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Differential Equations question

2011 · Shift 2 · Q32
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  5. /2011 · Shift 2 · Q32

Differential Equations question

2011 · Shift 2 · Q32

JEE AdvancedMathematicsDifferential EquationsNumerical+4 / −1
Let y′(x)+y(x)g′(x)=g(x),g′(x),y(0)=0,x∈R,y'\left( x \right) + y\left( x \right)g'\left( x \right) = g\left( x \right),g'\left( x \right),y\left( 0 \right) = 0,x \in R,y′(x)+y(x)g′(x)=g(x),g′(x),y(0)=0,x∈R, where f′(x)f'(x)f′(x) denotes df(x)dx{{df\left( x \right)} \over {dx}}dxdf(x)​ and g(x)g(x)g(x) is a given non-constant differentiable function on RRR with g(0)=g(2)=0.g(0)=g(2)=0.g(0)=g(2)=0. Then the value of y(2)y(2)y(2) is
Numerical answer
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Correct answer: 0

Step-by-step Solution:

  1. Identify the type of differential equation. The given differential equation is: y′(x)+y(x)g′(x)=g(x)g′(x)y'\left( x \right) + y\left( x \right)g'\left( x \right) = g\left( x \right)g'\left( x \right)y′(x)+y(x)g′(x)=g(x)g′(x) This is a first-order linear differential equation of the form dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x)dxdy​+P(x)y=Q(x), where:

    • P(x)=g′(x)P(x) = g'(x)P(x)=g′(x)
    • Q(x)=g(x)g′(x)Q(x) = g(x)g'(x)Q(x)=g(x)g′(x)
  2. Find the integrating factor (IF). The integrating factor is given by the formula I.F.=e∫P(x)dxI.F. = e^{\int P(x)dx}I.F.=e∫P(x)dx. I.F.=e∫g′(x)dx=eg(x)I.F. = e^{\int g'(x)dx} = e^{g(x)}I.F.=e∫g′(x)dx=eg(x) (We can omit the constant of integration here.)

  3. Solve the differential equation. Multiply the entire differential equation by the integrating factor eg(x)e^{g(x)}eg(x): eg(x)y′(x)+y(x)g′(x)eg(x)=g(x)g′(x)eg(x)e^{g(x)}y'(x) + y(x)g'(x)e^{g(x)} = g(x)g'(x)e^{g(x)}eg(x)y′(x)+y(x)g′(x)eg(x)=g(x)g′(x)eg(x) The left-hand side (LHS) of the equation is the derivative of the product of y(x)y(x)y(x) and the integrating factor: ddx[y(x)eg(x)]=g(x)g′(x)eg(x)\frac{d}{dx} \left[ y(x) e^{g(x)} \right] = g(x)g'(x)e^{g(x)}dxd​[y(x)eg(x)]=g(x)g′(x)eg(x)

  4. Integrate both sides with respect to x. ∫ddx[y(x)eg(x)]dx=∫g(x)g′(x)eg(x)dx\int \frac{d}{dx} \left[ y(x) e^{g(x)} \right] dx = \int g(x)g'(x)e^{g(x)} dx∫dxd​[y(x)eg(x)]dx=∫g(x)g′(x)eg(x)dx y(x)eg(x)=∫g(x)g′(x)eg(x)dx+Cy(x) e^{g(x)} = \int g(x)g'(x)e^{g(x)} dx + Cy(x)eg(x)=∫g(x)g′(x)eg(x)dx+C where C is the constant of integration.

  5. Evaluate the integral on the right-hand side (RHS). Let's solve the integral I=∫g(x)g′(x)eg(x)dxI = \int g(x)g'(x)e^{g(x)} dxI=∫g(x)g′(x)eg(x)dx. Use the substitution method. Let t=g(x)t = g(x)t=g(x). Then dt=g′(x)dxdt = g'(x)dxdt=g′(x)dx. I=∫tetdtI = \int t e^t dtI=∫tetdt Now, use integration by parts: ∫udv=uv−∫vdu\int u dv = uv - \int v du∫udv=uv−∫vdu. Let u=tu = tu=t and dv=etdtdv = e^t dtdv=etdt. Then du=dtdu = dtdu=dt and v=etv = e^tv=et. I=tet−∫etdt=tet−et=(t−1)etI = t e^t - \int e^t dt = t e^t - e^t = (t-1)e^tI=tet−∫etdt=tet−et=(t−1)et Substitute back t=g(x)t = g(x)t=g(x): I=(g(x)−1)eg(x)I = (g(x)-1)e^{g(x)}I=(g(x)−1)eg(x)

  6. Write the general solution. Substituting the result of the integral back into the equation from Step 4: y(x)eg(x)=(g(x)−1)eg(x)+Cy(x) e^{g(x)} = (g(x)-1)e^{g(x)} + Cy(x)eg(x)=(g(x)−1)eg(x)+C Divide by eg(x)e^{g(x)}eg(x) to isolate y(x)y(x)y(x): y(x)=g(x)−1+Ce−g(x)y(x) = g(x) - 1 + C e^{-g(x)}y(x)=g(x)−1+Ce−g(x)

  7. Use the initial condition to find the constant C. We are given the initial condition y(0)=0y(0) = 0y(0)=0 and also that g(0)=0g(0) = 0g(0)=0. Substitute x=0x=0x=0 into the general solution: y(0)=g(0)−1+Ce−g(0)y(0) = g(0) - 1 + C e^{-g(0)}y(0)=g(0)−1+Ce−g(0) 0=0−1+Ce−00 = 0 - 1 + C e^{-0}0=0−1+Ce−0 0=−1+C(1)0 = -1 + C(1)0=−1+C(1) C=1C = 1C=1

  8. Write the particular solution. With C=1C=1C=1, the particular solution is: y(x)=g(x)−1+e−g(x)y(x) = g(x) - 1 + e^{-g(x)}y(x)=g(x)−1+e−g(x)

  9. Calculate the value of y(2). We need to find y(2)y(2)y(2). We are given that g(2)=0g(2) = 0g(2)=0. Substitute x=2x=2x=2 into the particular solution: y(2)=g(2)−1+e−g(2)y(2) = g(2) - 1 + e^{-g(2)}y(2)=g(2)−1+e−g(2) y(2)=0−1+e−0y(2) = 0 - 1 + e^{-0}y(2)=0−1+e−0 y(2)=−1+1y(2) = -1 + 1y(2)=−1+1 y(2)=0y(2) = 0y(2)=0

Alternative Method (Using Definite Integration)

Starting from Step 3: ddx[y(x)eg(x)]=g(x)g′(x)eg(x)\frac{d}{dx} \left[ y(x) e^{g(x)} \right] = g(x)g'(x)e^{g(x)}dxd​[y(x)eg(x)]=g(x)g′(x)eg(x) Integrate both sides from x=0x=0x=0 to x=2x=2x=2: ∫02ddx[y(x)eg(x)]dx=∫02g(x)g′(x)eg(x)dx\int_{0}^{2} \frac{d}{dx} \left[ y(x) e^{g(x)} \right] dx = \int_{0}^{2} g(x)g'(x)e^{g(x)} dx∫02​dxd​[y(x)eg(x)]dx=∫02​g(x)g′(x)eg(x)dx By the Fundamental Theorem of Calculus, the LHS is: [y(x)eg(x)]02=y(2)eg(2)−y(0)eg(0)\left[ y(x) e^{g(x)} \right]_0^2 = y(2)e^{g(2)} - y(0)e^{g(0)}[y(x)eg(x)]02​=y(2)eg(2)−y(0)eg(0) Given y(0)=0y(0)=0y(0)=0, g(0)=0g(0)=0g(0)=0, and g(2)=0g(2)=0g(2)=0: LHS=y(2)e0−0⋅e0=y(2)LHS = y(2)e^{0} - 0 \cdot e^{0} = y(2)LHS=y(2)e0−0⋅e0=y(2) For the RHS, let t=g(x)t = g(x)t=g(x), so dt=g′(x)dxdt = g'(x)dxdt=g′(x)dx. The limits of integration change from x=0,2x=0, 2x=0,2 to t=g(0)=0,g(2)=0t=g(0)=0, g(2)=0t=g(0)=0,g(2)=0. RHS=∫g(0)g(2)tetdt=∫00tetdt=0RHS = \int_{g(0)}^{g(2)} t e^t dt = \int_{0}^{0} t e^t dt = 0RHS=∫g(0)g(2)​tetdt=∫00​tetdt=0 Equating LHS and RHS: y(2)=0y(2) = 0y(2)=0

The final answer is 0.

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