4.5 Article

Mechanism of mass transfer from bubbles in dispersions - Part II: Mass transfer coefficients in stirred gas-liquid reactor and bubble column

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ELSEVIER SCIENCE SA
DOI: 10.1016/j.cep.2004.05.009

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gas-liquid contactor; bubble column; agitated vessel; mass transfer coefficient; viscosity; surfactants

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Experimental data on the average mass transfer liquid film coefficient (k(L)) in an aerated tank stirred by Rushton turbine and in bubble column are presented. Liquid media were used as 0.8M sodium sulphite solution, pure or with the addition of Sokrat 44 (copolymer of acrylonitrile and acrylic acid) or short-fiber carboxymethylcellulose (CMC) for the Newtonian and long-fiber CMC for the non-Newtonian viscosity enhancement and ocenol (cis-9-octadecen-1-ol) or polyethylenglycol (PEG) 1000 for surface tension change. Volumetric mass transfer coefficient (k(L)a) and specific interfacial area (a) were measured by the Danckwerts' plot method. Coefficients kL measured by pure oxygen absorption in pure sulphite solution and Newtonian viscous liquids are well fitted by the eddy model in the form of k(L) = 0.448 (ev/p)(0.25) (D/v)(0.5) with a mean deviation of 20%. Surface-active agents (ocenol and PEG) and non-Newtonian additive (long-fiber CMC) reduced k(L) value significantly but their effect was not described satisfactorily neither by surface tension nor by surface pressure. It is shown that the decisive quantity to correlate k(L) in the stirred tank and bubble column is power dissipated in the liquid phase rather than the bubble diameter and the slip velocity. Absorption of air did not yield correct kL data, which did not depend on or slightly decreased with increasing power. This is due to the application of an improper gas phase mixing model for absorption data evaluation. (C) 2004 Elsevier B.V. All rights reserved.

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