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JEE Main 2024
Differential Equations
Differential Equations
Medium

Question

If y=y(x)y=y(x) is the solution of the differential equation, 4x2 dy dx=((sin1(x2))2y)sin1(x2),2x2,y(2)=π284\sqrt{4-x^2} \frac{\mathrm{~d} y}{\mathrm{~d} x}=\left(\left(\sin ^{-1}\left(\frac{x}{2}\right)\right)^2-y\right) \sin ^{-1}\left(\frac{x}{2}\right),-2 \leq x \leq 2, y(2)=\frac{\pi^2-8}{4}, then y2(0)y^2(0) is equal to ___________.

Answer: 1

Solution

Key Concepts and Formulas

  • First-Order Linear Differential Equation: A differential equation of the form dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x), where P(x)P(x) and Q(x)Q(x) are functions of xx.
  • Integrating Factor (IF): For a first-order linear differential equation, the integrating factor is given by IF=eP(x)dxIF = e^{\int P(x) dx}.
  • General Solution: The general solution to the first-order linear differential equation is yIF=Q(x)IFdx+Cy \cdot IF = \int Q(x) \cdot IF \, dx + C, where CC is the constant of integration.

Step-by-Step Solution

Step 1: Transform the Differential Equation into Standard Linear Form

The given differential equation is: 4x2dydx=((sin1(x2))2y)sin1(x2)\sqrt{4-x^2} \frac{dy}{dx} = \left( \left( \sin^{-1}\left(\frac{x}{2}\right) \right)^2 - y \right) \sin^{-1}\left(\frac{x}{2}\right) We want to rewrite it in the form dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x). Let t=sin1(x2)t = \sin^{-1}\left(\frac{x}{2}\right). Then, the equation becomes: 4x2dydx=(t2y)t=t3yt\sqrt{4-x^2} \frac{dy}{dx} = (t^2 - y)t = t^3 - yt Divide both sides by 4x2\sqrt{4-x^2}: dydx=t34x2yt4x2\frac{dy}{dx} = \frac{t^3}{\sqrt{4-x^2}} - \frac{yt}{\sqrt{4-x^2}} Rearrange the terms: dydx+t4x2y=t34x2\frac{dy}{dx} + \frac{t}{\sqrt{4-x^2}}y = \frac{t^3}{\sqrt{4-x^2}} Substitute back t=sin1(x2)t = \sin^{-1}\left(\frac{x}{2}\right): dydx+sin1(x2)4x2y=(sin1(x2))34x2\frac{dy}{dx} + \frac{\sin^{-1}\left(\frac{x}{2}\right)}{\sqrt{4-x^2}}y = \frac{\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^3}{\sqrt{4-x^2}} Now we have the standard form with: P(x)=sin1(x2)4x2P(x) = \frac{\sin^{-1}\left(\frac{x}{2}\right)}{\sqrt{4-x^2}} Q(x)=(sin1(x2))34x2Q(x) = \frac{\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^3}{\sqrt{4-x^2}}

Step 2: Calculate the Integrating Factor (IF)

The integrating factor is IF=eP(x)dxIF = e^{\int P(x) \, dx}. We need to calculate P(x)dx\int P(x) \, dx: sin1(x2)4x2dx\int \frac{\sin^{-1}\left(\frac{x}{2}\right)}{\sqrt{4-x^2}} \, dx Let t=sin1(x2)t = \sin^{-1}\left(\frac{x}{2}\right). Then, dtdx=11(x2)212=14x2/212=14x2\frac{dt}{dx} = \frac{1}{\sqrt{1 - \left(\frac{x}{2}\right)^2}} \cdot \frac{1}{2} = \frac{1}{\sqrt{4-x^2}/2} \cdot \frac{1}{2} = \frac{1}{\sqrt{4-x^2}}. Therefore, dt=dx4x2dt = \frac{dx}{\sqrt{4-x^2}}. The integral becomes: tdt=t22=12(sin1(x2))2\int t \, dt = \frac{t^2}{2} = \frac{1}{2} \left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2 The Integrating Factor is: IF=e12(sin1(x2))2IF = e^{\frac{1}{2}\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2}

Step 3: Find the General Solution

The general solution is given by yIF=Q(x)IFdx+Cy \cdot IF = \int Q(x) \cdot IF \, dx + C. Substitute Q(x)Q(x) and IFIF: ye12(sin1(x2))2=(sin1(x2))34x2e12(sin1(x2))2dx+Cy \cdot e^{\frac{1}{2}\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2} = \int \frac{\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^3}{\sqrt{4-x^2}} \cdot e^{\frac{1}{2}\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2} \, dx + C Let t=sin1(x2)t = \sin^{-1}\left(\frac{x}{2}\right). Then dt=dx4x2dt = \frac{dx}{\sqrt{4-x^2}}. The integral on the right-hand side becomes: t3e12t2dt\int t^3 e^{\frac{1}{2}t^2} \, dt Let u=t2u = t^2 and dv=te12t2dtdv = t e^{\frac{1}{2}t^2} dt. Then du=2tdtdu = 2t dt. To find vv, we integrate dvdv. Let s=12t2s = \frac{1}{2}t^2, so ds=tdtds = t dt. Then te12t2dt=esds=es=e12t2\int t e^{\frac{1}{2}t^2} dt = \int e^s ds = e^s = e^{\frac{1}{2}t^2}. Thus, v=e12t2v = e^{\frac{1}{2}t^2}. Using integration by parts udv=uvvdu\int u \, dv = uv - \int v \, du: t3e12t2dt=t2e12t2e12t2(2tdt)=t2e12t22te12t2dt\int t^3 e^{\frac{1}{2}t^2} \, dt = t^2 e^{\frac{1}{2}t^2} - \int e^{\frac{1}{2}t^2} (2t \, dt) = t^2 e^{\frac{1}{2}t^2} - 2 \int t e^{\frac{1}{2}t^2} \, dt Since te12t2dt=e12t2\int t e^{\frac{1}{2}t^2} \, dt = e^{\frac{1}{2}t^2}, we have: t3e12t2dt=t2e12t22e12t2=(t22)e12t2\int t^3 e^{\frac{1}{2}t^2} \, dt = t^2 e^{\frac{1}{2}t^2} - 2e^{\frac{1}{2}t^2} = (t^2 - 2)e^{\frac{1}{2}t^2} Substituting back t=sin1(x2)t = \sin^{-1}\left(\frac{x}{2}\right), we get: ye12(sin1(x2))2=((sin1(x2))22)e12(sin1(x2))2+Cy \cdot e^{\frac{1}{2}\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2} = \left(\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2 - 2\right) e^{\frac{1}{2}\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2} + C Divide both sides by e12(sin1(x2))2e^{\frac{1}{2}\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2}: y=(sin1(x2))22+Ce12(sin1(x2))2y = \left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2 - 2 + C e^{-\frac{1}{2}\left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2}

Step 4: Apply the Initial Condition to Find C

We are given y(2)=π284y(2) = \frac{\pi^2 - 8}{4}. When x=2x=2, sin1(22)=sin1(1)=π2\sin^{-1}\left(\frac{2}{2}\right) = \sin^{-1}(1) = \frac{\pi}{2}. So, y(2)=(π2)22+Ce12(π2)2=π242+Ceπ28y(2) = \left(\frac{\pi}{2}\right)^2 - 2 + C e^{-\frac{1}{2}\left(\frac{\pi}{2}\right)^2} = \frac{\pi^2}{4} - 2 + C e^{-\frac{\pi^2}{8}}. We are given y(2)=π284=π242y(2) = \frac{\pi^2 - 8}{4} = \frac{\pi^2}{4} - 2. Therefore, π242=π242+Ceπ28\frac{\pi^2}{4} - 2 = \frac{\pi^2}{4} - 2 + C e^{-\frac{\pi^2}{8}}, which implies Ceπ28=0C e^{-\frac{\pi^2}{8}} = 0, so C=0C=0. Thus, the particular solution is: y(x)=(sin1(x2))22y(x) = \left(\sin^{-1}\left(\frac{x}{2}\right)\right)^2 - 2

Step 5: Calculate y(0) and y^2(0)

We want to find y2(0)y^2(0). First, find y(0)y(0): y(0)=(sin1(02))22=(sin1(0))22=022=2y(0) = \left(\sin^{-1}\left(\frac{0}{2}\right)\right)^2 - 2 = \left(\sin^{-1}(0)\right)^2 - 2 = 0^2 - 2 = -2 Therefore, y2(0)=(2)2=4y^2(0) = (-2)^2 = 4.

Common Mistakes & Tips

  • Substitution: Using the substitution t=sin1(x2)t = \sin^{-1}\left(\frac{x}{2}\right) simplifies the integral calculations significantly.
  • Integration by Parts: Remember the integration by parts formula: udv=uvvdu\int u \, dv = uv - \int v \, du. Choose uu and dvdv strategically to simplify the integral.
  • Initial Condition: Make sure to use the given initial condition to find the value of the constant of integration, CC.

Summary

We solved the given differential equation by first transforming it into a standard first-order linear form. We then found the integrating factor and used it to obtain the general solution. Using the provided initial condition, we determined the particular solution. Finally, we evaluated the solution at x=0x=0 and squared the result to find y2(0)y^2(0).

The final answer is \boxed{4}.

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