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Global existence and stability of viscous Alfvén waves in the large-box limit for MHD systems

Li Xu, Jiahui Zhang

Abstract

This paper rigorously analyzes how the {\it large box limit} fundamentally alters the global existence theory and dynamics behavior of the incompressible magnetohydrodynamics (MHD) system with small viscosity/resistivity $(0<μ\ll 1)$ on periodic domains $Q_L=[-L,L]^3$, in presence of a strong background magnetic field. While the existence of global solutions (viscous Alfvén waves) on the whole space $\R^3$ was previously established in \cite{He-Xu-Yu}, such results cannot be expected for general finite periodic domains. We demonstrate that global solutions do exist on the torus $Q_L=[-L,L]^3$ precisely when the domain exceeds a size $L_μ>e^{\f1μ}$, providing the first quantitative characterization of the transition to infinite-domain-like behavior.

Global existence and stability of viscous Alfvén waves in the large-box limit for MHD systems

Abstract

This paper rigorously analyzes how the {\it large box limit} fundamentally alters the global existence theory and dynamics behavior of the incompressible magnetohydrodynamics (MHD) system with small viscosity/resistivity on periodic domains , in presence of a strong background magnetic field. While the existence of global solutions (viscous Alfvén waves) on the whole space was previously established in \cite{He-Xu-Yu}, such results cannot be expected for general finite periodic domains. We demonstrate that global solutions do exist on the torus precisely when the domain exceeds a size , providing the first quantitative characterization of the transition to infinite-domain-like behavior.

Paper Structure

This paper contains 37 sections, 29 theorems, 653 equations.

Key Result

Theorem 1.1

Let $B_0 = (0,0,1)$, $N^* \in \mathbb{Z}_{\geq 7}$, $0<\mu\ll1$, $R\gg 1$ and $L\geq e^{\frac{1}{\mu}}$. There exists a universal constant $\varepsilon_0\in (0,1)$, independent of both the viscosity coefficient $\mu$ and the domain scale $L$, such that if the initial divergence-free vector fields $( then eq:MHD-initial admits a unique solution $(z_{+}(t,x),z_{-}(t,x))$ on $[0,\log L]\times Q_L$ sa

Theorems & Definitions (60)

  • Theorem 1.1: Local existence of the solution
  • Remark 1.1
  • Theorem 1.2: Global existence and dynamics
  • Remark 1.2
  • Lemma 2.1
  • Lemma 2.2
  • proof
  • Remark 2.1
  • Lemma 2.3: weighted Sobolev inequality
  • proof
  • ...and 50 more