平面近场天线测量G/T的微波环境技术研究进展

R. Cutshall, B. Walkenhorst, J. Dobbins, Jacob Freking, B. Williams
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引用次数: 4

摘要

测量G/T的技术先前已在AMTA上提出;然而,很少有论文讨论如何在近场天线范围内测量G/T。最近的一篇论文讨论了这种方法,并在卫星有效载荷测试的大背景下进行了简要描述[1]。该文件对G/T的处理必然是简短的,并提出了与所提议的方法有关的几个问题。其他处理该主题的论文要求天线孔径与后端电子设备可分离,这在所有情况下可能都不可能[2-3]。在本文中,我们详细讨论了对[1]中提出的G/T测量方法稍加修改的版本。本文给出了一个信号和噪声功率图,它有助于理解系统信噪比(SNR)与G/T的关系,并解决了关于G/T主题的一些常见误解。本文详细描述了利用平面近场系统测量数据计算被测单位(UUT) G/T的CW-Ambient技术,并给出了CW-Ambient技术所固有的一系列假设。最后,通过对可分离UUT的实测数据进行分析,对该技术的有效性进行了评价。
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A Review of the CW-Ambient Technique for Measuring G/T in a Planar Near-Field Antenna Range
Techniques for measuring G/T have been previously presented at AMTA; however, there are very few papers that discuss how to measure G/T in a near-field antenna range. One recent paper discussed such a method and gave a brief description within the larger context of satellite payload testing [1]. The paper’s treatment of G/T was necessarily brief and gives rise to several questions in relation to the proposed method. Other papers that treated this topic required the antenna aperture to be separable from the back-end electronics, which may not be possible in all cases [2–3]. In this paper, we discuss in great detail a slightly modified version of the G/T measurement method presented in [1]. A signal and noise power diagram is presented that can be useful for understanding how system signal-to-noise ratio (SNR) relates to G/T, and a few common misconceptions concerning the topic of G/T are addressed. The CW-Ambient technique for computing G/T of a Unit Under Test (UUT) from measurements in a planar near-field system is described in detail, and a list of assumptions inherent to the CW-Ambient technique is presented. Finally, the validity of the CW-Ambient technique is assessed by analyzing measured data collected from a separable UUT.
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