“…Under suitable assumptions on F (t, x), it is proven that, when ε → 0, it holds (u ε (t), εBu ε (t)) → (u(t), 0), where u is a piecewise-continuous function solving ∇ x F (t, u(t)) = 0 (1.4) at every continuity time t. Moreover, the trajectories of the system at the jump times t i are described through the autonomous second order system It is worth noting that the presence of the damping term εBu ε is crucial for obtaining the above results, as it also will be in our setting. There are indeed examples of singularly perturbed second order potential-type equations (with vanishing inertial term), such that the dynamic solutions do not converge to equilibria, while the formal limit equation is (1.2) (see, e.g., [13]).…”