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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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344 <strong>George</strong> <strong>Wypych</strong><br />

Self-diffusion coefficient, 10 -8 cm 2 s -1<br />

surface appears dry (this stage ends when<br />

the surface is dry) and the diffusion rate becomes<br />

very low; in the third stage solvent<br />

diffuses from the cured film. This is a slow<br />

process during which diffusion rate drops to<br />

zero. These changes are shown in Figure<br />

7.1.8. The diffusion rate during drying decreases<br />

as the concentration <strong>of</strong> polymer<br />

(phenol resin) in varnish increases. Also,<br />

the time to reach the slope change point in<br />

diffusion/time relationship increases as the<br />

concentration <strong>of</strong> polymer increases. 8<br />

Two methods have been used to measure<br />

the diffusion coefficient <strong>of</strong> toluene in<br />

mixtures <strong>of</strong> polystyrenes having two different<br />

molecular weights: one was dynamic<br />

light scattering and the other, fluorescence<br />

recovery after bleaching. 10 The data show<br />

that the relationship between the diffusion<br />

coefficient and polymer concentration is not linear. The crossover point is shown in Figure<br />

7.1.9. Below a certain concentration <strong>of</strong> polymer, the diffusion rate drops rapidly according<br />

to different kinetics. This is in agreement with the above theory (see Figure 7.1.1 and explanations<br />

for equation [7.1.2]). The slope exponent in this study was -1.5 which is very close<br />

to the slope exponent predicted by the theory <strong>of</strong> reptation (-1.75).<br />

The above data show that theoretical predictions are accurate when modelling diffusion<br />

phenomena in both simple and complicated mixtures containing solvents.<br />

7.1.2 SWELLING<br />

Polymers differ from other solids because they may absorb large amounts <strong>of</strong> solvents<br />

without dissolving. They also undergo large deformations when relatively small forces are<br />

involved. 12 Swelling occurs in a heterogeneous two phase system a solvent surrounding a<br />

swollen body also called gel. Both phases are separated by the phase boundary permeable to<br />

solvent. 13<br />

The swelling process (or solvent diffusion into to the solid) occurs as long as the<br />

chemical potential <strong>of</strong> solvent is large. Swelling stops when the potentials are the same and<br />

this point is called the swelling equilibrium. Swelling equilibrium was first recognized by<br />

Frenkel 14 and the general theory <strong>of</strong> swelling was developed by Flory and Rehner. 15,16<br />

The general theory <strong>of</strong> swelling assumes that the free energy <strong>of</strong> mixing and the elastic<br />

free energy in a swollen network are additive. The chemical potential difference between<br />

gel and solvent is given by the equation:<br />

where:<br />

10<br />

1<br />

0.1 1<br />

Polymer concentration, g cm<br />

10<br />

-3<br />

Figure 7.1.9. Self-diffusion coefficient vs. polystyrene<br />

concentration. [Adapted, by permission, from<br />

L Meistermann, M Duval, B Tinland, Polym. Bull., 39,<br />

No.1, 101-8 (1997).]<br />

0<br />

0<br />

0<br />

( μ − μ ) = ( μ − μ ) + ( μ −μ<br />

)<br />

1 1<br />

μ 1<br />

0<br />

μ 1<br />

Light scattering<br />

Fluorescence recovery<br />

1 1<br />

mix 1 1 el [7.1.5]<br />

chemical potential <strong>of</strong> gel<br />

chemical potential <strong>of</strong> solvent

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