際際滷

際際滷Share a Scribd company logo
NPTEL  Physics  Mathematical Physics - 1
Lecture 40
Summary
Complex Analysis
 =  + 
= 
=  ( + )
,  are real
polar form
Cauchy Riemann Condition (CR condition)
Let a complex function be () = (, ) + (, ). The derivative () to exist at
a particular point z demands that,
 = p
} CR condition
Polar representation of the CR condition
 = p
 = p
 = p
}
Analytic functions
A function () is said to be analytic in a region if (a) it is defined, (b) and is
differentiable at every point in the region.
Example. () =  is analytic in the entire finite z plane, whereas () =  is
analytic nowhere.
() =     = ,  = 
CR conditions are not satisfied.
Thus CR conditions are equivalent to analyticity
Branch cut
Let us consider a function () = ,  =  ,

() =  2
Joint initiative of IITs and IISc  Funded by MHRD Page 54 of 66
NPTEL  Physics  Mathematical Physics - 1
The value of the function at A is () =  12. After a complete revolution,
() = 
(1+22
=  12
So it does not return to the same value. So the function is multivalued and 
12 is a
value on one of the branches and between 2    4, the function assumes another
branch. The line OB is called the branch cut.
Complex integration Cauchy  Goursat Theorem
If () is analytic in a region R and on its boundary , then  () = 0 Also known as
cauchys integral theorem.
Cauchys Integral formula
() =
1 ()
 
2  р
() is analytic inside and on the boundary c of a simply connected region R, excepting
at a point a.
Residue theorem
If () is analytic inside and on a simple closed curve c except for a pole of order m at 
= , inside c, prove that
1 1
2
 () = 瑞
р (  1)! ю1
1
[(  )()]

If there are two different poles of order 1and 2
1 1
2
 () = 瑞
р1 (11)! ю11

11
[(  1)1 ()] +
瑞
р2 (21)! ю21
Joint initiative of IITs and IISc  Funded by MHRD Page 55 of 66
1 21
[(   )2 ()]
2
Example
Integrate,
 
 =

0 1+3
The integrand I is not even so we cannot extend it up to -.
NPTEL  Physics  Mathematical Physics - 1
Let us evaluate the integral
3 = 1
 = 

1+3 over the Contour below
 = 3
1 are the
poles
3 
=  =  6
0 0
 = 
1 + 3 = 1 + 33
 = 
 
 =

1+3
2
+ 
3

1+3  1+3
0 
+ 
0
So,
0  
 = 
+ 


 1+33
 = 2
3
=  + (  
1
2
3
2 
 ) 
 0 
1+3
 3 =  + 
2 2
3
2
3
 = (1   3) 
2
=  
1 
3
2 2
2 = 2 + 2
= 1
Now  has a simple pole at  = 


3
 = 2
3
2

3
 =
2
33
Joint initiative of IITs and IISc  Funded by MHRD Page 56 of 66

More Related Content

lec40.ppt

  • 1. NPTEL Physics Mathematical Physics - 1 Lecture 40 Summary Complex Analysis = + = = ( + ) , are real polar form Cauchy Riemann Condition (CR condition) Let a complex function be () = (, ) + (, ). The derivative () to exist at a particular point z demands that, = p } CR condition Polar representation of the CR condition = p = p = p } Analytic functions A function () is said to be analytic in a region if (a) it is defined, (b) and is differentiable at every point in the region. Example. () = is analytic in the entire finite z plane, whereas () = is analytic nowhere. () = = , = CR conditions are not satisfied. Thus CR conditions are equivalent to analyticity Branch cut Let us consider a function () = , = , () = 2 Joint initiative of IITs and IISc Funded by MHRD Page 54 of 66
  • 2. NPTEL Physics Mathematical Physics - 1 The value of the function at A is () = 12. After a complete revolution, () = (1+22 = 12 So it does not return to the same value. So the function is multivalued and 12 is a value on one of the branches and between 2 4, the function assumes another branch. The line OB is called the branch cut. Complex integration Cauchy Goursat Theorem If () is analytic in a region R and on its boundary , then () = 0 Also known as cauchys integral theorem. Cauchys Integral formula () = 1 () 2 р () is analytic inside and on the boundary c of a simply connected region R, excepting at a point a. Residue theorem If () is analytic inside and on a simple closed curve c except for a pole of order m at = , inside c, prove that 1 1 2 () = 瑞 р ( 1)! ю1 1 [( )()] If there are two different poles of order 1and 2 1 1 2 () = 瑞 р1 (11)! ю11 11 [( 1)1 ()] + 瑞 р2 (21)! ю21 Joint initiative of IITs and IISc Funded by MHRD Page 55 of 66 1 21 [( )2 ()] 2 Example Integrate, = 0 1+3 The integrand I is not even so we cannot extend it up to -.
  • 3. NPTEL Physics Mathematical Physics - 1 Let us evaluate the integral 3 = 1 = 1+3 over the Contour below = 3 1 are the poles 3 = = 6 0 0 = 1 + 3 = 1 + 33 = = 1+3 2 + 3 1+3 1+3 0 + 0 So, 0 = + 1+33 = 2 3 = + ( 1 2 3 2 ) 0 1+3 3 = + 2 2 3 2 3 = (1 3) 2 = 1 3 2 2 2 = 2 + 2 = 1 Now has a simple pole at = 3 = 2 3 2 3 = 2 33 Joint initiative of IITs and IISc Funded by MHRD Page 56 of 66