Non-unique solution for combined-convection assisting flow over vertical flat plate
Author(s) -
K. Venkatasubbaiah,
Amrita Mittal,
Tapan K. Sengupta
Publication year - 2006
Publication title -
sadhana
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.268
H-Index - 49
eISSN - 0973-7677
pISSN - 0256-2499
DOI - 10.1007/bf02716890
Subject(s) - laminar flow , boundary layer , mechanics , convection , perturbation (astronomy) , shear flow , blasius boundary layer , boundary value problem , vector field , classical mechanics , mathematics , mathematical analysis , physics , boundary layer thickness , quantum mechanics
Non-unique solutions of flow and temperature field are reported here for the first time for non-similar flows given by the laminar boundary layer equations for combined-convection flow past a vertical flat plate. The solution of the boundary layer equation for natural convection constitutes the self-similar solution whose perturbation with respect to the small parameter (ε), which is inversely proportional to the square root of the Richardson number (G x ), provides the non-similar solution. Solutions obtained by the shooting method indicate two sets for the self-similar solution (ε = 0) — one of them showing positive velocity everywhere inside the shear layer (well-known oft-reported physical result). The other self-similar solution shows that recirculation in the outer part of the shear layer may not be physical — as it has not been experimentally demonstrated so far. In contrast, the perturbative part of the non-similar solution (ε ⊋ 0) is seen to be either convergent or divergent depending upon the choice of integration domain of the shear layer equations — bringing forth the question of the validity of such perturbation procedures and possible stability of the basic solution itself.
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