Fluid simulations of non-resonant anisotropic ion heating

The finite Larmor radius (FLR)-Landau fluid model, which extends the usual anisotropic magnetohydrodynamics to magnetized collisionless plasmas by retaining linear Landau damping and finite Larmor radius corrections down to the sub-ionic scales in the quasi-transverse directions, is used to stud...

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Main Authors: D. Laveder, T. Passot, P. L. Sulem
Format: Article
Language:English
Published: Copernicus Publications 2013-07-01
Series:Annales Geophysicae
Online Access:https://www.ann-geophys.net/31/1195/2013/angeo-31-1195-2013.pdf
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spelling doaj-a9cdbc463f6c436fa728ce5d21e1ebfa2020-11-24T23:15:14ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762013-07-01311195120410.5194/angeo-31-1195-2013Fluid simulations of non-resonant anisotropic ion heatingD. Laveder0T. Passot1P. L. Sulem2Université de Nice-Sophia Antipolis, CNRS, UMR7293, Observatoire de la Côte d'Azur, BP 4229, 06304 Nice Cedex 4, FranceUniversité de Nice-Sophia Antipolis, CNRS, UMR7293, Observatoire de la Côte d'Azur, BP 4229, 06304 Nice Cedex 4, FranceUniversité de Nice-Sophia Antipolis, CNRS, UMR7293, Observatoire de la Côte d'Azur, BP 4229, 06304 Nice Cedex 4, FranceThe finite Larmor radius (FLR)-Landau fluid model, which extends the usual anisotropic magnetohydrodynamics to magnetized collisionless plasmas by retaining linear Landau damping and finite Larmor radius corrections down to the sub-ionic scales in the quasi-transverse directions, is used to study the non-resonant heating of the plasma by randomly driven Alfvén waves. One-dimensional numerical simulations, free from any artificial dissipation, are used to analyze the influence on the thermal dynamics, of the beta parameter and of the separation between the driving and the ion scales. While the gyrotropic heat fluxes play a dominant role when the plasma is driven at large scales, leading to a parallel heating of the ions by Landau damping, a different regime develops when the driving acts at scales comparable to the ion Larmor radius. Perpendicular heating and parallel cooling of the ions are then observed, an effect that is mostly due to the work of the non-gyrotropic pressure force and that can be viewed as the fluid signature of the so-called stochastic heating. A partial characterization of the plasma by global quantities (such as the magnetic compressibility and the density-magnetic field correlations that provide information on the dominant type of waves) is also presented. The enhancement of the parallel electron heating by a higher level of fast magnetosonic waves is in particular pointed out.https://www.ann-geophys.net/31/1195/2013/angeo-31-1195-2013.pdf
collection DOAJ
language English
format Article
sources DOAJ
author D. Laveder
T. Passot
P. L. Sulem
spellingShingle D. Laveder
T. Passot
P. L. Sulem
Fluid simulations of non-resonant anisotropic ion heating
Annales Geophysicae
author_facet D. Laveder
T. Passot
P. L. Sulem
author_sort D. Laveder
title Fluid simulations of non-resonant anisotropic ion heating
title_short Fluid simulations of non-resonant anisotropic ion heating
title_full Fluid simulations of non-resonant anisotropic ion heating
title_fullStr Fluid simulations of non-resonant anisotropic ion heating
title_full_unstemmed Fluid simulations of non-resonant anisotropic ion heating
title_sort fluid simulations of non-resonant anisotropic ion heating
publisher Copernicus Publications
series Annales Geophysicae
issn 0992-7689
1432-0576
publishDate 2013-07-01
description The finite Larmor radius (FLR)-Landau fluid model, which extends the usual anisotropic magnetohydrodynamics to magnetized collisionless plasmas by retaining linear Landau damping and finite Larmor radius corrections down to the sub-ionic scales in the quasi-transverse directions, is used to study the non-resonant heating of the plasma by randomly driven Alfvén waves. One-dimensional numerical simulations, free from any artificial dissipation, are used to analyze the influence on the thermal dynamics, of the beta parameter and of the separation between the driving and the ion scales. While the gyrotropic heat fluxes play a dominant role when the plasma is driven at large scales, leading to a parallel heating of the ions by Landau damping, a different regime develops when the driving acts at scales comparable to the ion Larmor radius. Perpendicular heating and parallel cooling of the ions are then observed, an effect that is mostly due to the work of the non-gyrotropic pressure force and that can be viewed as the fluid signature of the so-called stochastic heating. A partial characterization of the plasma by global quantities (such as the magnetic compressibility and the density-magnetic field correlations that provide information on the dominant type of waves) is also presented. The enhancement of the parallel electron heating by a higher level of fast magnetosonic waves is in particular pointed out.
url https://www.ann-geophys.net/31/1195/2013/angeo-31-1195-2013.pdf
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