Solenoidal vector field

From Wikipedia, the free encyclopedia

In vector calculus a solenoidal vector field is a vector field v with divergence zero:

\nabla \cdot \mathbf{v} = 0.\,

This condition is satisfied whenever v has a vector potential, because if

\mathbf{v} = \nabla \times \mathbf{A}

then

\nabla \cdot \mathbf{v} = \nabla \cdot (\nabla \times \mathbf{A}) = 0.

The converse also holds: for any solenoidal v there exists a vector potential A such that \mathbf{v} = \nabla \times \mathbf{A}. (Strictly speaking, this holds only subject to certain technical conditions on v, see Helmholtz decomposition.)

[edit] Examples

This mathematical analysis-related article is a stub. You can help Wikipedia by expanding it.
In other languages