双空气多孔层的被动对流通风,内热产生取决于固体分数

E. Kolchanova, N. Kolchanov
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引用次数: 0

摘要

本文用数值方法研究了由空气区下面的发热多孔区组成的双层系统的对流稳定性。在多孔区考虑了热释放与固体体积分数的线性关系。在系统的外部不渗透边界上固定等温的值。在给定波数的情况下,确定了系统中以二维横摇形式诱导对流的临界内部瑞利-达西数。对流流动是由于存在内部热释放的不稳定密度分层的形成。研究了两种类型的静止对流,即局部对流和大尺度对流。局部气流产生于空气亚层,很少渗透到多孔亚层中。大尺度对流覆盖两个子层。对流状态的变化随系统某一或另一参数的增大而发生,表明不稳定类型的变化。它伴随着横摇型临界波数的突然(几倍甚至几十倍)变化。数值计算表明,随着多孔亚层中固体体积分数φ的增加和空气亚层相对厚度d的增加,两种对流的起始值都有所降低。达西数(多孔亚层的无量纲每渗透率)的增长也会导致空气静止状态在给定的ϕ和d处的不稳定。对流状态从大规模流动到局部流动的变化发生在空气亚层相对厚度的增加,而从局部到大尺度对流状态的相反转变则随着达西数的增加而发生。
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Passive convective ventilation in a double air-porous layer with internal heat generation depending on solid fraction
The convective stability of a two-layered system consisting of a heat-generating porous region underlying an air region has been numerically studied. The linear dependence of the heat release on the solid volume fraction is taken into account in the porous region. The equal constant temperature values are fixed on the external impermeable boundaries of the system. The critical internal Rayleigh-Darcy number at which the convection is induced in the system in the form of two-dimensional roll patterns with a given wave number has been determined. The convective flow is possible due to the formation of unstable density stratification in the presence of internal heat release. Two types of stationary convection, namely, the local and the large-scale convection, have been studied. The local flow arises in the air sublayer and scarcely penetrates into the porous sublayer. The large-scale convection covers both sublayers. The change in the convective regime occurs with the growth of one or another parameter of the system and indicates the variation of the instability type. It is accompanied by an abrupt (by times and tens of times) change in the critical wave number of roll patterns. Numerical calculations show a decrease in the onset value for both types of convection with increasing solid volume fraction ϕ in the porous sublayer and increasing relative thickness d of the air sublayer. The growth of the Darcy number (the dimensionless per-meability of the porous sublayer) also causes destabilization of the air motionless state at the given ϕ and d. The variation of the convection regime from a large-scale flow to a local one occurs with increasing relative thickness of the air sublayer, whereas an opposite transition from the local to the large-scale convection regime is observed with increasing Darcy number.
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