N个线性极化时谐平面波和的概率密度函数

J. E. Roy
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引用次数: 0

摘要

已知,在N相量在统计上独立且平稳的假设下(该假设导致每个相量相位的概率密度函数(PDF)在长度为2π的区间内是均匀的),Blanc-Lapierre变换给出了N相量之和的大小的概率密度函数作为每个相量大小的概率密度函数的表达式。然而,这个表达式没有考虑极化,只考虑了场的相位和大小。本文还包括极化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Probability Density Function for a sum of N linearly polarized time-harmonic plane waves
It is known that under the assumption that N phasors are statistically independent and stationary (which assumption leads to the Probability Density Function (PDF) for the phase of each phasor to be uniform over an interval of length 2π), the Blanc-Lapierre transformation gives the expression for the PDF of the magnitude of the sum of N phasors as a function of the PDF of the magnitude of each phasor. This expression, however, does not take into account the polarization, only the phase and magnitude of the field. This paper includes the polarization as well.
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