Vanishing Viscosity Limit to Planar Rarefaction Wave with Vacuum for 3D Compressible Navier-Stokes Equations

X. Bian, Yi Wang null, Lingyao Xie
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引用次数: 2

Abstract

. The vanishing viscosity limit of the three-dimensional (3D) compressible and isentropic Navier-Stokes equations is proved in the case that the corresponding 3D inviscid Euler equations admit a planar rarefaction wave so-lution connected with vacuum states. Moreover, a uniform convergence rate with respect to the viscosity coefficients is obtained. Compared with previous results on the zero dissipation limit to planar rarefaction wave away from vacuum states [27, 28], the new ingredients and main difficulties come from the degeneracy of vacuum states in the planar rarefaction wave in the multi-dimensional setting. Suitable cut-off techniques and some delicate estimates are needed near the vacuum states. The inviscid decay rate around the planar rarefaction wave with vacuum is determined by the cut-off parameter and the nonlinear advection flux terms of 3D compressible Navier-Stokes equations.
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三维可压缩Navier-Stokes方程在真空条件下平面稀疏波的消失粘度极限
. 证明了三维可压缩等熵Navier-Stokes方程在三维无粘欧拉方程中存在与真空态相关的平面稀疏波解的情况下,黏度的消失极限。此外,还得到了相对于黏度系数的均匀收敛速率。与以往关于平面稀薄波远离真空状态的零耗散极限的结果相比[27,28],新的组成部分和主要困难来自于平面稀薄波在多维环境下真空状态的简并。在真空状态附近需要适当的截止技术和精确的估计。三维可压缩Navier-Stokes方程的截止参数和非线性平流通量项决定了真空平面稀薄波周围的无粘衰减率。
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