NPTEL – Physics – Mathematical Physics - 1
Lecture 36
Caucly-Goursat theorem
Let 𝑓(𝑧) the analytic in a region R and on it’s boundary C. then
∮ 𝑓(𝑧)𝑑𝑧 = 0 → Cauchy’s integral theorem
Morera’s Theorem:
Let 𝑓(𝑧) be continuous in a simply connected and suppose that ∮ 𝑓(𝑧)𝑑𝑧 = 0 around
every simple closed curve C in R. Then 𝑓(𝑧) is analytic. This is converse of Cauchy’s
theorem.
Example. 1. Evaluate ∫ 𝑧∗ 𝑑𝑧 for the curve 𝐶 = 𝐶1 − 𝐶2
𝐶
∫ 𝑧∗𝑑𝑧 = ∫ (𝑥 − 𝑖𝑦)(𝑑𝑥 + 𝑖𝑑𝑦)
𝐶1−𝐶2
𝐶1− 𝐶2
1 1
= ∫𝑥=0 𝑥𝑑𝑥 + ∫𝑦=
(1 − 𝑖𝑦)(𝑖
𝑑𝑦)
0
= 1 + 𝑖
∫ 𝑧∗𝑑𝑧 = ∫
1
(𝑥 − 𝑖𝑥)(𝑑𝑥 + 𝑖𝑑𝑥)
𝑥=0
𝐶3
= 1
Since 𝑧∗ is not analytic, the results are not same.
𝑢𝑥 = 𝑣𝑦 and 𝑢𝑦 = −𝑣𝑥 are not satisfied for 𝑓(𝑧) = 𝑧 ∗. Then f (z)
not exist.
does
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NPTEL – Physics – Mathematical Physics - 1
Example.2.
Evaluate ∫
1
𝐶 𝑧
𝑑𝑧 for (a) a simple contour C not enclosing the origin. (b) a simple contour
C enclosing the origin.
(a) Because is analytic for all points (other then 𝑧 = 0), So
1
𝑧
∫
1
𝐶 𝑧
𝑑𝑧 = 0
(b) The contour can be deformed as above. In the limit of
𝑟 ⟶ 0 (of 𝐶1) and the lengths of 𝐿1 and 𝐿2 tending to zero, we have a
closed curve. 𝐶 = 𝐶2 + 𝐿1 + 𝐿2 − 𝐶1
1
Now as earlier ∫ 𝑧
𝑑𝑧 = 0
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NPTEL – Physics – Mathematical Physics - 1
as ∫𝐿1
+ ∫𝐿2
=
0
(𝑧 = 𝑟𝑒𝑖𝜃 , 𝑑𝑧 = 𝑟𝑖𝑒𝑖𝜃 𝑑𝜃
)
2𝜋
∫ 𝑑𝑧 = ∫ 𝑑𝑧 = ∫ 𝑟−1 𝑒−𝑖𝜃𝑖𝑒𝑖𝜃𝑟𝑑𝜃
1 1
𝑧
𝐶2 𝐶1
𝑧
0
= 2𝜋𝑖
Thus the integral ∫
1
𝑧
𝑑𝑧 around any closed curve that encloses the origin is zero.
Consequences of Cauchy’s integral theorem
𝑏
1. If 𝑓(𝑧) is analytic in a simply connected region R, prove that ∫ 𝑓(𝑧)𝑑𝑧 is
𝑎
independent of the path in R joining any two points. A and B in R.
2. Let 𝑓(𝑧) be analytic in a region R bounded by two simple closed curves
𝐶1and 𝐶2 and also on 𝐶1, 𝐶2. Prove that
∮𝐶 𝑓(𝑧)𝑑𝑧 = ∮𝐶 𝑓(𝑧)𝑑𝑧
1 2
Since 𝑓(𝑧) is analytic everywhere in R,
∫
𝐴𝐸𝐹𝐺𝐻𝐸𝐴𝐷𝐶𝐵𝐴
𝑓(𝑧)𝑑𝑧 = 0
∫ 𝑓(𝑧)𝑑𝑧 + ∫ 𝑓(𝑧)𝑑𝑧 + ∫ 𝑓(𝑧)𝑑𝑧 +
𝐴𝐸 𝐸𝐹𝐺𝐻 𝐸𝐴
∫ 𝑓(𝑧)𝑑𝑧 = 0
𝐴𝐷𝐶𝐵𝐴
Thus, ∫𝐸𝐹𝐺𝐻 𝑓(𝑧)𝑑𝑧 = − ∫𝐴𝐷𝐶𝐵𝐴 𝑓(𝑧)𝑑𝑧
∮𝐶 𝑓(𝑧)𝑑𝑧 = ∮𝐶 𝑓(𝑧)𝑑𝑧
1 2
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Prove Cauchy’s Theorem (Cauchy Goursat theorem)
The theorem states that,
∮𝐶 𝑓(𝑧)𝑑𝑧 = 0, if f(z) is analytic with derivatives 𝑓′(𝑧) which is continuous at all points
inside and on the simple closed curve C.
𝑓(𝑧) = 𝑢 + 𝑖𝑣 is analytic and has a continuous derivative.
𝑓́(𝑧) =
𝜕𝑢
+ 𝑖
𝜕𝑣
=
𝜕𝑣
− 𝑖
𝜕𝑢
𝜕𝑥 𝜕𝑥 𝜕𝑦 𝜕𝑦
It follows that the partial derivatives,
𝜕𝑢
= 𝜕𝑣
,
𝜕𝑥 𝜕𝑦 𝜕𝑥 𝜕𝑦
and
𝜕𝑣
= −
𝜕𝑢
are continuous inside and on C.
Thus, ∮ 𝑓(𝑧)𝑑𝑧 = ∮𝐶
(𝑢 + 𝑖𝑣)(𝑑𝑥 + 𝑖𝑑𝑦)
= ∮(𝑢𝑑𝑥 − 𝑣𝑑𝑦) + 𝑖 ∮𝐶 (𝑣𝑑𝑥 + 𝑢𝑑𝑦)
Using Green’s theorem,
∫ (−
𝜕𝑣
− 𝜕𝑢
) 𝑑𝑥𝑑𝑦 + 𝑖 ∫ (
𝜕𝑢
− 𝜕𝑣
) 𝑑𝑥𝑑𝑦
𝑅 𝜕𝑥 𝜕𝑦 𝑅 𝜕𝑥 𝜕𝑦
= 0 (Using CR Condition)
Cauchy’s Integral formula
If 𝑓(𝑧) is analytic inside and on the boundary C of a simply connected region R,
prove the following,
𝑓(𝑎) =
1 𝑓(𝑧)
∮ 𝑑𝑧 (Cauchy’s Integral formula)
2𝜋𝑖 𝐶 (𝑧−𝑎)
The function is analytic inside R and on C excepting the point. 𝑧 = 𝑎
𝑓(𝑧)
𝑧−𝑎
∮
𝑓(𝑧)
𝐶 𝑧−𝑎 Γ 𝑧−𝑎
𝑑𝑧 = ∮ 𝑑𝑧
𝑓(𝑧)
(1)
The equation for Γ is |𝑧 − 𝑎| = 𝜖
Joint initiative of IITs and IISc – Funded by MHRD Page 28 of 66
NPTEL – Physics – Mathematical Physics - 1
so, 𝑧 − 𝑎 = 𝜖𝑒𝑖𝜃, 0 ≤ 𝜃 < 2𝜋
𝑧 − 𝑎
Substituting 𝑧 = 𝑎 + 𝜖𝑒𝑖𝜃, 𝑑𝑧 = 𝑖𝜖𝑒𝑖𝜃𝑑𝜃
2𝜋
∮
Γ
𝑓(𝑧)
𝑑𝑧 = ∫
0
𝑓(𝑎 + 𝜖𝑒𝑖𝜃 )𝑖𝜖𝑒𝑖
𝜃
𝜖𝑒𝑖
𝜃
𝑑𝜃
2𝜋
= i∫ 𝑓(𝑎 +
𝜖𝑒𝑖𝜃)𝑑𝜃
0 (2)
Thus using (1) ∮
𝑓(𝑧)
𝐶 𝑧−𝑎 0
𝑑𝑧 = 𝑖 ∫ 𝑓(𝑎 + 𝜖𝑒𝑖𝜃 )𝑑
𝜃
2𝜋
Taking limit 𝜖 → 0 (remember 𝑓(𝑧) is continuous).
∮
𝐶
𝑓(𝑧)𝑑𝑧
𝑧 − 𝑎
= 𝐿𝑖𝑚 𝑖 ∫ 𝑓(𝑎 + 𝜖𝑒𝑖𝜃)𝑑𝜃 = 𝑖 ∫ 𝑓(𝑎)𝑑𝜃
𝜖→0
2𝜋 2𝜋
0 0
= 2𝜋𝑖𝑓(𝑎)
Example: If 𝑓(𝑧) is analytic inside and on the boundary C of a simply connected region
R, prove that,
𝑓′(𝑎) = ∮
1 𝑓(𝑧)
2𝜋𝑖 (𝑧 − 𝑎)2
𝑐
𝑑𝑧
𝑓′(𝑎) = 𝐿𝑖𝑚 𝑓(𝑎+ℎ)−𝑓(𝑎)
ℎ→0 ℎ
Consider both the points 𝑎 and 𝑎 + ℎ are inside the circle of radius 𝜖.
Joint initiative of IITs and IISc – Funded by MHRD Page 29 of 66
NPTEL – Physics – Mathematical Physics - 1
𝑓′(𝑎) = ∮ [
1 1 1 1
2𝜋𝑖 ℎ 𝑧 − (𝑎 + ℎ) 𝑧 − 𝑎
𝑐
− ] 𝑓(𝑧)𝑑𝑧
=
1 𝑓(𝑧)𝑑
𝑧
2𝜋𝑖 𝑐 (𝑧−𝑎−ℎ)(𝑧−𝑎)
∮
The result follows as ℎ → 0.
Important formula
If 𝑓(𝑧) is analytic inside and on a simple closed curve 𝐶 except for a pole of order m
at 𝑧 = 𝑎, inside 𝐶, prove that
1 1
2𝜋𝑖
∮ 𝑓(𝑧)𝑑𝑧 = 𝐿𝑡
𝑐
𝑧→𝑎 (𝑚 − 1)! 𝑑𝑧𝑚−1
𝑑𝑚
[(𝑧 − 𝑎)𝑚𝑓(𝑧)]
also for two different poles of order 𝑚1 and 𝑚2,
1 1
2𝜋𝑖
∮ 𝑓(𝑧)𝑑𝑧 = 𝐿𝑡
𝑧→𝑎1 (𝑚1 − 1)! 𝑑𝑧𝑚1−1
𝑐
𝑑𝑚1
[(𝑧 − 𝑎)𝑚1 𝑓(𝑧)]
+ 𝐿𝑡
𝑧→𝑎2 (𝑚2 − 1)! 𝑑𝑧𝑚2−1
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1 𝑑𝑚2
[(𝑧 − 𝑎)𝑚2 𝑓(𝑧)]
A similar formula can be worked out for more poles.

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lec36.ppt

  • 1. NPTEL – Physics – Mathematical Physics - 1 Lecture 36 Caucly-Goursat theorem Let 𝑓(𝑧) the analytic in a region R and on it’s boundary C. then ∮ 𝑓(𝑧)𝑑𝑧 = 0 → Cauchy’s integral theorem Morera’s Theorem: Let 𝑓(𝑧) be continuous in a simply connected and suppose that ∮ 𝑓(𝑧)𝑑𝑧 = 0 around every simple closed curve C in R. Then 𝑓(𝑧) is analytic. This is converse of Cauchy’s theorem. Example. 1. Evaluate ∫ 𝑧∗ 𝑑𝑧 for the curve 𝐶 = 𝐶1 − 𝐶2 𝐶 ∫ 𝑧∗𝑑𝑧 = ∫ (𝑥 − 𝑖𝑦)(𝑑𝑥 + 𝑖𝑑𝑦) 𝐶1−𝐶2 𝐶1− 𝐶2 1 1 = ∫𝑥=0 𝑥𝑑𝑥 + ∫𝑦= (1 − 𝑖𝑦)(𝑖 𝑑𝑦) 0 = 1 + 𝑖 ∫ 𝑧∗𝑑𝑧 = ∫ 1 (𝑥 − 𝑖𝑥)(𝑑𝑥 + 𝑖𝑑𝑥) 𝑥=0 𝐶3 = 1 Since 𝑧∗ is not analytic, the results are not same. 𝑢𝑥 = 𝑣𝑦 and 𝑢𝑦 = −𝑣𝑥 are not satisfied for 𝑓(𝑧) = 𝑧 ∗. Then f (z) not exist. does Joint initiative of IITs and IISc – Funded by MHRD Page 25 of 66
  • 2. NPTEL – Physics – Mathematical Physics - 1 Example.2. Evaluate ∫ 1 𝐶 𝑧 𝑑𝑧 for (a) a simple contour C not enclosing the origin. (b) a simple contour C enclosing the origin. (a) Because is analytic for all points (other then 𝑧 = 0), So 1 𝑧 ∫ 1 𝐶 𝑧 𝑑𝑧 = 0 (b) The contour can be deformed as above. In the limit of 𝑟 ⟶ 0 (of 𝐶1) and the lengths of 𝐿1 and 𝐿2 tending to zero, we have a closed curve. 𝐶 = 𝐶2 + 𝐿1 + 𝐿2 − 𝐶1 1 Now as earlier ∫ 𝑧 𝑑𝑧 = 0 Joint initiative of IITs and IISc – Funded by MHRD Page 26 of 66
  • 3. NPTEL – Physics – Mathematical Physics - 1 as ∫𝐿1 + ∫𝐿2 = 0 (𝑧 = 𝑟𝑒𝑖𝜃 , 𝑑𝑧 = 𝑟𝑖𝑒𝑖𝜃 𝑑𝜃 ) 2𝜋 ∫ 𝑑𝑧 = ∫ 𝑑𝑧 = ∫ 𝑟−1 𝑒−𝑖𝜃𝑖𝑒𝑖𝜃𝑟𝑑𝜃 1 1 𝑧 𝐶2 𝐶1 𝑧 0 = 2𝜋𝑖 Thus the integral ∫ 1 𝑧 𝑑𝑧 around any closed curve that encloses the origin is zero. Consequences of Cauchy’s integral theorem 𝑏 1. If 𝑓(𝑧) is analytic in a simply connected region R, prove that ∫ 𝑓(𝑧)𝑑𝑧 is 𝑎 independent of the path in R joining any two points. A and B in R. 2. Let 𝑓(𝑧) be analytic in a region R bounded by two simple closed curves 𝐶1and 𝐶2 and also on 𝐶1, 𝐶2. Prove that ∮𝐶 𝑓(𝑧)𝑑𝑧 = ∮𝐶 𝑓(𝑧)𝑑𝑧 1 2 Since 𝑓(𝑧) is analytic everywhere in R, ∫ 𝐴𝐸𝐹𝐺𝐻𝐸𝐴𝐷𝐶𝐵𝐴 𝑓(𝑧)𝑑𝑧 = 0 ∫ 𝑓(𝑧)𝑑𝑧 + ∫ 𝑓(𝑧)𝑑𝑧 + ∫ 𝑓(𝑧)𝑑𝑧 + 𝐴𝐸 𝐸𝐹𝐺𝐻 𝐸𝐴 ∫ 𝑓(𝑧)𝑑𝑧 = 0 𝐴𝐷𝐶𝐵𝐴 Thus, ∫𝐸𝐹𝐺𝐻 𝑓(𝑧)𝑑𝑧 = − ∫𝐴𝐷𝐶𝐵𝐴 𝑓(𝑧)𝑑𝑧 ∮𝐶 𝑓(𝑧)𝑑𝑧 = ∮𝐶 𝑓(𝑧)𝑑𝑧 1 2 Joint initiative of IITs and IISc – Funded by MHRD Page 27 of 66
  • 4. NPTEL – Physics – Mathematical Physics - 1 Prove Cauchy’s Theorem (Cauchy Goursat theorem) The theorem states that, ∮𝐶 𝑓(𝑧)𝑑𝑧 = 0, if f(z) is analytic with derivatives 𝑓′(𝑧) which is continuous at all points inside and on the simple closed curve C. 𝑓(𝑧) = 𝑢 + 𝑖𝑣 is analytic and has a continuous derivative. 𝑓́(𝑧) = 𝜕𝑢 + 𝑖 𝜕𝑣 = 𝜕𝑣 − 𝑖 𝜕𝑢 𝜕𝑥 𝜕𝑥 𝜕𝑦 𝜕𝑦 It follows that the partial derivatives, 𝜕𝑢 = 𝜕𝑣 , 𝜕𝑥 𝜕𝑦 𝜕𝑥 𝜕𝑦 and 𝜕𝑣 = − 𝜕𝑢 are continuous inside and on C. Thus, ∮ 𝑓(𝑧)𝑑𝑧 = ∮𝐶 (𝑢 + 𝑖𝑣)(𝑑𝑥 + 𝑖𝑑𝑦) = ∮(𝑢𝑑𝑥 − 𝑣𝑑𝑦) + 𝑖 ∮𝐶 (𝑣𝑑𝑥 + 𝑢𝑑𝑦) Using Green’s theorem, ∫ (− 𝜕𝑣 − 𝜕𝑢 ) 𝑑𝑥𝑑𝑦 + 𝑖 ∫ ( 𝜕𝑢 − 𝜕𝑣 ) 𝑑𝑥𝑑𝑦 𝑅 𝜕𝑥 𝜕𝑦 𝑅 𝜕𝑥 𝜕𝑦 = 0 (Using CR Condition) Cauchy’s Integral formula If 𝑓(𝑧) is analytic inside and on the boundary C of a simply connected region R, prove the following, 𝑓(𝑎) = 1 𝑓(𝑧) ∮ 𝑑𝑧 (Cauchy’s Integral formula) 2𝜋𝑖 𝐶 (𝑧−𝑎) The function is analytic inside R and on C excepting the point. 𝑧 = 𝑎 𝑓(𝑧) 𝑧−𝑎 ∮ 𝑓(𝑧) 𝐶 𝑧−𝑎 Γ 𝑧−𝑎 𝑑𝑧 = ∮ 𝑑𝑧 𝑓(𝑧) (1) The equation for Γ is |𝑧 − 𝑎| = 𝜖 Joint initiative of IITs and IISc – Funded by MHRD Page 28 of 66
  • 5. NPTEL – Physics – Mathematical Physics - 1 so, 𝑧 − 𝑎 = 𝜖𝑒𝑖𝜃, 0 ≤ 𝜃 < 2𝜋 𝑧 − 𝑎 Substituting 𝑧 = 𝑎 + 𝜖𝑒𝑖𝜃, 𝑑𝑧 = 𝑖𝜖𝑒𝑖𝜃𝑑𝜃 2𝜋 ∮ Γ 𝑓(𝑧) 𝑑𝑧 = ∫ 0 𝑓(𝑎 + 𝜖𝑒𝑖𝜃 )𝑖𝜖𝑒𝑖 𝜃 𝜖𝑒𝑖 𝜃 𝑑𝜃 2𝜋 = i∫ 𝑓(𝑎 + 𝜖𝑒𝑖𝜃)𝑑𝜃 0 (2) Thus using (1) ∮ 𝑓(𝑧) 𝐶 𝑧−𝑎 0 𝑑𝑧 = 𝑖 ∫ 𝑓(𝑎 + 𝜖𝑒𝑖𝜃 )𝑑 𝜃 2𝜋 Taking limit 𝜖 → 0 (remember 𝑓(𝑧) is continuous). ∮ 𝐶 𝑓(𝑧)𝑑𝑧 𝑧 − 𝑎 = 𝐿𝑖𝑚 𝑖 ∫ 𝑓(𝑎 + 𝜖𝑒𝑖𝜃)𝑑𝜃 = 𝑖 ∫ 𝑓(𝑎)𝑑𝜃 𝜖→0 2𝜋 2𝜋 0 0 = 2𝜋𝑖𝑓(𝑎) Example: If 𝑓(𝑧) is analytic inside and on the boundary C of a simply connected region R, prove that, 𝑓′(𝑎) = ∮ 1 𝑓(𝑧) 2𝜋𝑖 (𝑧 − 𝑎)2 𝑐 𝑑𝑧 𝑓′(𝑎) = 𝐿𝑖𝑚 𝑓(𝑎+ℎ)−𝑓(𝑎) ℎ→0 ℎ Consider both the points 𝑎 and 𝑎 + ℎ are inside the circle of radius 𝜖. Joint initiative of IITs and IISc – Funded by MHRD Page 29 of 66
  • 6. NPTEL – Physics – Mathematical Physics - 1 𝑓′(𝑎) = ∮ [ 1 1 1 1 2𝜋𝑖 ℎ 𝑧 − (𝑎 + ℎ) 𝑧 − 𝑎 𝑐 − ] 𝑓(𝑧)𝑑𝑧 = 1 𝑓(𝑧)𝑑 𝑧 2𝜋𝑖 𝑐 (𝑧−𝑎−ℎ)(𝑧−𝑎) ∮ The result follows as ℎ → 0. Important formula If 𝑓(𝑧) is analytic inside and on a simple closed curve 𝐶 except for a pole of order m at 𝑧 = 𝑎, inside 𝐶, prove that 1 1 2𝜋𝑖 ∮ 𝑓(𝑧)𝑑𝑧 = 𝐿𝑡 𝑐 𝑧→𝑎 (𝑚 − 1)! 𝑑𝑧𝑚−1 𝑑𝑚 [(𝑧 − 𝑎)𝑚𝑓(𝑧)] also for two different poles of order 𝑚1 and 𝑚2, 1 1 2𝜋𝑖 ∮ 𝑓(𝑧)𝑑𝑧 = 𝐿𝑡 𝑧→𝑎1 (𝑚1 − 1)! 𝑑𝑧𝑚1−1 𝑐 𝑑𝑚1 [(𝑧 − 𝑎)𝑚1 𝑓(𝑧)] + 𝐿𝑡 𝑧→𝑎2 (𝑚2 − 1)! 𝑑𝑧𝑚2−1 Joint initiative of IITs and IISc – Funded by MHRD Page 30 of 66 1 𝑑𝑚2 [(𝑧 − 𝑎)𝑚2 𝑓(𝑧)] A similar formula can be worked out for more poles.