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平行双线BCI等效替代强场连续波电磁辐射实验研究

杨茂松 孙永卫 潘晓东 万浩江 卢新福

杨茂松, 孙永卫, 潘晓东, 等. 平行双线BCI等效替代强场连续波电磁辐射实验研究[J]. 强激光与粒子束, 2018, 30: 093201. doi: 10.11884/HPLPB201830.180078
引用本文: 杨茂松, 孙永卫, 潘晓东, 等. 平行双线BCI等效替代强场连续波电磁辐射实验研究[J]. 强激光与粒子束, 2018, 30: 093201. doi: 10.11884/HPLPB201830.180078
Yang Maosong, Sun Yongwei, Pan Xiaodong, et al. Testing technology of using bulk current injection with parallel double line as substitute for high field continuous wave electromagnetic radiation[J]. High Power Laser and Particle Beams, 2018, 30: 093201. doi: 10.11884/HPLPB201830.180078
Citation: Yang Maosong, Sun Yongwei, Pan Xiaodong, et al. Testing technology of using bulk current injection with parallel double line as substitute for high field continuous wave electromagnetic radiation[J]. High Power Laser and Particle Beams, 2018, 30: 093201. doi: 10.11884/HPLPB201830.180078

平行双线BCI等效替代强场连续波电磁辐射实验研究

doi: 10.11884/HPLPB201830.180078
基金项目: 

国家自然科学基金项目 61372040

详细信息
    作者简介:

    杨茂松(1993—),男,硕士研究生,从事电磁辐射敏感性试验研究; 1084610202@qq.com

  • 中图分类号: TM15;TN97

Testing technology of using bulk current injection with parallel double line as substitute for high field continuous wave electromagnetic radiation

  • 摘要: 由于互联系统信号传输的基础是双线,以低频线缆耦合通道中比较典型的平行双线为研究对象,针对互联系统单端为非线性受试设备的电磁辐射敏感度进行实验研究。讨论了典型互联系统辐射与注入的等效以及在高场强下的外推条件,对所选非线性器件是否满足实验要求进行了实验验证。分析了大电流注入法等效替代强场连续波电磁辐射的实验结果,并对辐照时天线极化方式不同以及有无大电流注入探头对辐射与注入等效研究的影响进行了分析。
  • 图  1  互联系统结构示意图

    Figure  1.  Schematic diagram of interconnected system

    图  2  辐射响应等效电路模型

    Figure  2.  Equivalent circuit model of radiation response

    图  3  注入响应等效电路模型

    Figure  3.  Equivalent circuit model of injection response

    图  4  辐射和注入的实验配置

    Figure  4.  Experimental setup of radiation and injection

    图  5  屏蔽室内实验系统

    Figure  5.  Experimental setup in the shielding room

    图  6  屏蔽室外实验配置

    Figure  6.  Experimental setup out of shielding room

    图  7  各频点对应LNA输入功率增大S21的变化

    Figure  7.  S21 changes with LNA input power at three frequency points

    图  8  各频点对应LNA输入功率增大SWR的变化

    Figure  8.  SWR changes with LNA input power at three frequency points

    图  9  辐射时场强与低噪声放大器响应关系

    Figure  9.  Relationship between the field strength and the response of the low-noise amplifier in radiation

    图  10  等效注入电压与低噪声放大器响应关系

    Figure  10.  Relationship between the equivalent injection voltage and the response of the low-noise amplifier

    图  11  场强和等效注入电压关系

    Figure  11.  Relationship between field strength and equivalent injection voltage

    图  12  辐射和注入时低噪声放大器响应比较

    Figure  12.  Comparison of low-noise amplifier responses at radiation and injection

    图  13  不同极化方式下场强与终端响应关系

    Figure  13.  Relationship between field strength and terminal response under different polarization modes

    图  14  不同极化方式下等效注入电压与终端响应关系

    Figure  14.  Relationship between equivalent injection voltage and terminal response under different polarization modes

    图  15  垂直极化方式下场强与等效注入电压的关系

    Figure  15.  Relationship between field strength and equivalent injection voltage in vertical polarization

    图  16  有无探头时场强与低噪声放大器响应的比较

    Figure  16.  Comparison of the response to field strength in presence or absence of the probe of the low noise amplifier

    图  17  辐射时有无探头低噪声放大器响应的比较

    Figure  17.  Comparison of the response of the low noise amplifier in presence or absence of the probe

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  • 被引次数: 0
出版历程
  • 收稿日期:  2018-03-21
  • 修回日期:  2018-05-31
  • 刊出日期:  2018-09-15

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