Progress in Organic Coatings 40 (2000) 111–117
Rheology of sterically stabilized dispersions and latices
Jan Mewis
∗
, Jan Vermant
Department of Chemical Engineering, de Croylaan 46, Katholieke Universiteit Leuven, 3001 Leuven, Belgium
Abstract
Steric stabilization is a method that is often used to properly disperse small particles. It can be applied in aqueous as well as non-aqueous
media. The rheological properties of sterically stabilized dispersions are discussed here. The various controlling parameters and the physical
mechanisms involved are reviewed. Brownian hard spheres are used as a reference. Scaling relations are presented that make it possible
to reduce data sets and to predict properties. Viscosity, yield stress, shear thickening and viscoelasticity are included. The rheological
properties are also related to the fundamental colloidal properties of the dispersions under consideration. Quantitative results are available
for monodisperse spherical particles, although the effects of particle size distribution can sometimes be predicted also quite well. In other
cases the procedures presented here can be used qualitatively to predict viscosities. © 2000 Elsevier Science S.A. All rights reserved.
Keywords: Rheology; Latex; Suspensions; Steric stabilization; Viscosity predictions; Viscosity scaling; Dynamic moduli
1. Introduction
Because of the presence of small particles most liquid
coatings can be considered colloidal suspensions. The col-
loidal stability of the system then determines whether the
particles will remain well dispersed or whether they will
flocculate. When flocculation is not desirable stability can
be induced by electrostatic repulsion between the particles,
its application is mainly restricted to aqueous media. Steric
repulsion between layers attached to the particle surface can
provide stability in any suspending medium. Electrostatic
stabilization is very effective but makes the structure and
the rheology sensitive to variations in pH or ionic strength.
Steric, or polymeric, stabilization is not affected by these
parameters but, if the suspending medium is not a good sol-
vent for the stabilizer molecules, the stability might change
with temperature.
Steric stabilization is frequently used as a suitable and ro-
bust way of ensuring proper dispersion of the particles. The
stabilizer layer can be chemically grafted on the particle
surface or, more often, physically adsorbed. The formula-
tion of such materials would obviously be accelerated if the
rheology could be predicted or estimated rather accurately
on the basis of the composition. This is the problem which
is addressed here. Only stabilizer layers of grafted polymers
and adsorbed blockcopolymers or surfactants are consid-
ered, not homopolymers or statistical copolymers as such.
In the latter case the stabilizer layer consists of a complex
∗
Corresponding author.
mixture of “tails” and “loops” of the stabilizing polymer,
whereas only “tails” are present in the other two cases. The
suspending medium can be aqueous or non-aqueous.
2. Brownian hard spheres
Various parameters affect the rheology of stable colloidal
suspensions. In the limiting case of spheres without any
interparticle interactions, only Brownian (thermal) forces
and hydrodynamic forces affect the flow behaviour. The
case of “Brownian hard spheres” is quite well documented,
experimentally and theoretically, at least for monodisperse
particles (e.g. Ref. [1]). At sufficiently low shear rates Brow-
nian motion will dominate the convective motion caused by
the flow. Under these conditions the equilibrium structure
of the particles that exist at rest is preserved during flow.
As a result the viscosity does not change with shear rate
and the contribution of the Brownian forces to the viscos-
ity is at its maximum. When increasing the shear rate the
Brownian motion will, at a certain stage, become slower
than the convective motion. From then on the contribution
of the Brownian motion to the viscosity will gradually
decrease with increasing shear rate, whereas the hydrody-
namic contribution remains relatively constant. This causes
the viscosity to drop; a shear thinning region develops. At
still higher shear rates the Brownian contribution levels
off and becomes negligible, but an increase in hydrody-
namic effects can either compensate the decrease, causing a
pseudo-Newtonian high shear plateau, or overcompensate,
producing a shear thickening zone [2].
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