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Aspen Physical Property System - Physical Property Models

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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 – 1955.<br />

A. Peneloux, E. Rauzy, and R. Freze, "A Consistent Correction For Redlich-<br />

Kwong-Soave Volumes", Fluid Phase Eq., Vol. 8, (1982), pp. 7–23.<br />

H. Knapp, R. Döring, L. Oellrich, U. Plöcker, and J. M. Prausnitz. "Vapor-Liquid<br />

Equilibria for Mixtures of Low Boiling Substances." Dechema Chemistry Data<br />

Series, Vol. VI.<br />

Redlich-Kwong-Soave-Boston-Mathias<br />

The Redlich-Kwong-Soave-Boston-Mathias equation-of-state is the basis for<br />

the RKS-BM property method. It is the Redlich-Kwong-Soave equation-ofstate<br />

with the Boston-Mathias alpha function (see Soave Alpha Functions). It<br />

is recommended for hydrocarbon processing applications, such as gasprocessing,<br />

refinery, and petrochemical processes. Its results are comparable<br />

to those of the Peng-Robinson-Boston-Mathias equation-of-state.<br />

Note: You can choose any of the available alpha functions, but you cannot<br />

define multiple property methods based on this model using different alpha<br />

functions within the same run.<br />

The equation is:<br />

p =<br />

Where:<br />

a0 is the standard quadratic mixing term:<br />

a1 is an additional, asymmetric (polar) term:<br />

b =<br />

ai<br />

bi<br />

=<br />

=<br />

kij = kji<br />

2 Thermodynamic <strong>Property</strong> <strong>Models</strong> 55

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