Find $L^{-1}[\frac{1}{(p^2+a^2)^2}]$ by convolution.
I know that $L^{-1}[\frac{1}{(p^2+a^2)^2}]=\frac{1}{2a^2}(\frac{\sin ax}{a}-x\cos ax)$ but I don't know how to do this using convolutions. Some help would really be appreciated.
Find $L^{-1}[\frac{1}{(p^2+a^2)^2}]$ by convolution.
I know that $L^{-1}[\frac{1}{(p^2+a^2)^2}]=\frac{1}{2a^2}(\frac{\sin ax}{a}-x\cos ax)$ but I don't know how to do this using convolutions. Some help would really be appreciated.
On
While projectilemotion's answer is sound, it's worth emphasizing that the convolution theorem should hold for any factorization of the transform into well-behaved functions. For instance, we could factorize the transform of interest as \begin{align} F(p) &=\frac{1}{(p^2+a^2)^2}\\ &=\frac{1}{(p-ia)^2}\frac{1}{(p+ia)^2}\\ &=\frac{1}{p-ia}\frac{1}{p-ia}\frac{1}{p+ia}\frac{1}{p+ia}=G_+(p)^2 G_-(p)^2 \end{align} and then the convolution theorem yields
$$f(x)=L^{-1}[F(p)]=((g_+\ast g_+)\ast(g_- \ast g_-))(x)$$ where $g_\pm (x)$ are the inverse Laplace transforms of $G_\pm (p)$. But $L^{-1}[p^{-1}]=1$, so the frequency-shift formula implies $g_{\pm}(x)=L^{-1}[(p\pm i a)^{-1}]=e^{\mp i a x}$. Hence
$$(g_{\pm}\ast g_{\pm})(x) =\int_0^x g_{\pm}(y)g_{\pm}(x-y)\,dy =\int_0^x e^{\mp i a y}e^{\mp i a (x-y)}\,dx=xe^{\mp i a x}$$ and therefore
\begin{align} f(x) &=\int_0^x (g_{\pm}\ast g_{\pm})(y)(g_{\pm}\ast g_{\pm})(x-y)\,dy\\ &=\int_0^x ye^{-i a y}(x-y)e^{i a (x-y)}\,dy\\ &=e^{i a x}\int_0^x y(x-y)e^{-2i a y}\,dy. \end{align} This last integral is not simple to carry out by hand, but if we use Mathematica we correctly obtain $f(x)=\frac{1}{2a^3}\left[\sin(ax)-ax \cos(ax)\right]$. So both factorizations are equally valid as far as the convolution theorem goes (though the one used in the other answer is a good deal more efficient!)
You must evaluate $\mathcal{L}^{-1}\left\{\dfrac{1}{(s^2+a^2)^2}\right\}$
Recall that: $$\mathcal{L}^{-1}\{F(s)\cdot G(s)\}=f(t)\ast g(t)=\int_0^t f(t-\tau)g(\tau)~d\tau \tag{1}$$ Where $F(s)=\mathcal{L}\left\{f(t)\right\}$ and $G(s)=\mathcal{L}\left\{g(t)\right\}$.
The most logical and obvious choice in your case is to select $F(s)=G(s)=\dfrac{1}{s^2+a^2}$.
The inverse laplace transform of $\dfrac{1}{s^2+a^2}$ is obviously $f(t)=g(t)=\dfrac{\sin(at)}{a}$. Hence, from $(1)$ we must evaluate the following integral:
$$\begin{align} \mathcal{L}^{-1}\left\{\frac{1}{(s^2+a^2)^2}\right\}&=\int_0^t \frac{\sin(a(t-\tau))}{a}\cdot \frac{\sin(a\tau)}{a}~d\tau\\&=\frac{1}{a^2}\int_0^t \sin(a(t-\tau))\sin(a\tau)~d\tau \tag{2} \end{align}$$ Evaluating this will give you the same answer you have: $$\mathcal{L}^{-1}\left\{\frac{1}{(s^2+a^2)^2}\right\}=\frac{\sin(at)-at\cos(at)}{2a^3}$$