Abstract
In this study, fluid flow and heat transfer in a vertical lid-driven CuO–water nanofluid filled square cavity with a flexible fin attached to its upper wall under the influence of an inclined magnetic field are numerically investigated. The left vertical wall of the cavity is colder than right vertical wall, and it moves in + y direction with constant speed. Horizontal walls of the cavity are insulated. The governing equations are solved with finite element method. The arbitrary Lagrangian–Eulerian method is used to describe the fluid motion within the cavity for the flexible fin in the fluid-structure interaction model. The influence of Richardson number (between 0.01 and 100), Hartmann number (between 0 and 50), inclination angle of the magnetic field (between 0 and 90%), nanoparticle volume fraction (between 0 and 0.05) and Young’s modulus of flexible fin (between 250 and 5000) on the flow and heat transfer were numerically studied. It is observed that the presence of the elastic fin affects the flow field and thermal characteristics of the cavity. The local and average heat transfer enhance as the Richardson number, solid volume fraction of the nanoparticle increase whereas deteriorate as the value of the Hartmann number and inclination angle of the magnetic field increases due to the dampening of the fluid motion with Lorentz forces. The addition of the nanoparticles is more effective along the lower part of the right vertical wall where the heat transfer process is effective. The average heat transfer increases by 28.96% for solid volume fraction of 0.05% compared to base fluid when the flexible fin is attached to the upper wall. The average heat transfer deteriorates by 10.10% for cavity with and without fin at Hartmann number of 50 compared to the case without magnetic field. The average heat transfer enhances as the Young’s modulus of the flexible fin decreases and the average Nusselt number increases by 13.24% for Young’s modulus of 250 compared to configuration for the cavity having the Young’s modulus of 5000.
Similar content being viewed by others
Explore related subjects
Discover the latest articles, news and stories from top researchers in related subjects.Abbreviations
- B 0 :
-
Magnetic field strength
- E :
-
Young’s modulus (\(\hbox{N}\,\hbox{m}^{-2}\))
- Gr :
-
Grashof number
- h :
-
Local heat transfer coefficient (\(\hbox{W}\,\hbox{m}^{-2}\)\(\hbox {K}^{-1}\))
- Ha :
-
Hartmann number
- k :
-
Thermal conductivity (\(\hbox{W}\,\hbox{m}^{-1}\)\(\hbox {K}^{-1}\))
- H :
-
Length of the enclosure (m)
- n :
-
Unit normal vector
- \({Nu}_x\) :
-
Local Nusselt number
- \({Nu}_m\) :
-
Average Nusselt number
- p :
-
Pressure (Pa)
- Pr :
-
Prandtl number
- R :
-
Residual
- Re :
-
Reynolds number
- Ri :
-
Richardson number
- T :
-
Temperature (K)
- u, v :
-
x–y velocity components (\(\hbox{m}\,\hbox{s}^{-1}\))
- w :
-
Weight function
- x, y :
-
Cartesian coordinates (m)
- \(\alpha\) :
-
Thermal diffusivity (\(\hbox {m}^2\hbox { s}^{-1}\))
- \(\beta\) :
-
Expansion coefficient (\(\hbox {K}^{-1}\))
- \(\phi\) :
-
Solid volume fraction
- \(\nu\) :
-
Kinematic viscosity (\(\hbox {m}^2\hbox{ s}\)\(^{-1}\))
- \(\theta\) :
-
Non-dimensional temperature
- \(\rho\) :
-
Density of the fluid (\(\hbox {kg m}^{-3}\))
- \(\lambda\) :
-
Electrical conductivity (\(\hbox{S}\,\hbox{m}^{-1}\))
- \(\sigma\) :
-
Stress tensor (\(\hbox{N}\,\hbox{m}^{-2}\))
- c :
-
Cold
- h :
-
Hot
- m :
-
Average
- nf:
-
Nanofluid
- p :
-
Solid particle
- w :
-
Wall
References
Selimefendigil F, Oztop HF. Effect of a rotating cylinder in forced convection of ferrofluid over a backward facing step. Int J Heat Mass Transf. 2014;71:142–8.
Bednarz T, Patterson JC, Lei C, Ozoe H. Enhancing natural convection in a cube using a strong magnetic field—experimental heat transfer rate measurements and flow visualization. Int Commun Heat Mass Transf. 2009;36:781786.
Selimefendigil F, Oztop HF. MHD mixed convection of nanofluid filled partially heated triangular enclosure with a rotating adiabatic cylinder. J Taiwan Inst Chem Eng. 2014;45:2150–62.
Grosan T, Revnic C, Pop I, Ingham D. Magnetic field and internal heat generation effects on the free convection in a rectangular cavity filled with a porous medium. Int J Heat Mass Transf. 2009;52:15251533.
Rahman M, Oztop HF, Saidur R, Mekhilef S, Al-Salem K. Finite element solution of mhd mixed convection in a channel with a fully or partially heated cavity. Comput Fluids. 2013;79:53–64.
Selimefendigil F, Oztop HF. Numerical study and pod-based prediction of natural convection in ferrofluids filled triangular cavity with generalized neural networks (GRNN). Numer Heat Transf Part A. 2015;67:1136–61.
Nkurikiyimfura I, Wang Y, Pan Z. Heat transfer enhancement by magnetic nanofluids—a review. Renew Sustain Energy Rev. 2013;21:548–61.
Hasanuzzaman M, Oztop HF, Rahman M, Rahim N, Saidur R, Varol Y. Magnetohydrodynamic natural convection in trapezoidal cavities. Int Commun Heat Mass Transf. 2012;39:1384–94.
Hossain MS, Alim MA. Mhd free convection within trapezoidal cavity with non-uniformly heated bottom wall. Int J Heat Mass Transf. 2014;69:327–36.
Sheikholeslami M, Gorji-Bandpy M, Ganji D, Soleimani S, Seyyedi S. Natural convection of nanofluids in an enclosure between a circular and a sinusoidal cylinder in the presence of magnetic field. Int Commun Heat Mass Transf. 2012;39:1435–43.
Yu P, Qiu J, Qin Q, Tian ZF. Numerical investigation of natural convection in a rectangular cavity under different directions of uniform magnetic field. Int J Heat Mass Transf. 2013;67:1131–44.
Sheikholeslami M, Ganji DD. Ferrohydrodynamic and magnetohydrodynamic effects on ferrofluid flow and convective heat transfer. Energy. 2014;75:400–10.
Rahman M, Alim M, Sarker M. Numerical study on the conjugate effect of joule heating and magnato-hydrodynamics mixed convection in an obstructed lid-driven square cavity. Int Commun Heat Mass Transf. 2010;37(37):524–34.
Al-Salem K, Oztop HF, Pop I, Varol Y. Effects of moving lid direction on mhd mixed convection in a linearly heated cavity. Int J Heat Mass Transf. 2012;55:1103–12.
Oztop HF, Al-Salem K, Pop I. Mhd mixed convection in a lid-driven cavity with corner heater. Int J Heat Mass Transf. 2011;54:494–3504.
Rashad A, Armaghani T, Chamkha A, Mansour M. Entropy generation and mhd natural convection of a nanofluid in an inclined square porous cavity: effects of a heat sink and source size and location. Chin J Phys. 2018;56:193–211.
Mahmoudi AH, Pop I, Shahi M. Effect of magnetic field on natural convection in a triangular enclosure filled with nanofluid. Int J Therm Sci. 2012;59:12–140.
Ghasemi B, Aminossadati S, Raisi A. Magnetic field effect on natural convection in a nanofluid-filled square enclosure. Int J Therm Sci. 2011;50:1748–56.
Sheikholeslami M, Bandpy MG, Ganji D. Numerical investigation of mhd effects on Al2O3–water nanofluid flow and heat transfer in a semi-annulus enclosure using lbm. Energy. 2013;60:501–10.
Chamkha AJ, Rashad AM, Mansour MA, Armaghani T, Ghalambaz M. Effects of heat sink and source and entropy generation on mhd mixed convection of a Cu–water nanofluid in a lid-driven square porous enclosure with partial slip. Phys Fluids. 2017;29:052001.
Sarkar S, Ganguly S, Biswas G. Buoyancy driven convection of nanofluids in an infinitely long channel under the effect of a magnetic field. Int J Heat Mass Transf. 2014;71:328–40.
Hatami M, Sheikholeslami M, Hosseini M, Ganji DD. Analytical investigation of mhd nanofluid flow in non-parallel walls. J Mol Liq. 2014;194:251–9.
Sheikholeslami M, Bandpy MG, Ellahi R, Zeeshan A. Simulation of MHD Cuo–water nanofluid flow and convective heat transfer considering Lorentz forces. J Magn Magn Mater. 2014;369:69–80.
Kefayati G. Effect of a magnetic field on natural convection in an open cavity subjugated to water/alumina nanofluid using lattice Boltzmann method. Int Commun Heat Mass Transf. 2013;40:67–77.
Selimefendigil F, Oztop HF. Numerical study of MHD mixed convection in a nanofluid filled lid driven square enclosure with a rotating cylinder. Int J Heat Mass Transf. 2014;78:741–54.
Chamkha A. Hydromagnetic combined convection flow in a vertical lid-driven cavity enclosure with internal heat generation or absorption. Numer Heat Transf Part A. 2002;41:529–46.
Chamkha AJ, Rashad AM, Armaghani T, Mansour MA. Effects of partial slip on entropy generation and MHD combined convection in a lid-driven porous enclosure saturated with a Cu–water nanofluid. J Therm Anal Calorim. 2017 (in press). https://doi.org/10.1007/s10973-017-6918-8.
Oztop HF, Abu-Nada E. Numerical study of natural convection in partially heated rectangular enclosures filled with nanofluids. Int J Heat Fluid Flow. 2008;29:1326–36.
Armaghani T, Kasaeipoor A, Alavi N, Rashidi M. Numerical investigation of water–alumina nanofluid natural convection heat transfer and entropy generation in a baffled l-shaped cavity. J Mol Liq. 2016;223:243–51.
Meibodi SS, Kianifar A, Mahian O, Wongwises S. Second law analysis of a nanofluid-based solar collector using experimental data. J Therm Anal Calorim. 2016;126:617–25.
Rashidi S, Mahian O, Languri EM. Applications of nanofluids in condensing and evaporating systems. J Therm Anal Calorim. 2017;1–13 (in press). https://doi.org/10.1007/s10973-017-6773-7.
Chamkha A, Abu-Nada E. Mixed convection flow in single- and double-lid driven square cavities filled with water–Al2O3 nanofluid: effect of viscosity models. Eur J Mech B Fluids. 2012;36:82–96.
Abu-Nada E, Chamkha A. Mixed convection flow in a lid-driven inclined square enclosure filled with a nanofluid. Eur J Mech B Fluids. 2010;29:472–82.
Bahiraei M. A numerical study of heat transfer characteristics of CuO–water nanofluid by Euler–Lagrange approach. J Therm Anal Calorim. 2016;123:1591–9.
Armaghani T, Chamkha AJ, Maghrebi M, Nazari M. Numerical analysis of a nanofluid forced convection in a porous channel: a new heat flux model in ltne condition. J Porous Media. 2014;17:637–46.
Ismael MA, Armaghani T, Chamkha AJ. Conjugate heat transfer and entropy generation in a cavity filled with a nanofluid-saturated porous media and heated by a triangular solid. J Taiwan Inst Chem Eng. 2016;59:138–51.
Ben-Nakhi A, Chamkha A. Effect of length and inclination of a thin fin on natural convection in a square enclosure. Numer Heat Transf Part A. 2006;50:381–99.
Ben-Nakhi A, Chamkha A. Conjugate natural convection in a square enclosure with inclined thin fin of arbitrary length. Int J Therm Sci. 2007;46:467–78.
Varol Y, Oztop HF, Varol A. Effects of thin fin on natural convection in porous triangular enclosures. Int J Therm Sci. 2007;46:1033–45.
Sun C, Yu B, Oztop HF, Wang Y, Wei J. Control of mixed convection in lid-driven enclosures using conductive triangular fins. Int J Heat Mass Transf. 2011;54:894–909.
Selimefendigil F, Oztop HF. Fuzzy-based estimation of mixed convection heat transfer in a square cavity in the presence of an adiabatic inclined fin. Int Commun Heat Mass Transf. 2012;39:1639–46.
Khanafer K. Comparison of flow and heat transfer characteristics in a lid-driven cavity between flexible and modified geometry of a heated bottom wall. Int J Heat Mass Transf. 2014;78:1032–41.
Selimefendigil F, Oztop HF. Mixed convection in a two-sided elastic walled and SiO2 nanofluid filled cavity with internal heat generation: effects of inner rotating cylinder and nanoparticle’s shape. J Mol Liq. 2016;212:509–16.
Selimefendigil F, Oztop HF, Chamkha AJ. Analysis of mixed convection of nanofluid in a 3D lid-driven trapezoidal cavity with flexible side surfaces and inner cylinder. Int Commun Heat Mass Transf. 2017;87:40–51.
Al-Amiri A, Khanafer K. Fluid-structure interaction analysis of mixed convection heat transfer in a lid-driven cavity with a flexible bottom wall. Int J Heat Mass Transf. 2011;54:3826–36.
Selimefendigil F, Oztop HF. Mixed convection in a partially heated triangular cavity filled with nanofluid having a partially flexible wall and internal heat generation. J Taiwan Inst Chem Eng. 2017;70:168–78.
Chon CH, Kihm KD, Lee SP, Choi SU. Empirical correlation finding the role of temperature and particle size for nanofluid (Al2O3) thermal conductivity enhancement. Appl Phys Lett. 2005;87:153107.
Minsta HA, Roy G, Nguyen C, Doucet D. New temperature and conductivity data for water-based nanofluids. Int J Therm Sci. 2009;48:363–71.
Brinkman H. The viscosity of concentrated suspensions and solutions. J Chem Phys. 1952;20:571–81.
Bourantas G, Skouras E, Loukopoulos V, Burganos V. Heat transfer and natural convection of nanofluids in porous media. Eur J Mech B Fluids. 2014;43:45–56.
Selimefendigil F, Oztop HF. Modeling and optimization of mhd mixed convection in a lid-driven trapezoidal cavity filled with alumina-water nanofluid: Effects of electrical conductivity models. Int J Mech Sci. 2018;136:264–78.
Maxwell J. A treatise on electricity and magnetism. Oxford: Oxford University Press; 1873.
Pirmohammadi M, Ghassemi M. Effect of magnetic field on convection heat transfer inside a tilted square enclosure. Int Commun Heat Mass Transf. 2009;36:776–80.
Sarris I, Zikos G, Grecos A, Vlachos N. On the limits of validity of the low magnetic reynolds number approximation in MHD natural-convection heat transfer. Numer Heat Transf Part B. 2006;50:158–80.
Iwatsu R, Hyun J, Kuwahara K. Mixed convection in a driven cavity with a stable vertical temperature gradient. Int J Heat Mass Transf. 1993;36:1601–8.
Sheikholeslami M, Gorji-Bandpy M, Ganji D, Soleimani S. Natural convection heat transfer in a cavity with sinusoidal wall filled with cuo-water nanofluid in presence of magnetic field. J Taiwan Inst Chem Eng. 2014;45:40–9.
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
About this article
Cite this article
Selimefendigil, F., Oztop, H.F. & Chamkha, A.J. MHD mixed convection in a nanofluid filled vertical lid-driven cavity having a flexible fin attached to its upper wall. J Therm Anal Calorim 135, 325–340 (2019). https://doi.org/10.1007/s10973-018-7036-y
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s10973-018-7036-y