Vasantha, R and Nath, G (1986) Second-order boundary layers for steady, incompressible, three-dimensional stagnation point flows. In: International Journal of Heat and Mass Transfer, 29 (12). pp. 1993-1996.
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Abstract
It is well known that the classical boundary-layer theory represents the asymptotic solution of the Navier-Stokes equations for large Reynolds numbers. The succeeding approximation is the second-order boundary layer one which includes the effects of surface curvature, vorticity interaction and boundary-layer displacement. The second-order boundary-layer effects become important when the boundarylayer thickness becomes comparable with the characteristic body length. Van Dyke [1] and Gersten and Gross [2] have given an excellent survey of higher-order boundary layers.
Item Type: | Journal Article |
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Publication: | International Journal of Heat and Mass Transfer |
Publisher: | Elsevier |
Additional Information: | Copyright of this article belongs to Elsevier. |
Department/Centre: | Division of Physical & Mathematical Sciences > Mathematics |
Date Deposited: | 02 Jul 2008 |
Last Modified: | 19 Sep 2010 04:46 |
URI: | http://eprints.iisc.ac.in/id/eprint/14743 |
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