Solve $u_{tt}-u_{xx}=e^t\sin(5x), u(t,0)=u(t,\pi)=0, u(0,x)=0,u_t(0,x)=\sin(3x)$

Laplace transorm works wonderfully for this problem.

Let $F(s,x)=\mathcal{L}(u(t,x))=\int_0^{\infty}u(t,x)e^{-st}\mathrm{d}t$ i.e. $F(s,x)$ is the Laplace transform of $u(t,x)$. Then $$\begin{eqnarray*}\mathcal{L}\Big(u_{tt}(t,x)\Big)&=&s^2F(s,x)-su(0,x)-u_{t}(0,x) \\ &=&s^2 F(s,x)-(s+1)\sin(3x)\end{eqnarray*}$$ On the other hand, $$\mathcal{L}\Big(u_{xx}(t,x)\Big)=F_{xx}(s,x)$$ Your PDE becomes $$s^2F(s,x)-(s+1)\sin(3x)-F_{xx}(s,x)=\frac{\sin(5x)}{s-1}$$ Rearrange terms to see how $$F_{xx}(s,x)-s^2F(s,x)=\frac{\sin(5x)}{1-s}-(s+1)\sin(3x)$$ which is a second order linear non$-$homogeneous DE in the spatial variable $x$. Using the method of undetermined coefficients, the general solution to this DE becomes $$F(s,x)=C_1e^{sx}+C_2e^{-sx}+\frac{\sin(5x)}{(s-1)(s^2+25)}+ \frac{(s+1)\sin(3x)}{s^2+9}$$ Here, $C_1,C_2$ are functions of $s$. Enforcing $F(s,0)=F(s,\pi)=0$ gives $C_1=C_2=0$ and yields our particular solution. $$F(s,x)=\frac{\sin(5x)}{(s-1)(s^2+25)}+ \frac{(s+1)\sin(3x)}{s^2+9}$$ Apply $\mathcal{L}^{-1}$ to recover $u$... $$u(t,x)=\Bigg({e^t \over 26}-{\cos(5t) \over 26} - {\sin(5t) \over 130}\Bigg) \sin(5x)+\Bigg(\cos(3t)+{1 \over 3}\sin(3t)\Bigg)\sin(3x)$$