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Complex Analysis - Maths KU

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168 Chapter 3 Analytic Functions<br />

y<br />

C<br />

D<br />

Find φ so that<br />

∇ 2 φ = 0 in D<br />

Figure 3.9 Dirichlet problem<br />

φ = k 0<br />

y<br />

∇ 2 φ = 0<br />

x<br />

and φ=<br />

g<br />

on C<br />

–1 1<br />

φ = k 1<br />

Figure 3.10 Figure for Example 2<br />

x<br />

Table 3.1 summarizes some of the applications of the complex potential<br />

function Ω(z) and the names given to the level curves<br />

φ(x, y) =c1 and ψ(x, y) =c2.<br />

Application Level curves φ (x, y) =c1 Level curves ψ (x, y) =c2<br />

electrostatics equipotential curves lines of force<br />

fluid flow equipotential curves streamlines of flow<br />

gravitation equipotential curves lines of force<br />

heat flow isotherms lines of heat flux<br />

Table 3.1 <strong>Complex</strong> potential function Ω(z) =φ(x, y)+iψ(x, y)<br />

Dirichlet Problems A classical and important problem in applied<br />

mathematics involving Laplace’s equation is illustrated in Figure 3.9 and put<br />

into words next.<br />

Dirichlet Problem<br />

Suppose that D is a domain in the plane and that g is a function defined<br />

on the boundary C of D. The problem of finding a function φ(x, y), which<br />

satisfies Laplace’s equation in D and which equals g on the boundary C<br />

of D is called a Dirichlet problem.<br />

Such problems arise frequently in the two-dimensional modeling of electrostatics,<br />

fluid flow, gravitation, and heat flow.<br />

In the next example we solve a Dirichlet problem. Although the problem<br />

is quite simple, its solution will aid us in the solution of another problem in<br />

Section 4.5.<br />

EXAMPLE 2 A Simple Dirichlet Problem<br />

Solve the Dirichlet problem illustrated in Figure 3.10. The domain D is a<br />

vertical infinite strip defined by −1

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