@article{oai:nifs-repository.repo.nii.ac.jp:00000604,
 author = {IDA,  Katsumi and CHS Group, and the CHS Group, and the LHD Group , and LHD Group, and JFT-2M, Group and IDA,  Katsumi and CHS, Group and LHD, Group and JFT-2M, Group},
 journal = {Journal of Plasma and Fusion Research SERIES},
 month = {Jan},
 note = {The structure of the radial electric field and toroidal/poloidal flow is discussed for the high temperature plasma in torodidal systems, tokamak and Heliotron type magnetic configurations. The spontaneous toroidal and poloidal flows are observed in the plasma with improved confinement. The radial electric field is mainly determined by the poloidal flow, because the contribution of toroidal flow to the radial electric field is small. The jump of radial electric field and poloidal flow are commonly observed near the plasma edge in the so-called high confinement mode (H-mode) plasmas in tokamaks and electron root plasma in stellarators including Heliotrons. In general the toroidal flow is driven by the momentum input from neutral beam injected toroidally. There is toroidal flow not driven by neutral beam in the plasma and it will be more significant in the plasma with large electric field. The direction of these spontaneous toroidal flows depends on the symmetry of magnetic field. The spontaneous toroidal flow driven by the ion temperature gradient is in the direction to increase the negative radial electric field in tokamak. The direction of spontaneous toroidal flow in Heliotron plasmas is opposite to that in tokamak plasmas because of the helicity of symmetry of the magnetic field configuration.},
 pages = {36--42},
 title = {Structure of the radial electric field and toroidal/poloidal flow in high temperature toroidal plasma},
 volume = {4},
 year = {2001}
}