首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Open Geospace General Circulation Model simulation of a substorm: Axial tail instability and ballooning mode preceding substorm onset
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Open Geospace General Circulation Model simulation of a substorm: Axial tail instability and ballooning mode preceding substorm onset

机译:亚暴的开放地理空间一般环流模型模拟:亚暴爆发前的轴向尾部不稳定性和膨胀模式

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Recent global simulations of substorms show that before the onset of near-Earth reconnection the pressure equilibrium in the tail breaks down. This instability has no cross-tail variation and is thus not a ballooning mode, and it is also distinct from the tearing mode. Here, we analyze an Open Geospace General Circulation Model simulation run of the 23 March 2007 substorm and find the same instability. Because this mode has no significant cross-tail variation associated with it we call it the KYO mode. Besides the KYO mode we also find the classical ballooning mode in the simulation. It has a wavelength of –0.5 RE and is marginally, but sufficiently, resolved as shown by a higher-resolution control run. These results suggest a new scenario for the substorm expansion phase onset. During the growth phase magnetic flux is added to the lobes and the plasma sheet thins but remains in equilibrium. When force balance is no longer possible the KYO instability grows and accelerates plasma tailward. The divergence of the resulting tailward flow reduces the normal magnetic field and thereby makes the current sheet tearing unstable. The tearing mode grows right out of the KYO mode. The classical ballooning mode grows at the same time and is superimposed on the KYO mode, but its role in initiating reconnection is still unclear. The growth time of the KYO mode, ~2min, is both consistent with the notion of an explosive growth phase and with recent ground-based observation of the initial growth of auroral arcs before auroral breakup.
机译:最近的全球亚暴模拟显示,在近地重新连接开始之前,尾巴中的压力平衡就破裂了。该不稳定性没有交叉尾部变化,因此不是膨胀模式,并且也与撕裂模式不同。在这里,我们分析了2007年3月23日亚暴的开放地理空间一般环流模型模拟运行,并发现了相同的不稳定性。由于此模式没有明显的交叉尾部变化,因此我们将其称为KYO模式。除了KYO模式,我们还在仿真中找到了经典的气球模式。它具有–0.5 RE的波长,并且如高分辨率控制运行所示,已被分辨得很少,但是足够了。这些结果为亚暴扩张阶段的开始提出了新的设想。在生长阶段,磁通量被添加到叶片,等离子片变薄,但保持平衡。当不再可能达到力平衡时,KYO不稳定会增加并加速等离子体向后移动。产生的向后流动的发散会减小法向磁场,从而使当前的纸张撕裂不稳定。撕裂模式从KYO模式开始发展。经典膨胀模式会同时增长,并叠加在KYO模式上,但它在启动重新连接中的作用仍不清楚。 KYO模式的生长时间约为2分钟,既与爆炸性生长阶段的概念相一致,也与近期在极光破裂前对极光弧的初始生长的地面观测相一致。

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