Analyzing the Setup
We are given the differential equation:
with the initial constraint y(0)=0. At first glance, this equation appears complex, but it follows a standard structure waiting to be revealed.
The Art of Rearrangement
First, we distribute the sec2x term:
Next, we move the y term to the left side to align with the standard form of a Linear Differential Equation:
This matches the form dxdy+P(x)y=Q(x), where P(x)=sec2x and Q(x)=tanxsec2x.
The Magic of the Integrating Factor
To solve this, we calculate the Integrating Factor (I.F.):
I.F.=e∫P(x)dx=e∫sec2xdx=etanx
Multiplying the entire differential equation by etanx allows us to express the left side as the derivative of a product:
dxd(y⋅etanx)=(tanxsec2x)etanx
The Integration Challenge
Integrating both sides with respect to x, we obtain:
y⋅etanx=∫(tanxsec2x)etanxdx+C
To solve the integral on the right, we use the substitution t=tanx, which implies dt=sec2xdx:
Substituting back t=tanx, the general solution is:
Finding the Specific Path
We apply the initial condition y(0)=0 to determine the constant C:
Since tan0=0 and e0=1, we find 0=1(0−1)+C, which yields C=1. The particular solution is:
Final Calculation
Finally, we evaluate the function at x=−4π:
y(−4π)=tan(−4π)−1+e−tan(−4π)
Given tan(−4π)=−1, we substitute to get:
The final answer is e−2.