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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>
<abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys.</abbrev-journal-title>
</journal-title-group>
<issn pub-type="epub">1680-7324</issn>
<publisher><publisher-name>Copernicus Publications</publisher-name>
<publisher-loc>Göttingen, Germany</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.5194/acp-13-7813-2013</article-id>
<title-group>
<article-title>The roles of vertical advection and eddy diffusion in the equatorial mesospheric semi-annual oscillation (MSAO)</article-title>
</title-group>
<contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gattinger</surname>
<given-names>R. 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>Kyrölä</surname>
<given-names>E.</given-names>
<ext-link>https://orcid.org/0000-0001-9197-9549</ext-link>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Boone</surname>
<given-names>C. D.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Evans</surname>
<given-names>W. F. J.</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Walker</surname>
<given-names>K. A.</given-names>
<ext-link>https://orcid.org/0000-0003-3420-9454</ext-link>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<xref ref-type="aff" rid="aff6">
<sup>6</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>McDade</surname>
<given-names>I. C.</given-names>
</name>
<xref ref-type="aff" rid="aff7">
<sup>7</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Bernath</surname>
<given-names>P. F.</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<xref ref-type="aff" rid="aff8">
<sup>8</sup>
</xref>
</contrib>
<contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Llewellyn</surname>
<given-names>E. J.</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
</contrib>
</contrib-group><aff id="aff1">
<label>1</label>
<addr-line>ISAS, Department of Physics and Engineering Physics, 116 Science Place, University of Saskatchewan, Saskatoon SK, S7N 5E2, Canada</addr-line>
</aff>
<aff id="aff2">
<label>2</label>
<addr-line>Finnish Meteorological Institute, Earth Observation, P.O. Box 503, 00101, Helsinki, Finland</addr-line>
</aff>
<aff id="aff3">
<label>3</label>
<addr-line>Department of Chemistry, University of Waterloo, Waterloo, ON, N2L 3G1, Canada</addr-line>
</aff>
<aff id="aff4">
<label>4</label>
<addr-line>NorthWest Research Associates Inc., 4118 148 Avenue N.E., Redmond, WA 98052, USA</addr-line>
</aff>
<aff id="aff5">
<label>5</label>
<addr-line>Centre for Research in Earth and Space Science (CRESS), York University, 4700 Keele Street, Toronto, ON, M3J 1P3, Canada</addr-line>
</aff>
<aff id="aff6">
<label>6</label>
<addr-line>Department of Physics, University of Toronto, 60 St. George Street, Toronto, ON, M5S 1A7, Canada</addr-line>
</aff>
<aff id="aff7">
<label>7</label>
<addr-line>Department of Earth and Space Science and Engineering (ESSE), York University, 4700 Keele Street, Toronto, ON, M3J 1P3, Canada</addr-line>
</aff>
<aff id="aff8">
<label>8</label>
<addr-line>Department of Chemistry and Biochemistry, Old Dominion University, 4541 Hampton Boulevard, Norfolk, Virginia 23529-0126, USA</addr-line>
</aff>
<pub-date pub-type="epub">
<day>14</day>
<month>08</month>
<year>2013</year>
</pub-date>
<volume>13</volume>
<issue>15</issue>
<fpage>7813</fpage>
<lpage>7824</lpage>
<permissions>
<copyright-statement>Copyright: &#x000a9; 2013 R. L. Gattinger et al.</copyright-statement>
<copyright-year>2013</copyright-year>
<license license-type="open-access">
<license-p>This work is licensed under the Creative Commons Attribution 3.0 Unported License. To view a copy of this licence, visit <ext-link ext-link-type="uri"  xlink:href="https://creativecommons.org/licenses/by/3.0/">https://creativecommons.org/licenses/by/3.0/</ext-link></license-p>
</license>
</permissions>
<self-uri xlink:href="https://acp.copernicus.org/articles/13/7813/2013/acp-13-7813-2013.html">This article is available from https://acp.copernicus.org/articles/13/7813/2013/acp-13-7813-2013.html</self-uri>
<self-uri xlink:href="https://acp.copernicus.org/articles/13/7813/2013/acp-13-7813-2013.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/13/7813/2013/acp-13-7813-2013.pdf</self-uri>
<abstract>
<p>Observations of the mesospheric semi-annual oscillation (MSAO) in the
equatorial region have been reported dating back several decades. Seasonal
variations in both species densities and airglow emissions are well
documented. The extensive observations available offer an excellent case
study for comparison with model simulations. A broad range of MSAO
measurements is summarised with emphasis on the 80–100 km region. The
objective here is not to address directly the complicated driving forces of
the MSAO, but rather to employ a combination of observations and model
simulations to estimate the limits of some of the underlying dynamical
processes. Photochemical model simulations are included for near-equinox and
near-solstice conditions, the two times with notable differences in the
observed MSAO parameters. Diurnal tides are incorporated in the model to
facilitate comparisons of observations made at different local times. The
roles of water vapour as the &quot;driver&quot; species and ozone as the &quot;response&quot;
species are examined to test for consistency between the model results and
observations. The simulations suggest the interactions between vertical eddy
diffusion and background vertical advection play a significant role in the
MSAO phenomenon. Further, the simulations imply there are rigid limits on
vertical advection rates and eddy diffusion rates. For August at the Equator,
90 km altitude, the derived eddy diffusion rate is approximately
1 × 10&lt;sup&gt;6&lt;/sup&gt; cm&lt;sup&gt;2&lt;/sup&gt; s&lt;sup&gt;−1&lt;/sup&gt; and the vertical advection is
upwards at 0.8 cm s&lt;sup&gt;−1&lt;/sup&gt;. For April the corresponding values are
4 × 10&lt;sup&gt;5&lt;/sup&gt; cm&lt;sup&gt;2&lt;/sup&gt; s&lt;sup&gt;−1&lt;/sup&gt; and 0.1 cm s&lt;sup&gt;−1&lt;/sup&gt;. These results
from the current 1-D model simulations will need to be verified by a full 3-D
simulation. Exactly how vertical advection and eddy diffusion are related to
gravity wave momentum as discussed by Dunkerton (1982) three decades ago
remains to be addressed.</p>
</abstract>
<counts><page-count count="12"/></counts>
</article-meta>
</front>
<body/>
<back>
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