{ "id": "astro-ph/0409246", "version": "v1", "published": "2004-09-10T12:48:42.000Z", "updated": "2004-09-10T12:48:42.000Z", "title": "Differential rotation of main sequence F stars", "authors": [ "M. Kueker", "G. Ruediger" ], "comment": "7 pages, 10 figures", "doi": "10.1051/0004-6361:20041987", "categories": [ "astro-ph" ], "abstract": "The differential rotation of a 1.2 $M_\\odot$ zero age MS star (spectral type F8) is computed and the results are compared with those from a similar model of the Sun. The rotation pattern is determined by solving the Reynolds equation including the convective energy transport. The latter is anisotropic due to the Coriolis force causing a horizontal temperature gradient of ~ 7 K between the poles and the equator. Comparison of the transport mechanisms of angular momentum (the eddy viscosity, the $\\Lambda$-effect and the meridional flow) shows that for the F star the $\\Lambda$-effect is the most powerful transporter for rotation periods of 7 d or less. In the limit of very fast rotation the $\\Lambda$-effect is balanced by the meridional flow alone and the rotation is nearly rigid. The rotation pattern found for the F star is very similar to the solar rotation law, but the horizontal shear is about twice the solar value. As a function of the rotation period, the total equator-pole difference of the angular velocity has a (slight) maximum at a period of 7 d and (slowly) vanishes in both the limiting cases of very fast and very slow rotation. A comparison of the solar models with those for the F-type star shows a much stronger dependence of the differential surface rotation on the stellar luminosity rather than on the rotation rate.", "revisions": [ { "version": "v1", "updated": "2004-09-10T12:48:42.000Z" } ], "analyses": { "keywords": [ "differential rotation", "main sequence", "zero age ms star", "meridional flow", "rotation period" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 7, "language": "en", "license": "arXiv", "status": "editable", "inspire": 658832 } } }