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Green's second identity : ウィキペディア英語版
Green's identities

In mathematics, Green's identities are a set of three identities in vector calculus. They are named after the mathematician George Green, who discovered Green's theorem.
==Green's first identity==
This identity is derived from the divergence theorem applied to the vector field : Let and be scalar functions defined on some region , and suppose that is twice continuously differentiable, and is once continuously differentiable. Then
: \int_U \left( \psi \Delta \varphi + \nabla \psi \cdot \nabla \varphi \right)\, dV = \oint_ \psi \left( \nabla \varphi \cdot \bold \right)\, dS=\oint_\psi\nabla\varphi\cdot d\mathbf
where \Delta is the Laplace operator, is the boundary of region , is the outward pointing unit normal of surface element and is the oriented surface element. This theorem is a special case of the divergence theorem, and is essentially the higher dimensional equivalent of integration by parts with and the gradient of replacing and .
Note that Green's first identity above is a special case of the more general identity derived from the divergence theorem by substituting :
: \int_U \left( \psi \nabla \cdot \mathbf + \mathbf \cdot \nabla \psi\right)\, dV = \oint_ \psi \left( \mathbf \cdot \bold \right)\, dS=\oint_\psi\mathbf\cdot d\mathbf.

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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