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Complex Analysis - Maths KU

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442 Chapter 7 Conformal Mappings<br />

4<br />

3<br />

2<br />

1<br />

y<br />

1 2 3 4 x<br />

Figure 7.61 Figure for Example 8<br />

y<br />

(a) Flow around the unit circle<br />

y<br />

(b) Flow around a circle containing<br />

z1 = –1 and passing through z2 = 1<br />

y<br />

(c) Flow around an airfoil<br />

Figure 7.62 Flow around a Joukowski<br />

airfoil<br />

x<br />

x<br />

x<br />

we obtain a complex potential function for a flow in D byreplacing the symbol<br />

w with z 4 in (13). This yields<br />

Ω(z) =Ln � z 4 − 1 � − Ln � z 4 − 81 � . (14)<br />

Streamlines of this flow are given by ψ(x, y) =c2, or<br />

See Figure 7.61.<br />

Remarks<br />

Arg � z 4 − 1 � − Arg � z 4 − 81 � = c2.<br />

The complex mapping w = J(z) =z + k 2 /z is called the Joukowski<br />

transformation. Under this mapping, a circle in the z-plane that contains<br />

the point z1 = −1 and passes through the point z2 = 1 is mapped<br />

onto a curve in the w-plane that resembles the cross-section of an airplane<br />

wing. See Figure 7.62(c). The image curve is called a Joukowski airfoil,<br />

and the air flow around this curve can be determined using techniques<br />

from this section. We begin with the flow shown in Figure 7.62(a) given<br />

by Ω(z) =z +1/z around the unit circle |z| = 1. Using an appropriate<br />

linear mapping, we can adjust this flow to be one around a circle containing<br />

the point z1 = −1 and passing through the point z2 = 1. See Figure<br />

7.62(b). The Joukowski transformation is then used to “transform” this<br />

flow to one around the airfoil as shown in Figure 7.62(c).<br />

EXERCISES 7.5 Answers to selected odd-numbered problems begin on page ANS-23.<br />

7.5.1 Boundary-Value Problems<br />

In Problems 1–6, (a) find a conformal mapping of the domain shown in color onto<br />

the upper half-plane, and (b) use the mapping from (a) and the solution (7) in<br />

Section 7.4 to find the steady-state temperature φ(x, y) in the domain subject to<br />

the given boundary conditions.<br />

1. y<br />

2.<br />

y<br />

φ = 0<br />

∇ φ = 0<br />

2<br />

i<br />

φ = 1<br />

φ = 2 1 φ = 0<br />

Figure 7.63 Figure for Problem 1<br />

x<br />

φ = 0<br />

i<br />

∇ φ = 0<br />

2<br />

φ = 2<br />

φ = 1 –1 1 φ = –1<br />

Figure 7.64 Figure for Problem 2<br />

x

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