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Aspen Physical Property System - Physical Property Models

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References<br />

B.C. Cajander, H.G. Hipkin, and J.M. Lenoir, "Prediction of Equilibrium Ratios<br />

from Nomograms of Improved Accuracy," Journal of Chemical Engineering<br />

Data, vol. 5, No. 3, July 1960, p. 251-259.<br />

J.M. Lenoir, "Predict K Values at Low Temperatures, part 1," Hydrocarbon<br />

Processing, p. 167, September 1969.<br />

J.M. Lenoir, "Predict K Values at Low Temperatures, part 2," Hydrocarbon<br />

Processing, p. 121, October 1969.<br />

Chao-Seader Pure Component Liquid<br />

Fugacity Model<br />

The Chao-Seader model calculates pure component fugacity coefficient, for<br />

liquids. It is used in the CHAO-SEA property method. This is an empirical<br />

model with the Curl-Pitzer form. The general form of the model is:<br />

Where:<br />

188 2 Thermodynamic <strong>Property</strong> <strong>Models</strong><br />

=<br />

Parameter<br />

Name/Element<br />

Symbol Default MDS Lower Limit Upper<br />

Limit<br />

Units<br />

TC T ci — — 5.0 2000.0 TEMPERATURE<br />

PC p ci — — 10 5<br />

OMEGA � i<br />

References<br />

10 8<br />

— — -0.5 2.0 —<br />

PRESSURE<br />

K.C. Chao and J.D. Seader, "A General Correlation of Vapor-Liquid Equilibria<br />

in Hydrocarbon Mixtures," AIChE J., Vol. 7, (1961), p. 598.<br />

Grayson-Streed Pure Component Liquid<br />

Fugacity Model<br />

The Grayson-Streed model calculates pure component fugacity coefficients for<br />

liquids, and is used in the GRAYSON/GRAYSON2 property methods. It is an<br />

empirical model with the Curl-Pitzer form. The general form of the model is:<br />

Where:<br />

Parameter<br />

Name/Element<br />

Symbol Default MDS Lower Limit Upper<br />

Limit<br />

Units<br />

TC T ci — — 5.0 2000.0 TEMPERATURE

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