Lattice model of living polymerization. II. Interplay between polymerization and phase stability

Citation
J. Dudowicz et al., Lattice model of living polymerization. II. Interplay between polymerization and phase stability, J CHEM PHYS, 112(2), 2000, pp. 1002-1010
Citations number
67
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF CHEMICAL PHYSICS
ISSN journal
00219606 → ACNP
Volume
112
Issue
2
Year of publication
2000
Pages
1002 - 1010
Database
ISI
SICI code
0021-9606(20000108)112:2<1002:LMOLPI>2.0.ZU;2-A
Abstract
Representative spinodal curves and polymerization lines for the equilibrium polymerization of linear polymers in a solvent have been calculated using a Flory-Huggins-type mean-field theory. The calculations are primarily rest ricted to systems that polymerize upon cooling, but examples are also given for systems that polymerize upon heating. In the former case, we find that an increase in the magnitude of enthalpy of propagation \Delta h\ ("sticki ng energy") leads to an elevation of the critical temperature T-c and to a decrease of the critical composition phi(c) when \Delta h\ exceeds a critic al value \Delta h(c)\. The shifts in the critical temperature and compositi on, Delta T-c = T-c(Delta h) - T-c(Delta h = 0) and Delta phi(c) = phi(c)(D elta h)-phi(c)(Delta h = 0), vary linearly with Delta h for \Delta h\>\Delt a h(c)\ over a large range of sticking energies \Delta h\, so that Delta T- c is proportional to Delta phi(c) for a sufficiently large sticking energy. Variations in the phase boundaries with Delta h are also evaluated for sys tems that polymerize upon heating, but the presence of multiple critical po ints in this case renders a general description of these changes difficult. The polymerization line is found to be independent of solvent quality (chi interaction parameter) within the simple Flory-Huggins model, but the phas e stability is strongly influenced by the magnitude of both chi and Delta h . Similarities between living polymers and other types of associating polym ers (thermally reversible gels, micelles) suggest that some of the thermody namic consequences of particle association in these self-assembling systems are insensitive to the detailed nature of the clustering process. Thus, ou r results may have a much broader range of applicability than living polyme r solutions (e.g., gelation in clay and other colloidal suspensions, polyel ectrolyte solutions, cell aggregation, and self-organization of biologicall y significant structures that exist at equilibrium). (C) 2000 American Inst itute of Physics. [S0021-9606(00)50102-0].