When
,
,
, and
solutions of (14.2.2) are known as
toroidal or ring functions. This form of the differential equation
arises when Laplace’s equation is transformed into toroidal coordinates
, which are related to Cartesian coordinates
by
where the constant
is a scaling factor. Most required properties of
toroidal functions come directly from the results for
and
. In particular,
for
and
see §14.5(v).
With
,

With
,

With
,