Poisson’s equation
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 is
∇2ϕ(𝐫)=ρ(𝐫) |
where ∇2 is the Laplacian and ρ:D→ℝ, often called a source , is a given function
on some subset D of ℝn. If ρ is identically zero, the Poisson equation
reduces to the Laplace equation.
The Poisson equation is linear, and therefore obeys the superposition principle: if ∇2ϕ1=ρ1 and ∇2ϕ2=ρ2, then ∇2(ϕ1+ϕ2)=ρ1+ρ2. 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 ℝ3, and ϕ(𝐫)→0 as |𝐫|→∞. The general solution is then given by
ϕ(𝐫)=-14π∫ℝ3ρ(𝐫′)|𝐫-𝐫′|d3𝐫′. |
Title | Poisson’s equation |
---|---|
Canonical name | PoissonsEquation |
Date of creation | 2013-03-22 13:38:28 |
Last modified on | 2013-03-22 13:38:28 |
Owner | pbruin (1001) |
Last modified by | pbruin (1001) |
Numerical id | 6 |
Author | pbruin (1001) |
Entry type | Definition |
Classification | msc 35J05 |
Related topic | HelmholtzDifferentialEquation |
Related topic | LaplacesEquation |
Related topic | GreensFunction |