{"title":"Polyphase guided TEM waves","authors":"R. Ianconescu","doi":"10.1109/EEEI.2012.6377001","DOIUrl":null,"url":null,"abstract":"Guided TEM waves have been usually investigated between 2 conductors. There are several circumstances when one encounters TEM waves guided by multiple conductors, like in flat cables, high frequency polyphase transmission lines, etc. In this work we develop a methodology for multiconductor TEM waves, as follows. The two dimensional Laplace equation for the scalar potential is solved for the given cross section geometr y, having N+1 conductors. Then an N×N elastance matrix is derived, and from it a characteristic impedance matrix, defining the connection between the voltages and the currents of a forward moving wave. From the impedance matrix one calculates the values of N(N+1)/2 resistors network that consist the matched load for the given geometry.","PeriodicalId":177385,"journal":{"name":"2012 IEEE 27th Convention of Electrical and Electronics Engineers in Israel","volume":"66 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2012-12-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2012 IEEE 27th Convention of Electrical and Electronics Engineers in Israel","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/EEEI.2012.6377001","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 5
Abstract
Guided TEM waves have been usually investigated between 2 conductors. There are several circumstances when one encounters TEM waves guided by multiple conductors, like in flat cables, high frequency polyphase transmission lines, etc. In this work we develop a methodology for multiconductor TEM waves, as follows. The two dimensional Laplace equation for the scalar potential is solved for the given cross section geometr y, having N+1 conductors. Then an N×N elastance matrix is derived, and from it a characteristic impedance matrix, defining the connection between the voltages and the currents of a forward moving wave. From the impedance matrix one calculates the values of N(N+1)/2 resistors network that consist the matched load for the given geometry.