  This work is based on a formulation of the incompressible Navier-Stokes
equations developed by P. Constantin and G.Iyer, where the velocity field of a
viscous incompressible fluid is written as the expected value of a stochastic
process. If we take $N$ copies of the above process (each based on independent
Wiener processes), and replace the expected value with the empirical mean, then
it was shown that the particle system for the Navier-Stokes equations does not
dissipate all its energy as $t \to \infty$.
  In contrast to the true (unforced) Navier-Stokes equations, which dissipate
all of its energy as $t \to \infty$. The objective of this short note is to
describe a resetting procedure that removes this deficiency. We prove that if
we repeat this resetting procedure often enough, then the new particle system
for the Navier-Stokes equations dissipates all its energy.
