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Divergenceless Field


A divergenceless field, also called a solenoidal field, is a vector field for which del ·F=0. A sufficiently smooth divergenceless field can locally be written as F=del xG, where G is a vector potential.

Fix an origin, let r be the position vector from it, and write r=|r|. On a spherical shell centered at this origin, a sufficiently smooth divergenceless field satisfying int_(|r|=rho)F·da=0 for each sphere in the spherical shell can be written as

F=del x(Tr)+del x[del x(Sr)]
(1)
=T+S,
(2)

where T and S are scalar functions and

T=del x(Tr)
(3)
=-rx(del T)
(4)
S=del x[del x(Sr)]
(5)
=del [partial/(partialr)(rS)]-rdel ^2S.
(6)

The components T and S are called the toroidal field and poloidal field, respectively (Backus 1986). In general, these components change when the chosen origin changes. Here del is the gradient, del x is the curl, and del ^2 is the Laplacian.


See also

Beltrami Field, Divergence, Irrotational Field, Poloidal Field, Solenoidal Field, Toroidal Field, Vector Field

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References

Backus, G. "Poloidal and Toroidal Fields in Geomagnetic Field Modeling." Rev. Geophys. 24, 75-109, 1986. https://doi.org/10.1029/RG024i001p00075.Lamb, H. Hydrodynamics, 6th ed. Cambridge, England: Cambridge University Press, 1932. Reprinted 1993.

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Divergenceless Field

Cite this as:

Weisstein, Eric W. "Divergenceless Field." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/DivergencelessField.html

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