Abstract

We establish the global existence and uniqueness of strong solutions to the initial boundary value problem for the incompressible MHD equations in bounded smooth domains of $\mathbb R^3$ under some suitable smallness conditions. The initial density is allowed to have vacuum, in particular, it can vanish in a set of positive Lebessgue measure. More precisely, under the assumption that the production of the quantities $\|\sqrt\rho_0u_0\|_{L^2(\Omega)}^2+\|H_0\|_{L^2(\Omega)}^2$ and $\|\nabla u_0\|_{L^2(\Omega)}^2+\|\nabla H_0\|_{L^2(\Omega)}^2$ is suitably small, with the smallness depending only on the bound of the initial density and the domain, we prove that there is a unique strong solution to the Dirichlet problem of the incompressible MHD system.

Highlights

  • Magnetohydrodynamics (MHD for short) is the study of the interaction between magnetic fields and moving conducting fluids, which can be described by the following system ρt + div(ρu) = 0, ρ(ut + (u · ∇)u) − μ∆u + ∇p = (∇ × H) × H, Ht − λ∆H = ∇ × (u × H), divu = divH = 0, (1.1) (1.2) (1.3) (1.4)

  • The aim of this paper is to prove the global existence and uniqueness of strong solutions to system (1.1)–(1.6) with the initial data being allowed to have vacuum

  • Recall the boundary condition (1.6) and the identity ∆H = ∇divH − ∇ × (∇ × H), it follows from integrating by parts that

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Summary

Introduction

Is suitably small, with the smallness depending only on the bound of the initial density and the domain, we prove that there is a unique strong solution to the Dirichlet problem of the incompressible MHD system. Incompressible MHD; global existence and uniqueness; strong solutions.

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