期刊
JOURNAL OF FLUID MECHANICS
卷 964, 期 -, 页码 -出版社
CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2023.362
关键词
shock waves; turbulent mixing; transition to turbulence
The effects of initial conditions on the evolution of the Richtmyer-Meshkov instability (RMI) are analyzed using numerical simulations and compared with experimental results. Various measures of mixing layer width and decay rate of fluctuating kinetic energy are used to explore the effects of initial conditions, and good agreement is found with experimental data. The results demonstrate differences between broadband and narrowband perturbations and emphasize the importance of considering the concentration field when inferring properties based on the velocity field.
The effects of initial conditions on the evolution of the Richtmyer-Meshkov instability (RMI) at early to intermediate times are analysed, using numerical simulations of an idealised version of recent shock tube experiments performed at the University of Arizona (Sewell et al., J. Fluid Mech., vol. 917, 2021, A41). The experimental results are bracketed by performing both implicit large-eddy simulations of the high-Reynolds-number limit as well as direct numerical simulations (DNS) at Reynolds numbers lower than those observed in the experiments. Various measures of the mixing layer width h, known to scale as similar to t(theta) at late time, based on both the plane-averaged turbulent kinetic energy and volume fraction profiles are used to explore the effects of initial conditions on theta and are compared with the experimental results. The decay rate n of the total fluctuating kinetic energy is also used to estimate theta based on a relationship that assumes self-similar growth of the mixing layer. The estimates for theta range between 0.44 and 0.52 for each of the broadband perturbations considered and are in good agreement with the experimental results. Decomposing the mixing layer width into separate bubble and spike heights h(b) and hs shows that, while the bubbles and spikes initially grow at different rates, their growth rates theta(b) and theta(s) have equalised by the end of the simulations. Overall, the results demonstrate important differences between broadband and narrowband surface perturbations, as well as persistent effects of finite bandwidth on the growth rate of mixing layers evolving from broadband perturbations. Good agreement is obtained with the experiments for the different quantities considered; however, the results also show that care must be taken when using measurements based on the velocity field to infer properties of the concentration field.
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