离散守恒定律的流体力学

Patrick Sprenger, Christopher Chong, Emmanuel Okyere, Michael Herrmann, P. G. Kevrekidis, Mark A. Hoefer
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引用次数: 0

摘要

离散守恒定律的黎曼问题 $2 \dot{u}_n +u^2_{n+1}- u^2_{n-1} = 0$ 的黎曼问题,通过惠瑟姆调制理论、水连续近似和数值模拟进行了分类。对这个简单的离散正则化布尔格斯方程得到了一组令人惊讶的解。除了众所周知的离散流体力学解--稀释波(RWs)和离散冲击波(DSWs)--的离散类似解之外,还观察到了额外的非稳态解系列和无限时间炸裂。有两类解没有已知的守恒连续相关性:(i) 由对称、静止冲击波分隔的反向传播 DSW 和 RW 解;(ii) 非稳态冲击波发出两个频率相同的反向传播周期性波列,与部分 DSW 或 RW 相连。另一类解决方案称为行波 DSW,即(iii),由部分 DSW 和行波组成,行波由快速过渡到常数的周期波列构成。解(ii)和(iii)的部分内容被解释为惠森调制方程的冲击解。
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Hydrodynamics of a Discrete Conservation Law
The Riemann problem for the discrete conservation law $2 \dot{u}_n + u^2_{n+1} - u^2_{n-1} = 0$ is classified using Whitham modulation theory, a quasi-continuum approximation, and numerical simulations. A surprisingly elaborate set of solutions to this simple discrete regularization of the inviscid Burgers' equation is obtained. In addition to discrete analogues of well-known dispersive hydrodynamic solutions -- rarefaction waves (RWs) and dispersive shock waves (DSWs) -- additional unsteady solution families and finite time blow-up are observed. Two solution types exhibit no known conservative continuum correlates: (i) a counterpropagating DSW and RW solution separated by a symmetric, stationary shock and (ii) an unsteady shock emitting two counter-propagating periodic wavetrains with the same frequency connected to a partial DSW or a RW. Another class of solutions called traveling DSWs, (iii), consists of a partial DSW connected to a traveling wave comprised of a periodic wavetrain with a rapid transition to a constant. Portions of solutions (ii) and (iii) are interpreted as shock solutions of the Whitham modulation equations.
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