Journal
PHYSICS OF FLUIDS
Volume 16, Issue 5, Pages 1668-1693Publisher
AMER INST PHYSICS
DOI: 10.1063/1.1688328
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The turbulent Rayleigh-Taylor instability is investigated in the limit of strong mode-coupling using a variety of high-resolution, multimode, three dimensional numerical simulations (NS). The perturbations are initialized with only short wavelength modes so that the self-similar evolution (i.e., bubble diameter D(b)proportional to amplitude h(b)) occurs solely by the nonlinear coupling (merger) of saturated modes. After an initial transient, it is found that h(b) similar to alpha(b)Agt(2), where A=Atwood number, g=acceleration, and t=time. The NS yield D(b)similar toh(b)/3 in agreement with experiment but the simulation value alpha(b)similar to0.025+/-0.003 is smaller than the experimental value alpha(b)similar to0.057+/-0.008. By analyzing the dominant bubbles, it is found that the small value of alpha(b) can be attributed to a density dilution due to fine-scale mixing in our NS without interface reconstruction (IR) or an equivalent entrainment in our NS with IR. This may be characteristic of the mode coupling limit studied here and the associated alpha(b) may represent a lower bound that is insensitive to the initial amplitude. Larger values of alpha(b) can be obtained in the presence of additional long wavelength perturbations and this may be more characteristic of experiments. Here, the simulation data are also analyzed in terms of bubble dynamics, energy balance and the density fluctuation spectra. (C) 2004 American Institute of Physics.
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