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Alfven eigenmode stabillty and fast particle transport in JET

机译:JET中的Alfven本征模态稳定和快速粒子传输

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A hybrid magnetohydrodynamic-gyrokinetic model based on a Lagrangian formalism for the particle motion was developed for the stability analysis of global Alfven eigenmodes (AE) in the presence of energetic ions. A weak turbulence description was applied to the evolution of the unstable AE amplitudes and alpha particle redistribution and loss. It is found that finite orbit effects of very energetic ions reduce the instability drive by the alpha particles in JET, where the most unstable AE's have toroidal mode numbers between n = 4 to n = 10. Non-linear simulations show that wave saturation amplitude, proportional to the linear growth rate square, is delta B/B < 10~(-4) for the most un-stable JET scenarios. Therefore, no significant alpha particle redistribution is expected. Detailed simulations of JET DT experiments shows that the most unstable conditions occur in power switich off experiments. In this scenario the strong damping provided by the bulk and beam ions decreases faster than the drive provided by the slowing down alpha particles.
机译:建立了基于拉格朗日形式主义的粒子运动的混合磁流体动力学动力学模型,用于在高能离子存在下对整体Alfven本征模式(AE)进行稳定性分析。弱湍流描述应用于不稳定的AE振幅的演变以及α粒子的重新分布和损失。发现高能离子的有限轨道效应会降低JET中α粒子的不稳定性驱动,其中最不稳定的AE的环形模数在n = 4到n = 10之间。非线性模拟表明,波的饱和幅度,对于最不稳定的JET情景,与线性增长率平方成正比的是B / B <10〜(-4)。因此,预计不会出现明显的alpha粒子重新分布。 JET DT实验的详细模拟表明,最不稳定的条件发生在电源开关实验中。在这种情况下,由体离子和束离子提供的强阻尼比由减速的α粒子提供的驱动力下降得更快。

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