$$\begin{cases}
y''-y'=f(t) \\
y(0)=1 \\
y'(0)=1\\
\end{cases}
$$
$f(t)$ is
$$f(t)= \begin{cases}
-1 & 0\leq t < \pi \\
cos(t) & \pi\leq t < 2\pi \\
1 & t \geq 2\pi \\
\end{cases}
$$
what I need to do now?
- Convert $f(t)$ to one line function, if yes I would like to see.
- Force on LHS and RHS Laplace transform?
Thanks.
You can write $f(t)$ as:
$$-u(t) + u(t- \pi)(\cos t +1) + u(t-2\pi)(1- \cos t)$$
The Laplace Transform of the LHS is:
$$\mathcal{L}\{y''- y'\} = (s^2 y(s) - sy(0) - y'(0)) - (sy(s) - y(0))$$
with: $y(0)=1, y'(0)=1$
Can you continue?
Update
We now have:
$(s^2y(s) -s -1) -(s y(s)-1) = \left(-\dfrac{1}{s}\right) + \left(\dfrac{e^{-\pi s}}{s} - \dfrac{e^{-\pi s} s}{1 + s^2}\right) +\left(\dfrac{e^{-2 \pi s}}{s} - \dfrac{e^{-2 \pi s} s}{1 + s^2}\right)$
This reduces to:
$$y(s) = \dfrac{1}{s(s-1)}\left(s + \left(-\dfrac{1}{s}\right) + \left(\dfrac{e^{-\pi s}}{s} - \dfrac{e^{-\pi s} s}{1 + s^2}\right) +\left(\dfrac{e^{-2 \pi s}}{s} - \dfrac{e^{-2 \pi s} s}{1 + s^2}\right) \right)$$
An example of an inverse Laplace transform is:
$$\mathscr{L}^{-1}\left(\dfrac{1}{s(s-1)} \dfrac{e^{-\pi s}}{s} \right) = (-1 -t + \pi + e^{-\pi + t}) U(t -\pi)$$