{"title":"考虑无损传输线中的功率","authors":"C. N. Obiozor, M. Sadiku","doi":"10.1109/SECON.1996.510146","DOIUrl":null,"url":null,"abstract":"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.","PeriodicalId":338029,"journal":{"name":"Proceedings of SOUTHEASTCON '96","volume":"06 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1996-04-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Consideration of power in a lossless transmission line\",\"authors\":\"C. N. Obiozor, M. Sadiku\",\"doi\":\"10.1109/SECON.1996.510146\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"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.\",\"PeriodicalId\":338029,\"journal\":{\"name\":\"Proceedings of SOUTHEASTCON '96\",\"volume\":\"06 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1996-04-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of SOUTHEASTCON '96\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/SECON.1996.510146\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of SOUTHEASTCON '96","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/SECON.1996.510146","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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.