2015
DOI: 10.1063/1.4931927
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Rayleigh-Taylor mixing in supernova experiments

Abstract: We report a scrupulous analysis of data in supernova experiments that are conducted at high power laser facilities in order to study core-collapse supernova SN1987A. Parameters of the experimental system are properly scaled to investigate the interaction of a blast-wave with helium-hydrogen interface, and the induced Rayleigh-Taylor instability and Rayleigh-Taylor mixing of the denser and lighter fluids with time-dependent acceleration. We analyze all available experimental images of the Rayleigh-Taylor flow i… Show more

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Cited by 47 publications
(98 citation statements)
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“…The Pico2000 beam is used in bottom-up geometry [67] to acquire snapshots of RTI during the linear and highly nonlinear phases. We are interested in accurate measurement of the mixing zone width in the nonlinear stage [68] . The main advantage of a few weeks' campaigns on LULI is to test ideas for target designs and the capability to drive those targets in the relevant plasma regimes.…”
Section: Experimental Setup and The First Radiographsmentioning
confidence: 99%
See 1 more Smart Citation
“…The Pico2000 beam is used in bottom-up geometry [67] to acquire snapshots of RTI during the linear and highly nonlinear phases. We are interested in accurate measurement of the mixing zone width in the nonlinear stage [68] . The main advantage of a few weeks' campaigns on LULI is to test ideas for target designs and the capability to drive those targets in the relevant plasma regimes.…”
Section: Experimental Setup and The First Radiographsmentioning
confidence: 99%
“…We leverage the results of LULI2000 and use theoretical scaling laws [7] to define the most relevant LMJ experiments to create turbulent HED plasmas relevant for young SNRs [68] . Extensive simulations are performed using realistic EOS for the brominated pusher and the foam [86] .…”
Section: Postprocessed Simulationsmentioning
confidence: 99%
“…This motion occurs even for an ideally planar interface and is supersonic for strong shocks. The growth of the interface perturbations is due to impulsive acceleration by the shock; it develops only when the flow fields are perturbed; its growth rate is subsonic and the associated motion is incompressible 1,2,6,[16][17][18][19][20][21][22][23] . The growth rate is constant initially and decays with time later.…”
Section: Introductionmentioning
confidence: 99%
“…As regards the general theory, we have to develop new approaches for nonequilibrium multi-scale RM/RT dynamics, capture symmetries of these RM/RT dynamics and identify properties of their asymptotic solutions 5,14,15,[25][26][27][28][29][30] . Experimental work requires one to meet tight requirements on the flow implementation, diagnostics and control 2,6,[20][21][22][23][24] . Simulations must employ highly accurate numerical methods, requiring massive computations in order to capture shocks, track interfaces, and accurately model small-scale processes [16][17][18][19][30][31][32][33][34] .…”
Section: Introductionmentioning
confidence: 99%
“…1. If the driving is sufficiently strong, an explosion may develop instead of steady-state convection, with the rising plumes becoming Rayleigh-Taylor (RT) unstable and, depending upon the structure, turbulent (Swisher, et al 2015). Expansion causes a "freeze-out" of the motions (Abarzhi 2010) and of the compositional structure, tending toward a spherical explosion (a Hubble flow).…”
Section: Lorenz Convective Rollmentioning
confidence: 99%