Analytical and Numerical Study of Combined Effects of a Magnetic Field and an External Shear Stress on Soret Convection in a Horizontal Porous Enclosure (original) (raw)

Natural Convection of Liquid Metals in an Inclined Enclosure in the Presence of a Magnetic Field

The problem of steady, laminar, natural convective flow of electrically-conducting liquid metals such as gallium and germanium in an inclined rectangular enclosure in the presence of a uniform magnetic field is considered. Transverse gradient of heat is applied on two opposing walls of the inclined enclosure while the other two walls are adiabatic. A magnetic field is applied normal to the non-insulated walls. The problem is formulated in terms of the vorticity – stream function procedure. A numerical solution based on the finite-difference method is obtained. Representative results illustrating the effects of the enclosure inclination angle and the Hartmann number for two different Rayleigh numbers on the contour maps of the streamlines and temperature as well as the profiles of velocity components and temperature at mid-section of the enclosure are reported. In addition, results for the average Nusselt number are presented and discussed for various parametric conditions.

Magnetic Convection Heat Transfer in an Open Ended Enclosure Filled with Paramagnetic Fluids

Accepted for the publication in Applied Mechanics and Materials

Numerical simulations of thermomagnetic convection of paramagnetic fluids placed in a micro-gravity condition (g ~ 0) and under a uniform vertical gradient magnetic field in an open ended square enclosure with ramp heating temperature condition applied on a vertical wall is investigated in this study. In presence of the strong magnetic gradient field thermal convection of the paramagnetic fluid might take place even in a zero-gravity environment as a direct consequence of temperature differences occurring within the fluid. The thermal boundary layer develops adjacent to the hot wall as soon as the ramp temperature condition is applied on it. There are two scenario that can be observed based on the ramp heating time. The steady state of the thermal boundary layer can be reached before the ramp time is finished or vice versa. If the ramp time is larger than the quasi-steady time then the thermal boundary layer is in a quasi-steady mode with convection balancing conduction after the quasi-steady time. Further increase of the heat input simply accelerates the flow to maintain the proper thermal balance. Finally, the boundary layer becomes completely steady state when the ramp time is finished. Effects of magnetic Rayleigh number, Prandtl number and paramagnetic fluid parameter on the flow pattern and heat transfer are presented.

Influence of a horizontal magnetic field on the natural convection of paramagnetic fluid in a cube heated and cooled from two vertical side walls

International Journal of Thermal Sciences, 2008

A cube was filled with an aqueous solution of glycerol with the addition of gadolinium nitrate hexahydrate to make the working fluid paramagnetic. A very small amount of liquid crystal slurry was then added in order to visualize the local temperature inside the enclosure. One vertical wall of the cube was uniformly heated by nichrome wire from a DC power supply while the opposite one was cooled by cold water flowing from a thermostatic circulator. The system was placed close to the solenoid of a superconducting magnet which was horizontally oriented. Two cases were considered in the experiment: the first with the cooled wall close to the solenoid and the second with the heated wall close to the magnet's electric multi-wires. Natural convection was investigated for both cases: first without a magnetic field and second with various strengths of magnetic force acting on the system. The experimental results showed clearly suppression and enhancement of natural convection. Corresponding numerical computations were carried out for comparison with the experimental data. For this purpose, isotherms of the experimental data were extracted from the color images using the Particle Image Thermometry method and were compared with the numerical results.

A numerical study of natural convection in a vertical annulus filled with gallium in the presence of magnetic field

ScienceDirect, 2017

Presets work aims to investigate the natural convection inside a cylindrical annulus mold containing molten gallium under a horizontal magnetic field in three-dimensional coordinates. The modeling system is a vertical cylindrical annulus which is made by two co-axial cylinders of internal and external radii. The internal and external walls are maintained isothermal but in different temperatures. The upper and lower sides of annulus are also considered adiabatic while it is filled by an electrical conducting fluid. Three dimensional cylindrical coordinates as r θ z (, ,) are used to respond the velocity components as u v w (, ,). The governing equations are steady, laminar and Newtonian using the Boussinesq approximation. Equations are nonlinear and they must be corresponded by applying the finite volume approach; so that the hybrid-scheme is applied to discretize equations. The results imply that magnetic field existence leads to generate the Lorentz force in opposite direction of the buoyancy forces. Moreover the Lorentz force and its corresponded electric field are more significant in both Hartmann layer and Roberts layer, respectively. The strong magnetic field is required to achieve better quality products in the casting process of a liquid metal with a higher Prandtl number.

Natural convection of liquid metal under a uniform magnetic field with an electric current supplied from outside

Experimental Thermal and Fluid Science, 2006

The effect of an electric current supplied from outside on the natural convection of liquid metal under a uniform magnetic field is studied both experimentally and numerically. A cubic enclosure filled with the liquid metal is heated and cooled from the facing electro-conductive vertical sidewalls while other four walls are thermally and electrically insulated. A horizontal magnetic field is applied parallel to the hot and cold walls. Two electrodes to apply an electric current to the liquid metal are inserted at the center of the hot and cold electro-conductive sidewalls, respectively. With applying the magnetic field only, the natural convection is damped out by the Lorentz force which is the interaction between the induced electric current and the external magnetic field. When both the magnetic field and the additional electric current are applied, the convection pattern and heat transfer rate from the hot wall to the cold wall become different compared to the case of the magnetic field only.

Natural Convection in an Enclosure: Effect of Magnetic Field Dependent Thermal Conductivity

In this paper, the natural convection heat transfer process is investigated inside an annular enclosure filled with a magnetic nanofluid (Fe 3 O 4 magnetic nanoparticles dispersed in Kerosene). A uniform magnetic field (H) is applied along the axial direction of the enclosure. Thermal conductivity (k) is considered as a function of magnetic field. A nonlinear relationship between magnetic field and thermal conductivity in the magnetic nanofluid (MNF) is assumed and interpolated. Finite element method is utilized to solve the governing equations and calculate the Nusselt number and it is presented as a function of volume fraction and magnetic field strength. The results show the significant effect of applied magnetic field on heat transfer rate, more specifically on Nu, in the enclosure when higher volume fractions of nanoparticles are used. Thermal conductivity enhancement as a result of using magnetic field can be used for various applications such as thermal energy storage in which the heat transfer needs to be accurately controlled.

Axisymmetric Natural Convection of Liquid Metal in an Annular Enclosure under the Influence of Azimuthal Magnetic Field

Energies, 2020

Natural convection of liquid metal in an annular enclosure under the influence of azimuthal static magnetic field was numerically studied. The liquid metal in the enclosure whose cross-sectional area is square was heated from an inner vertical wall and cooled from an outer vertical wall both isothermally whereas the other two horizontal walls were assumed to be adiabatic. The static azimuthal magnetic field was imposed by a long straight electric coil that was located at the central axis of the annular enclosure. The computations were carried out for the Prandtl number 0.025, the Rayleigh number 104, 5 × 105 and 107, and the Hartmann number 0–100,000 by using an in-house code. It was found that the contour map of the electric potential was similar to that of the Stokes stream function of the velocity regardless of the Hartmann number. Likewise, the contour map of the pressure was similar to the Stokes stream function of the electric current density in the case of the high Hartmann n...

Magnetic field effects on natural convection flow of a non-Newtonian fluid in an L-shaped enclosure

Journal of Thermal Analysis and Calorimetry, 2018

The effect of magnetic field on natural convection heat transfer in an L-shaped enclosure filled with a non-Newtonian fluid is investigated numerically. The governing equations are solved by finite-volume method using the SIMPLE algorithm. The power-law rheological model is used to characterize the non-Newtonian fluid behavior. It is revealed that heat transfer rate decreases for shear-thinning fluids (of power-law index, n \ 1) and increases for shear-thickening fluids (n [ 1) in comparison with the Newtonian ones. Thermal behavior of shear-thinning and shear-thickening fluids is similar to that of Newtonian fluids for the angle of enclosure a \ 60°and a [ 60°, respectively. Keywords Magnetohydrodynamics (MHD) Á Natural convection Á Newtonian fluid Á Non-Newtonian fluid Á Enclosure List of symbols AR Aspect ratio B o Magnetic induction (T) g Gravitational acceleration (m s-2) Ha Hartmann number K Thermal conductivity (W m-1 K-1) L Specific length (m) n Power-law index Nu Local Nusselt number P Pressure (Pa) Pr Prandtl number Ra Rayleigh number Re Reynolds number T Wall temperature (K) u Velocity in x-direction (m s-1) v Velocity in y-direction (m s-1) U Dimensionless velocity in x-direction V Dimensionless velocity in y-direction x Distance along x-coordinate y Distance along y-coordinate Greek letters b Thermal expansion coefficient (k-1) l Dynamic viscosity (kg m-1 s-1) q Density (kg m-3) h Dimensionless temperature