基于Cattaneo-Christov模型的双层纳米流体磁流体动力学(MHD)流动和传热

N. Khashi’ie, N. Arifin, E. Hafidzuddin, N. Wahi, M. R. Ilias
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引用次数: 3

摘要

本文利用Cattaneo-Christov热流密度模型求解了纳米流体在存在磁场和双分层的垂直拉伸薄片上的流动和传热问题。热浮力和溶质浮力也进行了研究,以处理双重分层效应。Buongiorno的纳米流体模型被用来结合布朗运动和热泳的影响。采用适当的变换将具有非傅立叶能量方程的边界层简化为非线性常(相似)微分方程组,然后在MATLAB软件中使用bvp4c求解器进行数值求解。将少数有限情况下的局部努塞尔数和舍伍德数制成表格,并与早期发表的作品进行比较。结果表明,该方法与前人的研究结果是一致的,从而验证了本方法的有效性。数值解图形演示了几个参数,即磁,热松弛,分层(热和溶质),热泳动和布朗运动的速度,温度和纳米颗粒体积分数剖面。热松弛参数(Cattaneo-Christov模型)的施加使传热速率上升,而热分层参数和溶质分层参数的增加分别降低了温度和纳米颗粒浓度分布。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Magnetohydrodynamics (MHD) Flow and Heat Transfer of a Doubly Stratified Nanofluid Using Cattaneo-Christov Model
The present study utilized Cattaneo-Christov heat flux model for solving nanofluid flow and heat transfer towards a vertical stretching sheet with the presence of magnetic field and double stratification. Thermal and solutal buoyancy forces are also examined to deal with the double stratification effects. Buongiorno's model of nanofluid is used to incorporate the effects of Brownian motion and thermophoresis. The boundary layer with non-Fourier energy equations are reduced into a system of nonlinear ordinary (similarity) differential equations using suitable transformations and then numerically solved using bvp4c solver in MATLAB software. The local Nusselt and Sherwood numbers of few limited cases are tabulated and compared with the earlier published works. It showed that a positive agreement was found with the previous study and thus, validated the present method. Numerical solutions are graphically demonstrated for several parameters namely magnetic, thermal relaxation, stratifications (thermal and solutal), thermophoresis and Brownian motion on the velocity, temperature and nanoparticles volume fraction profiles. An upsurge of the heat transfer rate was observed with the imposition of the thermal relaxation parameter (Cattaneo-Christov model) whereas the accretion of thermal and solutal stratification parameters reduced the temperature and nanoparticles concentration profiles, respectively.
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