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		<title>Quasi-geostrophic equations - Revision history</title>
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		<updated>2026-04-04T21:14:32Z</updated>
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		<id>http://www.wiki.mohid.com/index.php?title=Quasi-geostrophic_equations&amp;diff=796&amp;oldid=prev</id>
		<title>Guillaume: 1 revision</title>
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				<updated>2008-12-03T10:39:02Z</updated>
		
		<summary type="html">&lt;p&gt;1 revision&lt;/p&gt;
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		<author><name>Guillaume</name></author>	</entry>

	<entry>
		<id>http://www.wiki.mohid.com/index.php?title=Quasi-geostrophic_equations&amp;diff=795&amp;oldid=prev</id>
		<title>192.168.20.111 at 17:36, 11 February 2007</title>
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				<updated>2007-02-11T17:36:35Z</updated>
		
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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;Geostrophic &lt;br /&gt;
ow means a stationary &lt;br /&gt;
ow where the Coriolis force is balanced&lt;br /&gt;
by the pressure gradient. This has several implications&lt;br /&gt;
* the flow is stationary,&lt;br /&gt;
* any flow that satisfies the geostrophic momentum equations also satisfies exactly the continuity equation,&lt;br /&gt;
* the horizontal flow is vertically independent,&lt;br /&gt;
* no divergent or convergent flow is allowed.&lt;br /&gt;
Consider the horizontal momentum equations for an inviscid &lt;br /&gt;
uid under the ''beta'' plane approximation. &lt;br /&gt;
Also, the flow is nearly geostrophic, but not quite,&lt;br /&gt;
so we will consider the full equations&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{D\,u}{Dt} - f\,v = -\frac{1}{\rho}\frac{\partial p}{\partial x}&amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>192.168.20.111</name></author>	</entry>

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