  We present a probabilistic proof of the mean-field limit and propagation of
chaos of a N-particle system in three dimensions with compactly supported pair
potentials of the form $N^{3\beta-1} \phi(N^{\beta}x)$ for
$\beta\in\left[0,\frac{1}{7}\right)$ and $\phi\in L^{\infty}(\mathbb{R}^3)\cap
L^1(\mathbb{R}^3)$. In particular, for typical initial data, we show
convergence of the Newtonian trajectories to the characteristics of the
Vlasov-Dirac-Benney system with delta-like interactions. The proof is based on
a Gronwall estimate for the maximal distance between the exact microscopic
dynamics and the approximate mean-field dynamics. Thus our result leads to a
derivation of the Vlasov-Dirac-Benney equation from the microscopic
$N$-particle dynamics with a strong short range force.
