Ain Shams Engineering Journal ( IF 6.0 ) Pub Date : 2021-08-23 , DOI: 10.1016/j.asej.2021.08.005 Noura Alsedais 1 , Abdelraheem M. Aly 2, 3 , Mohamed Ahmed Mansour 4
The paper is aiming to examine the magnetic impacts on the mixed convection of a nanofluid contained by an undulating porous cavity with the help of radiative and heat generation. The condition of the local thermal non-equilibrium (LTNE) is considered. The partial heater is in the corrugated bottom partition and the top corrugated partition has . The vertical walls are adiabatic with a lid-velocity in the right wall. The regulating equations are worked out by the finite volume method (FVM). The involved parameters are the heater length (between and ), heat generation/absorption coefficient (between −2 and 2), modified conductivity ratio (between ), thermal radiation parameter (between 0 and 5), a porosity parameter (between 0.4 and 0.9), heater position (between 0.3 and 0.7), thermal conductivity ratio (between 4 and 0.25), an undulating number (between 1 and 5), Darcy parameter (between and ), an inclination angle of a cavity (between and ), nanoparticles parameter (between 0 and 0.1), and coefficient of an inter-phase heat transfer (between 0 and 5000). The results indicated that the growth in nanoparticles parameter augments the profiles of average of a fluid phase. The heat transfer is influenced by the variations in the length/position of the heater source. The maximum of the streamlines decreases by 97.55% as decreases from to and increases by 42.86% as an undulating number raises from 1 to 5.
中文翻译:
含障碍物和多孔介质饱和的纳米流体填充波状空腔混合对流的局部热非平衡条件
该论文的目的是在辐射和发热的帮助下,研究磁性对包含在起伏多孔腔中的纳米流体的混合对流的影响。考虑了局部热非平衡 (LTNE) 的条件。局部加热器在波纹底部隔板上,顶部波纹隔板上有. 垂直壁是绝热的,右壁具有盖子速度。调节方程是通过有限体积法(FVM)计算出来的。涉及的参数是加热器长度 (之间 和 ), 发热/吸收系数 (-2 和 2 之间),修正的电导率比(在 )、热辐射参数 (介于 0 和 5 之间),孔隙度参数 (在 0.4 和 0.9 之间),加热器位置 (0.3~0.7之间),导热系数 (在 4 到 0.25 之间),一个起伏的数字 (1到5之间),达西参数 (之间 和 ),腔的倾角 (之间 和 ),纳米颗粒参数 (在 0 和 0.1 之间),以及相间传热系数 (在 0 到 5000 之间)。结果表明,纳米粒子参数的增长增加了平均的流体相。热传递受加热源长度/位置变化的影响。流线的最大值减少了 97.55% 为 从 到 并且以波动的形式增长了 42.86% 从 1 升至 5。