2020
DOI: 10.1007/s41614-019-0037-x
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Evolution of auroral substorm as viewed from MHD simulations: dynamics, energy transfer and energy conversion

Abstract: An auroral substorm is a visual manifestation of large-scale, transient disturbances taking place in space surrounding the Earth, and is one of the central issues in the space plasma physics. While a number of studies have been conducted, a unified picture of the overall evolution of the auroral substorm has not been drawn. This paper is aimed to overview the recently obtained results of global magnetohydrodynamics (MHD) simulations in a context of a priori presence of anomalous resistivity leading to magnetic… Show more

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Cited by 4 publications
(4 citation statements)
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References 218 publications
(281 reference statements)
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“…However, if we extract a time series, in the LT and R mentioned above we should get, after IMF orientation change, spikes in energy conversion when this setting is oscillating around position 7.64. In Figure 11b, after ∼77 min we observe a peak in the rate of conversion of magnetic energy into kinetic and internal energy, characteristic and also consistent with Load (Birn & Hesse, 2005; Ebihara & Tanaka, 2020). In this way, we find that the median of the energy conversion components, Figure 11a around the position R = 7.64 R E , is a representative amount of the energy conversion during the phase in which B z changes orientation.…”
Section: Resultssupporting
confidence: 85%
See 1 more Smart Citation
“…However, if we extract a time series, in the LT and R mentioned above we should get, after IMF orientation change, spikes in energy conversion when this setting is oscillating around position 7.64. In Figure 11b, after ∼77 min we observe a peak in the rate of conversion of magnetic energy into kinetic and internal energy, characteristic and also consistent with Load (Birn & Hesse, 2005; Ebihara & Tanaka, 2020). In this way, we find that the median of the energy conversion components, Figure 11a around the position R = 7.64 R E , is a representative amount of the energy conversion during the phase in which B z changes orientation.…”
Section: Resultssupporting
confidence: 85%
“…Three types of energy densities which correspond to the terms to the right‐hand side of Equations in the MHD approximation are analyzed here, namely, magnetic ( E m ), internal ( E i ) and kinetic ( E k ) energies (Birn & Hesse, 2005; Ebihara & Tanaka, 2017, 2020), and their equations are defined in units of (nW/m 3 ) as follows: Em=V()trueJ×trueB, ${E}_{m}=-\vec{V}\cdot \left(\vec{J}\times \vec{B}\right),$ Ei=VP, ${E}_{i}=\vec{V}\cdot \nabla P,$ Ek=V()trueJ×trueBP,0.3333em0.3333em ${E}_{k}=\vec{V}\cdot \left(\vec{J}\times \vec{B}-\nabla P\right),\ \ $ where trueV $\vec{V}$ is the plasma bulk velocity, trueB $\vec{B}$ is the magnetic field vector, trueJ $\vec{J}$ is the plasma current density as derived from Ampère's law, and P is the plasma pressure. Notice that Equations has dimensions of energy density flux, that is, Watt/m 3 , but hereafter we will refer to them only as either of the three energy forms mentioned above, that is, magnetic energy, kinetic energy, and internal energy.…”
Section: Methodsmentioning
confidence: 99%
“…The S‐M interactions are indispensable to generate the plasma regimes inside the magnetosphere. The energy source of the FAC is inside the magnetosphere (Ebihara & Tanaka, 2017, 2020). The thermal energy in the plasma regimes becomes energy of Poynting flux associated with the FAC.…”
Section: Discussionmentioning
confidence: 99%
“…In addition, field‐parallel flow (squeezing flow) from the NENL reaches the inner magnetosphere away from the equatorial plane, earlier than flow in the equatorial plane (Tanaka, Ebihara, et al., 2017). The near‐Earth dynamo forms following the occurrence of these flows (Ebihara and Tanaka, 2015, 2020). Figure 14 schematically draws the generation mechanism of the near‐Earth dynamos.…”
Section: Applications To Individual Structuresmentioning
confidence: 99%