1.0 at 288 K, 1.7&amp;plusmn;0.5 at
      282 K and 1.3&amp;plusmn;0.4 at 276 K, and for 1.0 M NaCl, leading to 3.2&amp;plusmn;1.0 at 288 K,
      1.3&amp;plusmn;0.4 at 282 K and 1.2&amp;plusmn;0.4 at 276 K, where the error limits include uncertainties of
      Henry&apos;s law constants and diffusion coefficients for DMS and O&lt;sub&gt;3&lt;/sub&gt;.</abstract>
	<references>
	</references>
</article>

