2,328 research outputs found

    Steady nearly incompressible vector fields in 2D: chain rule and renormalization

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    Given bounded vector field b:Rd→Rdb : \mathbb R^d \to \mathbb R^d, scalar field u:Rd→Ru : \mathbb R^d \to \mathbb R and a smooth function β:R→R\beta : \mathbb R \to \mathbb R we study the characterization of the distribution div(β(u)b)\mathrm{div}(\beta(u)b) in terms of div b\mathrm{div}\, b and div(ub)\mathrm{div}(u b). In the case of BVBV vector fields bb (and under some further assumptions) such characterization was obtained by L. Ambrosio, C. De Lellis and J. Mal\'y, up to an error term which is a measure concentrated on so-called \emph{tangential set} of bb. We answer some questions posed in their paper concerning the properties of this term. In particular we construct a nearly incompressible BVBV vector field bb and a bounded function uu for which this term is nonzero. For steady nearly incompressible vector fields bb (and under some further assumptions) in case when d=2d=2 we provide complete characterization of div(β(u)b)\mathrm{div}(\beta(u) b) in terms of div b\mathrm{div}\, b and div(ub)\mathrm{div}(u b). Our approach relies on the structure of level sets of Lipschitz functions on R2\mathrm R^2 obtained by G. Alberti, S. Bianchini and G. Crippa. Extending our technique we obtain new sufficient conditions when any bounded weak solution uu of ∂tu+b⋅∇u=0\partial_t u + b \cdot \nabla u=0 is \emph{renormalized}, i.e. also solves ∂tβ(u)+b⋅∇β(u)=0\partial_t \beta(u) + b \cdot \nabla \beta(u)=0 for any smooth function β:R→R\beta : \mathbb R \to \mathbb R. As a consequence we obtain new uniqueness result for this equation.Comment: 50 pages, 8 figure

    A connection between viscous profiles and singular ODEs

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    We deal with the viscous profiles for a class of mixed hyperbolic-parabolic systems. We focus, in particular, on the case of the compressible Navier Stokes equation in one space variable written in Eulerian coordinates. We describe the link between these profiles and a singular ordinary differential equation in the form dV/dt=F(V)/z(V). dV / dt = F(V) / z (V) . Here V∈RdV \in R^d and the function F takes values into RdR^d and is smooth. The real valued function z is as well regular: the equation is singular in the sense that z (V) can attain the value 0.Comment: 6 pages, minor change
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