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首页> 外文期刊>Journal of thermal analysis and calorimetry >LBM simulation of MHD nanofluid heat transfer in a square cavity with a cooled porous obstacle: effects of various temperature boundary conditions
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LBM simulation of MHD nanofluid heat transfer in a square cavity with a cooled porous obstacle: effects of various temperature boundary conditions

机译:用冷却多孔障碍物的平方腔中MHD纳米流体传热的LBM模拟:各种温度边界条件的影响

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摘要

Nanofluid natural convection inside a cavity with a porous square obstacle in the presence of magnetic field is simulated by lattice Boltzmann method. The porous obstacle is adopted by Sierpinski carpets fractal pattern, and three kinds of temperature boundary conditions are set up on the hot walls. The combination of five topics including LBM, Sierpinski carpets, nanofluid, magnetic field and various temperature boundary conditions is the main novelty of the present paper. The effects of temperature boundary condition, configuration of Sierpinski carpets porous obstacle, Rayleigh number, nanoparticle volume fraction and Hartmann number on the flow pattern, temperature distribution and heat transfer characteristics are studied. The results show that the local and average Nusselt numbers are increasing functions of phi and Ra, but a decreasing function of Ha, regardless of the boundary conditions. The heat transfer enhancement by adding nanoparticles is more effective at low phi. The rate of heat transfer with different temperature boundary conditions is Case 3 > Case 2 > Case 1. At high Hartmann number, the obstacle configuration affects the rate of heat transfer very slightly. However, at low Hartmann number, the effect of obstacle configuration on the average Nusselt number should be considered. The effect of obstacle configuration on the rate heat transfer is also influenced by the temperature boundary conditions.
机译:采用格子Boltzmann方法模拟了磁场作用下多孔方形障碍物空腔内纳米流体的自然对流。多孔障碍物采用Sierpinski地毯分形图案,并在热壁上设置了三种温度边界条件。将LBM、Sierpinski地毯、纳米流体、磁场和各种温度边界条件等五个主题结合起来是本论文的主要创新点。研究了温度边界条件、Sierpinski地毯多孔障碍物结构、瑞利数、纳米颗粒体积分数和哈特曼数对流型、温度分布和传热特性的影响。结果表明,无论边界条件如何,局部努塞尔数和平均努塞尔数都是φ和Ra的增函数,而不是Ha的减函数。在较低的phi下,添加纳米颗粒的强化传热效果更好。不同温度边界条件下的传热速率为案例3>案例2>案例1。在高哈特曼数时,障碍物构型对传热速率的影响非常小。然而,在哈特曼数较低时,应考虑障碍物结构对平均努塞尔数的影响。障碍物结构对传热速率的影响也受温度边界条件的影响。

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