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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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4.4 Measurement <strong>of</strong> solvent activity 189<br />

solid-liquid coexistence data <strong>of</strong> benzene in natural rubber and found good agreement to<br />

other data.<br />

Equation [4.4.55] could in principle also be used for the determination <strong>of</strong> thermodynamic<br />

data from the melting point depression <strong>of</strong> (semi)crystalline polymers when the subscripts<br />

changed from 1 to 2. This enables a second approach to data for the infinite dilution<br />

range <strong>of</strong> the solvent in the polymer. Such investigations have been made in the literature.<br />

However, these data are regarded as being less reliable by a number <strong>of</strong> reasons and no further<br />

discussion will be made here.<br />

4.4.3.2.7 Liquid-liquid equilibrium (LLE)<br />

There are two different situations for the liquid-liquid equilibrium in polymer-solvent systems:<br />

(i) the equilibrium between a dilute polymer solution (sol) and a polymer-rich<br />

solution (gel) and<br />

(ii) the equilibrium between the pure solvent and a swollen polymer network<br />

(gel).<br />

Case (i) is considered now, case (ii) is specially considered below as swelling equilibrium.<br />

LLE-measurements do not provide a direct result with respect to solvent activities.<br />

Equation (4.4.8) says that solvent activities at given temperature and pressure must be equal<br />

in both coexisting phases. Since the solvent activity <strong>of</strong> such a coexisting phase is a priori not<br />

known, one has to apply thermodynamic models to fit LLE-data as functions <strong>of</strong> temperature<br />

and concentration. Solvent activities can be obtained from the model in a subsequent step<br />

only.<br />

Figure 4.4.19. Principles <strong>of</strong> liquid-liquid demixing in polymer solutions, a) - strictly binary polymer solution <strong>of</strong> a<br />

monodisperse polymer, b) - quasi-binary polymer solution <strong>of</strong> a polydisperse polymer which is characterized by a<br />

distribution function: C - critical point, dashed lines - tie lines, T(1) - temperature/concentration in the homogeneous<br />

region, T(2) - temperature/concentrations <strong>of</strong> the cloud point (phase´) and the corresponding shadow point<br />

(phase´´), T(3) - temperature in the heterogeneous LLE region, coexistence concentrations <strong>of</strong> phase´ and phase´´ at<br />

T(3) are related to the starting concentration = cloud point concentration <strong>of</strong> (2).

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