Taylor’s Theorem: Suppose that a function f(z) is analytic throughout a disk z − z0 < R0 centered at z0 and with radius R0. Then f(z) has the power series representation
∞
f ( z ) = ∑ an ( z − z 0 ) , n= 0
n
( z − z0 < R0 )
where an =
f
( n)
( z0 )
n!
(n = 0,1, 2.....)
Maclaurin Series
Taylor Series about the point z 0 = 0 is called Maclaurin series, i. e. ∞
f ( z) = ∑
n =0
f
(n)
( 0) n z , ( z < R0 ) n!
Examples:
1. 2.
∞
n
z e = ∑ , ( z < ∞) n ! n= 0 z
∞
2 n +1
z sin z = ∑ (− 1) , ( 2 n + 1 )! n= 0 n
( z < ∞)
∞
2n
z 3. cos z = ∑ (− 1) , ( 2 n )! n= 0 n
( z < ∞) 4.
∞
2 n +1
z sinh z = ∑ , n = 0 ( 2n + 1)! ( z < ∞)
5.
∞
2n
z cosh z = ∑ , ( 2 n )! n= 0 ( z < ∞)
6.
∞
1 n =∑z , 1 − z n= 0
( z < 1)
∞
1 n n 7. = ∑ (− 1) z , 1 + z n= 0 ( z < 1)
Laurent’s Theorem: Suppose that a function f(z) is analytic throughout an annular domain R1 < z − z0 < R2 centered at z and 0 let C denote any positively oriented simple closed contour around z0 and lying in that domain.
Then, at each point in domain f(z) has the series representation ∞
f ( z ) = ∑ an ( z − z 0 ) n =0
bn +∑ n n =0 ( z − z0 )
(R < z − z 1
where
n
∞
0
< R2 )
1 f ( z ) dz an = ( n = 0 , 1 , 2 .....) ∫ n +1 2π i C ( z − z0 )
and 1 f ( z ) dz bn = ( n = 0 , 1 , 2 ,...) ∫ − n +1 2π i C ( z − z0 )
Example:
Find the Laurent series representation of z f ( z) = ( z − 1)( z − 3) when
(a) D1 : 0 < z < 1, (b) D 2 : 1 < z < 3, (c) D3 : 3 < z < ∞,
We have z f(z) = (z − 1)(z − 3) 1 3 =− + 2( z − 1) 2( z − 3)
(a) Consider the domain D1 : 0 < z < 1. Then f(z) is analytic in D1.
1 3 f(z) = − + 2( z −1) 2( z − 3) 1 3 = − 2(1 − z ) 2 × 3(1 − z ) 3 ∞
∞
1 1 z n = ∑ z − ∑ 2 n =0 2 n =0 3
n
∞
∞
1 z n 1 ⇒ f(z) = ∑ z − ∑ 2 n= 0 2 n= 0 3 ∞
1 1 n = ∑ 1− n z 2 n= 0 3
n
(b) Consider the domain D 2 : 1 < z < 3. Then f(z) is analytic in D 2 .
1 3 f(z) = − + 2( z − 1) 2( z − 3) 1 3 =− − 1 z 2 z (1 − ) 2 × 3(1 − ) z 3 ∞
n
∞
1 1 1 z = − ∑ − ∑ 2 z n =0 z 2 n =0 3
n
∞
∞
1 1 1 z ⇒ f(z) = − ∑ n+1 − ∑ 2 n= 0 z 2 n= 0 3
n
(c) Consider the domain D 3 : 3 < z < ∞. Then f(z) is analytic in D 3 . Note that 1 3 < < 1. z z
1 3 f(z) = − + 2( z − 1) 2( z − 3) 1 3 =− + 1 3 2 z (1 − ) 2 × z (1 − ) z z ∞
n
∞
1 3 1 3 = − ∑ + ∑ 2 z n =0 z 2 z n =0 z
n
∞
n
∞
1 3 3 1 ⇒ f(z) = − ∑ + ∑ 2 z n= 0 z 2 z n= 0 z ∞
∞
n +1
1 1 1 3 = − ∑ n +1 + ∑ n +1 2 n= 0 z 2 n= 0 z ∞
(
)
1 n +1 1 = − ∑ 1− 3 . n +1 2 n= 0 z
n
Excercise:
Show that, when 0 < z − 1 < 2, the Laurent series representation of z f ( z) = ( z − 1)( z − 3) is
∞
n
( z − 1) 1 f ( z ) = − 3∑ n+ 1 − . 2 ( z − 1 ) 2 n= 0
RESIDUE
(1) Consider a function f(z) & 1 let z = . Then w 1 f ( z ) = f = g ( w) w
(i ) f(z) is said to be analytic at infinity if g(w) is analytic at w = 0. (ii) f(z) is said to be singular at infinity if g(w) is singular at w = 0.
(2) Zero of an analytic function : Let f(z) is analytic in a domain D. If f(z 0 ) = 0 for some z = z 0 , then z = z 0 is called zero of f(z).
If f(z 0 ) = f ′( z0 ) = f ′′( z0 ) = .... = f f
(n)
( n −1)
( z0 ) = 0,
but
( z0 ) ≠ 0, then z = z0 is
called ZERO OF ORDER n of f ( z ).
i.e. z = z0 is called zero of order n of f(z) if n
f ( z ) = ( z − z0 ) g ( z ), where g ( z0 ) ≠ 0.
(3)Singular Point of a fn f(z) : (i) If a function f(z) fails to be analytic at a point z 0 , but it is analytic at some point in every nbd of z 0 , then z 0 is called Singular Point of f(z).
(ii) Isolated Singularity The point z 0 is called an isolated singularity of f(z) if (a) z 0 is a singular point of f(z) (b) f(z) is analytic in a deleted nbd N : 0 < z - z 0 <∈ .
(4) (i) Let z 0 is an isolated singularity of f(z) ⇒ ∃ R > 0 such that f(z) is analytic in 0 < z − z0 < R.
Hence f(z) has Laurent series expansion : ∞
∞
f(z) = ∑ an ( z − z0 ) + ∑ bn ( z − z0 ) , n= 0
n
n= 0
0 < z − z0 < R
−n
1 f ( z ) dz where an = , ∫ n +1 2πi c ( z − z0 ) 1 f ( z ) dz bn = , ∫ −n +1 2πi c ( z − z0 ) C is any positively oriented simple closed contour around z 0 and lying in the puctured disc 0 < z - z 0 < R.
∞
(ii ) ∑bn ( z − z0 )
−n
is called
n =1
principal part (PP) of the Laurent series, i.e. ∞
PP = ∑bn ( z − z0 )
−n
n =1
b1 b2 = + + ....... 2 z − z0 ( z − z0 )
If b k ≠ 0, for some k, say k = m, and b n = 0 ∀ n > m, then bm b1 b2 PP = + + ... + m z - z 0 ( z − z0 ) ( z − z0 )
Then the singularity z = z 0 of f(z) is called POLE OF ORDER m. If m = 1, then z 0 is a pole of order 1 and is called a SIMPLE POLE.
(iii) If an analytic function f(z) has a singularity other than a pole, then this singularity is known as ESSENTIAL SINGULARITY of f(z) , i.e.
if bn ≠ 0 for infinitely many n, then the singularity z 0 is called ESSENTIAL SINGULARITY of f(z).
(iv) If b n = 0
∀n,
then the singularity z 0 is called REMOVABLE SINGULARITY of f(z).
RESIDUE : The PP of the Laurent series is given by ∞
PP = ∑bn ( z − z0 )
−n
,
n =1
1
f ( z )dz bn = ∫ −n +1 2π i C ( z − z0 )
where
If n =1, then 1 b1 = 2πi
∫
f ( z ) dz
c
is called RESIDUE of f(z) at z = z 0 , and we write
b1 = Re s f ( z ) z = z0
1 = coeff of z − z0
Residue Theorem : Let C be a positively oriented simple closed contour. Suppose that f(z) is analytic within and on C except for a finite number of singular points z k (k = 1, 2,....n) inside C.
Then
∫
C
n
f ( z )dz = 2π i ∑ Re s f ( z ) z = zk k =1
How to find residue of a given fn f(z) : sin z Ex1 : Let f(z) = 4 , 0 < z < ∞. z 1 Now f(z) = 4 ( sin z ) z 3 5 7 1 z z z = 4 z − + − + .... (3)! (5)! (7)! z
1 1 1 1 1 3 f ( z) = 3 − . + .z − z + .... (7)! z (3)! z (5)! 0< z <∞ 1 1 1 PP = − . + 3 (3)! z z Note that z = 0 is a pole of order ???
Hence 1 1 Res f ( z ) = b1 = coeff of = − z =0 z 6 sin z ∴ ∫ dz = 2 π i Res f ( z ) 4 z =0 z c: z =1
πi =− 3
Ex 2. Find the residue of f ( z ) = exp(1 / z ), and hence evaluate
∫ c
f(z)dz, C : z = 1.
Soln : 1 f ( z ) = exp z 1 1 1 1 1 = 1+ + + + ..... 2 3 z 2! z 3! z
Note : z = 0 is an essential singularity of f(z). 1 ⇒ b1 = coeff of z = Re s f ( z ) z =0
=1
Hence
∫ c
f(z)dz = 2πi.
Ex 3. Find the residue of 2
f ( z ) = exp(1 / z ), and hence evaluate
∫ c
f(z)dz, C : z = 1.
Hints:
1. z = 0 is an essential singularity of f(z). 2. b1 = Re s f ( z ) = 0. z =0
3. I = 0.
How to find the residues ? We have ∞
∞
f(z) = ∑ an ( z − z0 ) + ∑ bn ( z − z0 ) n= 0
n
n =1
−n
Case IA : Let z = z 0 is a simple pole of f(z). Then ∞
f(z) = ∑ an ( z − z0 ) n =0
n
b1 + z − z0
⇒ ( z − z0 ) f ( z ) ∞
= b1 + ( z − z0 ) ∑ an ( z − z0 ) n= 0
⇒ lim ( z − z0 ) f ( z ) = b1 z → z0
= Re s f ( z ) z = z0
n
CaseIB : Let f(z) has a simple pole at z = z 0 and f(z) is of the form p( z ) f ( z) = , q( z ) where
(i) p(z) & q(z) are analytic at z = z 0 , (ii) p(z 0 ) ≠ 0, and (iii ) q( z ) has a simple zero at z = z 0 ,
Then p( z ) Re s f ( z ) = Re s z = z0 z = z0 q ( z ) p ( z0 ) = q′( z0 )
CaseII : Let z 0 be a pole of order m > 1 for the function f(z). ∞
Then f(z) = ∑ an ( z − z0 )
n
n =0
bm b1 b2 + + + .... + 2 m ( z − z0 ) ( z − z0 ) ( z − z0 )
⇒ ( z − z0 )
m
f ( z)
= ( z − z0 )
m
+ b1 ( z − z0 )
∞
∑ an ( z − z 0 )
n
n=0 m −1
+ b2 ( z − z0 )
+ ..... + bm−1 ( z − z0 ) + bm
m− 2
Let φ (z) = (z - z 0 )
m
f ( z)
then Res z =z 0
f ( z ) = b1 = coeff . of (z - z 0 )
m −1
in the
expansion of φ (z) =
φ
(m −1)
( z0 )
(m −1)!
by Taylor's Thm
Thus if z 0 is a pole of order m > 1 of f(z), then Res z = z0
φ
( m −1)
( z0 ) f ( z) = (m − 1)! 1 lim m −1 ( ) = φ z z → z0 (m − 1)!
[
]
Res z = z0
f ( z)
1 lim d m ( ) ( ) = z − z f z z → z0 m − 1 0 (m − 1)! dz m− 1
Ex1. Find the residue of f(z) at z = 0 and z = − 1, where 1 f(z) = . 2 z+z
Soln : Note that z = 0 and z = − 1 are simple poles of f(z).
∴
Res z= 0
f
lim ( z ) = z→ 0
lim = z→ 0
( z − 0) f ( z ) 1 =1 1+ z
∴
Res f z = −1
lim ( z ) = z→ 0
lim = z → −1
( z + 1) f ( z ) 1 = − 1. z
−z
e Q.2 (a) Evaluate I = ∫ dz . 2 z c: z =3 Soln : Clearly, z = 0 is a pole of order 2 of
−z
e f ( z) = 2 . z
Now I =
∫
f ( z )dz
c: z =3
= 2πi ∑ Re s f ( z ), z = zk
−z
e f ( z) = 2 z
∴
Re s z= 0
(
)
1 lim d 2 f ( z) = . z→ 0 z f ( z) (2 − 1)! dz =
lim z→ 0
d −z e dz
⇒
Re s z=0
f ( z) =
lim z→ 0
= −1 ∴ I = − 2π i
(− e ) −z
Q.2 (b) Evaluate −z
e I= ∫ dz . 2 z c: z −3 =1 Ans :
I = 0 (WHY ???)
Ex2(c). Evaluate I=
−z
e dz
∫ ( z −1) c: z =3
. 2
So ln : z = 1 is pole of order 2 of −z
e f ( z) = . 2 ( z −1)
Res ∴ z =1
( )
d −z f ( z) = e dz = −e
2πi ∴I = − e
−z
z =1
z =1
1 =− e
(c ) I =
∫
1 2 z z .e
dz
z =3
Let f(z)
1 2 z =z e
⇒ z = 0 is an essential singularity of f(z)
2
1 1 1 1 1 1 1 f ( z ) = z 1 + + . 2 + . 3 + 4 + ... z 2! z 3! z 4! z 1 1 1 1 1 2 = z + z + + . + . 2 + .... 2! 3! z 4! z
Re s 1 1 ∴ f ( z ) = coeff . of = z=0 z 6 1 πi ∴ I = 2π i × = 6 3
(d ) z +1 I= ∫ 2 dz z − 2 z z =3 z +1 z +1 Let f(z) = 2 = z − 2 z z ( z − 2) ⇒ z = 0 & z = 2 are simple poles
Re s f ( z ) = lim z f ( z ) z →0 z =0 z +1 = lim z →0 z − 2 1 =− 2
lim Re s f ( z ) = ( z − 2) f ( z ) z =2 z →2 3 = 2 ∴ I = 2π i ∑ Re s f ( z ) 1 3 = 2πi − + = 2πi. 2 2
Q.3, p.233 Let f ( z ) be analytic at z 0 , and consider f ( z) g ( z) = . z − z0 Then Show that
(a ) If f(z 0 ) ≠ 0, then z0 is a simple pole of g(z) and Re s g(z) = f(z 0 )
z =z0
(b) If f(z 0 ) = 0, then z0 is a removable singularity of g(z) and Re s g(z) = 0. z = z0
Sol :
f(z) is analytic at z 0
⇒ f(z) has Taylor's series expansion about z 0 , &
f ( z ) = f(z 0 ) + ( z − z0 ) f ′( z0 ) ′ ′ f ( z0 ) 2 + ( z − z0 ) 2! 3 f ′′′( z0 ) + ( z − z0 ) + ... 3!
f ( z) ⇒g ( z ) = z − z0 f ( z0 ) = + f ′( z0 ) z − z0 f ′′( z0 ) + ( z − z0 ) 2! 2 f ′′′( z 0 ) + ( z − z0 ) +... 3!
(a) Clearly if f ( z0 ) ≠ 0, Then principal part (P.P) of g(z) is f ( z0 ) = z − z0
∴ z0 is a simple pole of g(z) and 1 Res g ( z ) = b1 = coeff of z = z0 z − z0 = f ( z0 )
(b) If f ( z0 ) = 0, then p.p.of g(z) is 0 ⇒ bn = 0 ∀ n ⇒ z = z0 is a removable singularity of g(z), and Res z = z0
g ( z) = 0
3
3z + 2 Q.4 (a) I = ∫ , c : z − 2 = 2 2 ( ) z − 1 z + 9 c
(
3
)
3z + 2 Let f ( z ) = 2 ( z − 1) z + 9
(
)
Then 1, 3i, − 3i are simple poles of f(z)
2i
2 -2i
4
Note : z = 1 is only inside C 3z + 2 Res ∴ f ( z) = 2 z =1 z +9 3
5 1 = = 10 2 Re s ∴ I = 2πi ×z =1 f ( z ) = πi
z =1
(b) c : z = 4 Then 1,3i ,−3i are all inside C 1 Re s ∴ z =1 f ( z ) = 2 4i
3i
1
-4 3i
4
Re s z =3i
3
3z + 2 f ( z) = ( z − 1)( z + 3i ) − 81i + 2 = ( 3i − 1)( 6i ) 2 − 81i = − 18 − 6i
z =3i
3
3z + 2 Re s f ( z ) = z =−3i ( z − 1)( z − 3i ) + 81i + 2 = ( − 3i − 1)( − 6i ) 2 + 81i = − 18 + 6i
z =−3i
∴ ∑ Res f ( z )
1 2 + 81i 2 − 81i = + − 2 6i − 18 6i + 18 =3
∴ I = 2π i ∑ Res f ( z ) = 6π i
dz Q.5 (b) I = ∫ 3 ,c : z + 2 = 3 ( ) z z + 4 c Let
1 f ( z) = 3 z ( z + 4)
-5
-4
-3
-2
-1
1
⇒ z = 0 is a pole of order 3 and z = −4 is a simple pole & both lie inside C.
2
Re s
1 d 1 ∴ f ( z) = . 2 z=0 2 dz z + 4 1 = 3 4
z= 0
Re s
1 f (z ) = 3 z = −4 z
z = −4
1 =− 3 4
1 1 ∴I = 2πi 3 − 3 = 0 4 4