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JEE Main 202431 JanuaryMorning Shift
Exam
JEE Main
Year
2024
Date
31 January
Shift
Morning Shift
Subject
Mathematics
Chapter
Differential Equations

JEE Main 2024 · 31 January · Morning Shift · Mathematics · Differential Equations

Let y = y ( x ) be the solution of the differential equation...

Let y=y(x)y = y ( x ) be the solution of the differential equation dydx=(tan⁡x)+ysin⁡x(sec⁡x−sin⁡xtan⁡x),x∈(0,π2)\dfrac{dy}{dx} = \dfrac{\left(\tan x\right) + y}{\sin x\left(\sec x - \sin x \tan x\right)}, x \in \left(0, \dfrac{\pi}{2}\right) satisfying the condition y(π4)=2y\left(\dfrac{\pi}{4}\right) = 2. Then, y(π3)y\left(\dfrac{\pi}{3}\right) is

Options

  1. A3(2+log⁡e3)\sqrt{3}\left(2 + \log_{e}\sqrt{3}\right)
  2. B32(2+log⁡e3)\dfrac{\sqrt{3}}{2}\left(2 + \log_{e}3\right)
  3. C3(1+2log⁡e3)\sqrt{3}\left(1 + 2\log_{e}3\right)
  4. D3(2+log⁡e3)\sqrt{3}\left(2 + \log_{e}3\right)

Correct answer

A. 3(2+log⁡e3)\sqrt{3}\left(2 + \log_{e}\sqrt{3}\right)

Step-by-step solution

Given: dydx=tan⁡x+ysin⁡x(sec⁡x−sin⁡xtan⁡x)\dfrac{dy}{dx} = \dfrac{\tan x + y}{\sin x\left(\sec x - \sin x \tan x\right)}

⇒dydx=tan⁡x+ysin⁡x(1cos⁡x−sin⁡2xcos⁡x)⇒ \dfrac{dy}{dx} = \dfrac{\tan x + y}{\sin x\left(\dfrac{1}{\cos x} - \dfrac{\sin^{2}x}{\cos x}\right)}

⇒dydx=tan⁡x+ysin⁡x(cos⁡2xcos⁡x)⇒ \dfrac{dy}{dx} = \dfrac{\tan x + y}{\sin x\left(\dfrac{\cos^{2}x}{\cos x}\right)}

⇒dydx=tan⁡x+ysin⁡xcos⁡x⇒ \dfrac{dy}{dx} = \dfrac{\tan x + y}{\sin x \cos x}

⇒dydx−2ysin⁡2x=sec⁡2x⇒ \dfrac{dy}{dx} - \dfrac{2y}{\sin 2x} = \sec^{2}x

⇒IF=e−2∫cosec2xdx⇒ IF = {e}^{- 2 ∫ cosec2xdx}

⇒IF=e−log⁡∣cosec2x−cot⁡2x∣⇒ IF = {e}^{- \log \left|cosec2x - \cot 2x\right|}

⇒IF=1cosec2x−cot⁡2x=cosec2x+cot⁡2x⇒ IF = \dfrac{1}{cosec2x - \cot 2x} = cosec2x + \cot 2x

⇒IF=1sin⁡2x+cos⁡2xsin⁡2x⇒ IF = \dfrac{1}{\sin 2x} + \dfrac{\cos 2x}{\sin 2x}

⇒IF=2cos⁡2x2sin⁡xcos⁡x⇒ IF = \dfrac{2\cos^{2}x}{2\sin x \cos x}

⇒IF=cot⁡x⇒ IF = \cot x

⇒y×cot⁡x=∫cot⁡x×sec⁡2xdx⇒ y \times \cot x = ∫ \cot x \times \sec^{2}xdx

⇒y×cot⁡x=2∫cosec2xdx⇒ y \times \cot x = 2 ∫ cosec2xdx

⇒ycotx=log⁡∣cosec2x−cot⁡2x∣+c⇒ ycotx = \log \left|cosec2x - \cot 2x\right| + c

Now, using y(π4)=2y\left(\dfrac{\pi}{4}\right) = 2 we get,

⇒2cotπ4=log⁡∣cosecπ2−cotπ2∣+c⇒ 2cot\dfrac{\pi}{4} = \log \left|cosec\dfrac{\pi}{2} - cot\dfrac{\pi}{2}\right| + c

⇒c=2⇒ c = 2

⇒ycotx=log⁡∣cosec2x−cot⁡2x∣+2⇒ ycotx = \log \left|cosec2x - \cot 2x\right| + 2

Now, finding y(π3)y\left(\dfrac{\pi}{3}\right) we get,

⇒ycotπ3=log⁡∣cosec2π3−cot2π3∣+2⇒ ycot\dfrac{\pi}{3} = \log \left|cosec\dfrac{2\pi}{3} - cot\dfrac{2\pi}{3}\right| + 2

⇒y×13=log⁡∣23+13∣+2⇒ y \times \dfrac{1}{\sqrt{3}} = \log \left|\dfrac{2}{\sqrt{3}} + \dfrac{1}{\sqrt{3}}\right| + 2

⇒y×13=12log⁡3+2⇒ y \times \dfrac{1}{\sqrt{3}} = \dfrac{1}{2}\log 3 + 2

⇒y=32log⁡3+23⇒ y = \dfrac{\sqrt{3}}{2}\log 3 + 2\sqrt{3}

⇒y=3(log3+2)⇒ y = \sqrt{3}\left(log\sqrt{3} + 2\right)

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