yaozh.space

yaozh.spaceyaozh.spaceyaozh.space

yaozh.space

yaozh.spaceyaozh.spaceyaozh.space
More

Description

The numerical simulation is based on the three-dimensional global Jovian magnetosphere model. The MHD equations are solved on a non-orthogonal, curvilinear grid adapted to Jovian magnetospheric problems based on high-resolving power finite-volume techniques for resolving meso-scale structures. In the solar-magnetic (SM) coordinate system, a stretched spherical grid extends to +120 RJ in the sunward direction (XSM), -1300 RJ in the anti-sunward direction, and ±360 RJ in the directions perpendicular to the sun-Jupiter axis (YSM, ZSM directions), with 5123 computational cells which is currently the highest effective resolution used in global Jovian simulations. The grid is highly non-uniform and varies with radial distance, with ∆r = 0.06 RJ near the inner boundary, set as a spherical shell at 3.5 RJ Jovi-centric. The upstream SW velocity is VX = -380 km/s, VY = VZ = 0, and the SW density is 0.2 /cm3, corresponding to the median value of solar wind conditions observed near 5AU. The interplanetary magnetic field (IMF) is fixed as BX = BZ = 0, By = 0.5 nT to represent nominal IMF observed near Jupiter. The mass loading rate from Io is set to 800 kg/s.

Jupiter512_Density

Jupiter512_Density_XY

Jupiter512_Density_XZ

Jupiter512_Pressure

Jupiter512_Pressure_XY

Jupiter512_Pressure_XZ

Jupiter512_Bz

Jupiter512_Bz_XY

Jupiter512_Bz_XZ

Jupiter512_Vx

Jupiter512_Vx_XY

Jupiter512_Vx_XZ

Contact Information

Welcome to our page! If you have any questions,feel free to contact us.

Zhang,Binzheng,The University of Hong Kong, BINZH@HKU.HK

Liu,Jian,University of Science and Technology of China, jliuphy@ustc.edu.cn


Copyright © 2023 yaozh.space - All Rights Reserved.

This website uses cookies.

We use cookies to analyze website traffic and optimize your website experience. By accepting our use of cookies, your data will be aggregated with all other user data.

Accept