可运行的从太阳到地球的全三维磁流体动力学模型:COCONUT+Icarus

T. Baratashvili, M. Brchnelova, L. Linan, A. Lani, S. Poedts
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引用次数: 0

摘要

由于现代社会日益依赖技术、导航和电力系统,太阳风建模已成为一个重要的研究领域。准确的空间天气预报可以预测地球地球空间即将面临的威胁,从而减轻对社会经济的有害影响。日冕和日光层模型必须尽可能逼真,才能实现成功预测。在本研究中,我们研究了从太阳到地球的新型全磁流体动力(MHD)链。本研究的目标是通过将完整的 MHD 日冕模型最终实施到 COolfluid COroNaUnsTructured(COCONUT)模型中,并将其与 MHD 日光层模型 Icarus 相耦合,展示从太阳到地球的完整 MHD 建模链的能力。由此产生的日冕模型与先前存在的多向性替代模型相比具有显著优势,因为它包含了更多的物理知识,并允许对双模风进行更真实的建模,这对日光层研究至关重要。特别是,我们研究了 MHD 方程中加热项的不同经验公式,以确定能够最精确地模拟现实太阳风配置的最佳公式。新的加热源项被应用到先前存在的多向性 COCONUT 模型的 MHD 方程中。应用了现实的比热比。在这项研究中,能量方程只考虑了热传导、辐射损失和近似日冕加热函数。研究了多种近似加热曲线,以了解对太阳风的影响。日冕模型的输出被用于建立三维 MHD 日光层模型 Icarus。选择太阳活动最小的情况作为完整 MHD 模型的第一个测试案例。日冕和日光层的数值模拟数据与观测产品进行了比较。首先,我们将密度数据与太阳附近现有的层析成像数据进行了比较,然后将伊卡洛斯中模拟的太阳风时间序列与 1 AU 处的 OMNI 1 分钟数据进行了比较。在全 MHD 日冕模型中使用了一系列近似加热剖面,以获得逼真的太阳风配置。当引入取决于磁场的加热时,得到了日冕的双模太阳风。建模密度曲线与层析成像数据一致。日光层中的模拟风与观测结果基本一致。总体而言,密度被高估了,而 1 AU 处的风速与 OMNI 1 分钟数据比较接近。磁场成分的总体轮廓建模良好,但其大小被低估了。我们首次尝试利用 COCONUT 和 Icarus 获得从太阳到地球的完整 MHD 链。日冕模型已经升级为一个完整的 MHD 模型,用于现实的双模太阳风配置。近似的加热函数对风的模拟相当好,但简单的近似不足以获得真实的密度-速度平衡或低日冕和更远的外部边界附近的真实特征。完整的 MHD 模型在 Vlaams 超级计算中心 Genius 集群的 180 个内核上只用了 1.06 小时就完成了计算,这比多向模拟只用了 1.8 倍的时间。扩展模型提供了试验不同加热公式的机会,并改进了近似函数,从而更精确地模拟了真实的太阳风。
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The operationally ready full 3D magnetohydrodynamic model from the Sun to Earth: COCONUT+Icarus
Solar wind modelling has become a crucial area of study due to the increased dependence of modern society on technology, navigation, and power systems. Accurate space weather forecasts can predict upcoming threats to Earth's geospace and allow for harmful socioeconomic impacts to be mitigated. Coronal and heliospheric models must be as realistic as possible to achieve successful predictions. In this study, we examine a novel full magnetohydrodynamic (MHD) chain from the Sun to Earth. The goal of this study is to demonstrate the capabilities of the full MHD modelling chain from the Sun to Earth by finalising the implementation of the full MHD coronal model into the COolfluid COroNa UnsTructured (COCONUT) model and coupling it to the MHD heliospheric model Icarus. The resulting coronal model has significant advantages compared to the pre-existing polytropic alternative, as it includes more physics and allows for a more realistic modelling of bi-modal wind, which is crucial for heliospheric studies. In particular, we examine different empirical formulations for the heating terms in the MHD equations to determine an optimal one that would be able to mimic a realistic solar wind configuration most accurately. New heating source terms were implemented into the MHD equations of the pre-existing polytropic COCONUT model. A realistic specific heat ratio was applied. In this study, only thermal conduction, radiative losses, and approximated coronal heating function were considered in the energy equation. Multiple approximated heating profiles were examined to see the effect on the solar wind. The output of the coronal model was used to onset the 3D MHD heliospheric model Icarus. A minimum solar activity case was chosen as the first test case for the full MHD model. The numerically simulated data in the corona and the heliosphere were compared to observational products. First, we compared the density data to the available tomography data near the Sun and then the modelled solar wind time series in Icarus was compared to OMNI 1-min data at 1 AU. A range of approximated heating profiles were used in the full MHD coronal model to obtain a realistic solar wind configuration. The bi-modal solar wind was obtained for the corona when introducing heating that is dependent upon the magnetic field. The modelled density profiles are in agreement with the tomography data. The modelled wind in the heliosphere is in reasonable agreement with observations. Overall, the density is overestimated, whereas the speed at 1 AU is more similar to OMNI 1-min data. The general profile of the magnetic field components is modelled well, but its magnitude is underestimated. We present a first attempt to obtain the full MHD chain from the Sun to Earth with COCONUT and Icarus. The coronal model has been upgraded to a full MHD model for a realistic bi-modal solar wind configuration. The approximated heating functions have modelled the wind reasonably well, but simple approximations are not enough to obtain a realistic density-speed balance or realistic features in the low corona and farther, near the outer boundary. The full MHD model was computed in 1.06 h on 180 cores of the Genius cluster of the Vlaams Supercomputing Center, which is only 1.8 times longer than the polytropic simulation. The extended model gives the opportunity to experiment with different heating formulations and improves the approximated function to model the real solar wind more accurately.
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