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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-4-1869-2004</article-id>
<title-group>
<article-title>Implementing growth and sedimentation of NAT particles in a global Eulerian model</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>van den Broek</surname>
<given-names>M. M. 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>Williams</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>Bregman</surname>
<given-names>A.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>Space Research Organization of the Netherlands (SRON), Utrecht, The Netherlands</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Eindhoven University, Eindhoven, The Netherlands</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Royal Netherlands Meteorological Institute (KNMI), De Bilt, The Netherlands</addr-line>
</aff>
<pub-date pub-type="epub">
<day>14</day>
<month>09</month>
<year>2004</year>
</pub-date>
<volume>4</volume>
<issue>7</issue>
<fpage>1869</fpage>
<lpage>1883</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.net/4/1869/2004/acp-4-1869-2004.pdf">The full text article is available as a PDF file from http://www.atmos-chem-phys.net/4/1869/2004/acp-4-1869-2004.pdf</self-uri>
<abstract>
<p>Here we present a concise and efficient algorithm to mimic the growth and
sedimentation of Nitric Acid Trihydate (NAT) particles in the polar vortex
in a state-of-the-art 3D chemistry transport model. The particle growth and
sedimentation are calculated using the microphysical formulation of Carslaw
et al.&amp;nbsp;(2002). Once formed, NAT particles are transported in the model as
tracers in the form of size-segregated quantities or size bins. Two different approaches
were adopted for this purpose: one assuming a fixed particle number density
(&quot;FixedDens&quot;) and the other assuming a discrete set of particle diameter
values (&quot;FixedRad&quot;). Simulations were performed for three separate 10-day
periods during the 1999-2000 Arctic winter and compared to the results of an
existing Lagrangian model study, which uses similar microphysics in a
computationally more expensive method for the simulation of NAT particle
growth. The resulting particle sizes for both our approaches compare favourably at 430K with
those obtained from this previous model study, and also in-situ observations related
to the size of large NAT particles. The particle growth is faster for &quot;FixedDens&quot; resulting in
a difference in (de)nitrification by a factor of ~2 for all three simulation periods.
Comparisons were made with a standard equilibrium approach
and the differences in the redistribution of HNO&lt;sub&gt;3&lt;/sub&gt; were found to be substantial. For both
approaches the performance of the algorithm is rather insensitive to both
the number of size bins and the shape of the size distribution, and show a weak dependence on the
prescribed total particle number density during the coldest period. This results in an increase of
 7% for the &quot;FixedRad&quot; approach and 17% for the &quot;FixedDens&quot; approach when increasing the total particle
 number density by a factor of 2.5.</p>
</abstract>
<counts><page-count count="15"/></counts>
</article-meta>
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