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Aspen Physical Property System - Physical Property Models

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to multicomponent systems. In this simple system, three different<br />

arrangements exist:<br />

In the case of a central solvent molecule with other solvent molecules,<br />

cations, and anions in its immediate neighborhood, the principle of local<br />

electroneutrality is followed: the surrounding cations and anions are such that<br />

the neighborhood of the solvent is electrically neutral. In the case of a central<br />

cation (anion) with solvent molecules and anions (cations) in its immediate<br />

neighborhood, the principle of like-ion repulsion is followed: no ions of like<br />

charge exist anywhere near each other, whereas opposite charged ions are<br />

very close to each other.<br />

The effective local mole fractions are related by the following expressions:<br />

(central solvent cells)<br />

(central cation cells)<br />

(central anion cells)<br />

102 2 Thermodynamic <strong>Property</strong> <strong>Models</strong><br />

(11)<br />

(12)<br />

(13)<br />

Using equation 11 through 13 and the notation introduced in equations 9 and<br />

10 above, expressions for the effective local mole fractions in terms of the<br />

overall mole fractions can be derived.<br />

i = c, a, or B<br />

(14)<br />

(15)<br />

(16)<br />

To obtain an expression for the excess Gibbs energy, let the residual Gibbs<br />

energies, per mole of cells of central cation, anion, or solvent, respectively, be<br />

, , and . These are then related to the<br />

effective local mole fractions:<br />

(17)<br />

(18)<br />

(19)

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