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Titlebook: Convection in Porous Media; Donald A. Nield,Adrian Bejan Book 19921st edition Springer-Verlag New York 1992 convection.energy.environment.

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21#
發(fā)表于 2025-3-25 05:49:04 | 只看該作者
22#
發(fā)表于 2025-3-25 11:02:59 | 只看該作者
R. R. Van der Ploeg,F. Beese,P. Beneckeusual situation) or it undergoes small deformation. The interconnectedness of the void (the pores) allows the flow of one or more fluids through the material. In the simplest situation (“single-phase flow”) the void is saturated by a single fluid. In “two-phase flow” a liquid and a gas share the void space.
23#
發(fā)表于 2025-3-25 13:05:11 | 只看該作者
24#
發(fā)表于 2025-3-25 17:14:30 | 只看該作者
Voluntary Termination of Pregnancyreview paper by Lai, Prasad, and Kulacki (1991). We start with a treatment of boundary layer flow on heated plane walls inclined at some nonzero angle to the horizontal. This configuration is illustrated in Fig. 8.1. The boundary layer equations [compare Eqs. (5.5) and (5.6)] for steady flow are ., ..
25#
發(fā)表于 2025-3-25 22:32:41 | 只看該作者
H. Abramovici,A. Rofe,J. Atad,J. H. Faktor matter how intense the heating or cooling effect. In the present chapter we turn our attention to situations in which a change of phase occurs, for example, melting or evaporation upon heating, and solidification or condensation upon cooling. These convection problems constitute a relatively new area in the field of convection in porous media.
26#
發(fā)表于 2025-3-26 00:24:26 | 只看該作者
27#
發(fā)表于 2025-3-26 04:51:16 | 只看該作者
28#
發(fā)表于 2025-3-26 12:20:00 | 只看該作者
29#
發(fā)表于 2025-3-26 15:48:04 | 只看該作者
External Natural Convection,ortant. For small values of the Rayleigh number ., perturbation methods are appropriate. At large values of . thermal boundary layers are formed, and boundary layer theory is the obvious method of investigation. This approach forms the subject of much of this chapter. We follow to a large extent the
30#
發(fā)表于 2025-3-26 19:45:02 | 只看該作者
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