A divergenceless field, also called a solenoidal field, is a vector field for which . A sufficiently smooth
divergenceless field can locally be written as
, where
is a vector potential.
Fix an origin, let be the position vector from
it, and write
.
On a spherical shell centered at this origin,
a sufficiently smooth divergenceless field satisfying
for each sphere in the spherical
shell can be written as
|
(1)
| |||
|
(2)
|
where
and
are scalar functions and
|
(3)
| |||
|
(4)
| |||
|
(5)
| |||
|
(6)
|
The components
and
are called the toroidal field and poloidal
field, respectively (Backus 1986). In general, these components change when the
chosen origin changes. Here
is the gradient,
is the curl, and
is the Laplacian.