{"title":"A Model for Predicting the Surface Transfer Impedance of Braided Cable","authors":"L. Hoeft","doi":"10.1109/ISEMC.1986.7568276","DOIUrl":null,"url":null,"abstract":"A model for predicting the surface transfer impedance of non-optimized braided cables has been developed. This model is based on theory and is supported by extensive measurements. The transfer impedance of a braided cable is modeled as the sum of a transfer resistance and a transfer mutual inductance. The latter gives rise to a frequency dependent term. The transfer resistance is inversely proportional to cable diameter. The transfer mutual inductance is best modeled as being independent of diameter. A worst case cable overbraid model accounts for multiple layers of braid. Thus, the surface transfer impedance can be repre sented as the sum of a transfer resistance R, and a mutual inductance M-jg• To a first approximation, the transfer resist ance is determined by the amount of metal in the braid. This can be calculated using Equation 3","PeriodicalId":244612,"journal":{"name":"1986 IEEE International Symposium on Electromagnetic Compatibility","volume":"14 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1986-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"10","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1986 IEEE International Symposium on Electromagnetic Compatibility","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISEMC.1986.7568276","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 10
Abstract
A model for predicting the surface transfer impedance of non-optimized braided cables has been developed. This model is based on theory and is supported by extensive measurements. The transfer impedance of a braided cable is modeled as the sum of a transfer resistance and a transfer mutual inductance. The latter gives rise to a frequency dependent term. The transfer resistance is inversely proportional to cable diameter. The transfer mutual inductance is best modeled as being independent of diameter. A worst case cable overbraid model accounts for multiple layers of braid. Thus, the surface transfer impedance can be repre sented as the sum of a transfer resistance R, and a mutual inductance M-jg• To a first approximation, the transfer resist ance is determined by the amount of metal in the braid. This can be calculated using Equation 3