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<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>
<abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7324</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/acp-9-1289-2009</article-id>
<title-group>
<article-title>Turbulent dispersion in cloud-topped boundary layers</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Verzijlbergh</surname>
<given-names>R. A.</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>Jonker</surname>
<given-names>H. J. J.</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>Heus</surname>
<given-names>T.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Vilà-Guerau de Arellano</surname>
<given-names>J.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Department of Multi-Scale Physics, Delft University of Technology, Delft, The Netherlands</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Meteorology and Air Quality Section, Wageningen University, The Netherlands</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>current affiliation: Royal Netherlands Meteorological Institute, De Bilt, The Netherlands</addr-line>
</aff>
<pub-date pub-type="epub">
<day>18</day>
<month>02</month>
<year>2009</year>
</pub-date>
<volume>9</volume>
<issue>4</issue>
<fpage>1289</fpage>
<lpage>1302</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2009 R. A. Verzijlbergh et al.</copyright-statement>
<copyright-year>2009</copyright-year>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri"  xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions>
<self-uri xlink:href="https://acp.copernicus.org/articles/9/1289/2009/acp-9-1289-2009.html">This article is available from https://acp.copernicus.org/articles/9/1289/2009/acp-9-1289-2009.html</self-uri>
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<abstract>
<p>Compared to dry boundary layers, dispersion in cloud-topped boundary layers
has received less attention. In this LES based numerical study we investigate
the dispersion of a passive tracer in the form of Lagrangian particles for
four kinds of atmospheric boundary layers: 1) a dry convective boundary layer
(for reference), 2) a &quot;smoke&quot; cloud boundary layer in which the turbulence
is driven by radiative cooling, 3) a stratocumulus topped boundary layer and
4) a shallow cumulus topped boundary layer.

&lt;br&gt;&lt;br&gt;
We show that the dispersion characteristics of the smoke cloud boundary layer
as well as the stratocumulus situation can be well understood by borrowing
concepts from previous studies of dispersion in the dry convective boundary
layer. A general result is that the presence of clouds enhances mixing and
dispersion – a notion that is not always reflected well in traditional
parameterization models, in which clouds usually suppress dispersion by
diminishing solar irradiance.

&lt;br&gt;&lt;br&gt;
The dispersion characteristics of a cumulus cloud layer turn out to be
markedly different from the other three cases and the results can not be
explained by only considering the well-known top-hat velocity distribution.
To understand the surprising characteristics in the shallow cumulus layer,
this case has been examined in more detail by 1) determining the velocity
distribution conditioned on the distance to the nearest cloud and 2)
accounting for the wavelike behaviour associated with the stratified dry
environment.</p>
</abstract>
<counts><page-count count="14"/></counts>
</article-meta>
</front>
<body/>
<back>
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</article>