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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">ACP</journal-id>
<journal-title-group>
<journal-title>Atmospheric Chemistry and Physics</journal-title>
<abbrev-journal-title abbrev-type="publisher">ACP</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7324</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/acp-3-909-2003</article-id>
<title-group>
<article-title>A novel model to predict the physical state of atmospheric H&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt;/NH&lt;sub&gt;3&lt;/sub&gt;/H&lt;sub&gt;2&lt;/sub&gt;O aerosol particles</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Colberg</surname>
<given-names>C. 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>Luo</surname>
<given-names>B. P.</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>Wernli</surname>
<given-names>H.</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>Koop</surname>
<given-names>T.</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>Peter</surname>
<given-names>Th.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Institute for Atmospheric and Climate Science, Swiss Federal Institute of Technology, Zürich, Switzerland</addr-line>
</aff>
<pub-date pub-type="epub">
<day>02</day>
<month>07</month>
<year>2003</year>
</pub-date>
<volume>3</volume>
<issue>4</issue>
<fpage>909</fpage>
<lpage>924</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>
<self-uri xlink:href="http://www.atmos-chem-phys.net/3/909/2003/acp-3-909-2003.html">This article is available from http://www.atmos-chem-phys.net/3/909/2003/acp-3-909-2003.html</self-uri>
<self-uri xlink:href="http://www.atmos-chem-phys.net/3/909/2003/acp-3-909-2003.pdf">The full text article is available as a PDF file from http://www.atmos-chem-phys.net/3/909/2003/acp-3-909-2003.pdf</self-uri>
<abstract>
<p>The physical state of the tropospheric aerosol is largely unknown
      despite its importance for cloud formation and for the aerosol&apos;s radiative properties. Here we use detailed microphysical
      laboratory measurements to perform a systematic global modelling study of the physical state of the
      H&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt;/NH&lt;sub&gt;3&lt;/sub&gt;/H&lt;sub&gt;2&lt;/sub&gt;O aerosol, which constitutes an
      important class of aerosols in the free troposphere. The Aerosol Physical State Model (APSM) developed here is based on Lagrangian
      trajectories computed from ECMWF (European Centre for Medium Range Weather Forecasts) analyses, taking full account of the
      deliquescence/efflorescence hysteresis. As input APSM requires three data sets: (i) deliquescence and efflorescence relative
      humidities from laboratory measurements, (ii) ammonia-to-sulfate ratios (ASR) calculated by a global circulation model, and (iii)
      relative humidities determined from the ECMWF analyses. APSM results indicate that globally averaged a significant fraction
      (17-57%) of the ammoniated sulfate aerosol particles contain solids with the ratio of solid-containing to purely liquid
      particles increasing with altitude (between 2 and 10 km). In our calculations the most abundant solid is
      letovicite, (NH&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;3&lt;/sub&gt;H(SO&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;, while there is only little
      ammonium sulfate, (NH&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt;. Since ammonium
      bisulfate, NH&lt;sub&gt;4&lt;/sub&gt;HSO&lt;sub&gt;4&lt;/sub&gt;, does not nucleate homogeneously, it
      can only form via heterogeneous crystallization. As the ammonia-to-sulfate ratios of the atmospheric
      H&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt;/NH&lt;sub&gt;3&lt;/sub&gt;/H&lt;sub&gt;2&lt;/sub&gt;O aerosol usually do not
      correspond to the stoichiometries of known crystalline substances, all solids are expected to occur in mixed-phase aerosol particles.
      This work highlights the potential importance of letovicite, whose role as cloud condensation nucleus (CCN) and as scatterer of solar
      radiation remains to be scrutinized.</p>
</abstract>
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