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<record version="1" id="221">
 <title>divergence</title>
 <name>Divergence</name>
 <created>2006-08-28 23:46:39</created>
 <modified>2006-08-28 23:46:39</modified>
 <type>Definition</type>
 <creator id="1" name="bloftin"/>
 <modifier id="1" name="bloftin"/>
 <author id="1" name="bloftin"/>
 <classification>
	<category scheme="msc" code="02."/>
 </classification>
 <synonyms>
	<synonym concept="divergence" alias="divergence of a vector field"/>
 </synonyms>
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	<object name="curl"/>
	<object name="gradient"/>
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 <content>\section{Divergence}

The divergence of a vector field is defined as 


$$\nabla \cdot {\bf V} = \frac{\partial V_x}{\partial x} + \frac{\partial V_y}{\partial y} + \frac{\partial V_z}{\partial z}$$

This is easily seen from the definition of the dot product and that of the \emph{del} operator

$$ \mathbf{A} \cdot \mathbf{B} = A_x B_x + A_y B_y + A_z B_z $$
$$ \nabla = 
\frac{\partial}{\partial x} {\bf \hat{i}} + \frac{\partial}{\partial y}{\bf \hat{j}} + \frac{\partial}{\partial z}{\bf \hat{z}}$$

carrying out the dot product with ${\bf V}$ then gives (1).

\subsection{Physical Meaning}

Building physical intuition about the divergence of a vector field can be gained by considering the flow of a fluid.

\subsection{Coordinate Systems}

Cartesian Coordinates

$$ \nabla \cdot {\bf V} = \frac{\partial V_x}{\partial x} + \frac{\partial V_y}{\partial y} + \frac{\partial V_z}{\partial z}$$

Cylindrical Coordinates

$$\nabla \cdot {\bf V} = \frac{1}{r}\frac{\partial}{\partial r} (r V_r) + \frac{1}{r} \frac{\partial V_{\theta}}{\partial \theta} + \frac{\partial V_z}{\partial z}$$ 

Spherical Coordinates

$$\nabla \cdot {\bf V} = \frac{1}{r^2}\frac{\partial}{\partial r} (r^2 V_r) + \frac{1}{r sin \theta} \frac{\partial}{\partial \theta}(V_{\theta} sin \theta) + \frac{1}{r sin \theta}\frac{\partial V_{\phi}}{\partial \phi}$$</content>
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