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NCERT Exemplar · Q40

Q.∫sin⁡−1xa+x dx\int \sin^{-1}\sqrt{\dfrac{x}{a+x}}\,dx (Hint: Put x=atan⁡2θx=a\tan^2\theta)

Gujarat GsebLong· 3mImportance★★★★★
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The key idea is to simplify the integrand using the given substitution x=atan⁡2θx = a \tan^2 \theta, which turns the inverse sine into a simple angle. After substitution and integration by parts, the final result is (a+x)tan⁡−1xa−ax+C\boxed{(a+x) \tan^{-1}\sqrt{\frac{x}{a}} - \sqrt{ax} + C}.

The problem asks for the indefinite integral of sin⁡−1xa+x\sin^{-1}\sqrt{\frac{x}{a+x}}. The expression inside the inverse sine looks messy, but the hint suggests a clever substitution: x=atan⁡2θx = a \tan^2 \theta. Why does this work? Because xa+x\sqrt{\frac{x}{a+x}} becomes something like atan⁡2θa+atan⁡2θ=tan⁡2θ1+tan⁡2θ=sin⁡2θ=sin⁡θ\sqrt{\frac{a \tan^2 \theta}{a + a \tan^2 \theta}} = \sqrt{\frac{\tan^2 \theta}{1 + \tan^2 \theta}} = \sqrt{\sin^2 \theta} = \sin \theta (assuming θ\theta in a suitable range). Then sin⁡−1(sin⁡θ)=θ\sin^{-1}(\sin \theta) = \theta, which is much simpler to integrate.

Let’s walk through it step by step.

  1. Substitute x=atan⁡2θx = a \tan^2 \theta. We need dxdx in terms of dθd\theta. Differentiate:

dx=a⋅2tan⁡θ⋅sec⁡2θ dθ=2atan⁡θsec⁡2θ dθ.dx = a \cdot 2 \tan \theta \cdot \sec^2 \theta \, d\theta = 2a \tan \theta \sec^2 \theta \, d\theta.

Also, note that a+x=a+atan⁡2θ=a(1+tan⁡2θ)=asec⁡2θa + x = a + a \tan^2 \theta = a(1 + \tan^2 \theta) = a \sec^2 \theta.

  1. Simplify the integrand. Compute xa+x\sqrt{\frac{x}{a+x}}:

atan⁡2θasec⁡2θ=tan⁡2θsec⁡2θ=sin⁡2θ=sin⁡θ,\sqrt{\frac{a \tan^2 \theta}{a \sec^2 \theta}} = \sqrt{\frac{\tan^2 \theta}{\sec^2 \theta}} = \sqrt{\sin^2 \theta} = \sin \theta,

taking θ∈[0,π/2)\theta \in [0, \pi/2) so sin⁡θ≥0\sin \theta \ge 0.

Hence sin⁡−1xa+x=sin⁡−1(sin⁡θ)=θ\sin^{-1}\sqrt{\frac{x}{a+x}} = \sin^{-1}(\sin \theta) = \theta.

  1. Rewrite the integral. The integral becomes:

I=∫θ⋅(2atan⁡θsec⁡2θ) dθ=2a∫θtan⁡θsec⁡2θ dθ.I = \int \theta \cdot (2a \tan \theta \sec^2 \theta) \, d\theta = 2a \int \theta \tan \theta \sec^2 \theta \, d\theta.

  1. Simplify the trigonometric part. Notice tan⁡θsec⁡2θ=sin⁡θcos⁡3θ\tan \theta \sec^2 \theta = \frac{\sin \theta}{\cos^3 \theta}. But a better approach: let t=tan⁡θt = \tan \theta, then dt=sec⁡2θ dθdt = \sec^2 \theta \, d\theta, so tan⁡θsec⁡2θ dθ=t dt\tan \theta \sec^2 \theta \, d\theta = t \, dt. However, we still have θ\theta in terms of tt: θ=tan⁡−1t\theta = \tan^{-1} t. So:

I=2a∫θ⋅t dt=2a∫(tan⁡−1t)⋅t dt.I = 2a \int \theta \cdot t \, dt = 2a \int (\tan^{-1} t) \cdot t \, dt.

  1. Integrate by parts. Let u=tan⁡−1tu = \tan^{-1} t and dv=t dtdv = t \, dt. Then du=11+t2dtdu = \frac{1}{1+t^2} dt and v=t22v = \frac{t^2}{2}. Integration by parts gives:

∫u dv=uv−∫v du,\int u \, dv = uv - \int v \, du,

so:

I=2a[t22tan⁡−1t−∫t22⋅11+t2dt]=a[t2tan⁡−1t−∫t21+t2dt].I = 2a \left[ \frac{t^2}{2} \tan^{-1} t - \int \frac{t^2}{2} \cdot \frac{1}{1+t^2} dt \right] = a \left[ t^2 \tan^{-1} t - \int \frac{t^2}{1+t^2} dt \right].

  1. Simplify the remaining integral. Write t21+t2=1−11+t2\frac{t^2}{1+t^2} = 1 - \frac{1}{1+t^2}. Then:

∫t21+t2dt=∫(1−11+t2)dt=t−tan⁡−1t+C1.\int \frac{t^2}{1+t^2} dt = \int \left(1 - \frac{1}{1+t^2}\right) dt = t - \tan^{-1} t + C_1.

Substitute back: …

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