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@ARTICLE{Effenberger:15157,
author = {Effenberger, F. and Thust, K. and Arnold, L. and Grauer, R.
and Dreher, J.},
title = {{N}umerical simulation of current sheet formation in a
quasiseparatrix layer using adaptive mesh refinement},
journal = {Physics of plasmas},
volume = {18},
issn = {1070-664X},
address = {[S.l.]},
publisher = {American Institute of Physics},
reportid = {PreJuSER-15157},
pages = {032902},
year = {2011},
note = {This work was supported by Deutsche Forschungsgemeinschaft
through Forschergruppe FOR 1048 and by the European
Commission through the Solaire network (Grant No.
MTRN-CT-2006-035484).},
abstract = {The formation of a thin current sheet in a magnetic
quasiseparatrix layer (QSL) is investigated by means of
numerical simulation using a simplified ideal, low-beta, MHD
model. The initial configuration and driving boundary
conditions are relevant to phenomena observed in the solar
corona and were studied earlier by Aulanier et al. [Astron.
Astrophys. 444, 961 (2005)]. In extension to that work, we
use the technique of adaptive mesh refinement (AMR) to
significantly enhance the local spatial resolution of the
current sheet during its formation, which enables us to
follow the evolution into a later stage. Our simulations are
in good agreement with the results of Aulanier et al. up to
the calculated time in that work. In a later phase, we
observe a basically unarrested collapse of the sheet to
length scales that are more than one order of magnitude
smaller than those reported earlier. The current density
attains correspondingly larger maximum values within the
sheet. During this thinning process, which is finally
limited by lack of resolution even in the AMR studies, the
current sheet moves upward, following a global expansion of
the magnetic structure during the quasistatic evolution. The
sheet is locally one-dimensional and the plasma flow in its
vicinity, when transformed into a comoving frame,
qualitatively resembles a stagnation point flow. In
conclusion, our simulations support the idea that extremely
high current densities are generated in the vicinities of
QSLs as a response to external perturbations, with no sign
of saturation. (C) 2011 American Institute of Physics.
[doi:10.1063/1.3565018]},
keywords = {J (WoSType)},
cin = {JSC},
ddc = {530},
cid = {I:(DE-Juel1)JSC-20090406},
pnm = {Scientific Computing (FUEK411) / 411 - Computational
Science and Mathematical Methods (POF2-411)},
pid = {G:(DE-Juel1)FUEK411 / G:(DE-HGF)POF2-411},
shelfmark = {Physics, Fluids $\&$ Plasmas},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000289151900055},
doi = {10.1063/1.3565018},
url = {https://juser.fz-juelich.de/record/15157},
}