Formation of Radial Electric Field and Toroidal Flow
H. Saitoh, Z. Yoshida, H. Himura, J. Morikawa1), M. Fukao1), and H. Wakabayashi
Graduate School of Frontier Sciences, University of Tokyo, Bunkyo-ku, Tokyo 113-8656 Japan
Recently, a new relaxation theory of plasmas including the effects of flow has been constructed [1]. In this equilibrium state, two fluid (electron-ion) plasmas are represented by Double Beltrami fields and it provides a condition for the flow velocity v and β value of the plasmas to satisfy β + ( v / vA )2/2 = const., where vA is Alfven velocity. It follows from this equation ultra-high β (possibly β > 1) state will be realized due to the effects of the dynamic pressure of plasmas, when the plasma has fast flow comparable to vA. In experimental search for the relaxed states of the flowing plasmas, normal-conducting (Proto-RT) or superconducting (Mini-RT) internal coil devices [2] have been constructed and fundamental researches are being carried out. When a radial electric field is generated in a poloidal magnetic field configuration of the internal conductor device, the expected E × B drift flow is induced in the toroidal direction of the plasmas.
References
[1] S. M. Mahajan and Z Yoshida, Phys. Rev. Lett. 81, 4863 (2002).
[2] Z. Yoshida and S. M. Mahajan, Phys. Rev. Lett. 88, 095001 (2002). [3] Z. Yoshida, Y. Ogawa, H. Himura et al., in Nonneutral Plasma Physics III, IV (AIP 1999, 2002).
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