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Titlebook: Direct and Large-Eddy Simulation III; Proceedings of the I Peter R. Voke,Neil D. Sandham,Leonhard Kleiser Conference proceedings 1999 Sprin

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https://doi.org/10.1007/978-3-319-42928-1nt plumes compare well with the experimental results of Cetegen et. al. for different Froude numbers and density ratios. Comparisons have also been carried out between the results of a DNS and the present LES and good agreement has been reached. Some statistical quantities and different terms in the vorticity equation are analyzed.
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X-Ray Absorption Spectroscopy (XAS) the dissipation. As the eddies are regenerated, however, the secondary Reynolds stress 〈v′w′〉 becomes significant, the production increases again, and the flow reaches a quasi-equilibrium collateral state, characterized by higher turbulent kinetic energy and Reynolds stresses.
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Springer Handbook of Lasers and Opticsat the model, mixed or not, transforms appropriately when differing frames of reference are considered. Modifications to the model are suggested for the case in which the unfiltered field(s) has discontinuities.
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Large-Eddy Simulation of a Three-Dimensional Shear-Driven Turbulent Boundary Layer, the dissipation. As the eddies are regenerated, however, the secondary Reynolds stress 〈v′w′〉 becomes significant, the production increases again, and the flow reaches a quasi-equilibrium collateral state, characterized by higher turbulent kinetic energy and Reynolds stresses.
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A Tensor-Diffusivity Subgrid Model for Large-Eddy Simulation,at the model, mixed or not, transforms appropriately when differing frames of reference are considered. Modifications to the model are suggested for the case in which the unfiltered field(s) has discontinuities.
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1382-4309 utcome of which was the definition and agreement of the 1999 Newton Institute Research Programme on Turbulence. The main aim of the- month programme, held at the institute in Cambridge, was to bring together the mathematics and engineering communities involved in the turbulence area to address the m
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X-Ray Absorption Spectroscopy (XAS)Reynolds number to another. But our understanding of the turbulent mechanisms and interactions between the coherent structure in the boundary layer and the small scales is not clear yet. Our work lies within this scope.
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Reference work Apr 20071st editionct simulation and experimental results in two flows, a plane channel flow at ..= 395, and the turbulent flow over a two-dimensional wavy wall, were carried out. The LES results compare well with numerical and experimental data.
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