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Mathematical Physics

This document discusses complex analysis and contains the following key points: 1. It defines the residue of a complex function at a pole, and provides methods for calculating residues at simple poles, higher order poles, and at infinity. 2. It states the Cauchy residue theorem, which relates the integral of an analytic function around a closed contour to the sum of the residues of the poles enclosed by the contour. 3. It provides examples of calculating residues and evaluating contour integrals using the Cauchy residue theorem for different complex functions.

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0% found this document useful (0 votes)
94 views3 pages

Mathematical Physics

This document discusses complex analysis and contains the following key points: 1. It defines the residue of a complex function at a pole, and provides methods for calculating residues at simple poles, higher order poles, and at infinity. 2. It states the Cauchy residue theorem, which relates the integral of an analytic function around a closed contour to the sum of the residues of the poles enclosed by the contour. 3. It provides examples of calculating residues and evaluating contour integrals using the Cauchy residue theorem for different complex functions.

Uploaded by

hejan94618
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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Download as PDF, TXT or read online on Scribd
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COMPLEX ANALYSIS 199

 1   1 1 1 
(b)  z  3 sin     z  3   3
 5
 .........
 z 2  z  2 ( z  2) .3! ( z  2) .5! 
so, z = -2 is an isolated essential singular point.

5.6 Residue of a Complex Function

Residue at a pole:
Let, z = a be a pole of order ‘m’ of f (z) and C1 is a circle of radius ‘r’ with center at z = a which does not
contain singularities except z = a, then f(z) is analytic within the annular region r < | z – a | < R can be expanded
into Laurrent series within the annulur region as:

R
r
 
a
c1
f  z   an ( z  a )n   bn ( z  a ) n
n 0 n 1

1
2 i C1
Co-efficient b1 is known as residue of f (z) at z = a i.e. Res. f(z = a) = b1 = f ( z )dz

Methods of finding residues:

CASE 1: Residue at simple pole:


(a) Method 1: Res. f(z = a) = Lt (z  a)f (z)
z a

(z) (a)
(b) Method 2: If f(z) = where (a) = 0 but (a)  0, then Res. f(z = a) =
(z) (a)

CASE 2: Residue at a pole of order ‘n’:

1  d n1 n 
(a) Method 1: Res. f (z = a) =  n1 ( z  a) f ( z) 
(n  1)!  dz z  a
(b) Method 2: First put z - a = t and expand it into series, then Res. f (z = a) = co-efficient of 1/t.

CASE 3: Residue at z =  :

Res. f  z     Lt   zf ( z )
z 
Example 30: Find the singular points of the following function and the corresponding residues:

1  2z z2
(a) f ( z )  (b) f ( z )  2 (c) f ( z )  z 2 e1/ z
z  z  1 z  2  z  a2
200 COMPLEX ANALYSIS

Soln: (a) f  z   1  2z
 Poles : z  0, z  1, z  2
z  z  1  z  2 
1  2z 1
Res. f  z  0   Lt  z  0  f  z   Lt 
z 0 z0  z  1 z  2  2
1  2z
Res. f  z  1  Lt  z  1 f  z   Lt 1
z 1 z 1 z  z  2 

1  2z 3
Res. f  z  2   Lt  z  2  f  z   Lt 
z 2 z 2 z  z  1 2

z2
(b) f  z    Poles : z  ia, z  ia
z 2  a2
 z2  1  z2  1
Res. f  z  ia      ia; Res. f  z  ia       ia
 2 z  z ia 2  2 z  z ia 2

2 1/ z 2  1 1 1 
(c) f  z   z e  z 1   2  3  .......  Poles : z  0
 z z .2! z .3! 
1 1 1
Res. f  z  0   Coefficient of  
z 3! 6

sin z
Example 31: The value of the residue of is
z6
1 1 2 i 2 i
(a)  (b) (c) (d) 
5! 5! 5! 5!

sin z 1  z3 z5 z 7 
Soln: f z  6
 6 
z     ........
z z  3! 5! 7! 
1 1 1 11
    ......
z 5 3! z 3 5! z
1 1
Residue of f  z  = coefficient of   
 z  5!
Correct option is (b)

5.7 Cauchy Residue Theorem:

If f (z) in single-valued and analytic inside a simple closed curve ‘C, except at a finite number of singular
points within C, then

 f (z)dz  2i  sum of the residues at poles within 'C '


C
COMPLEX ANALYSIS 201

4  3z 3
Example 32: Evaluate the integral:  z  z  1 z  3 dz where z  2
C

4  3z
Soln: f  z    Poles : z  0, z  1, z  3
z  z  1 z  3
But, the given contour is circle centered at the origin and radius 3/2 units.
Therefore, only z = 0 and z = 1 within the contour.
 4 1  5 i
I  2 i  Re s. f  z  0   Re s. f  z  1   2 i    
3 2 3

e2 z  z 2
Example 33: Evaluate the integral:   z  1
C
5
dz where z  2

2z 2
Soln: f  z   e  z5  Poles : z  1 (order 5)
 z  1
1 d 4 2z 2 2e 2 4 ie2
I  2 i  Re s. f  z  1  2 i   e  z   2 i  
4! dz 4   z 1 3 3

z3
Example 34: The value of the integral  dz , where C is closed contour defined by the equation
C z 2  5z  6
2 | z | 5  0 , traversed in the anti-clockwise direction, is
(a) 16 i (b) 16 i (c) 8 i (d) 2 i

z3
Soln: f  z   ; Condition of singularity: z 2  5z  6  0  z  3, 2 1st order pole 
z 2  5z  6
5
Given closed contour: c : 2 z  5  0  z 
2
Only z = 2 i.e. point (2, 0) is within ‘c’

z3
Res.f  z  z 2   z  2   8
 z  3 z  2 z2
Given integral: I  2i   sum of the residues   16i
Correct answer is (a)
Example 35: The value of the integral  z10 dz , C is the unit circle with the origin as the centre is
C

11
(a) 0 (b) z / 11 (c) 2 iz11 / 11 (d) 1/1
Soln: f  z   z10 is analytic in the entire complex argand plane.
So, according to Cauchy integral theorem,
10
z dz  0
C

Correct option is (a)

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