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Complex Analysis - Maths KU

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

C<br />

T<br />

Figure 5.54 Flow of fluid tends to<br />

turn C.<br />

F<br />

�<br />

F · T ds < 0 mean that the fluid tends to rotate C in the counterclockwise<br />

C<br />

and clockwise directions, respectively. See Figure 5.54.<br />

Now if N =(dy/ds) i − (dx/ds) j denotes the normal unit vector to a<br />

positively oriented, simple closed contour C, and if F(x, y) =P (x, y)i +<br />

Q(x, y)j again represents a velocity field of a two-dimensional fluid flow, we<br />

define the net flux of F as the real line integral of the normal component of<br />

the velocity vector F:<br />

�<br />

net flux = F · N ds. (19)<br />

Specifically, (19) defines a net rate at which the fluid is crossing the curve C<br />

in the direction of the normal N and is measured in units of area per unit<br />

time. In other words, the net flux across C is the difference between the rate<br />

at which fluid enters and the rate at which fluid leaves the region bounded by<br />

C. A nonzero value of �<br />

C<br />

C<br />

F · N ds indicates the presence of sources or sinks<br />

for the fluid inside the curve C.<br />

Now if f(z) =P (x, y) +iQ(x, y) is the complex representation of the<br />

velocity field F of a fluid, the line integrals (18) and (19) can be computed<br />

simultaneously by evaluating the single contour integral �<br />

f(z) dz. To see<br />

C<br />

how this is done, first observe:<br />

�<br />

�<br />

�<br />

dx dy<br />

F · T ds = (P i + Q j) · i +<br />

C<br />

C<br />

ds ds j<br />

� �<br />

ds = Pdx+ Qdy<br />

C<br />

�<br />

�<br />

�<br />

dy dx<br />

F · N ds = (P i + Q j) · i −<br />

ds ds j<br />

� �<br />

ds = Pdy−Qdx, C<br />

and then:<br />

�<br />

C<br />

C<br />

�<br />

f(z) dz = (P − iQ)(dx + idy)<br />

C<br />

��<br />

� ��<br />

�<br />

= Pdx+ Qdy + i Pdy−Qdx C<br />

�� � ��<br />

C<br />

�<br />

= F · T ds + i F · N ds . (20)<br />

C<br />

Equation (20) shows that (18) and (19) can be found by computing �<br />

f(z) dz<br />

C<br />

and identifying the real and imaginary parts of the result. That is,<br />

�� �<br />

�� �<br />

circulation = Re f(z) dz and net flux = Im f(z) dz . (21)<br />

C<br />

EXAMPLE 5 Circulation and Net Flux<br />

Use (21) to compute the circulation and the net flux for the flow and curve C<br />

in part (a) of Example 4.<br />

Solution Frompart (a) of Example 4, the flow is f(z) =(z − i) 2 and C is<br />

the circle |z| = 1. Then f(z) = � z − i � 2 =(¯z + i) 2 =¯z 2 +2i¯z − 1, and C is<br />

C<br />

C<br />

C

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