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JEE Main 2023
Differential Equations
Differential Equations
Hard

Question

If y = y(x) is the solution of the equation esinycosydydx+esinycosx=cosx{e^{\sin y}}\cos y{{dy} \over {dx}} + {e^{\sin y}}\cos x = \cos x, y(0) = 0; then 1+y(π6)+32y(π3)+12y(π4)1 + y\left( {{\pi \over 6}} \right) + {{\sqrt 3 } \over 2}y\left( {{\pi \over 3}} \right) + {1 \over {\sqrt 2 }}y\left( {{\pi \over 4}} \right) is equal to ____________.

Answer: 0

Solution

Key Concepts and Formulas

  • Linear First-Order 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 (I.F.): For a linear first-order differential equation, the integrating factor is eP(x)dxe^{\int P(x) dx}.
  • Solution of Linear First-Order Differential Equation: The solution is given by y(I.F.)=Q(x)(I.F.)dx+Cy \cdot (\text{I.F.}) = \int Q(x) \cdot (\text{I.F.}) dx + C, where CC is the constant of integration.

Step 1: Analyze the Given Differential Equation and Prepare for Substitution

The given differential equation is: esinycosydydx+esinycosx=cosxe^{\sin y}\cos y\frac{dy}{dx} + e^{\sin y}\cos x = \cos x We observe that the term esinycosydydxe^{\sin y}\cos y\frac{dy}{dx} resembles the derivative of esinye^{\sin y} with respect to xx. This suggests a substitution to simplify the equation.

Step 2: Introduce a Substitution

Let t=esinyt = e^{\sin y}. Then, we find dtdx\frac{dt}{dx} using the chain rule: dtdx=dtdydydx=esinycosydydx\frac{dt}{dx} = \frac{dt}{dy} \cdot \frac{dy}{dx} = e^{\sin y} \cos y \frac{dy}{dx} Substituting t=esinyt = e^{\sin y} and dtdx=esinycosydydx\frac{dt}{dx} = e^{\sin y} \cos y \frac{dy}{dx} into the original equation, we get: dtdx+tcosx=cosx\frac{dt}{dx} + t\cos x = \cos x

Step 3: Transform the Equation into a Linear First-Order Differential Equation

Rearranging the equation, we have: dtdx+(cosx)t=cosx\frac{dt}{dx} + (\cos x)t = \cos x This is a linear first-order differential equation in the form dtdx+P(x)t=Q(x)\frac{dt}{dx} + P(x)t = Q(x), where P(x)=cosxP(x) = \cos x and Q(x)=cosxQ(x) = \cos x.

Step 4: Calculate the Integrating Factor

The integrating factor (I.F.) is given by: I.F.=eP(x)dx=ecosxdx=esinx\text{I.F.} = e^{\int P(x) dx} = e^{\int \cos x dx} = e^{\sin x}

Step 5: Find the General Solution

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 the values, we have: tesinx=cosxesinxdx+Ct \cdot e^{\sin x} = \int \cos x \cdot e^{\sin x} dx + C Let u=sinxu = \sin x, so du=cosxdxdu = \cos x dx. Then, the integral becomes: eudu=eu+C=esinx+C\int e^u du = e^u + C = e^{\sin x} + C Therefore, tesinx=esinx+Ct \cdot e^{\sin x} = e^{\sin x} + C t=1+Cesinxt = 1 + Ce^{-\sin x}

Step 6: Substitute Back to Find y(x)

Substitute t=esinyt = e^{\sin y} back into the equation: esiny=1+Cesinxe^{\sin y} = 1 + Ce^{-\sin x}

Step 7: Apply the Initial Condition y(0) = 0

Given y(0)=0y(0) = 0, we substitute x=0x = 0 and y=0y = 0 into the equation: esin0=1+Cesin0e^{\sin 0} = 1 + Ce^{-\sin 0} e0=1+Ce0e^0 = 1 + Ce^0 1=1+C1 = 1 + C C=0C = 0

Step 8: Obtain the Particular Solution

Since C=0C = 0, the particular solution is: esiny=1e^{\sin y} = 1 Taking the natural logarithm of both sides: siny=ln(1)=0\sin y = \ln(1) = 0 siny=0\sin y = 0 y=nπ,nZy = n\pi, \quad n \in \mathbb{Z} Since y(0)=0y(0) = 0, we consider the solution y=0y = 0 for all xx.

Step 9: Evaluate the Expression

We need to find the value of: 1+y(π6)+32y(π3)+12y(π4)1 + y\left( \frac{\pi}{6} \right) + \frac{\sqrt{3}}{2}y\left( \frac{\pi}{3} \right) + \frac{1}{\sqrt{2}}y\left( \frac{\pi}{4} \right) Since y(x)=0y(x) = 0 for all xx: 1+0+32(0)+12(0)=1+0+0+0=11 + 0 + \frac{\sqrt{3}}{2}(0) + \frac{1}{\sqrt{2}}(0) = 1 + 0 + 0 + 0 = 1

However, the correct answer is 0. There must be an error in our steps. Let's re-examine the solution from Step 5: tesinx=cosxesinxdx+Ct e^{\sin x} = \int \cos x e^{\sin x} dx + C tesinx=esinx+Ct e^{\sin x} = e^{\sin x} + C t=1+Cesinxt = 1 + Ce^{-\sin x} esiny=1+Cesinxe^{\sin y} = 1 + Ce^{-\sin x} Using y(0)=0y(0) = 0, we have esin0=1+Cesin0e^{\sin 0} = 1 + Ce^{-\sin 0} 1=1+C1 = 1 + C C=0C = 0. So esiny=1e^{\sin y} = 1, meaning siny=0\sin y = 0 and y=0y = 0 for all xx. The expression becomes: 1+y(π/6)+32y(π/3)+12y(π/4)=1+0+0+0=11 + y(\pi/6) + \frac{\sqrt{3}}{2} y(\pi/3) + \frac{1}{\sqrt{2}} y(\pi/4) = 1 + 0 + 0 + 0 = 1.

Let's go back to the original differential equation: esinycosydydx+esinycosx=cosx{e^{\sin y}}\cos y{{dy} \over {dx}} + {e^{\sin y}}\cos x = \cos x dtdx+tcosx=cosx\frac{dt}{dx} + t \cos x = \cos x dtdx=cosx(1t)\frac{dt}{dx} = \cos x (1-t) dt1t=cosxdx\frac{dt}{1-t} = \cos x dx ln1t=sinx+C-\ln|1-t| = \sin x + C ln1t=sinxC\ln|1-t| = -\sin x - C 1t=esinxC=Aesinx1-t = e^{-\sin x - C} = Ae^{-\sin x} for some constant A. 1esiny=Aesinx1-e^{\sin y} = Ae^{-\sin x} esiny=1Aesinxe^{\sin y} = 1 - Ae^{-\sin x} When x=0x=0, y=0y=0. So esin0=1Aesin0e^{\sin 0} = 1 - Ae^{-\sin 0}. 1=1A1 = 1 - A. Therefore, A=0A = 0. This leads to the same solution esiny=1e^{\sin y} = 1, so y=0y=0.

There seems to be an error in the question itself or the given answer. Let's assume there's a typo and the initial condition is different. Suppose we want the final answer to be 0. Then: 1+y(π/6)+32y(π/3)+12y(π/4)=01 + y(\pi/6) + \frac{\sqrt{3}}{2} y(\pi/3) + \frac{1}{\sqrt{2}} y(\pi/4) = 0 y(π/6)+32y(π/3)+12y(π/4)=1y(\pi/6) + \frac{\sqrt{3}}{2} y(\pi/3) + \frac{1}{\sqrt{2}} y(\pi/4) = -1

Since the initial condition led to y=0y=0, let's try separation of variables. dtdx=cosx(1t)\frac{dt}{dx} = \cos x (1-t) dt1t=cosxdx\int \frac{dt}{1-t} = \int \cos x dx ln1t=sinx+C-\ln|1-t| = \sin x + C ln1t=sinxC\ln|1-t| = -\sin x - C 1t=esinxC=Aesinx|1-t| = e^{-\sin x - C} = A e^{-\sin x} 1esiny=Aesinx1 - e^{\sin y} = A e^{-\sin x} esiny=1Aesinxe^{\sin y} = 1 - A e^{-\sin x} siny=ln(1Aesinx)\sin y = \ln(1 - A e^{-\sin x}) y=arcsin(ln(1Aesinx))y = \arcsin(\ln(1 - A e^{-\sin x})) y(0)=0y(0) = 0, so 0=arcsin(ln(1Ae0))0 = \arcsin(\ln(1 - A e^0)) 0=arcsin(ln(1A))0 = \arcsin(\ln(1 - A)) 0=ln(1A)0 = \ln(1 - A) 1=1A1 = 1 - A, so A=0A = 0. This means we are back to y=0y=0.

Let's try y=arcsin(0)=0y = \arcsin(0) = 0.

Common Mistakes & Tips

  • Be careful with the chain rule when differentiating composite functions.
  • Remember to substitute back the original variable after solving the differential equation.
  • Always check the initial conditions to find the particular solution.

Summary

We transformed the given differential equation into a linear first-order differential equation using a suitable substitution. After finding the integrating factor and solving for the general solution, we applied the initial condition to find the particular solution. However, the initial condition y(0)=0y(0) = 0 results in the trivial solution y(x)=0y(x) = 0, which yields a final answer of 1, not 0 as provided. There might be an error in the question or the expected answer.

The final answer is 1\boxed{1}.

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