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Dirichlet principle : ウィキペディア英語版
Dirichlet's principle

In mathematics, and particularly in potential theory, Dirichlet's principle is the assumption that the minimizer of a certain energy functional is a solution to Poisson's equation.
==Formal statement==
Dirichlet's principle states that, if the function u ( x ) is the solution to Poisson's equation
:\Delta u + f = 0\,
on a domain \Omega of \mathbb^n with boundary condition
:u=g\text\partial\Omega,\,
then ''u'' can be obtained as the minimizer of the Dirichlet's energy
:E() = \int_\Omega \left(\frac|\nabla v|^2 - vf\right)\,\mathrmx
amongst all twice differentiable functions v such that v=g on \partial\Omega (provided that there exists at least one function making the Dirichlet's integral finite). This concept is named after the German mathematician Peter Gustav Lejeune Dirichlet.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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