Y [vibrations] The displacement, $u(x, t)$, of a rod is a function of position $x$ and time $t$ :
$$
\begin{aligned}
u(x, t)=&\left(A \sin \left(\frac{\omega}{\alpha} x\right)+B \cos \left(\frac{\omega}{\alpha} x\right)\right) \\
& \times[\operatorname{Csin}(\omega t)+D \cos (\omega t)]
\end{aligned}
$$
where $\alpha=\sqrt{\frac{E}{\rho}},(E$ is modulus of elasticity, $\rho$ is density of rod and $\omega$ is natural frequency of vibration). Show that $u(x, t)$ satisfies the wave equation:
$$
\alpha^{2} \frac{\partial^{2} u}{\partial x^{2}}=\frac{\partial^{2} u}{\partial t^{2}}
$$