The Symphony of the Differential Equation
Welcome, future engineer. Today, we are not just solving a differential equation; we are embarking on a journey to uncover the hidden structure within a seemingly chaotic expression.
When you first look at the equation
it is natural to feel a moment of hesitation. It looks cluttered and intimidating, but in the world of JEE Advanced, intimidation is often just a mask for elegance.
Phase 1
The Hidden Identity
Let us pause and observe. We have the term 3(tan2x)y and the term 3y. Both terms share a common factor of 3y.
When we factor this out, we get 3y(tan2x+1). Recalling the fundamental trigonometric identity 1+tan2x=sec2x, the complexity collapses.
Our equation transforms into:
This is now a perfectly structured Linear Differential Equation of the form dxdy+P(x)y=Q(x).
Phase 2
The Integrating Factor
We identify P(x)=3sec2x and Q(x)=sec2x. We now calculate the Integrating Factor (IF), which is the key to unlocking the left side of the equation.
The IF is defined as:
Since the integral of sec2x is tanx, our Integrating Factor becomes:
Phase 3
The Integration
Multiplying the entire equation by e3tanx, the left side becomes the derivative of a product:
dxd(y⋅e3tanx)=sec2x⋅e3tanx
To solve for y, we integrate both sides:
Using the substitution u=3tanx, we have du=3sec2xdx, or sec2xdx=3du. The integral simplifies to:
∫eu3du=31eu+C=31e3tanx+C
Phase 4
The Boundary Condition
Our general solution is:
y⋅e3tanx=31e3tanx+C⟹y=31+Ce−3tanx
We apply the initial condition y(0)=31+e3. Substituting x=0 and y=31+e3:
Thus, the specific solution is:
y(x)=31+e3⋅e−3tanx=31+e3(1−tanx)
The Final Step
Finally, we evaluate the function at x=4π. Since tan(4π)=1, the exponent becomes 3(1−1)=0.
The final result is: