带有加热三角块的盖驱动梯形壳体磁流体动力混合对流的有限元分析

M. S. Hossain, M. A. Alim, L. S. Andallah
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引用次数: 2

摘要

对底壁非均匀加热条件下盖驱动梯形外壳内磁流体动力混合对流的数值研究。外壳也由隔热顶壁和冷侧壁组成。它还包含一个加热的三角形块(Rot=0°-90°),位于外壳内的某个位置。外壳的边界顶壁正以均匀的速度U0移动。根据适当的边界条件,用耦合控制方程对模型的几何结构进行数学表示,然后采用基于二维Galerkin有限元的数值方法对本文进行求解。对加热三角块不同旋转时的普朗特数(0.5≤Pr≤2)、雷诺数(60≤Re≤120)、瑞利数(Ra=103)和哈特曼数(Ha=20)等参数进行了数值计算。结果以流线、温度模式或等温线、平均努塞尔数和底壁非均匀加热时外壳中流体的平均体积温度的形式显示。还表明,流线和等温线图案都强烈依赖于上述控制参数和三角块的位置,但三角块的热导率对等温线图案线有着值得注意的作用。此外,本文还演示了热底壁的Nuav和外壳中的θav的变化,以显示外壳中的传热特性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Finite Element Analysis of Magnetohydrodynamic Mixed Convection in a Lid-Driven Trapezoidal Enclosure Having Heated Triangular Block
A numerical research on magnetohydrodynamic mixed convection flow in a lid-driven trapezoidal enclosure at non-uniform heating of bottom wall has been studied numerically. The enclosure consists of insulated top wall and cold side walls, too. It also contains a heated triangular block (Rot = 0° - 90°) located somewhere inside the enclosure. The boundary top wall of the enclosure is moving through uniform speed U0. The geometry of the model has been represented mathematically by coupled governing equations in accordance with proper boundary conditions and then a two-dimensional Galerkin finite element based numerical approach has been adopted to solve this paper. The numerical computations have been carried out for the wide range of parameters Prandtl number (0.5 ≤ Pr ≤ 2), Reynolds number (60 ≤ Re ≤ 120), Rayleigh number (Ra = 103) and Hartmann number (Ha = 20) taking with different rotations of heated triangular block. The results have been shown in the form of streamlines, temperature patterns or isotherms, average Nusselt number and average bulk temperature of the fluid in the enclosure at non-uniform heating of bottom wall. It is also indicated that both the streamlines, isotherm patterns strongly depend on the aforesaid governing parameters and location of the triangular block but the thermal conductivity of the triangular block has a noteworthy role on the isotherm pattern lines. Moreover, the variation of Nuav of hot bottom wall and θav in the enclosure is demonstrated here to show the characteristics of heat transfer in the enclosure.
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