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具有波浪形边界、底部加热且有旋转圆柱的三角形腔内纳米流体混合对流的热液与熵研究

Hydrothermal and Entropy Investigation of Nanofluid Mixed Convection in Triangular Cavity with Wavy Boundary Heated from below and Rotating Cylinders.

作者信息

Cherif Bellakhdar Mohamed, Abderrahmane Aissa, Saeed Abdulkafi Mohammed, Qasem Naef A A, Younis Obai, Marzouki Riadh, Chung Jae Dong, Shah Nehad Ali

机构信息

Laboratoire de Physique Quantique de la Matière et Modélisation Mathématique (LPQ3M), University Mustapha Stambouli of Mascara, Mascara 29000, Algeria.

Department of Mathematics, College of Science, Qassim University, P.O. Box 6644, Buraydah 51452, Saudi Arabia.

出版信息

Nanomaterials (Basel). 2022 Apr 26;12(9):1469. doi: 10.3390/nano12091469.

DOI:10.3390/nano12091469
PMID:35564178
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9099981/
Abstract

Nanofluids have become important working fluids for many engineering applications as they have better thermal properties than traditional liquids. Thus, this paper addresses heat transfer rates and entropy generation for a FeO/MWCNT-water hybrid nanoliquid inside a three-dimensional triangular porous cavity with a rotating cylinder. The studied cavity is heated by a hot wavy wall at the bottom and subjected to a magnetic field. This problem is solved numerically using the Galerkin finite element method (GFEM). The influential parameters considered are the rotating cylinder speed, Hartmann number (Ha), Darcy number (Da), and undulation number of the wavy wall. The results showed that higher Da and lower Ha values improved the heat transfer rates in the cavity, which was demonstrated by a higher Nusselt number and flow fluidity. The entropy generation due to heat losses was also minimized for the enhanced heat transfer rates. The decrease in Ha from 100 and 0 improved the heat transfer by about 8%, whereas a high rotational speed and high Da values yield optimal results. For example, for Ω = 1000 rad/s and Da = 10, the enhancement in the average Nusselt number is about 38% and the drop in the Bejan number is 65% compared to the case of Ω = 0 rad/s and Da = 10. Based on the applied conditions, it is recommended to have a high Da, low Ha, one undulation for the wavy wall, and high rotational speed for the cylinder in the flow direction.

摘要

纳米流体已成为许多工程应用中的重要工作流体,因为它们具有比传统液体更好的热性能。因此,本文研究了在带有旋转圆柱的三维三角形多孔腔内,FeO/MWCNT-水混合纳米流体的传热速率和熵产生。所研究的腔体底部由热的波浪壁加热,并施加磁场。该问题采用伽辽金有限元法(GFEM)进行数值求解。考虑的影响参数有旋转圆柱速度、哈特曼数(Ha)、达西数(Da)和波浪壁的波动数。结果表明,较高的Da值和较低的Ha值提高了腔内的传热速率,这通过较高的努塞尔数和流体流动性得到证明。对于增强的传热速率,由于热损失产生的熵也最小化。Ha从100降至0时,传热提高了约8%,而高转速和高Da值产生了最佳结果。例如,对于Ω = 1000 rad/s和Da = 10,与Ω = 0 rad/s和Da = 10的情况相比,平均努塞尔数的增强约为38%,贝詹数的下降为65%。基于所应用的条件,建议在流动方向上具有高Da、低Ha、波浪壁有一个波动以及圆柱的高转速。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/7204ab513b07/nanomaterials-12-01469-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/2dd29c9482a1/nanomaterials-12-01469-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/de2812765c53/nanomaterials-12-01469-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/1f8b7a963651/nanomaterials-12-01469-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/bf263b323736/nanomaterials-12-01469-g004a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/3abd828c0521/nanomaterials-12-01469-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/95daf5f3bbc8/nanomaterials-12-01469-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/0a95db713aa2/nanomaterials-12-01469-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/513b78ad12e0/nanomaterials-12-01469-g008a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/7204ab513b07/nanomaterials-12-01469-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/2dd29c9482a1/nanomaterials-12-01469-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/de2812765c53/nanomaterials-12-01469-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/1f8b7a963651/nanomaterials-12-01469-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/bf263b323736/nanomaterials-12-01469-g004a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/3abd828c0521/nanomaterials-12-01469-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/95daf5f3bbc8/nanomaterials-12-01469-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/0a95db713aa2/nanomaterials-12-01469-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/513b78ad12e0/nanomaterials-12-01469-g008a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b9f/9099981/7204ab513b07/nanomaterials-12-01469-g009.jpg

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