Animated Solution for Mathematics - Differential Equations: Let y=y(x) be the solution of the differential equation dxdy+2cos4x−cos2x2y=xetan−1(2cot2x),0<x<π/2 with y(4π)=32π2. If y(3π)=18π2e−tan−1(α), then the value of 3α2 is equal to _______.
Enter Numerical Value:
Visualized Solution
Identify the Form of the Differential Equation
The given equation is a Linear Differential Equation (LDE).
Welcome, future engineer. Today, we are going to dismantle a problem that, at first glance, looks like it was designed to haunt your dreams. You see an equation like
dxdy+2cos4x−cos2x2y=xetan−1(2cot2x)
and your instinct might be to panic. But take a deep breath. In the world of JEE Advanced, intimidation is just a mask for elegance.
This is a classic Linear Differential Equation (LDE) of the form dxdy+P(x)y=Q(x). Our mission is to identify P(x) and Q(x) and then find the key to the kingdom: the Integrating Factor.
Taming the Denominator
The Art of Simplification
The real challenge here is the denominator of P(x), which is 2cos4x−cos2x. If we try to integrate this directly, we will be stuck in a swamp of trigonometric powers. We need a transformation.
Recall the double-angle identity: cos2x=2cos2x−1. Let us substitute this into our denominator:
2cos4x−(2cos2x−1)=2cos4x−2cos2x+1
Now, look at the identity 1+cos22x. If we expand this, we get 1+(2cos2x−1)2=1+4cos4x−4cos2x+1=4cos4x−4cos2x+2.
Notice that this is exactly 2(2cos4x−2cos2x+1). This means our denominator is simply 21+cos22x.
Suddenly, the monster has been tamed. Our P(x) becomes:
P(x)=1+cos22x22
The Integrating Factor
The Strategic Substitution
Now that we have a clean P(x), we calculate the Integrating Factor (I.F.):
I.F.=e∫P(x)dx=e∫1+cos22x22dx
To solve this integral, we use a classic trick: divide the numerator and denominator by sin22x. This transforms the integral into:
∫csc22x+cot22x22csc22xdx
Using the identity csc22x=1+cot22x, the denominator becomes 1+2cot22x. Now, let u=2cot2x. Then du=−22csc22xdx.
The integral becomes ∫1+u2−du, which is simply −tan−1(u). Thus, our I.F. is e−tan−1(2cot2x).
The Grand Cancellation
The Moment of Clarity
This is the most satisfying part of the journey. The general solution is y⋅(I.F.)=∫Q(x)⋅(I.F.)dx+C. Substituting our values:
See that? The exponential terms are inverses of each other. They multiply to 1.
The entire complex exponential structure vanishes, leaving us with the simple integral:
∫xdx=2x2+C
The Final Stretch
Finding the Result
With the general solution y⋅e−tan−1(2cot2x)=2x2+C, we use the initial condition y(4π)=32π2 to find C. Since cot(2π)=0, the exponential term becomes 1, and we find C=0.
Finally, we evaluate y(3π). Substituting x=3π, we get cot(2x)=cot(32π)=−31.
This leads us to the final evaluation. Following the logic of the problem constraints, we arrive at our final answer: 2.