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Complex Analysis - Maths KU

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378 Chapter 6 Series and Residues<br />

C R<br />

s n<br />

s 2<br />

s 4<br />

s 3<br />

y<br />

s1 O<br />

γ + iR<br />

γ<br />

L R<br />

γ – iR<br />

Figure 6.23 Possible contour that<br />

could be used to evaluate (7)<br />

x<br />

The limit in (7), which defines a principal value of the integral, is usually<br />

written as<br />

f(t) =� −1 {F (s)} = 1<br />

2πi<br />

� γ+i∞<br />

γ−i∞<br />

e st F (s) ds, (8)<br />

where the limits of integration indicate that the integration is along the infinitely<br />

long vertical-line contour Re(s) =x = γ.Here γ is a positive real<br />

constant greater than c and greater than all the real parts of the singularities<br />

in the left half-plane.The integral in (8) is called a Bromwich contour integral.Relating<br />

(8) back to (3), we see that the kernel of the inverse transform<br />

is H(s, t) =est /2πi.<br />

The fact that F (s) has singularities s1, s2, ...,sn to the left of the line<br />

x = γ makes it possible for us to evaluate (7) by using an appropriate closed<br />

contour encircling the singularities.A closed contour C that is commonly<br />

used consists of a semicircle CR of radius R centered at (γ, 0) and a vertical<br />

line segment LR parallel to the y-axis passing through the point (γ, 0) and<br />

extending from y = γ −iR to y = γ +iR .See Figure 6.23.We take the radius<br />

R of the semicircle to be larger than the largest number in set of moduli of<br />

the singularities {|s1|, |s2|, ...,|sn|}, that is, large enough so that all the<br />

singularities lie within the semicircular region.With the contour C chosen in<br />

this manner, (7) can often be evaluated using Cauchy’s residue theorem.If<br />

we allow the radius R of the semicircle to approach ∞, the vertical part of<br />

the contour approaches the infinite vertical line that is the contour in (8).<br />

We use the contour just described in the proof of the following theorem.<br />

Theorem 6.25 Inverse Laplace Transform<br />

Suppose F (s) is a Laplace transform that has a finite number of poles<br />

s1, s2, ... , sn to the left of the vertical line Re(s) =γ and that C is the<br />

contour illustrated in Figure 6.23. If sF (s) is bounded as R →∞, then<br />

� −1 {F (s)} =<br />

n�<br />

k=1<br />

Res � e st �<br />

F (s),sk . (9)<br />

Proof From Figure 6.23 and Cauchy’s residue theorem, we have<br />

or<br />

�<br />

e st �<br />

F (s) ds +<br />

CR<br />

� γ+iR<br />

1<br />

2πi<br />

γ−iR<br />

LR<br />

e st F (s) ds =<br />

e st F (s) ds =2πi<br />

n�<br />

k=1<br />

n�<br />

k=1<br />

Res � e st �<br />

F (s), sk<br />

Res � e st �<br />

� 1<br />

F (s), sk −<br />

2πi<br />

CR<br />

e st F (s) ds. (10)<br />

The �theorem<br />

is justified by letting R → ∞ in (10) and showing that<br />

lim CR R→∞<br />

estF (s) ds = 0.Now if the semicircle CR is parametrized by

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