Cauchy's Integral Theorem | Mathquery
Cauchy's Integral Theorem:
Statement :
The theorem is usually formulated for closed paths as follows :
Let U be an open subset of C which is simply connected . Let f: U-->C be a holomorphic function , and let γ be a rectifiable path in U whose start point is equal to its end point . Then
∮ f(z) dz = 0
γ
∮ f(z) dz = 0
γ
Proof :
Let us assume that the partial derivatives of a holomorphic function are continuous , the Cauchy Integral Theorem can be proved as direct sequence of Green's Theorem and the fact that the real and imaginary parts of f = u + i v must satisfy the Cauchy - Riemann equations in the region bounded by γ , and moreover in the open neighbourhood U of this region.
Cauchy provided this proof , but it was later proved by Goursat without requiring techniques from vector calculus , or the continuity of partial derivatives .
Cauchy provided this proof , but it was later proved by Goursat without requiring techniques from vector calculus , or the continuity of partial derivatives .
We can break the integrand f , as well as the differential dz into their real and imaginary components .
f = u + i v ..............(1)
dz = dx + i dy .............(2)
Then we have
∮ f(z) dz = ∮ (u+iv)(dx+idy)
γ γ
= ∮(u dx - v dy)+i∮(v dx + u dy)
γ γ ........(3)
By Green's Theorem , we then replace the integrals around the closed contour γ with an area integral throughout the domain D that is enclosed by γ as follows.
∮(u dx - v dy) = ∫∫(-∂v/∂x - ∂u/∂y) dx dy
γ D ............(4)
∮(v dx + u dy) = ∫∫(∂u/∂x - ∂v/∂y) dx dy
γ D ............(5)
But the real and imaginary parts of a function holomorphic in the domain D , u and v must satisfy the Cauchy-Riemann equations so ,
∂u/∂x = ∂v/∂y ..............(6)
∂u/∂y = -∂v/∂x .............(7)
We therefore find that both integrands are zero
∫∫(-∂v/∂x - ∂u/∂y) dx dy
D
= ∫∫(∂u/∂y - ∂u/∂y) dx dy =0
D ...........(8)
∫∫(∂u/∂x - ∂v/∂y) dx dy
D
= ∫∫(∂u/∂x - ∂u/∂x) dx dy
D .............(9)
This gives the desired result
∮ f(z) dz = 0 ...............(10)
γ (Proved)
γ γ
= ∮(u dx - v dy)+i∮(v dx + u dy)
γ γ ........(3)
By Green's Theorem , we then replace the integrals around the closed contour γ with an area integral throughout the domain D that is enclosed by γ as follows.
∮(u dx - v dy) = ∫∫(-∂v/∂x - ∂u/∂y) dx dy
γ D ............(4)
∮(v dx + u dy) = ∫∫(∂u/∂x - ∂v/∂y) dx dy
γ D ............(5)
But the real and imaginary parts of a function holomorphic in the domain D , u and v must satisfy the Cauchy-Riemann equations so ,
∂u/∂x = ∂v/∂y ..............(6)
∂u/∂y = -∂v/∂x .............(7)
We therefore find that both integrands are zero
∫∫(-∂v/∂x - ∂u/∂y) dx dy
D
= ∫∫(∂u/∂y - ∂u/∂y) dx dy =0
D ...........(8)
∫∫(∂u/∂x - ∂v/∂y) dx dy
D
= ∫∫(∂u/∂x - ∂u/∂x) dx dy
D .............(9)
This gives the desired result
∮ f(z) dz = 0 ...............(10)
γ (Proved)
Example :
Prove that ∫ eᶻ dz = 0
c
Solution :
Here f(z) = eᶻ = e^(x+iy) (∵ In complex
z = x+iy)
= e^x . e^ iy
= e^x (cos y + i sin y)
(∵ polar form of
complex function)
= e^x cos y + i e^x sin y
= u + iv
where u = e^x cosy v= e^x sin y
∂u/∂x = e^x cosy ∂v/∂x = e^x sin y
∂u/∂y = -e^x sin y ∂v/∂y = e^x cos y
∴ ∂u/∂x = ∂v/∂y and ∂u/∂y = - ∂v/∂x
⇒ f(z) = eᶻ satisfy C-R equation
⇒ eᶻ is analytic for all z .
So ∫ eᶻ dz = 0 by Cauchy's Integral Theorem
c
Which is the required solution .
About Scientist :-
Baron Augustin-Louis Cauchy (21 August 1789 – 23 May 1857) was a French mathematician, engineer, and physicist who made pioneering contributions to several branches of mathematics, including mathematical analysis and continuum mechanics .For More
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