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Aspen Physical Property System - Physical Property Models

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Harlacher and Braun, "A Four-Parameter Extension of the Theorem of<br />

Corresponding States," Ind. Eng. Chem. Process Des. Dev., Vol. 9, (1970), p.<br />

479.<br />

W. Wagner, Cryogenics, Vol. 13, (1973), pp. 470-482.<br />

D. Ambrose, M. B. Ewing, N. B. Ghiassee, and J. C. Sanchez Ochoa "The<br />

ebulliometric method of vapor-pressure measurement: vapor pressures of<br />

benzene, hexafluorobenzene, and naphthalene," J. Chem. Thermodyn. 22<br />

(1990), p. 589.<br />

API Sour Model<br />

The API Sour model is based on the API sour water model for correlating the<br />

ammonia, carbon dioxide, and hydrogen sulfide volatilities from aqueous sour<br />

water system. The model assumes aqueous phase chemical equilibrium<br />

reactions involving CO2, H2S, and NH3. The model is not usable with chemistry<br />

in the true component approach. Use the apparent component approach with<br />

this model.<br />

The model is applicable from 20 C to 140 C. The authors developed the model<br />

using available phase equilibrium data and reported average errors between<br />

the model and measured partial pressure data as follows<br />

Compound Average Error, %<br />

Up to 60 C Above 60 C<br />

Ammonia 10 36<br />

Carbon dioxide 11 24<br />

Hydrogen sulfide 12 29<br />

Detail of the model is described in the reference below and is too involved to<br />

be reproduced here.<br />

Reference<br />

New Correlation of NH3, CO2, and H2S Volatility Data from Aqueous Sour<br />

Water <strong>System</strong>s, API Publication 955, March 1978 (American Petroleum<br />

Institute).<br />

Braun K-10 Model<br />

The BK10 model uses the Braun K-10 K-value correlations, which were<br />

developed from the K10 charts (K-values at 10 psia) for both real and pseudo<br />

components. The form of the equation used is an extended Antoine vapor<br />

pressure equation with coefficients specific to real components and pseudo<br />

component boiling ranges.<br />

This method is strictly applicable to heavy hydrocarbons at low pressures.<br />

However, our model includes coefficients for a large number of hydrocarbons<br />

and light gases. For pseudocomponents the model covers boiling ranges 450<br />

– 700 K (350 – 800F). Heavier fractions can also be handled using the<br />

methods developed by <strong>Aspen</strong>Tech.<br />

2 Thermodynamic <strong>Property</strong> <strong>Models</strong> 187

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