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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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4.4 Measurement <strong>of</strong> solvent activity 185<br />

A2,A3, ... second, third, ... osmotic virial coefficients<br />

M2 molar mass <strong>of</strong> the polymer<br />

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

the book written by Strobl), 147 the molar mass <strong>of</strong> the polymer, M2, is equal to the mass average,<br />

Mw, <strong>of</strong> polydisperse polymers. The exact application <strong>of</strong> Equation [4.4.47] is to be made<br />

again at the scattering angle θ = 0. The constant K is now given by:<br />

( Av )<br />

4 2 2 4<br />

K ≡ e Δ z / m N c<br />

[4.4.48]<br />

where:<br />

e electron charge<br />

m electron mass<br />

Δz excess number <strong>of</strong> electrons<br />

c speed <strong>of</strong> light in vacuum<br />

In principle, there is agreement between values <strong>of</strong> second virial coefficients from light<br />

scattering or X-ray scattering. Okano et al. 167,168 applied SAXS to semidilute solutions <strong>of</strong><br />

polystyrene in cyclohexane in the poor solvent regime and obtained virial coefficients in<br />

good agreement with liquid-liquid data from a coexistence curve. Takada et al. 169 provided a<br />

more recent example for poly(vinyl methyl ether) in cyclohexane, Horkay et al. 170 for<br />

poly(vinyl acetate) in toluene and poly(dimethyl siloxane) in octane. In comparison to data<br />

from osmotic pressure and neutron scattering, they observed good agreement.<br />

4.4.3.2.4 Neutron scattering<br />

Neutron scattering is an important method for investigating conformation and dynamics <strong>of</strong><br />

polymer molecules, Higgins, 171 or polymer mixtures, Hammouda. 172 A recent presentation<br />

<strong>of</strong> various techniques can be found in a new book edited by Pethrick and Dawkins. 26 Thermodynamics<br />

<strong>of</strong> polymer solutions is not the first task in neutron scattering experiments. The<br />

general set-up <strong>of</strong> the neutron scattering experiment is equivalent to the one used for light<br />

scattering, but applying a neutron source, and elastic neutron scattering at small angles<br />

(SANS) can be applied like light scattering or X-ray scattering to obtain second virial coefficients<br />

in dilute solutions. Similarly to the scattering <strong>of</strong> photons, it is the difference in scattering<br />

power between solvent molecules and polymer segments which determines the<br />

absolute scattering intensity. Formally, the virial equation has the same form as Equations<br />

[4.4.43 and 47], again neglecting P(θ):<br />

and<br />

where:<br />

( ) / ( ) ( / )<br />

2<br />

Kc Σ θ = 1 M + 2Ac+ 3Ac+�<br />

[4.4.49]<br />

2 2 2 2 3 2<br />

( 2 1 1 2 )<br />

K = b −b<br />

ρν , / N<br />

[4.4.50]<br />

spez Av<br />

c2 mass by volume concentration c2 =m2/ν A2,A3, ... second, third, ... osmotic virial coefficients<br />

M2 molar mass <strong>of</strong> the polymer<br />

Σ( θ) differential scattering cross section per volume unit<br />

K contrast factor for neutron scattering<br />

b1,b2 densities <strong>of</strong> solvent and polymer scattering length<br />

density <strong>of</strong> the solvent<br />

ρ 1

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