Brownian dynamics, simulation has been used to model the dynamics and rheol
ogy of transient particle colloidal gels during formation, by quenching mon
odisperse attractive spherical colloidal particles from a supercritical sta
te point into the vapor-liquid or vapor-solid parts of the phase diagram. C
alculations were performed with particles interacting via 12:6, 24:12, and
36:18 Lennard-Jones-type interaction laws at subcritical temperatures (kT/e
psilon > 0.3, where epsilon is the depth of the potential well) and low vol
ume fractions (phi less than or equal to 0.2). These systems developed a ge
l-like morphology during the simulation with the aggregate morphology and R
heology being sensitive to the range of the attractive part of the potentia
l and its underlying phase diagram. The long range 12:6 systems rapidly for
med compact structures, whereas the systems generated using the shorter-ran
ged 24:12 and 36:18 potentials persisted in a more diffuse network for the
duration of the simulations and evolved much more slowly with time, althoug
h none showed any indication of coming to a structural or rheological arres
t. The rheology of these systems was characterized principally using linear
stress relaxation functions computed using the Green-Kubo fluctuation form
ula. An approximate direct method for computing the dynamic moduli that doe
s not rely on a Fourier transformation of the stress relaxation function wa
s also tested.,The rheology of many of the systems evolved with time from t
he initial uniform distribution of particles, to a gel-like viscoelastic ma
terial, especially for the long-range attractive interaction potentials. De
spite being the most short lived, the 12:6 potential systems give the most
pronounced gel-like rheological features. (C) 1999 The Society of Rheology.
[S0148-6055(99)01501-1].