{"title":"材料性质(Ag、Cu、Al、W、C)对阴极电弧根特性的影响","authors":"M. Abbaoui, A. Lefort, S. Clain","doi":"10.1109/DEIV.2004.1418648","DOIUrl":null,"url":null,"abstract":"This paper describes a thermo physical phenomena analysis about a silver, copper, aluminium, iron, tungsten or graphite electrode submitted to a high density energy flux. The thermal flux necessary to create a cathode spot is about 1.10<sup>12</sup>Wm<sup>-2</sup>. For the studied metals and for values lower than 1.10<sup>12</sup> Wm<sup>-2</sup>, the liquid phase does not appears and the entire energy coming at the cathode surface diffuses in the electrode. For values upper than 5.10<sup>12</sup> Wm<sup>-2</sup> a large part of the energy is used for the vaporization and the electrode vaporized length depends of the material nature. The gap situated between the two extreme values 1.10<sup>11</> W m<sup>-2</sup> and 1.10<sup>13</sup> Wm<sup>-2</sup> corresponds to the cathode spot with liquid and vapour phases.","PeriodicalId":137370,"journal":{"name":"XXIst International Symposium on Discharges and Electrical Insulation in Vacuum, 2004. Proceedings. ISDEIV.","volume":"28 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2004-09-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Influence of the material nature (Ag, Cu, Al, W, C) on the arc root characteristics at the cathode\",\"authors\":\"M. Abbaoui, A. Lefort, S. Clain\",\"doi\":\"10.1109/DEIV.2004.1418648\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This paper describes a thermo physical phenomena analysis about a silver, copper, aluminium, iron, tungsten or graphite electrode submitted to a high density energy flux. The thermal flux necessary to create a cathode spot is about 1.10<sup>12</sup>Wm<sup>-2</sup>. For the studied metals and for values lower than 1.10<sup>12</sup> Wm<sup>-2</sup>, the liquid phase does not appears and the entire energy coming at the cathode surface diffuses in the electrode. For values upper than 5.10<sup>12</sup> Wm<sup>-2</sup> a large part of the energy is used for the vaporization and the electrode vaporized length depends of the material nature. The gap situated between the two extreme values 1.10<sup>11</> W m<sup>-2</sup> and 1.10<sup>13</sup> Wm<sup>-2</sup> corresponds to the cathode spot with liquid and vapour phases.\",\"PeriodicalId\":137370,\"journal\":{\"name\":\"XXIst International Symposium on Discharges and Electrical Insulation in Vacuum, 2004. Proceedings. ISDEIV.\",\"volume\":\"28 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2004-09-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"XXIst International Symposium on Discharges and Electrical Insulation in Vacuum, 2004. Proceedings. ISDEIV.\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/DEIV.2004.1418648\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"XXIst International Symposium on Discharges and Electrical Insulation in Vacuum, 2004. Proceedings. ISDEIV.","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DEIV.2004.1418648","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Influence of the material nature (Ag, Cu, Al, W, C) on the arc root characteristics at the cathode
This paper describes a thermo physical phenomena analysis about a silver, copper, aluminium, iron, tungsten or graphite electrode submitted to a high density energy flux. The thermal flux necessary to create a cathode spot is about 1.1012Wm-2. For the studied metals and for values lower than 1.1012 Wm-2, the liquid phase does not appears and the entire energy coming at the cathode surface diffuses in the electrode. For values upper than 5.1012 Wm-2 a large part of the energy is used for the vaporization and the electrode vaporized length depends of the material nature. The gap situated between the two extreme values 1.1011> W m-2 and 1.1013 Wm-2 corresponds to the cathode spot with liquid and vapour phases.