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<!DOCTYPE article SYSTEM "http://www.atmos-chem-phys-discuss.net/inc/acpd/copernicus.dtd">
<article language="en">
	<journal>
		<journal_title>Atmospheric Chemistry and Physics Discussions</journal_title>
		<journal_url>www.atmos-chem-phys-discuss.net</journal_url>
		<issn>1680-7367</issn>
		<eissn>1680-7375</eissn>
		<volume_number>4</volume_number>
		<issue_number>1</issue_number>
		<publication_year>2004</publication_year>
	</journal>
	<doi>10.5194/acpd-4-39-2004</doi>
	<article_url>http://www.atmos-chem-phys-discuss.net/4/39/2004/</article_url>
	<abstract_html>http://www.atmos-chem-phys-discuss.net/4/39/2004/acpd-4-39-2004.html</abstract_html>
	<fulltext_pdf>http://www.atmos-chem-phys-discuss.net/4/39/2004/acpd-4-39-2004.pdf</fulltext_pdf>
	<start_page>39</start_page>
	<end_page>69</end_page>
	<publication_date>2004-01-06</publication_date>
	<article_title content_type="html">A new time-resolved model of the mesospheric Na layer: constraints on the meteor input function</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>J. M. C. Plane</name>
			<email>j.plane@uea.ac.uk</email>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">School of Environmental Sciences, University of East Anglia, Norwich, UK</affiliation>
	</affiliations>
	<abstract content_type="html">A time-resolved model of the Na layer in the mesosphere/lower thermosphere region is
      described, where the continuity equations for the major sodium species Na,
      Na&lt;sup&gt;+&lt;/sup&gt; and NaHCO&lt;sub&gt;3&lt;/sub&gt; are solved explicity, and the other short-lived species are treated in steady-state.  It is shown
      that the diurnal variation of the Na layer can only be modelled satisfactorily if sodium species
      are permanently removed below about 85 km, both through the dimerization of
      NaHCO&lt;sub&gt;3&lt;/sub&gt; and the uptake of sodium species on meteoric smoke particles that are assumed to have formed
      from the recondensation of vaporized meteoroids. When the sensitivity of the Na layer to the
      meteoroid input function is considered, an inconsistent picture emerges.  The ratio of the
      column abundances of Na&lt;sup&gt;+&lt;/sup&gt; to Na is shown to increase strongly with the average meteoroid
      velocity, because the Na is injected at higher altitudes.  Comparison with a limited set of
      Na&lt;sup&gt;+&lt;/sup&gt; measurements indicates that the average meteoroid velocity is probably less than about
      25 km s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;, in agreement with velocity estimates from conventional meteor radars, and considerably
      slower than recent observations made by wide aperture incoherent scatter radars.  The Na
      column abundance is shown to be very sensitive to the meteoroid mass input rate, and to the
      rate of vertical transport by eddy diffusion.  Although the magnitude of the eddy diffusion
      coefficient in the 80&amp;ndash;90 km region is uncertain, there is a consensus between recent models
      using parameterisations of gravity wave momentum deposition that the average value is less
      than 3&amp;times;10&lt;sup&gt;5 &lt;/sup&gt;cm&lt;sup&gt;2&lt;/sup&gt; s&lt;sup&gt;&amp;minus;1&lt;/sup&gt;.  This requires that the global meteoric mass input rate is less than about
      20 t d&lt;sup&gt;&amp;minus;1&lt;/sup&gt;, which is closest to estimates from incoherent scatter radar observations.  Finally, the
      diurnal variation in the meteoroid input rate only slight perturbs the Na layer, because the
      residence time of Na in the layer is several days, and diurnal effects are effectively averaged
      out.</abstract>
	<references>
	</references>
</article>

