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Numerical Investigation on Interference and Absorption of Electromagnetic Waves in the Plasma-Covered Cavity Using FDTD Method

机译:用FDTD方法对等离子体覆盖腔中电磁波的干扰和吸收进行数值研究

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摘要

We present real-time status of the electromagnetic (EM) scattering by the plasma-covered metal cavity, using the 2-D finite-difference time-domain method. The interference and absorption of EM waves of such progresses were analyzed. The variations in their return loss as a function of incident angle, frequency of EM wave, electron density of plasma, and plasma collision frequency were also presented. The results show that when the EM wave hits the cavity at the front aspect angle, the signals propagate along the central axis of the cavity, and the returning waves converge to source for all incident frequencies. On the contrary, when the EM wave hits the cavity at the oblique aspect angle, the combining of reflected waves among the inner walls of the cavity will result in constructive or destructive interference, consequently the returning wave not converging to source any more. The values of peak return loss are extremely different between plasma-covered metal plate and plasma-covered metal cavity. The former is less than 4 dB, while the latter reach to as large as 25 dB. The appropriate parameter regimes of plasma can be chosen for more efficiency design.
机译:我们使用2-D有限差分时域方法,介绍了被等离子体覆盖的金属腔的电磁(EM)散射的实时状态。分析了这种进展对电磁波的干扰和吸收。还介绍了其回波损耗随入射角,电磁波频率,等离子体的电子密度和等离子体碰撞频率的变化。结果表明,当EM波以前纵横角撞击腔时,信号沿腔的中心轴传播,并且返回波会聚为所有入射频率的源。相反,当EM波以倾斜的长宽角度撞击腔体时,腔体内壁之间反射波的组合将导致相长干涉或相消干涉,因此返回波不再会聚为光源。等离子体覆盖的金属板和等离子体覆盖的金属腔之间的峰值回波损耗值差异很大。前者小于4 dB,而后者则高达25 dB。可以选择适当的等离子体参数方案进行更高效的设计。

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  • 来源
    《Plasma Science, IEEE Transactions on》 |2012年第4期|p.1010-1018|共9页
  • 作者

    Xiang He;

  • 作者单位
  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
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