To solve the heat conduction equation on a two-dimensional disk of radius , try to separate the equation using
|
(1)
|
Writing the
and
terms of the Laplacian in cylindrical
coordinates gives
|
(2)
|
so the heat conduction equation becomes
|
(3)
|
Multiplying through by gives
|
(4)
|
The
term can be separated.
|
(5)
|
which has a solution
|
(6)
|
The remaining portion becomes
|
(7)
|
Dividing by
gives
|
(8)
|
where a negative separation constant has been chosen so that the
portion remains finite
|
(9)
|
The radial portion then becomes
|
(10)
|
|
(11)
|
which is the spherical Bessel differential equation.
Consider disk or radius with initial temperature
and the boundary condition
. Then the solution is
|
(12)
|
where
is the
th
positive zero of the Bessel
function of the first kind
(Bowman 1958, pp. 37-39).