H. P. Wang, S. Poedts, A. Lani, M. Brchnelova, T. Baratashvili, L. Linan, F. Zhang, D. W. Hou, Y. H. Zhou
{"title":"基于 COCONUT 的高效、随时间演变的全球 MHD 日冕模型","authors":"H. P. Wang, S. Poedts, A. Lani, M. Brchnelova, T. Baratashvili, L. Linan, F. Zhang, D. W. Hou, Y. H. Zhou","doi":"arxiv-2409.02043","DOIUrl":null,"url":null,"abstract":"MHD coronal models are critical in the Sun-to-Earth model chain and the most\ncomplex and computationally intensive component, particularly the time-evolving\ncoronal models, typically driven by a series of time-evolving photospheric\nmagnetograms. There is an urgent need to develop efficient and reliable\ntime-evolving MHD coronal models to further improve our ability to predict\nspace weather. COCONUT is a rapidly developing MHD coronal model. Adopting the\nefficient implicit algorithm makes it suitable for performing computationally\nintensive time-evolving coronal simulations. This paper aims to extend COCONUT\nto an efficient time-evolving MHD coronal model. In this MHD model, as usual,\nan implicit temporal integration algorithm is adopted to avoid the CFL\nstability restriction and increase computational efficiency by large time\nsteps. The Newton iteration method is applied within each time step to enhance\nthe temporal accuracy. The unstructured geodesic mesh is used for flexibility\nin mesh division and to avoid degeneracy at the poles. Furthermore, an HLL\nRiemann solver with a self-adjustable dissipation term accommodates both low-\nand high-speed flows. A series of time-evolving photospheric magnetograms are\nutilized to drive the evolution of coronal structures from the solar surface to\n25Rs during two Carrington rotations (CRs) around the 2019 eclipse in an\ninertial coordinate system. It shows that COCONUT can mimic the coronal\nevolution during a full CR within 9 hours (1080 CPU cores, 1.5M cells). We also\ncompare the simulation results of time-evolving versus quasi-steady-state\ncoronal simulations in the thermodynamic MHD model to validate the\ntime-evolving approach. Additionally, we evaluate the effect of time steps on\nthe simulation results to find an optimal time step that simultaneously\nmaintains high efficiency and necessary numerical stability and accuracy.","PeriodicalId":501423,"journal":{"name":"arXiv - PHYS - Space Physics","volume":"8 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"An efficient, time-evolving, global MHD coronal model based on COCONUT\",\"authors\":\"H. P. Wang, S. Poedts, A. Lani, M. Brchnelova, T. Baratashvili, L. Linan, F. Zhang, D. W. Hou, Y. H. Zhou\",\"doi\":\"arxiv-2409.02043\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"MHD coronal models are critical in the Sun-to-Earth model chain and the most\\ncomplex and computationally intensive component, particularly the time-evolving\\ncoronal models, typically driven by a series of time-evolving photospheric\\nmagnetograms. There is an urgent need to develop efficient and reliable\\ntime-evolving MHD coronal models to further improve our ability to predict\\nspace weather. COCONUT is a rapidly developing MHD coronal model. Adopting the\\nefficient implicit algorithm makes it suitable for performing computationally\\nintensive time-evolving coronal simulations. This paper aims to extend COCONUT\\nto an efficient time-evolving MHD coronal model. In this MHD model, as usual,\\nan implicit temporal integration algorithm is adopted to avoid the CFL\\nstability restriction and increase computational efficiency by large time\\nsteps. The Newton iteration method is applied within each time step to enhance\\nthe temporal accuracy. The unstructured geodesic mesh is used for flexibility\\nin mesh division and to avoid degeneracy at the poles. Furthermore, an HLL\\nRiemann solver with a self-adjustable dissipation term accommodates both low-\\nand high-speed flows. A series of time-evolving photospheric magnetograms are\\nutilized to drive the evolution of coronal structures from the solar surface to\\n25Rs during two Carrington rotations (CRs) around the 2019 eclipse in an\\ninertial coordinate system. It shows that COCONUT can mimic the coronal\\nevolution during a full CR within 9 hours (1080 CPU cores, 1.5M cells). We also\\ncompare the simulation results of time-evolving versus quasi-steady-state\\ncoronal simulations in the thermodynamic MHD model to validate the\\ntime-evolving approach. Additionally, we evaluate the effect of time steps on\\nthe simulation results to find an optimal time step that simultaneously\\nmaintains high efficiency and necessary numerical stability and accuracy.\",\"PeriodicalId\":501423,\"journal\":{\"name\":\"arXiv - PHYS - Space Physics\",\"volume\":\"8 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-03\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Space Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.02043\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Space Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.02043","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
An efficient, time-evolving, global MHD coronal model based on COCONUT
MHD coronal models are critical in the Sun-to-Earth model chain and the most
complex and computationally intensive component, particularly the time-evolving
coronal models, typically driven by a series of time-evolving photospheric
magnetograms. There is an urgent need to develop efficient and reliable
time-evolving MHD coronal models to further improve our ability to predict
space weather. COCONUT is a rapidly developing MHD coronal model. Adopting the
efficient implicit algorithm makes it suitable for performing computationally
intensive time-evolving coronal simulations. This paper aims to extend COCONUT
to an efficient time-evolving MHD coronal model. In this MHD model, as usual,
an implicit temporal integration algorithm is adopted to avoid the CFL
stability restriction and increase computational efficiency by large time
steps. The Newton iteration method is applied within each time step to enhance
the temporal accuracy. The unstructured geodesic mesh is used for flexibility
in mesh division and to avoid degeneracy at the poles. Furthermore, an HLL
Riemann solver with a self-adjustable dissipation term accommodates both low-
and high-speed flows. A series of time-evolving photospheric magnetograms are
utilized to drive the evolution of coronal structures from the solar surface to
25Rs during two Carrington rotations (CRs) around the 2019 eclipse in an
inertial coordinate system. It shows that COCONUT can mimic the coronal
evolution during a full CR within 9 hours (1080 CPU cores, 1.5M cells). We also
compare the simulation results of time-evolving versus quasi-steady-state
coronal simulations in the thermodynamic MHD model to validate the
time-evolving approach. Additionally, we evaluate the effect of time steps on
the simulation results to find an optimal time step that simultaneously
maintains high efficiency and necessary numerical stability and accuracy.