40 research outputs found

    Shock waves for radiative hyperbolic--elliptic systems

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    The present paper deals with the following hyperbolic--elliptic coupled system, modelling dynamics of a gas in presence of radiation, ut+f(u)x+Lqx=0,−qxx+Rq+G⋅ux=0,u_{t}+ f(u)_{x} +Lq_{x}=0, -q_{xx} + Rq +G\cdot u_{x}=0, where u∈Rnu\in\R^{n}, q∈Rq\in\R and R>0R>0, GG, L∈RnL\in\R^{n}. The flux function f:Rn→Rnf : \R^n\to\R^n is smooth and such that ∇f\nabla f has nn distinct real eigenvalues for any uu. The problem of existence of admissible radiative shock wave is considered, i.e. existence of a solution of the form (u,q)(x,t):=(U,Q)(x−st)(u,q)(x,t):=(U,Q)(x-st), such that (U,Q)(±∞)=(u±,0)(U,Q)(\pm\infty)=(u_\pm,0), and u±∈Rnu_\pm\in\R^n, s∈Rs\in\R define a shock wave for the reduced hyperbolic system, obtained by formally putting L=0. It is proved that, if u−u_- is such that ∇λk(u−)⋅rk(u−)≠0\nabla\lambda_{k}(u_-)\cdot r_{k}(u_-)\neq 0,(where λk\lambda_k denotes the kk-th eigenvalue of ∇f\nabla f and rkr_k a corresponding right eigenvector) and (ℓk(u−)⋅L)(G⋅rk(u−))>0(\ell_{k}(u_{-})\cdot L) (G\cdot r_{k}(u_{-})) >0, then there exists a neighborhood U\mathcal U of u−u_- such that for any u+∈Uu_+\in{\mathcal U}, s∈Rs\in\R such that the triple (u−,u+;s)(u_{-},u_{+};s) defines a shock wave for the reduced hyperbolic system, there exists a (unique up to shift) admissible radiative shock wave for the complete hyperbolic--elliptic system. Additionally, we are able to prove that the profile (U,Q)(U,Q) gains smoothness when the size of the shock ∣u+−u−∣|u_+-u_-| is small enough, as previously proved for the Burgers' flux case. Finally, the general case of nonconvex fluxes is also treated, showing similar results of existence and regularity for the profiles.Comment: 32 page

    Energy method for multi-dimensional balance laws with non-local dissipation

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    AbstractIn this paper, we are concerned with a class of multi-dimensional balance laws with a non-local dissipative source which arise as simplified models for the hydrodynamics of radiating gases. At first we introduce the energy method in the setting of smooth perturbations and study the stability of constants states. Precisely, we use Fourier space analysis to quantify the energy dissipation rate and recover the optimal time-decay estimates for perturbed solutions via an interpolation inequality in Fourier space. As application, the developed energy method is used to prove stability of smooth planar waves in all dimensions n⩾2, and also to show existence and stability of time-periodic solutions in the presence of the time-periodic source. Optimal rates of convergence of solutions towards the planar waves or time-periodic states are also shown provided initially L1-perturbations

    Stability of scalar radiative shock profiles

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    This work establishes nonlinear orbital asymptotic stability of scalar radiative shock profiles, namely, traveling wave solutions to the simplified model system of radiating gas \cite{Hm}, consisting of a scalar conservation law coupled with an elliptic equation for the radiation flux. The method is based on the derivation of pointwise Green function bounds and description of the linearized solution operator. A new feature in the present analysis is the construction of the resolvent kernel for the case of an eigenvalue system of equations of degenerate type. Nonlinear stability then follows in standard fashion by linear estimates derived from these pointwise bounds, combined with nonlinear-damping type energy estimates
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