Table 1
Input parameters of the simulations.
Variable | Unit | Value | Description | |
---|---|---|---|---|
Normalisation | ||||
Density | n0 | Initial solar-wind density | ||
Magnetic field | B0 | Magnitude of the average solar-wind magnetic field | ||
Time | ![]() |
mpc / eB0 | Inverse of proton gyrofrequency | |
Speed | CA | ![]() | Alfvén speed | |
Length | di | CA/Ωci | Proton inertial length | |
Pressure | P0 | ![]() | Normalizing pressure | |
Solar-wind parameters | ||||
nsw | n0 | 1.0 | Solar-wind proton density | |
Bsw | B0 | ![]() | Solar-wind magnetic field vector | |
Usw | CA | (–10, 0, 0) | Solar-wind velocity vector in the planet’s reference frame | |
Ti/Te | – | 1.0 | Ratio of proton temperature to electron temperature | |
β = βi + βe | – | 1.0 | Solar wind plasma beta | |
Ye | – | d align="right">1.0 | Electron adiabatic index | |
Cs | CA | 1.4 | Solar-wind sound speed | |
Cms | CA | 1.7 | Solar-wind magnetosonic speed | |
MA | – | 10 | Bow shock Mach number | |
Turbulence | ||||
δB0/ B0 | – | 0.54 | Initial magnetic field fluctuations | |
δv0/CA | – | 0.54 | Initial velocity fluctuations | |
Magnetized planet | ||||
(XP, YP, Zp) | di | ![]() | Position of the planet’s centre in simulation box | |
τdip | – | (0, –1, 0) | Dipole moment direction | |
Dp | di | 200 | Distance to the magnetopause from the planet’s centre | |
Grid and numerics | ||||
∆X = ∆Y = ∆Z | di | 5.0 | Grid resolution | |
∆t | ![]() |
0.5 | Time resolution | |
Lbox = LX = LY = LZ | di | 2000 | Box size in each spatial direction | |
Npcc | – | 600 | Number of particles per cell | |
ηhup | – | 0.01 | Numerical hyper-resistivity | |
Simulation names | ||||
Sim 1 | Decaying solar-wind turbulence | |||
Sim 2.1 | Turbulent solar wind vs. planet | |||
Sim 2.2 | Laminar solar wind vs. planet |
Notes. Code normalizations, solar-wind parameters for all runs, initial amplitude of turbulence in the decaying run, characteristics of the magnetized planet, grid and time resolution for all runs. mp is the proton mass, c the speed of light in vacuum, and e the elementary charge. Simulation parameters are typical of the solar wind (Owens et al. 2023), with n0 and B0 being the initial solar-wind density and the magnetic field magnitude.
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