Sk. Lai et al., Realistic calculation of the low- and high-density liquid phase separationin a charged colloidal dispersion - art. no. 041511, PHYS REV E, 6304(4), 2001, pp. 1511
A realistic statistical-mechanics model is applied to describe the repulsiv
e interaction between charged colloids. The latter, in combination with the
long-range van der Waals attraction simulated under excess salt environmen
t, gives rise to a total intercolloidal particle potential showing a clear
second potential minimum. Differing from the usual Derjaguin-Landau-Verwey-
Overbeek (DLVO) model, the present model is valid at any finite concentrati
on of colloids and is thus an appropriate model for investigating the low-
and high-density liquid phase transition. Employing this two-body colloid-c
olloid potential and in conjunction with the Weeks-Chandler-Andersen [J. D.
Weeks. D. Chandler, and H. C. Andersen, J. Chem. Phys. 54, 5237 (1971)] th
ermodynamic perturbation theory, we derive analytical expressions for the p
ressure, chemical potential, and related thermodynamic functions. These the
rmodynamic quantities were used to calculate the phase diagrams of charged
colloidal dispersions in terms of the critical parameters: temperature, vol
ume fraction, and electrolyte concentration parameter k(D). Compared with t
he DLVO model, we find the areas enclosed within the spinodal decomposition
and also the liquid-liquid coexistence curves broader in the present model
for an excess salt condition kappa =k(D)sigma (0)less than or similar to 2
00, sigma (0) being the macroion diameter, in addition to exhibiting a shif
t in the critical point kappa (c) to lower values; for kappa >300, the disp
arities between the two models reduce. The same thermodynamic perturbation
theory has been employed to study also the weak reversible coagulation whos
e physical origin is attributed to the presence of the second potential min
imum. We examine various colloidal parameters that affect the structure of
the latter and deduce from our analysis the conditions of colloidal stabili
ty. In comparison with the measured flocculation data for a binary mixture
of polystyrene lattices and water, we find that our calculated results are
generally reasonable, thus lending great credence to the presently used mod
el.