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Additional resources for Computational Fluid Dynamics: Selected Topics
015 = 0,556 and t = 4,015 to three. 52) appearing in this figure was in fact explained above as the impossibility for the eighth layers to find room within the height of the tank, It is interesting to observe that the two ultimate interfaces were already at the same height as early as t = 1. 4b) is constant in each layer with a large gradient through the interfaces and near the horizontal walls (the concentration is kept fixed at these walls), The temperature field (Figs. 1 T o < ~ (b) ~--,---rl-'I--'I--'I T O.
PI/3d - 'P = 311"/2 =---11 » ...... lI/1J"' .. · " " · · ) / / 1111 11 " 111'' ' "",,. l\\\\\\'''·--· .. , .. ,· . . . , .. " . ~-=-::::::::::::::::=:::::::: - - Fig. 24. PI/3d (ur,z) - 'P 30 =0 '" .. " " •• - ' - - - q ' Fig. 25. PI/3d (ur,z) - 'P = 11" Fig. 26. Cylinder flow after 4000 steps Fig. 27. Cylinder flow after 14000 steps Fig. 28. Cylinder flow after 20000 steps Fig. 29. Cylinder flow after 21000 steps __ _ a~_ \ \ - - - - ... Fig. 30. Cylinder flow after 22000 steps Fig. 31. Cylinder flow after 22000 steps 31 References 1.
S):~ ~ . :. 556 lines ~. '*~ ~~ fn~ ,\,, ~ ~ !! :::::? 188 0. 300 Fig. 2. Streamlines and iso-concentration lines: first phase of the formation of layers work against gravitation. This explains why the first convective cell appears at the bottom of the tank near the heated walL Such a behaviour has been experimentally observed for exemple in , . The physical process above described was first observed in  and applied to the present problem in . After the first cell has been created, it acts like a boundary on the fluid located above and a second layer forms by a similar mechanism, and so on.