Effects of magnetic field on the liquid gallium thermosyphon fluid flow; a numerical study

Purpose This paper aims to numerically study the laminar natural convection in a thermosyphon filled with liquid gallium exposed to a constant magnetic field. The left wall of the thermosyphon is at an uniformed hot temperature, whereas the right wall is at a uniform cold temperature. The top and bottom walls are considered to be adiabatic. All walls are electrically insulated. The effects of Hartmann number, in a wide range of Rayleigh number and aspect ratio combinations, on the natural convection throughout the thermosyphon, are investigated and discussed. Furthermore, different forces that influence the natural flow structure are studied. Design/methodology/approach A Fortran code is developed based on the finite volume method to solve the two-dimensional unsteady governing equations. Findings Imposing a magnetic field improves the stability of the fluid flow and thus reduces the Nusselt number. For a given Hartmann and Rayleigh number, there is an optimum aspect ratio for which the average velocity becomes maximum. Research limitations/implications This paper is a two-dimensional investigation. Originality/value To the best of the authors’ knowledge, the effect of the magnetic field on natural convection of liquid gallium in the considered thermosyphon has not been studied numerically in detail. The results of this paper would be helpful in considering the application of the low Prandtl number’s liquid metals in thermosyphon MHD generators and certain cooling devices.

[1]  Ali J. Chamkha,et al.  MHD mixed convection of nanofluid due to an inner rotating cylinder in a 3D enclosure with a phase change material , 2019, International journal of numerical methods for heat & fluid flow.

[2]  Hamid Teimouri,et al.  Numerical investigation of a thermosyphon MHD electrical power generator , 2019, Energy Conversion and Management.

[3]  Ali J. Chamkha,et al.  MHD mixed convection of nanofluid in a cubic cavity with a conductive partition for various nanoparticle shapes , 2019, International Journal of Numerical Methods for Heat & Fluid Flow.

[4]  D. Toghraie,et al.  Effect of MHD on the flow and heat transfer characteristics of nanofluid in a grooved channel with internal heat generation , 2019, International Journal of Numerical Methods for Heat & Fluid Flow.

[5]  M. Arik,et al.  Numerical and experimental analysis of a heat-pipe-embedded printed circuit board for solid state lighting applications , 2019 .

[6]  K. Chau,et al.  Experimental and numerical analysis of a nanofluidic thermosyphon heat exchanger , 2018, Engineering Applications of Computational Fluid Mechanics.

[7]  I. Pop,et al.  MHD natural convection and entropy analysis of a nanofluid inside T-shaped baffled enclosure , 2018, International Journal of Numerical Methods for Heat & Fluid Flow.

[8]  Xiaowu Wang,et al.  Optimal Structure Design of a Thermosyphon Solar Water Heating System with Thermal and Dynamic Models , 2018 .

[9]  K. Matsubara,et al.  Loop thermosiphon thermal collector for waste heat recovery power generation , 2018, Experimental Heat Transfer.

[10]  Xiaohu Yang,et al.  Liquid metal enabled combinatorial heat transfer science: toward unconventional extreme cooling , 2018 .

[11]  O. Zikanov,et al.  Convection instability in a downward flow in a vertical duct with strong transverse magnetic field , 2018, Physics of Fluids.

[12]  I. Park,et al.  Numerical study of MHD natural convection in a rectangular enclosure with an insulated block , 2017 .

[13]  Ali J. Chamkha,et al.  MHD phase change heat transfer in an inclined enclosure: Effect of a magnetic field and cavity inclination , 2017 .

[14]  Yuwen Zhang,et al.  Double MRT thermal lattice Boltzmann method for simulating natural convection of low Prandtl number fluids , 2016, 1601.04633.

[15]  H. Yamaguchi,et al.  Characteristics of a MHD power generator using a low-melting-point Gallium alloy , 2014 .

[16]  In Cheol Bang,et al.  An experimental study on natural convection heat transfer of liquid gallium in a rectangular loop , 2013 .

[17]  B. Šarler,et al.  Solution of a low Prandtl number natural convection benchmark by a local meshless method , 2013 .

[18]  Ali J. Chamkha,et al.  Natural convection flow under magnetic field in a square cavity for uniformly (or) linearly heated adjacent walls , 2012 .

[19]  Jing Liu,et al.  Harvesting low grade heat to generate electricity with thermosyphon effect of room temperature liquid metal , 2011 .

[20]  A. Fattahi,et al.  Numerical study of steady magneto-convection around an adiabatic body inside a square enclosure in low Prandtl numbers , 2011 .

[21]  D. C. Lo,et al.  High-resolution simulations of magnetohydrodynamic free convection in an enclosure with a transverse magnetic field using a velocity–vorticity formulation ☆ , 2010 .

[22]  Majid Ghassemi,et al.  Effect of magnetic field on convection heat transfer inside a tilted square enclosure , 2009 .

[23]  M. Misale,et al.  Experiments in Single-Phase Natural Circulation Miniloops With Different Working Fluids and Geometries , 2008 .

[24]  Pallippattu Krishnan Vijayan,et al.  Effect of Loop Diameter on the Steady State and Stability Behaviour of Single-Phase and Two-Phase Natural Circulation Loops , 2008 .

[25]  Y. Okuno,et al.  Two‐dimensional numerical simulation on performance of liquid metal MHD generator , 2006 .

[26]  T. Mullin,et al.  Magnetohydrodynamic damping of oscillations in low-Prandtl-number convection , 2005, Journal of Fluid Mechanics.

[27]  Man Yeong Ha,et al.  A numerical study of natural convection in a horizontal enclosure with a conducting body , 2005 .

[28]  N. Ghaddar Numerical simulation of side‐heated free convection loop placed in transverse magnetic field; the induced electric current , 1998 .

[29]  H. Ozoe,et al.  OSCILLATORY PHENOMENA OF LOW-PRANDTL-NUMBER FLUIDS IN A RECTANGULAR CAVITY , 1996 .

[30]  P. J. Prescott,et al.  EFFECT OF TIME MARCHING SCHEMES ON PREDICTIONS OF OSCILLATORY NATURAL CONVECTION IN FLUIDS OF LOW PRANDTL NUMBER , 1996 .

[31]  Ronald M. Barron,et al.  Effect of a magnetic field on free convection in a rectangular enclosure , 1995 .

[32]  P. LeQuéré,et al.  Accurate solutions to the square thermally driven cavity at high Rayleigh number , 1991 .

[33]  Raymond Viskanta,et al.  Transient natural convection of low‐Prandtl‐number fluids in a differentially heated cavity , 1991 .

[34]  Adrian Bejan,et al.  The Ra-Pr domain of laminar natural convection in an enclosure heated from the side , 1991 .

[35]  R. Viskanta,et al.  AN EVALUATION OF DIFFERENT DISCRETIZATION SCHEMES FOR NATURAL CONVECTION OF LOW-PRANDTL-NUMBER FLUIDS IN CAVITIES , 1990 .

[36]  R. Greif Natural Circulation Loops , 1988 .

[37]  G. de Vahl Davis,et al.  Natural convection in a square cavity: A comparison exercise , 1983 .

[38]  H. F. Creveling,et al.  Stability characteristics of a single-phase free convection loop , 1975, Journal of Fluid Mechanics.