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<record version="26" id="100">
 <title>Laplacian in Spherical Coordinates</title>
 <name>LaplacianInSphericalCoordinates</name>
 <created>2005-12-30 20:39:07</created>
 <modified>2025-07-05 22:36:30</modified>
 <type>Definition</type>
 <creator id="1" name="bloftin"/>
 <modifier id="1" name="bloftin"/>
 <author id="1" name="bloftin"/>
 <classification>
	<category scheme="msc" code="02.40.Dr"/>
 </classification>
 <related>
	<object name="LaplacianInCylindricalCoordinates"/>
	<object name="LaplacianInCartesianCoordinates"/>
	<object name="Laplacian"/>
 </related>
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 <content>The Laplacian operator in spherical coordinates is 
\begin{equation}
\nabla _{sph}^{2} = \frac{1}{r^2} \frac{\partial}{\partial r}\left(r^2 \frac{\partial}{\partial r}\right) + \frac{1}{r^2 sin\theta} \frac{\partial}{\partial \theta} \left( sin \theta \frac{\partial}{\partial \theta}\right) + \frac{1}{r^2 sin^2 \theta} \frac{\partial^2}{\partial \phi^2}
\end{equation}

The derivation is fairly straight forward and begins with locating a vector {\bf r} in spherical coordinates as shown in the figure.

\begin{figure}
\includegraphics{SphericalCoordinates.eps}
\end{figure}</content>
</record>
