Development of Strongly Dissipative Mhd Structures

A plasma flow near a stagnation point, which may be produced by a local squeezing in one direction with outflow on both sides of a central channel, convects a magnetic field towards the inner layer, while enhancement of the initial magnetic energy and formation of a current sheet with intense Joule...

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Autores principales: Gratton, Fausto Tulio Livio, Gnavi, Graciela Delia, Bender, Laurence E.
Publicado: 1992
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Acceso en línea:https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_00933813_v20_n6_p882_Gratton
http://hdl.handle.net/20.500.12110/paper_00933813_v20_n6_p882_Gratton
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spelling paper:paper_00933813_v20_n6_p882_Gratton2023-06-08T15:08:33Z Development of Strongly Dissipative Mhd Structures Gratton, Fausto Tulio Livio Gnavi, Graciela Delia Bender, Laurence E. Magnetic fields Magnetohydrodynamics Numerical analysis Current sheets Joule dissipation Magnetic energy Plasma stability A plasma flow near a stagnation point, which may be produced by a local squeezing in one direction with outflow on both sides of a central channel, convects a magnetic field towards the inner layer, while enhancement of the initial magnetic energy and formation of a current sheet with intense Joule dissipation rates take place when the magnetic Reynolds number is large. In systems with no magnetic flux injection, starting from a generic initial magnetic field and after a transient in which amplification followed by annihilation of the odd component occurs, a large even magnetic remnant concentrated in a thin slab is formed in a few hydrodynamic times. If the pressure gradient that drives the motion is switched off, the magnetic field extinguishes at a much slower pace than the corresponding buildup process. When there is continuous magnetic flux injection, the even component of the magnetic field, in general, becomes dominant over the odd part after some number of hydrodynamic times. For astrophysical plasmas the significance of the mechanism considered here is that i) fast dissipation of magnetic energy does not invoke anomalous resistivity, and ii) neutral sublayers where change of sign of magnetic field occurs may vanish during the current sheet evolution, so that steady-state configurations prone to processes of reconnection or tearing instabilities do not develop. © 1992 IEEE Fil:Gratton, F.T. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Gnavi, G. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Bender, L. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. 1992 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_00933813_v20_n6_p882_Gratton http://hdl.handle.net/20.500.12110/paper_00933813_v20_n6_p882_Gratton
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Magnetic fields
Magnetohydrodynamics
Numerical analysis
Current sheets
Joule dissipation
Magnetic energy
Plasma stability
spellingShingle Magnetic fields
Magnetohydrodynamics
Numerical analysis
Current sheets
Joule dissipation
Magnetic energy
Plasma stability
Gratton, Fausto Tulio Livio
Gnavi, Graciela Delia
Bender, Laurence E.
Development of Strongly Dissipative Mhd Structures
topic_facet Magnetic fields
Magnetohydrodynamics
Numerical analysis
Current sheets
Joule dissipation
Magnetic energy
Plasma stability
description A plasma flow near a stagnation point, which may be produced by a local squeezing in one direction with outflow on both sides of a central channel, convects a magnetic field towards the inner layer, while enhancement of the initial magnetic energy and formation of a current sheet with intense Joule dissipation rates take place when the magnetic Reynolds number is large. In systems with no magnetic flux injection, starting from a generic initial magnetic field and after a transient in which amplification followed by annihilation of the odd component occurs, a large even magnetic remnant concentrated in a thin slab is formed in a few hydrodynamic times. If the pressure gradient that drives the motion is switched off, the magnetic field extinguishes at a much slower pace than the corresponding buildup process. When there is continuous magnetic flux injection, the even component of the magnetic field, in general, becomes dominant over the odd part after some number of hydrodynamic times. For astrophysical plasmas the significance of the mechanism considered here is that i) fast dissipation of magnetic energy does not invoke anomalous resistivity, and ii) neutral sublayers where change of sign of magnetic field occurs may vanish during the current sheet evolution, so that steady-state configurations prone to processes of reconnection or tearing instabilities do not develop. © 1992 IEEE
author Gratton, Fausto Tulio Livio
Gnavi, Graciela Delia
Bender, Laurence E.
author_facet Gratton, Fausto Tulio Livio
Gnavi, Graciela Delia
Bender, Laurence E.
author_sort Gratton, Fausto Tulio Livio
title Development of Strongly Dissipative Mhd Structures
title_short Development of Strongly Dissipative Mhd Structures
title_full Development of Strongly Dissipative Mhd Structures
title_fullStr Development of Strongly Dissipative Mhd Structures
title_full_unstemmed Development of Strongly Dissipative Mhd Structures
title_sort development of strongly dissipative mhd structures
publishDate 1992
url https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_00933813_v20_n6_p882_Gratton
http://hdl.handle.net/20.500.12110/paper_00933813_v20_n6_p882_Gratton
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AT gnavigracieladelia developmentofstronglydissipativemhdstructures
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