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首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Magnetohydrodynamic simulation of the interactionbetween two interplanetary magnetic cloudsand its consequent geoeffectiveness:2. Oblique collision
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Magnetohydrodynamic simulation of the interactionbetween two interplanetary magnetic cloudsand its consequent geoeffectiveness:2. Oblique collision

机译:磁流体动力模拟的interactionbetween两行星际磁场cloudsand顺向geoeffectiveness: 2。斜碰撞

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The numerical studies of the interplanetary coupling between multiple magneticclouds (MCs) are continued by a 2.5-dimensional ideal magnetohydrodynamic(MHD) model in the heliospheric meridional plane. The interplanetary direct collision(DC)/oblique collision (OC) between both MCs results from their same/different initialpropagation orientations. Here the OC is explored in contrast to the results of the DC. Boththe slow MC1 and fast MC2 are consequently injected from the different heliosphericlatitudes to form a compound stream during the interplanetary propagation. The MC1 andMC2 undergo contrary deflections during the process of oblique collision. Theirdeflection angles of 16011 and 16021 continuously increase until both MC-driven shockfronts are merged into a stronger compound one. The Oil, 16021, and total deflection angleAO (AO = 16011 + 16021) reach their corresponding maxima when the initial eruptionsof both MCs are at an appropriate angular difference. Moreover, with the increase ofMC2's initial speed, the OC becomes more intense, and the enhancement of 691 ismuch more sensitive to 602. The 18011 is generally far less than the 16021, and the unusualcase of 16011 _^2 16021 only occurs for an extremely violent OC. But because of the elasticityof the MC body to buffer the collision, this deflection would gradually approach anasymptotic degree. As a result, the opposite deflection between the two MCs, togetherwith the inherent magnetic elasticity of each MC, could efficiently relieve the external'compression for the OC in the interplanetary space. Such a deflection effect for the OCcase is essentially absent for the DC case. Therefore, besides the magnetic elasticity,magnetic helicity, and reciprocal compression, the deflection due to the OC should beconsidered for the evolution and ensuing geoeffectiveness of interplanetary interactionamong successive coronal mass ejections.
机译:星际的数值研究之间的耦合多个magneticclouds (MCs)持续了2.5维理想磁流体动力(磁流体动力)模型日球子午面。直接碰撞(DC) /斜碰撞(OC)两国MCs的结果相同/不同initialpropagation取向。这里的OC与探索直流的结果。因此注射的不同heliosphericlatitudes形成复合流在星际传播。andMC2期间接受相反的变形量斜碰撞的过程。16011年和16021年的角度不断增加直到两个MC-driven shockfronts并入一个更强的化合物。总挠度angleAO (AO = 16011 + 16021)初始时达到相应的最大值eruptionsof MCs都在适当的角的差异。ofMC2的初始速度,OC变得更多强烈,增强691要更多敏感到602。比16021年和16011年的unusualcase _ ^ 216021年,只有发生极端暴力OC。但由于elasticityof MC的身体缓冲碰撞,这种偏转逐渐接近anasymptotic学位。因此,两者之间相反的偏转MCs,联合固有的磁性每个MC的弹性,能有效地缓解外部'compression的OC行星际空间。OCcase本质上是没有的的情况。弹性、磁螺度和互惠的压缩,挠度由于OC看作是进化和随之而来的geoeffectiveness星际的连续interactionamong日冕物质抛射。

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