Models of high‐latitude electric potentials derived with a least error fit of spherical harmonic coefficients

New models of the high-latitude electric potentials have been developed. These models show how the polar ionospheric electric field, or plasma convection, responds to changes in the interplanetary magnetic field (IMF) and other parameters, such as dipole tilt angle. These patterns were derived from measurements of the electric field on the DE 2 satellite, using all polar cap passes during which high-resolution IMF data were available from the ISEE 3 or IMP 8 satellites. The data are sorted according to the angle of the IMF in the GSM Y-Z plane. The measurements are further divided into different groups according to the magnitude of the IMF or the dipole tilt angle. All measurements in each group are then used to derive a model of the electric potential for the given conditions, using a new technique where the coefficients of a spherical harmonic expansion are found by least square error fits. The resulting convection patterns are very realistic and show consistent variations as the IMF BY/BZ angle rotates. For northward IMF (positive BZ) evidently there are four convection “cells,” rather than a distortion of the two-cell pattern. Many other useful facts regarding the solar wind-ionosphere coupling can be extracted from the derived patterns, such as the relationship between the polar cap potential drop and the IMF clock angle.

[1]  W. J. Burke,et al.  S3‐2 measurements of the polar cap potential , 1983 .

[2]  R. Heelis,et al.  Model of the high‐latitude ionospheric convection pattern during southward interplanetary magnetic field using DE 2 data , 1990 .

[3]  J. Luhmann,et al.  Solar Wind Control of the Polar CAP Voltage , 1986 .

[4]  T. Hill,et al.  Mapping of the solar wind electric field to the Earth's polar caps , 1989 .

[5]  R. Schunk,et al.  Patches in the polar ionosphere: UT and seasonal dependence , 1994 .

[6]  D. A. Dunnett Classical Electrodynamics , 2020, Nature.

[7]  D. Weimer,et al.  The relationship between ionospheric convection and magnetic activity , 1994 .

[8]  N. Crooker Mapping the merging potential from the magnetopause to the ionosphere through the dayside cusp , 1988 .

[9]  Christopher T. Russell,et al.  GEOPHYSICAL COORDINATE TRANSFORMATIONS , 1971 .

[10]  B. Sonnerup,et al.  Magnetopause reconnection rate , 1974 .

[11]  P. Reiff,et al.  IMF By-dependent plasma flow and Birkeland currents in the dayside magnetosphere: 2. A global model for northward and southward IMF , 1985 .

[12]  N. Maynard,et al.  Empirical high‐latitude electric field models , 1987 .

[13]  J. Heppner Polar‐cap electric field distributions related to the interplanetary magnetic field direction , 1972 .

[14]  T. Hill Magnetic merging in a collisionless plasma , 1975 .

[15]  D. Weimer,et al.  Variations of the polar cap potential measured during magnetospheric substorms , 1992 .

[16]  L. Lyons A simple model for polar cap convection patterns and generation of θ auroras , 1985 .

[17]  S. Akasofu,et al.  Field-aligned currents and ionospheric electric fields , 1977 .

[18]  H. F. Burdick,et al.  Instrumentation for vector electric field measurements from DE-B. [Dynamics Explorer-B satellite , 1981 .

[19]  Frederick J. Rich,et al.  Large-scale convection patterns observed by DMSP , 1994 .

[20]  Daniel N. Baker,et al.  Magnetospheric Impulse Response for Many Levels of Geomagnetic Activity , 1985 .

[21]  N. Crooker,et al.  Lobe cell convection as a summer phenomenon , 1993 .

[22]  D. D. Barbosa Fourier analysis of polar cap electric field and current distributions , 1984 .

[23]  D. D. Barbosa High‐latitude field‐aligned current sources and induced electric fields , 1979 .

[24]  W. J. Burke,et al.  Interplanetary control of high latitude electrodynamics. , 1986 .

[25]  R. W. Spiro,et al.  A model of the high‐latitude ionospheric convection pattern , 1982 .

[26]  N. Maynard,et al.  Consequences of using simple analytical functions for the high-latitude convection electric field , 1989 .

[27]  Mike Lockwood,et al.  The excitation of plasma convection in the high‐latitude ionosphere , 1990 .

[28]  R. Heelis,et al.  Ionospheric convection signatures observed by De 2 during northward interplanetary magnetic field , 1986 .

[29]  W. J. Burke,et al.  Polar cap electric field structures with a northward interplanetary magnetic field , 1979 .

[30]  R. W. Spiro,et al.  Dependence of polar cap potential drop on interplanetary parameters , 1981 .

[31]  Lou‐Chuang Lee,et al.  Energy coupling function and solar wind‐magnetosphere dynamo , 1979 .

[32]  C. Russell,et al.  Patterns of potential magnetic field merging sites on the dayside magnetopause , 1984 .