We give a continuation principle for forced oscillations of second order differential
equations on not necessarily compact differentiable manifolds. A topological sufficient
condition for an equilibrium point to be a bifurcation point for periodic orbits is a
straightforward consequence of such a continuation principle. Known results on open
sets of euclidean spaces as well as a recent continuation principle for forced
oscillations on compact manifolds with nonzero Euler-Poincaré characteristic are
also included as particular cases.