5.1 Statement
Theorem 5.1 (Cauchy”s Theorem). If f is analytic on a connected domain D and γ Is a simple closed contour in DThen
∫γf(z)dz=0
Proof (for f′ continuous). By Green’s theorem in the plane, writing f=u+iv:
∫γfdz=∫γ(udx−vdy)+i∫γ(vdx+udy)
Applying Green’s theorem to each integral:
=∬D(−vx−uy)dA+i∬D(ux−vy)dA=0
By the Cauchy-Riemann equations. ■
5.2 Connected Domains
A domain D⊆C is ** connected** if every simple closed contour in D can Be continuously shrunk to a point within D.
Cauchy’s theorem may fail on multiply connected domains. For example, ∫γz1dz=2πi where γ is the unit circle (traversing a region that Excludes the singularity at z=0).
5.3 Path Independence
Corollary 5.2. If f is analytic on a connected domain DThen the integral ∫z0z1f(z)dz is independent of the path from z0 to z1 in D.
5.4 Antiderivatives
Theorem 5.3. If f is analytic on a connected domain DThen f has an antiderivative F in D (i.e., F′(z)=f(z)), and
∫γf(z)dz=F(z1)−F(z0)
Where z0 and z1 are the endpoints of γ.
5.5 Cauchy’s Theorem for Multiply Connected Domains
Theorem 5.4. If f is analytic on a domain D containing simple closed contours γ,γ1,…,γn where γ1,…,γn Lie in the interior of γ and the region between γ and the γk is contained in D And all contours are positively oriented, then
∫γf(z)dz=∑k=1n∫γkf(z)dz
Theorem 5.5 (Deformation of Contours). If f is analytic on a domain containing two simple Closed contours γ1 and γ2 where one can be continuously deformed into the other Within the domain of analyticity of fThen
∫γ1f(z)dz=∫γ2f(z)dz
Proof. This follows directly from Theorem 5.4 applied to the region between γ1 and γ2. ■
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 ∫γz−2dz where γ is the ellipse 4x2+9y2=1.
Since z=2 is inside the ellipse and z−21 is analytic everywhere else, By deformation of contours we can replace γ with a small circle around z=2:
∫γz−2dz=2πi.
Problem. Evaluate ∫γzezdz where γ is the square with vertices ±2±2i.
zez is analytic on and inside γ except at z=0. By deformation: ∫γzezdz=∫∣z∣=rzezdz=2πi⋅e0=2πi.
Problem. Evaluate ∫γz2−1dz where γ is ∣z∣=2.
z2−11=21(z−11−z+11).
Both z=±1 are inside ∣z∣=2.
∫γz2−1dz=21(2πi−2πi)=0.