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GraduateComplex AnalysisIntegration in the Complex Plane


Cauchy’s Theorem


Cauchy's theorem is a fundamental result in complex analysis, a branch of mathematics that deals with functions of a complex variable. This theorem plays a central role in the theory of analytic functions and has many profound implications, especially in the evaluation of integrals in the complex plane.

Understanding the Cauchy theorem

Cauchy's theorem essentially states that if we have a complex-valued function f(z) that is analytic on and inside some closed contour C in the complex plane, then the integral of f(z) around C is zero. Mathematically, this is expressed as:

c f(z) dz = 0

Here, ∮ C represents the line integral around the closed contour C, and f(z) is the function being integrated. The function must be analytic, which means that it is differentiable at every point in its domain in the complex plane.

This theorem can be viewed as the complex-plane counterpart to the fundamental theorem of calculus. The key aspect is that, under the conditions of the theorem, the integral of f(z) over a contour is zero as long as f(z) is analytic.

Contours in the complex plane

A contour line is a piecewise smooth, closed curve in the complex plane. This is an essential aspect of Cauchy's theorem, since the theorem applies to contour lines where the function f(z) is analytic inside and on this curve.

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Analytical functions

An analytic function (also called holomorphic) is a function that is locally given by a convergent power series. For the function f(z) = u(x, y) + iv(x, y), where u and v are real-valued functions, f(z) is analytic in an open set if it satisfies the Cauchy–Riemann equations:

∂u/∂x = ∂v/∂y
∂u/∂y = -∂v/∂x

This implies that the function f(z) has continuous partial derivatives and can be differentiated as a complex function.

Simple example and illustration

Example 1: static function

Consider the simplest example, a constant function f(z) = 1 If we integrate this function over some closed contour C, then the integral is:

c 1 dz = 0

This result makes intuitive sense, since moving around a contour in the complex plane is the same as moving around a complete circle, and the result of integrating a constant function over such a loop is zero.

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Example 2: f(z) = z

Now, consider the function f(z) = z. Again using Cauchy's theorem, if C encloses any part where f(z) is analytic, then we get:

c z dz = 0

This result arises from the fact that linear transformations preserve accretion symmetry about analytic paths.

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More formal proof

A more formal proof of Cauchy's theorem uses Green's theorem from vector calculus. We establish the relation by converting the line integral over the region enclosed by the contour into a double integral.

The proof involves important steps:

  1. Start by expressing the line integral of f(z) as follows:
  2. C f(z) dz = ∮ C (u + iv)(dx + i dy)
        
  3. Using the parameterization with z(t) = x(t) + iy(t), express the difference dz as:
  4. dz = (dx/dt + idy/dt)dt
        
  5. Applying Green's theorem, which relates the line integral around a closed curve to the double integral over the plane region bounded by the curve, we can express it as:
  6. C u dx + v dy = ∬ R (∂v/∂x – ∂u/∂y) dx dy
        
  7. Because f(z) is analytic, the partial derivatives ∂u/∂y and ∂v/∂x cancel according to the Cauchy–Riemann equations, giving:
  8. ∂v/∂x - ∂u/∂y = 0
        
  9. Thus, we conclude:
  10. c f(z) dz = 0
        

Applications of Cauchy theorem

Cauchy's theorem serves as the basis for many other powerful results in complex analysis, including Cauchy's integral formula, the residue theorem, and the concept of analyticity. In physics and engineering, this theorem helps solve problems related to fluid dynamics, electromagnetism, and other fields dealing with complex potentials.

Example 3: Applications in electromagnetism

Consider a problem where the electric field is defined by a complex potential function that is analytic. Using Cauchy's theorem allows us to directly evaluate interactions about closed paths, giving insight into potential fields:

C e(z) dz = 0

where E(z) is the electric field represented as a complex function.

Conclusion

Cauchy's theorem is a cornerstone of complex analysis, stating that the path taken in evaluating an integral does not affect the result, provided the function is analytic. It underlines the importance of analyticity in the treatment of complex functions and highlights the usefulness of complex integration in practical applications.


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