Simulations of the flow of concentrated aggregated colloidal systems, at th
e particulate level, are used to investigate the distribution of stresses i
n the shear-thinning regime. It is found that the distribution of shear str
ess carried by interparticle bonds decays approximately exponentially at la
rge stresses, but with a double-exponential distribution for values of posi
tive stress. The microstructural mechanisms associated with large stresses
are manifested in clusters which dominate the positive contribution to the
stress in the system. Towards the end of shear thinning the highest forces
occur along bonds defining rods of particles aligned approximately along th
e flow-compression direction. We propose that the rheology of such systems
is determined by a rupture-reformation process of these clusters of stress
concentration during the flow. The aggregation forces play the role of enha
ncing such stress concentration by stabilizing clusters against buckling. (
C) 1999 American Institute of Physics. [S0021-9606(99)51934-X].