Vasantha, R. ; Nath, G. (1986) Second-order boundary layers for steady, incompressible, three-dimensional stagnation point flows International Journal of Heat and Mass Transfer, 29 (12). pp. 1993-1996. ISSN 0017-9310
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Official URL: http://dx.doi.org/10.1016/0017-9310(86)90019-0
Related URL: http://dx.doi.org/10.1016/0017-9310(86)90019-0
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: | Article |
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Source: | Copyright of this article belongs to Elsevier Science. |
ID Code: | 37632 |
Deposited On: | 18 Apr 2011 13:12 |
Last Modified: | 18 Apr 2011 13:12 |
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