I am trying to think of what this kind of problem is called. I illustrate it with a telegrapher's equation with (hopefully) standard notation.
Find $u:\Omega\times \mathbb{R} \to \mathbb{R}$ such that
$$ \begin{align*} u_{tt}+u_t-\nabla^2 u &= 0& \mathrm{for}\, (x,t)\in \Omega\times \mathbb{R}\\ u&= u_{bc} \sin(\omega t)& \mathrm{for}\ (x,t)\in \partial\Omega \times \mathbb{R} \end{align*} $$
The main point is that I am interested in solving the PDE for all time, or perhaps more precisely I am interested in the limit cycle behavior of the PDE, (after any transients associated to the initial condition have died down).
Mathematically, I guess a valid problem would be the following. Fine $u: \Omega \times \mathbb{R}\to \mathbb{R}$ such that $$ \begin{align*} u_{tt} +u_t - \nabla^2 u &= 0 &\mathrm{for} (x,t)\in \Omega \times \mathbb{R}\\ u &= u_{bc} \sin(\omega t)& \mathrm{for} (x,t)\in \partial\Omega \times \mathbb{R}\\ u(x,t+2\pi/\omega) &= u(x,t)& \mathrm{for} (x,t)\in \Omega \times \mathbb{R} \end{align*} $$
Does this problem have a name?