2014
DOI: 10.1007/s00193-014-0515-6
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Shear-layer instability in the Mach reflection of shock waves

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Cited by 9 publications
(4 citation statements)
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“…The interaction of the oblique shock with perturbed shear layer triggers the unstable growth of the contact surface ripple, which can be seen as a combination of Kelvin-Helmholtz and Richtmyer-Meshkov instabilities (Samtaney 1993;Mikaelian 1994;Rikanati 2006;Rubidge 2014). In this respect, the analysis of the perturbations growth behind the shock impingement cannot be uniquely determined by the free-stream Mach numbers M 2 − M 1 , as the upstream shear (U 2 − U 1 )/δ u and the density ρ 2 − ρ 1 would contribute differently.…”
Section: Induced Vorticity Downstreammentioning
confidence: 99%
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“…The interaction of the oblique shock with perturbed shear layer triggers the unstable growth of the contact surface ripple, which can be seen as a combination of Kelvin-Helmholtz and Richtmyer-Meshkov instabilities (Samtaney 1993;Mikaelian 1994;Rikanati 2006;Rubidge 2014). In this respect, the analysis of the perturbations growth behind the shock impingement cannot be uniquely determined by the free-stream Mach numbers M 2 − M 1 , as the upstream shear (U 2 − U 1 )/δ u and the density ρ 2 − ρ 1 would contribute differently.…”
Section: Induced Vorticity Downstreammentioning
confidence: 99%
“…Therefore, the analysis assumes that the shear layer evolution ahead of the shock impingement is negligible in first approximation. Certainly, this might not be true if the shock is sufficiently far from the streams' contact point, partly due to the Kelvin-Helmholz instability triggered by the velocity shear that may eventually turn the initially-laminar layer into a turbulent mixing layer (Rikanati 2006;Rubidge 2014). However, as the convective Mach number may also be created by more stable configurations, as those involving same-velocity different-temperature streams, the focus is placed here on the large structures that are only dominated by the incident shock angle and the stream Mach numbers.…”
Section: Introductionmentioning
confidence: 99%
“…The mechanical disquisitions over the equilibrium and dynamics of high-speed flows have long benefited from theoretical approximations of ideal flow [28,29] and small-perturbation methods [30,31]. In addition, further efforts to include real-flow effects have shed light on viscous processes in the related mechanics [32][33][34][35][36]24] as well as thermal and thermochemical non-equilibrium [37]. However, besides few studies on one-dimensional [38][39][40] and two dimensional waves [41], ideal-gas and calorically-perfect assumptions have been adopted in the vast majority of the analyses of compressible continuum-model fluids.…”
Section: Introductionmentioning
confidence: 99%
“…In all experiments, the jets burned through the metal body of the cone and the striker, indicating that one jet was directed towards the moving striker fi lling the cavity, and the other toward the top of the cone. Perhaps this eff ect is associated with irregular refl ection of the shock front from the surface of the conical notch [20,21]. The second eff ect is associated with an anomalously high value of the manganese concentration at the interface between the metal and the cavity formed by the action of the jets.…”
mentioning
confidence: 99%