{ "id": "0812.1627", "version": "v1", "published": "2008-12-09T06:25:53.000Z", "updated": "2008-12-09T06:25:53.000Z", "title": "Long time behaviour of viscous scalar conservation laws", "authors": [ "Anne-Laure Dalibard" ], "comment": "36 pages", "journal": "Indiana University Mathematics Journal 59, 1 (2010) 257-300", "doi": "10.1512/iumj.2010.59.3874", "categories": [ "math.AP" ], "abstract": "This paper is concerned with the stability of stationary solutions of the conservation law $\\partial_t u + \\mathrm{div}_y A(y,u) -\\Delta_y u=0$, where the flux $A$ is periodic with respect to its first variable. Essentially two kinds of asymptotic behaviours are studied here: the case when the equation is set on $\\R$, and the case when it is endowed with periodic boundary conditions. In the whole space case, we first prove the existence of viscous stationary shocks - also called standing shocks - which connect two different periodic stationary solutions to one another. We prove that standing shocks are stable in $L^1$, provided the initial disturbance satisfies some appropriate boundedness conditions. We also extend this result to arbitrary initial data, but with some restrictions on the flux $A$. In the periodic case, we prove that periodic stationary solutions are always stable. The proof of this result relies on the derivation of uniform $L^\\infty$ bounds on the solution of the conservation law, and on sub- and super-solution techniques.", "revisions": [ { "version": "v1", "updated": "2008-12-09T06:25:53.000Z" } ], "analyses": { "subjects": [ "35B35", "35B40", "76L05" ], "keywords": [ "viscous scalar conservation laws", "long time behaviour", "periodic stationary solutions", "standing shocks", "periodic boundary conditions" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 36, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2008arXiv0812.1627D" } } }