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Fundamental Study on Sensing of Targets in Random Media

Fundamental Study on Sensing of Targets in Random Media
随机介质中目标感知的基础研究
批准号:
05452223
负责人:
YOSHITOMI Kuniaki
金额:
$4.93万
依托单位:
依托单位国家:
日本
项目类别:
Grant-in-Aid for General Scientific Research (B)
财政年份:
1993
资助国家:
日本
项目状态:
已结题
起止时间:
1993 至 1995

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中文摘要
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英文摘要
A method is presented for analyzing wave scattering of a conducting target in a random medium as a boundary value problem. The problem of the wave scattering can generally be formulated by introducing two operators : a Green's function in a random medium and a current generator, a new idea, which transforms any incident wave into a surface current on the target. The current generator depends on the target only and is mathematically constructed by Yasuura's method. The rader cross-section (RCS) of the target is expressed in terms of the current generator and the moment of the Green's function. The moment is approximately given as a solution of the moment equation in a random medium.The RCS of a conducting circular cylinder and elliptic cylinder in a strong turbulent medium where an incident wave becomes incoherent on the cylinder are numerically analyzed by a high-speed computer, and the characteristics of RCS are made clear for a conducting convex cylinder. As compared with the RCS of … More the cylinder in free space (sigma_0), the RCS in the turbulent medium (sigma_0) changes largely as a function of the spatial coherence length of the incident wave (L), the length of the axis transverse to the direction of incidence (d), the curvature of the cylinder surface directly illuminated by the incident wave, and the polarization of the incident wave : E-and H-waves. The change of sigma is summarized as follows : (1) For L*d, we have sigma*2sigma_0. (2) For L*d, sigma*2sigma_0 for E-wave incidence ; and the sigma for H-wave incidence changes largely, depending on the curvature of the cylinder, because of the creeping current on the cross-section surface. (3) For L<d, when the curvature changes rapidly, we have sigma_0<sigma*2sigma_0 for E-wave incidence and sigma*3sigma_0 in a case for H-wave incidence. When the curvature becomes flat, we have sigma*sigma_0 in some cases and sigma<sigma_0 in a case, for E-wave incidence, and sigma*0.5sigma_0 in a case for H-wave incidence. For L<d, we need to estimate the sigma in any cases carefully by our method. Less
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Z.Q.Meng and M.Tateiba: "Backscattering Cross-Section of a Conducting Circular Cylinder in Strong Turbulent Media" 電気学会 電磁界理論研究会シンポジウム. EMT-94. 37-46 (1994)
Z.Q.Meng 和 M.Tateiba:“强湍流介质中传导圆柱体的反向散射截面”日本电气工程师学会电磁场理论研究小组研讨会 EMT-94(1994 年)。
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K. Yoshitomi and H. Jia: "Analysis of a slot antenna with a lossy flange" Proc. APMC'95. 2. 498-501 (1995)
K. Yoshitomi 和 H. Jia:“带损耗法兰的缝隙天线的分析”Proc。
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26
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    • 批准号:
      20510157
    • 项目类别:
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    • 资助金额:
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    • 财政年份:
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    • 批准号:
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    • 项目类别:
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    • 财政年份:
      1992
    • 负责人:
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    • 依托单位:
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