Aim of the paper is to provide a method to analyze the behavior of
T-periodic solutions x_\eps, \eps>0, of a perturbed planar Hamiltonian
system near a cycle x0, of smallest period T, of the unperturbed system.
The perturbation is represented by a T-periodic multivalued map which
vanishes as \eps\to0. In several problems from nonsmooth mechanical systems
this multivalued perturbation comes from the Filippov regularization of a
nonlinear discontinuous T-periodic term. \noindent Through the paper,
assuming the existence of a T-periodic solution x_\eps for \eps>0 small,
under the condition that x0 is a nondegenerate cycle of the linearized
unperturbed Hamiltonian system we provide a formula for the distance between
any point x0(t) and the trajectories x_\eps([0,T]) along a transversal
direction to $x_0(t).