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Cauchy's Theorem

5.1 Statement

Theorem 5.1 (Cauchy”s Theorem). If ff is analytic on a connected domain DD and γ\gamma Is a simple closed contour in DDThen

γf(z)dz=0\int_\gamma f(z)\, dz = 0

Proof (for ff' continuous). By Green’s theorem in the plane, writing f=u+ivf = u + iv:

γfdz=γ(udxvdy)+iγ(vdx+udy)\int_\gamma f\, dz = \int_\gamma (u\, dx - v\, dy) + i\int_\gamma (v\, dx + u\, dy)

Applying Green’s theorem to each integral:

=D(vxuy)dA+iD(uxvy)dA=0= \iint_D (-v_x - u_y)\, dA + i\iint_D (u_x - v_y)\, dA = 0

By the Cauchy-Riemann equations. \blacksquare

5.2 Connected Domains

A domain DCD \subseteq \mathbb{C} is ** connected** if every simple closed contour in DD can Be continuously shrunk to a point within DD.

Cauchy’s theorem may fail on multiply connected domains. For example, γ1zdz=2πi\int_\gamma \frac{1}{z}\, dz = 2\pi i where γ\gamma is the unit circle (traversing a region that Excludes the singularity at z=0z = 0).

5.3 Path Independence

Corollary 5.2. If ff is analytic on a connected domain DDThen the integral z0z1f(z)dz\int_{z_0}^{z_1} f(z)\, dz is independent of the path from z0z_0 to z1z_1 in DD.

5.4 Antiderivatives

Theorem 5.3. If ff is analytic on a connected domain DDThen ff has an antiderivative FF in DD (i.e., F(z)=f(z)F'(z) = f(z)), and

γf(z)dz=F(z1)F(z0)\int_\gamma f(z)\, dz = F(z_1) - F(z_0)

Where z0z_0 and z1z_1 are the endpoints of γ\gamma.

5.5 Cauchy’s Theorem for Multiply Connected Domains

Theorem 5.4. If ff is analytic on a domain DD containing simple closed contours γ,γ1,,γn\gamma, \gamma_1, \ldots, \gamma_n where γ1,,γn\gamma_1, \ldots, \gamma_n Lie in the interior of γ\gamma and the region between γ\gamma and the γk\gamma_k is contained in DD And all contours are positively oriented, then

γf(z)dz=k=1nγkf(z)dz\int_\gamma f(z)\, dz = \sum_{k=1}^n \int_{\gamma_k} f(z)\, dz

5.6 Deformation of Contours

Theorem 5.5 (Deformation of Contours). If ff is analytic on a domain containing two simple Closed contours γ1\gamma_1 and γ2\gamma_2 where one can be continuously deformed into the other Within the domain of analyticity of ffThen

γ1f(z)dz=γ2f(z)dz\int_{\gamma_1} f(z)\, dz = \int_{\gamma_2} f(z)\, dz

Proof. This follows directly from Theorem 5.4 applied to the region between γ1\gamma_1 and γ2\gamma_2. \blacksquare

Remark. This theorem is enormously useful: we can replace a complicated contour with a simpler one (a small circle around each singularity) without changing the value of the integral.

Solution

Problem. Evaluate γdzz2\int_\gamma \frac{dz}{z - 2} where γ\gamma is the ellipse x24+y29=1\frac{x^2}{4} + \frac{y^2}{9} = 1.

Since z=2z = 2 is inside the ellipse and 1z2\frac{1}{z - 2} is analytic everywhere else, By deformation of contours we can replace γ\gamma with a small circle around z=2z = 2:

γdzz2=2πi\int_\gamma \frac{dz}{z - 2} = 2\pi i.

Problem. Evaluate γezzdz\int_\gamma \frac{e^z}{z}\, dz where γ\gamma is the square with vertices ±2±2i\pm 2 \pm 2i.

ezz\frac{e^z}{z} is analytic on and inside γ\gamma except at z=0z = 0. By deformation: γezzdz=z=rezzdz=2πie0=2πi\int_\gamma \frac{e^z}{z}\, dz = \int_{|z|=r} \frac{e^z}{z}\, dz = 2\pi i \cdot e^0 = 2\pi i.

Problem. Evaluate γdzz21\int_\gamma \frac{dz}{z^2 - 1} where γ\gamma is z=2|z| = 2.

1z21=12(1z11z+1)\frac{1}{z^2 - 1} = \frac{1}{2}\left(\frac{1}{z-1} - \frac{1}{z+1}\right).

Both z=±1z = \pm 1 are inside z=2|z| = 2.

γdzz21=12(2πi2πi)=0\int_\gamma \frac{dz}{z^2 - 1} = \frac{1}{2}(2\pi i - 2\pi i) = 0.