基于分形EBG结构的高性能圆极化天线

X. Bao, M. Ammann, G. Ruvio, M. John
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引用次数: 2

摘要

迭代)。对于第1次和第2次迭代,每边都替换为新的缩放生成器(A1=A/3;B1=0.5*A1, A2=A1/3, B2=0.5*A2),其中A1、A2和B1、B2分别为线段长度和缩进长度(图1)。提出的EBG结构周期为32.5mm, A=27mm。分形片通过短针与连续地平面相连,构成晶格单元。短针的半径为0.5mm。采用有限元法计算了分形高阻抗表面EBG结构的色散特性。结果如图2所示,显示了1.27GHz到2.05GHz的宽带隙。如图3所示,设计了一个对角截断的方形贴片天线,同时激励TM01和TM10正交模,可以产生圆极化场。方形贴片天线尺寸为56.0×56.0m
本文章由计算机程序翻译,如有差异,请以英文原文为准。
High Performance Circularly Polarized Antenna Based on the Fractal EBG structure
th iteration). For the 1 st and 2 rd iteration, each side is replaced with new scaled generator (A1=A/3; B1=0.5*A1, A2=A1/3, B2=0.5*A2), where A1, A2 and B1, B2 are segment and indentation lengths, respectively (Fig.1). The period of the proposed EBG structure is 32.5mm, and A=27mm. A fractal patch connected to the continuous ground plane through a shorting pin constitutes a unit of the lattice. The radius of the shorting pin is 0.5mm. The dispersion characteristics of the fractal Hi-Impedance Surface EBG structure is calculated using the Finite Element Method (FEM). The results illustrated in Fig.2 show a wide bandgap from 1.27GHz to 2.05GHz. A square patch antenna with truncated opposite corners is designed as Fig.3, which excites both the TM01 and TM10 orthogonal modes, can produce circularly polarized fields. The square patch antenna size is 56.0×56.0m
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