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Stability of quasi-equilibrium states and supercritical regimes of thermal vibrational convection of a Williamson fluid in zero gravity conditions

机译:零重力条件下Williamson流体的准平衡态的稳定性和热振动对流的超临界状态

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In this paper we investigate a linear stability of quasi-equilibrium states and supercritical regimes of thermal vibrational convection of a Williamson fluid between two rigid parallel plates, maintained at constant different temperatures in zero gravity conditions. Calculations are made for different angles of inclination of the vibration axis relative to the layer. It has been found that, as in the case of a Newtonian fluid, most dangerous are the hydrodynamic monotonic perturbations. Enhancement of viscoplastic properties of a fluid has a destabilizing effect at all angles of inclination of the vibration axis. An increase in the Prandtl number stabilizes the quasi-equilibrium states of the pseudoplastic fluids. In the viscoplastic limit, the critical value of the modified Rayleigh number, which determines the quasi-equilibrium stability threshold, does not depend on the Prandtl number and rheological parameters. The critical value of the perturbation wave number for pseudo- and viscoplastic fluids depends only on the angle of inclination of the vibration axis. The type of the convection excitation and the structure of the supercritical convective flows under longitudinal vibrations have been studied on the basis of full nonlinear equations of thermal vibrational convection. It has been found that the supercritical bifurcation takes place. (C) 2018 Elsevier Ltd. All rights reserved.
机译:在本文中,我们研究了两个刚性平行板之间的Williamson流体的准平衡态的线性稳定性和热振动对流的超临界状态,并在零重力条件下保持恒定的不同温度。针对振动轴相对于层的不同倾斜角度进行计算。已经发现,就牛顿流体而言,最危险的是流体动力学单调摄动。流体粘塑性的增强在振动轴的所有倾斜角上都具有不稳定作用。普朗特数的增加稳定了假塑性流体的准平衡态。在粘塑性极限中,确定准平衡稳定性阈值的修正瑞利数的临界值不取决于普朗特数和流变参数。假塑性和粘塑性流体的摄动波数的临界值仅取决于振动轴的倾斜角度。基于热振动对流的完全非线性方程,研究了纵向振动条件下对流激发的类型和超临界对流的结构。已经发现发生了超临界分叉。 (C)2018 Elsevier Ltd.保留所有权利。

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