Optimal time decay estimation for large-solution about 3D compressible MHD equations

Abstract

This paper mainly focus on optimal time decay estimation for large-solution about compressible magnetohydrodynamic equations in 3D whole space, provided that (Οƒ0βˆ’1,u0,M0)∈L1∩H2(\sigma_{0}-1,u_{0},M_{0})\in L^1\cap H^2. In [2](Chen et al.,2019), they proved time decay estimation of βˆ₯(Οƒβˆ’1,u,M)βˆ₯H1\|(\sigma-1,u,M)\|_{H^1} being (1+t)βˆ’34(1+t)^{-\frac{3}{4}}. Based on it, we obtained that of βˆ₯βˆ‡(Οƒβˆ’1,u,M)βˆ₯H1\|\nabla(\sigma-1,u,M)\|_{H^1} being (1+t)βˆ’54(1+t)^{-\frac{5}{4}} in [24]. Therefore, we are committed to improving that of βˆ₯βˆ‡2(Οƒβˆ’1,u,M)βˆ₯L2\|\nabla^2 (\sigma-1,u,M)\|_{L^2} in this paper. Thanks to the method adopted in [25] (Wang and Wen, 2021), we get the optimal time decay estimation to the highest-order derivative for space of solution, which means that time decay estimation of βˆ₯βˆ‡2(Οƒβˆ’1,u,M)βˆ₯L2\|\nabla^2 (\sigma-1,u,M)\|_{L^2} is (1+t)βˆ’74(1+t)^{-\frac{7}{4}}

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