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GITM (2.0)

Global Ionosphere Thermosphere Model (GITM)

Model Description

GITM is a 3-dimensional spherical code that models the Earth's thermosphere and ionosphere system using a stretched grid in latitude and altitude. The number of grid points in each direction can be specified, so the resolution is extremely flexible. GITM explicitly solves for the neutral densities of O, O2, N(2D), N(2P), N(4S), N2, and NO; and ion species O+(4S), O+(2D), O+(2P), O2+, N+, N2+, and NO+. One major difference between GITM and other thermosphere codes is the use of an altitude grid instead of a pressure grid. The vertical grid spacing is less than 3 km in the lower thermosphere, and over 10 km in the upper thermosphere. GITM allows for non-hydrostatic solutions to develop (i.e., the full vertical momentum equation is solved), so more realistic dynamics in the auroral zone can be simulated.

GITM includes a modern advection solver and realistic source terms for the continuity, momentum, and energy equations. Each neutral species has a separate vertical velocity, with coupling of the velocities through a frictional term. The ion momentum equation is solved for assuming steady state, taking into account the pressure, gravity, neutral winds, and external electric fields. GITM is coupled to a large number of models of the high-latitude ionospheric electrodynamics, for example, the assimilative mapping of ionospheric electrodynamics (AMIE) technique, Weimer, Foster, Heppner and Maynard or Ridley et al. electrodynamic potential patterns. The initial state can be set in three different ways: (1) using an ideal atmosphere, where the user inputs the densities and temperature at the bottom of the atmosphere; (2) using MSIS and IRI; and (3) restarting from a previous run. For the automated CCMC runs on request system, Weimer05 is used to specify high latitude electric potential, Fuller-Rowell and Evans [1987] is used to specify the aurora, and MSIS and IRI are used to set the initial state. GITM currently hosted at CCMC covers all latitudes and a vertical range from about 90 km to 600 km. The latitude resolution is 2.5º, and longitude resolution is 5º.

Model Figure(s) :

  • GITM 2.0 Sample Output Diagram 1
  • GITM 2.0 Sample Output Diagram 2
  • Model Inputs Description

    F10.7 (10.7 cm solar radio flux): data can be found at CCMC data generation pages or ftp://ftp.ngdc.noaa.gov/STP/SOLAR_DATA/SOLAR_RADIO/FLUX
    Hemispheric Power Index (HPI): data can be found at http://www.sec.noaa.gov/ftpdir/lists/hpi
    Interplanetary Magnetic Field
    Solar wind velocity
    Solar irradiance (for event runs): data can be found at http://lasp.colorado.edu/lisird/fism/?

    Model Outputs Description

    Temperatures: neutral, ion, electron (K)
    Neutral winds: zonal, meridional, vertical (m/s)
    Plasma velocities: zonal, meridional, vertical (m/s)
    Neutral mass density (kg/m3)
    Number densities: neutral (O, O2, N(2D), N(2P), N(4S), N2, and NO), ion (O+(4S), O+(2D), O+(2P), O2+, N+, N2+, and NO+), and electron (m-3)

    Model Caveats

    
    	
    	
    	
    	

    Change Log

    
    	
    	 
    	

    Model Acknowledgement/Publication Policy (if any)

    
    	
    	
    	

    Model Domains:

    Global_Ionosphere
    Thermosphere

    Space Weather Impacts:

    Ionosphere variability (navigation, communications)
    Atmosphere variability (satellite/debris drag)

    Phenomena :

    Variablility_of_Plasma_Density
    Atmosphere_Expansion
    Neutral_Composition_Change
    Neutral_Wind_Change
    Ion_Drift_Velocity
    Equatorial_Anomaly
    Traveling_Ionospheric_Disturbances
    Traveling_Atmospheric_Disturbances

    Simulation Type(s):

    Physics-based

    Temporal Dependence Possible? (whether the code results depend on physical time?)

    false

    Model is available at?

    CCMC

    Source code of the model is publicly available?

    false

    CCMC Model Status (e.g. onboarding, use in production, retired, only hosting output, only source is available):

    retired

    Code Language:


    Regions (this is automatically mapped based on model domain):

    Earth.NearSurface.Ionosphere
    Earth.NearSurface.Thermosphere

    Contacts :

    Aaron.Ridley, ModelDeveloper
    Katherine.Garcia-Sage, ModelHostContact
    Jia.Yue, ModelHostContact

    Acknowledgement/Institution :

    Department of Atmosphere, Oceanic and Space Sciences, University of Michigan

    Relevant Links :

    Publications :

  • Ridley, A. J., Y. Deng, and G. Toth., 2006, The Global Ionosphere-Thermosphere Model (GITM). J. Atmos. Solar-Terrestr. Phys. 68, 839-864.
  • Bilitza, D., 2001, International reference ionosphere 2000, Radio Science 36, 261.
  • Ridley, A., Crowley, G., Freitas, C., 2000, An empirical model of the ionospheric electric potential, Geophysics Research Letters 27, 3675.
  • Weimer, D., 1996, A flexible, IMF dependent model of high- latitude electric potential having space weather applications, Geophysics Research Letters 23, 254.
  • Weimer, D. R.: Improved ionospheric electrodynamic models and application to calculating Joule heating rates, J. Geophys. Res., 110, 05 306, doi:10.1029/2004JA010884, 2005.
  • Richmond, A., 1995, Ionospheric electrodynamics using magnetic apex coordinates, J. Geomagn. Geo-electr. 47, 191.
  • Hedin, A., 1991, Extension of the MSIS thermosphere model into the middle and lower atmosphere, Journal of Geophysical Research 96, 1159.
  • Heppner, J., Maynard, N., 1987, Empirical high-latitude electric field models, Journal of Geophysical Research 92, 4467.
  • Foster, J., 1983, An empirical electric field model derived from Chatanika radar data, Journal of Geophysical Research 90, 981.
  • Fuller-Rowell, T. and Evans, D.: Height-integrated Pedersen and Hall conductivity patterns inferred from TIROS-NOAA satellite data, J. Geophys. Res., 92, 7606, 1987.
  • Model Access Information :

    Linked to Other Spase Resource(s) (example: another SimulationModel) :

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