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<!DOCTYPE article SYSTEM "http://www.atmos-chem-phys.net/inc/acp/copernicus.dtd">
<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>6</volume_number>
		<issue_number>5</issue_number>
		<publication_year>2006</publication_year>
	</journal>
	<doi>10.5194/acp-6-1425-2006</doi>
	<article_url>http://www.atmos-chem-phys.net/6/1425/2006/</article_url>
	<abstract_html>http://www.atmos-chem-phys.net/6/1425/2006/acp-6-1425-2006.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys.net/6/1425/2006/acp-6-1425-2006.pdf</fulltext_pdf>
	<start_page>1425</start_page>
	<end_page>1434</end_page>
	<publication_date>2006-05-04</publication_date>
	<article_title content_type="html">A modelling study of the impact of cirrus clouds on the moisture budget of the upper troposphere</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>S. Fueglistaler</name>
		</author>
		<author numeration="2" affiliations="1">
			<name>M. B. Baker</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">University of Washington, Seattle, USA</affiliation>
	</affiliations>
	<abstract content_type="html">We present a modelling study of the effect of cirrus
  clouds
  on the moisture budget of the layer wherein the cloud formed.
  Our framework simplifies
  many aspects of cloud microphysics and collapses the problem
  of sedimentation onto
  a 0-dimensional box model, but retains essential feedbacks between
  saturation mixing ratio, particle growth, and water removal
  through particle sedimentation. The water budget is
  described by two coupled first-order differential equations for
  dimensionless particle number density
  and saturation point temperature,
  where the parameters defining the system
  (layer depth, reference temperature, amplitude and time scale
  of temperature perturbation
  and inital particle number density, which may or may not
  be a function of reference temperature and cooling rate)
  are encapsulated in a single coefficient.
  This allows us to scale the results to a broad range of
  atmospheric conditions, and to test sensitivities.
  Results of the moisture budget calculations
  are presented for a range of
  atmospheric conditions
  (&lt;i&gt;T&lt;/i&gt;: 238&amp;ndash;205 K; &lt;i&gt;p&lt;/i&gt;: 325&amp;ndash;180 hPa) and
  a range of time scales &amp;tau;&lt;sub&gt;T&lt;/sub&gt; of the temperature perturbation that
  induces the cloud formation.
  The cirrus clouds are found to efficiently
  remove water for
  &amp;tau;&lt;sub&gt;T&lt;/sub&gt; longer than a few hours,
  with longer perturbations (&amp;tau;&lt;sub&gt;T&lt;/sub&gt;&amp;#x2273;10 h)
  required at lower temperatures (&lt;i&gt;T&lt;/i&gt;&amp;#x2272;210 K).
  Conversely, we find that temperature
  perturbations of duration order 1 h and less (a typical timescale
  for e.g., gravity waves) do not
  efficiently dehydrate over most of the upper troposphere.
  A consequence is that (for particle densities typical
  of current cirrus clouds) the assumption of complete
  dehydration to the saturation mixing ratio may yield
  valid predictions for upper tropospheric moisture
  distributions if it is based on the large scale
  temperature field, but this assumption is not necessarily
  valid if it is based on smaller scale temperature fields.</abstract>
	<references>
	</references>
</article>

