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NCERT Exemplar · Q51

Q.∫sin⁡x3+4cos⁡2x dx=\int \dfrac{\sin x}{3+4\cos^2 x}\,dx = _______.

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Appeared in past exams:KCET 2024· Set A-1· 1mexactMHT-CET 2023· Set pcm-2023-05-09-E· 2mreworded
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The key idea is to rewrite the integral using a substitution that turns the denominator into a form matching the standard arctangent integral. The final result is −123tan⁡−1(2cos⁡x3)+C\boxed{-\frac{1}{2\sqrt{3}}\tan^{-1}\left(\frac{2\cos x}{\sqrt{3}}\right) + C}.

Why This Approach Works

When you see a denominator like 3+4cos⁡2x3 + 4\cos^2 x, your first instinct might be to try trigonometric identities. But notice the numerator is sin⁡x\sin x, which is almost the derivative of cos⁡x\cos x (up to a sign). That’s the real clue: whenever you have a function and its derivative nearby, substitution is the natural path.

The denominator is a sum of a constant and a square of cos⁡x\cos x. After substitution, this becomes a2+u2a^2 + u^2, which is the classic form for the arctangent integral:

∫dua2+u2=1atan⁡−1(ua)+C\int \frac{du}{a^2 + u^2} = \frac{1}{a} \tan^{-1}\left(\frac{u}{a}\right) + C

So the plan is: let u=cos⁡xu = \cos x, handle the sign from du=−sin⁡x dxdu = -\sin x\,dx, and then match the constants.

Step-by-Step Solution

1. Choose the substitution.

Let u=cos⁡xu = \cos x. Then du=−sin⁡x dxdu = -\sin x\,dx, which means sin⁡x dx=−du\sin x\,dx = -du.

2. Rewrite the integral.

The original integral becomes:

∫sin⁡x3+4cos⁡2x dx=∫−du3+4u2\int \frac{\sin x}{3 + 4\cos^2 x}\,dx = \int \frac{-du}{3 + 4u^2}

3. Factor the denominator to match the standard form.

We want something like 1a2+u2\frac{1}{a^2 + u^2}. Factor out the 4:

3+4u2=4(34+u2)=4(u2+34)3 + 4u^2 = 4\left(\frac{3}{4} + u^2\right) = 4\left(u^2 + \frac{3}{4}\right)

So the integral is:

∫−du4(u2+34)=−14∫duu2+34\int \frac{-du}{4\left(u^2 + \frac{3}{4}\right)} = -\frac{1}{4} \int \frac{du}{u^2 + \frac{3}{4}}

4. Identify a2a^2 and apply the arctangent formula.

Here a2=34a^2 = \frac{3}{4}, so a=32a = \frac{\sqrt{3}}{2}. Using ∫duu2+a2=1atan⁡−1(ua)+C\int \frac{du}{u^2 + a^2} = \frac{1}{a} \tan^{-1}\left(\frac{u}{a}\right) + C:

−14⋅132tan⁡−1(u32)+C=−14⋅23tan⁡−1(2u3)+C-\frac{1}{4} \cdot \frac{1}{\frac{\sqrt{3}}{2}} \tan^{-1}\left(\frac{u}{\frac{\sqrt{3}}{2}}\right) + C = -\frac{1}{4} \cdot \frac{2}{\sqrt{3}} \tan^{-1}\left(\frac{2u}{\sqrt{3}}\right) + C …

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