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Aspen Physical Property System - Physical Property Models

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<strong>Aspen</strong> Plus and <strong>Aspen</strong> Properties. �Hi and �Gi are the new contributions from<br />

the symmetric reference state.<br />

The unsymmetric enthalpy for an ionic component is calculated from<br />

the infinite dilution aqueous phase heat capacity as follows:<br />

170 2 Thermodynamic <strong>Property</strong> <strong>Models</strong><br />

(124)<br />

where T ref = 298.15K. By default, is calculated from the aqueous<br />

infinite dilution heat capacity polynomial. If the polynomial model parameters<br />

are not available, is calculated from the Criss-Cobble correlation.<br />

The unsymmetric Gibbs free energy for an ionic component is<br />

calculated from the infinite dilution aqueous phase heat capacity as<br />

follows:<br />

(125)<br />

(126)<br />

where the term RT ln (1000/Mw) is added because and<br />

are based on a molality scale, and is based on a mole fraction scale.<br />

�Hi and �Gi for the symmetric reference state<br />

The reference state for ionic components in the symmetric electrolyte NRTL<br />

model is the pure fused salts containing these ions, so the enthalpy or Gibbs<br />

free energy of the ionic components at the symmetric reference state is the<br />

enthalpy contributions or the Gibbs free energy contributions of these ions to<br />

the system of the pure fused salts. The condition of the pure fused salts can<br />

be defined as follows:<br />

which applies to all molecular components in the solution.<br />

(127)<br />

Given that the calculated total enthalpy or total Gibbs free energy of an<br />

electrolyte solution by any reference state should be the same, the<br />

formulation of enthalpy or Gibbs free energy of the ionic components at the<br />

symmetric reference state can be derived from the unsymmetric electrolyte<br />

NRTL enthalpy or Gibbs free energy calculations at the condition that all<br />

molecular components (solvents and Henry components) approach zero, i.e.

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