Abstract
A new riogorous equation of state (EOS) and its simplified version have been proposed by the present authors based on the full Guggenheim combinatorics ] of the nonrandom lattice hole theory. The simplified EOS. with the introduction of the concept of local composition, becomes similar to the density-dependent UNIQUAC model. However, im the present approach we have a volumetric EOS instead of the excess Gibbs function. Both EOSs were tested for their applicability in correlating the phase equilibria behavior of pure components and complex mixtures. Comparison of both models with experiment includes such systems as nonpolar nonpolar, nonpolar polar, and polar polar hydrocarbons, supercritical systems, and polymer solutions. With two parameters for each pure component and one binary interaction energy parameter, results obtained to date demonstrate that both formulations are quantitatively applicable to complex systems oer a wide range of temperatures, pressures, and concentrations.
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References
E. A. Guggenheim,Mixtures (Clarendon Press, Oxford, 1952), pp.215–252.
C. Panayiotou and J. H. Vera,Can. J. Chem. Eng. 59:501 (1981).
P. J. Flory,J. Chem. Phys. 9:660 (1941); J. Chem. Phys.10:51 (1942).
M. L. Huggins,J. Chem. Phys. 9:440 (1941).
D. Abrams and J. M. Prausnitz,AIChE J. 21:116 (1975).
I. C. Sanchez and R. H. Lacombe,J. Phys. Chem. 80:2352, 2568 (1976).
I. C. Sanchez and R. H. Lacombe,Macromolecules 11:1 145 (1978).
C. Panayiotou and J. H. Vera.Polym. J. 14:681 (1983).
H. V. Kehiaian, J.-P. E. Grolier, and G. C. Bebson,J. Chim. Phys. 75:1031 (1978).
M. Okada and T. Nose,Polym. J. 13:399, 591 (1981).
S. K. Kumar, U. W. Suter. and R. C. Reid.Ind. Eng. Chem. Res. 26:2532 (1987).
N. A. Smirnova and A. I. Victorov,Fluid Phase Equil. 34:235 (1987).
S. S. You, C. S. Lee, and K. P. Yoo,J. Supercrit. Fluids 6:69 (1991).
S. S. You, K. P. Yoo. and C. S. Lee,Fluid Phase Equil. 93:193 (1994).
S. S. You, K. P. Yoo, and C. S. Lee,Fluid Phase Equil. 93:215 (1994).
M. S. Shin, S. J. Yoo, K. P. Yoo, S, S. You, and C. S. Lee, Fluid Phase Equil. (1995). in press,
G. M. Wilson,J. Am. Chem. Soc. 86:127 (1964).
J. H. Hong and R. Kobayashi,Fluid Phase Equil. 41:269 (1988).
D. Peng and D. Robinson.Ind. Eng. Chem. Fundam. 15:59 (1976).
P. J. Flory,Trans, Faraday Soc. 49:7 (1970).
C. E. H. Bawn and R. D. Patel.Trans. Faraday. Soc. 52:1664 (1956).
B. E. Eichinger and P. J. Flory.Trans. Faraday Soc. 64:2742 (1953).
23.Y. H. Chang and D. C. Bonner,J. Appl. Polym. Sci. 19:2457 (1975).
C. Booth and G. N. Malcolm.Polymer 12:309 (1971).
T. Oishi and J. M. Prausnitz,Ind. Eng. Chem. Res. 26:1382 (1987).
J. H. Anderson, P. Rasmussen, and A. Fredenslund,Ind. Eng. Chem. Res. 26:382 (1987).
M. S. High and R. P. Danner,AIChE J. 36:1625 (1990).
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Shin, M.S., Yoo, K.P., You, S.S. et al. A new nonrandom lattice fluid model and its simplification by two-liquid theory for phase equilibria of complex mixtures. Int J Thermophys 16, 723–731 (1995). https://doi.org/10.1007/BF01438857
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DOI: https://doi.org/10.1007/BF01438857