20.6 Applications
INTRODUCTION
In Sections 20.2, 20.3, and 20.5 we demonstrated how Laplace’s partial differential equation can be solved with conformal mapping methods, and we interpreted a solution u = u(x, y) of the Dirichlet problem as either the steady-state temperature at the point (x, y) or the equilibrium displacement of a membrane at the point (x, y). Laplace’s equation is a fundamental partial differential equation that arises in a variety of contexts. In this section we will establish a general relationship between vector fields and analytic functions and use our conformal mapping techniques to solve problems involving electrostatic force fields and two-dimensional fluid flows.
Vector Fields
A vector field F(x, y) = P(x, y)i + ...
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