{"title":"PPPS-2013:使用改良MHD模型的离子电流FRC","authors":"H. Rahman, M. Binderbauer, N. Rostoker, F. Wessel","doi":"10.1109/PLASMA.2013.6633295","DOIUrl":null,"url":null,"abstract":"Summary form only given. In the standard MHD formulation the effects of finite gyroradius and gyroperiod are usually absent. To include these effects we have modified MACH2, a 2D MHD code, and then simulated recent experiments performed at Tri Alpha Energy, Inc.1 and the University of CA, Irvine.2 In the experiments an azimuthal-electric field is produced by a flux coil that is co-axially located with the plasma.3 In the presence of a pre-formed, magnetized plasma the Eθ field induces a diamagnetic-plasma current that reverses the applied-magnetic field, forming a FRC. The simulations suggest that the azimuthal current is due initially to ion flow, until the FRC is formed, when the electrons are free to accelerate in the field-free region, near the magnetic-null. For the same set of initial parameters there is good agreement between the simulations and the experiments.","PeriodicalId":6313,"journal":{"name":"2013 Abstracts IEEE International Conference on Plasma Science (ICOPS)","volume":"65 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2013-06-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"PPPS-2013: Ion-current FRC using a modified MHD model\",\"authors\":\"H. Rahman, M. Binderbauer, N. Rostoker, F. Wessel\",\"doi\":\"10.1109/PLASMA.2013.6633295\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Summary form only given. In the standard MHD formulation the effects of finite gyroradius and gyroperiod are usually absent. To include these effects we have modified MACH2, a 2D MHD code, and then simulated recent experiments performed at Tri Alpha Energy, Inc.1 and the University of CA, Irvine.2 In the experiments an azimuthal-electric field is produced by a flux coil that is co-axially located with the plasma.3 In the presence of a pre-formed, magnetized plasma the Eθ field induces a diamagnetic-plasma current that reverses the applied-magnetic field, forming a FRC. The simulations suggest that the azimuthal current is due initially to ion flow, until the FRC is formed, when the electrons are free to accelerate in the field-free region, near the magnetic-null. For the same set of initial parameters there is good agreement between the simulations and the experiments.\",\"PeriodicalId\":6313,\"journal\":{\"name\":\"2013 Abstracts IEEE International Conference on Plasma Science (ICOPS)\",\"volume\":\"65 1\",\"pages\":\"1-1\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2013-06-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2013 Abstracts IEEE International Conference on Plasma Science (ICOPS)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PLASMA.2013.6633295\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2013 Abstracts IEEE International Conference on Plasma Science (ICOPS)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PLASMA.2013.6633295","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
PPPS-2013: Ion-current FRC using a modified MHD model
Summary form only given. In the standard MHD formulation the effects of finite gyroradius and gyroperiod are usually absent. To include these effects we have modified MACH2, a 2D MHD code, and then simulated recent experiments performed at Tri Alpha Energy, Inc.1 and the University of CA, Irvine.2 In the experiments an azimuthal-electric field is produced by a flux coil that is co-axially located with the plasma.3 In the presence of a pre-formed, magnetized plasma the Eθ field induces a diamagnetic-plasma current that reverses the applied-magnetic field, forming a FRC. The simulations suggest that the azimuthal current is due initially to ion flow, until the FRC is formed, when the electrons are free to accelerate in the field-free region, near the magnetic-null. For the same set of initial parameters there is good agreement between the simulations and the experiments.