The anomalous behavior of the (zero frequency) shear viscosity of coll
oidal systems on approach of the gas-liquid critical point is analyzed
. As a result of hydrodynamic interactions, the anomalous behavior is
found to be qualitatively different from that of molecular systems. On
the basis of the asymptotic solution of the Smoluchowski equation for
the shear rate dependent pair-correlation function, an expression for
the non-Newtonian zero frequency viscosity of a near-critical suspens
ion is derived. The viscosity depends on two dimensionless groups: on
xi(-1) d via a cutoff function and on lambda alpha gamma xi(4) via the
structurefactor (xi is the correlation length in the equilibrium syst
em, d is the core diameter, and gamma is the shear rate). The transiti
on from weak to strong shear occurs at lambda approximate to 1. The an
omalous behavior of both the zero shear viscosity and the non-Newtonia
n characteristics is formally due to the fact that close to the critic
al point, where xi is large, a very small shear rate gamma is sufficie
nt to make lambda a large number. The critical exponent for the zero s
hear viscosity is found to be equal to that of the correlation length.
This exponent is much larger than for molecular systems, which is kno
wn to be very small (approximate to 0.03). The exponential behavior se
ts in at xi/d approximate to 3. (C) 1995 American Institute of Physics
.