interplanetary magnetic fields
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Author(s):  
Hsien‐Ming Li ◽  
Jih‐Hong Shue ◽  
Satoshi Taguchi ◽  
Masahito Nosé ◽  
Keisuke Hosokawa ◽  
...  

2020 ◽  
Vol 900 (1) ◽  
pp. 63
Author(s):  
Qing Chang ◽  
Xiaojun Xu ◽  
Qi Xu ◽  
Jing Wang ◽  
Jiaying Xu ◽  
...  

2020 ◽  
Author(s):  
Frances Staples ◽  
Jonathan Rae ◽  
Colin Forsyth ◽  
Ashley Smith ◽  
Kyle Murphy ◽  
...  

<p>Under steady-state conditions the magnetopause location is described as a pressure balance between internal magnetic pressures and the external dynamic pressure of the solar wind. The question is, does this approximation hold during more dynamic solar wind features?</p><p>Under more extreme solar wind driving, such as high solar wind pressures or strong southward-directed interplanetary magnetic fields, this boundary is significantly more compressed than in steady-state, playing a significant role in the depletion of magnetospheric plasma from the Van Allen Radiation Belts, via magnetopause shadowing. Large step-changes in solar wind conditions enable the real magnetopause to have a significant time-dependence which empirical models cannot capture.</p><p>We use a database of ~20,000 magnetopause crossings, to determine how the measured magnetopause differs from a statistical model, and under which conditions. We find that observed magnetopause is on average 6% closer to the radiation belts,  with a maximum of 42%, during periods of sudden dynamic pressure enhancement, such as during storm sudden commencement. Our results demonstrate that empirical magnetopause models such as the Shue et al. [1998] model should be used cautiously to interpret energetic electron losses by magnetopause shadowing. </p>


Author(s):  
Shaosui Xu ◽  
David L. Mitchell ◽  
Tristan Weber ◽  
David A. Brain ◽  
Janet G. Luhmann ◽  
...  

2020 ◽  
Vol 12 (1) ◽  
pp. 70-74
Author(s):  
Beena Bhatt ◽  
Harish Chandra

The current article demonstrates the geoeffectiveness of solar flare associated Coronal mass ejection (CME) accompanied with Deca-hectometric (DH) type II radio bursts by comparing the set of events in the rising phase of solar cycle 23rd (1996–2001) and 24th (2009–2014). Our observations are: (i) Solar cycle 23rd have high Dst index than the solar cycle 24th except for the year 1999. (ii) Dst has its peak between 3rd to 5th day after the CME onset for both the solar cycles. (iii) The correlation coefficient between Interplanetary magnetic fields (IMF) and Dst is good for both the solar cycles. (iv) Solar cycle 23rd have very strong correlation between CRI and Dst as compare to solar cycle 24th. Thus, our predictions show that solar cycle 23rd is more geoeffective than solar cycle 24th.


2019 ◽  
Author(s):  
Shaosui Xu ◽  
David L. Mitchell ◽  
Tristan Weber ◽  
David Andrew Brain ◽  
Janet G Luhmann ◽  
...  

2016 ◽  
Author(s):  
Arun Babu Kollamparambil Paul ◽  
H.M Antia ◽  
Shashikant Dugad ◽  
Sunil K Gupta ◽  
Yohio Hayashi ◽  
...  

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