The Effects of
Salts on the Lower Consolute Boundary of a Nonionic Micellar Solution
Paresh
U. Kenkare, Carol K. Hall and Peter K. Kilpatrick
Department of Chemical Engineering, North Carolina State University, Raleigh,
North Carolina, 27695-7905
Received 17 January 1996; accepted 6 August 1996. ; Available online
A molecular model based in statistical thermodynamics is used to study salt
effects on the lower consolute boundary of the
aqueous non-ionic surfactant C8E5. The C8E5micelles
are modeled as hard spheres interacting via a temperature-dependent Yukawa attraction and the salt ions are modeled as
positively and negatively charged hard spheres interacting via a Coulombic potential. The excess thermodynamic properties
due to the Coulombic and Yukawa
potentials are evaluated using the analytical solutions to the Ornstein–Zernike equation obtained for the mean spherical
approximation closure. The Yukawa parameters for the
micelle–micelle attractions are determined by fitting the theoretical phase
diagram for a pure Yukawa fluid to the experimental
lower consolute boundary for a salt-free C8E5micelle–water
solution. Ion–solvent interactions are indirectly accounted for by using
previously determined adjusted values for the cation
size and the dielectric constant of the medium. We evaluate theoretical
coexistence curves for the C8E5micelle–salt–water
mixtures in the temperature–micelle volume fraction and temperature–salt molarity planes. We calculate the changes in the lower
critical solution temperature (LCST) for the C8E5micelle–salt–water
mixture as a function of salt concentration for the salts NaF,
NaCl, NaBr, NaI, and Na2SO4and compare the trends
seen with experiments. When ion–solvent interactions are indirectly accounted
for, the theory correctly predicts the salting-out trends exhibited by NaF, NaCl, and NaBr. For the 1:2 salt (Na2SO4),
charge effects resulting from the higher charge on the ions play a more
important role in salting-out than ion–solvent interactions do. The theory,
however, cannot predict the salting-in phenomena exhibited by NaI, thus indicating that salting-in is the result of
variations in the intermicellar attraction as a
function of the salt type and salt concentration. The theoretical results also
indicate that excluded-volume forces resulting from the different sizes of the
salt ions cannot alone account for the salting-in and salting-out phenomena
seen in aqueous nonionic micellar solutions.