← 2018 Paper 2

UPSC 2018 Maths Optional Paper 2 Q3b — Step-by-Step Solution

15 marks · Section A

Contour integration of real integrals using residues · Complex Analysis · asked 9× in 13 yrs · Read the full method →

Question

Show by applying the residue theorem that 0dx(x2+a2)2=π4a3, a>0\displaystyle\int_0^\infty\frac{dx}{(x^2+a^2)^2}=\frac{\pi}{4a^3},\ a>0.

Technique

Semicircular contour in the upper half-plane; residue at the order-2 pole z=iaz=ia via ddz[(zia)2f]\frac{d}{dz}[(z-ia)^2 f]; Jordan-type estimate kills the arc.

Solution

Step 1 — Symmetrize and set up the contour integral

The integrand is even, so

I=0dx(x2+a2)2=12dx(x2+a2)2.I=\int_0^\infty\frac{dx}{(x^2+a^2)^2}=\frac12\int_{-\infty}^{\infty}\frac{dx}{(x^2+a^2)^2}.

Consider f(z)=1(z2+a2)2=1(zia)2(z+ia)2f(z)=\dfrac{1}{(z^2+a^2)^2}=\dfrac{1}{(z-ia)^2(z+ia)^2} and integrate over the contour CR=[R,R]ΓRC_R=[-R,R]\cup\Gamma_R, where ΓR\Gamma_R is the upper semicircle z=R|z|=R. For a>0a>0 the poles are at z=±iaz=\pm ia, each of order 22; only z=iaz=ia lies in the upper half-plane (inside CRC_R for R>aR>a).

Step 2 — Vanishing of the arc

On ΓR\Gamma_R, z=R|z|=R gives z2+a2R2a2|z^2+a^2|\ge R^2-a^2, so

ΓRf(z)dzπR(R2a2)2R0,\left|\int_{\Gamma_R}f(z)\,dz\right|\le \frac{\pi R}{(R^2-a^2)^2}\xrightarrow[R\to\infty]{}0,

since the numerator grows like RR while the denominator grows like R4R^4. Hence the arc contributes nothing in the limit.

Step 3 — Residue at the double pole z=iaz=ia

For a pole of order 22,

Resz=iaf=limziaddz[(zia)2f(z)]=limziaddz1(z+ia)2.\operatorname*{Res}_{z=ia}f=\lim_{z\to ia}\frac{d}{dz}\Big[(z-ia)^2 f(z)\Big]=\lim_{z\to ia}\frac{d}{dz}\frac{1}{(z+ia)^2}.

Differentiate:

ddz(z+ia)2=2(z+ia)3.\frac{d}{dz}(z+ia)^{-2}=-2(z+ia)^{-3}.

Evaluate at z=iaz=ia, where z+ia=2iaz+ia=2ia:

Resz=iaf=2(2ia)3=28i3a3=28(i)a3=28ia3=14ia3.\operatorname*{Res}_{z=ia}f=-\frac{2}{(2ia)^3}=-\frac{2}{8i^3a^3}=-\frac{2}{8(-i)a^3}=\frac{2}{8ia^3}=\frac{1}{4ia^3}.

(Using i3=ii^3=-i.) So Resz=iaf=14ia3=i4a3.\displaystyle\operatorname*{Res}_{z=ia}f=\frac{1}{4ia^3}=-\frac{i}{4a^3}.

Step 4 — Apply the residue theorem and take RR\to\infty

By the residue theorem, for R>aR>a,

CRfdz=2πiResz=iaf=2πi14ia3=2πi4ia3=π2a3.\oint_{C_R}f\,dz=2\pi i\operatorname*{Res}_{z=ia}f=2\pi i\cdot\frac{1}{4ia^3}=\frac{2\pi i}{4ia^3}=\frac{\pi}{2a^3}.

Letting RR\to\infty (the arc term vanishes by Step 2):

dx(x2+a2)2=π2a3.\int_{-\infty}^{\infty}\frac{dx}{(x^2+a^2)^2}=\frac{\pi}{2a^3}.

Therefore

I=12π2a3=  π4a3.  I=\frac12\cdot\frac{\pi}{2a^3}=\boxed{\;\frac{\pi}{4a^3}.\;}

\blacksquare

Verification

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