Titlebook: IUTAM Symposium on Variable Density Low-Speed Turbulent Flows; Proceedings of the I Louis Fulachier,John L. Lumley,Fabien Anselmet Conferen

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Direct Simulation of Multiphase Flows with Density Variationsnstability of a sheared liquid-gas interface. The two-dimensional simulations of the Navier-Stokes equation with surface tension show the formation of liquid sheets at sufficiently high Weber and Reynolds numbers. The three-dimensional simulations show two scenarios, depending on the degree of three

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Self-Turbulent Flame Simulation by a Cellular Automatonlular automata [2,3]. The automaton consists of individual particles moving in a two-dimensional square lattice. Two binary variables (accounting for temperature and fuel concentration) are associated to each individual particle. Thus, a normalized temperature equal to one is assigned to every hot p

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Some Problems on Single Point Modeling of Turbulent, Low-Speed, Variable Density Fluid Motionsmmonly quoted is probably aeronautics, where . flows are present in various applications, such as high speed aircraft and supersonic combustion ramjet engines for instance. However, as far as general industrial fluid applications are concerned, . are part of chemical engineering, energetics, science

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Second Order Modelling of Variable Density Jets: Favre Averaged Closures Versus Reynolds Averaged Clof density variations on the turbulence field can lead to complex behaviours and many of the underlying mechanisms are still incompletely understood. Several fundamental studies were published in the recent years literature (Chassaing et al., Fulachier et al., Panchakapesan and Lumley). The main pur

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Averaging Procedures for the Large Eddy Simulation of Variable Density Flowsighted averaging procedure. In this paper this procedure is extended to Large Eddy Simulations in terms of the operatorial multi level formulation proposed recently by the author (Germano, 1992). This formulation does not introduce explicitly the fluctuations, and in the paper two particular points

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