Results of magnetospheric simulations with artificial conditions



Run NumberKeywordModelModel VersionEvent dateGridVxN|B|IMF Clock AngleBxByBzConductance ModelDipole Tilt (in X-Z Plane) at start
HSS2011_LFMhr_052111_2 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_LFMhr_052111_3 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_LFMhr_052111_4 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_LFMhr_053011_2 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=2.5 h=0 0.0
HSS2011_LFMhr_053011_3 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=2.5 h=0 0.0
HSS2011_LFMhr_053011_4 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=2.5 h=0 0.0
HSS2011_LFMhr_053111_2 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=10 h=0 0.0
HSS2011_LFMhr_053111_3 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=10 h=0 0.0
HSS2011_LFMhr_053111_4 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=10 h=0 0.0
HSS2011_LFMhr_060211_1 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-200.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_LFMhr_060211_2 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-600.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_LFMhr_060211_3 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-600.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_LFMhr_060211_4 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-600.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_LFMhr_060311_1 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-200.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_LFMhr_060311_2 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.010.0180.0 0.0 0.0-10.0uniform p=5 h=0 0.0
HSS2011_LFMhr_060311_3 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-200.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_LFMhr_060311_4 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1Model 106x48x64-400.0 5.010.0 0.0 0.0 0.010.0uniform p=5 h=0 0.0
HSS2011_LFM_051111_1 HSS2011, equinox, quiet, increased resolution LFMLTR-2_1_1March 21 2007106x48x64-400.0 5.0 5.0180.0 0.0 0.0-5.0auroral -3.9
HSS2011_LFM_051111_2 HSS2011, equinox, quiet LFMLTR-2_1_1Modeled53x48x64-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_LFM_051111_3 HSS2011, equinox, quiet LFMLTR-2_1_1Modeled53x48x64-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_LFM_051111_4 HSS2011, equinox, quiet LFMLTR-2_1_1Modeled53x48x64-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_051111_1 HSS2011, equinox, quiet, increased resolution OpenGGCM3.1March 21 20076.5M overview-400.0 5.0 5.0180.0 0.0 0.0-5.0Sig-CTIM -3.9
HSS2011_OpenGGCM_051111_2 HSS2011, equinox, quiet, increased resolution OpenGGCM3.1Modeled6.5M overview-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_051111_3 HSS2011, equinox, quiet, increased resolution OpenGGCM3.1Modeled6.5M overview-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_052111_2 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_052111_3 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_052111_4 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_053011_2 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=2.5 h=0 0.0
HSS2011_OpenGGCM_053011_3 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=2.5 h=0 0.0
HSS2011_OpenGGCM_053011_4 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=2.5 h=0 0.0
HSS2011_OpenGGCM_053111_2 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=10 h=0 0.0
HSS2011_OpenGGCM_053111_3 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=10 h=0 0.0
HSS2011_OpenGGCM_053111_4 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=10 h=0 0.0
HSS2011_OpenGGCM_060211_1 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-200.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_060211_2 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-600.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_060211_3 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-600.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_060211_4 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-600.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_060311_1 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-200.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_060311_2 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.010.0180.0 0.0 0.0-10.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_060311_3 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-200.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_OpenGGCM_060311_4 HSS2011, equinox, quiet OpenGGCM3.1Model 3M cells-400.0 5.010.0 0.0 0.0 0.010.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_1 HSS2011, equinox, quiet BATSRUSv8.01March 21 20072M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0auroral -3.9
HSS2011_SWMF_051111_2 HSS2011, equinox, quiet, SSW16BATSRUSv8.01Modeled2M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_2a HSS2011, equinox, quiet, Sokolov scheme BATSRUSv8.01Model 2M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_2b HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_3 HSS2011, equinox, quiet BATSRUSv8.01Modeled2M cells-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_3a HSS2011, equinox, quiet, Sokolov scheme BATSRUSv8.01Model 2M cells-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_3b HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_4 HSS2011, equinox, quiet BATSRUSv8.01Modeled2M cells-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_4a HSS2011, equinox, quiet, Sokolov scheme BATSRUSv8.01Model 2M cells-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_SWMF_051111_4b HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_SWMF_053011_2 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=2.5 h=0 0.0
HSS2011_SWMF_053011_3 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=2.5 h=0 0.0
HSS2011_SWMF_053011_4 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=2.5 h=0 0.0
HSS2011_SWMF_053111_2 HSS2012, Southward IMFBATSRUSv8.01Model 3M cells-400.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=10 h=0 0.0
HSS2011_SWMF_053111_3 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=10 h=0 0.0
HSS2011_SWMF_053111_4 HSS2012, Northward IMFBATSRUSv8.01Model 3M cells-400.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=10 h=0 0.0
HSS2011_SWMF_060211_1 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-200.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_SWMF_060211_2 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-600.0 5.0 5.0180.0 0.0 0.0-5.0uniform p=5 h=0 0.0
HSS2011_SWMF_060211_3 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-600.0 5.0 9.0 0.0 0.0 0.0 9.0uniform p=5 h=0 0.0
HSS2011_SWMF_060211_4 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-600.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_SWMF_060311_1 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-200.0 5.0 5.0 0.0 0.0 0.0 5.0uniform p=5 h=0 0.0
HSS2011_SWMF_060311_2 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.010.0180.0 0.0 0.0-10.0uniform p=5 h=0 0.0
HSS2011_SWMF_060311_3 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-200.0 5.0 0.0 0.0 0.0 0.0 0.0uniform p=5 h=0 0.0
HSS2011_SWMF_060311_4 HSS2011, equinox, quiet, Sokolov scheme, increased resolution BATSRUSv8.01Model 3M cells-400.0 5.010.0 0.0 0.0 0.010.0uniform p=5 h=0 0.0
Masha_Kuznetsova_051111_1 HSS2011 eqinox BATSRUSv8.01March 21 20072M cells-600.010.010.0 0.0 0.0 0.010.0auroral -3.9
Masha_Kuznetsova_071810_1 HSS2010 solstice BATSRUSv8.01December 22 2006 2M cells-600.010.010.0180.0 0.0 0.0-10.0auroral -30.0
Masha_Kuznetsova_071810_1a HSS2010 solstice BATSRUSv8.01December 22 2006 2M cells-600.010.010.0110.0 0.0 9.4-3.4auroral -30.0
Masha_Kuznetsova_071910_3 HSS2010 equinox BATSRUSv8.01March 21 2007 2M cells-600.010.010.0180.0 0.0 0.0-10.0auroral 0.0
Masha_Kuznetsova_071910_3a HSS2010 equinox BATSRUSv8.01March 21 2007 2M cells-600.010.010.0110.0 0.0 9.4-3.4auroral 0.0

Output in CDF format:

HSS2011_OpenGGCM_051111_1_T200.out.cdf

HSS2011_OpenGGCM_051111_2_T200.out.cdf

HSS2011_OpenGGCM_051111_3_T200.out.cdf

HSS2011_OpenGGCM_052111_2_T200.out.cdf

HSS2011_OpenGGCM_052111_3_T200.out.cdf

HSS2011_OpenGGCM_052111_4_T200.out.cdf

HSS2011_OpenGGCM_053011_2_T200.out.cdf

HSS2011_OpenGGCM_053011_3_T200.out.cdf

HSS2011_OpenGGCM_053011_4_T200.out.cdf

HSS2011_OpenGGCM_053111_2_T200.out.cdf

HSS2011_OpenGGCM_053111_3_T200.out.cdf

HSS2011_OpenGGCM_053111_4_T200.out.cdf

HSS2011_OpenGGCM_060211_1_T200.out.cdf

HSS2011_OpenGGCM_060211_2_T200.out.cdf

HSS2011_OpenGGCM_060211_3_T200.out.cdf

HSS2011_OpenGGCM_060211_4_T200.out.cdf

HSS2011_OpenGGCM_060311_1_T200.out.cdf

HSS2011_OpenGGCM_060311_2_T200.out.cdf

HSS2011_OpenGGCM_060311_3_T200.out.cdf

HSS2011_OpenGGCM_060311_4_T200.out.cdf

HSS2011_SWMF_051111_1_T200.out.cdf

HSS2011_SWMF_051111_2_T200.out.cdf

HSS2011_SWMF_051111_2a_T200.out.cdf

HSS2011_SWMF_051111_2b_T200.out.cdf

HSS2011_SWMF_051111_3_T200.out.cdf

HSS2011_SWMF_051111_3a_T200.out.cdf

HSS2011_SWMF_051111_3b_T200.out.cdf

HSS2011_SWMF_051111_4_T200.out.cdf

HSS2011_SWMF_051111_4a_T200.out.cdf

HSS2011_SWMF_051111_4b_T200.out.cdf

HSS2011_SWMF_053011_2_T200.out.cdf

HSS2011_SWMF_053011_3_T200.out.cdf

HSS2011_SWMF_053011_4_T200.out.cdf

HSS2011_SWMF_053111_3_T200.out.cdf

HSS2011_SWMF_060211_1_T200.out.cdf

HSS2011_SWMF_060211_2_T200.out.cdf

HSS2011_SWMF_060211_3_T200.out.cdf

HSS2011_SWMF_060211_4_T200.out.cdf

HSS2011_SWMF_060311_1_T200.out.cdf

HSS2011_SWMF_060311_2_T200.out.cdf

HSS2011_SWMF_060311_3_T200.out.cdf

HSS2011_SWMF_060311_4_T200.out.cdf

Masha_Kuznetsova_051111_1_T200.out.cdf

Masha_Kuznetsova_071810_1_T200.out.cdf

Masha_Kuznetsova_071810_1a_T200.out.cdf

Masha_Kuznetsova_071910_3_T200.out.cdf

Masha_Kuznetsova_071910_3a_T200.out.cdf

Masha_Kuznetsova_072110_3_T200.out.cdf


Back to Top