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<article language="en">
	<journal>
		<journal_title>Ocean Science</journal_title>
		<journal_url>www.ocean-sci.net</journal_url>
		<issn>1812-0784</issn>
		<eissn>1812-0792</eissn>
		<volume_number>5</volume_number>
		<issue_number>3</issue_number>
		<publication_year>2009</publication_year>
	</journal>
	<doi>10.5194/os-5-271-2009</doi>
	<article_url>http://www.ocean-sci.net/5/271/2009/</article_url>
	<abstract_html>http://www.ocean-sci.net/5/271/2009/os-5-271-2009.html</abstract_html>
	<fulltext_pdf>http://www.ocean-sci.net/5/271/2009/os-5-271-2009.pdf</fulltext_pdf>
	<start_page>271</start_page>
	<end_page>283</end_page>
	<publication_date>2009-07-20</publication_date>
	<article_title content_type="html">Understanding mixing efficiency in the oceans: do the nonlinearities of the equation of state for seawater matter?</article_title>
	<authors>
		<author numeration="1" affiliations="1">
			<name>R. Tailleux</name>
			<email>r.g.j.tailleux@reading.ac.uk</email>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Department of Meteorology, University of Reading, UK</affiliation>
	</affiliations>
	<abstract content_type="html">There exist two central measures of turbulent mixing in
turbulent stratified fluids that are both caused by molecular diffusion:
1) the dissipation rate &lt;i&gt;D&lt;/i&gt;(APE) of available potential energy APE;
2) the turbulent rate of change &lt;i&gt;W&lt;/i&gt;&lt;sub&gt;&lt;i&gt;r&lt;/i&gt;, turbulent&lt;/sub&gt; of background gravitational
potential energy GPE&lt;sub&gt;&lt;i&gt;r&lt;/i&gt;&lt;/sub&gt;. So far, these two quantities have often been
regarded as the same energy conversion, namely the irreversible conversion
of APE into GPE&lt;sub&gt;&lt;i&gt;r&lt;/i&gt;&lt;/sub&gt;, owing to the well known exact equality &lt;i&gt;D&lt;/i&gt;(APE)=&lt;i&gt;W&lt;/i&gt;&lt;sub&gt;&lt;i&gt;r&lt;/i&gt;, turbulent&lt;/sub&gt;
for a Boussinesq fluid with a linear equation of state.
Recently, however, Tailleux (2009) pointed out that the above equality
no longer holds for a thermally-stratified compressible, with the ratio
&amp;xi;=&lt;i&gt;W&lt;/i&gt;&lt;sub&gt;&lt;i&gt;r&lt;/i&gt;, turbulent&lt;/sub&gt;/&lt;i&gt;D&lt;/i&gt;(APE) being generally lower than unity
and sometimes even negative for water or seawater, and argued that &lt;i&gt;D&lt;/i&gt;(APE)
and &lt;i&gt;W&lt;/i&gt;&lt;sub&gt;&lt;i&gt;r&lt;/i&gt;, turbulent&lt;/sub&gt; actually represent two distinct types of energy
conversion, respectively the dissipation of APE into one particular subcomponent
of internal energy called the &quot;dead&quot; internal energy IE&lt;sub&gt;0&lt;/sub&gt;, and the conversion
between GPE&lt;sub&gt;&lt;i&gt;r&lt;/i&gt;&lt;/sub&gt; and a different subcomponent of internal energy called
&quot;exergy&quot; IE&lt;sub&gt;exergy&lt;/sub&gt;. In this paper, the behaviour of the
ratio ξ is examined
for different stratifications having all the same buoyancy frequency
&lt;i&gt;N&lt;/i&gt; vertical profile, but different vertical profiles of the parameter
&amp;Upsilon;=&amp;alpha; &lt;i&gt;P&lt;/i&gt;/(&amp;rho;&lt;i&gt;C&lt;sub&gt;p&lt;/sub&gt;&lt;/i&gt;),
where α is the thermal expansion coefficient, &lt;i&gt;P&lt;/i&gt; the
hydrostatic pressure, &amp;rho; the density, and &lt;i&gt;C&lt;sub&gt;p&lt;/sub&gt;&lt;/i&gt; the specific heat capacity
at constant pressure, the equation
of state being that for seawater for different particular constant values of salinity.
It is found that ξ and &lt;i&gt;W&lt;/i&gt;&lt;sub&gt;&lt;i&gt;r&lt;/i&gt;, turbulent&lt;/sub&gt; depend critically on the sign
and magnitude of &lt;i&gt;d&lt;/i&gt;&amp;Upsilon;/&lt;i&gt;dz&lt;/i&gt;, in contrast with &lt;i&gt;D&lt;/i&gt;(APE), which appears largely
unaffected by the latter. These results have important consequences for how
the mixing efficiency should be defined and measured in practice, which are
discussed.</abstract>
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</article>

