The intermediate stage of the dead-end filtration process

Citation
Ma. Koenders et al., The intermediate stage of the dead-end filtration process, CHEM ENG SC, 55(18), 2000, pp. 3715-3728
Citations number
23
Categorie Soggetti
Chemical Engineering
Journal title
CHEMICAL ENGINEERING SCIENCE
ISSN journal
00092509 → ACNP
Volume
55
Issue
18
Year of publication
2000
Pages
3715 - 3728
Database
ISI
SICI code
0009-2509(200009)55:18<3715:TISOTD>2.0.ZU;2-0
Abstract
The volume-time curves in a dead-end filtration experiment can be approxima ted - in the intermediate stage - by a power law. The exponent of this law shows a marked dependence on the zeta potential and falls to nearly 0.5 in the vicinity of the isoelectric point. Two limiting cases have been investi gated: (1) high zeta potential where the particles have a strong interactio n and (2) zero zeta potential where the particles behave as a dense gas. Fo r (1) the forming cake can be assigned a stiffness and by solving a system of Blot equations the exponent of the volume-time curve is obtained; the va lue of the exponent must always be greater than 0.5. For (2) the 'granular temperature' theory by McTigue and Jenkins (1992, Channel flow of a concent rated suspension. In H. H. Shen et al., Advances in macromechanics of granu lar materials (pp. 381-390), Amsterdam: Elsevier) is made appropriate to th e geometry and the exponent of the volume-time curve is found to be exactly 0.5. The two limiting cases are associated with distinctly different cake formation processes: for (1) a smooth solidosity curve is found while for(2 ) the cake formation can be approximated by a solidosity step function (the 'two-solidosity' model). In all modelling in this paper the septum permeab ility is non-negligible, but a function of the solidosity of the filter cak e at the septum. (C) 2000 Elsevier Science Ltd. All rights reserved.