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Aspen Physical Property System - Physical Property Models

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using<br />

and<br />

68 2 Thermodynamic <strong>Property</strong> <strong>Models</strong><br />

(22)<br />

(23)<br />

(24)<br />

Using the association model, more different species occur than can be<br />

distinguished. Thus, the equivalent expression for the entropy of mixing<br />

should be written with the true concentrations. As eq. 24 refers to 1 mole<br />

monomers, the expression should be weighted by the compressibility factor<br />

representing the true number of moles. The new expression is<br />

For �ga we obtain<br />

and, analogously,<br />

Parameter<br />

Name/Element<br />

Symbol Default MDS Lower<br />

Limit<br />

(25)<br />

(26)<br />

(27)<br />

Upper<br />

Limit<br />

DMER/1 A i2 0 X – – –<br />

Units<br />

DMER/2 B i2 0 X – – TEMPERATURE<br />

TMER/1 A i4 0 X – – –<br />

TMER/2 B i4 0 X – – TEMPERATURE<br />

HMER/1 A i6 0 X – – –<br />

HMER/2 B i6 0 X – – TEMPERATURE<br />

References<br />

M. M. Abbott and H. C. van Ness, "Thermodynamics of Solutions Containing<br />

Reactive Species, a Guide to Fundamentals and Applications," Fluid Phase Eq.,<br />

Vol. 77, (1992) pp. 53–119.<br />

V. V. De Leeuw and S. Watanasiri, "Modeling Phase Equilibria and Enthalpies<br />

of the <strong>System</strong> Water and Hydrofluoric Acid Using an HF Equation-of-state in<br />

Conjunction with the Electrolyte NRTL Activity Coefficient Model," Paper<br />

Presented at the 13th European Seminar on Applied Thermodynamics, June<br />

9–12, Carry-le-Rouet, France, 1993.

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