dc.creator | San Martín, Jorge | |
dc.creator | Scheid, Jean-François | |
dc.creator | Smaranda, Loredana | |
dc.date.accessioned | 2014-01-09T13:45:50Z | |
dc.date.available | 2014-01-09T13:45:50Z | |
dc.date.created | 2014-01-09T13:45:50Z | |
dc.date.issued | 2012 | |
dc.identifier | Numer. Math. (2012) 122:341–382 | |
dc.identifier | DOI 10.1007/s00211-012-0460-1 | |
dc.identifier | https://repositorio.uchile.cl/handle/2250/126100 | |
dc.description.abstract | In this paper, we propose a new characteristics method for the
discretization of the two dimensional fluid-rigid body problem in the case where the
densities of the fluid and the solid are different. The method is based on a global weak
formulation involving only terms defined on the whole fluid-rigid domain. To take into
account the material derivative, we construct a special characteristic function which
maps the approximate rigid body at the (k +1)-th discrete time level into the approximate
rigid body at k-th time. Convergence results are proved for both semi-discrete
and fully-discrete schemes. | |
dc.language | en | |
dc.publisher | Springer | |
dc.rights | http://creativecommons.org/licenses/by-nc-nd/3.0/cl/ | |
dc.rights | Attribution-NonCommercial-NoDerivs 3.0 Chile | |
dc.title | A modified Lagrange-Galerkin method for a fluid-rigid system with discontinuous density | |
dc.type | Artículo de revista | |