用于照明和射频应用的微波驱动等离子体球发生器

P. Bernhardt, B. Rock, N. Pereira
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摘要

利用电磁理论和等离子体产生方程,利用室内实验研究了球形多孔腔腔腔内增强电场产生辉光放电等离子体的过程。实验室实验表明,在SPCR的侧面插入同轴驱动的短段,可以产生稳定的等离子体云。随着输入功率的增加,来自云的光的强度变得饱和。产生密度最大、亮度最高的等离子体球的频率随泵浦波功率的增加而变化。通过对射频驱动等离子体的理论研究,对这些实验结果进行了研究。电磁波与等离子体云相互作用的电磁模型表明:(1)在等离子体频率等于泵浦频率的临界表面形成了最强烈的场;(2)随着等离子体云密度的增加,SPCR和等离子体云共振频率上移;(3)电子中性碰撞阻尼降低了内部电磁波振幅。随着泵浦功率的增加,腔放大饱和和谐振腔频移限制了微波驱动SPCR作为照明源的使用。SPCR可以提供等离子体云,同时具有微波散射和紧凑的天线应用。在实验室中,利用2.45 GHz和14.1 GHz的传输频率探索了延伸到SPCR外的等离子体云的电磁波相互作用特性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Microwave Driven Plasma Ball Generator For Illumination And Rf Applications
The production of glow-discharge plasmas by enhanced electric fields inside a spherical porous cavity resonator (SPCR) was studied using laboratory experiments with support by electromagnetic (EM) theory 1 and plasma production equations. The laboratory experiments showed the generation of a stable plasma clouds with a coax-driven stub inserted in the side of the SPCR. The intensity of the light from the cloud became saturated with increased input power. The frequency for production of the densest and brightest plasma ball shifted with increased pump wave power. These experimental observations were investigated using theoretical investigations of the RF driven plasma. The electromagnetic models of the EM wave interactions with the plasma cloud showed (1) formation of the most intense fields at the critical surface where the plasma frequency equals the pump frequency, (2) up shifting of the SPCR plus plasma cloud resonance frequency with the enhancements in plasma cloud density, and (3) reduction of the internal EM wave amplitude from damping by electron-neutral collisions. Cavity amplification saturation and resonator frequency shifting with increased pump power makes the limits the use of the microwave driven SPCR as an illumination source. The SPCR can provide a plasma cloud that has both microwave scatter and compact antenna applications. The EM wave interaction property of the plasma cloud that extends outside the SPCR has been explored in the laboratory using transmissions at 2.45 GHz 2 and 14.1 GHz.
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