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Neumann problem (Definition)

Suppose $ \Omega$ is a region of $ \mathbb{R}^n$ and $ \partial\Omega$ is the boundary of $ \Omega$. Further suppose $ f$ is a function $ f\colon\partial \Omega\to\mathbb{C}$, 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 Neumann problem is to find a function $ \phi\colon \Omega\cup \partial \Omega \to\mathbb{C}$ such that

$\displaystyle \frac{\partial\phi}{\partial n}$ $\displaystyle =$ $\displaystyle f,$   on $ \partial \Omega$$\displaystyle ,$  
$\displaystyle \nabla^2 \phi$ $\displaystyle =$ $\displaystyle 0,$   in $ \Omega$$\displaystyle .$  

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
$\displaystyle \int_{\partial\Omega}\frac{\partial\phi}{\partial n}d\sigma= \int_\Omega\nabla\!\cdot\!(\nabla\phi)d\tau=\int_\Omega\nabla^2\phi\,d\tau$    

and from the fact that $ \nabla^2\phi=0$.



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See Also: harmonic function

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Cross-references: identic equation, vanish, entire, integral, solution, harmonic function, operator, Laplacian, represents, point, normal, derivative, function, boundary, region
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This is version 7 of Neumann problem, born on 2005-06-07, modified 2006-06-24.
Object id is 7147, canonical name is NeumannProblem.
Accessed 3390 times total.

Classification:
AMS MSC31A05 (Potential theory :: Two-dimensional theory :: Harmonic, subharmonic, superharmonic functions)
 31B05 (Potential theory :: Higher-dimensional theory :: Harmonic, subharmonic, superharmonic functions)
 31B15 (Potential theory :: Higher-dimensional theory :: Potentials and capacities, extremal length)

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