Spring 2015 - Problem 9

conformal mappings, harmonic functions

Let Ω={zCz>1 and Rez>2}\Omega = \set{z \in \C \mid \abs{z} > 1 \text{ and } \Re{z} > -2}. Suppose u ⁣:ΩR\func{u}{\cl{\Omega}}{\R} is bounded, continuous, and harmonic on Ω\Omega and also that u(z)=1u\p{z} = 1 when z=1\abs{z} = 1 and that u(z)=0u\p{z} = 0 when Rez=2\Re{z} = -2. Determine u(2)u\p{2}.

Solution.

First, consider the conformal map z1zz \mapsto \frac{1}{z}. This fixes the unit circle, and it maps the line Rez=2\Re{z} = -2 to the line containing

12,12+i=2i5,and1=0.-\frac{1}{2}, \quad \frac{1}{-2 + i} = \frac{-2 - i}{5}, \quad\text{and}\quad \frac{1}{\infty} = 0.

This is the circle centered at z=14z = -\frac{1}{4} and with radius 14\frac{1}{4}. Thus, we have an annular region, but the circles are not concentric. To fix this, we will apply a Blaschke factor, which is a Möbius transformation fixing the unit disk of the form

φ(z)=zα1αz.\phi\p{z} = \frac{z - \alpha}{1 - \conj{\alpha}z}.

By symmetry, we need to map 12r-\frac{1}{2} \mapsto -r and 0r0 \mapsto r, where r>0r > 0 will be the radius of the resulting inner circle. We also expect αR\alpha \in \R, so we get the system

φ(12)=12α1+12α=12α2+α=r,φ(0)=α=r.\begin{gathered} \phi\p{-\frac{1}{2}} = \frac{-\frac{1}{2} - \alpha}{1 + \frac{1}{2}\conj{\alpha}} = \frac{-1 - 2\alpha}{2 + \alpha} = -r, \\ \phi\p{0} = -\alpha = r. \end{gathered}

Substituting, we get

12α=α(2+α)    4α+α2=1    α{23,2+3}.-1 - 2\alpha = \alpha\p{2 + \alpha} \implies 4\alpha + \alpha^2 = -1 \implies \alpha \in \set{-2 - \sqrt{3}, -2 + \sqrt{3}}.

Since αD\alpha \in \D, we see that α=2+3\alpha = -2 + \sqrt{3} is the correct choice, and so φ\phi maps z+14=14\abs{z + \frac{1}{4}} = \frac{1}{4} to the circle of radius 232 - \sqrt{3} centered at the origin. From here, we see

v(z)=logz/rlog1/rv\p{z} = \frac{\log{\abs{z}}/r}{\log{1/r}}

satisfies f(z)=0f\p{z} = 0 on the inner circle z=r\abs{z} = r and that f(z)=1f\p{z} = 1 on the unit circle. Thus, v(z)=u(1φ1(z))v\p{z} = u\p{\frac{1}{\phi^{-1}\p{z}}} on z=r\abs{z} = r and z=1\abs{z} = 1, so because these are both harmonic functions, we see that

u(z)=(vφ)(1z)=1log1/rlog1+rzrz+r2u\p{z} = \p{v \circ \phi}\p{\frac{1}{z}} = \frac{1}{\log{1/r}} \log\,\abs{\frac{1 + rz}{rz + r^2}}

which gives

u(2)=1log1/rlog1+2r2r+r2.u\p{2} = \frac{1}{\log{1/r}} \log\,\abs{\frac{1 + 2r}{2r + r^2}}.