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A global stability result for incompressible magnetohydrodynamics

Livio Pizzocchero, Emanuele Tassi

TL;DR

This work proves a global stability result for the homogeneous, incompressible MHD system on the torus $\mathbf{T}^d$ with positive viscosity $\nu$ and resistivity $\eta$, in a $C^\infty$ setting and with fully explicit $H^p$-norm estimates. The authors develop an a posteriori framework based on approximate solutions, recasting the MHD equations via a linear operator $\mathscr{A}$ and a bilinear map $\mathscr{P}$, and establish quantitative control inequalities that guarantee global existence and decay of perturbations around a given global decaying solution $\mathbf{v}$. A key contribution is a global stability theorem that provides explicit bounds on the distance between nearby solutions and the decaying reference solution, with constants determined by Sobolev norms of $\mathbf{v}$ and integrals of its norms in time. The paper also introduces generalized Beltrami pairs as large-data initial configurations that yield global, decaying MHD solutions, and shows these data can have arbitrarily large $H^p$-norms, enriching the landscape of explicitly controllable MHD dynamics.

Abstract

We propose a result of global stability for the equations of homogeneous, incompressible magnetohydrodynamics (MHD) on a torus of any dimension $d \in \{2,3,...\}$, with positive viscosity and resistivity. This result applies to the $C^\infty$ global solutions, with a conveniently defined decay property for large times; it is expressed by fully explicit estimates, formulated via $H^p$-type Sobolev norms of arbitrarily high order $p$. The present stability result is similar to that proposed by one of us for the Navier-Stokes (NS) equation \cite{glosta}; it is derived from a suitable formulation of the MHD equations proposed in our previous work \cite{MHD}, emphasizing strong structural analogies with the NS case. A basic tool in the proof of the present stability result is a general theory of approximate solutions of the MHD Cauchy problem, that we developed in \cite{MHD} on the grounds of previous results on the NS equation \cite{smooth} and of the above structural similarities. We also introduce a class of Beltrami-type initial data for the MHD equations; although being arbitrarily large, these data produce global and decaying MHD solutions, fitting the framework of the present stability result. Comparisons with the previous literature on these subjects are performed.

A global stability result for incompressible magnetohydrodynamics

TL;DR

This work proves a global stability result for the homogeneous, incompressible MHD system on the torus with positive viscosity and resistivity , in a setting and with fully explicit -norm estimates. The authors develop an a posteriori framework based on approximate solutions, recasting the MHD equations via a linear operator and a bilinear map , and establish quantitative control inequalities that guarantee global existence and decay of perturbations around a given global decaying solution . A key contribution is a global stability theorem that provides explicit bounds on the distance between nearby solutions and the decaying reference solution, with constants determined by Sobolev norms of and integrals of its norms in time. The paper also introduces generalized Beltrami pairs as large-data initial configurations that yield global, decaying MHD solutions, and shows these data can have arbitrarily large -norms, enriching the landscape of explicitly controllable MHD dynamics.

Abstract

We propose a result of global stability for the equations of homogeneous, incompressible magnetohydrodynamics (MHD) on a torus of any dimension , with positive viscosity and resistivity. This result applies to the global solutions, with a conveniently defined decay property for large times; it is expressed by fully explicit estimates, formulated via -type Sobolev norms of arbitrarily high order . The present stability result is similar to that proposed by one of us for the Navier-Stokes (NS) equation \cite{glosta}; it is derived from a suitable formulation of the MHD equations proposed in our previous work \cite{MHD}, emphasizing strong structural analogies with the NS case. A basic tool in the proof of the present stability result is a general theory of approximate solutions of the MHD Cauchy problem, that we developed in \cite{MHD} on the grounds of previous results on the NS equation \cite{smooth} and of the above structural similarities. We also introduce a class of Beltrami-type initial data for the MHD equations; although being arbitrarily large, these data produce global and decaying MHD solutions, fitting the framework of the present stability result. Comparisons with the previous literature on these subjects are performed.
Paper Structure (6 sections, 92 equations)