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Beta limits for the N=1 mode in rotating-toroidal-resistive plasmas surrounded by a resistive wall

机译:被电阻壁包围的旋转环形电阻等离子体中N = 1模式的Beta极限

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The stability analysis of a high-beta toroidal tokamak plasma is carried out in the presence of toroidal flow, finite plasma resistivity, and a surrounding shell of finite electrical resistivity. The beta limits for the n=1 mode are set by the resistive-wall-tearing mode (RWTM), the ideal-wall-tearing mode (IWTM), and the ideal-plasma-resistive-wall mode (IPRWM). Slow plasma rotation suppresses the RWTM while the IPRWM is not directly affected by slow plasma flow. For small plasma resistivity, the IPRWM is stabilized by fast flow only. For large plasma resistivity, the IPRWM only exists in a plasma rotating faster than the typical tearing mode growth rate, and its instability threshold is a complicated function of the wall position and rotation frequency. Very fast rotation can destabilize the ideal kink through centrifugal effects. Furthermore, for b/a (wall radius/plasma radius) below a critical value, a stationary plasma is stable to the n=1 ideal kink and tearing mode for large values of beta. (C) 1998 American Institute of Physics. [S1070-664X(98)00210-9]. [References: 22]
机译:在存在环形流动,有限的等离子体电阻率和有限电阻率的周围壳体的情况下,对高β环形托卡马克等离子体进行了稳定性分析。 n = 1模式的beta限制由电阻壁撕裂模式(RWTM),理想壁撕裂模式(IWTM)和理想等离子体电阻壁模式(IPRWM)设置。缓慢的等离子体旋转抑制了RWTM,而IPRWM不受缓慢的等离子体流动的直接影响。对于较小的等离子体电阻率,仅通过快速流动来稳定IPRWM。对于较大的等离子体电阻率,IPRWM仅存在于旋转速度比典型撕裂模式增长率更快的等离子体中,并且其不稳定性阈值是壁位置和旋转频率的复杂函数。极快的旋转会通过离心作用破坏理想的扭结。此外,对于低于临界值的b / a(壁半径/等离子体半径),对于大的β值,固定的等离子体对n = 1理想的扭结和撕裂模式稳定。 (C)1998美国物理研究所。 [S1070-664X(98)00210-9]。 [参考:22]

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