Question 9: Prove that cotθ + tanθ = 2cosec2θ. Hence show that ∫(π/6)^(π/3) cosec2θ dθ = (1/2)ln3

Mathematics
Question 9: Prove that cotθ + tanθ = 2cosec2θ. Hence show that ∫(π/6)^(π/3) cosec2θ dθ = (1/2)ln3

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here's the solution to Question 9:

Part (i): Prove that cot⁡θ+tan⁡θ=2cosec⁡2θ\cot\theta + \tan\theta = 2\operatorname{cosec}2\theta.

Step 1.1: Start with the left-hand side (LHS) and express cot⁡θ\cot\theta and tan⁡θ\tan\theta in terms of sin⁡θ\sin\theta and cos⁡θ\cos\theta. LHS=cot⁡θ+tan⁡θ=cos⁡θsin⁡θ+sin⁡θcos⁡θ\text{LHS} = \cot\theta + \tan\theta = \frac{\cos\theta}{\sin\theta} + \frac{\sin\theta}{\cos\theta}

Step 1.2: Combine the fractions by finding a common denominator. cos⁡θsin⁡θ+sin⁡θcos⁡θ=cos⁡2θ+sin⁡2θsin⁡θcos⁡θ\frac{\cos\theta}{\sin\theta} + \frac{\sin\theta}{\cos\theta} = \frac{\cos^2\theta + \sin^2\theta}{\sin\theta\cos\theta}

Step 1.3: Use the Pythagorean identity sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1. cos⁡2θ+sin⁡2θsin⁡θcos⁡θ=1sin⁡θcos⁡θ\frac{\cos^2\theta + \sin^2\theta}{\sin\theta\cos\theta} = \frac{1}{\sin\theta\cos\theta}

Step 1.4: Use the double angle identity for sine, sin⁡2θ=2sin⁡θcos⁡θ\sin2\theta = 2\sin\theta\cos\theta, which implies sin⁡θcos⁡θ=12sin⁡2θ\sin\theta\cos\theta = \frac{1}{2}\sin2\theta. 1sin⁡θcos⁡θ=112sin⁡2θ=2sin⁡2θ\frac{1}{\sin\theta\cos\theta} = \frac{1}{\frac{1}{2}\sin2\theta} = \frac{2}{\sin2\theta}

Step 1.5: Express the result in terms of cosec⁡2θ\operatorname{cosec}2\theta, since cosec⁡x=1sin⁡x\operatorname{cosec}x = \frac{1}{\sin x}. 2sin⁡2θ=2cosec⁡2θ=RHS\frac{2}{\sin2\theta} = 2\operatorname{cosec}2\theta = \text{RHS} Thus, cot⁡θ+tan⁡θ=2cosec⁡2θ\cot\theta + \tan\theta = \boxed{2\operatorname{cosec}2\theta} is proven.

Part (ii): Hence show that ∫π6π3cosec⁡2θ dθ=12ln⁡3\int_{\frac{\pi}{6}}^{\frac{\pi}{3}} \operatorname{cosec}2\theta\,d\theta = \frac{1}{2}\ln3.

Step 2.1: Use the result from Part (i) to rewrite the integrand. From Part (i), we have 2cosec⁡2θ=cot⁡θ+tan⁡θ2\operatorname{cosec}2\theta = \cot\theta + \tan\theta, so cosec⁡2θ=12(cot⁡θ+tan⁡θ)\operatorname{cosec}2\theta = \frac{1}{2}(\cot\theta + \tan\theta). ∫π6π3cosec⁡2θ dθ=∫π6π312(cot⁡θ+tan⁡θ) dθ\int_{\frac{\pi}{6}}^{\frac{\pi}{3}} \operatorname{cosec}2\theta\,d\theta = \int_{\frac{\pi}{6}}^{\frac{\pi}{3}} \frac{1}{2}(\cot\theta + \tan\theta)\,d\theta

Step 2.2: Integrate the terms. Recall that ∫cot⁡θ dθ=ln⁡∣sin⁡θ∣\int \cot\theta\,d\theta = \ln|\sin\theta| and ∫tan⁡θ dθ=−ln⁡∣cos⁡θ∣\int \tan\theta\,d\theta = -\ln|\cos\theta|. 12∫π6π3(cot⁡θ+tan⁡θ) dθ=12[ln⁡∣sin⁡θ∣−ln⁡∣cos⁡θ∣]π6π3\frac{1}{2} \int_{\frac{\pi}{6}}^{\frac{\pi}{3}} (\cot\theta + \tan\theta)\,d\theta = \frac{1}{2} \left[ \ln|\sin\theta| - \ln|\cos\theta| \right]_{\frac{\pi}{6}}^{\frac{\pi}{3}}

Step 2.3: Use the logarithm property ln⁡a−ln⁡b=ln⁡(ab)\ln a - \ln b = \ln\left(\frac{a}{b}\right). 12[ln⁡∣sin⁡θcos⁡θ∣]π6π3=12[ln⁡∣tan⁡θ∣]π6π3\frac{1}{2} \left[ \ln\left|\frac{\sin\theta}{\cos\theta}\right| \right]_{\frac{\pi}{6}}^{\frac{\pi}{3}} = \frac{1}{2} \left[ \ln|\tan\theta| \right]_{\frac{\pi}{6}}^{\frac{\pi}{3}}

Step 2.4: Apply the limits of integration. 12(ln⁡∣tan⁡(π3)∣−ln⁡∣tan⁡(π6)∣)\frac{1}{2} \left( \ln\left|\tan\left(\frac{\pi}{3}\right)\right| - \ln\left|\tan\left(\frac{\pi}{6}\right)\right| \right)

Step 2.5: Evaluate the tangent values: tan⁡(π3)=3\tan\left(\frac{\pi}{3}\right) = \sqrt{3} and tan⁡(π6)=13\tan\left(\frac{\pi}{6}\right) = \frac{1}{\sqrt{3}}. 12(ln⁡(3)−ln⁡(13))\frac{1}{2} \left( \ln(\sqrt{3}) - \ln\left(\frac{1}{\sqrt{3}}\right) \right)

Step 2.6: Simplify the logarithmic expression using ln⁡(1a)=−ln⁡a\ln\left(\frac{1}{a}\right) = -\ln a and ln⁡(ab)=bln⁡a\ln(a^b) = b\ln a. 12(ln⁡(312)−ln⁡(3−12))=12(12ln⁡3−(−12ln⁡3))\frac{1}{2} \left( \ln(3^{\frac{1}{2}}) - \ln(3^{-\frac{1}{2}}) \right) = \frac{1}{2} \left( \frac{1}{2}\ln3 - \left(-\frac{1}{2}\ln3\right) \right) =12(12ln⁡3+12ln⁡3)=12(ln⁡3)=12ln⁡3= \frac{1}{2} \left( \frac{1}{2}\ln3 + \frac{1}{2}\ln3 \right) = \frac{1}{2} (\ln3) = \boxed{\frac{1}{2}\ln3} The result is shown.

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