Model/data comparisons of ionospheric outflow as a function of invariant latitude and magnetic local time

[1] Globally quantifying ionospheric outflows as a function of local time, invariant latitude and solar wind conditions is the key to determining the mass loading of the magnetosphere, and it subsequent dynamics. This paper provides a first comparison of model predicted outflows with Polar and Akebono outflow measurements for a quiet period that occurred on 18 March 1997. It is shown that that the model is able to account for the H+ fluxes observed on the dayside by Akebono with fluxes of the order of several times 109 ions/cm2/s. H+ fluxes observed by Polar in the midnight auroral zone are lower by an order of magnitude than the model fluxes. The difference is attributed to the presence of a lower energy component below the low energy cutoff of TIMAS. During the geomagnetically quiet conditions considered here, the model underestimates the O+ flux seen by Akebono on the dayside. The model correctly predicts the energetic fluxes of O+ seen on the nightside by Polar at several 107 ions/cm2/s. This calibration of the outflow model predicts the following magnetospheric features: (1) the dayside ionospheric outflows leads to substantial (≳10 cm−3) densities of cold plasma in the vicinity of the magnetopause, particularly on the dusk side during periods of enhanced convection; (2) the composition of the magnetosphere can change over the course of very small IMF changes (±1–2 nT in the present study) with northerly turnings allowing solar wind entry via the low latitude boundary layer, while pressure pulses aid high latitude entry across a magnetopause that is otherwise dominated by ionospheric plasma on the earthward side of the magnetopause; and (3) the calculated changes in the ionospheric outflow rate are sufficiently large that composition of the magnetosphere can change from one that is predominantly ionospheric in origin to one that is primarily of solar wind origin for changes in the IMF as small as ±1 nT.

[1]  O. W. Lennartsson,et al.  Quiet time solar illumination effects on the fluxes and characteristic energies of ionospheric outflow , 2006 .

[2]  E. Harnett,et al.  Multi‐scale/multi‐fluid simulations of the post plasmoid current sheet in the terrestrial magnetosphere , 2006 .

[3]  T. Moore,et al.  Magnetospheric convection and thermal ions in the dayside outer magnetosphere , 2006 .

[4]  T. Moore,et al.  An examination of the process and magnitude of ionospheric plasma supply to the magnetosphere , 2005 .

[5]  Robert M. Winglee,et al.  Mapping of the heavy ion outflows as seen by IMAGE and multifluid global modeling for the 17 April 2002 storm , 2005 .

[6]  O. W. Lennartsson,et al.  Solar wind control of Earth's H+ and O+ outflow rates in the 15‐eV to 33‐keV energy range , 2004 .

[7]  Robert M. Winglee,et al.  Ion cyclotron and heavy ion effects on reconnection in a global magnetotail , 2004 .

[8]  W.K. (Bill) Peterson,et al.  Dynamic coordinates for auroral ion outflow , 2004 .

[9]  M. Spasojević,et al.  Simultaneous remote sensing and in situ observations of plasmaspheric drainage plumes , 2004 .

[10]  G. Wilson,et al.  Nightside auroral zone and polar cap ion outflow as a function of substorm size and phase , 2004 .

[11]  R. Winglee Circulation of ionospheric and solar wind particle populations during extended southward interplanetary magnetic field , 2003 .

[12]  C. Cully,et al.  Akebono/Suprathermal Mass Spectrometer observations of low‐energy ion outflow: Dependence on magnetic activity and solar wind conditions , 2003 .

[13]  C. Cully,et al.  Investigation into the Spatial and Temporal Coherence of Ionospheric Outflow on January 9-12, 1997 , 2002 .

[14]  G. Parks,et al.  Global impact of ionospheric outflows on the dynamics of the magnetosphere and cross-polar cap potential , 2002 .

[15]  F. Frutos-Alfaro,et al.  Ion composition of substorms during storm-time and non-storm-time periods , 2002 .

[16]  O. W. Lennartsson,et al.  Polar/Toroidal Imaging Mass-Angle Spectrograph observations of suprathermal ion outflow during solar minimum conditions , 2001 .

[17]  Bill R. Sandel,et al.  Global dynamics of the plasmasphere and ring current during magnetic storms , 2001 .

[18]  O. W. Lennartsson,et al.  Observations of centrifugal acceleration during compression of magnetosphere , 2000 .

[19]  R. Winglee Mapping of ionospheric outflows into the magnetosphere for varying IMF conditions , 2000 .

[20]  T. Moore,et al.  The adequacy of the ionospheric source in supplying magnetospheric plasma , 2000 .

[21]  Lockheed Martin POLAR/TIMAS observations of suprathermal ion outflow during solar minimum conditions , 2000 .

[22]  R. Winglee,et al.  Multi‐fluid simulations of the magnetosphere: The identification of the geopause and its variation with IMF , 1998 .

[23]  T. Mukai,et al.  Statistical properties and possible supply mechanisms of tailward cold O + beams in the lobe/mantle regions , 1998 .

[24]  R. Lin,et al.  Flux rope structures in the magnetotail: Comparison between Wind/Geotail observations and global simulations , 1998 .

[25]  M. André,et al.  Sources of Ion Outflow in the High Latitude Ionosphere , 1997 .

[26]  T. Mukai,et al.  Coexistence of Earth‐origin O+ and solar wind‐origin H+/He++ in the distant magnetotail , 1996 .

[27]  T. Mukai,et al.  Cold dense ion flows with multiple components observed in the distant tail lobe by Geotail , 1996 .

[28]  B. A. Whalen,et al.  The Toroidal Imaging Mass-Angle Spectrograph (TIMAS) for the polar mission , 1995 .

[29]  R. Winglee Non-MHD influences on the magnetospheric current system , 1994 .

[30]  Yoshitaka Saito,et al.  Geotail observation of cold ion streams in the medium distance magnetotail lobe in the course of a substorm , 1994 .

[31]  B. A. Whalen,et al.  EXOS D (Akebono) observations of molecular NO+ and N2 + upflowing ions in the high‐altitude auroral ionosphere , 1993 .

[32]  J. Sauvaud,et al.  Polar wind ion dynamics in the magnetotail , 1993 .

[33]  T. Moore Origins of magnetospheric plasma , 1991 .

[34]  D. Gurnett,et al.  A survey of upwelling ion event characteristics , 1990 .

[35]  B. Whalen The suprathermal ion mass spectrometer (SMS) for the Akebono (EXOS-D) spacecraft , 1990 .

[36]  S. Watanabe,et al.  The suprathermal ion mass spectrometer (SMS) onboard the Akebono (EXOS-D) satellite , 1990 .

[37]  T. Moore,et al.  A three‐dimensional numerical model of ionospheric plasma in the magnetosphere , 1989 .

[38]  W. T. Roberts,et al.  Heavy ion density enhancements in the outer plasmasphere , 1987 .

[39]  T. Moore,et al.  The ionosphere as a fully adequate source of plasma for the Earth's magnetosphere , 1987 .

[40]  W.K. (Bill) Peterson,et al.  Solar cycle variation of some mass dependent characteristics of upflowing beams of terrestrial ions , 1987 .

[41]  J. Horwitz Core plasma in the magnetosphere , 1987 .

[42]  J. Cladis Parallel acceleration and transport of ions from polar ionosphere to plasma sheet , 1986 .

[43]  M. Lockwood,et al.  Upwelling O(+) ion source characteristics. [in polar magnetosphere] , 1986 .

[44]  W.K. (Bill) Peterson,et al.  Long-term (solar cycle) and seasonal variations of upflowing ionospheric ion events at DE 1 altitudes , 1985 .

[45]  T. Killeen,et al.  Escape of suprathermal O(+) ions in the polar cap , 1985 .

[46]  J. Luhmann,et al.  The distribution of ion beams and conics below 8000 km , 1981 .

[47]  D. Klumpar Transversely accelerated ions - An ionospheric source of hot magnetospheric ions , 1979 .

[48]  R. D. Sharp,et al.  The latitudinal, diurnal, and altitudinal distributions of upward flowing energetic ions of ionospheric origin , 1978 .

[49]  E. Shelley,et al.  Observation of an ionospheric acceleration mechanism producing energetic (keV) ions primarily normal to the geomagnetic field direction , 1977 .