Thermal analysis of transient MHD ferrofluid flow and natural convection in a Porous cavity with a cylindrical barrier

The effects of Darcy, Rayleigh, and Hartmann numbers on the time-dependent (0≤t≤0.15seconds) This article investigates the ferrofluid flow behavior in a porous square cavity with a cylindrical barrier filled with 5 % iron oxide III ferroparticles (Fe3O4) and water (H2O) as the base fluid. The govern...

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Main Authors: Pan Zhang, Hassan Roshani, Payam Jalili, Bahram Jalili, Hammad. Alotaibi, Davood Domiri Ganji
Format: Article
Language:English
Published: Elsevier 2025-02-01
Series:Case Studies in Thermal Engineering
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Online Access:http://www.sciencedirect.com/science/article/pii/S2214157X24017246
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author Pan Zhang
Hassan Roshani
Payam Jalili
Bahram Jalili
Hammad. Alotaibi
Davood Domiri Ganji
author_facet Pan Zhang
Hassan Roshani
Payam Jalili
Bahram Jalili
Hammad. Alotaibi
Davood Domiri Ganji
author_sort Pan Zhang
collection DOAJ
description The effects of Darcy, Rayleigh, and Hartmann numbers on the time-dependent (0≤t≤0.15seconds) This article investigates the ferrofluid flow behavior in a porous square cavity with a cylindrical barrier filled with 5 % iron oxide III ferroparticles (Fe3O4) and water (H2O) as the base fluid. The governing equations for the ferrofluid flow have been solved using Galerkin's finite element method. The boundary conditions are the cylindrical barrier, a part of the lower face of the cavity having a high temperature, the side faces of the cavity having a low temperature, and the remaining parts adiabatic. While observing the non-slip condition in all geometry surfaces, the square cavity, cylindrical barrier, and ferrofluid inside are under the magnetic field's influence. The range of Rayleigh numbers studied in the article is 103≤Ra≤105, Darcy number 10−5≤Da≤10−3 and Hartmann number Ha=20,100, and finally, their effect on heat transfer and flow behavior has been investigated. The results show that increasing the Darcy number affected the velocity profiles in each Rayleigh and Hartmann number. Also, changes in ferrofluid velocity with respect to time according to different Rayleigh, Darcy, and Hartmann numbers were significant, while temperature changes with time were less compared to velocity changes with time.
format Article
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institution Kabale University
issn 2214-157X
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publishDate 2025-02-01
publisher Elsevier
record_format Article
series Case Studies in Thermal Engineering
spelling doaj-art-dde4837301df49619310ea8b712907592025-02-02T05:27:11ZengElsevierCase Studies in Thermal Engineering2214-157X2025-02-0166105693Thermal analysis of transient MHD ferrofluid flow and natural convection in a Porous cavity with a cylindrical barrierPan Zhang0Hassan Roshani1Payam Jalili2Bahram Jalili3Hammad. Alotaibi4Davood Domiri Ganji5School of Mechanical Engineering, Sichuan University Jinjiang College, Meishan, Sichuan, 620860, ChinaDepartment of Mechanical Engineering, North Tehran Branch, Islamic Azad University, Tehran, IranDepartment of Mechanical Engineering, North Tehran Branch, Islamic Azad University, Tehran, IranDepartment of Mechanical Engineering, North Tehran Branch, Islamic Azad University, Tehran, IranDepartment of Mathematics and Statistics, College of Science, Taif University, P.O. Box 11099, Taif, 21944, Saudi ArabiaDepartment of Mechanical Engineering, Babol Noshirvani University of Technology, P.O. Box 484, Babol, Iran; Corresponding author.The effects of Darcy, Rayleigh, and Hartmann numbers on the time-dependent (0≤t≤0.15seconds) This article investigates the ferrofluid flow behavior in a porous square cavity with a cylindrical barrier filled with 5 % iron oxide III ferroparticles (Fe3O4) and water (H2O) as the base fluid. The governing equations for the ferrofluid flow have been solved using Galerkin's finite element method. The boundary conditions are the cylindrical barrier, a part of the lower face of the cavity having a high temperature, the side faces of the cavity having a low temperature, and the remaining parts adiabatic. While observing the non-slip condition in all geometry surfaces, the square cavity, cylindrical barrier, and ferrofluid inside are under the magnetic field's influence. The range of Rayleigh numbers studied in the article is 103≤Ra≤105, Darcy number 10−5≤Da≤10−3 and Hartmann number Ha=20,100, and finally, their effect on heat transfer and flow behavior has been investigated. The results show that increasing the Darcy number affected the velocity profiles in each Rayleigh and Hartmann number. Also, changes in ferrofluid velocity with respect to time according to different Rayleigh, Darcy, and Hartmann numbers were significant, while temperature changes with time were less compared to velocity changes with time.http://www.sciencedirect.com/science/article/pii/S2214157X24017246Heat transferConvectionMHDTime-dependentPorous mediumFerrofluid
spellingShingle Pan Zhang
Hassan Roshani
Payam Jalili
Bahram Jalili
Hammad. Alotaibi
Davood Domiri Ganji
Thermal analysis of transient MHD ferrofluid flow and natural convection in a Porous cavity with a cylindrical barrier
Case Studies in Thermal Engineering
Heat transfer
Convection
MHD
Time-dependent
Porous medium
Ferrofluid
title Thermal analysis of transient MHD ferrofluid flow and natural convection in a Porous cavity with a cylindrical barrier
title_full Thermal analysis of transient MHD ferrofluid flow and natural convection in a Porous cavity with a cylindrical barrier
title_fullStr Thermal analysis of transient MHD ferrofluid flow and natural convection in a Porous cavity with a cylindrical barrier
title_full_unstemmed Thermal analysis of transient MHD ferrofluid flow and natural convection in a Porous cavity with a cylindrical barrier
title_short Thermal analysis of transient MHD ferrofluid flow and natural convection in a Porous cavity with a cylindrical barrier
title_sort thermal analysis of transient mhd ferrofluid flow and natural convection in a porous cavity with a cylindrical barrier
topic Heat transfer
Convection
MHD
Time-dependent
Porous medium
Ferrofluid
url http://www.sciencedirect.com/science/article/pii/S2214157X24017246
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