By G. Bärwolff, H. Wengle, H. Jeggle (auth.), S. Gavrilakis, L. Machiels, P. A. Monkewitz (eds.)
Advances in Turbulence VI provides an replace at the country of turbulence examine with a few bias in the direction of examine in Europe, because it represents a nearly whole number of the paper displays on the Sixth eu Turbulence Conference, subsidized by way of EUROMECH, ERCOFTAC and price, and held on the Swiss Federal Institute of expertise in Lausanne, July 2-5, 1996. the matter of transition, including the structural description of turbulence, and the scaling legislation of totally constructed turbulence have endured to obtain such a lot recognition through the examine neighborhood and lots more and plenty development has been made because the final eu Turbulence convention in 1994. the quantity is therefore geared in the direction of experts within the zone of movement turbulence who couldn't attend the convention, in addition to anyone who needs quick to evaluate the main lively present learn parts and the teams linked to them.
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Extra resources for Advances in Turbulence VI: Proceedings of the Sixth European Turbulence Conference, held in Lausanne, Switzerland, 2–5 July 1996
Box 38000 1030 BN Amsterdam The Netherlands 1. Motivation Baffled stirred tank reactors are frequently used in the (petro)chemical industry for mixing purposes and detailed information on the (time-dependent) flow patterns and turbulence statistics in such reactors is important for an optimal design. The flow in these systems is highly unsteady and in particular near the turbine, quasi-periodic fluid motion can be observed. Since large-eddy simulation (LES) is inherently a time-dependent technique, this unsteady and quasi-periodic behavior of the flow is accounted for in a natural way.
8]. The reaction chemistry in the layer is assumed to be governed by the irreversible reaction F + 0- > P, with the assumption of infinite rate chemistry. Equal diffusivities is assumed for the species and the passive scalar transported with this hypothesis is the Shvab-Zeldovich mixture fraction. The numerical resolution is 200x64x48 with a sub-grid domain containing 150 41 points. a). ration profiles across the layer are given figure (1. b). for different positions along the stream-wise axis, and are in good agreelllent with the experimental results.
00 Figure 2. 5. z / D = -1 corresponds with the solid wall at the bottom of the reactor, z/ D = 2 with the free surface at the top. All velocities are scaled with the tip velocity of the turbine. M. A. (1995) Numerical simulation of free convective flow using the lattice-Boltzmann scheme J. Heat and Fluid Flow 16, pp. 357-364. M. (1996) Direct and large-eddy simulation of turbulent fluid flow using the lattice-Boltzmann scheme. To appear in J. Heat and Fluid Flow. Smagorinsky, J. (1963) General circulation experiments with the primitive equations: 1.