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Solenoidal vector field: Difference between revisions

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'''A''' such that <math>\mathbf{v} = \nabla \times \mathbf{A}</math>. (Strictly, this holds only subject to certain technical conditions on '''v'''.)
'''A''' such that <math>\mathbf{v} = \nabla \times \mathbf{A}</math>. (Strictly, this holds only subject to certain technical conditions on '''v'''.)


Examples:
==Examples==

* one of [[Maxwell's equations]] states that the [[magnetic field]] '''B''' is solenoidal;
* one of [[Maxwell's equations]] states that the [[magnetic field]] '''B''' is solenoidal;
* the [[velocity]] field of an [[incompressible fluid flow]] is solenoidal.
* the [[velocity]] field of an [[incompressible fluid flow]] is solenoidal.


A word of caution:
This is the "layman's" proof. The del operator (or nabla) cannot be crossed or dotted with any other vector (strictly speaking) because it is not a real vector. It is an imaginary scalar quantity which corresponds to a mathematical operation.
{{Mathanalysis-stub}}
{{Mathanalysis-stub}}

[[it:Campo vettoriale solenoidale]]


[[Category:Vector calculus]]
[[Category:Vector calculus]]
[[Category:Fluid dynamics]]
[[Category:Fluid dynamics]]

[[it:Campo vettoriale solenoidale]]

Revision as of 22:20, 13 November 2005

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

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

then

The converse holds: for any solenoidal v there exists a vector potential A such that . (Strictly, this holds only subject to certain technical conditions on v.)

Examples