A high time resolution study of the solar wind-magnetosphere energy coupling function

1982 ◽  
Vol 30 (6) ◽  
pp. 537-543 ◽  
Author(s):  
S.-I. Akasofu ◽  
J.F. Carbary ◽  
C.-I. Meng ◽  
J.P. Sullivan ◽  
R.P. Lepping
2017 ◽  
Vol 55 (1) ◽  
pp. 30-45 ◽  
Author(s):  
V. G. Eselevich ◽  
N. L. Borodkova ◽  
M. V. Eselevich ◽  
G. N. Zastenker ◽  
Y. Šafránkova ◽  
...  

2008 ◽  
Vol 26 (7) ◽  
pp. 1889-1895 ◽  
Author(s):  
G. Li ◽  
E. Lee ◽  
G. Parks

Abstract. Recent studies of solar wind MHD turbulence show that current-sheet-like structures are common in the solar wind and they are a significant source of solar wind MHD turbulence intermittency. While numerical simulations have suggested that such structures can arise from non-linear interactions of MHD turbulence, a recent study by Borovsky (2006), upon analyzing one year worth of ACE data, suggests that these structures may represent the magnetic walls of flux tubes that separate solar wind plasma into distinct bundles and these flux tubes are relic structures originating from boundaries of supergranules on the surface of the Sun. In this work, we examine whether there are such structures in the Earth's magnetotail, an environment vastly different from the solar wind. We use high time resolution magnetic field data of the FGM instrument onboard Cluster C1 spacecraft. The orbits of Cluster traverse through both the solar wind and the Earth's magnetosheath and magnetotail. This makes its dataset ideal for studying differences between solar wind MHD turbulence and that inside the Earth's magnetosphere. For comparison, we also perform the same analysis when Cluster C1 is in the solar wind. Using a data analysis procedure first introduced in Li (2007, 2008), we find that current-sheet-like structures can be clearly identified in the solar wind. However, similar structures do not exist inside the Earth's magnetotail. This result can be naturally explained if these structures have a solar origin as proposed by Borovsky (2006). With such a scenario, current analysis of solar wind MHD turbulence needs to be improved to include the effects due to these curent-sheet-like structures.


2019 ◽  
Vol 882 (2) ◽  
pp. 133
Author(s):  
D. Kaur ◽  
N. D. R. Bhat ◽  
S. E. Tremblay ◽  
R. M. Shannon ◽  
S. J. McSweeney ◽  
...  

1982 ◽  
Vol 2 (7) ◽  
pp. 75-79 ◽  
Author(s):  
V.M. Balebanov ◽  
O.L. Vaisberg ◽  
E.M. Vasiliev ◽  
G.N. Zastenker ◽  
V.P. Evdokimov ◽  
...  

1999 ◽  
Vol 17 (12) ◽  
pp. 1574-1581 ◽  
Author(s):  
G. K. Parks ◽  
S. Datta ◽  
M. McCarthy ◽  
R. P. Lin ◽  
H. Reme ◽  
...  

Abstract. An electrostatic analyser (ESA) onboard the Equator-S spacecraft operating in coordination with a potential control device (PCD) has obtained the first accurate electron energy spectrum with energies ≈7 eV–100 eV in the vicinity of the magnetopause. On 8 January, 1998, a solar wind pressure increase pushed the magnetopause inward, leaving the Equator-S spacecraft in the magnetosheath. On the return into the magnetosphere approximately 80 min later, the magnetopause was observed by the ESA and the solid state telescopes (the SSTs detected electrons and ions with energies ≈20–300 keV). The high time resolution (3 s) data from ESA and SST show the boundary region contains of multiple plasma sources that appear to evolve in space and time. We show that electrons with energies ≈7 eV–100 eV permeate the outer regions of the magnetosphere, from the magnetopause to ≈6Re. Pitch-angle distributions of ≈20–300 keV electrons show the electrons travel in both directions along the magnetic field with a peak at 90° indicating a trapped configuration. The IMF during this interval was dominated by Bx and By components with a small Bz.Key words. Magnetospheric physics (magnetopause · cusp · and boundary layers; magnetospheric configuration and dynamics; solar wind · magnetosphere interactions)


1983 ◽  
Vol 88 (A8) ◽  
pp. 6230 ◽  
Author(s):  
D. N. Baker ◽  
R. D. Zwickl ◽  
S. J. Bame ◽  
E. W. Hones ◽  
B. T. Tsurutani ◽  
...  

2016 ◽  
Author(s):  
N. P. Janitzek ◽  
A. Taut ◽  
L. Berger ◽  
P. Bochsler ◽  
C. Drews ◽  
...  

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