内壁涂覆吸波材料腔体屏蔽效能计算方法研究

    Research on the Calculation Method of Shielding Efficiency of Inner Wall Coating Absorbing Material Cavity

    • 摘要: 屏蔽腔体内壁涂覆吸波材料可显著提高金属腔体的屏蔽效能。采用数值方法计算腔体屏蔽效能的效率较低。因此,文中针对矩形开孔腔体内壁涂覆石墨烯、碳化硅、聚四氟乙烯(PTFE)和Ni/rGO复合材料四种吸波材料情况,提出了一种基于BLT方程的解析方法计算开孔腔体屏蔽效能,对照涂覆四种材料的电磁仿真软件CST仿真结果,能准确计算出腔体谐振频率点,平均误差不超过8 dB。此种方法计算效率更高且占用计算资源更少,验证了BLT方程方法的快速性和准确性;并分析了腔体内壁涂覆不同厚度的四种材料对屏蔽效能影响。结果表明,四种材料中,相对介电常数越高的材料,腔体屏蔽效能值越大;腔体内壁涂覆PTFE材料时,材料厚度变化不会影响腔体谐振频率,且当涂覆1 mm的PTFE材料时可达到最佳的屏蔽效果。涂覆石墨烯、碳化硅、Ni/rGO复合材料三种材料时,材料厚度变化不影响TE101和TE102处的谐振频率,仅影响高次谐振TE103的频率,且这三种材料均涂覆2 mm的厚度时腔体屏蔽能力最佳。

       

      Abstract: The Coating the inner wall of the shielding cavity with absorbing materials can significantly improve the shielding efficiency of the metal cavity, but numerical calculation methods have lower efficiency in calculating the shielding effectiveness of the cavity. Therefore, this paper proposes an analytical method based on the BLT equation to calculate the shielding effectiveness of a rectangular aperture cavity with graphene, silicon carbide, polytetrafluoroethylene (PTFE), and Ni/rGO composite materials coated on its inner wall. By comparing the numerical simulation results of CST, the resonant frequencies of the cavity can be accurately calculated, with an average error of no more than 8 dB. This method has higher computational efficiency and requires fewer computational resources, the rapidity and effectiveness of the BLT equation analytical model are verified. At the same time, the influence of different thicknesses of graphene, silicon carbide, PTFE, and Ni/rGO composite materials coated on the shielding effectiveness of the cavity inner wall is analyzed. The results show that among the four materials, the higher the relative dielectric constant of the material, the greater the shielding effectiveness of the cavity; when PTFE material is coated on the inner wall of the cavity, the change in material thickness will not affect the resonant frequency of the cavity, and when 1 mm PTFE material is coated, the best shielding effect can be achieved; when coating the remaining three materials, the change in material thickness does not affect the resonance frequency at TE101 and TE102, but only affects the frequency of high order resonance TE103. Moreover, when all three materials are coated with a thickness of 2 mm, the cavity shielding ability is the best.

       

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