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NCERT Exemplar · Q21

Q.Evaluate: ∫sin⁡−1x(1−x2)3/2 dx\int \dfrac{\sin^{-1}x}{(1-x^2)^{3/2}}\,dx

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The integral is solved by substituting x=sin⁡θx = \sin\theta, which simplifies the integrand to θsec⁡2θ dθ\theta \sec^2\theta \, d\theta. Integrating by parts gives xsin⁡−1x1−x2+log⁡∣1−x2∣+C\frac{x \sin^{-1}x}{\sqrt{1-x^2}} + \log|\sqrt{1-x^2}| + C.

The key insight here is that the denominator (1−x2)3/2(1-x^2)^{3/2} looks like a derivative of something involving sin⁡−1x\sin^{-1}x or cos⁡−1x\cos^{-1}x. When you see 1−x2\sqrt{1-x^2} raised to a power, the substitution x=sin⁡θx = \sin\theta (or x=cos⁡θx = \cos\theta) is almost always the cleanest path — it turns the algebraic mess into a trigonometric playground.

Let’s walk through it.

  1. Set up the substitution.

    Let x=sin⁡θx = \sin\theta, so dx=cos⁡θ dθdx = \cos\theta \, d\theta.

    The domain: x∈(−1,1)x \in (-1, 1) corresponds to θ∈(−π/2,π/2)\theta \in (-\pi/2, \pi/2), where cos⁡θ>0\cos\theta > 0 — this keeps signs tidy.

  2. Rewrite the integrand.

    • sin⁡−1x=θ\sin^{-1}x = \theta (since x=sin⁡θx = \sin\theta and θ\theta is in the principal range).
    • 1−x2=1−sin⁡2θ=cos⁡2θ1 - x^2 = 1 - \sin^2\theta = \cos^2\theta, so (1−x2)3/2=(cos⁡2θ)3/2=∣cos⁡θ∣3(1-x^2)^{3/2} = (\cos^2\theta)^{3/2} = |\cos\theta|^3. Because cos⁡θ>0\cos\theta > 0 in our range, ∣cos⁡θ∣=cos⁡θ|\cos\theta| = \cos\theta, so (1−x2)3/2=cos⁡3θ(1-x^2)^{3/2} = \cos^3\theta.

    The integral becomes:

∫θcos⁡3θ⋅cos⁡θ dθ=∫θ⋅1cos⁡2θ dθ=∫θsec⁡2θ dθ.\int \frac{\theta}{\cos^3\theta} \cdot \cos\theta \, d\theta = \int \theta \cdot \frac{1}{\cos^2\theta} \, d\theta = \int \theta \sec^2\theta \, d\theta.

  1. Integrate by parts.

    This is a classic product: θ\theta (algebraic) times sec⁡2θ\sec^2\theta (trigonometric).

    Let u=θu = \theta, dv=sec⁡2θ dθdv = \sec^2\theta \, d\theta.

    Then du=dθdu = d\theta, and v=tan⁡θv = \tan\theta (since ddθtan⁡θ=sec⁡2θ\frac{d}{d\theta}\tan\theta = \sec^2\theta).

    Integration by parts: ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du gives:

∫θsec⁡2θ dθ=θtan⁡θ−∫tan⁡θ dθ.\int \theta \sec^2\theta \, d\theta = \theta \tan\theta - \int \tan\theta \, d\theta.

  1. Handle the leftover integral. ∫tan⁡θ dθ=∫sin⁡θcos⁡θ dθ\int \tan\theta \, d\theta = \int \frac{\sin\theta}{\cos\theta} \, d\theta. Substitute t=cos⁡θt = \cos\theta, dt=−sin⁡θ dθdt = -\sin\theta \, d\theta, giving:

∫sin⁡θcos⁡θ dθ=−∫dtt=−log⁡∣t∣+C=−log⁡∣cos⁡θ∣+C.\int \frac{\sin\theta}{\cos\theta} \, d\theta = -\int \frac{dt}{t} = -\log|t| + C = -\log|\cos\theta| + C.

So:

∫θsec⁡2θ dθ=θtan⁡θ−(−log⁡∣cos⁡θ∣)+C=θtan⁡θ+log⁡∣cos⁡θ∣+C.\int \theta \sec^2\theta \, d\theta = \theta \tan\theta - (-\log|\cos\theta|) + C = \theta \tan\theta + \log|\cos\theta| + C. …

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