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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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4.4 Measurement <strong>of</strong> solvent activity 211<br />

by Chen and Kreglewski, 356 and a hard-sphere pair-correlation function for the chain term as<br />

following the arguments <strong>of</strong> Wertheim. The Huang-Radosz-form <strong>of</strong> the SAFT-equation <strong>of</strong><br />

state without an association term reads: 355<br />

PV<br />

RT<br />

2<br />

4y −2y<br />

5y −2<br />

mDnm<br />

⎡ u<br />

= 1+<br />

r + ( 1−r)<br />

+ r<br />

3 m<br />

( y − ) ( y − )( y − )<br />

∑∑<br />

1<br />

1 2 1<br />

~<br />

n m ⎣kT V<br />

⎢<br />

⎤<br />

⎦<br />

⎥<br />

n<br />

[4.4.97]<br />

where:<br />

Dnm empirical coefficients from the attractive perturbation term<br />

k Boltzmann’s constant<br />

r chain segment number<br />

In comparison to the PHC equation <strong>of</strong> state, the new term between the Carnahan-Starling<br />

term and the double sum accounts for chain-bonding. The terms are proportional to the<br />

segment number,r,<strong>of</strong>thechain molecule. However, the hard-sphere volume, V0, is now a<br />

slight function <strong>of</strong> temperature which is calculated according to the result <strong>of</strong> Chen and<br />

Kreglewski: 356<br />

[ 1 012 ( 3 0 ) ]<br />

00<br />

V = V − . exp − u / kT<br />

[4.4.98]<br />

0<br />

3<br />

where:<br />

V 00<br />

hard-sphere volume at T=0K<br />

u0 well-depth <strong>of</strong> a square-well potential u/k = u0/k (1 + 10K/T) with 10K being an<br />

average for all chain molecules.<br />

The ratio u0/k or u/k is analogous to the characteristic parameter T* in the equations<br />

above. There are two additional volume and energy parameters if association is taken into<br />

account. In its essence, the SAFT equation <strong>of</strong> state needs three pure component parameters<br />

which have to be fitted to equilibrium data: V 00 ,u0/k and r. Fitting <strong>of</strong> the segment number<br />

looks somewhat curious to a polymer scientist, but it is simply a model parameter, like the<br />

c-parameter in the equations above, which is also proportional to r. One may note additionally<br />

that fitting to specific volume PVT-data leads to a characteristic ratio r/M (which is a<br />

specific r-value), as in the equations above, with a specific c-parameter. Several modifications<br />

and approximations within the SAFT-framework have been developed in the literature.<br />

Banaszak et al. 357-359 or Shukla and Chapman 360 extended the concept to copolymers.<br />

Adidharma and Radosz 361 provides an engineering form for such a copolymer SAFT approach.<br />

SAFT has successfully applied to correlate thermodynamic properties and phase<br />

behavior <strong>of</strong> pure liquid polymers and polymer solutions, including gas solubility and supercritical<br />

solutions by Radosz and coworkers 355,357-359,361-368 Sadowski et al. 369 applied SAFT to<br />

calculate solvent activities <strong>of</strong> polycarbonate solutions in various solvents and found that it<br />

may be necessary to refit the pure-component characteristic data <strong>of</strong> the polymer to some<br />

VLE-data <strong>of</strong> one binary polymer solution to calculate correct solvent activities, because<br />

otherwise demixing was calculated. Groß and Sadowski 370 developed a “Perturbed-Chain<br />

SAFT” equation <strong>of</strong> state to improve for the chain behavior within the reference term to get<br />

better calculation results for the PVT- and VLE-behavior <strong>of</strong> polymer systems. McHugh and<br />

coworkers applied SAFT extensively to calculate the phase behavior <strong>of</strong> polymers in supercritical<br />

fluids, a comprehensive summary is given in the review by Kirby and McHugh. 371<br />

They also state that characteristic SAFT parameters for polymers from PVT-data lead to

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