Abstract

This is the third in a series of papers that investigate the semi-annual, annual and Universal Time variations in the magnetosphere. In this paper, we use the Lin et al. (2010) empirical model of magnetopause locations, along with the assumption of pressure equilibrium and the Newtonian approximation of magnetosheath pressure, to show that the equinoctial pattern arises in both the cross-tail current at the tail hinge point and in the total energy stored in the tail. The model allows us to study the effects of both dipole tilt and hemispheric asymmetries. As a test of the necessary assumptions made to enable this analysis, we also study simulations by the BATSRUS global MHD magnetosphere model. These also show that the reconnection voltage in the tail is greatest when the dipole tilt is small but this only applies at low solar wind dynamic pressurepSWand does not, on its own, explain why the equinoctial effect increases in amplitude with increasedpSW, as demonstrated by Paper 2. Instead, the effect is consistent with the dipole tilt effect on the energy stored in the tail around the reconnection X line. A key factor is that a smaller/larger fraction of the open polar cap flux threads the tail lobe in the hemisphere that is pointed toward/away from the Sun. The analysis using the empirical model uses approximations and so is not definitive; however, because the magnetopause locations in the two hemispheres were fitted separately in generating the model, it gives a unique insight into the effect of the very different offsets of the magnetic pole from the rotational pole in the two hemispheres. It is therefore significant that our analysis using the empirical model does predict aUTvariation that is highly consistent with that found in both transpolar voltage data and in geomagnetic activity.

Highlights

  • This is the third in a series of papers investigating semi-annual, annual, and Universal Time (UT) variations in the magnetosphere

  • It is significant that our analysis using the empirical model does predict a UT variation that is highly consistent with that found in both transpolar voltage data and in geomagnetic activity

  • In the first paper of the series (Lockwood et al, 2020a: hereafter Paper 1) it was shown that the RussellMcPherron (R-M) effect is at the heart on the semiannual variation of geomagnetic activity, as is taken to be the case in a great many publications since it was originally proposed by Russell & McPherron (1973), this seminal paper having been cited over 750 times in the literature at the time of writing

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Summary

Modelling

We use the Lin et al (2010) empirical model of magnetopause locations, along with the assumption of pressure equilibrium and the Newtonian approximation of magnetosheath pressure, to show that the equinoctial pattern arises in both the cross-tail current at the tail hinge point and in the total energy stored in the tail. As a test of the necessary assumptions made to enable this analysis, we study simulations by the BATSRUS global MHD magnetosphere model. These show that the reconnection voltage in the tail is greatest when the dipole tilt is small but this only applies at low solar wind dynamic pressure pSW and does not, on its own, explain why the equinoctial effect increases in amplitude with increased pSW, as demonstrated by Paper 2. It is significant that our analysis using the empirical model does predict a UT variation that is highly consistent with that found in both transpolar voltage data and in geomagnetic activity

Introduction
The Russell-McPherron effect and large geomagnetic storms
The am geomagnetic index and power input into the magnetosphere
The effect of solar wind dynamic pressure
UT variations in geomagnetic activity
Magnetospheric compression by solar wind dynamic pressure
Application of an empirical model of the magnetopause
Tail lobe field intensity and magnetic energy density
Equinoctial patterns in tail lobe energy and magnetic shear
Detection of the annual variation in geomagnetic activity
Global numerical MHD modelling
Simulated magnetospheric fields
 106 mÀ3 2  105 K
Magnetic fluxes and total energy in the tail lobes
Findings
Discussion and Conclusions
Full Text
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