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首页> 外文期刊>Magnetics, IEEE Transactions on >Microwave Absorbing Properties of Magnetic Composite Sheets for Oblique Incidence Angles
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Microwave Absorbing Properties of Magnetic Composite Sheets for Oblique Incidence Angles

机译:倾斜角入射的磁性复合片的微波吸收特性

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摘要

Single-layered magnetic microwave absorbers are designed for the achievement of low reflection coefficient over wide incidence angles at intelligent transport system (ITS) frequency (5.9 GHz). For the acquirement of microwave absorbers with a matching frequency of 5.9 GHz, three kinds of magnetic composite sheets were fabricated whose filler material is iron particles, TiCo- and RuCo-substituted M-hexaferrite particles. On the basis of transmission line theory, reflection loss has been calculated with variation of incident angles for both transverse electric (TE) and transverse magnetic (TM) polarization. The minimum reflection loss (less than $-$20 dB) is predicted at 6 GHz for the three specimens with a different matching thickness. The smallest matching thickness is determined in the composite of iron particles ($sim$ 2 mm) due to its high magnetic permeability and dielectric permittvity as compared with other ferrite composites (4 mm and 3 mm for TiCo- and RuCo-substituted M-hexaferrites, respectively). At this matching thickness of the magnetic composites, a low value of reflection loss (less than $-$ 20 dB) is predicted for wide incidence angles for TM polarization. In particular, Brewster angle $(theta_{rm B})$ is observed for TM polarization with no wave reflection. On the while, Brewster angle is not observed for TE polarization, resulting in higher reflection loss relative to TM polarization for oblique incidence.
机译:单层磁性微波吸收器设计用于在智能运输系统(ITS)频率(5.9 GHz)的宽入射角上实现低反射系数。为了获得匹配频率为5.9 GHz的微波吸收器,制造了三种磁性复合片,其填充材料为铁颗粒,TiCo和RuCo取代的M-六价铁氧体颗粒。根据传输线理论,已经计算了横向电(TE)和横向磁(TM)极化随入射角变化的反射损耗。对于三个具有不同匹配度的样本,在6 GHz时预测了最小反射损耗(小于 $-$ 20 dB)厚度。最小的匹配厚度是由铁颗粒的复合材料( $ sim $ 2 mm)确定的,这是由于其高磁导率和介电常数与其他铁氧体复合材料相比(TiCo和RuCo取代的M-六铁氧体分别为4 mm和3 mm)。在此磁性复合材料的匹配厚度下,反射损耗的值较低(小于 $-$ 20 dB)用于TM偏振的宽入射角。尤其是,对于TM极化,在没有波反射的情况下,观察到了布鲁斯特角 $(theta_ {rm B})$ 。同时,对于TE偏振,未观察到布儒斯特角,导致倾斜入射时相对于TM偏振,反射损耗更高。

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