  In this paper we study Kac's 1D particle system, consisting of the velocities
of $N$ particles colliding at constant rate and randomly exchanging energies.
We prove uniform (in time) propagation of chaos in Wasserstein distance with
explicit polynomial rates in $N$, for both the squared (i.e., the energy) and
non-squared particle system. These rates are of order $N^{-1/3}$ (almost, in
the non-squared case), assuming that the initial distribution of the limit
nonlinear equation has finite moments of sufficiently high order ($4+\epsilon$
is enough when using the 2-Wasserstein distance). The proof relies on a
convenient parametrization of the collision recently introduced by Hauray, as
well as on a coupling technique developed by Cortez and Fontbona.
