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JEE Main 202228 JuneMorning Shift
Exam
JEE Main
Year
2022
Date
28 June
Shift
Morning Shift
Subject
Mathematics
Chapter
Differential Equations

JEE Main 2022 · 28 June · Morning Shift · Mathematics · Differential Equations

Let the solution curve y = y(x) of the differential equation, [ x x...

Let the solution curve y=y(x)y = y\left(x\right) of the differential equation, \left[\dfrac{x}{\sqrt{{x}^{2} - {y}^{2}}} + e\dfrac{y}{x}\right]x\dfrac{dy}{dx} = x + [xx2−y2+eyx]y\left[\dfrac{x}{\sqrt{{x}^{2} - {y}^{2}}} + e\dfrac{y}{x}\right]y pass through the points \left(1, 0\right)and(2α,α),α>0and \left(2\alpha, \alpha\right), \alpha > 0. Then α\alpha is equal to

Options

  1. A12exp(π6+e−1)\dfrac{1}{2}exp\left(\dfrac{\pi}{6} + \sqrt{e} - 1\right)
  2. B12exp(π3+e−1)\dfrac{1}{2}exp\left(\dfrac{\pi}{3} + \sqrt{e} - 1\right)
  3. Cexp(π6+e+1)exp\left(\dfrac{\pi}{6} + \sqrt{e} + 1\right)
  4. D2exp(π3+e−1)2exp\left(\dfrac{\pi}{3} + \sqrt{e} - 1\right)

Correct answer

A. 12exp(π6+e−1)\dfrac{1}{2}exp\left(\dfrac{\pi}{6} + \sqrt{e} - 1\right)

Step-by-step solution

Given x(xx2−y2+eyx)dydx=y(xx2−y2+eyx)+xx\left(\dfrac{x}{\sqrt{{x}^{2} - {y}^{2}}} + e\dfrac{y}{x}\right)\dfrac{dy}{dx} = y\left(\dfrac{x}{\sqrt{{x}^{2} - {y}^{2}}} + e\dfrac{y}{x}\right) + x

Taking xx common & cancelling them we get,

dydx×(11−(yx)2+eyx)=yx(11−(yx)2+eyx)+1\dfrac{dy}{dx} \times \left(\dfrac{1}{\sqrt{1 - {\left(\dfrac{y}{x}\right)}^{2}}} + e\dfrac{y}{x}\right) = \dfrac{y}{x}\left(\dfrac{1}{\sqrt{1 - {\left(\dfrac{y}{x}\right)}^{2}}} + e\dfrac{y}{x}\right) + 1

Let y=vx⇒dydx=v+xdvdxy = vx⇒ \dfrac{dy}{dx} = v + x\dfrac{dv}{dx}

\left(v + x\dfrac{dv}{dx}\right)\left(\dfrac{1}{\sqrt{1 - {v}^{2}}} + {e}^{v}\right) = v\left(\dfrac{1}{\sqrt{1 - {v}^{2}}} + {e}^{v}\right) + 1</p><p></p><p>v + x\dfrac{dV}{dx} = v + \dfrac{1}{\left(\dfrac{1}{\sqrt{1 - {v}^{2}}} + {e}^{v}\right)}</p><p></p><p>x\dfrac{dv}{dx} = \dfrac{1}{\left(\dfrac{1}{\sqrt{1 - {v}^{2}}} + {e}^{v}\right)} ⇒ \left(\dfrac{1}{\sqrt{1 - {v}^{2}}} + {e}^{v}\right)dv = \dfrac{dx}{x}</p><p>Integratingbothsideweget,</p><p></p><p>Integrating both side we get,</p><p>⇒ ∫ \left(\dfrac{1}{\sqrt{1 - {v}^{2}}} + {e}^{v}\right)dv = ∫ \dfrac{dx}{x}</p><p></p><p>⇒ \sin^{- 1}v + {e}^{v} = \ln x + c ⇒ \sin^{- 1}\left(\dfrac{y}{x}\right) + e\dfrac{y}{x} = \ln x + c</p><p>Now</p><p>Nowy\left(1\right) = 0</p><p></p><p>⇒ \sin^{- 1}\left(\dfrac{0}{1}\right) + {e}^{0} = \ln 1 + c</p><p></p><p>⇒ c = 1</p><p></p><p>⇒ \sin^{- 1}\left(\dfrac{y}{x}\right) + e\dfrac{y}{x} = \ln x + 1........(i)</p><p>Now........(i)</p><p>Nowy\left(2\alpha\right) = \alphaputtinginequation(i)weget,</p><p>putting in equation (i) we get,</p><p>⇒ \sin^{- 1}\left(\dfrac{\alpha}{2\alpha}\right) + e\dfrac{\alpha}{2\alpha} = \ln 2\alpha + 1</p><p></p><p>⇒ \dfrac{\pi}{6} + e\dfrac{1}{2} = \ln 2\alpha + 1 ⇒ \alpha = \dfrac{1}{2}{e}^{\dfrac{\pi}{6} + \sqrt{e} - 1}$

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