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INACCURACY IN SPHERICAL NEAR-FIELD ANTENNA MEASUREMENTS DUE TO ANECHOIC CHAMBER REFLECTIVITY

机译:由于化学腔室反射率,球形近场天线测量的不准确性

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The need for a well-defined accuracy estimate in antenna measurements requires identification of all possible sources of inaccuracy and determination of their influence on the measured parameters. For anechoic chambers, one important source of inaccuracy is the reflection from the absorbers on walls, ceiling, and floor, which gives rise to so-called stray signals that interfere with the desired signal. These stray signals are usually quantified in terms of the reflectivity level. For near-field measurements, the reflectivity level is not sufficient information for estimation of inaccuracy due to the stray signals since the near-to-far-field transformation of the measured near-field may essentially change their influence. Moreover, the inaccuracies are very different for antennas of different directivity and with different level of sidelobes, and for different parts of the radiation pattern. In this paper, the simulation results of a spherical near-field antenna measurement in an anechoic chamber are presented and discussed. The influence of the stray signals on the directivity at all levels of the radiation pattern is investigated for several levels of the chamber reflectivity and for different antennas. The antennas are modeled by two-dimensional arrays of Huygens' sources that allow calculation of both the exact near-field and the exact far-field. The near-field with added stray signals is then transformed to the far-field and compared to the exact far-field. The co-polar and cross-polar directivity patterns are compared at different levels down from the peak directivity.
机译:在天线测量中对明确定义的精度估计需要识别所有可能的不准确源和对测量参数的影响。对于AneChice腔室,一个重要的不准确来源是从墙壁,天花板和地板上的吸收器的反射,这导致了干扰所需信号的所谓的杂散信号。这些杂散信号通常在反射率水平上量化。对于近场测量,由于偏移近场的近乎远场变换可以基本上改变它们的影响,因此反射率水平是由于杂散信号而导致的不准确性的足够的信息。此外,对于不同方向性的天线以及不同水平的侧链和辐射图案的不同部分,不准确性是差异。本文介绍并讨论了展示并讨论了一个浮雕室中的球形近场天线测量的模拟结果。研究了杂散信号对辐射图案的各级方向性的影响,用于几个腔室反射率和不同天线。天线由惠更斯源的二维阵列进行建模,允许计算精确的近场和确切的远场。然后将具有添加杂散信号的近场转换为远场并与精确的远场相比。在峰值方向性下,在不同的水平下比较有源和交叉极性方向模式。

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