Abstract
以Harris Sheet作为初始条件, 使用数值模拟的方法, 研究了二级磁岛不稳定重联的一些性质. 在模拟中随着初始扰动的加入, Harris Sheet将演化到非线性阶段, 形成更薄的有剪切速度的电流片, 并伴有一级磁岛产生. 当Lundquist数大于或等于10<sup>5</sup>时, 非均匀剪切速度的Sweet-Parker电流片开始不稳定, 并有二级磁岛出现. 不稳定Sweet-Parker电流片对应的临界长宽比为65. Lundquist数越大, 演化形成的Sweet-Parker电流片越薄, 更多的二级磁岛将出现, 且沿电流片两边向外喷出, 随时间变大, 相互合并. 二级磁岛的出现使重联率增大, 并与Lundquist数之间不再满足S<sup>-1/2</sup>的关系, 而似乎对它的依赖关系不明显.
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