Sharp decay estimates and asymptotic stability for incompressible MHD equations without viscosity or magnetic diffusion

IF 4.6 Q2 MATERIALS SCIENCE, BIOMATERIALS
Yaowei Xie, Quansen Jiu, Jitao Liu
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引用次数: 0

Abstract

Whether the global existence and uniqueness of strong solutions to n-dimensional incompressible magnetohydrodynamic (MHD for short) equations with only kinematic viscosity or magnetic diffusion holds true or not remains an outstanding open problem. In recent years, stared from the pioneer work by Lin and Zhang (Commun Pure Appl Math 67(4):531–580, 2014), much more attention has been paid to the case when the magnetic field close to an equilibrium state (the background magnetic field for short). Specifically, when the background magnetic field satisfies the Diophantine condition (see (1.2) for details), Chen et al. (Sci China Math 41:1–10, 2022) first studied the perturbation system and established the decay estimates and asymptotic stability of its solutions in 3D periodic domain \(\mathbb {T}^3\), which was then improved to \(H^{(3+2\beta )r+5+(\alpha +2\beta )}(\mathbb {T}^2)\) for 2D periodic domain \(\mathbb {T}^2\) and any \(\alpha >0\), \(\beta >0\) by Zhai (J Differ Equ 374:267–278, 2023). In this paper, we seek to find the optimal decay estimates and improve the space where the global stability is taking place. Through deeply exploring and effectively utilizing the structure of perturbation system, we discover a new dissipative mechanism, which enables us to establish the decay estimates in the Sobolev spaces with much lower regularity. Based on the above discovery, we greatly reduce the initial regularity requirement of aforesaid two works from \(H^{4r+7}(\mathbb {T}^3)\) and \(H^{(3+2\beta )r+5+(\alpha +2\beta )}(\mathbb {T}^2)\) to \(H^{(3r+3)^+}(\mathbb {T}^n)\) for \(r>n-1\) when \(n=3\) and \(n=2\) respectively. Additionally, we first present the linear stability result via the method of spectral analysis in this paper. From which, the decay estimates obtained for the nonlinear system can be seen as sharp in the sense that they are in line with those for the linearized system.

无粘性或磁扩散的不可压缩多流体力学方程的尖锐衰减估计和渐近稳定性
对于只有运动粘度或磁扩散的n维不可压缩磁流体动力学(简称MHD)方程,强解的全局存在性和唯一性是否成立仍然是一个悬而未决的问题。近年来,从 Lin 和 Zhang 的开创性工作(Commun Pure Appl Math 67(4):531-580, 2014)开始,人们开始更多地关注磁场接近平衡态(简称背景磁场)的情况。具体地说,当背景磁场满足二阶条件时(详见(1.2)),Chen et al.(Sci China Math 41:1-10, 2022)首先研究了扰动系统,并建立了其在三维周期域 \(\mathbb {T}^3\) 中的衰减估计和渐近稳定性、随后,对于二维周期域 \(\mathbb {T}^2\) 和任意 \(\alpha >;0), \(\beta >0\) by Zhai (J Differ Equ 374:267-278, 2023).在本文中,我们试图找到最优衰减估计值,并改善全局稳定性发生的空间。通过对扰动系统结构的深入探索和有效利用,我们发现了一种新的耗散机制,它使我们能在规律性更低的索波列夫空间中建立衰减估计。基于上述发现当 \(r>. n-1\) 时,我们大大降低了前述两项工作的初始正则性要求,从 \(H^{4r+7}(\mathbb {T}^3)\) 和 \(H^{(3+2\beta )r+5+(\alpha +2\beta )}(\mathbb {T}^2)\) 降为 \(H^{(3r+3)^+}(\mathbb {T}^n)\)n-1)时分别为(n=3)和(n=2)。此外,本文首先通过谱分析方法给出了线性稳定性结果。由此可见,非线性系统的衰减估计值与线性化系统的衰减估计值是一致的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
ACS Applied Bio Materials
ACS Applied Bio Materials Chemistry-Chemistry (all)
CiteScore
9.40
自引率
2.10%
发文量
464
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