{"title":"编织电缆表面传递阻抗的预测模型","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":"{\"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}","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}
A Model for Predicting the Surface Transfer Impedance of Braided Cable
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