Laidoudi Houssem, Abderrahmane Aissa, Saeed Abdulkafi Mohammed, Guedri Kamel, Weera Wajaree, Younis Obai, Mourad Abed, Marzouki Riadh
Laboratory of Sciences and Marine Engineering, Faculty of Mechanical Engineering, University of Science and Technology of Oran-Mohamed Boudiaf, Oran 31000, Algeria.
Laboratoire de Physique Quantique de la Matière et Modélisation Mathématique (LPQ3M), University of Mascara, Mascara 29000, Algeria.
Nanomaterials (Basel). 2022 May 20;12(10):1747. doi: 10.3390/nano12101747.
This paper presents a numerical simulation of a magneto-convection flow in a 3D chamber. The room has a very specific permeability and a zigzag bottom wall. The fluid used in this study is AlO-Cu/water with 4% nanoparticles. The Galerkin finite element technique (GFEM) was developed to solve the main partial equations. The hybrid nanofluid inside the container is subjected to the horizontal motion of the upper wall, an external magnetic field, and a thermal buoyancy force. The present numerical methodology is validated by previous data. The goal of this investigation was to understand and determine the percentage of heat energy transferred between the nanofluid and the bottom wall of the container under the influence of a set of criteria, namely: the movement speed of the upper wall of the cavity (Re = 1 to 500), the amount of permeability (Da = 10 to 10), the intensity of the external magnetic field (Ha = 0 to 100), the number of zigzags of the lower wall (N = 1 to 4), and the value of thermal buoyancy when the force is constant (Gr = 1000). The contours of the total entropy generation, isotherm, and streamline are represented in order to explain the fluid motion and thermal pattern. It was found that the heat transfer is significant when (N = 4), where the natural convection is dominant and (N = 2), and the forced convection is predominant.
本文呈现了对三维腔体内磁对流流动的数值模拟。该腔室具有非常特殊的磁导率和锯齿形底壁。本研究中使用的流体是含4%纳米颗粒的AlO-Cu/水。采用伽辽金有限元技术(GFEM)来求解主要的偏微分方程。容器内的混合纳米流体受到上壁的水平运动、外部磁场和热浮力的作用。当前的数值方法通过先前的数据进行了验证。本研究的目的是在一组条件的影响下,理解并确定纳米流体与容器底壁之间传递的热能百分比,这些条件即:腔室上壁的移动速度(雷诺数Re = 1至500)、磁导率数值(达西数Da = 10至10)、外部磁场强度(哈特曼数Ha = 0至100)、下壁的锯齿数量(N = 1至4)以及力恒定时的热浮力值(格拉晓夫数Gr = 1000)。为了解释流体运动和热模式,给出了总熵产生、等温线和流线的等高线图。结果发现,当(N = 4)时热传递显著,此时自然对流占主导,以及(N = 2)时,强制对流占主导。