中国物理B ›› 2004, Vol. 13 ›› Issue (9): 1510-1515.doi: 10.1088/1009-1963/13/9/025

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Study of particle behaviour at the edge in HT-7 tokamak

万宝年1, 周倩1, 吴振伟1, 毛剑珊1, 李建刚1, 徐伟2   

  1. (1)Institute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, China; (2)Institute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, China; Department of Physics, Guangzhou University, Guangzhou 510405, China
  • 收稿日期:2003-08-24 修回日期:2004-04-26 出版日期:2004-06-21 发布日期:2005-06-21
  • 基金资助:
    Project supported by the National Natural Science Foundation of China (Grant Nos 19775013 and 10275014).

Study of particle behaviour at the edge in HT-7 tokamak

Xu Wei (徐伟)ab, Wan Bao-Nian (万宝年)a, Zhou Qian (周倩)a, Wu Zhen-Wei (吴振伟)a, Mao Jiao-Shan (毛剑珊)a, Li Jian-Gang (李建刚)a   

  1. a Institute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, China; b Department of Physics, Guangzhou University, Guangzhou 510405, China
  • Received:2003-08-24 Revised:2004-04-26 Online:2004-06-21 Published:2005-06-21
  • Supported by:
    Project supported by the National Natural Science Foundation of China (Grant Nos 19775013 and 10275014).

摘要: The cross-field diffusion coefficient (D_⊥) at the edge in the HT-7 tokamak is close to the Bohm value when the line average electron density ranges from 1.5×10^{19} to 3.0×10^{19}m^{-3}. The energy profile of the particles is derived directly from the H_α(D_α) line shape; the dissociative excitation of molecules is dominating when the local electron temperature is above 10eV. By means of the Monte Carlo method the D_α line shape is also simulated. We find that the molecular dissociation contributes to 57% of neutral atoms and 53% of emission intensity in front of the limiter, and 85% of neutral atoms and 82% of emission intensity in front of the wall. The influence of atomic and molecular processes on the energy balance is discussed for the scrape-off layer (SOL), and the power loss from molecular dissociation is found to be 6×10^4kW at the SOL. The ion Bernstein wave (IBW) can effectively suppress the magnetohydrodynamic behaviour, the fluctuation levels and the turbulence; the D_⊥ in front of the limiter declines from 0.84 to 0.2m^2·s^{-1} and the particle confinement time rises from 9 to 12ms.

关键词: plasma, diffusion coefficients, energy profile, atomic and molecular processes, simulation of D_α line shape

Abstract: The cross-field diffusion coefficient (D) at the edge in the HT-7 tokamak is close to the Bohm value when the line average electron density ranges from $1.5\times10^{19}$ to $3.0\times10^{19}$m$^{-3}$. The energy profile of the particles is derived directly from the $H_{\alpha}(D_{\alpha}$) line shape; the dissociative excitation of molecules is dominating when the local electron temperature is above 10eV. By means of the Monte Carlo method the $D_{\alpha}$ line shape is also simulated. We find that the molecular dissociation contributes to 57% of neutral atoms and 53% of emission intensity in front of the limiter, and 85% of neutral atoms and 82% of emission intensity in front of the wall. The influence of atomic and molecular processes on the energy balance is discussed for the scrape-off layer (SOL), and the power loss from molecular dissociation is found to be $6\times10^4$kW at the SOL. The ion Bernstein wave (IBW) can effectively suppress the magnetohydrodynamic behaviour, the fluctuation levels and the turbulence; the D in front of the limiter declines from 0.84 to 0.2m$^2$$\cdot$s$^{-1}$ and the particle confinement time rises from 9 to 12ms.

Key words: plasma, diffusion coefficients, energy profile, atomic and molecular processes, simulation of $D_{\alpha}$ line shape

中图分类号:  (Tokamaks, spherical tokamaks)

  • 52.55.Fa
52.35.Ra (Plasma turbulence) 52.25.Fi (Transport properties) 52.40.Hf (Plasma-material interactions; boundary layer effects) 52.30.Cv (Magnetohydrodynamics (including electron magnetohydrodynamics)) 52.25.Gj (Fluctuation and chaos phenomena) 52.25.Tx (Emission, absorption, and scattering of particles) 52.65.Pp (Monte Carlo methods) 52.65.Kj (Magnetohydrodynamic and fluid equation) 52.35.Hr (Electromagnetic waves (e.g., electron-cyclotron, Whistler, Bernstein, upper hybrid, lower hybrid))