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 study with a few bias in the direction of examine in Europe, because it represents a nearly whole choice of the paper shows on the Sixth eu Turbulence Conference, backed via 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 absolutely built turbulence have endured to obtain so much recognition by way of the examine group and masses development has been made because the final ecu Turbulence convention in 1994. the amount is hence geared in the direction of experts within the quarter of move turbulence who couldn't attend the convention, in addition to anyone who needs quick to evaluate the main lively present examine parts and the teams linked to them.
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Additional info for Advances in Turbulence VI: Proceedings of the Sixth European Turbulence Conference, held in Lausanne, Switzerland, 2–5 July 1996
N (10- 2 s-I) D" (m 2 s- l ) Du (m 2 s- l to;; ) 600 s D,. 1l:.! () 1 3. Investigation of situations with mean-flow shear Secondly, the influence of mean wind shear is investigated. 001 s- L. 005 s-1 to verify whether our findings for the cases above remaill valid for the case of an atmosphere that is only weakly stable. )). ) 18 It is found that under these typical conditions the diffusion coefficients are hardly influenced by shear. This is not surprising because the bulk Richardson numbers of the flows are high.
This smoothing process is not necessarily strict in the sense that the the filter has a sharp "cut-off" frequency. Rather, the filter has to be positive in the real-space, in order to be realizable, Yerman et al. (1994). Consider a spatial filter kernel G( x - x') applied to a function q( x; t), resulting in a "smooth" function q(x, t; ,6,): q(x, t;,6,) = JG(x - x/;,6,) q(X/, t) dx' 23 S. Gavrilakis et al. ), Advances in Turbulence VI, 23-26. © 1996 Kluwer Academic Publishers. (1) 24 The choice of the filter may be more or less arbitrary, unless one wants to utilise the properties of the chosen filter.
A. (1995) Laser-Doppler measurements in a baffled stirred tank reactor with a disc turbine. D. thesis, Delft University of Technology, the Netherlands. 8 inC n mu ~. --.. 0 t ~ ~ ~ \\. ,-. -. 30 O. IS /,~ Q. -... ---=- . I - """'\ + "\ + + ·0. 10 ·O. 00 ~ ~ ... 25 ~= ~ [! 50 vo -- ... 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.