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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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發(fā)表于 2025-3-25 05:31:15 | 只看該作者
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發(fā)表于 2025-3-26 01:09:58 | 只看該作者
Springer Monographs in Mathematicsmple dynamical particle models [2, 3]. We have widely investigated Lagrangian particle models evolving in a turbulent environment which is described from an Eulerian point of view. In this abstract we shortly review the methods employed: the models for particle dynamics together with the numerical m
27#
發(fā)表于 2025-3-26 08:11:05 | 只看該作者
Springer Monographs in Mathematicsses. 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
28#
發(fā)表于 2025-3-26 08:58:50 | 只看該作者
The Basics of Processes and Modelsresult, during the condensation stage the droplet population becomes more and more homogeneous, while the growth slows down. On the one hand, this slowing process cannot lead to a precipitation in reasonable times; on the other hand, the explosive process ensured by collisions cannot occur, if all t
29#
發(fā)表于 2025-3-26 16:08:44 | 只看該作者
Girjesh Govil,Ramakrishna V. Hosurhe 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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發(fā)表于 2025-3-26 18:30:22 | 只看該作者
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