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JEE Main 202122 JulyMorning Shift
Exam
JEE Main
Year
2021
Date
22 July
Shift
Morning Shift
Subject
Mathematics
Chapter
Differential Equations

JEE Main 2021 · 22 July · Morning Shift · Mathematics · Differential Equations

Let y = y(x) be the solution of the differential equation cosec ^ 2...

Let y=y(x)y = y\left(x\right) be the solution of the differential equation cosec2xdy+2dx=(1+ycos2x)cosec2xdx,{cosec}^{2}xdy + 2dx = \left(1 + ycos2x\right){cosec}^{2}xdx, with y(π4)=0.y\left(\dfrac{\pi}{4}\right) = 0 . Then, the value of (y(0)+1)2{\left(y\left(0\right) + 1\right)}^{2} is equal to:

Options

  1. Ae1/2{e}^{1 / 2}
  2. Be−1/2{e}^{- 1 / 2}
  3. Ce−1{e}^{- 1}
  4. Dee

Correct answer

C. e−1{e}^{- 1}

Step-by-step solution

Given, cosec2xdy+2dx=(1+ycos2x)cosec2xdx{cosec}^{2}xdy + 2dx = \left(1 + ycos2x\right){cosec}^{2}xdx

⇒dysin⁡2x+2dx=(1+ycos2xsin⁡2x)dx⇒ \dfrac{dy}{\sin^{2}x} + 2dx = \left(\dfrac{1 + ycos2x}{\sin^{2}x}\right)dx

⇒dydx+2sin⁡2x=1+ycos2x⇒ \dfrac{dy}{dx} + 2\sin^{2}x = 1 + ycos2x

⇒dydx+2sin⁡2x−1=ycos2x⇒ \dfrac{dy}{dx} + 2\sin^{2}x - 1 = ycos2x

Using, cos⁡2x=1−2sin⁡2x,\cos 2x = 1 - 2\sin^{2}x, we get

dydx+(−cos⁡2x)=ycos2x\dfrac{dy}{dx} + \left(- \cos 2x\right) = ycos2x

⇒dydx+(−cos⁡2x)y=cos⁡2x⇒ \dfrac{dy}{dx} + \left(- \cos 2x\right)y = \cos 2x

This is a linear differential equation of the type dydx+Py=Q,\dfrac{dy}{dx} + Py = Q, where P and QP \text{ and } Q are the functions of xx or constants.

Thus, P=−cos⁡2x and Q=cos⁡2xP = - \cos 2x \text{ and } Q = \cos 2x

Now, we have integrating factor I.F.=e∫Pdx=e∫−cos⁡2xdx=e−(sin⁡2x2)= {e}^{∫ Pdx} = {e}^{∫ - \cos 2xdx} = {e}^{- \left(\dfrac{\sin 2x}{2}\right)}

And, the solution of the given differential equation is

y(I.F.)=∫Q(I.F.)dx+cy\left(I . F .\right) = ∫ Q\left(I . F .\right)dx + c

⇒y⋅e−(sin⁡2x2)=∫(cos⁡2x)⋅e−(sin⁡2x2)dx+c⇒ y \cdot {e}^{- \left(\dfrac{\sin 2x}{2}\right)} = ∫ \left(\cos 2x\right) \cdot {e}^{- \left(\dfrac{\sin 2x}{2}\right)}dx + c

Put sin⁡2x2=t,⇒2cos⁡2x2dx=dt\dfrac{\sin 2x}{2} = t, ⇒ \dfrac{2\cos 2x}{2}dx = dt

⇒y⋅e−(sin⁡2x2)=∫e−tdt+c⇒ y \cdot {e}^{- \left(\dfrac{\sin 2x}{2}\right)} = ∫ {e}^{- t}dt + c

⇒y⋅e−(sin⁡2x2)=−e−tdt+c⇒ y \cdot {e}^{- \left(\dfrac{\sin 2x}{2}\right)} = - {e}^{- t}dt + c

⇒y⋅e−(sin⁡2x2)=−e−(sin⁡2x2)+c⇒ y \cdot {e}^{- \left(\dfrac{\sin 2x}{2}\right)} = - {e}^{- \left(\dfrac{\sin 2x}{2}\right)} + c

Given, y(π4)=0y\left(\dfrac{\pi}{4}\right) = 0

⇒0⋅e−(sin⁡(π2)2)=−e−(sin⁡(π2)2)+c⇒ 0 \cdot {e}^{- \left(\dfrac{\sin \left(\dfrac{\pi}{2}\right)}{2}\right)} = - {e}^{- \left(\dfrac{\sin \left(\dfrac{\pi}{2}\right)}{2}\right)} + c

⇒c=−e−(12)⇒ c = - {e}^{- \left(\dfrac{1}{2}\right)}

⇒y⋅e−(sin⁡2x2)=−e−(sin⁡2x2)+e−12⇒ y \cdot {e}^{- \left(\dfrac{\sin 2x}{2}\right)} = - {e}^{- \left(\dfrac{\sin 2x}{2}\right)} + {e}^{- \dfrac{1}{2}}

Now, at x=0x = 0

⇒y(0)⋅e−(sin⁡02)=−e−(sin⁡02)+e−12⇒ y\left(0\right) \cdot {e}^{- \left(\dfrac{\sin 0}{2}\right)} = - {e}^{- \left(\dfrac{\sin 0}{2}\right)} + {e}^{- \dfrac{1}{2}}

⇒y(0)⋅e0=−e0+e−12⇒ y\left(0\right) \cdot {e}^{0} = - {e}^{0} + {e}^{- \dfrac{1}{2}}

⇒y(0)=−1+e−12⇒ y\left(0\right) = - 1 + {e}^{- \dfrac{1}{2}}

⇒y(0)+1=e−12⇒ y\left(0\right) + 1 = {e}^{- \dfrac{1}{2}}

⇒(y(0)+1)2=e−1.⇒ {\left(y\left(0\right) + 1\right)}^{2} = {e}^{- 1} .

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