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Exercise 7.9 · Q3

Q.Evaluate the integral using substitution ∫01sin⁡−1(2x1+x2)dx\int_{0}^{1}\sin^{-1}\left(\frac{2x}{1+x^2}\right)dx

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The key idea is to use the substitution x=tan⁡θx = \tan \theta, which simplifies the integrand’s argument to 2θ2\theta for θ∈[0,π/4]\theta \in [0, \pi/4], turning the integral into 2∫0π/4θsec⁡2θ dθ2\int_{0}^{\pi/4} \theta \sec^2 \theta \, d\theta. Integration by parts then yields the value π2−log⁡2\frac{\pi}{2} - \log 2.

We are asked to evaluate

I=∫01sin⁡−1(2x1+x2)dx.I = \int_{0}^{1} \sin^{-1}\left( \frac{2x}{1+x^2} \right) dx.

The expression inside the inverse sine, 2x1+x2\frac{2x}{1+x^2}, is a classic double-angle form. If you recall the tangent half-angle identities, you know that for x=tan⁡θx = \tan \theta,

2tan⁡θ1+tan⁡2θ=sin⁡2θ.\frac{2 \tan \theta}{1 + \tan^2 \theta} = \sin 2\theta.

This is the natural path: the substitution x=tan⁡θx = \tan \theta will simplify the integrand dramatically.

But there is a subtlety: the range of sin⁡−1\sin^{-1} is [−π/2,π/2][-\pi/2, \pi/2], and for x∈[0,1]x \in [0,1], θ\theta runs from 00 to π/4\pi/4, so 2θ2\theta lies in [0,π/2][0, \pi/2], safely inside the principal range. No sign issues.

Let’s work through it step by step.

  1. Substitute x=tan⁡θx = \tan \theta. Then dx=sec⁡2θ dθdx = \sec^2 \theta \, d\theta. When x=0x = 0, θ=0\theta = 0; when x=1x = 1, θ=π/4\theta = \pi/4. The integral becomes

I=∫0π/4sin⁡−1(2tan⁡θ1+tan⁡2θ)sec⁡2θ dθ.I = \int_{0}^{\pi/4} \sin^{-1}\left( \frac{2 \tan \theta}{1 + \tan^2 \theta} \right) \sec^2 \theta \, d\theta.

  1. Simplify the argument. Since 1+tan⁡2θ=sec⁡2θ1 + \tan^2 \theta = \sec^2 \theta, we have

2tan⁡θ1+tan⁡2θ=2tan⁡θsec⁡2θ=2sin⁡θcos⁡θ=sin⁡2θ.\frac{2 \tan \theta}{1 + \tan^2 \theta} = \frac{2 \tan \theta}{\sec^2 \theta} = 2 \sin \theta \cos \theta = \sin 2\theta.

Therefore,

I=∫0π/4sin⁡−1(sin⁡2θ) sec⁡2θ dθ.I = \int_{0}^{\pi/4} \sin^{-1}(\sin 2\theta) \, \sec^2 \theta \, d\theta.

  1. Handle the inverse sine. For θ∈[0,π/4]\theta \in [0, \pi/4], 2θ∈[0,π/2]2\theta \in [0, \pi/2], and on this interval sin⁡−1(sin⁡2θ)=2θ\sin^{-1}(\sin 2\theta) = 2\theta (since sine is one-to-one and increasing there). So

I=∫0π/42θ sec⁡2θ dθ=2∫0π/4θsec⁡2θ dθ.I = \int_{0}^{\pi/4} 2\theta \, \sec^2 \theta \, d\theta = 2 \int_{0}^{\pi/4} \theta \sec^2 \theta \, d\theta.

  1. Integrate 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. Integration by parts gives

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

We know ∫tan⁡θ dθ=−log⁡∣cos⁡θ∣+C\int \tan \theta \, d\theta = -\log |\cos \theta| + C, so

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

  1. Evaluate the definite integral.

I=2[θtan⁡θ+log⁡(cos⁡θ)]0π/4.I = 2 \left[ \theta \tan \theta + \log(\cos \theta) \right]_{0}^{\pi/4}.

At θ=π/4\theta = \pi/4: tan⁡(π/4)=1\tan(\pi/4) = 1, cos⁡(π/4)=2/2\cos(\pi/4) = \sqrt{2}/2, so log⁡(cos⁡(π/4))=log⁡(1/2)=−12log⁡2\log(\cos(\pi/4)) = \log(1/\sqrt{2}) = -\frac{1}{2} \log 2.

At θ=0\theta = 0: θtan⁡θ=0⋅0=0\theta \tan \theta = 0 \cdot 0 = 0, and log⁡(cos⁡0)=log⁡1=0\log(\cos 0) = \log 1 = 0.

Hence

I=2(π4⋅1−12log⁡2−0)=2(π4−12log⁡2)=π2−log⁡2.I = 2 \left( \frac{\pi}{4} \cdot 1 - \frac{1}{2} \log 2 - 0 \right) = 2 \left( \frac{\pi}{4} - \frac{1}{2} \log 2 \right) = \frac{\pi}{2} - \log 2.

Watch out

A common mistake is to forget that sin⁡−1(sin⁡2θ)=2θ\sin^{-1}(\sin 2\theta) = 2\theta only holds when 2θ2\theta is in [−π/2,π/2][-\pi/2, \pi/2]. Here it’s fine, but if the upper limit were larger (say x>1x > 1), the identity would need adjustment.

Tip

The substitution x=tan⁡θx = \tan \theta is a reflex for integrands involving 2x1+x2\frac{2x}{1+x^2} or 1−x21+x2\frac{1-x^2}{1+x^2} — they become sin⁡2θ\sin 2\theta and cos⁡2θ\cos 2\theta respectively. Keep it in your toolkit.

✓Final answer

The value of the integral is π2−log⁡2\boxed{\frac{\pi}{2} - \log 2}.

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