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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>
</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-9-4315-2009</article-id>
<title-group>
<article-title>Summertime impact of convective transport and lightning NO&lt;sub&gt;x&lt;/sub&gt; production over North America: modeling dependence on meteorological simulations</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhao</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>Wang</surname>
<given-names>Y.</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>Choi</surname>
<given-names>Y.</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>Zeng</surname>
<given-names>T.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>School of Earth and Atmospheric Sciences, Georgia Institute of Technology, Atlanta, GA, USA</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Jet Propulsion Laboratory, Pasadena, CA, USA</addr-line>
</aff>
<pub-date pub-type="epub">
<day>03</day>
<month>07</month>
<year>2009</year>
</pub-date>
<volume>9</volume>
<issue>13</issue>
<fpage>4315</fpage>
<lpage>4327</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/9/4315/2009/acp-9-4315-2009.html">This article is available from http://www.atmos-chem-phys.net/9/4315/2009/acp-9-4315-2009.html</self-uri>
<self-uri xlink:href="http://www.atmos-chem-phys.net/9/4315/2009/acp-9-4315-2009.pdf">The full text article is available as a PDF file from http://www.atmos-chem-phys.net/9/4315/2009/acp-9-4315-2009.pdf</self-uri>
<abstract>
<p>Global-scale chemical transport model simulations
indicate lightning NO&lt;sub&gt;x&lt;/sub&gt; dominates upper tropospheric O&lt;sub&gt;3&lt;/sub&gt; production
above Eastern North America during summertime but vary in their estimates.
To improve our understanding, a regional-scale model (REAM) with higher
resolution is applied. To examine the uncertainties in modeling the impact
of convective transport and lightning NO&lt;sub&gt;x&lt;/sub&gt; production on upper
tropospheric chemical tracer distributions, REAM simulations of chemical
tracers are driven by two meteorological models, WRF and MM5, with different
cumulus convective parameterizations. The model simulations are evaluated
using INTEX-A aircraft measurements and satellite measurements of NO&lt;sub&gt;2&lt;/sub&gt;
columns and cloud top pressure, and we find that mid and upper tropospheric
trace gas concentrations are affected strongly by convection and lightning
NO&lt;sub&gt;x&lt;/sub&gt; production. WRF with the KF-eta convection scheme simulates larger
convective updraft mass fluxes below 150 hPa than MM5 with the Grell scheme.
The inclusion of the entrainment and detrainment processes leads to more
outflow in the mid troposphere in WRF than MM5. The ratio of
C&lt;sub&gt;2&lt;/sub&gt;H&lt;sub&gt;6&lt;/sub&gt;/C&lt;sub&gt;3&lt;/sub&gt;H&lt;sub&gt;8&lt;/sub&gt; is found to be a sensitive parameter to
convective outflow; the simulation by WRF-REAM is in closer agreement with
INTEX-A measurements than MM5-REAM, implying that convective mass fluxes by
WRF are more realistic. WRF also simulates lower cloud top heights (10–12 km)
than MM5 (up to 16 km), and hence smaller amounts of estimated
(intra-cloud) lightning NO&lt;sub&gt;x&lt;/sub&gt; and lower emission altitudes. WRF simulated
cloud top heights are in better agreement with GOES satellite measurements
than MM5. Simulated lightning NO&lt;sub&gt;x&lt;/sub&gt; production difference (due primarily
to cloud top height difference) is mostly above 12 km. At 8–12 km, the
models simulate a contribution of 60–75% of NO&lt;sub&gt;x&lt;/sub&gt; and up to 20 ppbv of
O&lt;sub&gt;3&lt;/sub&gt; from lightning, although the decrease of lightning NO&lt;sub&gt;x&lt;/sub&gt; effect
from the Southeast to Northeast and eastern Canada is overestimated. The
model differences and biases found in this study reflect some major
uncertainties of upper tropospheric NO&lt;sub&gt;x&lt;/sub&gt; and O&lt;sub&gt;3&lt;/sub&gt; simulations driven
by those in meteorological simulations and lightning parameterizations.</p>
</abstract>
<counts><page-count count="13"/></counts>
</article-meta>
</front>
<body/>
<back>
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