  We discuss numerical aspects related to a new class of nonlinear Stochastic
Differential Equations in the sense of McKean, which are supposed to represent
non conservative nonlinear Partial Differential equations (PDEs). We propose an
original interacting particle system for which we discuss the propagation of
chaos. We consider a time-discretized approximation of this particle system to
which we associate a random function which is proved to converge to a solution
of a regularized version of a nonlinear PDE.
