Understanding Cauchy's Integral Theorem

In summary, a Jordan curve contained in a simply connected domain and bounded by a closed contour has a value of zero for the integral of the function over the contour.
  • #1
futurebird
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The Cauchy Integral Theorem says that given f(z), an analytic function in a simply connected domain D and C, a Jordan curve contained in D:

[tex]\int_{C}^{}f(z)dz=0[/tex]

The words "simply connected" are important because if the closed contour encloses points where the function is not analytic it may have a value other than zero.

There are a few things that confuse me here:

  1. Is a branch point always a point where the function is not analytic?
  2. Is a point where the function is undefined, that is not a branch point always a point where the function is not analytic?
  3. Intuitively, why should the integral be zero? Is it because the line integral of a complex function is summing up direction vectors at every point in the curve, and when you return to where you started on a closed curve you have essentially "not moved" so the sum of the direction vectors is zero?
  4. When a closed contour's integral has a value other than zero, is this ever related to the fact that you went over a branch cut? If not why will this happen?
 
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  • #2
1) Yes, at a branch point the function is not analytic.

2) Yes, if the function is not defined at a point then you cannot say that it is analytic at that point. It could be that you could define the function at that point in such a way that it would become analytical, but as long as you don't, it is not analytical.

3) What is the integral of a function along the real axis? If F is the antiderivative it is the difference of F at the end and starting point. You can think of the contour integral being zero as saying that an integral from z1 to z2 will yield the same value irrespective of which path is used (because the difference of the integral along two paths is a contour integral along a closed path which is zero). Now, fix a point z0 and define a function F(z) as some path integral from z0 to z. Now, what do you think is the derivative of F? :smile:

4) It will be more closely related to the fact that you went over a brach cut of F, not f. Example: evaluate the contour integral over the unit circle of the function [tex]\frac{1}{z}[/tex]. If we naively try to evaluate the integral using a antiderivative as I explained above you would get the difference of Log(z) at end and starting point. Now log has a brach cut singularity so the value jumps by [tex]2\pi i[/tex].
 
  • #3
Count Iblis said:
3) What is the integral of a function along the real axis? If F is the antiderivative it is the difference of F at the end and starting point. You can think of the contour integral being zero as saying that an integral from z1 to z2 will yield the same value irrespective of which path is used (because the difference of the integral along two paths is a contour integral along a closed path which is zero). Now, fix a point z0 and define a function F(z) as some path integral from z0 to z. Now, what do you think is the derivative of F? :smile:

f(x) right?

Are you saying that the entire complex plane is like a big real number line in 2D? That alomst makes sense, though I'm still having a hard time seeing why the integrals over paths that "look like differnt lengths" give the same result.

I mean, on the real line there is only one way to get fron 2.5 to -3.

So is it that there are many ways to get from 2 + 3i to 3 - i? ... I'm still not getting this...
 
  • #4
Yes, the derivative is f, you could try to prove it...

You can take any arbitrary path from 2 + 3i to 3 - i (not just a straight line) and the integral will be the same (if the function is analytic). It's just like the case of a conservative force field in physics, where the integral of the inner product of the force with the path length element along a path equals the potential energy difference at the end and starting points and is thus path independent.
 

FAQ: Understanding Cauchy's Integral Theorem

What is Cauchy's Integral Theorem?

Cauchy's Integral Theorem, also known as Cauchy's Residue Theorem, is a fundamental theorem in complex analysis that states that the value of a contour integral around a closed path in the complex plane is equal to the sum of the residues of the function inside the contour.

What is the significance of Cauchy's Integral Theorem?

Cauchy's Integral Theorem is significant because it allows for the evaluation of complex integrals using the residues of a function, which can be much simpler to calculate than the integral itself. It also has many applications in mathematics and physics, including in the study of complex functions and the behavior of electric fields.

How is Cauchy's Integral Theorem used in complex analysis?

In complex analysis, Cauchy's Integral Theorem is used to evaluate contour integrals, to find the zeros and poles of complex functions, and to prove other important theorems such as the Cauchy Integral Formula and the Cauchy-Riemann equations. It is also used in the study of analytic functions and their properties.

Can Cauchy's Integral Theorem be extended to higher dimensions?

Yes, Cauchy's Integral Theorem can be extended to higher dimensions through the use of the Cauchy Integral Formula for higher dimensions. This formula allows for the evaluation of integrals over arbitrary paths in higher dimensional spaces, and has many applications in complex analysis and differential geometry.

What are some common misconceptions about Cauchy's Integral Theorem?

One common misconception about Cauchy's Integral Theorem is that it only applies to functions that are analytic everywhere inside the contour. In reality, the theorem can still be used for functions with isolated singularities, as long as the contour does not enclose any of these singularities. Another misconception is that the Cauchy Integral Formula only applies to simple closed curves, when in fact it can be applied to any smooth, closed path in the complex plane.

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