{"title":"Swarm parameters along gas-solid dielectric interfaces","authors":"S. Mahajan, T. Sudarshan, R. Dougal","doi":"10.1109/CEIDP.1986.7726500","DOIUrl":null,"url":null,"abstract":"In order to understand the surface flashover mechanisms in a spacer-bridged, compressed-gas-insulated system, it is essential to have a detailed knowledge of the associated physical parameters, these being dominantly the first Townsend ionization coefficient (α) and the electron drift velocity (Ve). As the addition of a solid spacer to a compressed gas insulated system inevitably reduces the breakdown strength it is important to know how α and Ve are modified or if these are modified at all. These parameters can be determinated through the measurement of electron avalanches using the pulsed Townsend technique [1,2]. Jaksts and Cross attempted such measurements, however, the relatively long pulse width (∼10ns) of the laser used for photo-initiation of the electron avalanche and the poor bandwidth of the electron current amplifier, coupled with noise from the laser, prevented accurate measurements [3].","PeriodicalId":354533,"journal":{"name":"Conference on Electrical Insulation & Dielectric Phenomena — Annual Report 1986","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1986-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Conference on Electrical Insulation & Dielectric Phenomena — Annual Report 1986","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CEIDP.1986.7726500","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
In order to understand the surface flashover mechanisms in a spacer-bridged, compressed-gas-insulated system, it is essential to have a detailed knowledge of the associated physical parameters, these being dominantly the first Townsend ionization coefficient (α) and the electron drift velocity (Ve). As the addition of a solid spacer to a compressed gas insulated system inevitably reduces the breakdown strength it is important to know how α and Ve are modified or if these are modified at all. These parameters can be determinated through the measurement of electron avalanches using the pulsed Townsend technique [1,2]. Jaksts and Cross attempted such measurements, however, the relatively long pulse width (∼10ns) of the laser used for photo-initiation of the electron avalanche and the poor bandwidth of the electron current amplifier, coupled with noise from the laser, prevented accurate measurements [3].