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Numerical and experimental study of the dynamics of a mu s helium plasma gun discharge with various amounts of N-2 admixture

机译:不同量N-2掺混物对氦等离子体枪放电动力学的数值和实验研究

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摘要

This paper presents a combined 2D numerical and experimental study of the influence of N-2 admixture on the dynamics of a He-N-2 discharge in the 10 cm long dielectric tube of a plasma gun set-up. First, the comparison between experiments and simulations is carried out on the ionization front propagation velocity in the tube. The importance of taking into account a detailed kinetic scheme for the He-N-2 mixture in the simulations to obtain a good agreement with the experiments is put forward. For the mu s driven plasma gun, the two- and three-body Penning reactions occurring in the plasma column behind the ionization front, are shown to play a key role on the discharge dynamics. In the experiments and simulations, the significant influence of the amplitude of the applied voltage on the ionization front propagation velocity is observed. As the amount of N-2 varies, simulation results show that the ionization front velocity, depends on a complex coupling between the kinetics of the discharge, the photoionization and the 2D structure of the discharge in the tube. Finally, the time evolution of axial and radial components of the electric field measured by an electro-optic probe set outside the tube are compared with simulation results. A good agreement is obtained on both components of the electric field. In the tube, simulations show that the magnitude of the axial electric field on the discharge axis depends weakly on the amount of N-2 conversely to the magnitude of the off-axis peak electric field. Both, simulations and first measurements in the tube or within the plasma plume show peak electric fields of the order of 45 kV.cm(-1).
机译:本文介绍了二维二维数值模拟和实验研究,研究了N-2混合物对等离子枪装置10 cm长介电管中He-N-2放电动力学的影响。首先,对管中的电离前沿传播速度进行了实验和模拟之间的比较。提出了在仿真中考虑He-N-2混合物的详细动力学方案以与实验取得良好一致性的重要性。对于mus驱动的等离子枪,显示出在电离前沿后面的等离子柱中发生的两体和三体Penning反应在放电动力学中起关键作用。在实验和仿真中,观察到施加电压的幅度对电离前沿传播速度的显着影响。随着N-2数量的变化,模拟结果表明,电离前沿速度取决于管内放电动力学,光电离和放电的2D结构之间的复杂耦合。最后,将管外的电光探头测得的电场的轴向和径向分量随时间的变化与仿真结果进行了比较。在电场的两个分量上都取得了良好的共识。在管中,仿真显示,放电轴上的轴向电场的大小与离轴峰值电场的大小相反,在很大程度上取决于N-2的量。在管中或等离子羽流内的模拟和首次测量都显示出45 kV.cm(-1)量级的峰值电场。

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