{"title":"瞬态过电压的能量计算","authors":"R. B. Standler","doi":"10.1109/NSEMC.1989.37183","DOIUrl":null,"url":null,"abstract":"It is argued that the calculation of the energy in a transient overvoltage using the time integral of V/sup 2/(t)/Z, where Z has the default value of 50 Omega and the voltage, V(t), is that between the hot conductor in the AC line and ground, is inaccurate. A quantitative error analysis is presented that uses an artificial AC line network to simulate a long branch circuit and to give the impedance of the AC line as a function of frequency. A method for measuring energy dissipated in a varistor is advocated for use in future experiments. While measuring the energy in a varistor avoids many of the problems associated with the overvoltage energy, the energy dissipated in a varistor is also an underestimate of the total energy in the transient overvoltage.<<ETX>>","PeriodicalId":408694,"journal":{"name":"National Symposium on Electromagnetic Compatibility","volume":"7 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1989-05-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"10","resultStr":"{\"title\":\"Calculation of energy in transient overvoltages\",\"authors\":\"R. B. Standler\",\"doi\":\"10.1109/NSEMC.1989.37183\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"It is argued that the calculation of the energy in a transient overvoltage using the time integral of V/sup 2/(t)/Z, where Z has the default value of 50 Omega and the voltage, V(t), is that between the hot conductor in the AC line and ground, is inaccurate. A quantitative error analysis is presented that uses an artificial AC line network to simulate a long branch circuit and to give the impedance of the AC line as a function of frequency. A method for measuring energy dissipated in a varistor is advocated for use in future experiments. While measuring the energy in a varistor avoids many of the problems associated with the overvoltage energy, the energy dissipated in a varistor is also an underestimate of the total energy in the transient overvoltage.<<ETX>>\",\"PeriodicalId\":408694,\"journal\":{\"name\":\"National Symposium on Electromagnetic Compatibility\",\"volume\":\"7 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1989-05-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"10\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"National Symposium on Electromagnetic Compatibility\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/NSEMC.1989.37183\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"National Symposium on Electromagnetic Compatibility","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/NSEMC.1989.37183","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
It is argued that the calculation of the energy in a transient overvoltage using the time integral of V/sup 2/(t)/Z, where Z has the default value of 50 Omega and the voltage, V(t), is that between the hot conductor in the AC line and ground, is inaccurate. A quantitative error analysis is presented that uses an artificial AC line network to simulate a long branch circuit and to give the impedance of the AC line as a function of frequency. A method for measuring energy dissipated in a varistor is advocated for use in future experiments. While measuring the energy in a varistor avoids many of the problems associated with the overvoltage energy, the energy dissipated in a varistor is also an underestimate of the total energy in the transient overvoltage.<>