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arXiv physics/0211009physics.plasm-ph
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考虑非局域无碰撞电子动力学的低压放电动力学描述的自洽方程组

Self-consistent system of equations for a kinetic description of the low-pressure discharges accounting for the nonlocal and collisionless electron dynamics

Igor D. Kaganovich

摘要:

对于低压放电,当电子的平均自由程大于放电长度或与放电长度相当时,电子动力学本质上是非局域的。此外,电子能量分布函数(EEDF)大大偏离麦克斯韦。因此,一个准确的动力学描述的低压放电需要的非局部电导率算子的知识和计算的nonMaxwellian EEDF。以前的处理利用简化的假设:均匀的密度分布和麦克斯韦EEDF。在本研究中,一个自洽系统的动力学方程描述的非局域,非均匀,几乎无碰撞的低压放电等离子体。它包括非局部电导率算子和计算非麦克斯韦EEDF的平均动力学方程。的重要性,占不均匀的等离子体密度分布的电流密度分布和EEDF的证明。

英文摘要:

For low-pressure discharges, when the electron mean free path is larger or comparable with the discharge length, the electron dynamics is essentially nonlocal. Moreover, the electron energy distribution function (EEDF) deviates considerably from a Maxwellian. Therefore, an accurate kinetic description of the low-pressure discharges requires knowledge of the nonlocal conductivity operator and calculation of the nonMaxwellian EEDF. The previous treatments made use of simplifying assumptions: a uniform density profile and a Maxwellian EEDF. In the present study a self-consistent system of equations for the kinetic description of nonlocal, nonuniform, nearly collisionless plasmas of low-pressure discharges is derived. It consists of the nonlocal conductivity operator and the averaged kinetic equation for calculation of the nonMaxwellian EEDF. The importance of accounting for the nonuniform plasma density profile on both the current density profile and the EEDF is demonstrated.

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