<?xml version="1.0" encoding="utf-8" standalone="no"?>
<!DOCTYPE article SYSTEM "http://www.atmos-chem-phys-discuss.net/inc/acpd/copernicus.dtd">
<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>4</issue_number>
		<publication_year>2003</publication_year>
	</journal>
	<doi>10.5194/acpd-3-3991-2003</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/3/3991/2003/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/3/3991/2003/acpd-3-3991-2003.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/3/3991/2003/acpd-3-3991-2003.pdf</fulltext_pdf>
	<start_page>3991</start_page>
	<end_page>4036</end_page>
	<publication_date>2003-07-28</publication_date>
	<article_title content_type="html">The isotope composition of water vapour: A powerful tool to study transport and chemistry of middle atmospheric water vapour</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>C. Bechtel</name>
		</author>
		<author numeration="2" affiliations="2">
			<name>A. Zahn</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Institut für Umweltphysik, University of Heidelberg, Heidelberg, Germany</affiliation>
		<affiliation numeration="2" content_type="html">Institute of Meteorology and Climate Research, Forschungszentrum Karlsruhe, Germany</affiliation>
	</affiliations>
	<abstract content_type="html">A one-dimensional chemistry model is applied to study the stable hydrogen (D) and stable
      oxygen isotope (&lt;sup&gt;17&lt;/sup&gt;O, &lt;sup&gt;18&lt;/sup&gt;O) composition of water vapour in stratosphere and
      mesosphere. The stable isotope ratios of tropospheric H&lt;sub&gt;2&lt;/sub&gt;O are determined by
      &amp;quot;physical&apos;&apos; fractionation effects, i.e. phase changes, diffusion processes, and mixing of air
      masses. Due to these processes water vapour entering the stratosphere (i) is
      mass-dependently fractionated (MDF), i.e. shifts in the isotope ratio &lt;sup&gt;17&lt;/sup&gt;O/&lt;sup&gt;16&lt;/sup&gt;O
      are ~0.52 times of those of &lt;sup&gt;18&lt;/sup&gt;O/&lt;sup&gt;16&lt;/sup&gt;O and (ii) shows isotope shifts in D/H,
      which are ~5 times of those in &lt;sup&gt;18&lt;/sup&gt;O/&lt;sup&gt;16&lt;/sup&gt;O. In stratosphere and mesosphere
      &amp;quot;chemical&apos;&apos; fractionation, that are the oxidation of methane, re-cycling of
      H&lt;sub&gt;2&lt;/sub&gt;O via the HO&lt;sub&gt;x&lt;/sub&gt; family, and isotope exchange reactions are shown to considerably enhance
      the isotope ratios in the imported tropospheric H&lt;sub&gt;2&lt;/sub&gt;O. Enrichments relative to the
      isotope ratios at the tropopause are used to derive the partitioning of tropospheric
      (unmodified), re-cycled and in situ generated H&lt;sub&gt;2&lt;/sub&gt;O. The model reasonably predicts
      overall increases of the stable isotope ratios in H&lt;sub&gt;2&lt;/sub&gt;O by ~23% for D/H,
      ~8.5% for &lt;sup&gt;17&lt;/sup&gt;O/&lt;sup&gt;16&lt;/sup&gt;O, and ~14% for &lt;sup&gt;18&lt;/sup&gt;O/&lt;sup&gt;16&lt;/sup&gt;O. The&lt;sup&gt;17&lt;/sup&gt;O/&lt;sup&gt;16&lt;/sup&gt;O and
      &lt;sup&gt;18&lt;/sup&gt;O/&lt;sup&gt;16&lt;/sup&gt;O ratios in H&lt;sub&gt;2&lt;/sub&gt;O are shown to be a measure of the partitioning of
      HO&lt;sub&gt;x&lt;/sub&gt; that receives its O atom either from the reservoirs O&lt;sub&gt;2&lt;/sub&gt; or
      O&lt;sub&gt;3&lt;/sub&gt;. In the entire middle atmosphere, MDF O&lt;sub&gt;2&lt;/sub&gt; is the major donator of oxygen atoms incorporated in
      OH and HO&lt;sub&gt;2&lt;/sub&gt; and thus in H&lt;sub&gt;2&lt;/sub&gt;O. It is demonstrated that in the stratosphere mass-independent fractionation
      (MIF) in O&lt;sub&gt;3&lt;/sub&gt; in a first step is transferred to the NO&lt;sub&gt;x&lt;/sub&gt; family and only in a
      second step to HO&lt;sub&gt;x&lt;/sub&gt; and H&lt;sub&gt;2&lt;/sub&gt;O. In contrast to CO&lt;sub&gt;2&lt;/sub&gt;,
      O(&lt;sup&gt;1&lt;/sup&gt;D) only plays a minor role in this MIF transfer. The major uncertainty in our calculation arises from the many
      badly quantified isotope exchange reactions and kinetic isotope fractionation factors.</abstract>
	<references>
	</references>
</article>

