{"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}
引用次数: 0
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.