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<record version="3" id="193">
 <title>Reynolds' Transport Theorem</title>
 <name>ReynoldsTransportTheorem</name>
 <created>2006-07-05 12:34:49</created>
 <modified>2006-07-06 15:23:55</modified>
 <type>Theorem</type>
 <creator id="141" name="PhysBrain"/>
 <modifier id="141" name="PhysBrain"/>
 <comment>Changes for correction #29 ('capitalization, extra article').</comment>
 <author id="141" name="PhysBrain"/>
 <classification>
	<category scheme="msc" code="51.10.+y"/>
	<category scheme="msc" code="47.10.+g"/>
 </classification>
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 <content>Let $F(\mathbf{r},t)$ represent the amount of some physical property of a continuous material medium per unit volume.  The total amount of this property present in a finite region ${\cal V}$ of the material is obtained through the volume integral.
\[
\int_{\cal V} F(\mathbf{r},t) \;dV
\]

If this property is being transported by the action of the flow of the material with a velocity $\mathbf{u}(\mathbf{r},t)$, then the \emph{Reynolds' transport theorem} states that the rate of change of the total amount of $F$ within the material volume is equal to the volume integral of the instantaneous changes of $F$ occuring within the volume, plus the surface integral of the rate at which $F$ is being transported through the surface ${\cal S}$ (bounding ${\cal V}$) to and from the surrounding region.
\[
\frac{d}{d t} \int_{\cal V} F(\mathbf{r},t) \;dV = 
\int_{\cal V} \frac{\partial F}{\partial t} \;dV +
\int_{\cal S} F\mathbf{u} \cdot \mathbf{n} \;dS
\]
Here, $\mathbf{n}$ is a unit vector indicating the normal direction of the surface (oriented to point out of the volume).</content>
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