TY - JOUR

T1 - Tail plasma sheet models derived from Geotail particle data

AU - Tsyganenko, NA

AU - Mukai, T

PY - 2003/3/28

Y1 - 2003/3/28

N2 - Simple analytical models have been derived for the first time, describing the 2-D distribution (along and across the Earth's magnetotail) of the central plasma sheet (CPS) ion temperature, density, and pressure, as functions of the incoming solar wind and interplanetary magnetic field (IMF) parameters, at distances between 10 and 50 R-E. The models are based on a large set of data of the Low-Energy Particle (LEP) and Magnetic Field (MGF) instruments, taken by Geotail spacecraft between 1994 and 1998, comprising 7234 1-min average values of the CPS temperature and density. Concurrent solar wind and IMF data were provided by the Wind and IMP 8 spacecraft. The accuracy of the models was gauged by the correlation coefficient (c.c.) R between the observed and predicted values of a parameter. The CPS ion density N is controlled mostly by the solar wind proton density and by the northward component of the IMF. Being the least stable characteristic of the CPS, it yielded the lowest c.c. R-N = 0.57. The CPS temperature T, controlled mainly by the solar wind speed V and the IMF B-z, gave a higher c.c. R-T = 0.71. The CPS ion pressure P was best controlled by the solar wind ram pressure P-sw and by an IMF-related parameter F = B(perpendicular to)rootsin(theta/2), where B-perpendicular to is the perpendicular component of the IMF and theta is its clock angle. In a striking contrast with N and T, the model pressure P revealed a very high c.c. with the data, R-P = 0.95, an apparent consequence of the force balance between the CPS and the tail lobe magnetic field. No significant dawn-dusk asymmetry of the CPS was found beyond the distance 10 R-E, in line with the observed symmetry of the tail lobe magnetic field. The plasma density N is lowest at midnight and increases toward the tail's flanks. Larger (smaller) solar wind ion densities and northward (southward) IMF B-z result in larger (smaller) N in the CPS. In contrast to the density N, the temperature T peaks at the midnight meridian and falls off toward the dawn/dusk flanks. Faster (slower) solar wind flow and southward (northward) IMF B-z result in a hotter (cooler) CPS. The CPS ion pressure P is essentially a function of only X-GSM in the midtail (20-50 R-E); at closer distances the isobars gradually bend to approximately follow the contours of constant geomagnetic field strength. For northward IMF conditions combined with a slow solar wind, the isobars remain quasi-circular up to larger distances, reflecting a weaker tail current and, hence, more dipole-like magnetic field.

AB - Simple analytical models have been derived for the first time, describing the 2-D distribution (along and across the Earth's magnetotail) of the central plasma sheet (CPS) ion temperature, density, and pressure, as functions of the incoming solar wind and interplanetary magnetic field (IMF) parameters, at distances between 10 and 50 R-E. The models are based on a large set of data of the Low-Energy Particle (LEP) and Magnetic Field (MGF) instruments, taken by Geotail spacecraft between 1994 and 1998, comprising 7234 1-min average values of the CPS temperature and density. Concurrent solar wind and IMF data were provided by the Wind and IMP 8 spacecraft. The accuracy of the models was gauged by the correlation coefficient (c.c.) R between the observed and predicted values of a parameter. The CPS ion density N is controlled mostly by the solar wind proton density and by the northward component of the IMF. Being the least stable characteristic of the CPS, it yielded the lowest c.c. R-N = 0.57. The CPS temperature T, controlled mainly by the solar wind speed V and the IMF B-z, gave a higher c.c. R-T = 0.71. The CPS ion pressure P was best controlled by the solar wind ram pressure P-sw and by an IMF-related parameter F = B(perpendicular to)rootsin(theta/2), where B-perpendicular to is the perpendicular component of the IMF and theta is its clock angle. In a striking contrast with N and T, the model pressure P revealed a very high c.c. with the data, R-P = 0.95, an apparent consequence of the force balance between the CPS and the tail lobe magnetic field. No significant dawn-dusk asymmetry of the CPS was found beyond the distance 10 R-E, in line with the observed symmetry of the tail lobe magnetic field. The plasma density N is lowest at midnight and increases toward the tail's flanks. Larger (smaller) solar wind ion densities and northward (southward) IMF B-z result in larger (smaller) N in the CPS. In contrast to the density N, the temperature T peaks at the midnight meridian and falls off toward the dawn/dusk flanks. Faster (slower) solar wind flow and southward (northward) IMF B-z result in a hotter (cooler) CPS. The CPS ion pressure P is essentially a function of only X-GSM in the midtail (20-50 R-E); at closer distances the isobars gradually bend to approximately follow the contours of constant geomagnetic field strength. For northward IMF conditions combined with a slow solar wind, the isobars remain quasi-circular up to larger distances, reflecting a weaker tail current and, hence, more dipole-like magnetic field.

KW - plasma sheet

KW - solar wind

KW - modeling

KW - ion pressure

KW - density

KW - temperature

KW - MAGNETOSPHERIC MAGNETIC-FIELD

KW - SOLAR-WIND

KW - MAGNETOPAUSE

KW - TEMPERATURE

KW - PRESSURE

KW - DENSITY

U2 - 10.1029/2002JA009707

DO - 10.1029/2002JA009707

M3 - Article

VL - 108

JO - Journal of Geophysical Research: Biogeosciences

JF - Journal of Geophysical Research: Biogeosciences

SN - 0148-0227

IS - A3

M1 - 1136

ER -