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基于Hasegawa-Wakatani湍流模型,数值模拟了托卡马克边缘等离子体中漂移波湍流和相关的反常粒子输运.从等离子体动量守恒方程出发导出了不采用常规的布辛涅斯克近似的带状流方程,论证了大振幅密度扰动和湍性粒子流对激发带状流的贡献可等效地对应于低阶负粘滞阻尼效果.数值模拟表明,大振幅密度扰动的非线性大大增强了带状流饱和振幅,从而有效抑制了湍性粒子输运.研究结果阐明了托卡马克边缘等离子体大振幅密度扰动的非线性对驱动等离子体旋转、动量输运和带状流的重要性.     

Determination of q=1 surface by the variation of pellet ablation rate on the HL-1M

Strong drop of Hα emission has been observed on the HL-1M tokamak by means of a detector array while a pellet crosses the q=1 surface. In this article, the q=1 surface has been determined precisely by the interval and the shape of the Hα emission striations on the pellet trajectory due to the variation of pellet ablation rate. The q-profile and current density distribution at the plasma centre region have been calculated according to the pellet ablation rate and the magnetic shear feature.     

非圆截面环流器等离子体对于高n理想磁流体气球模的最佳压强分布

本文假定等离子体局部压强梯度由理想磁流体高n气球模所限定,讨论了非圆截面环流器的最佳压强剖面。分析了椭圆及三角变形的效应,发现三角变形对提高稳定性很有利;q剖面对平均比压值及中心比压值都有强烈影响,而沿半径下降的q剖面对提高比压值很有利。     

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介绍了在已知环形轴对称等离子体平衡位形的条件下,建立磁力线为直线的坐标系的方法。该坐标系被广泛应用于托卡马克等离子体的磁流体稳定性和动理论物理问题的理论分析,但文献中对坐标系建立方法却很少有介绍。结合几类托卡马克位形和球形环位形,对该类坐标系的特征进行了分析。     

等离子体理论——具有内部输运垒的托卡马克平衡位形关于高n理想磁流体气球模的稳定性

内部输运垒是一种与托卡马克等离子体的改善约束态相联系的现象。在内部输运垒所在区域，等离子体的压强梯度非常大而磁剪切极小，因此，接近内部输运垒的区域，剪切的绝对值很小。与这一现象相关的物理内容非常丰富，如磁流体稳定性问题，以及微观不稳定性（人们认为它们是产生反常输运的原因）的抑制问题等。关于小剪切条件下稳定性的处理方法本身也是一个难题.最近，Connor和Hastie（下面简称CH模型）重新研究了具有内部输运垒的等离子体的高n（环向模数）理想磁流体气球模的稳定性，     

几种典型轻杂质非日冕辐射的计算与分析

利用Hulse原子速率系数代码和简单的0维模型，计算了聚变实验装置中几种典型轻杂质的非日冕辐射特性的结果，并分析了它们辐射的特点。     

Stability of tokamak plasmas with internal transport barriers against high n ideal magnetohydrodynamic ballooning mode

A ballooning mode equation for tokamak plasma, with the toroidicity and the Shafranov shift effects included, is derived for a shift circular flux tokamak configuration. Using this equation, the stability of the plasma configuration with an internal transport barrier （ITB） against the high n （the toroidal mode number） ideal magnetohydrodynamic （MHD） ballooning mode is analysed. It is shown that both the toroidicity and the Shaftanov shift effects are stabilizing. In the ITB region, these effects give rise to a low shear stable channel between the first and the second stability regions. Out of the ITB region towards the plasma edge, the stabilizing effect of the Shaftanov shift causes the unstable zone to be significantly narrowed.