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Exercise 7.6 · Q22

Q.Integrate the function sin⁡−1(2x1+x2)\sin^{-1}\left(\frac{2x}{1+x^2}\right)

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The key idea is to simplify the integrand using the substitution x=tan⁡θx = \tan \theta, which converts the inverse sine expression into 2θ2\theta (for a restricted domain). The integral then reduces to 2∫θsec⁡2θ dθ2 \int \theta \sec^2 \theta \, d\theta, which is solved by integration by parts, yielding 2θtan⁡θ−2log⁡∣sec⁡θ∣+C2\theta \tan \theta - 2 \log|\sec \theta| + C. Back-substituting gives the final result: 2xtan⁡−1x−log⁡(1+x2)+C\boxed{2x \tan^{-1} x - \log(1+x^2) + C}.

We start with the integral:

I=∫sin⁡−1(2x1+x2)dxI = \int \sin^{-1}\left(\frac{2x}{1+x^2}\right) dx

Why This Approach Works

The expression 2x1+x2\frac{2x}{1+x^2} is a dead giveaway for the tangent double-angle identity. Recall that tan⁡(2θ)=2tan⁡θ1−tan⁡2θ\tan(2\theta) = \frac{2\tan\theta}{1-\tan^2\theta}, but here we have a plus sign in the denominator. That points to the sine double-angle identity in a different form: if x=tan⁡θx = \tan \theta, then sin⁡(2θ)=2tan⁡θ1+tan⁡2θ=2x1+x2\sin(2\theta) = \frac{2\tan\theta}{1+\tan^2\theta} = \frac{2x}{1+x^2}. So the integrand becomes sin⁡−1(sin⁡(2θ))\sin^{-1}(\sin(2\theta)), which simplifies to 2θ2\theta — but only for a specific range of θ\theta where the inverse sine is well-defined. This substitution turns a messy inverse trigonometric function into a simple algebraic one.

Watch out

The identity sin⁡−1(sin⁡(2θ))=2θ\sin^{-1}(\sin(2\theta)) = 2\theta holds only when 2θ∈[−π/2,π/2]2\theta \in [-\pi/2, \pi/2], i.e., θ∈[−π/4,π/4]\theta \in [-\pi/4, \pi/4]. For x=tan⁡θx = \tan \theta, this corresponds to x∈[−1,1]x \in [-1, 1]. Outside this interval, the simplification would involve a piecewise constant shift (like π−2θ\pi - 2\theta). Most exam problems implicitly assume the principal branch and the domain ∣x∣≤1|x| \le 1, so we proceed with 2θ2\theta.

Step-by-Step Solution

  1. Substitute x=tan⁡θx = \tan \theta. Then dx=sec⁡2θ dθdx = \sec^2 \theta \, d\theta, and the integrand becomes:

sin⁡−1(2tan⁡θ1+tan⁡2θ)=sin⁡−1(sin⁡2θ)=2θ\sin^{-1}\left(\frac{2\tan\theta}{1+\tan^2\theta}\right) = \sin^{-1}(\sin 2\theta) = 2\theta

(for θ∈[−π/4,π/4]\theta \in [-\pi/4, \pi/4]). So the integral transforms to:

I=∫2θ⋅sec⁡2θ dθ=2∫θsec⁡2θ dθI = \int 2\theta \cdot \sec^2 \theta \, d\theta = 2 \int \theta \sec^2 \theta \, d\theta

  1. Apply integration by parts. Let u=θu = \theta and dv=sec⁡2θ dθdv = \sec^2 \theta \, d\theta. Then du=dθdu = d\theta and v=tan⁡θv = \tan \theta. Using ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du:

I=2(θtan⁡θ−∫tan⁡θ dθ)I = 2 \left( \theta \tan \theta - \int \tan \theta \, d\theta \right)

  1. Integrate tan⁡θ\tan \theta. …

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