Any real-valued 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
![\begin{displaymath}
u=\ln[(x-a)^2+(y-b)^2]^{1/2} = {\textstyle{1\over 2}}\ln\left[{(x-a)^2+(y-b)^2}\right].
\end{displaymath}](h_460.gif)  | 
(11) | 
 
Other solutions may be obtained by differentiation, such as
and
  | 
(16) | 
 
Harmonic functions containing azimuthal dependence include
The Poisson Kernel
  | 
(19) | 
 
is another harmonic function.
See also Scalar Potential, Vector Potential
References
 Potential Theory
Ash, J. M. (Ed.)  Studies in Harmonic Analysis.  Washington, DC: Math. Assoc. Amer., 1976.
Axler, S.; Pourdon, P.; and Ramey, W.  Harmonic Function Theory.  Springer-Verlag, 1992.
Benedetto, J. J.  Harmonic Analysis and Applications.  Boca Raton, FL: CRC Press, 1996.
Cohn, H.  Conformal Mapping on Riemann Surfaces.  New York: Dover, 1980.
© 1996-9 Eric W. Weisstein 
1999-05-25