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指数拉伸表面上交叉纳米流体流动的热对流创新建模与模拟

Innovation modeling and simulation of thermal convective on cross nanofluid flow over exponentially stretchable surface.

作者信息

Ali Mehboob, Pasha Amjad Ali, Nawaz Rab, Khan Waqar Azeem, Irshad Kashif, Algarni Salem, Alqahtani Talal

机构信息

School of Mathematics and Physics, Guangxi Minzu University, Nanning, 530006, China.

Aerospace Engineering Department, King Abdulaziz University, Jeddah, 21589, Saudi Arabia.

出版信息

Heliyon. 2023 Jul 26;9(8):e18672. doi: 10.1016/j.heliyon.2023.e18672. eCollection 2023 Aug.

DOI:10.1016/j.heliyon.2023.e18672
PMID:37576213
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10412758/
Abstract

This work reported to investigate convective flow of non-Newtonian fluid effect on an exponentially stretchable surface. Effect of nanoparticle is considered in heat and mass equation. The transformation technique utilized on dimensionless equations is converted to non-dimensionless equations are solved thought numerical approach Bvp4c. Influence of approatiate analysis of velocities, heat and mass transport are scrutinized through figures. Furthermore, the comparative analysis of drag forces, Nusselt number and Sherwood number are evaluated over and done with tabulated values. It is give details that the temperature field strengthens with intensification in thermophoresis and random diffusions. Similarly, rises in thermophoresis effect parameter both temperature and concentration profile increasing.

摘要

这项工作旨在研究非牛顿流体对流对指数可拉伸表面的影响。在热量和质量方程中考虑了纳米颗粒的影响。利用变换技术将无量纲方程转化为无量纲方程,并通过数值方法Bvp4c求解。通过图表详细研究了速度、热量和质量传输的适当分析的影响。此外,通过表格值对阻力、努塞尔数和舍伍德数进行了比较分析。详细说明了温度场随着热泳和随机扩散的增强而增强。同样,热泳效应参数的增加会使温度和浓度分布都增加。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/714b26998cd5/gr11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/ecc692f4b362/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/29ef6be2803c/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/f3bdb0702655/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/64783ff6780a/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/669d799f83a8/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/10cc6ede1494/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/18fca95d107a/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/38d919680be0/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/26b8845fec61/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/cfa5046283d7/gr10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/714b26998cd5/gr11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/ecc692f4b362/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/29ef6be2803c/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/f3bdb0702655/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/64783ff6780a/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/669d799f83a8/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/10cc6ede1494/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/18fca95d107a/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/38d919680be0/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/26b8845fec61/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/cfa5046283d7/gr10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/83c0/10412758/714b26998cd5/gr11.jpg

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