Run Status: Run Complete
Status updated: 2021-08-02T15:56:33+0000

Note: CMIT-LFM simulation runs submitted before October 31, 2018 used solar wind data propagated to the model run's upstream (sunward) boundary (typically at Xmax=30 RE).
However, the model assumes solar wind to be propagated to X=0 instead, causing features in the solar wind to occur in the LFM model simulation a few minutes earlier than expected (for example, 8 minutes earlier for Vx=-400 km/s and Xmax=30 RE).
The propagation has been adjusted in the run request system for "event" runs with CMIT-LFM where solar wind data are obtained automatically from one of the available solar wind monitor spacecraft or data sources (solar wind data in uploaded file are not propagated and need to be adjusted before file upload to make LFM runs comparable to runs of the other magnetosphere models).

Run Metadata
Metadata Record:View Full Run Metadata in the CCMC Metadata Registry (CMR)
Metadata as JSON:View Full Run Metadata as JSON
 
Model Domain:GM
Model Name:LFM
Model Version:LTR-2_1_5
Title/Introduction:Magnetopause Motion
Key Word:magnetopause
 
Run type:Simulation with modeled conditions
Inflow Boundary Conditions:Time-dependent
Start Time:2015/07/04 14:20
End Time:2015/07/05 06:20
Dipole Tilt at Start in X-Z Plane:30.82 °
Dipole Tilt in Y-Z GSE Plane:-12.26 °
Dipole Update With Time:yes
Ionospheric Conductance:auroral
Radio Flux 10.7 cm:120.7
Co-rotation:Corotation potential is being applied
Grid:53x48x64 cells
Coordinate System for the Output:SM
Solar wind input source:user-uploaded
Initial Solar Wind (SW) Parameters in SM Coordinates:
  SW Density:27.12700 n/cc
  SW Temperature:77927.90000 Kelvin
  X Component of SW Velocity:-364.54300 km/s
  Y Component of SW Velocity:-34.55300 km/s
  Z Component of SW Velocity:-13.42100 km/s
  IMF Bx:0.00000 nT
  IMF By:-3.34800 nT
  IMF Bz:16.90100 nT
  IMF |B|:17.23000 nT
  IMF Clock Angle:-11.20000 °
 
Input Data
  • View solar wind input data
  • List solar wind input data in ASCII format (see format description here).
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