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Main Authors: Cobb, Dimitri, del Pino, Daniel Sánchez-Simón, Velázquez, Juan J. L.
Format: Preprint
Published: 2025
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Online Access:https://arxiv.org/abs/2503.24055
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author Cobb, Dimitri
del Pino, Daniel Sánchez-Simón
Velázquez, Juan J. L.
author_facet Cobb, Dimitri
del Pino, Daniel Sánchez-Simón
Velázquez, Juan J. L.
contents In this article we study a one dimensional model for Magnetic Relaxation. This model was introduced by Moffatt and describes a low resistivity viscous plasma, in which the pressure and the inercia are much smaller than the magnetic pressure. In the limit of resistivity $\varepsilon\rightarrow 0$, we prove the existence of two time scales for the evolution of the magnetic field: a fast one for times of order $\log(\varepsilon^{-1})$ in which the resistivity plays no role and the energy is dissipated only via viscosity; and a slow one for times of order $\varepsilon^{-1}$ characterized by the influence of the resistivity. We show that in this second time scale, as $\varepsilon\rightarrow 0$, the modulus of magnetic field approaches a function that depends only on time. We also prove that, in this regime, the magnetic field $b_\varepsilon(t,x)$ can be approximated as $\varepsilon \rightarrow 0$ by the solution of a PDE whose solutions exhibit blow up for some choices of initial data.
format Preprint
id arxiv_https___arxiv_org_abs_2503_24055
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Effective Dynamics and Blow Up in a Model of Magnetic Relaxation
Cobb, Dimitri
del Pino, Daniel Sánchez-Simón
Velázquez, Juan J. L.
Analysis of PDEs
Mathematical Physics
Plasma Physics
35Q35 (main), 76W05, 35B25, 35B40, 35B44 (secondary)
In this article we study a one dimensional model for Magnetic Relaxation. This model was introduced by Moffatt and describes a low resistivity viscous plasma, in which the pressure and the inercia are much smaller than the magnetic pressure. In the limit of resistivity $\varepsilon\rightarrow 0$, we prove the existence of two time scales for the evolution of the magnetic field: a fast one for times of order $\log(\varepsilon^{-1})$ in which the resistivity plays no role and the energy is dissipated only via viscosity; and a slow one for times of order $\varepsilon^{-1}$ characterized by the influence of the resistivity. We show that in this second time scale, as $\varepsilon\rightarrow 0$, the modulus of magnetic field approaches a function that depends only on time. We also prove that, in this regime, the magnetic field $b_\varepsilon(t,x)$ can be approximated as $\varepsilon \rightarrow 0$ by the solution of a PDE whose solutions exhibit blow up for some choices of initial data.
title Effective Dynamics and Blow Up in a Model of Magnetic Relaxation
topic Analysis of PDEs
Mathematical Physics
Plasma Physics
35Q35 (main), 76W05, 35B25, 35B40, 35B44 (secondary)
url https://arxiv.org/abs/2503.24055