“…When Kn O(1), one must account for the finite persistence length of the particles' Brownian motion. Several approximate treatments of this effect have been given in the literature (Fuchs, 1964;Sitarski and Seinfeld, 1977;Narsimhan and Ruckenstein, 1984). However, one also requires a solution for the non-continuum gas flow driven by particle motion when the particle radius, interparticle separation, and mean-free path are all comparable, in order to accurately compute the interparticle hydrodynamic interactions.…”