Calculation of the Initial Magnetic Field for Mercury’s Magnetosphere Hybrid Model
- Authors: Alexeev I.1, Parunakian D.1, Dyadechkin S.2,3, Belenkaya E.1, Khodachenko M.1,2, Kallio E.3, Alho M.3
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Affiliations:
- Moscow State University Skobeltsyn Institute of Nuclear Physics
- Space Research Institute of the Austrian Academy of Sciences
- Aalto University
- Issue: Vol 56, No 2 (2018)
- Pages: 108-114
- Section: Article
- URL: https://journals.rcsi.science/0010-9525/article/view/153431
- DOI: https://doi.org/10.1134/S0010952518020028
- ID: 153431
Cite item
Abstract
Several types of numerical models are used to analyze the interactions of the solar wind flow with Mercury’s magnetosphere, including kinetic models that determine magnetic and electric fields based on the spatial distribution of charges and currents, magnetohydrodynamic models that describe plasma as a conductive liquid, and hybrid models that describe ions kinetically in collisionless mode and represent electrons as a massless neutralizing liquid. The structure of resulting solutions is determined not only by the chosen set of equations that govern the behavior of plasma, but also by the initial and boundary conditions; i.e., their effects are not limited to the amount of computational work required to achieve a quasi-stationary solution. In this work, we have proposed using the magnetic field computed by the paraboloid model of Mercury’s magnetosphere as the initial condition for subsequent hybrid modeling. The results of the model have been compared to measurements performed by the Messenger spacecraft during a single crossing of the magnetosheath and the magnetosphere. The selected orbit lies in the terminator plane, which allows us to observe two crossings of the bow shock and the magnetopause. In our calculations, we have defined the initial parameters of the global magnetospheric current systems in a way that allows us to minimize paraboloid magnetic field deviation along the trajectory of the Messenger from the experimental data. We have shown that the optimal initial field parameters include setting the penetration of a partial interplanetary magnetic field into the magnetosphere with a penetration coefficient of 0.2.
About the authors
Igor Alexeev
Moscow State University Skobeltsyn Institute of Nuclear Physics
Author for correspondence.
Email: alexeev@dec1.sinp.msu.ru
Russian Federation, Moscow, 119234
David Parunakian
Moscow State University Skobeltsyn Institute of Nuclear Physics
Email: alexeev@dec1.sinp.msu.ru
Russian Federation, Moscow, 119234
Sergey Dyadechkin
Space Research Institute of the Austrian Academy of Sciences; Aalto University
Email: alexeev@dec1.sinp.msu.ru
Austria, Graz, 8042; Helsinki, 02150
Elena Belenkaya
Moscow State University Skobeltsyn Institute of Nuclear Physics
Email: alexeev@dec1.sinp.msu.ru
Russian Federation, Moscow, 119234
Maxim Khodachenko
Moscow State University Skobeltsyn Institute of Nuclear Physics; Space Research Institute of the Austrian Academy of Sciences
Email: alexeev@dec1.sinp.msu.ru
Russian Federation, Moscow, 119234; Graz, 8042
Esa Kallio
Aalto University
Email: alexeev@dec1.sinp.msu.ru
Finland, Helsinki, 02150
Markku Alho
Aalto University
Email: alexeev@dec1.sinp.msu.ru
Finland, Helsinki, 02150
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