## A complete theory of diffusion of absorbing gases in porous solids is developed. Both ordinary and thermal diffusion are considered. The thermodynamics of irreversible processes is used to derive the general flur equations. A new rheoretical model of surface diffusion is presented. Moreover, th
The diffusion of moisture in sorbent solids part II. activated alumina
β Scribed by Stanley H. Jury; Mark A. Pollock; Eul K. Kim
- Publisher
- Elsevier Science
- Year
- 1977
- Tongue
- English
- Weight
- 713 KB
- Volume
- 303
- Category
- Article
- ISSN
- 0016-0032
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β¦ Synopsis
Ordinary and thermal diffusion of moisture in activated alumina are investigated using a new diffusion cell design and scheme of analysis reported earlier. The specific form of the mass flux equation has a pronounced effect on the magnitude of the associated thermal diffusion ratio. In the case of activated alumina-moist air, if a partial pressure gradient is used, then the thermal diffusion term is small if not zero. Free, Knudsen and surface diffusion all play a part in the diffusion through activated alumina. However, surface diffusion makes the major contribution and for this reason the model in this case can be simplified to a two parameter surface model. The activation energy for surface diffusion is constant and is approximately equal fo the mean isosteric heat of adsorption. In addition, mean pore radius, tortuosity, and other physical constants are computed from the least square fit of experimental data. Furthermore, the model is theoretically consistent over the entire concetration range (OS C, 5 C4,).
A new fact about activated alumina (Grade Fl) it that it does not transfer moisture in a nonisothermal condition so long as the partial pressures of moisture on the two sides of the pellet are the same. There appears to be no previous report of this fact in the periodical literature.
(1) HIGH/LOW: Diffusion from HIGH humidity (PA = 16.5 mmHg) supply air to LOW humidity (PA = 0.002 mmHg) supply air.
π SIMILAR VOLUMES
When dlffuslon mslde the sohd particles which are dried m a fluldlsed bed can not be neglected this Internal ddTuslon can be accounted for by two mechanisms (a) the long term response which describes the gradual build up of a concentrahon profile inside the solid particles as function of the total d