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Failure of microemulsion models to exhibit a triple line in two dimensions

M. W. Matsen

  • Sektion Physik der Ludwig-Maximilians-Universität München, 8000 München 2, Germany

Phys. Rev. E 48, 2292 – Published 1 September, 1993

DOI: https://doi.org/10.1103/PhysRevE.48.2292

Abstract

Evidence has recently been presented [P. A. Slotte, Phys. Rev. A 46, 6469 (1992)] showing that a two-dimensional lattice model for water-oil-surfactant mixtures exhibits a triple line along which water-rich, oil-rich, and microemulsion phases coexist. We present an argument and numerical evidence that such a triple line will not exist if the efficiency of the surfactant is sufficient to produce a lamellar phase. The failure of the model to produce a triple line for an efficient surfactant can be linked to the fact that the surfactant monolayers separating regions of water and oil are only one dimensional. The implication is that two-dimensional models are somewhat inappropriate for modeling the amphiphilic behavior of real three-dimensional ternary mixtures.

References (20)

  1. M. W. Matsen and D. E. Sullivan, Phys. Rev. A 41, 2021 (1990); , J. Phys. II (France) 2, 93 (1992).
  2. G. Gompper and M. Schick, in Modern Ideas and Problems in Amphiphilic Science, edited by W. M. Gelbart, D. Roux, and A. Ben-Shaul (Springer-Verlag, Berlin, in press); Chem. Phys. Lett. 163, 475 (1989) Phys. Rev. B 41, 9148 (1990) M. Schick, Physica A 172, 200 (1991); J. Lerczak, M. Schick and G. Gompper, Phys. Rev. A 46, 985 (1992); M. W. Matsen, M. Schick and D. E. Sullivan, J. Chem. Phys. 98, 2341 (1993).
  3. A. Ciach, J. S. Høye and G. Stell, J. Phys. A 21, L777 (1988); J. Chem. Phys. 90, 1214 (1989) ibid. 95, 5300 (1991); A. Ciach and J. S. Høye, ibid 90, 1222 (1989); A. Ciach, ibid 96, 1399 (1992).
  4. M. Kahlweit et al., Colloid Interface Sci. 118, 436 (1987); M. Kahlweit, R. Strey, D. Haase and P. Firman, Langmuir 4, 785 (1988).
  5. M. Laradji, H. Guo, M. Grant and M. J. Zuckermann, Phys. Rev. A 44, 8184 (1991).
  6. G. Gompper and M. Schick, Phys. Rev. A 42, 2137 (1990).
  7. P. A. Slotte, Phys. Rev. A 46, 6469 (1992).
  8. M. W. Matsen and D. E. Sullivan, Phys. Rev. A 46, 1985 (1992).
  9. G. Gompper and M. Schick, Phys. Rev. 62, 1647 (1989).
  10. M. W. Matsen and D. E. Sullivan, Phys. Rev. A 44, 3710 (1991); L. Renlie, J. S. Høye, M. S. Skaf and G. Stell, J. Chem. Phys. 95, 5305 (1991).
  11. K.-V. Schubert and R. Strey, J. Chem. Phys. 95, 8532 (1991).
  12. K. Binder and D. Stauffer, in Applications of the Monte Carlo Method in Statistical Physics, edited by K. Binder (Springer-Verlag, Berlin, 1984), p. 28; D. P. Landau and K. Binder, Phys. Rev. B 17, 2328 (1978).
  13. M. Blume, Phys. Rev. 141, 517 (1966); H. W. Capel, Physica (Utrecht) 32, 966 (1966).
  14. D. P. Landau and R. H. Swendsen, Phys. Rev. B 33, 7700 (1986).
  15. P. D. Beale, Phys. Rev. B 33, 1717 (1986).
  16. W. Selke, Phys. Rep. 170, 213 (1988).
  17. I. Peschel and V. J. Emery, Z. Phys. B 43, 241 (1981).
  18. Locating the tricritical point is done by adjusting all the fields but one, phi, satisfying all but one self-consistency condition, f( φ ) =0. Then, f( φ ), which is an odd function due to the symmetry of the model, is expanded about the disordered phase solution, φ =0, in a Taylor series, f( φ ) = A φ +B φ3+ O( φ5). The locus A=0 is the second-order line, and the tricritical point occurs when A=B=0.
  19. K. Chen, C. Ebner, C. Jayaprakash and R. Pandit, Phys. Rev. A 38, 6240 (1988).
  20. We suspect the disorder phase in Ref. [18] may extend to zero temperature between their lamellar phase and their coexisting water- and oil-rich phases for the same reason we have argued that it does in the present model.

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