The Dirichlet Problem

 

Introduction

 

Invariance of Laplace's Equation and the Dirichlet Problem

Let D be a domain whose boundary is made up of piecewise smooth contours joined end to end. The Dirichelet problem is to find a function [Graphics:d0.txtgr1.gif] that is harmonic in D such that [Graphics:d0.txtgr2.gif] takes on prescribed values at points on the boundary. Let us first study the problem in the upper half plane.

Theorem 10.1. (Invariance of Laplace's Equation) Let [Graphics:d0.txtgr3.gif] be harmonic in a domain G in the w plane. Then [Graphics:d0.txtgr4.gif] satisfies Laplace's equation [Graphics:d0.txtgr5.gif] at each point [Graphics:d0.txtgr6.gif] in G. If [Graphics:d0.txtgr7.gif] is a conformal mapping from a domain D in the z plane onto G, then the composition [Graphics:d0.txtgr8.gif] is harmonic in D, and [Graphics:d0.txtgr9.gif] satisfies Laplace's equation [Graphics:d0.txtgr10.gif] at each point [Graphics:d0.txtgr11.gif] in D.

Theorem 10.2. (N-Value Dirichlet Problem for the Upper Half Plane)
Let [Graphics:d0.txtgr12.gif] denote [Graphics:d0.txtgr13.gif] real constants. The function
[Graphics:d0.txtgr14.gif]
is harmonic in the upper half plane [Graphics:d0.txtgr15.gif] and takes on the boundary values
[Graphics:d0.txtgr16.gif]

 

 

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(c) John Mathews, 1998, 2006