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<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>GÃ¶ttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/acpd-11-24813-2011</article-id>
<title-group>
<article-title>Aerosol hygroscopic growth parameterization based on a solute specific coefficient</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Metzger</surname>
<given-names>S.</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>Steil</surname>
<given-names>B.</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>Xu</surname>
<given-names>L.</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>Penner</surname>
<given-names>J. E.</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>Lelieveld</surname>
<given-names>J.</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-group><aff id="aff1">
<label>1</label>
<addr-line>Max Planck Institute for Chemistry, Mainz, Germany</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>University of Michigan, Ann Arbor, Michigan, USA</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>The Cyprus Institute, Nicosia, Cyprus</addr-line>
</aff>
<pub-date pub-type="epub">
<day>05</day>
<month>09</month>
<year>2011</year>
</pub-date>
<volume>11</volume>
<issue>9</issue>
<fpage>24813</fpage>
<lpage>24855</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/11/24813/2011/acpd-11-24813-2011.pdf">The full text article is available as a PDF file from http://www.atmos-chem-phys-discuss.net/11/24813/2011/acpd-11-24813-2011.pdf</self-uri>
<abstract>
<p>Water is a main component of atmospheric aerosols and its amount depends on
the particle chemical composition. We introduce a new parameterization for
the aerosol hygroscopic growth factor (HGF), based on an empirical relation
between water activity (&lt;i&gt;a&lt;/i&gt;&lt;sub&gt;w&lt;/sub&gt;) and solute molality (&amp;mu;&lt;sub&gt;s&lt;/sub&gt;) through a
single solute specific coefficient &amp;nu;&lt;sub&gt;i&lt;/sub&gt;. Three main advantages are: (1)
wide applicability, (2) simplicity and (3) analytical nature. (1) Our
approach considers the Kelvin effect and covers ideal solutions at large
relative humidity (RH), including CCN activation, as well as concentrated
solutions with high ionic strength at low RH such as the relative humidity of
deliquescence (RHD). (2) A single &amp;nu;&lt;sub&gt;i&lt;/sub&gt; coefficient suffices to
parameterize the HGF for a wide range of particle sizes, from nanometer
nucleation mode to micrometer coarse mode particles. (3) In contrast to
previous methods, our analytical &lt;i&gt;a&lt;/i&gt;&lt;sub&gt;w&lt;/sub&gt; parameterization depends not only
on a linear correction factor for the solute molality, instead &amp;nu;&lt;sub&gt;i&lt;/sub&gt; also
appears in the exponent in form &lt;i&gt;x&lt;/i&gt; Â· &lt;i&gt;a&lt;/i&gt;&lt;sup&gt;x&lt;/sup&gt;. According to our findings,
&amp;nu;&lt;sub&gt;i&lt;/sub&gt; can be assumed constant for the entire &lt;i&gt;a&lt;/i&gt;&lt;sub&gt;w&lt;/sub&gt; range (0â€“1). Thus,
the &amp;nu;&lt;sub&gt;i&lt;/sub&gt; based method is computationally efficient. In this work we
focus on single solute solutions, where &amp;nu;&lt;sub&gt;i&lt;/sub&gt; is pre-determined with the
bisection method from our analytical equations using RHD measurements and the
saturation molality &amp;mu;&lt;sub&gt;s&lt;/sub&gt;&lt;sup&gt;sat&lt;/sup&gt;. The computed aerosol HGF and
supersaturation (KÃ¶hler-theory) compare well with the results of the
thermodynamic reference model E-AIM for the key compounds NaCl and
(NH&lt;sub&gt;4&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;SO&lt;sub&gt;4&lt;/sub&gt; relevant for CCN modeling and calibration studies.
The equations introduced here provide the basis of our revised
gas-liquid-solid partitioning model, i.e. version 4 of the EQuilibrium
Simplified Aerosol Model (EQSAM4), described in a companion paper.</p>
</abstract>
<counts><page-count count="43"/></counts>
</article-meta>
</front>
<body/>
<back>
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