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Stokes operator : ウィキペディア英語版
Stokes operator

The Stokes operator, named after George Gabriel Stokes, is an unbounded linear operator used in the theory of partial differential equations, specifically in the fields of fluid dynamics and electromagnetics.
==Definition==

If we define P_\sigma as the Leray-Helmholtz projector onto divergence free vector fields, then the Stokes Operator A is defined by
:A:=-P_\sigma\triangle,
where \triangle\equiv\nabla^2 is the Laplacian. Since A is unbounded, we must also give its domain of definition, which is defined as \mathcal(A)=H^2\cap V, where V=\\,\vec=0\}. Here, \Omega is a bounded open set in \mathbb^n (usually ''n'' = 2 or 3), H^2(\Omega) and H^1_0(\Omega) are the standard Sobolev spaces, and the divergence of \vec is taken in the distribution sense.

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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