The behaviour of the long-time self-diffusion tensor in concentrated colloi
dal dispersions is studied using dynamic simulation The simulations are of
a suspension of monodisperse Brownian hard spheres in simple shear flow as
a function of the Peclet number, Pe, which measures the relative importance
of shear and Brownian forces, and the volume fraction, phi. Here, Pe = (y)
over dot a(2)/D-0, where (y) over dot is the shear rate, a the particle si
ze and D-0 = kT/6 pi eta a is the Stokes-Einstein diffusivity of an isolate
d particle of size a with thermal energy kT in a solvent of viscosity eta.
Two simulations algorithms are used: Stokesian Dynamics for inclusion of th
e many-body hydrodynamic interactions, and Brownian Dynamics for suspension
s without hydrodynamic interactions. A new procedure for obtaining high-qua
lity diffusion data based on averaging the results of many short simulation
s is presented and utilized. At low shear rates, low Pe, Brownian diffusion
due to a random walk process dominates and the characteristic scale for di
ffusion is the Stokes-Einstein diffusivity, D-0. At zero Pe the diffusivity
is found to be a decreasing function of phi. As Pe is slowly increased, O(
Pe) and O(Pe(3/2)) corrections to the diffusivity due to the flow are clear
ly seen in the Brownian Dynamics system in agreement with the theoretical r
esults of Morris & Brady (1996). At large shear rates, large Pe, both syste
ms exhibit diffusivities that grow linearly with the shear rate by the non-
Brownian mechanism of shear-induced diffusion. In contrast to the behaviour
at low Pe, this shear-induced diffusion mode is an increasing function of
phi. Long-time rotational self-diffusivities are of interest in the Stokesi
an Dynamics system and show similar behaviour to their translational analog
ues. An off-diagonal long-time self-diffusivity, D-xy, is reported for both
systems. Results for both the translational and rotational D-xy show a sig
n change from low Pe to high Pe due to different mechanisms in the two regi
mes. A physical explanation for the off-diagonal diffusivities is proposed.