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Poisson's equation (Definition)

Poisson's equation is a second-order partial differential equation which arises in physical problems such as finding the electric potential of a given charge distribution. Its general form in $ n$ dimensions is

$\displaystyle \nabla^2\phi(\mathbf r)=\rho(\mathbf r) $
where $ \nabla^2$ is the Laplacian and $ \rho:D\to\mathbb{R}$, often called a source function, is a given function on some subset $ D$ of $ \mathbb{R}^n$. If $ \rho$ is identically zero, the Poisson equation reduces to the Laplace equation.

The Poisson equation is linear, and therefore obeys the superposition principle: if $ \nabla^2\phi_1=\rho_1$ and $ \nabla^2\phi_2=\rho_2$, then $ \nabla^2(\phi_1+\phi_2)=\rho_1+\rho_2$. This fact can be used to construct solutions to Poisson's equation from fundamental solutions, or Green's functions, where the source distribution is a delta function.

A very important case is the one in which $ n=3$, $ D$ is all of $ \mathbb{R}^3$, and $ \phi(\mathbf r)\to 0$ as $ \vert\mathbf r\vert\to\infty$. The general solution is then given by

$\displaystyle \phi(\mathbf r)=-\frac{1}{4\pi}\int_{\mathbb{R}^3}\frac{\rho(\mathbf{r'})}{\vert\mathbf{r}-\mathbf{r'}\vert}\mathrm{d}^3\mathbf{r'}. $



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See Also: Helmholtz equation, Laplace equation, Green's function

Keywords:  partial differential equation
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Cross-references: general solution, delta function, Green's functions, solutions, Laplace equation, subset, function, Laplacian, potential, partial differential equation, second-order
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This is version 3 of Poisson's equation, born on 2003-05-22, modified 2004-02-27.
Object id is 4291, canonical name is PoissonsEquation.
Accessed 15521 times total.

Classification:
AMS MSC35J05 (Partial differential equations :: Partial differential equations of elliptic type :: Laplace equation, reduced wave equation , Poisson equation)

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