Aqueous
electrolyte solutions containing multivalent ions exhibit
various intriguing properties, including attraction between like-charged
colloidal particles, which results from strong ion–ion correlations.
In contrast, the classical Derjaguin–Landau–Verwey–Overbeek
theory of colloidal stability, based on the Poisson–Boltzmann
mean-field theory, always predicts a repulsive electrostatic contribution
to the disjoining pressure. Here, we formulate a general theory of
surface forces, which predicts that the contribution to the disjoining
pressure resulting from ion–ion correlations is always attractive
and can readily dominate over entropic-induced repulsions for solutions
containing multivalent ions, leading to the phenomenon of like-charge
attraction. Ion-specific short-range hydration interactions, as well
as surface charge regulation, are shown to play an important role
at smaller separation distances but do not fundamentally change these
trends. The theory is able to predict the experimentally observed
strong cohesive forces reported in cement pastes, which result from
strong ion–ion correlations involving the divalent calcium
ion.