Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
Large-scale energy budget of impulsive magnetic reconnection : Theory and simulation. / Kiehas, S. A.; Volkonskaya, N. N.; Semenov, V. S.; Erkaev, N. V.; Kubyshkin, I. V.; Zaitsev, I. V.
в: JOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICS, Том 122, № 3, 01.03.2017, стр. 3212-3231.Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
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TY - JOUR
T1 - Large-scale energy budget of impulsive magnetic reconnection
T2 - Theory and simulation
AU - Kiehas, S. A.
AU - Volkonskaya, N. N.
AU - Semenov, V. S.
AU - Erkaev, N. V.
AU - Kubyshkin, I. V.
AU - Zaitsev, I. V.
N1 - Funding Information: This work is supported by the Austrian Science Fund (FWF)J3041-N16 and P27012-N27 and by grants 16-05-00470, and 15-05-00879-a from the Russian Foundation of Basic Research. No data were used. Publisher Copyright: ©2017. The Authors. Copyright: Copyright 2017 Elsevier B.V., All rights reserved.
PY - 2017/3/1
Y1 - 2017/3/1
N2 - We evaluate the large-scale energy budget of magnetic reconnection utilizing an analytical time-dependent impulsive reconnection model and a numerical 2-D MHD simulation. With the generalization to compressible plasma, we can investigate changes in the thermal, kinetic, and magnetic energies. We study these changes in three different regions: (a) the region defined by the outflowing plasma (outflow region, OR), (b) the region of compressed magnetic fields above/below the OR (traveling compression region, TCR), and (c) the region trailing the OR and TCR (wake). For incompressible plasma, we find that the decrease inside the OR is compensated by the increase in kinetic energy. However, for the general compressible case, the decrease in magnetic energy inside the OR is not sufficient to explain the increase in thermal and kinetic energy. Hence, energy from other regions needs to be considered. We find that the decrease in thermal and magnetic energy in the wake, together with the decrease in magnetic energy inside the OR, is sufficient to feed the increase in kinetic and thermal energies in the OR and the increase in magnetic and thermal energies inside the TCR. That way, the energy budget is balanced, but consequently, not all magnetic energy is converted into kinetic and thermal energies of the OR. Instead, a certain fraction gets transfered into the TCR. As an upper limit of the efficiency of reconnection (magnetic energy → kinetic energy) we find ηeff=1/2. A numerical simulation is used to include a finite thickness of the current sheet, which shows the importance of the pressure gradient inside the OR for the conversion of kinetic energy into thermal energy.
AB - We evaluate the large-scale energy budget of magnetic reconnection utilizing an analytical time-dependent impulsive reconnection model and a numerical 2-D MHD simulation. With the generalization to compressible plasma, we can investigate changes in the thermal, kinetic, and magnetic energies. We study these changes in three different regions: (a) the region defined by the outflowing plasma (outflow region, OR), (b) the region of compressed magnetic fields above/below the OR (traveling compression region, TCR), and (c) the region trailing the OR and TCR (wake). For incompressible plasma, we find that the decrease inside the OR is compensated by the increase in kinetic energy. However, for the general compressible case, the decrease in magnetic energy inside the OR is not sufficient to explain the increase in thermal and kinetic energy. Hence, energy from other regions needs to be considered. We find that the decrease in thermal and magnetic energy in the wake, together with the decrease in magnetic energy inside the OR, is sufficient to feed the increase in kinetic and thermal energies in the OR and the increase in magnetic and thermal energies inside the TCR. That way, the energy budget is balanced, but consequently, not all magnetic energy is converted into kinetic and thermal energies of the OR. Instead, a certain fraction gets transfered into the TCR. As an upper limit of the efficiency of reconnection (magnetic energy → kinetic energy) we find ηeff=1/2. A numerical simulation is used to include a finite thickness of the current sheet, which shows the importance of the pressure gradient inside the OR for the conversion of kinetic energy into thermal energy.
KW - magnetic reconnection
KW - magnetospheric physics
KW - plasma physics
KW - substorms
UR - http://www.scopus.com/inward/record.url?scp=85015278139&partnerID=8YFLogxK
U2 - 10.1002/2016JA023169
DO - 10.1002/2016JA023169
M3 - Article
VL - 122
SP - 3212
EP - 3231
JO - Journal of Geophysical Research: Biogeosciences
JF - Journal of Geophysical Research: Biogeosciences
SN - 0148-0227
IS - 3
ER -
ID: 7743261