• Matter and Radiation at Extremes
  • Vol. 6, Issue 3, 035901 (2021)
Hong-bo Cai1、2, Xin-xin Yan3, Pei-lin Yao4, and Shao-ping Zhu1、5、6
Author Affiliations
  • 1Institute of Applied Physics and Computational Mathematics, Beijing 100094, China
  • 2Center for Applied Physics and Technology, HEDPS, and College of Engineering, Peking University, Beijing 100871, China
  • 3Center for Applied Physics and Technology, HEDPS, School of Physics, and College of Engineering, Peking University, Beijing 100871, China
  • 4Department of Engineering Physics, Tsinghua University, Beijing 100084, China
  • 5Graduate School, China Academy of Engineering Physics, P.O. Box 2101, Beijing 100088, China
  • 6Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, CAEP, 621900 Mianyang, China
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    DOI: 10.1063/5.0042973 Cite this Article
    Hong-bo Cai, Xin-xin Yan, Pei-lin Yao, Shao-ping Zhu. Hybrid fluid–particle modeling of shock-driven hydrodynamic instabilities in a plasma[J]. Matter and Radiation at Extremes, 2021, 6(3): 035901 Copy Citation Text show less

    Abstract

    Shock-driven hydrodynamic instabilities in a plasma usually lead to interfacial mixing and the generation of electromagnetic fields, which are nonequilibrium processes coupling kinetics with meso- and macroscopic dynamics. The understanding and modeling of these physical processes are very challenging tasks for single-fluid hydrodynamic codes. This work presents a new framework that incorporates both kinetics and hydrodynamics to simulate shock waves and hydrodynamic instabilities in high-density plasmas. In this hybrid code, ions are modeled using the standard particle-in-cell method together with a Monte Carlo description of collisions while electrons are modeled as a massless fluid, with the electron heat flux and fluid–particle energy exchange being considered in the electron pressure equation. In high-density plasmas, Maxwell’s equations are solved using Ohm’s law instead of Ampère’s law. This hybrid algorithm retains ion kinetic effects and their consequences for plasma interpenetration, shock wave propagation, and hydrodynamic instability. Furthermore, we investigate the shock-induced (or gravity-induced) turbulent mixing between a light and a heavy plasma, where hydrodynamic instabilities are initiated by a shock wave (or gravity). This study reveals that self-generated electromagnetic fields play a role in the formation of baroclinic vorticity along the interface and in late-time mixing of the plasmas. Our results confirm the ability of the proposed method to describe shock-driven hydrodynamic instabilities in a plasma, in particular, nonequilibrium processes that involve mixing and electromagnetic fields at the interface.
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    nemedVedt=eneE+Ve×BcpeπeR,

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    Ru=αuαu+α(b×u),

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    RT=βuTTeβuTTeβuT(b×Te),

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    ωce=eB/mec=1.76×107Brad/s.

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    Bt=c×E.

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    Bt=×(V×B)×Jene×B+c×peenec×RT+Ruenec×ηJ+ηJ.

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    Je=c4π×B14πEt(Ji+Jp),

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    ρt+J=0,

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    t+Vepe=γPeVeqe+Qe,

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    qeu=βTuu+βTuu+βTu(b×u),

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    qeT=κeTe+κeTe+κe(b×Te),

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    Qe=(Ru+RT)uQi,

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    Fie=νiemie(vevi)+νieε(TiTe)vi2vi2νiemie2(vevi)2mi(vi2vi2)(vivi),

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    dTαdt=βνεα\β(TβTα),

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    νεα\β=1.8×1019(mαmβ)1/2Zα2Zβ2nβlnΛαβ(mαTβ+mβTα)3/2s1.

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    Hong-bo Cai, Xin-xin Yan, Pei-lin Yao, Shao-ping Zhu. Hybrid fluid–particle modeling of shock-driven hydrodynamic instabilities in a plasma[J]. Matter and Radiation at Extremes, 2021, 6(3): 035901
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