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Equilibrium and stability studies of oblate field-reversed configurations in the Magnetic Reconnection Experiment

机译:磁重联实验中扁圆磁场反转构型的平衡和稳定性研究

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The equilibrium and stability of oblate field-reversed configurations (FRCs) have been studied in the Magnetic Reconnection Experiment [M. Yamada , Phys. Plasmas 4, 1936 (1997)]. In the absence of a passive stabilization, tilt and shift instabilities often become unstable, with the tilt in particular limiting the plasma lifetime. The tilt instability can be mitigated by either including a passive stabilizing conductor, or by forming very oblate plasmas. Large perturbations (n=2 and 3) may still remain after passive stabilization is applied. These perturbations have the characteristics of co-interchange modes, which have never been observed, and can lead to the early termination of the plasma. The co-interchange modes can be minimized through the formation of plasmas with a very oblate shape, leading to the maximum FRC lifetime. A code has been developed to calculate equilibria for these plasmas. A rigid-body model explains the improved stability of oblate plasmas to n=1 tilt modes. Numerical calculations indicate improved stability to n >= 2 co-interchange modes for the very oblate plasma shapes. (c) 2006 American Institute of Physics.
机译:在磁重联实验中已经研究了扁圆反向结构(FRC)的平衡和稳定性[M.山田物理Plasmas 4,1936(1997)]。在没有被动稳定的情况下,倾斜和移位不稳定性通常变得不稳定,尤其是倾斜限制了等离子体寿命。可以通过包括无源稳定导体或通过形成非常扁平的等离子体来减轻倾斜不稳定性。应用被动稳定后,仍然可能会出现较大的扰动(n = 2和3)。这些扰动具有从未被观察到的共交换模式的特征,并且可以导致等离子体的尽早终止。可以通过形成非常扁形的等离子体来最小化共交换模式,从而获得最大的FRC寿命。已经开发了用于计算这些血浆的平衡的代码。刚体模型解释了扁球形等离子体对n = 1倾斜模式的改进的稳定性。数值计算表明,对于非常扁平的等离子体形状,n> = 2互交换模式的稳定性得到了改善。 (c)2006年美国物理研究所。

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