i need to solve this ODE using Laplace transform. $\theta(t)$ is the Heaviside step function. $x$ and $x'$ both have a Laplace Transform.
$$ x'(t) = \sin(2t)\theta(t-\pi)+\int_0^{\infty}x(t-\tau)d\tau~~~~, ~~~~~x(0)=0 $$
I'm having trouble with the improper integral. By definition know that: $$ \mathcal{L}\{f(t)\}(s)=\int_0^\infty e^{-st}f(t)dt $$
So
$$\mathcal{L}\left\{\int_0^{\infty}x(t-\tau)d\tau\right\}(s)=\int_0^\infty e^{-st}\int_0^{\infty}x(t-\tau)d\tau dt $$
Since $e^{-st}$ does not depend of $\tau$
$$\mathcal{L}\left\{\int_0^{\infty}x(t-\tau)d\tau\right\}(s)=\int_0^\infty \int_0^{\infty}e^{-st}x(t-\tau)d\tau dt $$
And using a Laplace Transform Table the equation would be:
$$sX(s) = e^{-\pi s}\frac{2}{s^2+4} + \int_0^\infty \int_0^{\infty}e^{-st}x(t-\tau)d\tau dt ~~~~,~~~~X(s)=\mathcal{L}\{x(t)\}(s)$$
As I said before, I am having a lot of trouble with the improper integral... don't really know what to do so i can find $X(s)$ and then do the inverse transform. Really blocked here.
Thanks a lot.
EDIT:
$$\int_0^\infty \int_0^{\infty}e^{-st}x(t-\tau)d\tau dt = \int_0^\infty \int_0^{\infty}e^{-st}x(t-\tau) \frac{e^{-\tau t}}{e^{-\tau t}}d\tau dt $$ If I change switch $dt$ and $d \tau$ $$\int_0^\infty e^{-\tau t} \int_0^{\infty}e^{-s(t-\tau)}x(t-\tau) e^{-\tau t} dt d\tau ≟ \int_0^\infty e^{-\tau t} \mathcal{L}\{x(t-\tau)\}(s) d\tau $$ Now, how can I take this to an expression with $X(s)$?
EDIT2: Someone told me I could use the convolution product. This solves my problem but i'd really like to know if I could've done something with what I tried in the first place. $$\int_0^{\infty}x(t-\tau)d\tau = 1 \ast x(t) $$