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Worked Examples · Example 20

Q.Find ∫xsin⁡−1x1−x2 dx\int \dfrac{x \sin^{-1} x}{\sqrt{1 - x^2}}\, dx

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The integral simplifies by substituting x=sin⁡θx = \sin \theta, converting it into ∫θsin⁡θ dθ\int \theta \sin \theta \, d\theta, which is solved using integration by parts. The final result is x−1−x2sin⁡−1x+C\boxed{x - \sqrt{1 - x^2} \sin^{-1} x + C}.

The key insight here is that the denominator 1−x2\sqrt{1 - x^2} is a dead giveaway for a trigonometric substitution. When you see 1−x2\sqrt{1 - x^2}, your mind should immediately jump to x=sin⁡θx = \sin \theta (or x=cos⁡θx = \cos \theta). This substitution will not only simplify the square root but also turn the sin⁡−1x\sin^{-1} x into something much friendlier — just θ\theta.

Let’s walk through it.

  1. Set up the substitution.

    Let x=sin⁡θx = \sin \theta, where θ∈[−π/2,π/2]\theta \in [-\pi/2, \pi/2] (the principal range of sin⁡−1\sin^{-1}). Then dx=cos⁡θ dθdx = \cos \theta \, d\theta, and 1−x2=1−sin⁡2θ=cos⁡θ\sqrt{1 - x^2} = \sqrt{1 - \sin^2 \theta} = \cos \theta (positive in this range). Also, sin⁡−1x=θ\sin^{-1} x = \theta.

  2. Rewrite the integral.

    The numerator becomes xsin⁡−1x=(sin⁡θ)(θ)x \sin^{-1} x = (\sin \theta)(\theta). The denominator is 1−x2=cos⁡θ\sqrt{1 - x^2} = \cos \theta. So the integral becomes:

∫(sin⁡θ)(θ)cos⁡θ⋅(cos⁡θ dθ)=∫θsin⁡θ dθ.\int \frac{(\sin \theta)(\theta)}{\cos \theta} \cdot (\cos \theta \, d\theta) = \int \theta \sin \theta \, d\theta.

The cos⁡θ\cos \theta cancels neatly — that’s the beauty of this substitution.

  1. Integrate ∫θsin⁡θ dθ\int \theta \sin \theta \, d\theta. This is a classic product of a polynomial (θ\theta) and a trigonometric function (sin⁡θ\sin \theta). Use integration by parts. Let u=θu = \theta and dv=sin⁡θ dθdv = \sin \theta \, d\theta. Then du=dθdu = d\theta and v=−cos⁡θv = -\cos \theta. Integration by parts gives:

∫u dv=uv−∫v du=θ(−cos⁡θ)−∫(−cos⁡θ) dθ=−θcos⁡θ+∫cos⁡θ dθ.\int u \, dv = uv - \int v \, du = \theta(-\cos \theta) - \int (-\cos \theta) \, d\theta = -\theta \cos \theta + \int \cos \theta \, d\theta.

And ∫cos⁡θ dθ=sin⁡θ\int \cos \theta \, d\theta = \sin \theta, so:

∫θsin⁡θ dθ=−θcos⁡θ+sin⁡θ+C.\int \theta \sin \theta \, d\theta = -\theta \cos \theta + \sin \theta + C. …

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