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Analytical studies on the evolution processes of rarefied deuterium plasma shell Z-pinch by PIC and MHD simulations

机译:通过PIC和MHD模拟分析稀有氘等离子体壳Z型夹层的演化过程

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摘要

In this paper,we analytically explore the magnetic field and mass density evolutions obtained in particle-in-cell (PIC) and magnetohydrodynamics (MHD) simulations of a rarefied deuterium shell Z-pinch and compare those results,and also we study the effects of artificially increased Spitzer resistivity on the magnetic field evolution and Z-pinch dynamic process in the MHD simulation.There are significant differences between the profiles of mass density in the PIC and MHD simulations before 45 ns of the Z-pinch in this study.However,after the shock formation in the PIC simulation,the mass density profile is similar to that in the MHD simulation in the case of using multiplier 2 to modify the Spitzer resistivity.Compared with the magnetic field profiles of the PIC simulation of the shell,the magnetic field diffusion has still not been sufficiently revealed in the MHD simulation even though their convergence ratios become the same by using larger multipliers in the resistivity.The MHD simulation results suggest that the magnetic field diffusion is greatly enhanced by increasing the Spitzer resistivity used,which,however,causes the implosion characteristic to change from shock compression to weak shock,even shockless evolution,and expedites the expansion of the shell.Too large a multiplier is not suggested to be used to modify the resistivity in some Z-pinch applications,such as the Z-pinch driven inertial confinement fusion (ICF) in a dynamic hohlraum.Two-fluid or Hall MHD model,even the PIC/fluid hybrid simulation would be considered as a suitable physical model when there exist the plasma regions with very low density in the simulated domain.
机译:在本文中,我们分析性地研究了稀有氘壳Z型捏的单元粒子(PIC)和磁流体动力学(MHD)模拟中获得的磁场和质量密度演化,并比较了这些结果,并且我们研究了在MHD模拟中,人为地增加了Spitzer电阻对磁场演化和Z捏动态过程的影响。在本研究中,在45 ns Z捏之前,PIC和MHD仿真中的质量密度曲线之间存在显着差异。在PIC模拟中形成冲击之后,在使用乘数2修改Spitzer电阻率的情况下,质量密度分布与MHD模拟中的相似。与壳体PIC模拟的磁场分布相比,磁尽管通过使用更大的电阻率乘数可以使它们的收敛率相同,但在MHD模拟中仍然没有充分揭示场扩散。相关结果表明,通过增加所使用的Spitzer电阻率可以大大增强磁场扩散,但是,这会使内爆特性从冲击压缩变为弱冲击,甚至无冲击演化,并加速了壳体的膨胀。建议不要在某些Z捏应用中使用倍增器来修改电阻率,例如动态水平仪中的Z捏驱动惯性约束融合(ICF)。双流体或霍尔MHD模型,甚至是PIC /流体混合当在模拟域中存在密度非常低的等离子体区域时,模拟将被视为合适的物理模型。

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  • 来源
    《中国物理:英文版》 |2018年第2期|457-467|共11页
  • 作者单位

    Institute of Applied Physics and Computational Mathematics, Beijing 100088, China;

    Institute of Applied Physics and Computational Mathematics, Beijing 100088, China;

    Institute of Applied Physics and Computational Mathematics, Beijing 100088, China;

    Institute of Applied Physics and Computational Mathematics, Beijing 100088, China;

    Institute of Applied Physics and Computational Mathematics, Beijing 100088, China;

    Institute of Applied Physics and Computational Mathematics, Beijing 100088, China;

    Institute of Applied Physics and Computational Mathematics, Beijing 100088, China;

  • 收录信息 中国科学引文数据库(CSCD);中国科技论文与引文数据库(CSTPCD);
  • 原文格式 PDF
  • 正文语种 eng
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