Scaling up bubble column reactors with the aid of CFD

Krishna, R. ; Van Baten, J. M. (2001) Scaling up bubble column reactors with the aid of CFD Chemical Engineering Research and Design, 79 (3). pp. 283-309. ISSN 0263-8762

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Official URL: http://www.sciencedirect.com/science/article/pii/S...

Related URL: http://dx.doi.org/10.1205/026387601750281815

Abstract

Bubble column reactors, used widely in industry, often have large column diameters (up to 6 m) and are operated at high superficial gas velocities (in the range of 0.1 to 0.4 ms−1) in the churn-turbulent flow regime. Experimental work on bubble column hydrodynamics is usually carried out on a scale smaller than 0.3 m, at superficial gas velocities lower than 0.25 ms−1. The extrapolation of data obtained in such laboratory scale units to the commercial scale reactors requires a systematic approach based on the understanding of the scaling principles of bubble dynamics and of the behaviour of two-phase dispersions in large scale columns. We discuss a multi-tiered approach to bubble column reactor scale up, relying on a combination of experiments, backed by Computational Fluid Dynamics (CFD) simulations for physical understanding. This approach consists of the following steps: (a) description of single bubble morphology and rise dynamics (in this case both experiments and Volume-of-Fluid (VOF) simulations are used); (b) modelling of bubble-bubble interactions, with experiments and VOF simulations as aids; (c) description of behaviour of bubble swarms and the development of the proper interfacial momentum exchange relations between the bubbles and the liquid; and (d) CFD simulations in the Eulerian framework for extrapolation of laboratory scale information to large-scale commercial reactors.

Item Type:Article
Source:Copyright of this article belongs to Institution of Chemical Engineers.
Keywords:Bubble Columns; Flow Regimes; Scale up Strategy; Hold-up; Bubble Rise; Bubble Interactions; CFD
ID Code:65470
Deposited On:17 Oct 2011 03:11
Last Modified:17 Oct 2011 03:11

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