{ "id": "1204.6465", "version": "v1", "published": "2012-04-29T09:35:39.000Z", "updated": "2012-04-29T09:35:39.000Z", "title": "Logarithmic temperature profiles in turbulent Rayleigh-Bénard convection", "authors": [ "Guenter Ahlers", "Eberhard Bodenschatz", "Denis Funfschilling", "Siegfried Grossmann", "Xiaozhou He", "Detlef Lohse", "Richard J. A. M. Stevens", "Roberto Verzicco" ], "journal": "Phys. Rev. Lett. 109, 114501 (2012)", "doi": "10.1103/PhysRevLett.109.114501", "categories": [ "physics.flu-dyn" ], "abstract": "We report results for the temperature profiles of turbulent Rayleigh-B\\'enard convection (RBC) in the interior of a cylindrical sample of aspect ratio $\\Gamma \\equiv D/L = 0.50$ ($D$ and $L$ are the diameter and height respectively). Results from experiment over the Rayleigh number range $4\\times 10^{12} \\alt Ra \\alt 10^{15}$ for a Prandtl number $\\Pra \\simeq 0.8$ and from direct numerical simulation (DNS) at $Ra = 2 \\times 10^{12}$ for $\\Pra = 0.7$ are presented. We find that the temperature varies as $A*ln(z/L) + B$ where $z$ is the distance from the bottom or top plate. This is the case in the classical as well as in the ultimate state of RBC. From DNS we find that $A$ in the classical state decreases in the radial direction as the distance from the side wall increases and becomes small near the sample center.", "revisions": [ { "version": "v1", "updated": "2012-04-29T09:35:39.000Z" } ], "analyses": { "subjects": [ "47.27.te", "47.20.Bp", "47.27.ek", "47.32.Ef" ], "keywords": [ "turbulent rayleigh-bénard convection", "logarithmic temperature profiles", "turbulent rayleigh-benard convection", "side wall increases", "rayleigh number range" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review Letters", "year": 2012, "month": "Sep", "volume": 109, "number": 11, "pages": 114501 }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2012PhRvL.109k4501A" } } }