Predictions of the solubility of gases in glassy polymers based on the NELF model
β Scribed by Giulio C. Sarti; Ferruccio Doghieri
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 218 KB
- Volume
- 53
- Category
- Article
- ISSN
- 0009-2509
No coin nor oath required. For personal study only.
β¦ Synopsis
A reliable, predictive model for the solubility of gases and vapours in glassy polymers has been recently presented: it is based on the free energy expression for the polymer penetrant mixture as obtained from the lattice fluid theory and on the idea that the partial polymer density is an internal state variable for the system. When the polymer density for the sorption condition is known, the model can be used in a pure predictive way as the solubility is estimated on the basis of pure penetrant and pure polymer PVT properties. In this work the basic assumptions of the model and its development are discussed in detail. The pseudoequilibrium condition and the calculation of the penetrant solubility under pseudo-equilibrium conditions are clearly stated. In closure, several examples comparing model predictions and experimental results for the solubility in glassy polymers are presented. In all the cases considered, the comparison confirms the model capability to satisfactorily predict solubility data in nonequilibrium glassy polymers and supports the validity of the underlying physical model.
π SIMILAR VOLUMES
## Abstract The diffusion of gases through glassy polymers is studied and the effective diffusion coefficient __D__^eff^ is represented as the result of the superposition of two fundamental mechanisms, namely slipping and hopping. __D__^eff^ is calculated by a twoβpoint correlation method. Comparis
Sorption isotherms of glassy polymers are concave to the pressure axis, and the absolute sorption levels are almost an order of magnitude higher than that of rubbery polymers on the relatively low-pressure side. There are several models to interpret this behavior, and the dual sorption model is the