Abstract

Abstract. A detailed statistical study of the magnetic structure of the dayside polar cusps is presented, based on multi-year sets of magnetometer data of Polar and Cluster spacecraft, taken in 1996–2006 and 2001–2007, respectively. Thanks to the dense data coverage in both Northern and Southern Hemispheres, the analysis spanned nearly the entire length of the cusps, from low altitudes to the cusp "throat" and the magnetosheath. Subsets of data falling inside the polar cusp "funnels" were selected with the help of TS05 and IGRF magnetic field models, taking into account the dipole tilt and the solar wind/IMF conditions. The selection funnels were shifted within ±10° of SM latitude around the model cusp location, and linear regression parameters were calculated for each sliding subset, further divided into 10 bins of distance in the range 2≤R≤12 RE, with the following results. (1) Diamagnetic depression, caused by the penetrated magnetosheath plasma, becomes first visible at R~4–5 RE, rapidly deepens with growing R, peaks at R~6–9 RE, and then partially subsides and widens in latitude at the cusp's outer end. (2) The depression peak is systematically shifted poleward (by ~2° of the footpoint latitude) with respect to the model cusp field line, passing through the min{|B|} point at the magnetopause. (3) At all radial distances, clear and distinct peaks of the correlation between the local By and By(IMF) and of the corresponding proportionality coefficient are observed. A remarkably regular variation of that coefficient with R quantitatively confirms the field-aligned geometry of the cusp currents associated with the IMF By, found in earlier observations.

Highlights

  • This paper addresses two characteristic features of the polar cusps: (1) the diamagnetic depression and (2) the effect of the IMF By “penetration”

  • The selection funnel spanned the interval within ±10◦ around the footpoint latitude of the cusp central line, predicted by the TS05 model individually for each magnetic field data record in the cumulative set

  • Each subset was further divided into ten 1 RE bins of the radial distance in the range 2≤R≤12 RE and, for each bin, we calculated (a) the average value and the rms scatter of the difference B=|Bobs|−|BIGRF| between the magnitudes of the total observed field and of the Earth’s main field, (b) correlation coefficients between the By field component observed in and around the cusp and By(IMF), and (c) parameters C1 and C2 in the linear regression equation

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Summary

Objectives

The goal of the present work is to systematically explore the IMF By effects and analyze in detail the near-noon cusp currents in the entire range of radial distances, in both Northern and Southern Hemispheres

Results
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