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JEE Main 202331 JanuaryMorning Shift
Exam
JEE Main
Year
2023
Date
31 January
Shift
Morning Shift
Subject
Mathematics
Chapter
Definite Integration

JEE Main 2023 · 31 January · Morning Shift · Mathematics · Definite Integration

The value of ∫ _ (π)/(3) ^ (π)/(2) (2 + 3 x ) x (1 + x) dx is equal...

The value of {∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{\left(2 + 3\text{ \sin x }\right)}{\sin x\left(1 + \cos x\right)}dx is equal to

Options

  1. A72−3−log⁡e3\dfrac{7}{2} - \sqrt{3} - \log_{e}\sqrt{3}
  2. B−2+33+log⁡e3- 2 + 3\sqrt{3} + \log_{e}\sqrt{3}
  3. C103−3+log⁡e3\dfrac{10}{3} - \sqrt{3} + \log_{e}\sqrt{3}
  4. D103−3−log⁡e3\dfrac{10}{3} - \sqrt{3} - \log_{e}\sqrt{3}

Correct answer

C. 103−3+log⁡e3\dfrac{10}{3} - \sqrt{3} + \log_{e}\sqrt{3}

Step-by-step solution

Let, I=∫π3π22+3sin⁡xsin⁡x(1+cos⁡x)dxI = {∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{2 + 3\sin x}{\sin x\left(1 + \cos x\right)}dx

Now rearranging the above integral we get,

I=∫π3π22sin⁡x(1+cos⁡x)dx+∫π3π23(1+cos⁡x)dxI = {∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{2}{\sin x\left(1 + \cos x\right)}dx + {∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{3}{\left(1 + \cos x\right)}dx

⇒I=∫π3π22sin⁡xsin⁡2x(1+cos⁡x)dx+∫π3π23(2cos⁡2x2)dx⇒ I = {∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{2\sin x}{\sin^{2}x\left(1 + \cos x\right)}dx + {∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{3}{\left(2\cos^{2}\dfrac{x}{2}\right)}dx

⇒I=∫π3π22sin⁡xsin⁡2x(1+cos⁡x)dx⏟I1+32∫π3π2sec⁡2(x2)dx⏟I2⇒ I = \mathop{\mathop{{∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{2\sin x}{\sin^{2}x\left(1 + \cos x\right)} d x}_{⏟}}_{{I}_{1}} + \dfrac{3}{2}\mathop{\mathop{{∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\sec^{2}\left(\dfrac{x}{2}\right) d x}_{⏟}}_{{I}_{2}}

⇒I=∫π3π22sin⁡xsin⁡2x(1+cos⁡x)dx⏟I1+32×2[tanx2]π3π2⏟I2⇒ I = \mathop{\mathop{{∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{2\sin x}{\sin^{2}x\left(1 + \cos x\right)}dx}_{⏟}}_{{I}_{1}} + \dfrac{3}{2} \times 2\mathop{\mathop{{\left[tan\dfrac{x}{2}\right]}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}}_{⏟}}_{{I}_{2}}

⇒I=∫π3π22sin⁡xsin⁡2x(1+cos⁡x)dx⏟I1+3(1−13)⇒ I = \mathop{\mathop{{∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{2\sin x}{\sin^{2}x\left(1 + \cos x\right)}dx}_{⏟}}_{{I}_{1}} + 3\left(1 - \dfrac{1}{\sqrt{3}}\right)

Now solving I1{I}_{1} we get,

I1=∫π3π22sin⁡xsin⁡2x(1+cos⁡x)dx{I}_{1} = {∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{2\sin x}{\sin^{2}x\left(1 + \cos x\right)}dx

⇒I1=2∫π3π21sin⁡x(1+cos⁡x)dx⇒ {I}_{1} = 2{∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{1}{\sin x\left(1 + \cos x\right)}dx

⇒I1=2∫π3π21(2tan⁡(x2)1+tan⁡2(x2))(1+1−tan⁡(x2)1+tan⁡2(x2))dx⇒ {I}_{1} = 2{∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{1}{\left(\dfrac{2\tan \left(\dfrac{x}{2}\right)}{1 + \tan^{2}\left(\dfrac{x}{2}\right)}\right)\left(1 + \dfrac{1 - \tan \left(\dfrac{x}{2}\right)}{1 + \tan^{2}\left(\dfrac{x}{2}\right)}\right)}dx

⇒I1=12∫π3π2[1+tan⁡2(x2)]sec⁡2(x2)tan⁡(x2)dx⇒ {I}_{1} = \dfrac{1}{2}{∫}_{\dfrac{\pi}{3}}^{\dfrac{\pi}{2}}\dfrac{\left[1 + \tan^{2}\left(\dfrac{x}{2}\right)\right]\sec^{2}\left(\dfrac{x}{2}\right)}{\tan \left(\dfrac{x}{2}\right)}dx

Put tan⁡(x2)=v⇒12sec⁡2(x2)dx=dv\tan \left(\dfrac{x}{2}\right) = v ⇒ \dfrac{1}{2}\sec^{2}\left(\dfrac{x}{2}\right)dx = dv

⇒I1=∫131(1+v2)dvv⇒ {I}_{1} = {∫}_{\dfrac{1}{\sqrt{3}}}^{1}\dfrac{\left(1 + {v}^{2}\right)dv}{v}

⇒I1=[log⁡e(v)+v22]131⇒ {I}_{1} = {\left[\log_{e}\left(v\right) + \dfrac{{v}^{2}}{2}\right]}_{\dfrac{1}{\sqrt{3}}}^{1}

⇒I1=log⁡e(1)−log⁡e(13)+12(1−13)⇒ {I}_{1} = \log_{e}\left(1\right) - \log_{e}\left(\dfrac{1}{\sqrt{3}}\right) + \dfrac{1}{2}\left(1 - \dfrac{1}{3}\right)

⇒I1=log⁡e(13)+13⇒ {I}_{1} = \log_{e}\left(\dfrac{1}{\sqrt{3}}\right) + \dfrac{1}{3}

So,

I=13+log⁡e3+3(1−13)I = \dfrac{1}{3} + \log_{e}\sqrt{3} + 3\left(1 - \dfrac{1}{\sqrt{3}}\right)

⇒I=103−3+log⁡e3⇒ I = \dfrac{10}{3} - \sqrt{3} + \log_{e}\sqrt{3}

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