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JEE Main 202229 JuneMorning Shift
Exam
JEE Main
Year
2022
Date
29 June
Shift
Morning Shift
Subject
Mathematics
Chapter
Differential Equations

JEE Main 2022 · 29 June · Morning Shift · Mathematics · Differential Equations

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

Let y=yy = y\left(x\right)bethesolutionofthedifferentialequationbe the solution of the differential equation\dfrac{dy}{dx} + \dfrac{\sqrt{2}y}{2\cos^{4}x - \cos 2x} = x{e}^{\tan^{- 1}\left(\sqrt{2}\cot 2x\right)}, 0 < x < \dfrac{\pi}{2}withwithy\left(\dfrac{\pi}{4}\right) = \dfrac{{\pi}^{2}}{32}.If. Ify\left(\dfrac{\pi}{3}\right) = \dfrac{{\pi}^{2}}{18}{e}^{- \tan^{- 1}\left(\alpha\right)},thenthevalueof, then the value of3{\alpha}^{2} is equal to ______.

Correct answer

0

Step-by-step solution

Given dydx+22cos⁡4x−cos⁡2xy=xetan⁡−1(2cot⁡2x)\dfrac{dy}{dx} + \dfrac{\sqrt{2}}{2\cos^{4}x - \cos 2x}y = x{e}^{\tan^{- 1}\left(\sqrt{2}\cot 2x\right)}

This is a linear differential equation.

Here I=∫dx2cos⁡4x−cos⁡2x=∫dx(12+cos⁡22x2+cos⁡2x)−cos⁡2xI = ∫ \dfrac{dx}{2\cos^{4}x - \cos 2x} = ∫ \dfrac{dx}{\left(\dfrac{1}{2} + \dfrac{\cos^{2}2x}{2} + \cos 2x\right) - \cos 2x}

=22∫sec⁡22xdx2+tan⁡22x= 2\sqrt{2} ∫ \dfrac{\sec^{2}2xdx}{2 + \tan^{2}2x}

Put tan⁡2x=t\tan 2x = t

I=tan⁡−1tan⁡2x2I = \tan^{- 1}\dfrac{\tan 2x}{\sqrt{2}}

∴IF=etan⁡−1(tan⁡2x2)=ecot⁡−1(2cot⁡2x)∴ IF = {e}^{\tan^{- 1}\left(\dfrac{\tan 2x}{\sqrt{2}}\right)} = {e}^{\cot^{- 1}\left(\sqrt{2}\cot 2x\right)}

So general solution will be

yecot⁡−1(2cot⁡2x)=∫xetan⁡−1(2cot⁡2x)ecot⁡−1(2cot⁡2x)dxy{e}^{\cot^{- 1}\left(\sqrt{2}\cot 2x\right)} = ∫ x{e}^{\tan^{- 1}\left(\sqrt{2}\cot 2x\right)}{e}^{\cot^{- 1}\left(\sqrt{2}\cot 2x\right)}dx

yecot⁡−1(2cot⁡2x)=eπ2(x22)+cy{e}^{\cot^{- 1}\left(\sqrt{2}\cot 2x\right)} = e\dfrac{\pi}{2}\left(\dfrac{{x}^{2}}{2}\right) + c

y(π4)=π232⇒c=0y\left(\dfrac{\pi}{4}\right) = \dfrac{{\pi}^{2}}{32} ⇒ c = 0

i.e. y=x22etan⁡−1(2cot⁡2x)y = \dfrac{{x}^{2}}{2}{e}^{\tan^{- 1}\left(\sqrt{2}\cot 2x\right)}

Given y(π3)=π218e−tan⁡−1αy\left(\dfrac{\pi}{3}\right) = \dfrac{{\pi}^{2}}{18}{e}^{- \tan^{- 1}\alpha}

⇒π218e−tan⁡−1α=π218etan⁡−1(2cot2π3)⇒ \dfrac{{\pi}^{2}}{18}{e}^{- \tan^{- 1}\alpha} = \dfrac{{\pi}^{2}}{18}{e}^{\tan^{- 1}\left(\sqrt{2}cot\dfrac{2\pi}{3}\right)}=π218e−tan⁡−1(23)= \dfrac{{\pi}^{2}}{18}{e}^{- \tan^{- 1}\left(\sqrt{\dfrac{2}{3}}\right)}

Hence α=23⇒3α2=2\alpha = \sqrt{\dfrac{2}{3}} ⇒ 3{\alpha}^{2} = 2

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