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		<id>https://en.formulasearchengine.com/w/index.php?title=Fragmentation_(computing)&amp;diff=12684</id>
		<title>Fragmentation (computing)</title>
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		<updated>2014-01-27T07:58:56Z</updated>

		<summary type="html">&lt;p&gt;173.75.247.232: Numerous additions, clarifications, and a few corrections.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;In [[fluid statics]], &#039;&#039;&#039;capillary pressure&#039;&#039;&#039; is the difference in [[pressure]] across the interface between two [[immiscible]] fluids, and thus defined as&lt;br /&gt;
:&amp;lt;math&amp;gt;p_c=p_{\text{non-wetting phase}}-p_{\text{wetting phase}}&amp;lt;/math&amp;gt;&lt;br /&gt;
In oil-water systems, water is typically the [[wetting]] phase, while for gas-oil systems, oil is typically the wetting phase.  &lt;br /&gt;
&lt;br /&gt;
The [[Young–Laplace equation]] states that this pressure difference is proportional to the [[interfacial tension]], &amp;lt;math&amp;gt;\gamma&amp;lt;/math&amp;gt;, and inversely proportional to the effective radius, &amp;lt;math&amp;gt;r&amp;lt;/math&amp;gt;, of the interface, it also depends on the [[contact angle|wetting angle]], &amp;lt;math&amp;gt;\theta&amp;lt;/math&amp;gt;, of the liquid on the surface of the capillary.&lt;br /&gt;
:&amp;lt;math&amp;gt;p_c=\frac{2\gamma \cos \theta}{r}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The equation for capillary pressure is only valid under capillary equilibrium, which means that there can not be any flowing phases.&lt;br /&gt;
&lt;br /&gt;
== In porous media==&lt;br /&gt;
In [[porous media]], capillary pressure is the force necessary to squeeze a hydrocarbon droplet through a pore throat (works against the interfacial tension  between oil and water phases) and is higher for smaller pore diameter. The expression for the capillary pressure remains as before, &#039;&#039;i.e.,&#039;&#039; &lt;br /&gt;
&amp;lt;math&amp;gt;p_c=p_{\text{non-wetting phase}}-p_{\text{wetting phase.}}&amp;lt;/math&amp;gt;&lt;br /&gt;
However, the quantities &amp;lt;math&amp;gt;p_c&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;p_{\text{non-wetting phase}}&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;p_{\text{wetting phase}}&amp;lt;/math&amp;gt; are quantities that are obtained by averaging these quantities within the pore space of porous media either statistically or using the volume averaging method.&amp;lt;ref&amp;gt;Jacob Bear: “Dynamics of Fluids in Porous Media,” Dover Publications, 1972.&amp;lt;/ref&amp;gt;  &lt;br /&gt;
&lt;br /&gt;
The Brooks-Corey correlation&amp;lt;ref&amp;gt;Brooks, R.H. and Corey, A.T.: “Hydraulic properties of porous&lt;br /&gt;
 media,” Hydraulic paper no. 3, Colorado State University, 1964.&amp;lt;/ref&amp;gt; for capillary pressure reads&lt;br /&gt;
:&amp;lt;math&amp;gt;p_c = cS_w^{-a}&amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;c&amp;lt;/math&amp;gt; is the entry capillary pressure, &amp;lt;math&amp;gt;1/a&amp;lt;/math&amp;gt; is the pore-size distribution index and &amp;lt;math&amp;gt;S_w&amp;lt;/math&amp;gt; is the normalized water saturation (see [[Relative permeability]])&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Capillary action]]&lt;br /&gt;
* [[Capillary number]]&lt;br /&gt;
* [[Disjoining pressure]]&lt;br /&gt;
* [[Leverett J-function]]&lt;br /&gt;
* [[Young–Laplace equation]]&lt;br /&gt;
* [[Amott test]]&lt;br /&gt;
* [[Laplace pressure]]&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
* Kim Kinoshita, Electrochemical Oxygen Technology p139, John Wiley &amp;amp; Sons, Inc. 1992.&lt;br /&gt;
* [http://www.articleworld.org/index.php/Capillary_pressure Capillary pressure equations]&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Fluid dynamics]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{fluiddynamics-stub}}&lt;/div&gt;</summary>
		<author><name>173.75.247.232</name></author>
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