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Titlebook: Small Viscosity and Boundary Layer Methods; Theory, Stability An Guy Métivier Book 2004 Springer Science+Business Media New York 2004 Appli

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樓主: fitful
21#
發(fā)表于 2025-3-25 03:48:35 | 只看該作者
22#
發(fā)表于 2025-3-25 09:15:15 | 只看該作者
23#
發(fā)表于 2025-3-25 12:27:27 | 只看該作者
Guy Métivierion, already established in discussing literature as discourse (Chapter 1), is that literary texts can be best understood in comparison with non-literary texts, because there are different tendencies, but they are subtle and not dichotomous differences. Rather a discourse-based approach to literatur
24#
發(fā)表于 2025-3-25 16:40:56 | 只看該作者
25#
發(fā)表于 2025-3-25 22:52:59 | 只看該作者
26#
發(fā)表于 2025-3-26 03:34:42 | 只看該作者
27#
發(fā)表于 2025-3-26 05:21:52 | 只看該作者
Quasilinear Boundary Layers: The Inner Layer ODEnifold theorem, which determines the boundary conditions associated to the limiting hyperbolic system. The local structure of . depends on transversality conditions or equivalently on stability conditions of the ODE.
28#
發(fā)表于 2025-3-26 09:35:22 | 只看該作者
Plane Wave Stability the normal variable. We refer to the Introduction for references concerning these notions. A key point in this chapter is the theorem of F. Rousset [Ro1] asserting that the uniform Evans condition implies that the limiting hyperbolic boundary value problem satisfies the uniform Lopatinski condition (see also [Zu-Se] for viscous shocks).
29#
發(fā)表于 2025-3-26 14:45:28 | 只看該作者
Stability Estimatesltipliers. A corollary of the construction of symmetrizers is the continuous extendability of the spectral spaces E_ stated in Lemma 6.2.8 and Theorem 6.4.8 (see [MZ2]). In this chapter, we always suppose that Assumption 5.1.1 is satisfied and we consider the linearized equations (6.1.2) around a profile . that satisfies (6.1.1).
30#
發(fā)表于 2025-3-26 18:54:37 | 只看該作者
Kreiss Symmetrizers for Hyperbolic-Parabolic Systemsbolicity can be somewhat relaxed and that the construction extends to systems satisfying .. Finally, it is proven in [Mé3] that the block structure condition is satisfied for all hyperbolic systems with constant multiplicity. We discuss in this chapter the extension of Kreiss construction to hyperbolic-parabolic systems given in [MZ1].
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