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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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186 Christian Wohlfarth<br />

ν 2,spez<br />

∞<br />

specific volume <strong>of</strong> the polymer (more exact, ν2,spez, the partial specific volume at<br />

infinite dilution)<br />

According to the scattering theory <strong>of</strong> polydisperse polymers, please see, for example,<br />

in the book written by Strobl, 147 the molar mass <strong>of</strong> the polymer, M 2, is equal to the mass average,<br />

M w, <strong>of</strong> polydisperse polymers. The contrast factor for neutron scattering takes into<br />

account for the difference in scattering power <strong>of</strong> solvent molecules and polymer segments.<br />

Again, Zimm plots can be constructed, as was explained above, for light scattering measurements<br />

to take into account for angular and concentration dependence - for a demonstration<br />

see Vennemann et al. 173<br />

The transformation <strong>of</strong> the obtained second virial coefficients into solvent activities is<br />

as explained above, Equations [4.4.34 and 4.4.35]. A recent example for the determination<br />

<strong>of</strong> second virial coefficients from SANS is the investigation <strong>of</strong> aggregation phenomenon in<br />

associating polymer solutions by Pedley et al., 174 where sodium sulfonated polystyrene<br />

ionomers in deuterated xylene were considered. Enthalpic and entropic contributions to A 2<br />

were calculated (as in the paper by Wolf and Adams 149 for A 2 from light scattering) and an<br />

enthalpy <strong>of</strong> aggregation was estimated from these data. A high-pressure investigation on<br />

aqueous poly(ethylene oxide) solutions was made by Vennemann et al. 173 who measured<br />

second virial coefficients by a SANS experiment for pressures up to 200 MPa and combined<br />

these data with PVT-measurements to obtain also excess and partial excess volumes and<br />

gained information about the pressure dependence <strong>of</strong> the chemical potential.<br />

4.4.3.2.5 Ultracentrifuge<br />

The analytical ultracentrifuge is a powerful tool for polymer characterization. Technical details<br />

<strong>of</strong> ultracentrifugation will not be considered here - please see Refs. 26,35-37 for more information.<br />

In a typical ultracentrifuge experiment, the polymer solution is put in a sample<br />

tube and rotated at high speed. Thermodynamic data can be obtained either from the sedimentation<br />

velocity (sedimentation coefficient) or from the sedimentation-diffusion equilibrium<br />

since the centrifugal forces are balanced by the activity gradient. The concentration<br />

gradient is conventionally measured via the refractive index gradient along the axis <strong>of</strong> the<br />

tube using Schlieren photography or various optics.<br />

The sedimentation coefficient is defined as the sedimentation velocity in a unit force<br />

field:<br />

dh / dt<br />

s =<br />

ω h<br />

2<br />

[4.4.51]<br />

where:<br />

s sedimentation coefficient<br />

h distance from the center <strong>of</strong> rotation<br />

t time<br />

ω angular velocity<br />

For a given polymer-solvent system, the sedimentation coefficient is dependent on<br />

temperature, pressure and polymer concentration. For obtaining thermodynamic data from<br />

sedimentation coefficients, one additionally has to measure the diffusion coefficient. This<br />

can be made with an ultracentrifuge in special diffusion cells 35 or with dynamic light<br />

scattering 32 based on the theory <strong>of</strong> Pecora. 175 Nearly all diffusion coefficients have been<br />

measured by this method since it became available in 1970. The determination <strong>of</strong> sedimen-

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