  In the present paper, the reducibility is derived for the wave equations with
finitely smooth and time-quasi-periodic potential subjects to periodic boundary
conditions. More exactly, the linear wave equation
$u_{tt}-u_{xx}+Mu+\varepsilon (V_0(\omega t)u_{xx}+V(\omega t, x)u)=0,\;x\in
\mathbb{R}/2\pi \mathbb{Z}$ can be reduced to a linear Hamiltonian system of a
constant coefficient operator which is of pure imaginary point spectrum set,
where $V$ is finitely smooth in $(t, x)$, quasi-periodic in time $t$ with
Diophantine frequency $\omega\in \mathbb{R}^{n},$ and $V_0$ is finitely smooth
and quasi-periodic in time $t$ with Diophantine frequency $\omega\in
\mathbb{R}^{n},$ Moreover, it is proved that the corresponding wave operator
possesses the property of pure point spectra and zero Lyapunov exponent.
