Criticisms of the Woodward-Lawson method

R. Elliott
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引用次数: 9

Abstract

An antenna pattern synthesis technique, applicable to equispaced linear arrays and continuous 1 ine sources, was first introduced by Woodward [l] in 1946 and then elaborated in collaboration with Lawson [21 in 1948. Known as the Woodward-Lawson method, it has been used to synthesize shaped beam patterns. Simply stated, it consists of the superposition of a family of excitations, each with au niform amplitude distribution and a uniform progressive phase distribution. The first partial excitation produces a pattern with a main beam s iadnde lobes that tail off from a level of -13.5 dB; the placement of the main beam is governed by the value of the uniform progressive phase. The second partial excitation does likewise, but its uniform progressive phase is adjusted so that its main beam peak coincides with an innermost null of the first pattern, etc. This scheme results in the filling in of a sequence of nulls in the first pattern; the amount of null-filling i s governed by the relative amplitudes of the partial excitations.
对伍德沃德-劳森方法的批评
一种适用于等间距线性阵列和连续线源的天线方向图合成技术,由Woodward[1]于1946年首次提出,1948年与Lawson[21]共同阐述。这种方法被称为伍德沃德-劳森方法,它已被用于合成异形光束图样。简单地说,它由一组激励的叠加组成,每个激励都具有均匀的振幅分布和均匀的递进相位分布。第一部分激发产生的图形具有主束和两个垂瓣,在-13.5 dB的电平处逐渐消失;主梁的位置由均匀渐进相位的值决定。第二部分激励也是如此,但其均匀渐进相位被调整,使其主束峰与第一模式的最内层零重合,等等。该方案导致在第一个模式中填充一系列null;填充零的量由部分激励的相对振幅决定。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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