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Exercise 7.10 · Q10

Q.By using the properties of definite integrals, evaluate the integral ∫0π/2(2log⁡sin⁡x−log⁡sin⁡2x) dx\int_{0}^{\pi/2}(2\log\sin x-\log\sin 2x)\,dx

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Using symmetry and the property ∫0af(x)dx=∫0af(a−x)dx\int_{0}^{a} f(x) dx = \int_{0}^{a} f(a-x) dx, the given integral simplifies to −π2log⁡2-\frac{\pi}{2}\log 2.

The key to this problem lies in recognising that the integrand can be rewritten using logarithm properties, and then applying the standard definite integral symmetry trick. When you see an integral from 00 to π2\frac{\pi}{2} involving log⁡sin⁡x\log\sin x, your first instinct should be to use the substitution x→π2−xx \to \frac{\pi}{2} - x — this often creates a second copy of the same integral, allowing you to solve for it algebraically.

Let’s break it down.

  1. Simplify the integrand using log rules. The expression inside the integral is 2log⁡sin⁡x−log⁡sin⁡2x2\log\sin x - \log\sin 2x. Using log⁡ab=blog⁡a\log a^b = b\log a and log⁡a−log⁡b=log⁡ab\log a - \log b = \log\frac{a}{b}, we get:

2log⁡sin⁡x−log⁡sin⁡2x=log⁡(sin⁡2x)−log⁡(sin⁡2x)=log⁡(sin⁡2xsin⁡2x).2\log\sin x - \log\sin 2x = \log(\sin^2 x) - \log(\sin 2x) = \log\left(\frac{\sin^2 x}{\sin 2x}\right).

Now recall the double-angle identity: sin⁡2x=2sin⁡xcos⁡x\sin 2x = 2\sin x \cos x. Substituting:

sin⁡2xsin⁡2x=sin⁡2x2sin⁡xcos⁡x=sin⁡x2cos⁡x=12tan⁡x.\frac{\sin^2 x}{\sin 2x} = \frac{\sin^2 x}{2\sin x \cos x} = \frac{\sin x}{2\cos x} = \frac{1}{2}\tan x.

So the integrand becomes log⁡(12tan⁡x)=log⁡12+log⁡(tan⁡x)=−log⁡2+log⁡(tan⁡x)\log\left(\frac{1}{2}\tan x\right) = \log\frac{1}{2} + \log(\tan x) = -\log 2 + \log(\tan x).

Therefore, the integral II is:

I=∫0π/2(−log⁡2+log⁡(tan⁡x))dx=−log⁡2∫0π/2dx+∫0π/2log⁡(tan⁡x) dx.I = \int_{0}^{\pi/2} \left( -\log 2 + \log(\tan x) \right) dx = -\log 2 \int_{0}^{\pi/2} dx + \int_{0}^{\pi/2} \log(\tan x) \, dx.

The first part is easy: ∫0π/2dx=π2\int_{0}^{\pi/2} dx = \frac{\pi}{2}, so that term is −π2log⁡2-\frac{\pi}{2}\log 2.

  1. Now handle the tricky part: J=∫0π/2log⁡(tan⁡x) dxJ = \int_{0}^{\pi/2} \log(\tan x) \, dx.

    At first glance, log⁡(tan⁡x)\log(\tan x) looks like it might be messy. But here’s the beautiful symmetry trick: use the substitution x→π2−xx \to \frac{\pi}{2} - x.

    Let x=π2−tx = \frac{\pi}{2} - t. Then dx=−dtdx = -dt, and when x=0x=0, t=π2t=\frac{\pi}{2}; when x=π2x=\frac{\pi}{2}, t=0t=0. So:

J=∫0π/2log⁡(tan⁡x) dx=∫π/20log⁡(tan⁡(π2−t))(−dt)=∫0π/2log⁡(tan⁡(π2−t))dt.J = \int_{0}^{\pi/2} \log(\tan x) \, dx = \int_{\pi/2}^{0} \log\left(\tan\left(\frac{\pi}{2} - t\right)\right) (-dt) = \int_{0}^{\pi/2} \log\left(\tan\left(\frac{\pi}{2} - t\right)\right) dt.

Now, tan⁡(π2−t)=cot⁡t=1tan⁡t\tan\left(\frac{\pi}{2} - t\right) = \cot t = \frac{1}{\tan t}. So: …

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