微波参数对金属腔体强耦合覆盖率的影响研究

Study on effect of microwave parameters on coverage of strong-coupled region of metal cavies

  • 摘要: 针对精确评估目标高功率微波后门耦合效应困难的问题,以典型金属腔体为对象,提出“强耦合区域覆盖率”指标,采用时域有限差分法(FDTD)建立仿真模型,分析了高功率微波波形参数对后门耦合效应的影响。研究发现:腔体固有谐振频率下强耦合覆盖率显著高于非谐振频率;脉冲宽度增至特定值时,谐振频率下覆盖率趋于稳定;极化角从水平向垂直变化时,覆盖率有显著变化;叠加不同谐振频率可填补非强耦合区域空白,进一步提高覆盖率;脉冲前沿对覆盖率影响较小。该研究可为高功率微波后门耦合效应机理及参数优化提供关键技术支撑。

     

    Abstract:
    Background
    High-power microwave (HPM) pulses, which can interfere with or damage electronic components and circuits, have attracted considerable research interest in recent years. Aperture coupling represents a primary mechanism for such pulses to penetrate shielded metallic enclosures, significantly affecting the electromagnetic compatibility and resilience of electronic systems. Although substantial studies have focused on shielding effectiveness and resonant behaviors, the spatial distribution of coupling parameters—particularly the extent of strongly coupled regions within the cavity—remains inadequately investigated. This paper proposes a quantitative metric termed “the coverage rate of the strong-coupled region” to better evaluate HPM backdoor coupling effects.
    Purpose
    The objective is to systematically examine the influence of key HPM waveform parameters on this coverage rate within a representative metallic cavity.
    Methods
    A three-dimensional simulation model of a rectangular metallic cavity with an aperture was developed by the finite-difference time-domain (FDTD) method. The internal field distribution was monitored via an array of electric field probes. Numerical simulations were performed to assess the effects of various HPM parameters, including frequency, pulse width, pulse rise time, and polarization angle, on the coverage of strongly coupled regions.
    Results
    The coverage rate was markedly higher at the cavity’s inherent resonant frequencies than at non-resonant frequencies. Increasing the pulse width led to a saturation of coverage beyond a specific threshold. Variations in polarization angle from horizontal to vertical considerably enhanced the coverage, with vertical polarization yielding the maximum value. Superimposing multiple resonant frequencies effectively compensated for weakly coupled areas, further increasing the overall coverage. In contrast, the pulse rise time had a negligible effect on the coverage rate. The proposed coverage rate of the strong-coupled region effectively addresses the practical dilemma wherein strong local coupling does not necessarily lead to significant system-level effects.
    Conclusions
    This metric provides a quantitative basis for optimizing the alignment between sensitive components and highly coupled zones. Frequency and polarization are identified as decisive parameters for enhancing coupling effectiveness, while pulse width and multi-frequency excitation can be utilized to achieve more uniform and robust coupling coverage. These findings offer valuable guidance for the design and assessment of HPM protection measures and electromagnetic compatibility analysis.

     

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