{"title":"仿星器中托卡马克低模-高模跃迁理论的检验","authors":"K. Shaing","doi":"10.1063/1.860605","DOIUrl":null,"url":null,"abstract":"The tokamak L–H (low‐mode–high mode) transition theory can be tested in stellarators in a controlled manner by making use of the two or more local maxima in poloidal viscosity in these devices. Depending on the relative magnitudes of the toroidal and helical components of the magnetic‐field spectrum, the local maxima, and thus transition, can occur either at a critical poloidal E×B Mach number Mp of the order of unity, similar to that of a tokamak, or at an Mp of the order of ‖m−nq‖/m, similar to that of a helically symmetric torus. Here, E(B) is the electric (magnetic) field strength, m (n) is the poloidal (toroidal) mode number of the helical component of the ‖B‖ spectrum, and q is the safety factor. Possible limitations on the test due to the effects of the charge‐exchange momentum loss are discussed.","PeriodicalId":113346,"journal":{"name":"Physics of fluids. B, Plasma physics","volume":"25 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1993-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"47","resultStr":"{\"title\":\"Test of tokamak low‐mode–high‐mode transition theory in stellarators\",\"authors\":\"K. Shaing\",\"doi\":\"10.1063/1.860605\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The tokamak L–H (low‐mode–high mode) transition theory can be tested in stellarators in a controlled manner by making use of the two or more local maxima in poloidal viscosity in these devices. Depending on the relative magnitudes of the toroidal and helical components of the magnetic‐field spectrum, the local maxima, and thus transition, can occur either at a critical poloidal E×B Mach number Mp of the order of unity, similar to that of a tokamak, or at an Mp of the order of ‖m−nq‖/m, similar to that of a helically symmetric torus. Here, E(B) is the electric (magnetic) field strength, m (n) is the poloidal (toroidal) mode number of the helical component of the ‖B‖ spectrum, and q is the safety factor. Possible limitations on the test due to the effects of the charge‐exchange momentum loss are discussed.\",\"PeriodicalId\":113346,\"journal\":{\"name\":\"Physics of fluids. B, Plasma physics\",\"volume\":\"25 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1993-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"47\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physics of fluids. B, Plasma physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.860605\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physics of fluids. B, Plasma physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.860605","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Test of tokamak low‐mode–high‐mode transition theory in stellarators
The tokamak L–H (low‐mode–high mode) transition theory can be tested in stellarators in a controlled manner by making use of the two or more local maxima in poloidal viscosity in these devices. Depending on the relative magnitudes of the toroidal and helical components of the magnetic‐field spectrum, the local maxima, and thus transition, can occur either at a critical poloidal E×B Mach number Mp of the order of unity, similar to that of a tokamak, or at an Mp of the order of ‖m−nq‖/m, similar to that of a helically symmetric torus. Here, E(B) is the electric (magnetic) field strength, m (n) is the poloidal (toroidal) mode number of the helical component of the ‖B‖ spectrum, and q is the safety factor. Possible limitations on the test due to the effects of the charge‐exchange momentum loss are discussed.