Exploring the Microscopic Physical Processes of Z-pinch by a Modified Electrostatic Direct Implicit Particle-in-Cell Algorithm

Kaixuan Li, Cheng Ning, Ye Dong, Chuang Xue
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Abstract

For investigating efficiently the stagnation kinetic-process of Z-pinch, we develop a novel modified electrostatic implicit particle-in-cell (PIC) algorithm in radial one-dimension for Z-pinch simulation in which a small-angle cumulative binary collision algorithm is used. In our algorithm, the electric field in z-direction is solved by a parallel electrode-plate model, the azimuthal magnetic field is obtained by Ampere's law, and the term for charged particle gyromotion is approximated by the cross product of the averaged velocity and magnetic field. In simulation results of 2 MA deuterium plasma shell Z-pinch, the mass center implosion trajectory agree generally with that obtained by one dimensional MHD simulation, and the plasma current also closely aligns with the external current. The phase space diagrams and radial velocity probability distributions of ions and electrons are obtained. The main kinetic characteristic of electron motion is thermal equilibrium and oscillation, which should be oscillated around the ions, while that of ion motion is implosion inwards. In the region of stagnation radius, the radial velocity probability distributions of ions transit from the non-equilibrium to equilibrium state with the current increasing, while electron’s is basically the equilibrium state. When the initial ion density and current peak aren’t high enough, the ions may not reach their thermal equilibrium state through collisions even in its stagnation phase.
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用修正的静电直接隐含粒子池算法探索 Z-pinch 的微观物理过程
为了有效研究 Z-夹子的停滞动力学过程,我们开发了一种新颖的径向一维静电隐式粒子入胞(PIC)算法,用于 Z-夹子模拟,其中使用了小角度累积二元碰撞算法。在我们的算法中,Z 方向的电场由平行电极板模型求解,方位磁场由安培定律求得,带电粒子回旋运动项由平均速度和磁场的乘积近似得到。在 2 MA 氘等离子体壳 Z-pinch 的模拟结果中,质心内爆轨迹与一维 MHD 模拟结果基本一致,等离子体电流也与外部电流密切相关。得到了离子和电子的相空间图和径向速度概率分布。电子运动的主要动力学特征是热平衡和振荡,应围绕离子振荡,而离子运动的主要动力学特征是向内内爆。在停滞半径区域,随着电流的增大,离子的径向速度概率分布从非平衡态过渡到平衡态,而电子的径向速度概率分布基本处于平衡态。当初始离子密度和电流峰值不够高时,即使在停滞阶段,离子也可能无法通过碰撞达到热平衡状态。
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