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Source Current Polarization Impact on the Cross-Polarization Definition of Practical Antenna Elements: Theory and Applications

机译:源电流极化对实用天线元件交叉极化定义的影响:理论与应用

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With the growing interest in polarization diversity in communications and radar systems, the use of Ludwig’s second and third definitions has become controversial among scientists and antenna engineers. Therefore, this paper is an attempt to clarify some of the ambiguity and confusion caused by these definitions. A detailed comparison of Ludwig’s second and thirrd definitions of cross polarization, as applied to linearly polarized antennas, was performed. The results show that, in the diagonal plane, Ludwig’s second definition leads to a lower cross-polarization level than the third definition forn$x$n- orn$y$n-polarized current sources. For a Huygens source, by Ludwig’s third definition, the radiation pattern has a lower cross-polarization level than that obtained by Ludwig’s second definition. For some applications, the antenna is usually placed in then$y{z}$nplane. Therefore, new polarization bases are proposed according to which the source is used as a reference, and also on how this source is oriented in then$y{z}$nplane. To complement the theoretical framework demonstrated in this contribution and to provide readers with a better and simpler understanding of the cross-polarization definition, the analysis of several practical antennas for diverse applications was presented. Numerical and measured radiation patterns of wire and printed dipoles, rectangular patch, pyramidal horn, and open-ended rectangular waveguide (OEWG) antennas were investigated according to the polarization formulations presented in this paper. In addition, a dual-polarized element and a dual-polarized active phased array at broadside were utilized to generalize the application.
机译:随着对通信和雷达系统极化分集的兴趣日益浓厚,路德维希的第二和第三种定义的使用在科学家和天线工程师中引起了争议。因此,本文试图澄清由这些定义引起的一些歧义和混淆。进行了路德维希关于线极化天线的第二和第三交叉极化定义的详细比较。结果表明,在对角线平面中,路德维希的第二个定义导致的交叉极化水平低于第三种定义。n $ x $ n-orn <内联公式xmlns:mml =“ http://www.w3.org/1998/Math/MathML” xmlns:xlink =“ http://www.w3.org/1999/xlink”> $ y $ n极化电流源。对于惠更斯源,根据路德维希的第三个定义,辐射图的交叉极化水平低于路德维希的第二个定义所获得的交叉极化水平。对于某些应用,通常将天线放在 $ y {z} $ nplane。因此,提出了新的极化基础,根据该极化基础,该光源被用作参考,并且还取决于该光源在随后的方向如何。 $ y {z} $ nplane。为了补充此贡献中展示的理论框架并为读者提供更好和更简单的交叉极化定义理解,本文介绍了几种用于各种应用的实用天线的分析。根据本文介绍的极化公式,研究了导线和印刷偶极子,矩形贴片,金字塔形喇叭和开放式矩形波导(OEWG)天线的数值和实测辐射方向图。另外,利用宽侧的双极化元件和双极化有源相控阵来推广应用。

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