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Extended Oberbeck-Boussinesq approximation study of convective instabilities in a porous layer with horizontal flow and bottom heating

机译:具有水平流动和底部加热的多孔层对流不稳定性的扩展Oberbeck-Boussinesq近似研究

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摘要

A study of the onset of convective instabilities in a porous layer with a horizontal basic flow is performed by including the effects of viscous dissipation and pressure work in the energy balance. Firstly, the so-called extended Oberbeck-Boussinesq approximation, i.e. the model based on the enthalpy formulation of the energy balance, is adopted. Then, the results for the marginal stability condition are compared with those obtained by the so-called Chandrasekhar approximation, i.e. the model based on the internal-energy formulation of the energy balance. It is shown that a marked discrepancy occurs between the two approaches, that becomes specially evident for high values of the Gebhart number. According to the extended Oberbeck-Boussinesq approximation, the effects of the viscous dissipation and of the pressure work result in a stabilization of the basic flow. On the contrary, the Chandrasekhar approximation predicts a destabilization of the basic flow induced by the viscous dissipation. The destabilization can be so intense that the onset of convective rolls may occur even in the absence of a boundary temperature difference, i.e. with a vanishing Darcy-Rayleigh number.
机译:通过在能量平衡中包括粘性耗散和压力功的影响,对具有水平基本流动的多孔层中对流不稳定性的开始进行了研究。首先,采用所谓的扩展的Oberbeck-Boussinesq近似,即基于能量平衡的焓公式的模型。然后,将边际稳定条件的结果与通过所谓的Chandrasekhar近似(即基于能量平衡的内部能量公式的模型)获得的结果进行比较。结果表明,两种方法之间存在明显的差异,对于高Gebhart数值,这尤其明显。根据扩展的Oberbeck-Boussinesq逼近,粘性耗散和压力功的作用导致基本流量的稳定。相反,Chandrasekhar近似预测了由粘性耗散引起的基本流量的不稳定。失稳可能非常剧烈,以至于即使在没有边界温度差的情况下,即在达西-瑞利数消失的情况下,也可能发生对流辊的开始。

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