Abstract
Recent experiments on phase separation and criticality in ionic fluids are reviewed briefly. The data suggest a sharp distinction betweensolvophobic criticality, displayed by nonionic fluids and some electrolytes, that is associated with Ising-like exponents, β≅0.325, γ≅1.239, and ν≅0.631, andCoulombic (orionic)criticality characterized by classical, van der Waals exponents, β=0.5, γ=1, and ν=0.5. Only experiments on the sodium-ammonia system seem to straddle this dichotomy: they show crossover from classical to Ising behavior close toT c at a characteristic crossover scalet x=|Tx−Tc|/Tc. A range of theoretical issues thus raised is discussed, including other conceivable options (spherical model, tricriticality, etc.). Attention is drawn to Nabutovskii's work and various scenarios are illustrated with the aid of schematic phase diagrams containing multicritical points that could, in principle, separate two distinct universality classes of electrolyte criticality. The advantages of examining a basic four-state lattice model that allows for ionic association-dissociation, etec., are reviewed. The issue of the existence, location, and nature of the long-heralded but still elusive gas-liquid transition and critical point in the continuum restricted primitive model (hard spheres carrying charges +q and −q) is taken up in further detail. Earlier theoretical work and recent Monte Carlo simulations are summarized. In an effort to obtain a physically transparent, semiquantitative description, the work of Debye and Hückel and its subsequent elaboration via Bjerrum's concept of bound ion paris is revisited and seen to predict phase separation and criticality. Recent work by Levin and the author is described which repairs serious defects of the earlier theories by including the interaction of the ion-pair dipoles with the screening ionic fluid, following Debye-Hückel methods. The resulting mean field theory agrees quite well with the simulations and appears to embody the most crucial physical effects. However, the role of critical fluctuations, the related interplay of the charge and density correlation functions, the likelihood of Ising-like behavior, and the associated crossover scalet x remain important unsettled questions. An Appendix presents a critique of arguments by Stell to the effect that the restricted primitive model should display Ising behavior and that 1/r 4 effective interactions might be significant.
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References
P. Chieux and M. J. Sienko,J. Chem. Phys. 53:566 (1970).
R. R. Singh and K. S. Pitzer,J. Am. Chem., Soc. 110:8723 (1988).
R. R. Singh and K. S. Pitzer,J. Chem. Phys. 92:6775 (1990).
M. L. Japas and J. M. H. Levelt Sengers,J. Phys. Chem. 94:5361 (1990).
K. S. Pitzer,Acc. Chem. Res. 23:333 (1990).
J. M. H. Levelt Sengers and J. A. Given,Mol. Phys. 80:899 (1993).
B. Hafskjold and G. Stell, inThe Liquid State of Matter, E. W. Montroll and J. L. Lebowitz, eds. (North-Holland, Amsterdam, 1982), p. 175, esp. Section 6.4.
J. S. Høye and G. Stell,J. Phys. Chem. 94:7899 (1990).
G. Stell,Phys. Rev. A 45:7628 (1992).
J.-H. Chen, M. E. Fisher, and B. G. Nickel,Phys. Rev. Lett. 48:630 (1982).
P. Chieux, J.-F. Lal, L. Hily, J. Dupuy, F. Leclercq, and P. Damay,J. Phys. (Paris)Ser. IV 1991:C5-3; P. Chieux,J. Phys. (Paris)Ser. IV 1991:C5-373.
C. Caccamo and A. Giacoppo,Phys. Rev. A 42:6285 (1990).
A. Kholodenko and A. L. Beyerlein,J. Chem. Phys. 93:8405 (1990).
A. Kholodenko and A. L. Beyerlein,Phys. Lett. A 132:347 (1988).
M. E. Fisher,J. Chem. Phys. 96:3352 (1992).
H. Weingärtner, S. Wiegand, and W. Schröer,J. Chem. Phys. 96:848 (1992).
K. C. Zhang, M. E. Briggs, R. W. Gammon, and J. M. H. Levelt Sengers,J. Chem. Phys. 97:8692 (1992).
A. Kholodenko and A. L. Beyerlein,Phys. Lett. A 175:366 (1993).
M. E. Fisher, inMagnetism and Magnetic Materials 1974, AIP Conf. Proc. 24 (American Institute for Physics, New York, 1975), p. 273; M. E. Fisher and S. Sarbach,Phys. Rev. Lett. 41:1127 (1978); S. Sarbach and M. E. Fisher,J. Appl. Phys. 49:1350 (1978);50:1802 (1979).
C. J. Thompson,Mathematical Statistical Mechanics (Macmillan, New York, 1972), pp. 94–95, 104–105, Appendix C.
H. Weingärtner, T. Merkel, U. Maurer, J.-P. Conzen, H. Glasbrenner, and S. Käshammer,Ber. Buns. Phys. Chem. 95:1579 (1991).
H. L. Friedman and B. Larsen,J. Chem. Phys. 70:92 (1979).
H. Xu, H. L. Friedman, and F. O. Raineri,J. Solution Chem. 20:739 (1991).
P.-G. de Gennes,Scaling Concepts in Polymer Physics, (Cornell University Press, Ithaca, New York, 1979), Sect. IV 3et seq.
J. P. Valleau,J. Chem. Phys. 95:584 (1991).
A. Z. Panagiotopoulos,Fluid Phase Equilibria 76:97 (1992).
J. F. Douglas, private communication cited in ref. 6. J. M. H. Levelt Sengers and J. A. Given,Mol. Phys. 80:899 (1993).
P. W. Debye and E. Hückel,Physik. Z. 24:185 (1923).
D. A. McQuarrie,Statistical Mechanics (Harper and Row, New York, 1976), Chapter 15.
H. Falkenhagen and W. Ebeling, inIonic Interactions, Vol. 1, S. Petrucci, ed. (Academic Press, New York, 1971), but note slips in Eqs. (49) M. E. Fisher, S.-K. Ma, and B. G. Nickel,Phys. Rev. Lett. 29:917 (1972). and (51) G. Dietler and D. S. Cannell,Phys. Rev. Lett. 60:1852 (1988).
M. E. Fisher and M. M. Telo da Gama, unpublished.
A. Liu and M. E. Fisher,Physica A 156:35 (1989).
K. Binder, inPhase Transitions and Critical Phenomena, Vol. 5b, C. Domb and M. S. Green, eds. (Academic Press, London, 1976).
V. M. Nabutovskii, N. A. Nemov, and Yu. G. Peisakhovich,Sov. Phys. JETP 52:111 (1980) [Zh. Eksp. Teor. Fiz. 79:2196 (1980)];Phys. Lett. 79A:98 (1980);Mol. Phys. 54:979 (1985).
R. M. Hornreich, M. Luban, and S. Shtrikman,Phys. Rev. Lett. 35:1678 (1975).
S. A. Brazovskii,Sov. Phys. JETP 41:85 (1975( [Zh. Eksp. Teor. Fiz. 68:175 (1975)].
M. E. Fisher,J. Appl. Phys. 52:2014 (1981).
M. E. Fisher and W. Selke,Phys. Rev. Lett. 44:1502 (1980).
W. Selke and M. E. Fisher,Physica 15–18:403 (1982);Phys. Rev. B 20:257 (1979).
M. E. Fisher,Phys. Rev. Lett. 34:1634 (1975).
A. A. Migdal,Sov. Phys. JETP 42:743 (1976) [Zh. Eksp. Teor. Fiz. 69:1457 (1975)].
L. P. Kadanoff,Ann. Phys. (N.Y.) 100:359 (1976).
Th. Niemeijer and J. M. J. van Leeuwen, inPhase Transitions and Critical Phenomena, Vol. 6, C. Domb and M. S. Green, eds. (Academic Press, London, 1976), p. 425.
H. E. Stanley, P. J. Reynolds, S. Redner, and F. Family, inReal Space Renormalization Groups, T. W. Burkhardt and J. M. J. van Leeuwen, eds. (Springer-Verlag, Berlin, 1982).
M. Kaufman, R. B. Griffiths, J. M. Yeomans, and M. E. Fisher,Phys. Rev. B 23: 3448 (1981); J. M. Yeomans and M. E. Fisher,Phys. Rev. B 24:2825 (1981).
S. F. Edwards,Phil. Mag. 4:1171 (1959).
J. Glimm and A. Jaffe,Quantum Physics: A Functional Integral Point of View, 2nd ed. (Springer-Verlag, Berlin, 1987), Section 23.6.
D. Brydges,Commun. Math. Phys. 58:313 (1978); D. Brydges and P. Federbush,Commun. Math. Phys. 73:197 (1980).
M. E. Fisher, S.-K. Ma, and B. G. Nickel,Phys. Rev. Lett. 29:917 (1972).
V. Degiorgio, R. Piazza, M. Corti, and C. Minero,J. Chem. Phys. 82:1025 (1985); M. Corti and V. Degiorgio,Phys. Rev. Lett. 55:2005 (1985).
G. Dietler and D. S. Cannell,Phys. Rev. Lett. 60:1852 (1988).
M. E. Fisher,Phys. Rev. Lett. 57:1911 (1986).
C. Bagnuls and C. Bervillier,Phys. Rev. Lett. 58:435 (1987).
M. E. Fisher and M. C. Barbosa,Phys. Rev B 43:11117 (1991); M. C. Barbosa and M. E. Fisher,Phys. Rev. B 43:10635 (1991).
P. T. Cummings and G. Stell,J. Chem. Phys. 78:1917 (1983).
E. R. Smith,J. Stat. Phys. 50:813 (1988).
F. H. Stillinger, Jr., and R. Lovett,J. Chem. Phys. 48:3858 (1968).
D. A. McQuarrie,J. Phys. Chem. 66:1508 (1962).
G. R. Stell, K. C. Wu, and B. Larsen,Phys. Rev. Lett. 37:1369 (1976).
M. E. Fisher and Y. Levin,Phys. Rev. Lett. 71:3826 (1993); Y. Levin and M. E. Fisher, to be published.
P. N. Vorontsov-Veliaminov, A. M. El'yashevich, L. A. Morgenshtern, and V. P. Chasovshikh,Teplofiz. Vys. Temp. 8:277 (1970) [High Temp. (USSR)8:261 (1970)]
V. P. Chasovshikh, P. N. Vorontsov-Veliaminov, and A. M. El'yashevich,Dokl. Akad. Nauk. Tadzhiksko SSR 16(10):23 (1973).
V. P. Chasovskikh and P. N. Vorontsov-Veliaminov,Teplofiz. Vys. Temp. 14:199 (1976) [High Temp. (USSR)14:174 (1976)].
M. J. Gillan,Mol. Phys. 49:421 (1983).
K. S. Pitzer and D. R. Schreiber,Mol. Phys. 60:1067 (1987).
N. Bjerrum,Kgl. Danske Vidensk. Selsk. Mat.-Fys. Medd.,7:1 (1926).
B. Larsen,Chem. Phys. Lett. 27:47 (1974);J. Chem. Phys. 65:3431 (1976).
M. E. Fisher, inCritical Phenomena, Proc. 1970, E. Fermi,Int. Sch. Phys. Varenna, M. S. Green, ed., (Academic Press New York, 1971), p. 1.
V. Privman, ed.,Finite Size Scaling and Numerical Simulation of Statistical Systems (World Scientific, Singapore, 1990); J. L. Cardy, ed.Finite-Size Scaling (North-Holland, Amsterdam, 1988).
V. McGahay and M. Tomozawa,J. NonCryst. Solids 109:27 (1989);J. Chem. Phys. 97:2609 (1992).
J. S. Høye, E. Lomba, and G. Stell,Mol. Phys. 75:1217 (1992).
L. Belloni,J. Chem. Phys. 98:8080 (1993).
M. E. Fisher and S. Fishman,Phys. Rev. Lett. 47:421 (1981), and references therein.
W. Ebeling,Z. Phys. Chem. 238:400 (1968).
W. Ebeling and M. Grigo,Ann. Phys. (Leipzig)37:21 (1980).
H. Yokoyama and H. Yamatera,Bull. Chem. Soc. Japan 48:1770, (1975);Chem. Lett. 1973:337.
M.-C. Justice and J.-C. Justice,J. Solution Chem. 5:543 (1976);6:819 (1977).
R. M. Fuoss,J. Am. Chem. Soc. 80:5058 (1958).
H. L. Friedman,J. Phys. Chem. 66:1595 (1962).
M. E. Fisher, inCritical Phenomena, F. J. W. Hahne, ed. (Springer-Verlag, Berlin, 1983), p. 1.
G. Stell,Phys. Rev. B 1:2265 (1970), Section 4.
G. Stell, private communication.
Xiaojun Li, Y. Levin, and M. E. Fisher, submitted for publication; reported at the 2nd Liquid Matter Conference, Florence, Italy, September 1993.
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This article is based on a lecture delivered at the First Lars Onsager Symposium held at the Norwegian Institute of Technology, Trondheim, Norway, 2–4 June 1993.
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Fisher, M.E. The story of coulombic critiality. J Stat Phys 75, 1–36 (1994). https://doi.org/10.1007/BF02186278
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DOI: https://doi.org/10.1007/BF02186278