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Aspen Physical Property System - Physical Property Models

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standard RKS alpha function, except that the Grabovsky-Daubert alpha<br />

function is used for H2: � = 1.202 exp(-0.30228xTri)<br />

References<br />

J. F. Boston and P.M. Mathias, "Phase Equilibria in a Third-Generation Process<br />

Simulator" in Proceedings of the 2nd International Conference on Phase<br />

Equilibria and Fluid Properties in the Chemical Process Industries, West Berlin,<br />

(17-21 March 1980), pp. 823-849.<br />

P. M. Mathias, "A Versatile Phase Equilibrium Equation-of-state", Ind. Eng.<br />

Chem. Process Des. Dev., Vol. 22, (1983), pp. 385–391.<br />

P.M. Mathias and T.W. Copeman, "Extension of the Peng-Robinson Equationof-state<br />

To Complex Mixtures: Evaluation of the Various Forms of the Local<br />

Composition Concept", Fluid Phase Eq., Vol. 13, (1983), p. 91.<br />

O. Redlich and J. N. S. Kwong, "On the Thermodynamics of Solutions V. An<br />

Equation-of-state. Fugacities of Gaseous Solutions," Chem. Rev., Vol. 44,<br />

(1949), pp. 223–244.<br />

J. Schwartzentruber and H. Renon, "Extension of UNIFAC to High Pressures<br />

and Temperatures by the Use of a Cubic Equation-of-state," Ind. Eng. Chem.<br />

Res., Vol. 28, (1989), pp. 1049–1055.<br />

J. Schwartzentruber, H. Renon, and S. Watanasiri, "K-values for Non-Ideal<br />

<strong>System</strong>s:An Easier Way," Chem. Eng., March 1990, pp. 118-124.<br />

G. Soave, "Equilibrium Constants for a Modified Redlich-Kwong Equation-ofstate,"<br />

Chem Eng. Sci., Vol. 27, (1972), pp. 1196-1203.<br />

C.H. Twu, W.D. Sim, and V. Tassone, "Getting a Handle on Advanced Cubic<br />

Equations of State", Chemical Engineering Progress, Vol. 98 #11 (November<br />

2002) pp. 58-65.<br />

Huron-Vidal Mixing Rules<br />

Huron and Vidal (1979) used a simple thermodynamic relationship to equate<br />

the excess Gibbs energy to expressions for the fugacity coefficient as<br />

computed by equations of state:<br />

Equation 1 is valid at any pressure, but cannot be evaluated unless some<br />

assumptions are made. If Equation 1 is evaluated at infinite pressure, the<br />

mixture must be liquid-like and extremely dense. It can be assumed that:<br />

Using equations 2 and 3 in equation 1 results in an expression for a/b that<br />

contains the excess Gibbs energy at an infinite pressure:<br />

2 Thermodynamic <strong>Property</strong> <strong>Models</strong> 79<br />

(1)<br />

(2)<br />

(3)<br />

(4)

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