M. Nakamura, T. Cho, S. Kubo, T. Shimozuma, H. Kawai, Y. Yamazaki, T. Maekawa, Y. Terumichi, Shigetoshi Tanaka, Y. Hamada
{"title":"TOROIDAL PLASMA CURRENT SUSTAINMENT BY LOWER HYBRID WAVES IN THE WT-2 TOKAMAK","authors":"M. Nakamura, T. Cho, S. Kubo, T. Shimozuma, H. Kawai, Y. Yamazaki, T. Maekawa, Y. Terumichi, Shigetoshi Tanaka, Y. Hamada","doi":"10.1103/PHYSREVLETT.47.1902","DOIUrl":null,"url":null,"abstract":"By injecting rf power P/sub rf/ near the lower hybrid frequency into an Ohmically heated plasma near the end of tokamak discharge in the WT-2, an rf-driven current-sustained plasma is produced and continues to exist during the rf injection period, the toroidal current (I/sub p/approx.10 kA) being generated by the lower hybrid wave only without the Ohmic power. The efficiency of rf-driven current generation is high and attains I/sub p//P/sub rf/roughly-equal0.9 kA/kW at the plasma density n/sub e/approx. =1.4 x 10/sup 12/ cm/sup -3/, with somewhat lower efficiency at higher density.","PeriodicalId":22276,"journal":{"name":"The annual research report","volume":"56 1","pages":"1-14"},"PeriodicalIF":0.0000,"publicationDate":"1981-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"54","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The annual research report","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1103/PHYSREVLETT.47.1902","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 54
Abstract
By injecting rf power P/sub rf/ near the lower hybrid frequency into an Ohmically heated plasma near the end of tokamak discharge in the WT-2, an rf-driven current-sustained plasma is produced and continues to exist during the rf injection period, the toroidal current (I/sub p/approx.10 kA) being generated by the lower hybrid wave only without the Ohmic power. The efficiency of rf-driven current generation is high and attains I/sub p//P/sub rf/roughly-equal0.9 kA/kW at the plasma density n/sub e/approx. =1.4 x 10/sup 12/ cm/sup -3/, with somewhat lower efficiency at higher density.