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High-order schemes, entropy inequalities, and nonclassical shocks

机译:高阶方案,熵不等式和非经典冲击

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We are concerned with the approximation of undercompressive, regularization-sensitive, nonclassical solutions of hyperbolic systems of conservation laws by high-order accurate, conservative, and semidiscrete finite difference schemes. Nonclassical shock waves can be generated by diffusive and dispersive terms kept in balance. Particular attention is given here to a class of systems of conservation laws including the scalar equations and the system of nonlinear elasticity and to linear diffusion and dispersion in either the conservative or the entropy variables. First, we investigate the existence and the properties of entropy conservative schemes a notion due to Tadmor [Math. Comp., 49 (1987), pp. 91-103]. In particular we exhibit a new five-point scheme which is third-order accurate, at least. Second, we study a class of entropy stable and high-order accurate schemes satisfying a single cell entropy inequality. They are built from any high-order entropy conservative scheme by adding to it a mesh-independent, numerical viscosity, which preserves the order of accuracy of the base scheme. These schemes can only converge to solutions of the system of conservation laws satisfying the entropy inequality. These entropy stable schemes exhibit mild oscillations near shocks and, interestingly, may converge to classical or nonclassical entropy solutions, depending on the sign of their dispersion coefficient. Then, based on a third-order, entropy conservative scheme, we propose a general scheme for the numerical computation of nonclassical shocks. Importantly, our scheme satis es a cell entropy inequality. Following Hayes and LeFloch [SIAM J. Numer. Anal., 35 (1998), pp. 2169-2194], we determine numerically the kinetic function which uniquely characterizes the dynamics of nonclassical shocks for each regularization of the conservation laws. Our results compare favorably with previous analytical and numerical results. Finally, we prove that there exists no fully discrete and entropy conservative scheme and we investigate the entropy stability of a class of fully discrete, Lax-Wendroff type schemes. [References: 51]
机译:我们关注高阶精确,保守和半离散有限差分方案对双曲守恒律系统的负压缩,正则化敏感,非经典解的逼近。非经典冲击波可以通过保持平衡的扩散项和色散项产生。这里特别注意一类守恒律系统,包括标量方程和非线性弹性系统,以及保守变量或熵变量中的线性扩散和弥散。首先,我们研究熵保守方案的存在和性质。 《比较》,第49卷,1987年,第91-103页]。特别是,我们展示了一种至少三阶精确的新五点方案。其次,我们研究了一类满足单细胞熵不等式的熵稳定和高阶精确格式。它们是通过从任何高阶熵保守方案中添加与网格无关的数值粘度而构建的,从而保留了基本方案的准确性。这些方案只能收敛到满足熵不等式的守恒律系统的解。这些熵稳定方案在冲击附近表现出轻微的振荡,有趣的是,取决于它们的分散系数的符号,它们可能会收敛到经典或非经典的熵解。然后,基于三阶熵保守方案,提出了一种用于非经典冲击数值计算的通用方案。重要的是,我们的方案满足了细胞熵不等式。继Hayes和LeFloch [SIAM J. Numer。 Anal。,35(1998),pp。2169-2194],我们在数值上确定了动力学函数,该动力学函数对于守恒律的每个正则化都是唯一表征非经典冲击动力学的。我们的结果与以前的分析和数值结果相比具有优势。最后,我们证明不存在完全离散和熵保守的方案,并且研究了一类完全离散的Lax-Wendroff型方案的熵稳定性。 [参考:51]

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