The intermediate stage of the dead-end filtration process
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Koenders, MA
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Kingston Univ, Mat Res Grp, Dept Chem Engn, Kingston upon Thames KT1 2EE, Surrey, EnglandKingston Univ, Mat Res Grp, Dept Chem Engn, Kingston upon Thames KT1 2EE, Surrey, England
Koenders, MA
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Reymann, S
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机构:Kingston Univ, Mat Res Grp, Dept Chem Engn, Kingston upon Thames KT1 2EE, Surrey, England
Reymann, S
Wakeman, RJ
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机构:Kingston Univ, Mat Res Grp, Dept Chem Engn, Kingston upon Thames KT1 2EE, Surrey, England
Wakeman, RJ
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[1] Kingston Univ, Mat Res Grp, Dept Chem Engn, Kingston upon Thames KT1 2EE, Surrey, England
The volume-time curves in a dead-end filtration experiment can be approximated - 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 investigated: (1) high zeta potential where the particles have a strong interaction and (2) zero zeta potential where the particles behave as a dense gas. For (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 value 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 concentrated suspension. In H. H. Shen et al., Advances in macromechanics of granular materials (pp. 381-390), Amsterdam: Elsevier) is made appropriate to the 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 permeability is non-negligible, but a function of the solidosity of the filter cake at the septum. (C) 2000 Elsevier Science Ltd. All rights reserved.