{"title":"Heliotron E装置的ECE实验","authors":"Motoyasu Sato","doi":"10.1109/irmm.1983.9126341","DOIUrl":null,"url":null,"abstract":"Electron cyclotron heating experiments have been perfomed in Heliotron E device to produce and heat the high temperature plasma. Varian VGE 8G50 Gyratrons provide 300–400 kw, 53.2 GKz microwave to the vacuum chamber. The typical plasma parameters obtained are Tc =1.5 keV, ne = 1–3 × 10 cm−3. The heating rates are 6–10 eV/kw and 6–8 J/kw. These values are 1–2 times larger than that of tokamaks.","PeriodicalId":314918,"journal":{"name":"1983 Eighth International Conference on Infrared and Millimeter Waves","volume":"62 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1983-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"ECE experiments on Heliotron E device\",\"authors\":\"Motoyasu Sato\",\"doi\":\"10.1109/irmm.1983.9126341\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Electron cyclotron heating experiments have been perfomed in Heliotron E device to produce and heat the high temperature plasma. Varian VGE 8G50 Gyratrons provide 300–400 kw, 53.2 GKz microwave to the vacuum chamber. The typical plasma parameters obtained are Tc =1.5 keV, ne = 1–3 × 10 cm−3. The heating rates are 6–10 eV/kw and 6–8 J/kw. These values are 1–2 times larger than that of tokamaks.\",\"PeriodicalId\":314918,\"journal\":{\"name\":\"1983 Eighth International Conference on Infrared and Millimeter Waves\",\"volume\":\"62 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1983-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1983 Eighth International Conference on Infrared and Millimeter Waves\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/irmm.1983.9126341\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1983 Eighth International Conference on Infrared and Millimeter Waves","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/irmm.1983.9126341","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Electron cyclotron heating experiments have been perfomed in Heliotron E device to produce and heat the high temperature plasma. Varian VGE 8G50 Gyratrons provide 300–400 kw, 53.2 GKz microwave to the vacuum chamber. The typical plasma parameters obtained are Tc =1.5 keV, ne = 1–3 × 10 cm−3. The heating rates are 6–10 eV/kw and 6–8 J/kw. These values are 1–2 times larger than that of tokamaks.
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