N. Talwalkar, P. Lauritzen, B. Fatemizadeh, D. Perlman, C.L. Ma
{"title":"用于电路仿真的电源BJT模型","authors":"N. Talwalkar, P. Lauritzen, B. Fatemizadeh, D. Perlman, C.L. Ma","doi":"10.1109/PESC.1996.548558","DOIUrl":null,"url":null,"abstract":"The power BJT is modeled using the lumped-charge method using simplified forms of the Poisson's equation, the continuity equation and the Boltzmann relation. All important one-dimensional effects are included in the model. Only nine parameters are needed to completely specify the model except for junction capacitances and parasitic resistances. This model can be easily extended to make a BJT Darlington model.","PeriodicalId":19979,"journal":{"name":"PESC Record. 27th Annual IEEE Power Electronics Specialists Conference","volume":"22 1","pages":"50-55 vol.1"},"PeriodicalIF":0.0000,"publicationDate":"1996-06-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"16","resultStr":"{\"title\":\"A power BJT model for circuit simulation\",\"authors\":\"N. Talwalkar, P. Lauritzen, B. Fatemizadeh, D. Perlman, C.L. Ma\",\"doi\":\"10.1109/PESC.1996.548558\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The power BJT is modeled using the lumped-charge method using simplified forms of the Poisson's equation, the continuity equation and the Boltzmann relation. All important one-dimensional effects are included in the model. Only nine parameters are needed to completely specify the model except for junction capacitances and parasitic resistances. This model can be easily extended to make a BJT Darlington model.\",\"PeriodicalId\":19979,\"journal\":{\"name\":\"PESC Record. 27th Annual IEEE Power Electronics Specialists Conference\",\"volume\":\"22 1\",\"pages\":\"50-55 vol.1\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1996-06-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"16\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"PESC Record. 27th Annual IEEE Power Electronics Specialists Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PESC.1996.548558\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"PESC Record. 27th Annual IEEE Power Electronics Specialists Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PESC.1996.548558","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The power BJT is modeled using the lumped-charge method using simplified forms of the Poisson's equation, the continuity equation and the Boltzmann relation. All important one-dimensional effects are included in the model. Only nine parameters are needed to completely specify the model except for junction capacitances and parasitic resistances. This model can be easily extended to make a BJT Darlington model.
求助内容：
应助结果提醒方式：
京公网安备 11010802042870号
