{"title":"Thermally stimulated and isothermal discharge of corona-charged polypropylene","authors":"R. Singh, J. Keller, S. Datt","doi":"10.1109/ISE.1988.38571","DOIUrl":null,"url":null,"abstract":"Details are reported of short- and open-circuit thermally stimulated current (TSC), isothermal charge decay, and absorption current measurements. These measurements were conducted on corona-charged 50- mu m-thick commercial-grade isotactic polypropylene (PP). The appearance of a peak centered at 140 degrees C in open-circuit TSCs that is absent in short-circuit TSCs shows that this peak is due to the charge trapped in trapping sites located at the surface or in the near-surface region. However, the traps giving rise to three other peaks common to both type of TSCs are clearly bulk traps. Anomalous short-circuit TSCs (flowing in the same direction as the charging current), observed for high-temperature-charged samples, can be understood in terms of space-charge-limited drift of charge carriers toward the collecting electrode.<<ETX>>","PeriodicalId":199976,"journal":{"name":"6th International Symposium on Electrets,(ISE 6) Proceedings.","volume":"2 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1988-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"6th International Symposium on Electrets,(ISE 6) Proceedings.","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISE.1988.38571","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
Details are reported of short- and open-circuit thermally stimulated current (TSC), isothermal charge decay, and absorption current measurements. These measurements were conducted on corona-charged 50- mu m-thick commercial-grade isotactic polypropylene (PP). The appearance of a peak centered at 140 degrees C in open-circuit TSCs that is absent in short-circuit TSCs shows that this peak is due to the charge trapped in trapping sites located at the surface or in the near-surface region. However, the traps giving rise to three other peaks common to both type of TSCs are clearly bulk traps. Anomalous short-circuit TSCs (flowing in the same direction as the charging current), observed for high-temperature-charged samples, can be understood in terms of space-charge-limited drift of charge carriers toward the collecting electrode.<>