← 2022 Paper 2

UPSC 2022 Maths Optional Paper 2 Q1b — Step-by-Step Solution

10 marks · Section A

Harmonic functions and harmonic conjugate · Complex Analysis · asked 7× in 13 yrs · Read the full method →

Question

If f(z)=u+ivf(z)=u+iv is analytic and uv=cosx+sinxey2cosxeyeyu-v=\dfrac{\cos x+\sin x-e^{-y}}{2\cos x-e^y-e^{-y}}, find f(z)f(z) subject to f(π/2)=0f(\pi/2)=0.

Technique

Milne-Thomson method on g(z)=(1i)f(z)g(z)=(1-i)f(z) where g=uv\Re g=u-v; restrict to y=0y=0, simplify with half-angle identities; analytically continue to recover g(z)g(z).

Solution

Strategy. Use Milne-Thomson’s method: if f(z)=u+ivf(z)=u+iv is analytic, then f(z)=ux+ivx=uxiuyf'(z)=u_x+iv_x=u_x-iu_y (using CR equations).

Let ψ(x,y)=uv\psi(x,y)=u-v. We can construct (1i)f(z)=uv+i(u+v)(1-i)f(z)=u-v+i(u+v). So define g(z)=(1i)f(z)g(z)=(1-i)f(z), with g=uv\Re g=u-v and g=u+v\Im g=u+v.

Alternative cleaner approach: Let U=uvU=u-v, V=u+vV=u+v (the real and imaginary parts of (1i)f(1-i)f). The function (1i)f(1-i)f is analytic, so UU is harmonic and VV is its conjugate.

Given U=cosx+sinxey2cosxeyeyU=\dfrac{\cos x+\sin x-e^{-y}}{2\cos x-e^y-e^{-y}}.

Simplify denominator: 2cosxeyey=2cosx2coshy=2(cosxcoshy)2\cos x-e^y-e^{-y}=2\cos x-2\cosh y=2(\cos x-\cosh y).

Numerator: cosx+sinxey\cos x+\sin x-e^{-y}.

So U=cosx+sinxey2(cosxcoshy)U=\dfrac{\cos x+\sin x-e^{-y}}{2(\cos x-\cosh y)}.

Step 1 — Apply Milne-Thomson to g(z)=(1i)f(z)g(z)=(1-i)f(z)

g(z)=UxiUyg'(z)=U_x-i U_y (using CR on gg).

We need Ux,UyU_x,U_y at y=0y=0 (where the formula reduces to a function of xx alone).

At y=0y=0: cosh0=1\cosh 0=1, e0=1e^{0}=1. So U(x,0)=cosx+sinx12(cosx1)U(x,0)=\dfrac{\cos x+\sin x-1}{2(\cos x-1)}.

Simplify: numerator =cosx1+sinx=2sin2(x/2)+2sin(x/2)cos(x/2)=2sin(x/2)[cos(x/2)sin(x/2)]=\cos x-1+\sin x=-2\sin^2(x/2)+2\sin(x/2)\cos(x/2)=2\sin(x/2)[\cos(x/2)-\sin(x/2)].

Denominator: 2(cosx1)=2[2sin2(x/2)]=4sin2(x/2)2(\cos x-1)=2[-2\sin^2(x/2)]=-4\sin^2(x/2).

U(x,0)=2sin(x/2)[cos(x/2)sin(x/2)]4sin2(x/2)=cos(x/2)sin(x/2)2sin(x/2)=sin(x/2)cos(x/2)2sin(x/2)=12cos(x/2)2sin(x/2)=1212cot(x/2)U(x,0)=\dfrac{2\sin(x/2)[\cos(x/2)-\sin(x/2)]}{-4\sin^2(x/2)}=\dfrac{\cos(x/2)-\sin(x/2)}{-2\sin(x/2)}=\dfrac{\sin(x/2)-\cos(x/2)}{2\sin(x/2)}=\dfrac{1}{2}-\dfrac{\cos(x/2)}{2\sin(x/2)}=\dfrac{1}{2}-\dfrac{1}{2}\cot(x/2).

So U(x,0)=1212cot(x/2)U(x,0)=\dfrac{1}{2}-\dfrac{1}{2}\cot(x/2).

Step 2 — Construct g(z)g(z) via Milne-Thomson

Since g(z)g(z) on the real axis (y=0y=0) equals U(x,0)+iV(x,0)U(x,0)+iV(x,0), and we want to identify the analytic function whose real part on the real axis matches U(x,0)U(x,0).

By Milne-Thomson: g(z)=U(z,0)iUy(z,0)dzg(z)=U(z,0)-i\int U_y(z,0)\,dz… but actually the simpler version is:

If U(x,y)=gU(x,y)=\Re g, replace xz,  y0x\to z,\;y\to 0 to get g(z)g(z) on the real axis. For analytic functions, the formula extends.

g(z)=U(z,0)g(z)=U(z,0) formally (where the formula U(x,0)U(x,0) is analytically continued to complex zz).

g(z)=1212cot(z/2)g(z)=\dfrac{1}{2}-\dfrac{1}{2}\cot(z/2).

(Note: this gives gg up to an additive imaginary constant, which we’ll fix using the initial condition.)

Step 3 — Recover f(z)f(z)

g(z)=(1i)f(z)f(z)=g(z)1i=g(z)(1+i)2g(z)=(1-i)f(z)\Rightarrow f(z)=\dfrac{g(z)}{1-i}=\dfrac{g(z)(1+i)}{2}.

f(z)=(1+i)2 ⁣[1212cot(z/2)]=1+i4[1cot(z/2)].f(z)=\dfrac{(1+i)}{2}\!\left[\dfrac{1}{2}-\dfrac{1}{2}\cot(z/2)\right]=\dfrac{1+i}{4}[1-\cot(z/2)].

Step 4 — Apply initial condition f(π/2)=0f(\pi/2)=0

f(π/2)=1+i4[1cot(π/4)]=1+i4[11]=0f(\pi/2)=\dfrac{1+i}{4}[1-\cot(\pi/4)]=\dfrac{1+i}{4}[1-1]=0 ✓.

So the additive constant is 00:

Answer

  f(z)=1+i4[1cot(z/2)].  \boxed{\;f(z)=\dfrac{1+i}{4}[1-\cot(z/2)].\;}
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