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Frontiers of Electrical and Electronic Engineering

ISSN 2095-2732

ISSN 2095-2740(Online)

CN 10-1028/TM

Front Elect Electr Eng Chin    2009, Vol. 4 Issue (2) : 210-213    https://doi.org/10.1007/s11460-009-0030-1
RESEARCH ARTICLE
Absorption of electromagnetic wave by inhomogeneous, unmagnetized plasma
Ming YAN1(), Gang LEI1, Xiwei HU1, Keran SHAO2
1. National Key Laboratory for Vessel Integrated Power System Technology, Navy University of Engineering, Wuhan 430033, China; 2. College of Electrical and Electronic Engineering, Huazhong University of Science and Technology, Wuhan 430074, China
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Abstract

In this article, a novel and normalized Z-transform finite-difference time-domain (ZTFDTD) method is presented. This method uses a more general form of Maxwell’s equations using the BoldItalic, BoldItalic, BoldItalic fields. The iterative model of BoldItalic-BoldItalic-BoldItalic-BoldItalic can be obtained by using the Z-transform resulted frequency-dependent formula between BoldItalic and BoldItalic. The advantages of the ZTFDTD consist in that the discrete equations are simple, the results are precise, easy to program and capable of dealing with the key technologies of finite-difference time-domain (FDTD), such as absorbing boundary conditions (uniaxial anisotropic perfectly matched layer, UPML) and near-to-far-field transformation. The ZTFDTD method is then used to simulate the interaction of electromagnetic wave with plasma. Using a simplified two-dimensional model, the stealth effect of inhomogeneous, unmagnetized plasma is studied both in different electron densities of plasma, different electromagnetic wave frequencies and different plasma collision frequencies. The numerical results indicate that plasma stealth is effective in theory and a reasonable selection with the plasma parameters that can greatly enhance the effectiveness of plasma stealth.

Keywords finite-difference time-domain (FDTD)      Z-transform      anisotropic perfectly matched layer      plasma stealth      radar cross section (RCS)     
Corresponding Author(s): YAN Ming,Email:hustym@sohu.com   
Issue Date: 05 June 2009
 Cite this article:   
Ming YAN,Gang LEI,Xiwei HU, et al. Absorption of electromagnetic wave by inhomogeneous, unmagnetized plasma[J]. Front Elect Electr Eng Chin, 2009, 4(2): 210-213.
 URL:  
https://academic.hep.com.cn/fee/EN/10.1007/s11460-009-0030-1
https://academic.hep.com.cn/fee/EN/Y2009/V4/I2/210
Fig.1  Three boundaries and zoning of ZTFDTD grid
Fig.2  Amplitude and RCS of perfectly conducting plate covered with nothing and IUP. (a) Amplitude of perfectly conducting plate covered with nothing; (b) amplitude of perfectly conducting plate covered with IUP; (c) RCS of perfectly conducting plate covered with nothing and IUP
Fig.3  RCS of perfectly conducting plate covered with IUP in different electron densities
Fig.4  RCS of perfectly conducting plate covered with IUP in different EM wave frequencies
Fig.5  RCS of perfectly conducting plate covered with IUP in different plasma collision frequencies
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[1] LIU Liye, SU Yi, MAO Junjie. FDTD analysis of ground-penetrating radar antennas with shields and absorbers[J]. Front. Electr. Electron. Eng., 2008, 3(1): 90-95.
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