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By H.E.A. van den Akker (Editor), J.J. Derksen (Editor)
Characteristically, fluid blending and the similar multiphase contacting procedures have consistently been considered as an empirical know-how. Many elements of combining, dispersing and contacting have been regarding strength draw, yet realizing of the phenomena used to be constrained or qualitative on the such a lot.
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3. Nouri, J. M. and Whitelaw, J. H. 1990, Effect of Size and Confinement on the Flow Characteristics in Stirred Reactors, Proc. Fifth Int. Symposium on Application of Laser Techniques to Fluid Mechanics, Lisbon, Portugal, pp. 8. 4. Yianneskis, M. and Whitelaw, J. H. 1993, On the Structure of the Trailing Vortices around Rushton Turbine Blades, Trans. , vol. 17, Part A, pp. 543 - 550. 5. , Breuer, M. , 1999, Steady and Unsteady Computations of Turbulent Flows Induced by a 4/45 ~ Pitched-Blade Impeller, J.
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Therefore, it is important to gain more knowledge on how impellers distribute turbulence within the reactor. The trailing vortex system contains the highest values of turbulence kinetic energy [6, 7] and it is interesting to compare the turbulence values generated by the different types of impellers. In Figures 5 and 6 the distribution of turbulence kinetic energy is shown for profiles which cut through the trailing vortices. The dimensionless variable x/T indicates the distance from the middle of the impeller blade.