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<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" article-type="research-article" dtd-version="3.0" xml:lang="en">
<front>
<journal-meta>
<journal-id journal-id-type="publisher">ACPD</journal-id>
<journal-title-group>
<journal-title>Atmospheric Chemistry and Physics Discussions</journal-title>
<abbrev-journal-title abbrev-type="publisher">ACPD</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7375</issn>
<publisher><publisher-name>Copernicus GmbH</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/acpd-4-753-2004</article-id>
<title-group>
<article-title>Explicit simulation of aerosol physics in a cloud-resolving model</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ekman</surname>
<given-names>A. M. L.</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>Wang</surname>
<given-names>C.</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>Wilson</surname>
<given-names>J.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ström</surname>
<given-names>J.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Massachusetts Institute of Technology, Cambridge, Massachusetts, USA</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Institute for Environment and Sustainability, European Commission, Ispra, Italy</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Institute of Applied Environmental Research, Stockholm University, Stockholm, Sweden</addr-line>
</aff>
<pub-date pub-type="epub">
<day>02</day>
<month>02</month>
<year>2004</year>
</pub-date>
<volume>4</volume>
<issue>1</issue>
<fpage>753</fpage>
<lpage>803</lpage>
<permissions>
<license xlink:type="simple">
<license-p>This is an open-access article ditributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.</license-p>
</license>
</permissions>
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<self-uri xlink:href="http://www.atmos-chem-phys-discuss.net/4/753/2004/acpd-4-753-2004.pdf">The full text article is available as a PDF file from http://www.atmos-chem-phys-discuss.net/4/753/2004/acpd-4-753-2004.pdf</self-uri>
<abstract>
<p>The role of convection in introducing aerosols and promoting the formation
      of new particles to the upper troposphere has been examined using a cloud-resolving model coupled with an 
interactive explicit aerosol module. A
      baseline simulation suggests good agreement in the upper troposphere between modeled and observed
 results including concentrations of aerosols in
      different size ranges, mole fractions of key chemical species, and concentrations of ice particles. In addition, a set of 34 sensitivity
      simulations has been carried out to investigate the sensitivity of modeled
      results to the treatment of various aerosol physical and chemical processes
      in the model. The size distribution of aerosols is proved to be an important
      factor in determining the aerosols&apos; fate within the convective cloud. Nucleation mode aerosols
      (0&amp;lt;&amp;minus;d&amp;lt;&amp;minus;5.84 nm) are quickly transferred to the larger modes as they grow through coagulation and condensation of
      H&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt;. Accumulation mode aerosols (d&amp;gt;&amp;minus;31.0 nm) are almost
      completely removed by nucleation (activation of cloud droplets) and impact
      scavenging. However, a substantial part (up to 10% of the boundary layer concentration) of the Aitken mode aerosol population
      (5.84 nm&amp;lt;&amp;minus;d&amp;lt;&amp;minus;31.0 nm) reaches the top of the cloud and the free troposphere. These
      particles may continually survive in the upper troposphere, or over time form ice crystals, both that could impact the atmospheric radiative budget.
      The sensitivity simulations performed indicate that critical processes in the model causing a substantial change in the upper 
tropospheric Aitken mode
      number concentration are coagulation, condensation, nucleation scavenging,
      nucleation of aerosols and the transfer of aerosol mass and number between
      different aerosol bins. In particular, for aerosols in the Aitken mode to grow to CCN size, coagulation appears to be more important than
      condensation. Less important processes are dry deposition, impact scavenging
      and the initial vertical distribution and concentration of aerosols. It is
      interesting to note that in order to sustain a vigorous storm cloud, the supply of CCN must be continuous over a 
considerably long time period of the
      simulation. Hence, the treatment of the growth of particles is in general much more important than the initial aerosol concentration itself.</p>
</abstract>
<counts><page-count count="51"/></counts>
</article-meta>
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