Animated Solution for Mathematics - Differential Equations: If y=y(x) is the solution of the equation esinycosydxdy+esinycosx=cosx,y(0)=0; then 1+y(2π)+2πy′(2π)+21y′′(2π) is equal to
Enter Numerical Value:
Visualized Solution
The Given Differential Equation
Given: esinycosydxdy+esinycosx=cosx
Initial condition: y(0)=0
Substitution t=esiny
Let t=esiny
Differentiating both sides with respect to x using the chain rule:
dxdt=esiny⋅cosy⋅dxdy
Transforming to Linear Form
Substitute dxdt and t into the original equation:
dxdt+tcosx=cosx
This is a Linear Differential Equation of the form: dxdt+P(x)t=Q(x)
Calculating the Integrating Factor
Integrating Factor (I.F.) =e∫P(x)dx
I.F. =e∫cosxdx=esinx
General Solution Setup & Integration
Solution form: t⋅(I.F.)=∫Q(x)⋅(I.F.)dx
t⋅esinx=∫cosx⋅esinxdx
Let u=sinx⟹du=cosxdx
∫eudu=eu+C=esinx+C
Substituting back t
We have: tesinx=esinx+C
Substitute t=esiny back into the solution:
esinyesinx=esinx+C
Applying Initial Condition y(0)=0
Given y(0)=0, substitute x=0 and y=0:
esin0⋅esin0=esin0+C
e0⋅e0=e0+C
1⋅1=1+C⟹C=0
Simplifying the Solution
Substitute C=0 into the general solution:
esinyesinx=esinx
Dividing by esinx (since esinx=0):
esiny=1
Deducing y(x)=0
esiny=1⟹siny=0
y=nπ where n is an integer.
Since y(0)=0, the continuous solution is y(x)=0 for all x.
Finding Derivatives at x=2π
If y(x)=0 is a constant function, then:
y(2π)=0
y′(2π)=0
y′′(2π)=0
Final Evaluation
Expression to evaluate: 1+y(2π)+2πy′(2π)+21y′′(2π)
Substituting the values: 1+0+2π(0)+21(0)
Final Result: 1
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The Sigma Insight: Linear Differential Equations
Solution Diagram
Analyzing the Setup
The given differential equation is:
esinycosydxdy+esinycosx=cosx
In the heat of the JEE Advanced exam, your first instinct might be panic. You see exponentials, trigonometric functions, and a derivative all tangled together. However, the secret to mastering differential equations is to stop looking at the equation as a whole and start looking at the relationships between its parts.
The Spark of Substitution
Look at the term esiny and the term cosydxdy. The latter is the derivative of siny. This is the 'Spark' of the problem.
We define a new variable t=esiny. When we differentiate this with respect to x, we apply the chain rule:
dxdt=esiny⋅cosy⋅dxdy
By substituting this back into our original equation, we transform a non-linear nightmare into a linear dream:
dxdt+tcosx=cosx
This is a standard linear differential equation of the form dxdt+P(x)t=Q(x), where P(x)=cosx and Q(x)=cosx.
The Machinery of Integration
Now that we have a linear form, we calculate the Integrating Factor (I.F.):
I.F.=e∫P(x)dx=e∫cosxdx=esinx
We multiply the entire equation by this factor:
esinxdxdt+tcosxesinx=cosxesinx
Notice that the left side is the derivative of the product tesinx. Thus, we have:
dxd(tesinx)=cosxesinx
Integrating both sides, we get:
tesinx=∫cosxesinxdx
The integral on the right is solved by substituting u=sinx, which gives du=cosxdx. The integral becomes ∫eudu=eu+C=esinx+C. Thus:
tesinx=esinx+C
The Final Revelation
Substituting back t=esiny, we obtain:
esinyesinx=esinx+C
Applying the initial condition y(0)=0:
esin0esin0=esin0+C⇒1⋅1=1+C⇒C=0
The equation simplifies to esinyesinx=esinx. Since esinx is never zero, we divide by it to get esiny=1, which implies siny=0. Given the initial condition, y(x)=0 is the only continuous solution.
The final expression 1+y(2π)+2πy′(2π)+21y′′(2π) evaluates to: