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Microislands and transport in tokamaks

机译:托卡马克的小岛和运输

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Kadomtsev, proposed a self-generation mechanism of microislands (whose half-width is smaller than the Larmor radius of the ions) based on momentum and energy exchange between the electrostatic field of the islands and the ions of the background tokamak plasma. In this paper we study the motion of the ions intersecting, within a Larmor rotation. the electric field in the interspace between adjacent microisland chains. After appropriate average over the ensemble of ions and island chains, the interaction with the electric field gives rise to a net slow cumulative drift of the assembly of ions in the outward direction of the major radius. This effect is the consequence of nonlinearity and toroidal geometry in the equation of motion. The outward motion is associated with a decrease of the perpendicular plasma kinetic energy and a concomitant increase of the island's electrostatic energy. which can be described consistently by a 'pumping term' in the energy integral of the magnetohydrodynamic reduced equations for the islands. The, pumping term can be contrasted by anomalous dissipation due to resonant interaction between the background electrons and the island waves. A stationary system of self-sustained microisland chains can then be formed in the tokamak plasma preferentially in the region q > 2 of the safety factor. Thus, the plasma acquires a spongy structure, where the sponginess (that is to say,. the density of packing of the island structures) is measured by the ratio, lower than one, between the island width and the distance between adjacent rational surfaces. This Structure determines an electron heat conductivity, which is strictly related to the sponginess and to the macroscopic equilibrium. Examples of scalings of the electron confinement time, predicted in zero-dimensional approximation, are given for typical tokamak conditions.
机译:Kadomtsev根据岛上静电场与背景托卡马克等离子体的离子之间的动量和能量交换,提出了微岛的自生机制(半宽度小于离子的拉莫尔半径)。在本文中,我们研究了在拉莫尔旋转中相交的离子的运动。相邻微岛链之间的空间中的电场。在对离子和岛链的整体进行适当的平均后,与电场的相互作用会导致离子集合在主半径的向外方向上出现缓慢的净累积累积漂移。这种影响是运动方程中非线性和环形几何的结果。向外运动与垂直等离子体动能的降低以及岛的静电能的随之增加有关。可以用这些岛的磁流体动力学简化方程的能量积分中的“泵项”来一致地描述。泵浦项可以与背景电子与岛波之间的共振相互作用引起的异常耗散形成对比。然后可以在托卡马克血浆中优先在安全系数q> 2的区域中形成一个自持的微岛链固定系统。因此,等离子体获得海绵状结构,其中海绵状性(即,岛状结构的堆积密度)通过岛状宽度与相邻有理表面之间的距离之比小于1的比率来测量。这种结构决定了电子的热导率,这与海绵状性和宏观平衡密切相关。对于典型的托卡马克条件,给出了以零维近似预测的电子约束时间的缩放比例示例。

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