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Exercise 9.4 · Q2

Q.∫01sin⁡(3tan⁡−1x)tan⁡−1x1+x2 dx\displaystyle\int_0^1 \dfrac{\sin(3\tan^{-1}x)\tan^{-1}x}{1+x^2}\,dx

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The integrand is NOT a polynomial times a trig function of xx — tan⁡−1x\tan^{-1}x is not a polynomial, so Bernoulli's formula does not apply directly in xx. Substituting θ=tan⁡−1x\theta=\tan^{-1}x converts the awkward tan⁡−1x\tan^{-1}x factor into a genuine linear polynomial in θ\theta, after which Bernoulli's formula applies cleanly.

Step 1. Substitute θ=tan⁡−1x\theta=\tan^{-1}x. Then dθ=dx1+x2d\theta=\dfrac{dx}{1+x^2}, and the limits become x=0⇒θ=0x=0\Rightarrow\theta=0, x=1⇒θ=π/4x=1\Rightarrow\theta=\pi/4. Since tan⁡−1x1+x2dx=θ dθ\dfrac{\tan^{-1}x}{1+x^2}dx=\theta\,d\theta, the integral becomes

∫01sin⁡(3tan⁡−1x)tan⁡−1x1+x2dx=∫0π/4θsin⁡3θ dθ.\int_0^1\dfrac{\sin(3\tan^{-1}x)\tan^{-1}x}{1+x^2}dx=\int_0^{\pi/4}\theta\sin3\theta\,d\theta.

Step 2. Recognize this is now a Bernoulli's-formula case. u=θu=\theta is a polynomial (degree 1) and v=sin⁡3θv=\sin3\theta is repeatedly integrable, so Bernoulli's formula applies with u(1)=1, u(2)=0u^{(1)}=1,\ u^{(2)}=0.

Step 3. List the successive anti-derivatives of v=sin⁡3θv=\sin3\theta.

v(1)=∫sin⁡3θ dθ=−13cos⁡3θv_{(1)}=\displaystyle\int\sin3\theta\,d\theta=-\dfrac13\cos3\theta

v(2)=∫v(1) dθ=−19sin⁡3θv_{(2)}=\displaystyle\int v_{(1)}\,d\theta=-\dfrac19\sin3\theta

Step 4. Apply Bernoulli's formula. ∫uv dθ=uv(1)−u(1)v(2)\int uv\,d\theta=uv_{(1)}-u^{(1)}v_{(2)} (terminates since u(2)=0u^{(2)}=0):

∫θsin⁡3θ dθ=θ ⁣(−13cos⁡3θ)−1 ⁣(−19sin⁡3θ)=−θ3cos⁡3θ+19sin⁡3θ=F(θ).\int\theta\sin3\theta\,d\theta=\theta\!\left(-\dfrac13\cos3\theta\right)-1\!\left(-\dfrac19\sin3\theta\right)=-\dfrac{\theta}{3}\cos3\theta+\dfrac19\sin3\theta=F(\theta).

Step 5. Self-verify by differentiating. F′(θ)=−13cos⁡3θ+θsin⁡3θ+13cos⁡3θ=θsin⁡3θF'(\theta)=-\dfrac13\cos3\theta+\theta\sin3\theta+\dfrac13\cos3\theta=\theta\sin3\theta ✓, matching the integrand.

Step 6. Evaluate F(π/4)−F(0)F(\pi/4)-F(0). At θ=π/4\theta=\pi/4: cos⁡3π4=−22, sin⁡3π4=22\cos\tfrac{3\pi}{4}=-\tfrac{\sqrt2}2,\ \sin\tfrac{3\pi}{4}=\tfrac{\sqrt2}2.

F(π/4)=−π/43(−22)+19 ⁣(22)=π224+218.F(\pi/4)=-\dfrac{\pi/4}{3}\left(-\dfrac{\sqrt2}2\right)+\dfrac19\!\left(\dfrac{\sqrt2}2\right)=\dfrac{\pi\sqrt2}{24}+\dfrac{\sqrt2}{18}.

At θ=0\theta=0: F(0)=0(cos⁡0)+19sin⁡0=0F(0)=0(\cos0)+\tfrac19\sin0=0.

Step 7. Combine over a common denominator. π224=3π272\dfrac{\pi\sqrt2}{24}=\dfrac{3\pi\sqrt2}{72} and 218=4272\dfrac{\sqrt2}{18}=\dfrac{4\sqrt2}{72}, so

∫0π/4θsin⁡3θ dθ=3π2+4272=2(3π+4)72.\int_0^{\pi/4}\theta\sin3\theta\,d\theta=\dfrac{3\pi\sqrt2+4\sqrt2}{72}=\dfrac{\sqrt2(3\pi+4)}{72}.

✓Final answer

∫01sin⁡(3tan⁡−1x)tan⁡−1x1+x2 dx=2(3π+4)72\displaystyle\int_0^1\dfrac{\sin(3\tan^{-1}x)\tan^{-1}x}{1+x^2}\,dx = \boxed{\dfrac{\sqrt2(3\pi+4)}{72}}

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