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Equatorial magnetic field of the near‐Earth magnetotail
Author(s) -
Ohtani S.,
Motoba T.
Publication year - 2017
Publication title -
journal of geophysical research: space physics
Language(s) - English
Resource type - Journals
eISSN - 2169-9402
pISSN - 2169-9380
DOI - 10.1002/2017ja024115
Subject(s) - substorm , physics , magnetic field , magnetosphere , geophysics , l shell , dipole , magnetic reconnection , mercury's magnetic field , magnetic dipole , field (mathematics) , dipole model of the earth's magnetic field , interplanetary magnetic field , convection , earth's magnetic field , condensed matter physics , computational physics , solar wind , mechanics , quantum mechanics , mathematics , pure mathematics
The equatorial magnetic field of the nightside magnetosphere is critical for understanding not only the configuration of the magnetotail but also its state and dynamics. The present study observationally addresses various aspects of the equatorial magnetic field, such as its spatial distribution, possible antisunward gradients, and extremely weak magnetic fields, with emphasis on the transition region between dipolar and stretched magnetic configurations. The results are summarized as follows: (1) the transition of the tail magnetic field from a near‐Earth dipolar configuration to a stretched one farther out takes place around −12 ≤ X agsm ≤ −9 R E , although instantaneous configurations can vary significantly; (2) the average equatorial magnetic field in this transition region is noticeably weaker at solar minimum presumably reflecting weaker nightside magnetospheric currents closer to Earth; (3) the statistical comparison of equatorial magnetic fields measured simultaneously at two locations indicates that the gradient of the equatorial magnetic field is directed predominantly earthward, and it is suggested that apparent tailward gradients observed can be very often attributed to other factors such as structures in the Y direction and local fluctuations; (4) however, the gradient can be transiently directed tailward in association with the dipolarization of local magnetic field; (5) extremely weak (≤ 2 nT) magnetic fields are occasionally observed in the transition region during the substorm growth phase and during prolonged quiet intervals, but the association with steady magnetospheric convection, which was suggested before, cannot be confirmed possibly because of its rare occurrence.