Processing math: 51%
PHYS20672 Summary 2
Conformal mappings
- If u(x,y)+iv(x,y) is an analytic function of z=x+iy,
contours of constant u and v intersect each other at right
angles in the z-plane at every point where f′(z)≠0.
- If f is analytic, the mapping w=f(z) preserves angles
and, for sufficiently small regions, shapes, wherever
f′(z)≠0. The mapping is called conformal.
- Suppose we wish to find u(x,y), the solution to Laplace's
equation ∇2u=0 subject to certain boundary conditions,
and that the mapping Z=X+iY=f(z) maps the boundaries to a
new, simpler geometry in which Laplace's equation can be
solved to give the potential function Φ(X,Y). Then
u(x,y)=Φ(X(x,y),Y(x,y)) will be the solution to the
original problem.
- If Ψ(X,Y) is conjugate to Φ(X,Y) (i.e., if
Φ+iΨ is an analytic function of Z=X+iY), lines
of constant v(x,y)=Ψ(X(x,y),Y(x,y)) represent field
lines, lines of heat flow or streamlines according to the
physical interpretation of the function u(x,y). The analytic
function u+iv is called the "complex potential".

In the diagrams above, the coloured lines are equipotentials
and flow/field lines for a variety of problems.
Spiegel 8.1-8.3, 9.1-3, 9.6, 9.7-12, 9.15-18, 9.22-23
Riley 18.7-9; Boas 14.9, 14.10; (Arfken 6.7)
Integration in the complex plane
- The path (or contour) integral of a complex function is
defined as ∫Cf(z)dz=lim where z_0 and z_n are the
end-points of the contour, the other z_k are points
distributed in order along the contour, and the points \xi_k
are chosen to lie between z_{k-1} and z_k on the contour.
Provided f(z) is continuous and the limit is taken so that
all (z_k-z_{k-1})\to 0, the limit is unique for a given
path.
- For real functions of x only, this corresponds to the
usual (Riemann) integral, i.e. the area under the curve
f(x).
- We have
\int_C f(z)\,\d z=\int u\,\d x-\int v\,\d y+\ii\int v\,\d x+\ii\int
u\,\d y=\int(u,-v)\cdot\d\mathbf{r}+\ii\int(v,u)\cdot\d\mathbf{r},
where \d\mathbf{r}\equiv(\d x,\d y). The last two integrals
are real line integrals in the xy-plane.
- Reversing the direction of the contour changes the sign of the integral.
- For compound curves,
\int_{C_1+C_2} f(z)\,\d z=\int_{C_1} f(z)\,\d z+\int_{C_2} f(z)\,\d
z\qquad\text{and}\qquad\int_{C_1-C_2} f(z)\,\d z=\int_{C_1} f(z)\,\d
z-\int_{C_2} f(z)\,\d z.
- The estimation lemma states |\int_C f(z)\,\d z|\le ML
where L is the length of the curve and M is the maximum
value of |f(z)| along the curve.
- A Jordan curve is a closed, non-self-intersecting curve.
The integral along such a curve is denoted by \oint, and is
taken in an anticlockwise direction by default.
Spiegel 4.1-4.4, 4.7-8
Riley 18.10; (Boas 14.3); Arfken 6.3