Radiation and heat transport in divergent shock–bubble interactions

Author:

Kurzer-Ogul K.12ORCID,Haines B. M.2ORCID,Montgomery D. S.2ORCID,Pandolfi S.3ORCID,Sauppe J. P.2ORCID,Leong A. F. T.2ORCID,Hodge D.4ORCID,Kozlowski P. M.2ORCID,Marchesini S.3ORCID,Cunningham E.3ORCID,Galtier E.3ORCID,Khaghani D.3ORCID,Lee H. J.3ORCID,Nagler B.3ORCID,Sandberg R. L.4ORCID,Gleason A. E.3ORCID,Aluie H.15ORCID,Shang J. K.15ORCID

Affiliation:

1. Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14620, USA

2. Los Alamos National Laboratory 2 , Los Alamos, New Mexico 87545, USA

3. SLAC National Accelerator Laboratory 3 , Menlo Park, California 94025, USA

4. Department of Physics and Astronomy, Brigham Young University 4 , Provo, Utah 84602, USA

5. Laboratory for Laser Energetics, University of Rochester 5 , Rochester, New York 14620, USA

Abstract

Shock–bubble interactions (SBIs) are important across a wide range of physical systems. In inertial confinement fusion, interactions between laser-driven shocks and micro-voids in both ablators and foam targets generate instabilities that are a major obstacle in achieving ignition. Experiments imaging the collapse of such voids at high energy densities (HED) are constrained by spatial and temporal resolution, making simulations a vital tool in understanding these systems. In this study, we benchmark several radiation and thermal transport models in the xRAGE hydrodynamic code against experimental images of a collapsing mesoscale void during the passage of a 300 GPa shock. We also quantitatively examine the role of transport physics in the evolution of the SBI. This allows us to understand the dynamics of the interaction at timescales shorter than experimental imaging framerates. We find that all radiation models examined reproduce empirical shock velocities within experimental error. Radiation transport is found to reduce shock pressures by providing an additional energy pathway in the ablation region, but this effect is small (∼1% of total shock pressure). Employing a flux-limited Spitzer model for heat conduction, we find that flux limiters between 0.03 and 0.10 produce agreement with experimental velocities, suggesting that the system is well-within the Spitzer regime. Higher heat conduction is found to lower temperatures in the ablated plasma and to prevent secondary shocks at the ablation front, resulting in weaker primary shocks. Finally, we confirm that the SBI-driven instabilities observed in the HED regime are baroclinically driven, as in the low energy case.

Funder

National Nuclear Security Administration

National Science Foundation

Office of Science

National Aeronautics and Space Administration

Publisher

AIP Publishing

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