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JEE Main 202427 JanuaryEvening Shift
Exam
JEE Main
Year
2024
Date
27 January
Shift
Evening Shift
Subject
Mathematics
Chapter
Definite Integration

JEE Main 2024 · 27 January · Evening Shift · Mathematics · Definite Integration

For 0 < a < 1 , the value of the integral ∫ _ 0 ^ π dx 1 - 2acosx +...

For 0<a<10 < a < 1, the value of the integral ∫0πdx1−2acosx+a2{∫}_{0}^{\pi}\dfrac{dx}{1 - 2acosx + {a}^{2}} is :

Options

  1. Aπ2π+a2\dfrac{{\pi}^{2}}{\pi + {a}^{2}}
  2. Bπ2π−a2\dfrac{{\pi}^{2}}{\pi - {a}^{2}}
  3. Cπ1−a2\dfrac{\pi}{1 - {a}^{2}}
  4. Dπ1+a2\dfrac{\pi}{1 + {a}^{2}}

Correct answer

C. π1−a2\dfrac{\pi}{1 - {a}^{2}}

Step-by-step solution

Given: I=∫0πdx1−2acosx+a2...(i)I = {∫}_{0}^{\pi}\dfrac{dx}{1 - 2acosx + {a}^{2}} . . . \left(i\right)

⇒I=∫0πdx1−2acos(π−x)+a2⇒ I = {∫}_{0}^{\pi}\dfrac{dx}{1 - 2acos\left(\pi - x\right) + {a}^{2}}

⇒I=∫0πdx1+2acosx+a2...(ii)⇒ I = {∫}_{0}^{\pi}\dfrac{dx}{1 + 2acosx + {a}^{2}} . . . \left(ii\right)

Adding \left(i\right)and (ii)and \left(ii\right),

⇒2I=∫0πdx1−2acosx+a2+∫0πdx1+2acosx+a2⇒ 2I = {∫}_{0}^{\pi}\dfrac{dx}{1 - 2acosx + {a}^{2}} + {∫}_{0}^{\pi}\dfrac{dx}{1 + 2acosx + {a}^{2}}

⇒2I=∫0π(11−2acosx+a2+11+2acosx+a2)dx⇒ 2I = {∫}_{0}^{\pi}\left(\dfrac{1}{1 - 2acosx + {a}^{2}} + \dfrac{1}{1 + 2acosx + {a}^{2}}\right)dx

⇒2I=∫0π(1+2acosx+a2+1−2acosx+a2(1+a2)2−(2acosx)2)dx⇒ 2I = {∫}_{0}^{\pi}\left(\dfrac{1 + 2acosx + {a}^{2} + 1 - 2acosx + {a}^{2}}{{\left(1 + {a}^{2}\right)}^{2} - {\left(2acosx\right)}^{2}}\right)dx

⇒2I=∫0π(2(1+a2)(1+a2)2−(2acosx)2)dx⇒ 2I = {∫}_{0}^{\pi}\left(\dfrac{2\left(1 + {a}^{2}\right)}{{\left(1 + {a}^{2}\right)}^{2} - {\left(2acosx\right)}^{2}}\right)dx

⇒2I=2∫0π22(1+a2)(1+a2)2−4a2cos⁡2xdx⇒ 2I = 2{∫}_{0}^{\dfrac{\pi}{2}}\dfrac{2\left(1 + {a}^{2}\right)}{{\left(1 + {a}^{2}\right)}^{2} - 4{a}^{2}\cos^{2}x}dx

⇒I=∫0π22(1+a2)⋅sec⁡2x(1+a2)2⋅sec⁡2x−4a2dx⇒ I = {∫}_{0}^{\dfrac{\pi}{2}}\dfrac{2\left(1 + {a}^{2}\right) \cdot \sec^{2}x}{{\left(1 + {a}^{2}\right)}^{2} \cdot \sec^{2}x - 4{a}^{2}}dx

⇒I=∫0π22(1+a2)⋅sec⁡2x(1+a2)2+(1+a2)2tan⁡2x−4a2dx⇒ I = {∫}_{0}^{\dfrac{\pi}{2}}\dfrac{2\left(1 + {a}^{2}\right) \cdot \sec^{2}x}{{\left(1 + {a}^{2}\right)}^{2} + {\left(1 + {a}^{2}\right)}^{2}\tan^{2}x - 4{a}^{2}}dx

⇒I=∫0π22(1+a2)⋅sec⁡2x(1+a2−2a)2+(1+a2)2tan⁡2xdx⇒ I = {∫}_{0}^{\dfrac{\pi}{2}}\dfrac{2\left(1 + {a}^{2}\right) \cdot \sec^{2}x}{{\left(1 + {a}^{2} - 2a\right)}^{2} + {\left(1 + {a}^{2}\right)}^{2}\tan^{2}x}dx

⇒I=∫0π22⋅(1+a2)⋅sec⁡2x(1+a2)2⋅tan⁡2x+(1−a2)2dx⇒ I = {∫}_{0}^{\dfrac{\pi}{2}}\dfrac{2 \cdot \left(1 + {a}^{2}\right) \cdot \sec^{2}x}{{\left(1 + {a}^{2}\right)}^{2} \cdot \tan^{2}x + {\left(1 - {a}^{2}\right)}^{2}}dx

⇒I=∫0π22⋅sec⁡2x1+a2⋅dxtan⁡2x+(1−a21+a2)2⇒ I = {∫}_{0}^{\dfrac{\pi}{2}}\dfrac{\dfrac{2 \cdot \sec^{2}x}{1 + {a}^{2}} \cdot dx}{\tan^{2}x + {\left(\dfrac{1 - {a}^{2}}{1 + {a}^{2}}\right)}^{2}}

Let, tan⁡x=t\tan x = t

⇒sec⁡2xdx=dt⇒ \sec^{2}xdx = dt

⇒I=21+a2∫0∞dtt2+(1−a21+a2)2⇒ I = \dfrac{2}{1 + {a}^{2}}{∫}_{0}^{\infty}\dfrac{dt}{{t}^{2} + {\left(\dfrac{1 - {a}^{2}}{1 + {a}^{2}}\right)}^{2}}

⇒I=21+a2×1(1−a21+a2)[tan⁡−1t(1−a21+a2)]0∞⇒ I = \dfrac{2}{1 + {a}^{2}} \times \dfrac{1}{\left(\dfrac{1 - {a}^{2}}{1 + {a}^{2}}\right)}{\left[\tan^{- 1}\dfrac{t}{\left(\dfrac{1 - {a}^{2}}{1 + {a}^{2}}\right)}\right]}_{0}^{\infty}

⇒I=21−a2[tan⁡−1(∞)−tan⁡−1(0)]⇒ I = \dfrac{2}{1 - {a}^{2}}\left[\tan^{- 1}\left(\infty\right) - \tan^{- 1}\left(0\right)\right]

⇒I=2(1−a2)[π2−0]⇒ I = \dfrac{2}{\left(1 - {a}^{2}\right)}\left[\dfrac{\pi}{2} - 0\right]

⇒I=π1−a2⇒ I = \dfrac{\pi}{1 - {a}^{2}}

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