Partially dissipative systems in the critical regularity setting, and strong relaxation limit

IF 1.3 Q1 MATHEMATICS
R. Danchin
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引用次数: 1

Abstract

. Many physical phenomena may be modelled by first order hyperbolic equations with degenerate dissipative or diffusive terms. This is the case for example in gas dynamics, where the mass is conserved during the evolution, but the momentum balance includes a diffusion (viscosity) or damping (relaxation) term, or, in numerical simulations, of conservation laws by relaxation schemes. Such so-called partially dissipative systems have been first pointed out by S.K. Go-dunov in a short note in Russian in 1961. Much later, in 1984, S. Kawashima high-lighted in his PhD thesis a simple criterion ensuring the existence of global strong solutions in the vicinity of a linearly stable constant state. This criterion has been revisited in a number of research works. In particular, K. Beauchard and E. Zuazua proposed in 2010 an explicit method for constructing a Lyapunov functional allowing to refine Kawashima’s results and to establish global existence results in some situations that were not covered before. These notes originate essentially from the PhD thesis of T. Crin-Barat that was initially motivated by an earlier observation of the author in a Chapter of the handbook coedited by Y. Giga and A. Novotn´y. Our main aim is to adapt the method of Beauchard and Zuazua to a class of symmetrizable quasilinear hyperbolic systems (containing the compressible Euler equations), in a critical regularity setting that allows to keep track of the dependence with respect to e.g. the relaxation parameter. Compared to Beauchard and Zuazua’s work, we exhibit a ‘damped mode’ that will have a key role in the construction of global solutions with critical regularity, in the proof of optimal time-decay estimates and, last but not least, in the study of the strong relaxation limit. For simplicity, we here focus on a simple class of partially dissipative systems, but the overall strategy is rather flexible, and adaptable to much more involved situations.
部分耗散系统处于临界正则态,且有强松弛极限
许多物理现象可以通过具有退化耗散项或微分项的一阶双曲方程来建模。例如,在气体动力学中,质量在演化过程中是守恒的,但动量平衡包括扩散(粘度)或阻尼(弛豫)项,或者在数值模拟中,弛豫方案的守恒定律。1961年,S.K.Go dunov在一篇俄语短文中首次指出了这种所谓的部分耗散系统。很久以后,1984年,S.Kawashima在他的博士论文中提出了一个简单的准则,确保在线性稳定常态附近存在全局强解。这一标准已经在许多研究工作中被重新审视。特别是,K.Beauchard和E.Zuazua在2010年提出了一种构造李雅普诺夫函数的显式方法,允许重新定义Kawashima的结果,并在一些以前没有涉及的情况下建立全局存在性结果。这些注释主要源于T.Crin Barat的博士论文,该论文最初的动机是作者在Y.Giga和a.Novotn´Y合著的手册的一章中的早期观察。我们的主要目标是将Beauchard和Zuazua的方法应用于一类可对称的拟线性双曲型系统(包含可压缩欧拉方程),在临界正则性设置中,允许跟踪与松弛参数等的相关性。与Beauchard和Zuazua的工作相比,我们展示了一种“阻尼模式”,它将在构造具有临界正则性的全局解、证明最佳时间衰减估计以及最后但并非最不重要的是,在研究强弛豫极限方面发挥关键作用。为了简单起见,我们在这里关注一类简单的部分耗散系统,但总体策略相当灵活,并适用于更复杂的情况。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
2.30
自引率
0.00%
发文量
4
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