{"title":"非均匀和准均匀电场作用下聚乙烯脉冲树形击穿","authors":"K. Kudo","doi":"10.1109/CEIDP.1989.69556","DOIUrl":null,"url":null,"abstract":"The polarity effect of the impulse tree inception and complete breakdown (puncture) of low-density polyethylene is described as a function of the radius of the needle tip. Furthermore, the morphology of the impulse tree and breakdown channels is examined. It is shown that the puncture field strength E/sub b/ for both polarities is about 6 MV/cm at 500 mu m and is of the same order as the intrinsic breakdown strength of low-density polyethylene. The shapes of impulse tree and breakdown channels for both polarities are shown for varying tip radius and gap distance. Although the E/sub b/ obtained has almost the same value as the intrinsic breakdown strength at larger tip radii, it can be seen that the morphologies of the breakdown channels for the two polarities are different. Especially at larger tip radii, the difference of the morphology is remarkable. One explanation for this difference may be the high-density gaseous plasma and the joule heating in the tree channels.<<ETX>>","PeriodicalId":10719,"journal":{"name":"Conference on Electrical Insulation and Dielectric Phenomena,","volume":"43 1","pages":"259-264"},"PeriodicalIF":0.0000,"publicationDate":"1989-10-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"Impulse treeing breakdown in polyethylene under non-uniform and quasi-uniform fields\",\"authors\":\"K. Kudo\",\"doi\":\"10.1109/CEIDP.1989.69556\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The polarity effect of the impulse tree inception and complete breakdown (puncture) of low-density polyethylene is described as a function of the radius of the needle tip. Furthermore, the morphology of the impulse tree and breakdown channels is examined. It is shown that the puncture field strength E/sub b/ for both polarities is about 6 MV/cm at 500 mu m and is of the same order as the intrinsic breakdown strength of low-density polyethylene. The shapes of impulse tree and breakdown channels for both polarities are shown for varying tip radius and gap distance. Although the E/sub b/ obtained has almost the same value as the intrinsic breakdown strength at larger tip radii, it can be seen that the morphologies of the breakdown channels for the two polarities are different. Especially at larger tip radii, the difference of the morphology is remarkable. One explanation for this difference may be the high-density gaseous plasma and the joule heating in the tree channels.<<ETX>>\",\"PeriodicalId\":10719,\"journal\":{\"name\":\"Conference on Electrical Insulation and Dielectric Phenomena,\",\"volume\":\"43 1\",\"pages\":\"259-264\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1989-10-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Conference on Electrical Insulation and Dielectric Phenomena,\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CEIDP.1989.69556\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Conference on Electrical Insulation and Dielectric Phenomena,","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CEIDP.1989.69556","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Impulse treeing breakdown in polyethylene under non-uniform and quasi-uniform fields
The polarity effect of the impulse tree inception and complete breakdown (puncture) of low-density polyethylene is described as a function of the radius of the needle tip. Furthermore, the morphology of the impulse tree and breakdown channels is examined. It is shown that the puncture field strength E/sub b/ for both polarities is about 6 MV/cm at 500 mu m and is of the same order as the intrinsic breakdown strength of low-density polyethylene. The shapes of impulse tree and breakdown channels for both polarities are shown for varying tip radius and gap distance. Although the E/sub b/ obtained has almost the same value as the intrinsic breakdown strength at larger tip radii, it can be seen that the morphologies of the breakdown channels for the two polarities are different. Especially at larger tip radii, the difference of the morphology is remarkable. One explanation for this difference may be the high-density gaseous plasma and the joule heating in the tree channels.<>