posted on 2021-12-01, 09:05authored bySamuel Stenberg, Jan Forsman
The stability of
dispersions containing charged particles may obviously
be regulated by salt. In some systems, the effective charge, as measured
by the potential some small distance away from the particles, can
have a sign opposite to the bare surface charge. If charge reversal
takes place, there is typically a salt concentration regime within
which colloidal stability increases with added salt. These experimental
findings on dispersions have been corroborated by atomic force microscopy
investigations, where an attraction is found at short separations.
This attraction is stronger than expected from standard DLVO theory,
and there has been considerable debate concerning its origin. In this
work, we use simple coarse-grained models of these systems, where
the bare surfaces carry a uniform charge density, and ion-specific
adsorption is absent. Our hypothesis is that these experimental observations
can be explained by such a simplistic pure Coulomb based model. Our
approach entails grand canonical Metropolis Monte Carlo (MC) simulations
as well as correlation-corrected Poisson-Boltzmann (cPB) calculations.
In the former case, all ions have a common size, while the cPB utilizes
a point-like model. We devote significant attention on apparent surface
charge densities and interactions between large flat model surfaces
immersed in either a 2:1 salt or a 3:1 salt. In contrast to most of
the previous theoretical efforts in this area, we mainly focus on
the weak long-ranged repulsion and its connection to an effective
surface charge. We find a charge reversal and a concomitant development
of a free energy barrier for both salts. The experimentally observed
nonmonotonic dependence of colloidal stability on the salt concentration
is reproduced using MC simulations as well as cPB calculations. A
strong attraction is observed at short range for all investigated
cases. We argue that in our model, all non-DLVO aspects can be traced
to ion–ion correlations.