Consider the change of variables $\xi=x+t$, $\eta=x-t$. Then
\begin{align}
\frac{\partial^2 }{\partial t^2}=\frac{\partial^2}{\partial\xi^2}-2\frac{\partial^2}{\partial\xi\partial\eta}+\frac{\partial^2}{\partial \eta^2}
\end{align}
and
\begin{align}
\frac{\partial^2 }{\partial x^2}=\frac{\partial^2}{\partial\xi^2}+2\frac{\partial^2}{\partial\xi\partial\eta}+\frac{\partial^2}{\partial \eta^2}.
\end{align}
Then the equation now becomes
\begin{align}
4\frac{\partial^2 u}{\partial\xi\partial\eta}=\cos\left[\frac{\pi}{2}(\xi-\eta)\right]\sin\left[\frac{\pi}{2}(\xi+\eta)\right]
\end{align}
since $t=\frac{1}{2}(\xi-\eta)$ and $x=\frac{1}{2}(\xi+\eta)$. The general solution to this PDE is given by
\begin{align}
u(\xi,\eta) &= \frac{1}{4}\left\{c_2(\xi)+\xi c_1(\eta)+\int_0^\xi\int_0^\eta\cos\left[\frac{\pi}{2}(s-r)\right]\sin\left[\frac{\pi}{2}(s+r)\right]\,dr\,ds\right\} \\
&= \frac{1}{4}\left\{c_2(\xi)+\xi c_1(\eta)+\frac{1}{2\pi}[\eta+\xi-\xi\cos(\pi\eta)-\eta\cos(\pi\xi)] \right\}\\
\end{align}
(just integrate with respect to both variables). Substituting our original variables, we have
\begin{align}
u(x,t)=\frac{1}{4}\left\{c_2(x+t)+(x+t)c_1(x-t)+\frac{1}{2\pi}[2x-(x+t)\cos(\pi x-\pi t)-(x-t)\cos(\pi x+\pi t)]\right\}.
\end{align}
Use the initial conditions to determine expressions for $c_1$ and $c_2$.