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A Theory of L 1 -Dissipative Solvers for Scalar Conservation Laws with Discontinuous Flux

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In this paper, a general framework for the study of L1 contractive semigroups of solutions to conservation laws with discontinuous flux is proposed, where the fluxes fl, fr are mainly assumed to be continuous.
Abstract
We propose a general framework for the study of L1 contractive semigroups of solutions to conservation laws with discontinuous flux: $$ u_t + \mathfrak{f}(x,u)_x=0, \qquad \mathfrak{f}(x,u)= \left\{\begin{array}{ll} f^l(u),& x 0, \end{array} \right\quad\quad\quad (\rm CL) $$ where the fluxes fl, fr are mainly assumed to be continuous Developing the ideas of a number of preceding works (Baiti and Jenssen in J Differ Equ 140(1):161–185, 1997; Towers in SIAM J Numer Anal 38(2):681–698, 2000; Towers in SIAM J Numer Anal 39(4):1197–1218, 2001; Towers et al in Skr K Nor Vidensk Selsk 3:1–49, 2003; Adimurthi et al in J Math Kyoto University 43(1):27–70, 2003; Adimurthi et al in J Hyperbolic Differ Equ 2(4):783–837, 2005; Audusse and Perthame in Proc Roy Soc Edinburgh A 135(2):253–265, 2005; Garavello et al in Netw Heterog Media 2:159–179, 2007; Burger et al in SIAM J Numer Anal 47:1684–1712, 2009), we claim that the whole admissibility issue is reduced to the selection of a family of “elementary solutions”, which are piecewise constant weak solutions of the form $$ c(x)=c^l11_{\left\{{x 0}\right\}} $$ We refer to such a family as a “germ” It is well known that (CL) admits many different L1 contractive semigroups, some of which reflect different physical applications We revisit a number of the existing admissibility (or entropy) conditions and identify the germs that underly these conditions We devote specific attention to the “vanishing viscosity” germ, which is a way of expressing the “Γ-condition” of Diehl (J Hyperbolic Differ Equ 6(1):127–159, 2009) For any given germ, we formulate “germ-based” admissibility conditions in the form of a trace condition on the flux discontinuity line {x = 0} [in the spirit of Vol’pert (Math USSR Sbornik 2(2):225–267, 1967)] and in the form of a family of global entropy inequalities [following Kruzhkov (Math USSR Sbornik 10(2):217–243, 1970) and Carrillo (Arch Ration Mech Anal 147(4):269–361, 1999)] We characterize those germs that lead to the L1-contraction property for the associated admissible solutions Our approach offers a streamlined and unifying perspective on many of the known entropy conditions, making it possible to recover earlier uniqueness results under weaker conditions than before, and to provide new results for other less studied problems Several strategies for proving the existence of admissible solutions are discussed, and existence results are given for fluxes satisfying some additional conditions These are based on convergence results either for the vanishing viscosity method (with standard viscosity or with specific viscosities “adapted” to the choice of a germ), or for specific germ-adapted finite volume schemes

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Journal ArticleDOI

Finite volume schemes for locally constrained conservation laws

TL;DR: This paper produces a simple scheme for the constrained problem and shows its convergence, and reformulates accordingly the notion of entropy solution introduced by Colombo and Goatin, and extends the well-posedness results to the L∞ framework.
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On vanishing viscosity approximation of conservation laws with discontinuous flux

TL;DR: The vanishing viscosity limit for multi-dimensional conservation laws of the form $ u_t + $div$ \mathfrak{f}(x,u) = 0, \quad u|_{t=0}=u_0 = u_0 $ in the domain $\mathbb R^+\times\mathb R^N$.
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Flux-limited solutions for quasi-convex Hamilton-Jacobi equations on networks

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Flux-limited solutions for quasi-convex Hamilton-Jacobi equations on networks

TL;DR: In this article, the existence and uniqueness result for quasi-convex Hamilton-Jacobi equations on networks is proved. But the authors do not consider the case where the gradient variable is discontinuous with respect to the space variable at vertices.
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Vanishing capillarity solutions of Buckley–Leverett equation with gravity in two-rocks’ medium

TL;DR: In this article, a finite volume numerical method for the Buckley-Leverett equation with interface coupling was proposed, which retains information from the vanishing capillarity model and shows that the "optimal" entropy condition is not always the appropriate one, contrary to the erroneous interpretation of Kaasschieter's results which is sometimes encountered in the literature.
References
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Book

Partial Differential Equations

TL;DR: In this paper, the authors present a theory for linear PDEs: Sobolev spaces Second-order elliptic equations Linear evolution equations, Hamilton-Jacobi equations and systems of conservation laws.
Journal ArticleDOI

First order quasilinear equations in several independent variables

TL;DR: In this paper, a theory of generalized solutions in the large Cauchy's problem for the equations in the class of bounded measurable functions is constructed, and the existence, uniqueness and stability theorems for this solution are proved.
Book ChapterDOI

Finite Volume Methods

TL;DR: The finite volume method is a discretization method that is well suited for the numerical simulation of various types (for instance, elliptic, parabolic, or hyperbolic) of conservation laws.
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