{ "id": "1005.5517", "version": "v1", "published": "2010-05-30T11:44:04.000Z", "updated": "2010-05-30T11:44:04.000Z", "title": "Chaotic dynamics in two-dimensional Rayleigh-Bénard convection", "authors": [ "Supriyo Paul", "Mahendra K. Verma", "Pankaj Wahi", "Sandeep K. Reddy", "Krishna Kumar" ], "comment": "16 pages, 13 figures", "categories": [ "physics.flu-dyn", "nlin.CD" ], "abstract": "We investigate the origin of various convective patterns using bifurcation diagrams that are constructed using direct numerical simulations. We perform two-dimensional pseudospectral simulations for a Prandtl number 6.8 fluid that is confined in a box with aspect ratio $\\Gamma = 2\\sqrt{2}$. Steady convective rolls are born from the conduction state through a pitchfork bifurcation at $r=1$, where $r$ is the reduced Rayleigh number. These fixed points bifurcate successively to time-periodic and quasiperiodic rolls through Hopf and Neimark-Sacker bifurcations at $r \\simeq 80$ and $r \\simeq 500 $ respectively. The system becomes chaotic at $r \\simeq 750$ through a quasiperiodic route to chaos. The size of the chaotic attractor increases at $r \\simeq 840$ through an \"attractor-merging crisis\" which also results in travelling chaotic rolls. We also observe coexistence of stable fixed points and a chaotic attractor for $ 846 \\le r \\le 849$ as a result of a subcritical Hopf bifurcation. Subsequently the chaotic attractor disappears through a \"boundary crisis\" and only stable fixed points remain. Later these fixed points become periodic and chaotic through another set of bifurcations which ultimately leads to turbulence.", "revisions": [ { "version": "v1", "updated": "2010-05-30T11:44:04.000Z" } ], "analyses": { "keywords": [ "two-dimensional rayleigh-bénard convection", "chaotic dynamics", "bifurcation", "perform two-dimensional pseudospectral simulations", "chaotic attractor increases" ], "note": { "typesetting": "TeX", "pages": 16, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2010arXiv1005.5517P" } } }