Chapter 3. Laminar Mixing: A Dynamical Systems Approach

  1. Edward L. Paul4,
  2. Victor A. Atiemo-Obeng5,
  3. Suzanne M. Kresta6
  1. Edit S. Szalai1,
  2. Mario M. Alvarez2,
  3. Fernando J. Muzzio3

Published Online: 30 JAN 2004

DOI: 10.1002/0471451452.ch3

Handbook of Industrial Mixing: Science and Practice

Handbook of Industrial Mixing: Science and Practice

How to Cite

Szalai, E. S., Alvarez, M. M. and Muzzio, F. J. (2004) Laminar Mixing: A Dynamical Systems Approach, in Handbook of Industrial Mixing: Science and Practice (eds E. L. Paul, V. A. Atiemo-Obeng and S. M. Kresta), John Wiley & Sons, Inc., Hoboken, NJ, USA. doi: 10.1002/0471451452.ch3

Editor Information

  1. 4

    Merck & Co., Inc. (retired); 308 Brooklyn Boulevard, Sea Girt, NJ 08750, USA

  2. 5

    The Dow Chemical Company, Building 1776, Midland, MI 48674, USA

  3. 6

    Department of Chemical and Materials Engineering, University of Alberta, Edmonton, AB, Canada T6G 2G6

Author Information

  1. 1

    Schering-Plough Research Institute, 200 Galloping Hill Road, Mailstop F31A, Kenilworth, NJ 07033, USA

  2. 2

    Department of Biochemical Engineering, Ave. Eugenio Garza Sada 2501 Sur, C. P. 64849, Monterrey, N.L. Mexico, USA

  3. 3

    Department of Chemical and Biological Engineering, Rutgers University, 98 Brett Road, Piscataway, NJ 08854-3058, USA

Publication History

  1. Published Online: 30 JAN 2004
  2. Published Print: 14 NOV 2003

ISBN Information

Print ISBN: 9780471269199

Online ISBN: 9780471451457

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Keywords:

  • laminar mixing;
  • chaos;
  • stretching;
  • striation thickness;
  • measures of mixing;
  • coefficient of variation

Summary

The only efficient route to good mixing in laminar flows is by chaos. The dynamics of chaotic mixing processes is examined in this chapter using two examples: a simple 2D model, the sine flow, and a practical industrial mixer, the Kenics static mixer. Chaotic motion creates complex and intricate mixing structures, but after sufficient time a universal and predictable length scale distribution emerges in all these flows. The basic mechanism that controls mixing in the simple 2D model and the 3D device is identical and common to all laminar chaotic flows. The continuous repetition of two simple actions, stretching and folding, creates robust and complex mixing structures that have self-similar statistical properties. A collection of scaling relationships can be developed from the self-similarity concepts for predicting and optimizing mixing performance in these flows. Moreover, since stretching controls the location and density of the intermaterial area between mixture components, it has a direct impact on the evolution of reactions. The location of the reactive zones is practically identical to the mixing structure determined only by the chaotic stretching process.