Hyperbolic conservation laws with discontinuous fluxes and hydrodynamic limit for particle systems

We study the following class of scalar hyperbolic conservation laws with discontinuous fluxes:equation(0.1)∂tρ+∂xF(x,ρ)=0.∂tρ+∂xF(x,ρ)=0. The main feature of such a conservation law is the discontinuity of the flux function in the space variable x  . Kruzkov's approach for the L1L1-contraction does not apply since it requires the Lipschitz continuity of the flux function in x  ; an additional jump wave may occur in the solution besides the classical waves; and entropy solutions even for the Riemann problem are not unique under the classical entropy conditions. On the other hand, it is known that, in statistical mechanics, some microscopic interacting particle systems with discontinuous speed-parameter λ(x)λ(x) in the hydrodynamic limit formally lead to scalar hyperbolic conservation laws with discontinuous fluxes of the formequation(0.2)∂tρ+∂x(λ(x)h(ρ))=0.∂tρ+∂x(λ(x)h(ρ))=0. The natural question arises which entropy solution the hydrodynamic limit selects, thereby leading to a suitable, physical relevant notion of entropy solutions of this class of conservation laws. This paper is a first step and provides an answer to this question for a family of discontinuous flux functions. In particular, we identify the entropy condition for (0.1) and proceed to show the well-posedness by combining our existence result with a uniqueness result of Audusse and Perthame (2005) for the family of flux functions; we establish a compactness framework for the hydrodynamic limit of large particle systems and the convergence of other approximate solutions to (0.1), which is based on the notion and reduction of measure-valued entropy solutions; and we finally establish the hydrodynamic limit for a ZRP with discontinuous speed-parameter governed by an L∞L∞ entropy solution to (0.2).