2000
DOI: 10.1029/2000ja000006
|View full text |Cite
|
Sign up to set email alerts
|

Reply [to “Comment on ‘Modeling the magnetosphere for northward interplanetary magnetic field: Effects of electrical resistivity’ by Joachim Raeder”]

Abstract: In their comment, Gombosi et al. [this issue] (hereinafter referred to as GPL99) claim that the conclusions reachedby Raeder [1999] (hereinafter referred to as R99) are not correct and not supported by their simulations. Specifically, they raise the issues of (1) results from other codes for northward interplanetary magnetic field (IMF), (2) the inherent numerical resistivity of different schemes, (3) mesh convergence, and (4) the diffusion of the bow shock in the highresistivity cases. Each of these issues w… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
6
0

Year Published

2001
2001
2023
2023

Publication Types

Select...
5
4

Relationship

0
9

Authors

Journals

citations
Cited by 13 publications
(6 citation statements)
references
References 30 publications
0
6
0
Order By: Relevance
“…It has been proposed by Raeder (1999) that the tail length during northward IMF depends strongly on the rate of numerical diffusion. A high diffusion rate results in a partial decoupling between magnetic flux tube motion and plasma convection, leading to a short closed field line region in the tail (see also the following discussion by Gombosi et al, 2000;Raeder, 2000). Figure 11 shows the B y B z vector components of the total magnetic field in tail cross sections at x=−10, −15 and −30 R E after a 2 h run with a constant pure IMF B y field of 5 nT.…”
Section: The Constant Imf Clock Angle Cases: Comparison With Earlier mentioning
confidence: 99%
“…It has been proposed by Raeder (1999) that the tail length during northward IMF depends strongly on the rate of numerical diffusion. A high diffusion rate results in a partial decoupling between magnetic flux tube motion and plasma convection, leading to a short closed field line region in the tail (see also the following discussion by Gombosi et al, 2000;Raeder, 2000). Figure 11 shows the B y B z vector components of the total magnetic field in tail cross sections at x=−10, −15 and −30 R E after a 2 h run with a constant pure IMF B y field of 5 nT.…”
Section: The Constant Imf Clock Angle Cases: Comparison With Earlier mentioning
confidence: 99%
“…Although the previous simulation suggested that the magnetotail length could vary with the reciprocal of the IMF B Z component (1/B Z ) 17,18,27 , and attempted to explained HCA appearance or polar cap disappearance due to dual-lobe reconnections 24,28 , there are still some controversy, e.g. 17,25,26,29,30 and neither study had provided a complete picture or explanation of all observed features.…”
mentioning
confidence: 99%
“…The criticism culminated in a paper by Raeder (2000) that tried to discredit the 8-wave scheme. The subsequent comment and reply exchange (Gombosi et al, 2000;Raeder, 2000) stopped the open criticism, but the underlying skepticism from some competitors still lingers even today.…”
Section: A1 8-wave Riemann Solvermentioning
confidence: 99%