利用EUHFORIA探测日冕物质抛射的倾角效应

Karmen Martinić, Eleanna Asvestari, Mateja Dumbović, Tobias Rindlisbacher, Manuela Temmer, Bojan Vršnak
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摘要

日冕物质抛射(CMEs)是一种复杂的磁化等离子体结构,其中的磁场围绕中心轴旋转,形成所谓的磁通绳(FR)。通量绳的中心轴可以与南北半球成任意角度。在整个飞行过程中,CME 会遇到行星际磁场和太阳风,它们既不是同质的,也不是各向同性的。因此,不同方向的 CME 将遇到不同的环境介质条件,因此,CME 与周围环境的相互作用将因其 FR 轴的方向等因素而异。我们使用 EUHFORIA 三维磁流体动力学模型进行了模拟。这项研究的重点是两个被模拟成球泡的 CME,它们的特性几乎完全相同,只是倾角不同。我们通过分析散布在内日球层的 81 个虚拟航天器群的模型数据,展示了 CME 方向对鞘演化、MHD 阻力和非径向流的影响。我们发现,鞘的持续时间随距离太阳的径向距离增加而增加,而且在 CME 的侧翼增加的速度更大。所研究的鞘区内的非径向流在黄道面外显得更大,表明IMF在黄道面外 "滑动"。我们发现,计算出的阻力参数并不与径向距离保持恒定,我们的数值设置无法解决阻力参数的倾角依赖性问题。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Probing coronal mass ejections inclination effects with EUHFORIA
Coronal mass ejections (CMEs) are complex magnetized plasma structures in which the magnetic field spirals around a central axis, forming what is known as a flux rope (FR). The central FR axis can be oriented at any angle to the ecliptic. Throughout its journey, a CME will encounter interplanetary magnetic field and solar wind which are neither homogeneous nor isotropic. Consequently, CMEs with different orientations will encounter different ambient medium conditions and, thus, the interaction of a CME with its surrounding environment will vary depending on the orientation of its FR axis, among other factors. This study aims to understand the effect of inclination on CME propagation. We performed simulations with the EUHFORIA 3D magnetohydrodynamic model. This study focuses on two CMEs modelled as spheromaks with nearly identical properties, differing only by their inclination. We show the effects of CME orientation on sheath evolution, MHD drag, and non-radial flows by analyzing the model data from a swarm of 81 virtual spacecraft scattered across the inner heliospheric. We have found that the sheath duration increases with radial distance from the Sun and that the rate of increase is greater on the flanks of the CME. Non-radial flows within the studied sheath region appear larger outside the ecliptic plane, indicating a "sliding" of the IMF in the out-of ecliptic plane. We found that the calculated drag parameter does not remain constant with radial distance and that the inclination dependence of the drag parameter can not be resolved with our numerical setup.
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