Convective Rolls in a Compressible Fluid

Katherine J. Simzer, G. Lewis
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Abstract

Rayleigh-Bénard convection occurs between two horizontally infinite plates when the lower plate is heated with respect to the upper one. The temperature gradient between the two plates causes convective rolls to form as the warmer fluid below becomes more buoyant than the cooler fluid above it. The standard (classical) analysis uses the Boussinesq approximation, which neglects the variations of fluid density except in relation to buoyancy forces. This approximation is not accurate for some real-world applications. This project is inspired by the atmosphere, so we will consider the onset of convection in a vertically stratified layer of fluid which we model using the anelastic equations. The standard analysis is presented in many textbooks and is used as a comparison to the analysis for the compressible fluid presented here. Using linear stability analysis, we compute the critical temperature differences required to induce convection. It is not possible to find analytical solutions, and therefore, numerical methods implemented in Python using LAPACK subroutines are used. Results of the critical Rayleigh number at the half-height of the fluid for a range of plate separation distances are computed. For all the cases that are considered, the solution for the compressible problem follows the standard solution for plate separation distances smaller than some viscosity-dependent value that increases with the viscosity of the fluid. For larger d, it is observed that the stratification inhibits the onset of convection. Our solution is far more idealized than any actual convection happening in the atmosphere. However, it does demonstrate, in this context, the limits of the Boussinesq approximation.
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可压缩流体中的对流滚动
当下层板相对于上层板受热时,在两个水平无限大的板之间就会发生瑞利-伯氏对流。当下面较热的流体比上面较冷的流体浮力更大时,两个板块之间的温度梯度导致对流翻滚形成。标准(经典)分析使用Boussinesq近似,除了与浮力有关的变化外,它忽略了流体密度的变化。对于某些实际应用程序,这种近似并不准确。该项目受到大气的启发,因此我们将考虑垂直分层流体层中对流的开始,我们使用非弹性方程对其进行建模。标准分析在许多教科书中都有介绍,并被用作与这里介绍的可压缩流体分析的比较。利用线性稳定性分析,我们计算了诱导对流所需的临界温差。不可能找到解析解,因此,使用使用LAPACK子程序在Python中实现的数值方法。计算了一定距离下流体半高处的临界瑞利数。对于所考虑的所有情况,可压缩问题的解遵循板分离距离小于某个随流体粘度增加的粘度相关值的标准解。对于较大的d,可以观察到分层抑制对流的发生。我们的解决方案比大气中发生的任何实际对流都要理想化得多。然而,在这种情况下,它确实证明了Boussinesq近似的局限性。
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