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<record version="7" id="7147">
 <title>Neumann problem</title>
 <name>NeumannProblem</name>
 <created>2005-06-07 22:57:56</created>
 <modified>2006-06-24 03:18:49</modified>
 <type>Definition</type>
 <creator id="9747" name="dczammit"/>
 <author id="2872" name="pahio"/>
 <author id="2192" name="perucho"/>
 <author id="8565" name="Cartan"/>
 <author id="9747" name="dczammit"/>
 <classification>
	<category scheme="msc" code="31A05"/>
	<category scheme="msc" code="31B05"/>
	<category scheme="msc" code="31B15"/>
 </classification>
 <related>
	<object name="HarmonicFunction"/>
 </related>
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 <content>Suppose $\Omega$ is a region of $\sR^n$ and $\partial\Omega$ is the boundary of $\Omega$. 
Further suppose $f$ is a function $f\colon\partial \Omega\to\sC$, and suppose $\frac{\partial}{\partial n}$ corresponds to taking a derivative in a direction normal to the boundary $\partial\Omega$ at any point.  Then the 
\emph{Neumann problem} is to find a function $\phi\colon \Omega\cup \partial \Omega \to\sC$
such that 
\begin{eqnarray*}
\frac{\partial\phi}{\partial n} &amp;=&amp; f,\quad \text{on $\partial \Omega$}, \\
\nabla^2 \phi &amp;=&amp; 0,\quad \text{in $\Omega$}. 
\end{eqnarray*}
Here $\nabla^2$ represents the Laplacian operator and the second condition is that $\phi$ be a harmonic function on $\Omega$. The condition for the existence of a solution $\phi$ of the Neumann problem is that integral of the normal derivative of the function $\phi$, calculated over the entire boundary $\partial\Omega$, vanish. This follows from the identic equation
\begin{align*}
\int_{\partial\Omega}\frac{\partial\phi}{\partial n}d\sigma=
\int_\Omega\nabla\!\cdot\!(\nabla\phi)d\tau=\int_\Omega\nabla^2\phi\,d\tau
\end{align*}
and from the fact that $\nabla^2\phi=0$.
</content>
</record>
