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Complex Analysis - Maths KU

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296 Chapter 5 Integration in the <strong>Complex</strong> Plane<br />

–1 1<br />

Figure 5.57 Figure for Problem 24<br />

x<br />

24. The complex potential Ω(z) =kLn(z − 1) − kLn(z +1), k>0, determines<br />

the flow of an ideal fluid on the upper half-plane y>0 with a single source at<br />

z = 1 and a single sink at z = −1. Show that the streamlines are the family of<br />

circles x 2 +(y − c2) 2 =1+c 2 2. See Figure 5.57.<br />

In Problems 25–30, compute the circulation and net flux for the given flow and the<br />

indicated closed contour C.<br />

25. f(z) = 1<br />

; where C is the circle |z| =1<br />

z<br />

26. f(z) =2z; where C is the circle |z| =1<br />

27. f(z) = 1<br />

; where C is the circle |z − 1| =2<br />

z − 1<br />

28. f(z) =¯z; where C is the square with vertices z =0, z =1, z =1+i, z = i<br />

29. F(x, y) =(4x +3y)i +(2x − y)j, where C is the circle x 2 + y 2 =4<br />

30. F(x, y) =(x +2y)i +(x − y)j, where C is the square with vertices z =0,<br />

z =1+i, z =2i, z = −1+i<br />

Focus on Concepts<br />

31. Suppose f(z) =P (x, y)+iQ(x, y) is a complex representation of a velocity field<br />

F of the flow of an ideal fluid on a simply connected domain D of the complex<br />

plane. Assume P and Q have continuous partial derivatives throughout D. IfC<br />

is any simple closed curve C lying within D, show that the circulation around<br />

C and the net flux across C are zero.<br />

32. The flow described by the velocity field f(z) =(a + ib)/z is said to have a<br />

vortex at z = 0. The geometric nature of the streamlines depends on the<br />

choice of a and b.<br />

(a) Show that if z(t) =x(t)+iy(t) is the path of a particle in the flow, then<br />

dx<br />

dt<br />

dy<br />

dt<br />

= ax − by<br />

x 2 + y 2<br />

bx + ay<br />

=<br />

x2 .<br />

+ y2 (b) Rectangular and polar coordinates are related by r 2 = x 2 +y 2 , tan θ = y/x.<br />

Use these equations to show that<br />

�<br />

dr 1<br />

= x<br />

dt r<br />

dx<br />

�<br />

dy<br />

+ y ,<br />

dt dt<br />

dθ 1<br />

=<br />

dt r2 �<br />

−y dx<br />

�<br />

dy<br />

+ x .<br />

dt dt<br />

(c) Use the equations in parts (a) and (b) to establish that<br />

dr<br />

dt<br />

a dθ<br />

= ,<br />

r dt<br />

b<br />

= .<br />

r2 (d) Use the equations in part (c) to conclude that the streamlines of the flow<br />

are logarithmic spirals r = ce aθ/b , b �= 0. Use a graphing utility to verify<br />

that a particle traverses a path in a counterclockwise direction if and only<br />

if a

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