初步设计程序,以确定能够满足辐射测量要求的进给孔直径和其他基本参数

P. Foldes, F. Marinelli
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引用次数: 0

摘要

本文从抛物面天线所要满足的辐射要求出发,给出了确定主馈源尺寸的简单准则。特别考虑了天线的波束效率和半功率波束宽度。波束效率的损失预算以这种方式给出了能够提供所需波束效率值的进给孔径的主要模式。本文所包含的所有考虑都可以定性地应用于任何天线,只要它是一个偏置抛物面反射器。并以多频成像微波辐射计(MIMR)天线光学为例进行了定量分析。此外,由于不同的原因,考虑到该辐射计的较高频率(90 GHz)。与制造小尺寸进料有关的所需公差可能会遇到困难。由于上述原因,所描述的程序是保守的,可以毫无困难地应用于较低的频率。给出辐射计温度分辨率的波束效率要求是针对天线波束峰值周围的2个角区域指定的。显然,随着进给孔径的增大而增加抛物线照度的边缘锥度是不够的,但必须非常注意不要超过进给孔径直径的一定上限,以避免抛物线半功率波束宽度大于0.174/spl度/的要求值。最好有一个形状类似于高斯函数的初级图案,并具有适当的边缘锥度。列出了影响光束效率的退化因素。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A preliminary design procedure to find the aperture diameter and other basic parameters of a feed able to satisfy radiometric requirements
An analysis is presented which, starting from the radiometric requirements to be satisfied by a parabolic antenna, gives simple guidelines to properly size the primary feed. In particular the beam efficiency and the half power beamwidth of the antenna are taken into account. A loss budget for the beam efficiency is made giving in this way the feed aperture able with its primary pattern to provide the required beam efficiencies values. All the considerations contained in the paper can be qualitatively applied to whatever antenna at the condition that it is an offset parabolic reflector. Nevertheless a quantitative analysis is given taking as a practical case the MIMR (Multifrequency Imaging Microwave Radiometer) antenna optic. Moreover the higher frequency of this radiometer (90 GHz) is taken into account for different reasons. The required tolerances related to the manufacturing of a feed with small dimensions can be met with difficulties. For the above reasons the procedure described is conservative and can be applied without difficulties to lower frequencies. The beam efficiency requirements which give the radiometer temperature resolution are specified for 2 angular zones around the antenna beam peak. It is clear that it is not sufficient to increase the edge taper of the parabola illumination with the enlargement of the feed aperture but it is necessary to take great care to not exceed certain upper limits for the feed aperture diameter to avoid a parabola half power beamwidth larger than the required value of 0.174/spl deg/. It would be preferable to have a primary pattern with a shape similar to a gaussian function and with an adequate edge taper. The degradation factors which affect the beam efficiency are listed.<>
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