scholarly journals Why doesn't the ring current injection rate saturate?

2009 ◽  
Vol 114 (A2) ◽  
pp. n/a-n/a ◽  
Author(s):  
R. E. Lopez ◽  
J. G. Lyon ◽  
E. Mitchell ◽  
R. Bruntz ◽  
V. G. Merkin ◽  
...  
1983 ◽  
Vol 31 (8) ◽  
pp. 901-911 ◽  
Author(s):  
L.C. Lee ◽  
G. Corrick ◽  
S.-I. Akasofu

2006 ◽  
Vol 24 (12) ◽  
pp. 3547-3556 ◽  
Author(s):  
L. Xie ◽  
Z. Y. Pu ◽  
X. Z. Zhou ◽  
S. Y. Fu ◽  
Q.-G. Zong ◽  
...  

Abstract. An extensive study of ring current injection and intensification of the storm-time ring current is conducted with three-dimensional (3-D) test particle trajectory calculations (TPTCs). The TPTCs reveal more accurately the process of ring current injection, with the main results being the following: (1) an intense convection electric field can effectively energize and inject plasma sheet particles into the ring current region within 1–3 h. (2) Injected ions often follow chaotic trajectories in non-adiabatic regions, which may have implications in storm and ring current physics. (3) The shielding electric field, which arises as a consequence of enhanced convection and co-exists with the injection and convection electric field, may cause the original open trajectories of injected ions with higher energy to change into closed ones, thus playing a role in the formation of the symmetric ring current.


2003 ◽  
Vol 55 (7) ◽  
pp. 427-435 ◽  
Author(s):  
P. Ballatore ◽  
W. D. Gonzalez

2015 ◽  
Vol 134 ◽  
pp. 118-129 ◽  
Author(s):  
R.E. Lopez ◽  
W.D. Gonzalez ◽  
V. Vasyliūnas ◽  
I.G. Richardson ◽  
C. Cid ◽  
...  

2004 ◽  
Vol 31 (21) ◽  
pp. n/a-n/a ◽  
Author(s):  
C. Lemon ◽  
R. A. Wolf ◽  
T. W. Hill ◽  
S. Sazykin ◽  
R. W. Spiro ◽  
...  

2008 ◽  
Vol 26 (9) ◽  
pp. 2543-2550 ◽  
Author(s):  
R. Monreal MacMahon ◽  
C. Llop-Romero

Abstract. The ring current growth and decay, characterized by the Dst index, has been studied for thirty years using the Burton et al. (1975) equation. The original formula is based on the restriction of the DPS (Dessler, Parker, and Schoppke) theorem and assuming a constant decay time of particles. The decay time scale is important because the energy injection rate cannot be determined it without the knowledge of this parameter. In a previous work, instead of using a constant value, we introduced the decay time of particles in the energy rate balance equation as a continuous function of the absolute value of the pressure corrected Dst index to avoid the reported discontinuities determining it. Here, based on the DPS restriction, we extend our previous empirical work to obtain analytically the proposed continuous function considering losses due to a global resistive force as a product of viscous-like, and other related dissipation processes. We test our model predicting Dst for a couple of specific storm events and also comparing our results with forecasts of a good reference model appeared in the literature.


2000 ◽  
Vol 27 (9) ◽  
pp. 1371-1374 ◽  
Author(s):  
C. T. Russell ◽  
Gang Lu ◽  
J. G. Luhmann

1990 ◽  
Vol 34 (2) ◽  
pp. 129-136 ◽  
Author(s):  
Ya. I. Feldstein ◽  
V. Yu. Pisarskij ◽  
A. Prigancová ◽  
P. Ivanova

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