{"title":"液体介质中的空间电荷","authors":"Z. Croitoru, M. Colombeau, R. Coelho","doi":"10.1109/CEI.1961.7473169","DOIUrl":null,"url":null,"abstract":"The field distribution in \"technical\" chlorobenzene between parallel electrodes, and its dynamics after application of the voltage have been studied by means of the electrooptic Kerr effect. Figure 1 represents the optical set up, composed of a light source 1 (mercury lamp or sliding spark), a vertical slit 2, in the focal plane of a collimator 3, an interference filter 4 followed by a polarizer 5 oriented at 45°, the Kerr cell 6, a quarter-wave plate a rotary power compensator 8, an analyzer 9 and finally a photosensitive surface 10.","PeriodicalId":8239,"journal":{"name":"Annual Report 1961 Conference on Electrical Insulation","volume":"3 1","pages":"21-24"},"PeriodicalIF":0.0000,"publicationDate":"1961-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"Space charges in liquid dielectrics\",\"authors\":\"Z. Croitoru, M. Colombeau, R. Coelho\",\"doi\":\"10.1109/CEI.1961.7473169\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The field distribution in \\\"technical\\\" chlorobenzene between parallel electrodes, and its dynamics after application of the voltage have been studied by means of the electrooptic Kerr effect. Figure 1 represents the optical set up, composed of a light source 1 (mercury lamp or sliding spark), a vertical slit 2, in the focal plane of a collimator 3, an interference filter 4 followed by a polarizer 5 oriented at 45°, the Kerr cell 6, a quarter-wave plate a rotary power compensator 8, an analyzer 9 and finally a photosensitive surface 10.\",\"PeriodicalId\":8239,\"journal\":{\"name\":\"Annual Report 1961 Conference on Electrical Insulation\",\"volume\":\"3 1\",\"pages\":\"21-24\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1961-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Annual Report 1961 Conference on Electrical Insulation\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CEI.1961.7473169\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Annual Report 1961 Conference on Electrical Insulation","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CEI.1961.7473169","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The field distribution in "technical" chlorobenzene between parallel electrodes, and its dynamics after application of the voltage have been studied by means of the electrooptic Kerr effect. Figure 1 represents the optical set up, composed of a light source 1 (mercury lamp or sliding spark), a vertical slit 2, in the focal plane of a collimator 3, an interference filter 4 followed by a polarizer 5 oriented at 45°, the Kerr cell 6, a quarter-wave plate a rotary power compensator 8, an analyzer 9 and finally a photosensitive surface 10.
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