Global stability of rarefaction wave for the outflow problem governed by the radiative Euler equations

IF 1.2 2区 数学 Q1 MATHEMATICS Indiana University Mathematics Journal Pub Date : 2022-01-01 DOI:10.1512/iumj.2022.71.8925
Lili Fan, Lizhi Ruan, Wei Xiang
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Abstract

This paper is devoted to the study of the initial-boundary value problem for the radiative full Euler equations, which are a fundamental system in the radiative hydrodynamics with many practical applications in astrophysical and nuclear phenomena. It turns out that the pattern of the asymptotic states is not unique and depends on the data both on the boundary and at the far field. In this paper, we focus our attention on the outflow problem when the flow velocity on the boundary is negative, and give a rigorous proof of the asymptotic stability of the rarefaction wave without restrictions on the smallness of the wave strength. Different from our previous work on the inflow problem for the radiative Euler equations in [6], lack of boundary conditions on the density and velocity prevents us from applying the integration by part to derive the energy estimates directly. So the outflow problem is more challenging in mathematical analysis than the inflow problem studied in [6]. New weighted energy estimates are introduced and the trace of the density and velocity on the boundary are handled by some subtle analysis. The weight is chosen based on the new observation on the key decay properties of the smooth rarefaction wave. Our investigations on the inflow and outflow problem provide a good understanding on the radiative effect and boundary effect in the setting of rarefaction wave.
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辐射欧拉方程下外流问题稀疏波的全局稳定性
本文研究了辐射全欧拉方程的初边值问题。辐射全欧拉方程是辐射流体力学中的一个基本系统,在天体物理和核现象中有许多实际应用。结果表明,渐近态的模式不是唯一的,它取决于边界和远场的数据。本文研究了边界上流速为负时的流出问题,给出了不受波强小限制的稀疏波的渐近稳定性的严格证明。与我们之前在[6]中对辐射欧拉方程的入流问题的研究不同,由于缺乏密度和速度的边界条件,我们无法直接应用部分积分法来推导能量估计。因此流出问题在数学分析上比b[6]研究的流入问题更具挑战性。引入了新的加权能量估计,并对密度和速度在边界上的轨迹进行了精细的分析处理。权重的选择是基于对光滑稀薄波关键衰减特性的新观测。我们对流入和流出问题的研究,对稀薄波背景下的辐射效应和边界效应有了较好的认识。
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2.10
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0.00%
发文量
52
审稿时长
4.5 months
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