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SIAM J. APPLIED DYNAMICAL SYSTEMS c 2009 Society for Industrial and Applied Mathematics
Vol. 8, No. 3, pp. 822–853
Persistence of Rarefactions under Dafermos Regularization: Blow-Up and an
Exchange Lemma for Gain-of-Stability Turning Points
∗
Stephen Schecter
†
and Peter Szmolyan
‡
Abstract. We construct self-similar solutions of the Dafermos regularization of a system of conservation laws
near structurally stable Riemann solutions composed of Lax shocks and rarefactions, with all waves
possibly large. The construction requires blowing up a manifold of gain-of-stability turning points
in a geometric singular perturbation problem as well as a new exchange lemma to deal with the
remaining hyperbolic directions.
Key words. conservation laws, Riemann problem, geometric singular perturbation theory, loss of normal hy-
perbolicity, blow-up
AMS subject classifications. 35L65, 34E15
DOI. 10.1137/080715305
1. Introduction. This paper is the last in a series of three; the others are [22] and [23].
An introduction to the series is in [22]. We construct self-similar solutions of the Dafermos
regularization of a system of conservation laws near structurally stable Riemann solutions
composed of Lax shocks and rarefactions, with all waves possibly large. The construction
requires blowing up a manifold of gain-of-stability turning points in a geometric singular per-
turbation problem. In addition, it requires a new exchange lemma to deal with the remaining
hyperbolic directions. The latter is a consequence of the general exchange lemma from [23].
In this introduction, we briefly describe the conservation law background, and we describe
some solutions near gain-of-stability turning points in order to help the reader’s intuition.
A system of conservation laws in one space dimension is a partial differential equation of
the form
(1.1) u
T
+ f (u)
X
=0,
with X ∈ R, u ∈ R
n
, and f : R
n
→ R
n
a smooth function. For background on this class of
equations, see, for example, [26]. An important initial value problem is the Riemann problem,
which has piecewise constant initial conditions:
(1.2) u(X, 0) =
u
L
for X< 0,
u
R
for X> 0.
∗
Received by the editors February 7, 2008; accepted for publication (in revised form) by C. Wayne May 4, 2009;
published electronically July 10, 2009.
http://www.siam.org/journals/siads/8-3/71530.html
†
Mathematics Department, North Carolina State University, Box 8205, Raleigh, NC 27695 (schecter@math.ncsu.
edu). This author’s research was supported by the National Science Foundation under grant DMS-0406016.
‡
Institute for Analysis and Scientific Computing, Vienna University of Technology, Wiedner Hauptstraße 6–10,
A-1040 Vienna, Austria (szmolyan@tuwien.ac.at). This author’s research was supported by the Austrian Science
Foundation under grant Y 42-MAT.
822
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