Motivated by radiation hydrodynamics, we analyse a 2 2 system consisting of a one-dimensional viscous conservation law with strictly convex ux -the viscous Burgers' equation being a paradigmatic example- coupled with an elliptic equation, named viscous Hamer-type system. In the regime of small viscosity and for large shocks, namely when the pro le of the corresponding underlying inviscid model undergoes a discontinuity {usually called sub-shock{ it is proved the existence of a smooth propagating front, regularising the jump of the corresponding inviscid equation. The proof is based on Geometric Singular Perturbation Theory (GSPT) as introduced in the pioneering work of Fenichel [5] and subsequently developed by Szmolyan [21]. In addition, the case of small shocks and large viscosity is also addressed via a standard bifurcation argument.
Propagating fronts for a viscous Hamer-type system / Cianfarani Carnevale, Giada; Lattanzio, Corrado; Mascia, Corrado. - In: DISCRETE AND CONTINUOUS DYNAMICAL SYSTEMS. - ISSN 1078-0947. - 42:2(2022), pp. 605-621. [10.3934/dcds.2021130]
Propagating fronts for a viscous Hamer-type system
Mascia, CorradoUltimo
2022
Abstract
Motivated by radiation hydrodynamics, we analyse a 2 2 system consisting of a one-dimensional viscous conservation law with strictly convex ux -the viscous Burgers' equation being a paradigmatic example- coupled with an elliptic equation, named viscous Hamer-type system. In the regime of small viscosity and for large shocks, namely when the pro le of the corresponding underlying inviscid model undergoes a discontinuity {usually called sub-shock{ it is proved the existence of a smooth propagating front, regularising the jump of the corresponding inviscid equation. The proof is based on Geometric Singular Perturbation Theory (GSPT) as introduced in the pioneering work of Fenichel [5] and subsequently developed by Szmolyan [21]. In addition, the case of small shocks and large viscosity is also addressed via a standard bifurcation argument.File | Dimensione | Formato | |
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