← 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 10× in 14 yrs · Read the full method →

Question

Show by applying the residue theorem that ∫0∞dx(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[(z−ia)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=∫0∞dx(x2+a2)2=12∫−∞∞dx(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(z−ia)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+a2∣≥R2−a2|z^2+a^2|\ge R^2-a^2, so

∣∫ΓRf(z) dz∣≤πR(R2−a2)2→R→∞0,\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,

Res⁡z=iaf=lim⁡z→iaddz[(z−ia)2f(z)]=lim⁡z→iaddz1(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:

Res⁡z=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 Res⁡z=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 R→∞R\to\infty

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

∮CRf dz=2πiRes⁡z=iaf=2πi⋅14ia3=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 R→∞R\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=12⋅π2a3=  π4a3.  I=\frac12\cdot\frac{\pi}{2a^3}=\boxed{\;\frac{\pi}{4a^3}.\;}

■\blacksquare

Verification

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