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<record version="4" id="3593">
 <title>Laplace equation</title>
 <name>LaplacesEquation</name>
 <created>2002-11-13 06:38:41</created>
 <modified>2006-11-13 22:58:45</modified>
 <type>Definition</type>
 <creator id="13753" name="Mathprof"/>
 <author id="13753" name="Mathprof"/>
 <author id="919" name="giri"/>
 <classification>
	<category scheme="msc" code="26B12"/>
 </classification>
 <defines>
	<concept>harmonic</concept>
 </defines>
 <synonyms>
	<synonym concept="Laplace equation" alias="Laplace differential equation"/>
 </synonyms>
 <related>
	<object name="PoissonsEquation"/>
	<object name="ExampleOfSolvingTheHeatEquation"/>
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 <content>The scalar form of \emph{Laplace's equation} is the partial differential equation $$\vnabla^2f = 0$$ and the vector form is $$\vnabla^2\vA = 0,$$where $\vnabla^2$ is the Laplacian. It is a special case of the Helmholtz differential equation with $k = 0.$

A function $f$ which satisfies Laplace's equation is said to be \emph{harmonic}. Since Laplace's equation is linear, the superposition of any two solutions is also a solution.</content>
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