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JEE Main 2024
Differential Equations
Differential Equations
Hard

Question

Let αx=exp(xβyγ)\alpha x=\exp \left(x^{\beta} y^{\gamma}\right) be the solution of the differential equation 2x2y dy(1xy2)dx=0,x>0,y(2)=loge22 x^{2} y \mathrm{~d} y-\left(1-x y^{2}\right) \mathrm{d} x=0, x > 0,y(2)=\sqrt{\log _{e} 2}. Then α+βγ\alpha+\beta-\gamma equals :

Options

Solution

Key Concepts and Formulas

  • First-Order Linear Differential Equation (LDE): 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 (I.F.): For a linear differential equation dydx+P(x)y=Q(x)\frac{dy}{dx} + P(x)y = Q(x), the integrating factor is given by I.F. =eP(x)dx= e^{\int P(x) dx}. The solution is then given by y(I.F.)=Q(x)(I.F.)dx+Cy \cdot (\text{I.F.}) = \int Q(x) \cdot (\text{I.F.}) \, dx + C.
  • Substitution: Transforming a differential equation into a simpler form by replacing a function of the dependent variable with a new variable. The chain rule is key here: ddxf(y)=f(y)dydx\frac{d}{dx}f(y) = f'(y)\frac{dy}{dx}

Step-by-Step Solution

Step 1: Rearrange the Given Differential Equation

We begin by rearranging the given differential equation to a more convenient form. The goal is to isolate dydx\frac{dy}{dx} and look for opportunities for substitution.

  • The given equation is: 2x2y dy(1xy2)dx=02 x^{2} y \mathrm{~d} y-\left(1-x y^{2}\right) \mathrm{d} x=0
  • Move the dxdx term to the right-hand side: 2x2y dy=(1xy2)dx2 x^{2} y \mathrm{~d} y = \left(1-x y^{2}\right) \mathrm{d} x
  • Divide both sides by dxdx: 2x2ydy dx=1xy22 x^{2} y \frac{\mathrm{d} y}{\mathrm{~d} x} = 1-x y^{2}
  • Divide both sides by x2x^2 (since x>0x > 0): 2ydy dx=1x2y2x2 y \frac{\mathrm{d} y}{\mathrm{~d} x} = \frac{1}{x^2} - \frac{y^{2}}{x}
  • Rearrange to group the terms containing yy: 2ydy dx+y2x=1x22 y \frac{\mathrm{d} y}{\mathrm{~d} x} + \frac{y^{2}}{x} = \frac{1}{x^2} Why this step? This arrangement highlights the term 2ydydx2y \frac{dy}{dx}, which is the derivative of y2y^2. This strongly suggests a substitution t=y2t = y^2.

Step 2: Apply the Substitution

We introduce a substitution to transform the equation into a linear differential equation.

  • Let t=y2t = y^2. Then, differentiating with respect to xx gives: dt dx=2ydy dx\frac{\mathrm{d} t}{\mathrm{~d} x} = 2y \frac{\mathrm{d} y}{\mathrm{~d} x} Why this substitution? This substitution simplifies the equation by replacing 2ydydx2y\frac{dy}{dx} with dtdx\frac{dt}{dx}, making it linear.

Step 3: Transform the Equation

Substitute t=y2t = y^2 and dtdx=2ydydx\frac{dt}{dx} = 2y \frac{dy}{dx} into the rearranged equation from Step 1:

  • Substituting into 2ydy dx+y2x=1x22 y \frac{\mathrm{d} y}{\mathrm{~d} x} + \frac{y^{2}}{x} = \frac{1}{x^2} yields: dt dx+tx=1x2\frac{\mathrm{d} t}{\mathrm{~d} x} + \frac{t}{x} = \frac{1}{x^2} This is a first-order linear differential equation in the form dtdx+P(x)t=Q(x)\frac{dt}{dx} + P(x)t = Q(x), where P(x)=1xP(x) = \frac{1}{x} and Q(x)=1x2Q(x) = \frac{1}{x^2}.

Step 4: Calculate the Integrating Factor

We calculate the integrating factor for the linear differential equation.

  • The integrating factor is given by: I.F.=eP(x)dx=e1xdx\text{I.F.} = e^{\int P(x) \, dx} = e^{\int \frac{1}{x} \, dx}
  • Since x>0x > 0, 1xdx=lnx\int \frac{1}{x} \, dx = \ln x. Therefore, I.F.=elnx=x\text{I.F.} = e^{\ln x} = x Why this step? The integrating factor transforms the left-hand side of the equation into an exact derivative.

Step 5: Find the General Solution

We find the general solution of the linear differential equation.

  • The general solution is given by: t(I.F.)=Q(x)(I.F.)dx+Ct \cdot (\text{I.F.}) = \int Q(x) \cdot (\text{I.F.}) \, dx + C
  • Substituting tt, I.F.=x\text{I.F.} = x, and Q(x)=1x2Q(x) = \frac{1}{x^2}: tx=1x2xdx+Ct x = \int \frac{1}{x^2} \cdot x \, dx + C tx=1xdx+Ct x = \int \frac{1}{x} \, dx + C
  • Since x>0x > 0, 1xdx=lnx\int \frac{1}{x} \, dx = \ln x. Thus, tx=lnx+Ct x = \ln x + C
  • Substitute back t=y2t = y^2: y2x=lnx+Cy^2 x = \ln x + C

Step 6: Apply the Initial Condition

We use the initial condition y(2)=ln2y(2) = \sqrt{\ln 2} to find the particular solution.

  • Substitute x=2x = 2 and y=ln2y = \sqrt{\ln 2} into the general solution: (ln2)22=ln2+C(\sqrt{\ln 2})^2 \cdot 2 = \ln 2 + C 2ln2=ln2+C2 \ln 2 = \ln 2 + C
  • Solve for CC: C=2ln2ln2=ln2C = 2 \ln 2 - \ln 2 = \ln 2
  • Substitute C=ln2C = \ln 2 back into the general solution: y2x=lnx+ln2y^2 x = \ln x + \ln 2 y2x=ln(2x)y^2 x = \ln(2x)

Step 7: Match the Given Form

We rewrite the particular solution to match the form αx=exp(xβyγ)\alpha x=\exp \left(x^{\beta} y^{\gamma}\right).

  • We have y2x=ln(2x)y^2 x = \ln(2x). Exponentiating both sides: ey2x=eln(2x)e^{y^2 x} = e^{\ln(2x)} ey2x=2xe^{y^2 x} = 2x 2x=exp(y2x)2x = \exp(y^2 x)
  • Rewrite y2xy^2 x as x1y2x^1 y^2: 2x=exp(x1y2)2x = \exp(x^1 y^2)

Step 8: Determine α,β,γ\alpha, \beta, \gamma

We compare 2x=exp(x1y2)2x = \exp(x^1 y^2) with αx=exp(xβyγ)\alpha x=\exp \left(x^{\beta} y^{\gamma}\right) to find the values of α,β,\alpha, \beta, and γ\gamma.

  • By comparison, we have: α=2\alpha = 2 β=1\beta = 1 γ=2\gamma = 2

Step 9: Calculate α+βγ\alpha + \beta - \gamma

Finally, we compute the value of α+βγ\alpha + \beta - \gamma.

  • α+βγ=2+12=1\alpha + \beta - \gamma = 2 + 1 - 2 = 1

Common Mistakes & Tips

  • Sign Errors: Be very careful with signs during rearrangement and substitution.
  • Logarithm Properties: Remember to use logarithm properties correctly, especially when combining or separating logarithmic terms. Also, remember that 1xdx=lnx+C\int \frac{1}{x} dx = \ln|x| + C, but since x>0x > 0, we can write lnx+C\ln x + C.
  • Integrating Factor: Double-check the calculation of the integrating factor and its application in solving the linear differential equation.

Summary

We solved the given differential equation by rearranging it, applying a suitable substitution (t=y2t = y^2), solving the resulting linear differential equation using an integrating factor, applying the initial condition to find the particular solution, and then matching the solution to the given form to determine the values of α,β,\alpha, \beta, and γ\gamma. Finally, we calculated α+βγ=1\alpha + \beta - \gamma = 1.

The final answer is 1\boxed{1}, which corresponds to option (A).

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