考虑MHD效应的实心球混合对流的Keller-Box格式

Mohammad Ghani, Wayan Rumite
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引用次数: 4

摘要

混合对流是由于密度不同而产生的浮力引起的自由对流和由于增加热交换率的外力引起的强制对流的结合。这意味着,在自由对流中,除了浮力外,外力的作用也很重要。在本研究中,具有粘弹性效应的流体类型是非牛顿流体。通过球体表面的粘弹性流体形成一薄层,由于它们的主要粘度,这一薄层被称为边界层。将得到的极限层与边界层的厚度——下停滞点附近进行分析,得到了三维边界层方程、连续性方程、动量方程和能量方程。然后利用无量纲变量将这些有量纲的边界层方程转化为无量纲的边界层方程。利用流函数将无量纲边界层方程转化为常微分方程,得到了非相似边界层方程。采用凯勒盒有限差分法对这些非相似边界层方程进行了数值求解。离散化结果是非线性的,应采用牛顿线性化技术进行线性化处理。数值解分析了普朗特数、粘弹性、混合对流和MHD参数对速度分布、温度分布和壁面温度的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Keller-Box Scheme to Mixed Convection Flow Over a Solid Sphere with the Effect of MHD
Mixed convection is the combination of a free convection caused by the buoyancy forces due to the different density and a forced convection due to external forces that increase the heat exchange rate. This means that, in free convection, the effect of external forces is significant besides buoyancy forces. In this study the fluid type with viscoelastic effect is non-Newtonian. The viscoelastic fluids that pass over a surface of a sphere form a thin layer, which due to their dominant viscosity is called by the border layer. The obtained limiting layer is analyzed with the thickness of the boundary layer-  near the lower stagnating point, then obtained dimensional boundary layer equations, continuity, momentum, and energy equations. These dimensional boundary layer equations are then transformed into non-dimensional boundary layer equations by using non-dimensional variables. Further, the non-dimensional boundary layer equations are transformed into ordinary differential equations by using stream function, so that obtained the non-similar boundary layer equations. These non-similar boundary layer equations are solved numerically by using finite difference method of Keller-Box. The discretization results are non-linear and it should be linearized using newton linearization technique. The numerical solutions are analyzed the effect of Prandtl number, viscoelastic, mixed convection, and MHD parameters towards velocity profile, temperature profile, and wall temperature.
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