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中国物理学会期刊

介质阻挡均匀大气压辉光放电数值模拟研究

CSTR: 32037.14.aps.52.1694

Numerical simulation of dielectric-barrier-controlled glow discharge at atmosphe ric pressure

CSTR: 32037.14.aps.52.1694
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  • 通过数值求解一维电子、离子连续性方程和动量方程,以及电流连续性方程,计算了氦气介 质阻挡大气压辉光放电电子、离子密度和电场在放电空间的时空分布,以及放电电流密度和 绝缘介质板充电电荷密度随时间的变化. 分析讨论所加电压频率、幅值及介质板性质等对均 匀大气压辉光放电性质的影响. 当外加电压频率足够高时,大量离子被俘获在放电空间,空 间电荷场又引起足够多的电子滞留在放电空间. 这些种子电子使得在大气压下发生汤森放电 ,放电空间结构类似于低气压辉光放电,即存在明显的阴极位降区、负辉区、法拉第暗区和 等离子体正柱

     

    The space and time distributions of the electric field and the electron and ion densities, as well as the time evolutions of the discharge current density and the surface charge density of the dielectric layer in He dielectric-barrier-controlled glow discharge at atmospheric pressure are calculated by solving the on e-dimensional continuity and momentum equations for electrons and ions, coupled to the current continuity equation. The properties of uniform atmospheric pressu re glow discharge under the conditions of different driving frequency, voltage o r dielectric layer are discussed and analyzed. When the driving frequency is hig h enough, a large number of ions are trapped and the induced space charge field makes a great many of electrons stay in the discharge volume. These seed electro ns lead to a Townsend discharge at atmosphere pressure. The structure of this di scharge is similar to that of low-pressure glow discharge, i.e. there exist four specific regions: the cathode fall, the negative glow, the Faraday dark space a nd the positive column. The discharge current becomes small with decreasing voltage amplitude applied. The secondary electron emission from the dielectric layer makes the discharge current increase. The thicker the dielectric layer is or the smaller the permittivity, the smaller the discharge current is.

     

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