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JEE Main 202429 JanuaryMorning Shift
Exam
JEE Main
Year
2024
Date
29 January
Shift
Morning Shift
Subject
Mathematics
Chapter
Definite Integration

JEE Main 2024 · 29 January · Morning Shift · Mathematics · Definite Integration

For x ∈ (- (π)/(2), (π)/(2)) , if y(x) = ∫ cosec x + x cosec xsecx...

For x∈(−π2,π2)x \in \left(- \dfrac{\pi}{2}, \dfrac{\pi}{2}\right), if y(x)=∫cosecx+sin⁡xcosecxsecx+tan⁡xsin⁡2xdxy\left(x\right) = ∫ \dfrac{cosec x + \sin x}{cosec xsecx + \tan x\sin^{2}x}dx and lim⁡x→(π2)−y(x)=0\lim_{x \to {\left(\dfrac{\pi}{2}\right)}^{-}}y\left(x\right) = 0 then y(π4)y\left(\dfrac{\pi}{4}\right) is equal to

Options

  1. Atan⁡−1(12)\tan^{- 1}\left(\dfrac{1}{\sqrt{2}}\right)
  2. B12tan⁡−1(12)\dfrac{1}{2}\tan^{- 1}\left(\dfrac{1}{\sqrt{2}}\right)
  3. C−12tan⁡−1(12)- \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{1}{\sqrt{2}}\right)
  4. D12tan⁡−1(−12)\dfrac{1}{\sqrt{2}}\tan^{- 1}\left(- \dfrac{1}{2}\right)

Correct answer

D. 12tan⁡−1(−12)\dfrac{1}{\sqrt{2}}\tan^{- 1}\left(- \dfrac{1}{2}\right)

Step-by-step solution

Given:

f(x)=∫cosecx+sin⁡xcosecxsecx+tan⁡xsin⁡2xdxf\left(x\right) = ∫ \dfrac{cosecx + \sin x}{cosecxsecx + \tan x\sin^{2}x}dx

⇒f(x)=∫1sin⁡x+sin⁡x1sin⁡xcos⁡x+sin⁡xcos⁡x(sin⁡2x)dx⇒ f\left(x\right) = ∫ \dfrac{\dfrac{1}{\sin x} + \sin x}{\dfrac{1}{\sin x \cos x} + \dfrac{\sin x}{\cos x}\left(\sin^{2}x\right)}dx

⇒f(x)=∫1+sin⁡2xsin⁡x1+sin⁡4xsin⁡xcos⁡xdx⇒ f\left(x\right) = ∫ \dfrac{\dfrac{1 + \sin^{2}x}{\sin x}}{\dfrac{1 + \sin^{4}x}{\sin x \cos x}}dx

⇒f(x)=∫(1+sin⁡2x)cos⁡x1+sin⁡4xdx⇒ f\left(x\right) = ∫ \dfrac{\left(1 + \sin^{2}x\right)\cos x}{1 + \sin^{4}x}dx

Let, sin⁡x=t\sin x = t

cosxdx=dtcosxdx = dt

⇒f(x)=∫1+t21+t4dt⇒ f\left(x\right) = ∫ \dfrac{1 + {t}^{2}}{1 + {t}^{4}}dt

⇒f(x)=∫1+1t2t2+1t2dt⇒ f\left(x\right) = ∫ \dfrac{1 + \dfrac{1}{{t}^{2}}}{{t}^{2} + \dfrac{1}{{t}^{2}}}dt

⇒f(x)=∫1+1t2(t−1t)2+2dt⇒ f\left(x\right) = ∫ \dfrac{1 + \dfrac{1}{{t}^{2}}}{{\left(t - \dfrac{1}{t}\right)}^{2} + 2}dt

Let, t−1t=ut - \dfrac{1}{t} = u

⇒f(x)=∫1u2+2du⇒ f\left(x\right) = ∫ \dfrac{1}{{u}^{2} + 2}du

⇒f(x)=12tan⁡−1(u2)+C⇒ f\left(x\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{u}{\sqrt{2}}\right) + C

⇒f(x)=12tan⁡−1(t−1t2)+C⇒ f\left(x\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{t - \dfrac{1}{t}}{\sqrt{2}}\right) + C

⇒f(x)=12tan⁡−1(sin⁡x−1sin⁡x2)+C⇒ f\left(x\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{\sin x - \dfrac{1}{\sin x}}{\sqrt{2}}\right) + C

⇒f(x)=12tan⁡−1(sin⁡x−cosecx2)+C⇒ f\left(x\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{\sin x - cosecx}{\sqrt{2}}\right) + C

Now, lim⁡x→π2−f(x)=0\lim_{x \to \dfrac{\pi}{2} -}f\left(x\right) = 0

⇒lim⁡x→π2−f(x)=lim⁡x→π2−[12tan⁡−1(sin⁡x−cosecx2)+C]=0⇒ \lim_{x \to \dfrac{\pi}{2} -}f\left(x\right) = \lim_{x \to \dfrac{\pi}{2} -}\left[\dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{\sin x - cosecx}{\sqrt{2}}\right) + C\right] = 0

⇒12tan⁡−1(0)+C=0⇒ \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(0\right) + C = 0

⇒C=0⇒ C = 0

⇒f(x)=12tan⁡−1(sin⁡x−cosecx2)⇒ f\left(x\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{\sin x - cosecx}{\sqrt{2}}\right)

⇒y(π4)=12tan⁡−1(sinπ4−cosecπ42)⇒ y\left(\dfrac{\pi}{4}\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{sin\dfrac{\pi}{4} - cosec\dfrac{\pi}{4}}{\sqrt{2}}\right)

⇒y(π4)=12tan⁡−1(12−22)⇒ y\left(\dfrac{\pi}{4}\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{\dfrac{1}{\sqrt{2}} - \sqrt{2}}{\sqrt{2}}\right)

⇒y(π4)=12tan⁡−1(−122)⇒ y\left(\dfrac{\pi}{4}\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{\dfrac{- 1}{\sqrt{2}}}{\sqrt{2}}\right)

⇒y(π4)=12tan⁡−1(−12)⇒ y\left(\dfrac{\pi}{4}\right) = \dfrac{1}{\sqrt{2}}\tan^{- 1}\left(\dfrac{- 1}{2}\right)

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