
Laplace's equation in two dimensions is given by:

.
Let the unit square have a Dirichlet boundary condition

everywhere except

, where the condition is

for

. The formal solution is

,
where

.
Solutions for boundary conditions on the other sides of the square are obtained by switching variables in the formula. For instance, the solution for

applied to

for

simply switches

and

in the formula. Similar formulas are then obtained for

applied at either

or

, with switching

as appropriate. (Reference: E. D. Rainville,
Elementary Differential Equations, 3rd ed., New York: Macmillan, 1964 p. 474)
This Demonstration deals with the square

and

by shifting the variables, leading to slightly more complicated solutions.
Solutions to Laplace's equation are called harmonic functions. One of the properties of harmonic functions is that they will not attain any local minima or maxima inside the boundary; thus the minima and maxima are on the boundary, as defined by the Dirichlet conditions. Another property is that the solution at any point

has a value that is the average of the values over the area of a circle defined with

at its center.