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Thermal convection of non-Newtonian fluids.

机译:非牛顿流体的热对流。

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摘要

The thermo-gravitational instability in a fluid layer of a non-Newtonian medium heated from below is investigated. The non-Newtonian fluids under study are the generalized Newtonian (shear-thinning and –thickening) fluids with and without elasticity. The fluid is assumed to obey the Carreau-Bird model of viscosity for the case of inelastic shear-thinning/thickening fluids, and for the case of elastic shear-thinning fluids the Oldroyd-B constitutive equation is applied. For the dependence of the viscosity on the rate of strain, the Carreau-Bird model of viscosity is applied on the polymeric solute contribution to the solution viscosity. This model is traditionally called the Phan-Thien-Tanner-B constitutive equation. Linear and weakly nonlinear analyses are successively presented.;Next, the weakly nonlinear method of amplitude equations is implemented to investigate the convective flow patterns of inelastic shear-thinning and –thickening fluids in a slightly supercritical range. Although the critical threshold is the same as for a Newtonian fluid, it is found that non-Newtonian fluids can convect in the form of rolls, squares or hexagons depending on the shear-thinning level. Similarly to Newtonian fluids, shear-thickening fluids convect only in the form of rolls. The stability of the convective steady branches is carried out to determine under which specific conditions a pattern is preferred. The influence of the rheological and physical parameters is examined and discussed in detail. Next, the weakly nonlinear method of amplitude equations is implemented to investigate the convective flow patterns of shear-thinning and – thickening fluids in a slightly supercritical range.;Finally, the low order dynamical system approach (the modified Lorenz model) is implemented to investigate the Rayleigh-Bénard convection of the elastic shear-thinning fluids. It is found that interaction between elasticity and shear-thinning limits the domain of stability of rolls further compared to the inelastic shear-thinning fluids or viscoelatsic fluids with constant viscosity.;Keywords: Rayleigh-Bénard convection, generalized Newtonian fluids, elastic shear-thinning fluids, linear stability analysis, amplitude equations approach, the Lorenz model.;First, the conventional nonlinear approaches for the Rayleigh-Bénard convection are reviewed. Two of the famous nonlinear approaches for the slightly post-critical range, namely, the Lorenz model and the method of amplitude equations are emphasized here. Similarities and differences of the results of these approaches on steady two-dimensional flow and its stability, and the transient behavior are investigated. Moreover, the role of the non-dimensional groups, the Rayleigh number and the Prandtl number are scrutinized.
机译:研究了从下方加热的非牛顿介质的流体层中的热重力不稳定性。所研究的非牛顿流体是具有和没有弹性的广义牛顿流体(剪切变稀和增稠)。对于非弹性剪切稀化/增稠流体,假定流体服从Carreau-Bird粘度模型;对于弹性剪切稀化流体,假定应用Oldroyd-B本构方程。为了使粘度取决于应变速率,将Carreau-Bird粘度模型应用于聚合物溶质对溶液粘度的贡献。传统上将此模型称为Phan-Thien-Tanner-B本构方程。依次介绍了线性分析和弱非线性分析。接着,采用振幅方程的弱非线性方法研究了在稍微超临界范围内非弹性剪切稀化和增稠流体的对流流动模式。尽管临界阈值与牛顿流体的临界阈值相同,但是发现非牛顿流体可以根据剪切稀化水平以辊,正方形或六边形的形式对流。与牛顿流体相似,增稠剪切流体仅以辊的形式对流。进行对流稳定分支的稳定性以确定在哪种特定条件下优选图案。流变和物理参数的影响进行了检查和详细讨论。接下来,采用振幅方程的弱非线性方法来研究稀薄稠化流体在较超临界范围内的对流流动模式。最后,采用低阶动力系统方法(改进的Lorenz模型)进行研究。弹性剪切稀化流体的瑞利-贝纳德对流。与恒定粘度的非弹性剪切稀化流体或粘弹性流体相比,弹性与剪切稀化之间的相互作用进一步限制了轧辊的稳定性。关键词:瑞利-贝纳德对流广义牛顿流体弹性剪切稀化流体,线性稳定性分析,振幅方程法,洛伦兹模型。首先,回顾了常规的瑞利-贝纳德对流非线性方法。在此重点介绍了后临界范围内的两种著名的非线性方法,即Lorenz模型和振幅方程方法。研究了这些方法对稳定二维流动及其稳定性以及瞬态行为的结果的异同。此外,仔细研究了无量纲组的作用,瑞利数和普朗特数。

著录项

  • 作者

    Albaalbaki, Bashar.;

  • 作者单位

    The University of Western Ontario (Canada).;

  • 授予单位 The University of Western Ontario (Canada).;
  • 学科 Engineering Mechanical.
  • 学位 Ph.D.
  • 年度 2011
  • 页码 141 p.
  • 总页数 141
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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