考虑无损传输线中的功率

C. N. Obiozor, M. Sadiku
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引用次数: 1

摘要

在电磁学或电力系统的本科电气工程课程中,输电线路是其中一个主题。当用分布参数对线路进行建模时,传递给无损线路末端负载的功率P通常是我们感兴趣的,它的表达式为:P=1/2|V/sup +/| R/sub 0/(1-|K/sub L/|/sup 2/),其中V/sup +/是入射电压的峰值,K/sub L/是负载处的电压反射系数,R/sub 0/是线路的特性电阻。本文指出,对于低损耗线路,上述方程是传递给负荷的更一般方程的一个特例。从时域和频域两方面考虑了低损耗线传递给负载的功率。给出了数值算例。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Consideration of power in a lossless transmission line
One of the topics in an undergraduate electrical engineering curriculum in a electromagnetics or power systems course is the transmission line. When the line is modeled with the distributed parameters, the power P, delivered to the load at the end of a lossless line is usually of interest and is given by: P=1/2|V/sup +/|/R/sub 0/(1-|K/sub L/|/sup 2/) where V/sup +/ is the peak value of incident voltage, K/sub L/ is the voltage reflection coefficient at the load, and R/sub 0/ is the characteristic resistance of the line. This paper points out that the above equation is a special case of a more general equation for the power delivered to the load for a low loss line. The power delivered to a load by a low loss line is obtained from time domain and frequency domain considerations. Numerical examples are given.
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