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METHOD FOR MODIFYING REFLECTOR FOR MIRROR-MODIFYING ANTENNA

机译:反射镜修饰天线的修饰方法

摘要

PURPOSE:To obtain a highly accurate formed beam antenna capable of simply modifying a mirror face and having a smooth mirror face by finding out points on a reflector so that a phase obtained by the length of a path from a feeding horn up to the aperture face of a reflector through the reflector is made equal to optimized phase distribution. CONSTITUTION:The phase distribution on the aperture face of the reflector is optimized in accordance with the sectional shape of a prescribed formed beam obtained from the antenna consisting of one feeding horn and one reflector, and in order to attain the phase distribution, points on the reflector are found out so that the phase obtained by the length of the path from the horn up to the aperture face of the reflector through the reflector is made equal to the optimized phase distribution. These points are interpolated to constitute the reflector. For instance, the phase distribution is optimized so that the sum of the square of a difference between the objective gain of a gain restricting point 4 in a remote field and antenna gain is minimized in the amplitude distribution on the aperture face of the reflector 2 which is determined by the radiation characteristic of the horn 1. Consequently, the mirror modification can be comparatively simplified, the mirror face can be smoothly formed and high accuracy can be obtained.
机译:目的:获得一种高精度的成形波束天线,该波束天线可以通过找出反射器上的点来简单地修改镜面并具有光滑的镜面,从而使从馈电喇叭到孔径面的路径长度获得的相位使通过反射器的反射器的Δθ等于优化的相位分布。组成:反射器孔径面上的相位分布是根据从一个由一个馈电喇叭和一个反射器组成的天线获得的规定成形波束的截面形状进行优化的,为了获得相位分布,找出反射器,使得从喇叭到反射器通过反射器的孔面的路径长度获得的相位等于优化的相位分布。对这些点进行插值以构成反射器。例如,优化相位分布,使得在反射器2的孔径面上的振幅分布中,使远场中的增益限制点4的目标增益与天线增益之间的差的平方和最小。由角1的辐射特性决定。因此,可以相对简化镜的变形,可以平滑地形成镜面,并且可以获得高精度。

著录项

  • 公开/公告号JPH03253107A

    专利类型

  • 公开/公告日1991-11-12

    原文格式PDF

  • 申请/专利权人 NIPPON HOSO KYOKAI NHK;

    申请/专利号JP19900049231

  • 发明设计人 SASAKI ISATO;SHIYOUGEN KAZUYOSHI;

    申请日1990-03-02

  • 分类号H01Q19/13;

  • 国家 JP

  • 入库时间 2022-08-22 05:41:13

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