Any real function with continuous second partial derivatives which satisfies Laplace's equation,
| (1) |
is called a harmonic function. Harmonic functions are called potential functions in physics and engineering. Potential functions are extremely useful, for example, in electromagnetism, where they reduce the study of a 3-component vector field to a 1-component scalar function. A scalar harmonic function is called a scalar potential, and a vector harmonic function is called a vector potential.
To find a class of such functions in the plane, write the Laplace's equation in polar coordinates
| (2) |
and consider only radial solutions
| (3) |
This is integrable by quadrature, so define ,
| (4) |
| (5) |
| (6) |
| (7) |
| (8) |
| (9) |
so the solution is
| (10) |
Ignoring the trivial additive and multiplicative constants, the general pure radial solution then becomes
| (11) | |||
| (12) |
Other solutions may be obtained by differentiation, such as
| (13) | |||
| (14) |
| (15) | |||
| (16) |
and
| (17) |
Harmonic functions containing azimuthal dependence include
| (18) | |||
| (19) |
The Poisson kernel
| (20) |
is another harmonic function.