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n - PATh :.: Process and Product Applied Thermodynamics research ...

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Modeling<br />

Figure III.10 compares experimental results with the predictions given by the PR-<br />

EOS using the average binary interaction parameter kij given in Table III.4. It can be<br />

observed that a temperature independent kij cannot describe the oxygen solubility in<br />

perfluoroalkanes. The average absolute deviation given in Table III.4 decreases from the<br />

O2-C6F14 to the O2-C9F20 systems because the temperature dependence of the solubility<br />

decreases along the perfluorocarbon series. The Peng-Robinson EoS, with one adjusted<br />

interaction binary parameter, has limited predictive capability providing only a qualitative<br />

description of the temperature dependence of the oxygen solubility in linear saturated<br />

perfluoroalkanes.<br />

2. Regular Solution Theory<br />

According to the definition of Hildebr<strong>and</strong> <strong>and</strong> Scott (1970) a regular solution is one<br />

involving no entropy <strong>and</strong> no volume change when a small amount of one of its components<br />

is transferred to it. Considering this assumption, the following equation can be deduced in<br />

order to describe the solubility of a non-polar gas in a non-polar solvent:<br />

−<br />

x<br />

2<br />

log 2 = −log<br />

2 + δ 1 − δ 2<br />

(<br />

i 0.<br />

4343V<br />

2<br />

x<br />

) (III.41)<br />

RT<br />

where x2 is the mole fraction gas solubility, x i 2 is the ideal gas solubility, V 2 is the partial<br />

molar volume of the gas in the solution <strong>and</strong> δ1 <strong>and</strong> δ2 are the solubility parameters for the<br />

solvent <strong>and</strong> the solute, respectively.<br />

When the entropic contribution is significant, the Regular Solution Theory alone<br />

cannot describe correctly the solubility of a solute in a solvent. The entropic contribution<br />

can be accounted for, if the Flory-Huggins combinatorial term is introduced:<br />

−<br />

i V ⎛ V<br />

⎜ −<br />

⎞<br />

⎟<br />

0.<br />

4343V<br />

2 ) (III.42)<br />

⎝ ⎠<br />

2<br />

2<br />

2<br />

log x2<br />

= −log<br />

x 2 + log + 0.<br />

4343⎜1<br />

⎟ + δ 1 − δ 2<br />

V1<br />

V1<br />

RT<br />

where V1 is the molar volume of the solvent.<br />

Equation III.42 requires three parameters for the solute ( x 2 , V2<br />

, δ 2<br />

i<br />

) <strong>and</strong> two<br />

parameters for the solvent (V1 <strong>and</strong> δ1). All these parameters are temperature dependent, but<br />

- 125 -<br />

(

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