3 1 Laplaces Equation Common situation Conductors in

3. 1 Laplace’s Equation Common situation: Conductors in the system, which are a at given potential V or which carry a fixed amount of charge Q. The surface charge distribution is not known. We want to know the field in regions, where there is no charge. Reformulate the problem.

+ Boundary conditions. (e. g. over a surface V=const. ) Important in various branches of physics: gravitation, magnetism, heat transportation, soap bubbles (surface tension) … fluid dynamics

One dimension Boundary conditions:

V has no local minima or maxima.

Two Dimensions Partial differential equation. To determine the solution you must fix V on the boundary – boundary condition. V has no local minima or maxima inside the boundary. A ball will roll to the boundary and out. Rubber membrane Soap film

Three Dimensions Partial differential equation. To determine the solution you must fix V on the boundary, which is a surface, – boundary condition. V has no local minima or maxima inside the boundary. Earnshaw’s Theorem: A charged particle cannot be held in a stable equilibrium by electrostatic forces alone.

First Uniqueness Theorem The solution to Laplace’s equation in some volume V is uniquely determined if V is specified on the boundary surface S. The potential in a volume V is uniquely determined if a) the charge density in the region, and b) the values of the potential on all boundaries are specified.

Second Uniqueness Theorem In a volume surrounded by conductors and containing a specified charge density, the electrical field is uniquely determined if the charge on each conductor is given.

Image Charges What is V above the plane? Boundary conditions: There is only one solution.

Image charge The region z<0 does not matter. There, V=0.

Induced surface charge: Force on q: Energy: Force exerted by the image charge Different from W of 2 charges!!

Example 3. 2 Find the potential outside the conducting grounded sphere.