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Aspen Physical Property System - Physical Property Models

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Specifically,<br />

The long range interaction term for the logarithm of the activity coefficient of<br />

component I is computed as the sum of the individual segment contributions.<br />

Activity coefficients given by Eq. 65 are already normalized for molecular<br />

components as well as for ionic components with the infinite-dilution aqueous<br />

solution reference state.<br />

References<br />

Pitzer, K.S., J.M. Simonson, "Thermodynamics of Multicomponent, Miscible,<br />

Ionic <strong>System</strong>s: Theory and Equations," J. Phys. Chem., 1986, 90, 3005-3009.<br />

2 Thermodynamic <strong>Property</strong> <strong>Models</strong> 127<br />

(62)<br />

(63)<br />

(64)<br />

(65)<br />

Robinson, R.A., Stokes, R.H., Electrolyte Solutions, 2nd revised edition,<br />

Dover, 1970.<br />

Rashig, A.A., Honig, B., "Reevaluation of the Born Model of Ion Hydration," J.<br />

Phys. Chem., 1985, 89, 5588.<br />

NRTL-SAC Flory-Huggins Term<br />

We use the Flory-Huggins term to describe the combinatorial term:<br />

(66)<br />

(67)<br />

where G ex,FH is the Flory-Huggins term for the excess Gibbs energy, �I is the<br />

segment fraction of component I, and rI is the number of all conceptual<br />

segments in component I:<br />

(68)<br />

(69)

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