部分由电介质填充的扇形波导上的偏振器

Vitaly Pochernyaev, Mariia Mahomedova
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引用次数: 0

摘要

本文研究了一种基于部分介质填充扇形波导的偏振器。本文提出了一种基于扇形波导的偏振器,它比基于圆形波导-矩形波导的矩形波导偏振器具有更小的介电片尺寸和更好的驻波矩形波导-扇形波导-矩形波导结的偏振器系数。给出了矩形波导上带偏振器的扇形波导和带偏振器的圆波导上的天线馈线路径波导段的衔接图。给出了部分填充介质的扇形波导的传播常数和有效介电常数的计算公式。给出了平行于入射波偏振面和垂直于入射波偏振面的扇形介质片波导的相对介电常数与扇形介质片平均厚度的关系。本文分析了具有휃=휋/3、훷=휋/6的部分填充电介质的扇形波导。在这种情况下,准퐻ଷଵ波的扇形波导的标量特征函数被使用。给出了所考虑的波范围内的差相移变化与扇形片平均厚度的相应关系。在相位板厚度小的情况下,偏振器宽带的减小是由于在波长范围的长波长部分相移的增加,而在波长范围的短波长部分的厚度大的情况下。通过选择材料的介电常数,可以增加偏振片的宽带,但代价是增加板的长度。结型矩形波导-极化器-矩形波导驻波系数与휆/휆଴值的关系。矩形波导-偏振器在扇形波导-矩形波导上的接合处的驻波系数为3。比圆波导-矩形波导的矩形波导-偏振器结小5%。当在矩形波导上构建天线馈线路径时,基于带介电板的扇形波导的偏振器比基于带介电板的圆形波导的偏振器具有优势。这一优势在于通过偏振器和较短的介电板长度在波导部分实现较低的驻波系数值- 1,25휆଴。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
POLARIZER ON A SECTOR WAVEGUIDE PARTIALLY FILLED BY DIELECTRIC
In the article a polarizer based on a sector waveguide partially filled by dielectric is studied. The design of a polarizer based on a sector waveguide with smaller dimensions of the dielectric plate and a better coefficient of the standing wave rectangular waveguide - polarizer on sector waveguide - rectangular waveguide junction compared with rectangular waveguide-polarizer based on a circular waveguide -rectangular waveguide junction has been developed. The diagrams of the articulateon of the waveguide segments of the antenna-feeder path on rectangular waveguides with a polarizer on a sector waveguide and with a polarizer on a circular waveguide are shown. Formulas for the propagation constant of a sector waveguide partially filled with a dielectric and the effective permittivity of a sector waveguide are given. The dependences of the relative permittivities of a waveguide with a sector dielectric plate parallel and perpendicular to the plane of polarization of the incident wave on the average thickness of the sector dielectric plate are presented. The paper analyzes a sector waveguide partially filled with a dielectric, which has휃=휋/3 и 훷=휋/6. In this case, the scalar eigenfunction of the sector waveguide for the quasi-퐻ଷଵ wave is used. The corresponding dependences of the change in the differential phase shift in the considered wave range on the average thickness of the sector plate are presented. At small thicknesses of the phasing plates the decrease in the polarizer broadband is due to an increase in the phase shift in the long-wavelength part of the range and at large thicknesses in the short-wavelength one. By choosing the permittivity of the material, it is possible to increase the broadband of the polarizer at the expense of some increase in the length of the plate. The dependence of the standing wave coefficient of the junction rectangular waveguide - polarizer - rectangular waveguide on the value 휆/휆଴. The standing wave coefficient for the junction of rectangular waveguide - polarizer on a sector waveguide - rectangular waveguide is 3...5 % less than for a junction of rectangular waveguide - polarizer on a circular waveguide - rectangular waveguide. A polarizer based on a sector waveguide with a dielectric plate has an advantage over a polarizer based on a circular waveguide with a dielectric plate when building antenna-feeder paths on rectangular waveguides. This advantage consists in achieving a lower value of the standing wave coefficient on the waveguide section of the path with a polarizer and a shorter length of the dielectric plate – 1,25휆଴.
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