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NCERT Exemplar · Q44

Q.∫0π/2dx(a2cos⁡2x+b2sin⁡2x)2\int_{0}^{\pi/2} \dfrac{dx}{(a^2\cos^2 x+b^2\sin^2 x)^2} (Hint: Divide numerator and denominator by cos⁡4x\cos^4 x)

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Using the symmetry of definite integrals and the given hint, we transform the integral into a rational function in tan⁡x\tan x, then evaluate it via substitution and standard integration formulas. The final value is π(a2+b2)4a3b3\boxed{\frac{\pi(a^2+b^2)}{4a^3b^3}}.

The key insight here is that the integrand is a rational function of cos⁡2x\cos^2 x and sin⁡2x\sin^2 x, which suggests a substitution involving tan⁡x\tan x. The hint to divide numerator and denominator by cos⁡4x\cos^4 x is the classic trick to convert everything into powers of tan⁡x\tan x, making the integral tractable.

Let’s work through it step by step.

  1. Rewrite the integrand using the hint. Divide numerator and denominator by cos⁡4x\cos^4 x:

1(a2cos⁡2x+b2sin⁡2x)2=1/cos⁡4x(a2+b2tan⁡2x)2\frac{1}{(a^2\cos^2 x + b^2\sin^2 x)^2} = \frac{1/\cos^4 x}{(a^2 + b^2\tan^2 x)^2}

Since 1/cos⁡4x=sec⁡4x=(1+tan⁡2x)21/\cos^4 x = \sec^4 x = (1+\tan^2 x)^2, we get:

I=∫0π/2(1+tan⁡2x)2(a2+b2tan⁡2x)2 dxI = \int_{0}^{\pi/2} \frac{(1+\tan^2 x)^2}{(a^2 + b^2\tan^2 x)^2} \, dx

  1. Substitute t=tan⁡xt = \tan x. Then dt=sec⁡2x dx=(1+tan⁡2x) dxdt = \sec^2 x \, dx = (1+\tan^2 x)\, dx, so dx=dt1+t2dx = \frac{dt}{1+t^2}. When x=0x=0, t=0t=0; when x=π/2x=\pi/2, t→∞t \to \infty. The integral becomes:

I=∫0∞(1+t2)2(a2+b2t2)2⋅dt1+t2=∫0∞1+t2(a2+b2t2)2 dtI = \int_{0}^{\infty} \frac{(1+t^2)^2}{(a^2 + b^2 t^2)^2} \cdot \frac{dt}{1+t^2} = \int_{0}^{\infty} \frac{1+t^2}{(a^2 + b^2 t^2)^2} \, dt

  1. Split into two simpler integrals.

I=∫0∞1(a2+b2t2)2 dt  +  ∫0∞t2(a2+b2t2)2 dtI = \int_{0}^{\infty} \frac{1}{(a^2 + b^2 t^2)^2} \, dt \;+\; \int_{0}^{\infty} \frac{t^2}{(a^2 + b^2 t^2)^2} \, dt

Call these I1I_1 and I2I_2 respectively.

  1. Evaluate I1I_1 using a standard formula. Recall:

∫0∞dt(t2+c2)2=π4c3\int_{0}^{\infty} \frac{dt}{(t^2 + c^2)^2} = \frac{\pi}{4c^3}

(This comes from the substitution t=ctan⁡θt = c\tan\theta.)

Here c2=a2/b2c^2 = a^2/b^2, so c=a/bc = a/b. Thus:

I1=∫0∞dt(a2+b2t2)2=1b4∫0∞dt(t2+(a/b)2)2=1b4⋅π4(a/b)3=π4a3bI_1 = \int_{0}^{\infty} \frac{dt}{(a^2 + b^2 t^2)^2} = \frac{1}{b^4} \int_{0}^{\infty} \frac{dt}{(t^2 + (a/b)^2)^2} = \frac{1}{b^4} \cdot \frac{\pi}{4 (a/b)^3} = \frac{\pi}{4 a^3 b}

  1. Evaluate I2I_2 by relating it to I1I_1. Notice that:

I2=∫0∞t2(a2+b2t2)2 dtI_2 = \int_{0}^{\infty} \frac{t^2}{(a^2 + b^2 t^2)^2} \, dt

Differentiate the known integral ∫0∞dta2+b2t2=π2ab\int_{0}^{\infty} \frac{dt}{a^2 + b^2 t^2} = \frac{\pi}{2ab} with respect to aa? That’s messy. Instead, use a clever trick:

Write t2=1b2(a2+b2t2)−a2b2t^2 = \frac{1}{b^2}(a^2 + b^2 t^2) - \frac{a^2}{b^2}, so:

t2(a2+b2t2)2=1b2⋅1a2+b2t2−a2b2⋅1(a2+b2t2)2\frac{t^2}{(a^2 + b^2 t^2)^2} = \frac{1}{b^2} \cdot \frac{1}{a^2 + b^2 t^2} - \frac{a^2}{b^2} \cdot \frac{1}{(a^2 + b^2 t^2)^2}

Then: …

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