{"title":"静电充电及放电过程模拟","authors":"H. Kunz","doi":"10.1109/ISEMC.1982.7567746","DOIUrl":null,"url":null,"abstract":"When two isolating materials with different dielectric constants are rubbed against each other, the materials charge up; i.e. one material gives up electrons to the other isolating material. Such an effect is des cribed as electrostatic charging. The same can happen to a person. If he moves in a dry atmosphere on a well insulated carpet he can charge himself to several thousand volts. Upon approaching a conducting object, his potential is discharged with intensive arcing via the conductor.","PeriodicalId":280076,"journal":{"name":"1982 IEEE International Symposium on Electromagnetic Compatibility","volume":"54 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1982-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Electrostatic Charging and Simulation of the Discharging Process\",\"authors\":\"H. Kunz\",\"doi\":\"10.1109/ISEMC.1982.7567746\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"When two isolating materials with different dielectric constants are rubbed against each other, the materials charge up; i.e. one material gives up electrons to the other isolating material. Such an effect is des cribed as electrostatic charging. The same can happen to a person. If he moves in a dry atmosphere on a well insulated carpet he can charge himself to several thousand volts. Upon approaching a conducting object, his potential is discharged with intensive arcing via the conductor.\",\"PeriodicalId\":280076,\"journal\":{\"name\":\"1982 IEEE International Symposium on Electromagnetic Compatibility\",\"volume\":\"54 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1982-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1982 IEEE International Symposium on Electromagnetic Compatibility\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ISEMC.1982.7567746\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1982 IEEE International Symposium on Electromagnetic Compatibility","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISEMC.1982.7567746","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Electrostatic Charging and Simulation of the Discharging Process
When two isolating materials with different dielectric constants are rubbed against each other, the materials charge up; i.e. one material gives up electrons to the other isolating material. Such an effect is des cribed as electrostatic charging. The same can happen to a person. If he moves in a dry atmosphere on a well insulated carpet he can charge himself to several thousand volts. Upon approaching a conducting object, his potential is discharged with intensive arcing via the conductor.