Relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approach

Abstract We derive the relativistic non-resistive, viscous second-order magnetohydrodynamic equations for the dissipative quantities using the relaxation time approximation. The Boltzmann equation is solved for a system of particles and antiparticles using Chapman-Enskog like gradient expansion of t...

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Main Authors: Ankit Kumar Panda, Ashutosh Dash, Rajesh Biswas, Victor Roy
Format: Article
Language:English
Published: SpringerOpen 2021-03-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP03(2021)216
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spelling doaj-e6c2ca7a6c024ba495f5b1b342ff5fd32021-03-28T11:07:04ZengSpringerOpenJournal of High Energy Physics1029-84792021-03-012021313210.1007/JHEP03(2021)216Relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approachAnkit Kumar Panda0Ashutosh Dash1Rajesh Biswas2Victor Roy3School of Physical Sciences, National Institute of Science Education and Research, HBNISchool of Physical Sciences, National Institute of Science Education and Research, HBNISchool of Physical Sciences, National Institute of Science Education and Research, HBNISchool of Physical Sciences, National Institute of Science Education and Research, HBNIAbstract We derive the relativistic non-resistive, viscous second-order magnetohydrodynamic equations for the dissipative quantities using the relaxation time approximation. The Boltzmann equation is solved for a system of particles and antiparticles using Chapman-Enskog like gradient expansion of the single-particle distribution function truncated at second order. In the first order, the transport coefficients are independent of the magnetic field. In the second-order, new transport coefficients that couple magnetic field and the dissipative quantities appear which are different from those obtained in the 14-moment approximation [1] in the presence of a magnetic field. However, in the limit of the weak magnetic field, the form of these equations are identical to the 14-moment approximation albeit with different values of these coefficients. We also derive the anisotropic transport coefficients in the Navier-Stokes limit.https://doi.org/10.1007/JHEP03(2021)216Phenomenological ModelsHeavy Ion Phenomenology
collection DOAJ
language English
format Article
sources DOAJ
author Ankit Kumar Panda
Ashutosh Dash
Rajesh Biswas
Victor Roy
spellingShingle Ankit Kumar Panda
Ashutosh Dash
Rajesh Biswas
Victor Roy
Relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approach
Journal of High Energy Physics
Phenomenological Models
Heavy Ion Phenomenology
author_facet Ankit Kumar Panda
Ashutosh Dash
Rajesh Biswas
Victor Roy
author_sort Ankit Kumar Panda
title Relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approach
title_short Relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approach
title_full Relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approach
title_fullStr Relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approach
title_full_unstemmed Relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approach
title_sort relativistic non-resistive viscous magnetohydrodynamics from the kinetic theory: a relaxation time approach
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-03-01
description Abstract We derive the relativistic non-resistive, viscous second-order magnetohydrodynamic equations for the dissipative quantities using the relaxation time approximation. The Boltzmann equation is solved for a system of particles and antiparticles using Chapman-Enskog like gradient expansion of the single-particle distribution function truncated at second order. In the first order, the transport coefficients are independent of the magnetic field. In the second-order, new transport coefficients that couple magnetic field and the dissipative quantities appear which are different from those obtained in the 14-moment approximation [1] in the presence of a magnetic field. However, in the limit of the weak magnetic field, the form of these equations are identical to the 14-moment approximation albeit with different values of these coefficients. We also derive the anisotropic transport coefficients in the Navier-Stokes limit.
topic Phenomenological Models
Heavy Ion Phenomenology
url https://doi.org/10.1007/JHEP03(2021)216
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