We introduce a dissipative measure-valued solution to the compressible non-Newtonian system. We generalized a result given by Novotný, Ne£asová [14]. We derive a relative entropy inequality for measure-valued solution as an extension of the "classical" entropy inequality introduced by Dafermos
1Formulation of the problemWe consider measure-valued solutions of the compressible non-Newtonian system. The advantage of measure-valued solutions is the property that in many cases, the solutions can be obtained from weakly convergent sequences of approximate solutions. Measure-valued solutions for systems of hyperbolic conservations laws were initially introduced by DiPerna [3]. He used Young measures to pass to limit in the articial viscosity term. In the case of the incompressible Euler equations, DiPerna and Majda [4] also proved global existence of measure-valued solutions for any initial data with nite energy. They introduced generalized Young measures to take into account oscillation and concentration phenomena. Thereafter the existence of measure-valued solutions was nally shown for further models of uids, e.g. compressible Euler and Navier-Stokes equations [13]. The measure-valued solution to the non-Newtonian case was proved by Novotný, Ne£asová [14].Recently, weak-strong uniqueness for measure-valued solutions of isentropic Euler equations were proved in [8]. Inspired by previous results, the concept of dissipative measure-valued solution was nally applied to the barotropic compressible Navier-Stokes system [9]. It is a generalization of classical measure-valued solution.The motion of the uid is governed by the following system of equationswhere is the mass density and u is the velocity eld, functions of the spatial position x ∈ R 3 and the time t ∈ R. The scalar function p is termed pressure, given function of the density. In particular, we consider the isothermal case, namely p = λ , with λ > 0 a constant. The stress tensor is given by S ij = βu l,l δ ij