A. Chaly, I. N. Poluyanova, V. Yakovlev, K. K. Zabello, A. A. Logatchev, S. M. Shkolanik
{"title":"在一定电流水平范围内，电流为零后阳极表面温度的实验研究","authors":"A. Chaly, I. N. Poluyanova, V. Yakovlev, K. K. Zabello, A. A. Logatchev, S. M. Shkolanik","doi":"10.1109/DEIV.2016.7748737","DOIUrl":null,"url":null,"abstract":"The main reason of breakdown after kA arc extinction is considered to be the overheating of anode surface during arc burning. The aim of this work is to experimentally determine the anode surface temperature distribution just after current zero for the range of arc currents from successfully interrupted levels up to the levels of guaranteed failure. The measurements were done by a high-speed video camera Phantom M310 equipped by a Carl Zeiss 100/2 macro lens. The anode surface temperature distribution was obtained by comparison of the results of anode surface filming and the results of calibrated band-lamp filming in identical conditions. The measurements were done for SSS CuCr 70/30 AMF electrodes for the currents up to the interruption limit.","PeriodicalId":296641,"journal":{"name":"2016 27th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV)","volume":"108 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2016-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":"{\"title\":\"Experimental study of anode surface temperature after current zero for a range of current levels\",\"authors\":\"A. Chaly, I. N. Poluyanova, V. Yakovlev, K. K. Zabello, A. A. Logatchev, S. M. Shkolanik\",\"doi\":\"10.1109/DEIV.2016.7748737\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The main reason of breakdown after kA arc extinction is considered to be the overheating of anode surface during arc burning. The aim of this work is to experimentally determine the anode surface temperature distribution just after current zero for the range of arc currents from successfully interrupted levels up to the levels of guaranteed failure. The measurements were done by a high-speed video camera Phantom M310 equipped by a Carl Zeiss 100/2 macro lens. The anode surface temperature distribution was obtained by comparison of the results of anode surface filming and the results of calibrated band-lamp filming in identical conditions. The measurements were done for SSS CuCr 70/30 AMF electrodes for the currents up to the interruption limit.\",\"PeriodicalId\":296641,\"journal\":{\"name\":\"2016 27th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV)\",\"volume\":\"108 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2016-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"6\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2016 27th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/DEIV.2016.7748737\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2016 27th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DEIV.2016.7748737","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Experimental study of anode surface temperature after current zero for a range of current levels
The main reason of breakdown after kA arc extinction is considered to be the overheating of anode surface during arc burning. The aim of this work is to experimentally determine the anode surface temperature distribution just after current zero for the range of arc currents from successfully interrupted levels up to the levels of guaranteed failure. The measurements were done by a high-speed video camera Phantom M310 equipped by a Carl Zeiss 100/2 macro lens. The anode surface temperature distribution was obtained by comparison of the results of anode surface filming and the results of calibrated band-lamp filming in identical conditions. The measurements were done for SSS CuCr 70/30 AMF electrodes for the currents up to the interruption limit.
京公网安备 11010802042870号
京ICP备2023020795号-1
分享
求助内容：
应助结果提醒方式：
扫码关注我们
