  The framework of entropic dynamics (ED) allows one to derive quantum
mechanics as an application of entropic inference. In this work we derive the
classical limit of quantum mechanics in the context of ED. Our goal is to find
conditions so that the center of mass (CM) of a system of N particles behaves
as a classical particle. What is of interest is that Planck's constant remains
finite at all steps in the calculation and that the classical motion is
obtained as the result of a central limit theorem. More explicitly we show that
if the system is sufficiently large, and if the CM is initially uncorrelated
with other degrees of freedom, then the CM follows a smooth trajectory and
obeys the classical Hamilton-Jacobi with a vanishing quantum potential.
