Abstract
The endeavor of solving the initial-value problem for the scalar conservation law, in Chapter VI, owes its spectacular success to the L 1 -contraction property, which applies not only to the solutions themselves but even to their approximations by means of vanishing viscosity, layering, relaxation, etc. For systems, however, the situation is different: L 1-contraction no longer applies; in its place, L 1-Lipschitz continuity will eventually be established, in Chapter XIV, albeit under substantial restrictions on the initial data. Furthermore, at the time of this writing, the requisite stability estimates have been established solely in the context of highly specialized approximating schemes that employ as building blocks the solution of the Riemann problem.
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Dafermos, C.M. (2000). The Random Choice Method. In: Hyperbolic Conservation Laws in Continuum Physics. Grundlehren der mathematischen Wissenschaften, vol 325. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-22019-1_13
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