2003
DOI: 10.1017/s0263034603213112
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Late-time growth of the Richtmyer–Meshkov instability for different Atwood numbers and different dimensionalities

Abstract: The late-time growth rate of the Richtmyer-Meshkov instability was experimentally studied at different Atwood numbers with two-dimensional~2D! and three-dimensional~3D! single-mode initial perturbations. The results of these experiments were found to be in good agreement with the results of the theoretical model and numerical simulations. In another set of experiments a bubble-competition phenomenon, which was observed in previous work for 2D initial perturbation~Sadot et al., 1998!, was shown to exist also wh… Show more

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Cited by 17 publications
(8 citation statements)
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“…The interface formed is free of supporting mesh or pins and, therefore, the initial condition can be well controlled. Owing to the minimum-surface feature, this interface has a zero mean curvature, which is different from the interface used in the previous literature (Yosef-Hai et al 2003;Chapman & Jacobs 2006;Long et al 2009). Krechetnikov (2009) directions are not understood yet.…”
mentioning
confidence: 76%
See 1 more Smart Citation
“…The interface formed is free of supporting mesh or pins and, therefore, the initial condition can be well controlled. Owing to the minimum-surface feature, this interface has a zero mean curvature, which is different from the interface used in the previous literature (Yosef-Hai et al 2003;Chapman & Jacobs 2006;Long et al 2009). Krechetnikov (2009) directions are not understood yet.…”
mentioning
confidence: 76%
“…Recently, the three-dimensional (3D) RMI has received much attention due to its more practical nature. A few 3D configurations such as the 3D single-mode and the random-perturbed cases have been considered experimentally and theoretically (Zhang & Sohn 1999;Yosef-Hai et al 2003;Chapman & Jacobs 2006;Leinov et al 2009;Long et al 2009). However, there is a scarcity of 3D RMI experimental studies.…”
mentioning
confidence: 99%
“…The boundary conditions at the shock front suggest that the pressure perturbation is proportional to ka(k) (Wouchuk & Nishihara, 1997;Wouchuk & Nishihara, 1996, Eqs. (Yosef-Hai et al, 2003;Vandenboomgaerde et al, 2003) is quite different. The lowering of the value of the Fourier component as in Example 1 (Eq.…”
Section: Resultsmentioning
confidence: 96%
“…However, due to the difficulties in experimental realization and theoretical analysis, only a few 3D configurations such as the 3D random-perturbed and the single-mode cases have been treated experimentally and theoretically. [27][28][29][30][31] Previous studies indicated that the evolution of perturbation with 3D features differs from that of perturbation with 2D features. When the directions of the principal curvatures are the same, the perturbation growth rate in 3D flows is larger than that in 2D flows.…”
Section: Two-dimensional Single-mode Interfacementioning
confidence: 99%