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Fluid magnetohydrodynamic stabilit in a heliotron with anisotropic fast particle species

机译:具有各向异性快粒子种类的日光加速器中的流体磁流体动力稳定器

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The local and global fluid magnetohydrodynamic stability properties of anisotropic pressure plasmas are investigated with the Kruskal-Oberman and rigid hot particle Johnson et al energy principles. A Heliotron configuration that models the Large Helical Device with finite pressure anisotropy driven by neutral beams at beta = 4% shows that the Kruskal-Oberman model predicts stability when beta(h)/beta similar to 1/3 provided that the hot particle pressure profile is sufficiently peaked. The rigid hot particle model, on the other hand, is stable to local and global modes for broad and peaked profiles. For central deposition, the marginal pressure profiles are somewhat broader for p(parallel to) > p(perpendicular to) than for p(perpendicular to)> p(parallel to). Global n = 3 modes produce stricter stability criteria than n = 1,2 and 4 modes. Off-axis hot particle deposition yields more unstable conditions with respect to global and local modes than on-axis deposition. The mode structures localize near the plasma periphery according to the Kruskal-Oberman model and near the plasma core according to the Johnson et al model. This observation could help resolve the appropriate model to apply to the experimental conditions in Heliotron devices.
机译:利用Kruskal-Oberman和刚性热粒子Johnson等人的能量原理研究了各向异性压力等离子体的局部和全局流体磁流体动力学稳定性。如果Heliotron配置通过由中性束在beta = 4%的驱动下具有有限压力各向异性的大型螺旋装置进行建模,则表明,当热粒子压力分布曲线的beta(h)/ beta与1/3相似时,Kruskal-Oberman模型可以预测稳定性已达到足够的峰值。另一方面,刚性热粒子模型对于局部和全局模式在宽广和峰值轮廓方面都是稳定的。对于中心沉积,p(平行于)> p(垂直于)的边际压力分布要比p(垂直于)> p(平行于)的边缘压力分布宽一些。全局n = 3模式产生比n = 1,2和4模式更严格的稳定性标准。离轴热粒子沉积在整体和局部模式方面比在轴沉积更不稳定。根据Kruskal-Oberman模型,模式结构位于等离子体外围附近,而根据Johnson等人模型,模式结构位于等离子体核心附近。该观察结果可以帮助解析适当的模型以应用于Heliotron设备的实验条件。

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