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solenoidal vector field : ウィキペディア英語版
solenoidal vector field
In vector calculus a solenoidal vector field (also known as an incompressible vector field or a divergence free vector field ) is a vector field v with divergence zero at all points in the field:
: \nabla \cdot \mathbf = 0.\,
==Properties==
The fundamental theorem of vector calculus states that any vector field can be expressed as the sum of an irrotational and a solenoidal field. The condition of zero divergence is satisfied whenever a vector field v has only a vector potential component, because the definition of the vector potential A as:
:\mathbf = \nabla \times \mathbf
automatically results in the identity (as can be shown, for example, using Cartesian coordinates):
:\nabla \cdot \mathbf = \nabla \cdot (\nabla \times \mathbf) = 0.
The converse also holds: for any solenoidal v there exists a vector potential A such that \mathbf = \nabla \times \mathbf. (Strictly speaking, this holds only subject to certain technical conditions on v, see Helmholtz decomposition.)
The divergence theorem gives the equivalent integral definition of a solenoidal field; namely that for any closed surface, the net total flux through the surface must be zero:
:
where d\mathbf is the outward normal to each surface element.

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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