This is a similar problem to the one I posted earlier with some differences.
Attempt at solution:
- Write $g(t)$ as a heaviside function.
- Take Laplace transform of LHS and RHS.
- Solve for Y.
- Take inverse laplace of Y. This gives me a function $y(t) = something$.
How do I change my answer that I get as $y(t)$ into the form they want in the image?
How do I write $g(t)$ as a Heaviside function? I get $g(t) = t + (2\pi-t)u$, where $u$ is the Heaviside $u$ of $2\pi$.
$g(t) $ should have the form in terms of Heaviside function