84 | | - Boundary conditions |
85 | | - Minimizing distance b/w boundaries (in 1d this is a line, in 2d this is soap bubble) |
86 | | - Physical interprestaion - no charge within the domain, but elsewhere. |
| 84 | The most interesting property of the harmonic function is that it minimizes the distance (in 1D), or the surface area (in 2D), (or the analogous topology in higher dimensions). So in 1D, the solution to Laplace's equation is a line, and in 2D it is a soap bubble (or a waxy film, pulled taught over box with curvy top edges). Thus, solutions to Laplace's equation DOES NOT contain any local mins or maxs. |
| 85 | |
| 86 | The equation describes regions that contain no charge (be it electrical, or gravitational), but describes how the potential due to charge elsewhere effects the region of interest. |
90 | | While the interpreation of the solution propertoies are not as clear cut and intuitive as Laplace, the solution can be thoguht of as composing green's functions (cite references). |
| 90 | While the interpretation of Laplace's equation and the harmonic functions are nice, the same does not seem to apply for the more general Poisson's equation. Instead, the solutions to Poisson's equation are called Green's functions, and they are stitched together out of the solutions to the homogenous part of the PDE (namely, Laplace's equation. Here are some references: |
| 91 | |
| 92 | = Boundary Conditions = |
| 93 | |
| 94 | In 1D, either the value of u is to be given at both boundaries (Dirchlet boundary condition), or EITHER a normal derivative (von Neumann) plus the value of u (but not 2 normal derivatives, for this would not satisfy the boundary conditions). |
| 95 | |
| 96 | In 2D (or higher), one can have either Dirchlet or von Neumann conditions all around the region. |