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Titlebook: Advances in Turbulence XII; Proceedings of the 1 Bruno Eckhardt Conference proceedings 20091st edition Springer-Verlag Berlin Heidelberg 20

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楼主: DUBIT
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Pavel G. Khalatur,Alexei R. Khokhlov. For instance, existing numerical studies are limited within frameworks of a semi-realistic model [3] or of a tilted geometry with a minimal domain [4]. However, owing to the recent development of computers, DNS of the subcritical CF is now possible to be performed.
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https://doi.org/10.1007/11570325an be used to predict directly from the fundamental equations physical quantities such as bulk flow rate and mean wall drag. All results and the code that generates them are disseminated through through our group‘s open-source CFD software and solution database Channelflow.org and the collaborative
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Lagrangian analysis of turbulent convectionses. We apply a pseudospectral method for the Cartesian case and a second-order finite difference method for the cylindrical one. The Prandtl number is . = 0.7 for all cases. The Rayleigh numbers . vary between 10. and 10.. Figure 1 shows a snapshot of the temperature field in the Cartesian cell. Cl
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Flow reversals in a vertical channelhe bottom one is hot. The section of the cell is 40 × 10 cm. and its height is 40 cm. The thickness of the walls, made with PMMA, is 2 cm. Furthermore, two honeycomb structures allow to prevent convection from appearing in about 50% of the cell and, as we can see on Fig. 1, between these structures,
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DNS of turbulent plane Couette flow with emphasis on turbulent stripe. For instance, existing numerical studies are limited within frameworks of a semi-realistic model [3] or of a tilted geometry with a minimal domain [4]. However, owing to the recent development of computers, DNS of the subcritical CF is now possible to be performed.
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