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Applied Mathematics Colloquium


Friday, December 1, 2006, 11:30 am
Cullimore Lecture Hall II
New Jersey Institute of Technology

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Turbulent Mixing in Real (Non-Ideal) Fluids




James Glimm

Department of Applied Mathematics and Statistics

Stony Brook University and Brookhaven National Laboratory

Stony Brook, NY






Abstract


    Turbulent mixing is an important but difficult problem in fluid dynamics. We consider the mixing zone generated by the acceleration of a fluid interface between two fluids of different densities. The case of steady acceleration is called the Rayleigh-Taylor instability, and it gives rise to a mixing zone of the two fluids, growing in thckness as time increases. The mixing rate, experimentally, shows a universal growth rate, as multiple of t2, but simulations in most cases disagree with experiments by a factor of 2 or more. We report on a new class of simulations (based on (a) an improved front tracking algorithm and on (b) inclusion of real fluid effects) which agree with experiment. Here the real fluid effect is surface tension for immiscible fluids and mass diffusion, initial (t = 0) mass diffusion, or viscosity for miscible fluids. We document significant dependence of the mixing rate on both physical effects (e.g. surface tension) and on numerical artifacts such as mass diffusion (for untracked simulations). We conclude that modeling of turbulent mixing is sensitive to details of transport, surface tension, and to their numerical analogues. The full dependence of the mixing rates on these physical phenoma and their numerical analogues is only partially understood.
    When we consider the averaged equations, which remove all of the microphysical complexity of the mixing process and replace it with mean or averaged flow properties, serious difficulties emerge in the problem of closure, or the proper definition of the new nonlinear terms arising from the averaging process to define the closed equations. The averaged equations are never in conservation form, and for this reason the proper meaning of the nonlinear terms and their discretization and regularization is still a research issue. The numerical data base resulting from experimentally validated simulations becomes invaluable in providing a rational and systematic way to evaluate proposed closures. We find excellent agreement between the direct average of the simulated data and closures we have proposed. We also find a fair degree of insensitivity in comparing the data to other closures.
    It is a pleasure to thank the many colleagues and collaborators who have contributed to the work presented here.
    Finally, we discuss briefly plans at Stony Brook and Brookhaven National Laboratory for computational science.