The problem is the following

The thing that puzzles me here is the integral on the right hand side, so:
How to take the laplace transform on the right hand side?
Any help to get me going would be greatly appreciated.
The problem is the following

The thing that puzzles me here is the integral on the right hand side, so:
How to take the laplace transform on the right hand side?
Any help to get me going would be greatly appreciated.
On
The convolution theorem is \begin{align} F(s)*G(s) = \int_{0}^{t} g(t-\tau) f(\tau) d\tau \end{align} such that \begin{align} L\{ f*g\} = L\{ \int_{0}^{t} g(t-\tau) f(\tau) d\tau \} = F(s)G(s). \end{align} The differential equation then becomes \begin{align} L\{ y^{''} + 3 y^{'} + 2y \} = L\{ H(t-\pi) \sin(2t) \} + \delta(s) f(s) - \delta(s-2) f(s). \end{align} Completing the transform the equation becomes \begin{align} (s+1)(s+2) y(s) - (s+1) y(0) - y^{'}(0) = \frac{2 e^{-\pi s}}{s^{2} + 4} + \delta(s) f(s) - \delta(s-2) f(s). \end{align} Since $y^{'}(0) = 0$ and $y(0) = 1$, and $f(t+2) = f(t)$ then \begin{align} y(s) &= \frac{1}{s+2} + \frac{1}{(s+1)(s+2)} \left[ \frac{2 e^{-\pi s}}{s^{2} + 4} + \delta(s) f(s) - \delta(s-2) f(s) \right] \\ &= \frac{1}{s+2} + \frac{1}{(s+1)(s+2)} \left[ \frac{2 e^{-\pi s}}{s^{2} + 4} + f(0) - f(2) \right] \\ &= \frac{1}{s+2} + \frac{1}{(s+1)(s+2)} \left[ \frac{2 e^{-\pi s}}{s^{2} + 4} \right] \\ \end{align} Inversion leads to \begin{align} y(t) &= e^{-2t} + L^{-1}\{ \frac{1}{(s+1)(s+2)} \cdot \frac{2 e^{-\pi s}}{s^{2} + 4} \} \\ &= e^{-2t} + \frac{1}{20} H(t-\pi) \left[ 8 e^{\pi - t} - 5 e^{2(\pi -t)} - \sin(2t) - 3 \cos(2t) \right]. \end{align}
note: the convolution theorem is in most standard tables such as this one http://tutorial.math.lamar.edu/pdf/Laplace_Table.pdf
The integral on the right-hand side can be rewritten as
$$\int_{0}^t(\delta(t-\tau)-\delta(t-2-\tau))f(\tau)d\tau=f(t)-f(t-2)=f(t),\quad 0\le t<2\quad\textrm{(and zero otherwise)}$$
So its Laplace transform is simply
$$\int_0^2f(t)e^{-st}dt$$
Also note that $h(t-\pi)\sin(2t)=h(t-\pi)\sin(2(t-\pi))$, so you can simply use the transform of $h(t)\sin(2t)$ and use the shifting property, i.e. multiply by $e^{-s\pi}$.