Numéro |
J. Phys. II France
Volume 7, Numéro 2, February 1997
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Page(s) | 343 - 361 | |
DOI | https://doi.org/10.1051/jp2:1997129 |
J. Phys. II France 7 (1997) 343-361
Simplified Mean Field Theory for Polyelectrolyte Phase Behaviour
Patrick B. WarrenUnilever Research Port Sunlight Laboratory, Quarry Road East, Bebington, Wirral L63 3JW, UK
(Received 21 September 1996, accepted 21 October 1996)
Abstract
Simplified mean field theory for the phase behaviour of polyelectrolytes in solution is described in detail. It can be viewed
as the polyelectrolyte analogue of Flory-Huggins theory. A basic model is analyzed, then extended to look at the effects of
multivalent ions (specifically divalent coions), of distinguishable counterions, and of an ionization equilibrium between
counterions and polyelectrolyte. Analytic transformation of the free energy to reduce the number of extensive variables facilitates
the calculation of binodal curves, tielines, spinodal curves, and the spinodal instability directions. Typical salting out
behaviour and salt partitioning are seen. Unexpectedly, a small region of three phase coexistence is found: it is examined
in detail for the basic model. In addition, the mean field spinodal is found to be identical to that occurring in common applications
of the random phase approximation, and to have an interpretation in terms of electrostatic excluded volume, including for
the ionizable polyelectrolyte case where fluctuations in the ionization equilibrium give an additional contribution to the
Debye-Hückel screening length. The reasons for this are elucidated in an Appendix.
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