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

preprint2022arXivOpen access

Abstract

This paper mainly focus on optimal time decay estimation for large-solution about compressible magnetohydrodynamic equations in 3D whole space, provided that (σ0−1,u0,M0)∈L1∩H2(σ_{0}-1,u_{0},M_{0})\in L^1\cap H^2. In [2](Chen et al.,2019), they proved time decay estimation of ∥(σ−1,u,M)∥H1\|(σ-1,u,M)\|_{H^1} being (1+t)−34(1+t)^{-\frac{3}{4}}. Based on it, we obtained that of ∥∇(σ−1,u,M)∥H1\|\nabla(σ-1,u,M)\|_{H^1} being (1+t)−54(1+t)^{-\frac{5}{4}} in [24]. Therefore, we are committed to improving that of ∥∇2(σ−1,u,M)∥L2\|\nabla^2 (σ-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 ∥∇2(σ−1,u,M)∥L2\|\nabla^2 (σ-1,u,M)\|_{L^2} is (1+t)−74(1+t)^{-\frac{7}{4}}.

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