RIEMANN PROBLEMS FOR THE 2-DIMENSIONAL UNSTEADY TRANSONIC SMALL DISTURBANCE EQUATION

Citation
S. Canic et Bl. Keyfitz, RIEMANN PROBLEMS FOR THE 2-DIMENSIONAL UNSTEADY TRANSONIC SMALL DISTURBANCE EQUATION, SIAM journal on applied mathematics, 58(2), 1998, pp. 636-665
Citations number
16
Categorie Soggetti
Mathematics,Mathematics
ISSN journal
00361399
Volume
58
Issue
2
Year of publication
1998
Pages
636 - 665
Database
ISI
SICI code
0036-1399(1998)58:2<636:RPFT2U>2.0.ZU;2-6
Abstract
We study a two-parameter family of Riemann problems for the unsteady t ransonic small disturbance (UTSD) equation, also called the two-dimens ional Burgers equation, which is used to model the transition from reg ular to Mach reflection for weak shock waves. The related initial-valu e problem consists of oblique shock data in the upper half-plane, with two parameters a and b corresponding to the slopes of the initial sho ck waves. The study of quasi-steady solutions leads to a problem that changes type when written in self-similar coordinates. The problem is hyperbolic in the region where the flow is supersonic, and elliptic wh ere the flow is subsonic. In this paper we give a complete description of the flow in the hyperbolic region by resolving the hyperbolic wave interactions in the form of quasi-one-dimensional Riemann problems. I n the region of physical space where the flow is subsonic, we pose the related free-boundary problems and discuss the behavior of the subson ic solution using results from our previous work. Based on this approa ch we establish the existence of regions of different qualitative beha vior in parameter (a, b) space. Our results reveal that the UTSD equat ion seems to be particularly suitable for the study of the so-called v on Neumann paradox in which linearly degenerate waves can be ignored. We establish the region in the parameter space where a prototype of vo n Neumann reflection takes place. In other regions of parameter space we find prototypes for Mach reflection, regular reflection, and transi tional Mach reflection. The lack of linearly degenerate waves in this model is resolved by the presence of a small rarefaction wave emerging from the triple point.