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Structures of strong shocks in low-density helium and neon gases.
Hua, R; Bailly-Grandvaux, M; May, J; Sherlock, M; Dozières, M; McGuffey, C; Ping, Y; Mori, W; Beg, F N.
Afiliação
  • Hua R; Center for Energy Research and Department of Mechanical and Aerospace Engineering, University of California, San Diego, La Jolla, California 92093, USA.
  • Bailly-Grandvaux M; Center for Energy Research and Department of Mechanical and Aerospace Engineering, University of California, San Diego, La Jolla, California 92093, USA.
  • May J; Department of Physics, University of California, Los Angeles, Los Angeles, California 90095, USA.
  • Sherlock M; Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Dozières M; Center for Energy Research and Department of Mechanical and Aerospace Engineering, University of California, San Diego, La Jolla, California 92093, USA.
  • McGuffey C; Center for Energy Research and Department of Mechanical and Aerospace Engineering, University of California, San Diego, La Jolla, California 92093, USA.
  • Ping Y; Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Mori W; Department of Physics, University of California, Los Angeles, Los Angeles, California 90095, USA.
  • Beg FN; Center for Energy Research and Department of Mechanical and Aerospace Engineering, University of California, San Diego, La Jolla, California 92093, USA.
Phys Rev E ; 108(3-2): 035202, 2023 Sep.
Article em En | MEDLINE | ID: mdl-37849193
Strong shocks are essential components in many high-energy-density environments such as inertial confinement fusion implosions. However, the experimental measurements of the spatial structures of such shocks are sparse. In this paper, the soft x-ray emission of a shock front in a helium gas mixture (90% helium, 10% neon) and a pure neon gas was spatially resolved using an imaging spectrometer. We observe that the shock width in the helium mixture gas is about twice as large as in the pure neon gas. Moreover, they exhibit different precursor layers, where electron temperature greatly exceeds ion temperature, extending for more than ∼350µm with the helium gas mixture but less than 30µm in the pure neon. At the shock front, calculations show that the electrons are strongly collisional with mean-free path two orders of magnitude shorter than the characteristic length of the shock. However, the helium ions can reach a kinetic regime as a consequence of their mean-free path being comparable to the scale of the shock. A radiation-hydrodynamic simulation demonstrates the impact of thermal conduction on the formation of the precursors with charge state, Z, playing a major role in heat flow and the precursor formation in both the helium mixture and the pure neon gases. Particle-in-cell simulations are also performed to study the ion kinetic effects on the formation of the observed precursors. A group of fast-streaming ions is observed leading the shock only in the helium gas mixture. Both effects explain the longer precursor layer in the helium shock.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article