8 results on '"Farhadi M"'
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2. Free Convection in a MHD Porous Cavity with using Lattice Boltzmann Method
- Author
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Hamid Reza Ashorynejad, Farhadi, M., Sedighi, K., and Hasanpour, A.
- Subjects
Physics::Fluid Dynamics ,Natural convection ,Lattice Boltzmann method ,Porous medium ,Magnetohydrodynamic - Abstract
We report the results of an lattice Boltzmann simulation of magnetohydrodynamic damping of sidewall convection in a rectangular enclosure filled with a porous medium. In particular we investigate the suppression of convection when a steady magnetic field is applied in the vertical direction. The left and right vertical walls of the cavity are kept at constant but different temperatures while both the top and bottom horizontal walls are insulated. The effects of the controlling parameters involved in the heat transfer and hydrodynamic characteristics are studied in detail. The heat and mass transfer mechanisms and the flow characteristics inside the enclosure depended strongly on the strength of the magnetic field and Darcy number. The average Nusselt number decreases with rising values of the Hartmann number while this increases with increasing values of the Darcy number., {"references":["G.M. Oreper and J.Szekely, \"The effect of an externally imposed\nmagnetic field on buoyancy driven flow in a rectangular cavity\". J.\nCrystal Growth, vol. 64, 1983, pp. 505-515.","K. Vajravelu and A. Hadjinicolaou,\" Nonlinear hydromagnetic\nconvection at a continuous moving surface,\" Nonlinear Analysis,\nTheory, Methods and Applications vol. 31, 1998 , pp. 867-882.","M.A. Al-Nimr and M.A. Hader, \"MHD free convection flow in openended\nvertical porous channels,\" Chemical Eng. Sci. vol. 54, 1999, pp.\n1883-1889.","A.J. Chamkha, \"Hydromagnetic combined convection flow in a vertical\nlid-driven avity with internal heat generation of absorption,\" Numer.\nHeat Transfer Part A vol. 41, 2002, pp. 529-546.","M.N. Borjini, H.B. Aissia, K. Halouani, and B. Zeghmati, \"Effect of\noptical properties on oscillatory hydromagnetic double-diffusive\nconvection within semitransparent fluid,\" Int. J. Heat Mass Transfer vol.\n49,2006, pp. 3984-3996.","S. Alchaar, P. Vasseur and E. Bilgen, \"Natural convection heat transfer\nin a rectangular enclosure with a transverse magnetic field,\" J. Heat\nTransfer, vol. 117, 1995, pp. 668-673.","D.A. Nield, \"Impracticality of MHD convection in a porous medium,\"\nTransport Porous Med. vol. 73, 2008, pp-379.","A. Barletta, S. Lazzari, E. Magayri and I. Pop,\" Mixed convection with\nheating effectin a vertical porous annulus with a radially varying\nmagnetic field,\" Int. J. Heat Mass Transfer vol. 51 (25-26) ,2008, pp.\n5777-5784.","N. Rudraiah, R.M. Barron, M. Venkatachalappa, and C.K. Subbaraya,\n\"Effect of a magnetic field on free convection in a rectangular\nenclosure,\" Int. J. Engng. Sci. vol. 33, 1995, pp. 1075-1084.\n[10] L. Robillard, A. Bahloul, and P. Vasseur, \"Hydromagnetic natural\nconvection of a binary fluid in a vertical porous enclosure,\" Chem. Eng.\nComm. vol. 193, 2006, pp. 1431-1444.\n[11] B.J. Pangrle, E.G. Walsh, S.C. Moore, and D. Dibiasio-o, \"Magnetic\nresonance imaging of laminar in porous tube and shell systems flow,\"\nChemical Eng. Sci. vol. 47 ,1992, pp. 517-526.\n[12] J.D. McWhirter, M.E. Crawford, and D.E. Klein, \"Magneto\nhydrodynamic flows porous media ii: Experimental results,\" Fusion\nScience and Tech. vol. 34,1998, pp. 187-197.\n[13] P. Kuzhir, G. Bossis, V. Bashtovoi, and O.Volkova, \"Flow of\nmagnetorheological fluidthrough porous media,\" European Journal of\nMechanics B/Fluids. vol. 22, 2003, pp. 331-343.\n[14] K.M. Khanafer and A.J. Chamkha, \"Hydromagnetic natural convection\nfrom an inclined porous square enclosure with heat generation,\" Numer.\nHeat Transfer Part A. vol. 33, 1998, pp. 891-910.\n[15] G. R. McNamara, and G. Zanetii, , \"Use of the Boltzmann Equation to\nSimulate Lattice-Gas Automata,\" Phys. Rev. Lett., vol.61, 1988,\npp.2332-2335.\n[16] J. Onishi, Y. Chen, and H. Ohashi, \"Lattice Boltzmann simulation of\nnatural convection in a square cavity,\" JSME Int. J. Ser. B, vol. 44,\n2001, pp.53-62.\n[17] D. Zhang , R. Zhang, S. Chen, and W. Soll, \"Pore scale study of flow in\nporous media: Scale dependency,\" REV, and statistical REV,\nGeophysical Research Letters, vol. 27, 2000, pp.1195-1198.\n[18] D.A. Nield, and A. Bejan, Convection in Porous Media, 3rd ed,\nSpringer, New York, 2006.\n[19] O.Dardis, and J. McCloskey, \"Lattice Boltzmann scheme with real\nnumbered solid density for the simulation of flow in porous media,\"\nPhys. Rev. E, vol. 57, 1998, pp.4834-4837.\n[20] M.A.A. Spaid, and F.R. Phelan, \"Lattice Boltzmann methods for\nmodeling micro scale flow in fibrous porous media,\" Phys. Fluids, vol.\n9, 1997, pp. 2468-2474.\n[21] S. J. Kim, and K.Vafai, \"Analysis of natural convection about a vertical\nplate embedded in a porous medium,\" Int. J. Heat Mass Transfer, vol.\n32, 1989, pp. 665-677.\n[22] Z. Guo, and T.S. Zhao, \"Lattice Boltzmann model for incompressible\nflows through porous media,\" Phys. Rev. E, vol. 66, 2002,pp.036304-1-\n036304-9.\n[23] D. Montgomery and G. D. Doolen, \"Magneto hydrodynamic cellular\nautomata,\" Phys. Lett. A, vol. 120, 1987 , pp.229.\n[24] H.Chen And W.H. Matthaeus, \"An analytical theory and formulation of\na local magnetohydrodynamic lattice gas model,\" Phys. Fluids, vol. 31,\n1988, pp. 1439-1455.\n[25] D. Martinez, S. Chen and W.H. Matthaeus, \"Lattice Boltzmann magneto\nhydrodynamics,\" Phys. Plasmas, vol. 6, 1994.\n[26] A. MacNab, G. Vahala, L. P. Vahala Pavlo and M. Soe, Lattice\nBoltzmann model for dissipative incompressible MHD, 28rd, EPS\nconference on controlled fusion and plasma physics, Madeira, Portugal,\n2001.\n[27] C. Xing-Wang and S. Bao- Chang, \"A new lattice Boltzmann model for\nincompressible magneto hydrodynamics incompressible,\" Chinese\nPhysics, vol. 14 No. 7, 2005.\n[28] P.J.Dellar, \"Lattice kinetic schemes for magnetohydrodynamics,\" J.\nComp. Phys, vol. 179, 2002,pp. 95-126.\n[29] X. He, S. Chen and G.D. Doolen, \"A novel thermal model for the\nlattice Boltzmann method in incompressible limit,\" J. Comp. Phys, vol.\n146, 1998, pp. 282-300.\n[30] X. He and L.S. Luo, \"A priori derivation of the lattice Boltzmann\nequation,\" Phys. Rev. E, 2000.\n[31] K.R. Cramer and S.I. Pai, \"Magnatofluid Dynamics for Engineers and\nPhysicists,\" McGraw-Hill, New York, 1973.\n[32] T. Seta, E. Takegoshi, K. Kitano and K. Okui, \"Thermal Lattice\nBoltzmann Model for Incompressible Flows through Porous Media,\"\nJ.Thermal Science and Technology, vol. 1, No.2, 2006, pp.90.\n[33] S. Ergun, \"Flow through Packed Columns,\" Chemical Engineering\nProgress, vol. 48 , 1952 ,pp.89-94.\n[33] Z.Guo, C. Zheng, and B. Shi, \"Discrete lattice effects on the forcing\nterm in the lattice Boltzmann method,\" Phys Rev E, vol. 65, 2002,\npp.046308-1-046308-6.\n[34] A.A. Mohammad, \"Applied lattice Boltzmann method for transport\nphenomena, momentum, heat and mass transfer,\" Canadian J. Chemical\nEngineering, 2007.\n[35] P. Nithiarasu, K.N. Seetharamuand, T. Sundararajan, \"Natural\nconvective heat transfer in a fluid saturated variable porosity medium,\"\nInt. J. Heat Mass Transfer, vol. 40,1997, pp. 3955-3967"]}
- Published
- 2011
- Full Text
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3. Natural convection flow of Cu–Water nanofluid in horizontal cylindrical annuli with inner triangular cylinder using lattice Boltzmann method.
- Author
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Mehrizi, A. Abouei, Farhadi, M., and Shayamehr, S.
- Subjects
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NATURAL heat convection , *NANOFLUIDS , *FLUID dynamics , *COPPER , *BOLTZMANN'S equation , *PHYSIOLOGICAL effects of nanoparticles , *SURFACE temperature - Abstract
Abstract: In this paper the lattice Boltzmann method is used to investigate the effect of nanoparticles on natural convection heat transfer in two-dimensional horizontal annulus. The study consists of an annular-shape enclosure, which is created between a heated triangular inner cylinder and a circular outer cylinder. The inner and outer surface temperatures were set as hot (Th) and cold temperatures (Tc), respectively and assumed to be isotherms. The effect of nanoparticle volume fraction to the enhancement of heat transfer was examined at different Rayleigh numbers. Furthermore, the effect of vertical, horizontal, and diagonal eccentricities at various locations is examined at Ra=104. The result is presented in the form of streamlines, isotherms, and local and average Nusselt number. Results show that the Nusselt number and the maximum stream functions increase by augmentation of solid volume fraction. Average Nusselt number increases when the inner cylinder moves downward, but it decreases, when the location of inner cylinder changes horizontally. [Copyright &y& Elsevier]
- Published
- 2013
- Full Text
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4. Numerical study of Prandtl effect on MHD flow at a lid-driven porous cavity.
- Author
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Hasanpour, A., Farhadi, M., Sedighi, K., and Ashorynejad, H.R.
- Abstract
SUMMARY In this paper, the lattice Boltzmann method is used to study the Prandtl number effect on flow structure and heat transfer rates in a magnetohydrodynamic flow mixed convection in a lid-driven cavity filled with a porous medium. The right and left walls are at constant but different temperatures ( θ
h and θc ), while the other walls are adiabatic. Gallium and salt water (0.02 < Pr < 13.4) are used as samples of the electroconducting fluids in the cavity. Typical sets of streamlines and isotherms are presented to analyze the flow patterns set up by the competition among the forced flow created by the lid-driven wall, the buoyancy force of the fluid and the magnetic force of the applied magnetic field. Mathematical formulations in the porous media were constructed based on the Brinkman-Forchheimer model, while the multidistribution-function model was used for the magnetic field effect. Numerical results were obtained and the effects of the Prandtl number and the other effective parameters such as Richardson, Hartman, and Darcy numbers were investigated. It was found that the fluid fluctuations within the cavity were reduced by increasing the Hartman number. A similar pattern was observed for the Darcy number reduction. Heat transfer was essentially dominated by the conduction for the low Prandtl number and forced convection dominated as the Prandtl number increased. Also, the average Nusselt number was raised by increasing the Prandtl number. It was discovered that a remarkable heat transfer enhancement of up to 28% could be reached by increasing the Prandtl number (from 0.02 to 13.4) at constant Richardson and Darcy numbers. Copyright © 2011 John Wiley & Sons, Ltd. [ABSTRACT FROM AUTHOR]- Published
- 2012
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5. Simulation of natural convection melting in an inclined cavity using lattice Boltzmann method.
- Author
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Jourabian, M., Farhadi, M., and Darzi, A.A. Rabienataj
- Subjects
LATTICE Boltzmann methods ,NATURAL heat convection ,SIMULATION methods & models ,ENTHALPY ,CAVITATION ,RAYLEIGH number - Abstract
Abstract: In this study, a numerical analysis of the melting process with natural convection in an inclined cavity has been performed using the enthalpy-based lattice Boltzmann method. The D2Q9 and D2Q5 models were applied to determine the density and velocity fields, and the temperature field, respectively. The study was carried out for Stefan number of 10, Rayleigh number ranging from to , and inclination angle ranging from to . The predicted results indicate that an increase in Rayleigh number leads to intensifying the melting rate at each inclination angle. In addition, when the cavity is inclined counterclockwise, the effect of natural convection becomes more dominant, while, if it is inclined clockwise, the conduction regime endures longer. [Copyright &y& Elsevier]
- Published
- 2012
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6. Magnetic field effects on natural convection flow of nanofluid in a rectangular cavity using the Lattice Boltzmann model.
- Author
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Nemati, H., Farhadi, M., Sedighi, K., Ashorynejad, H.R., and Fattahi, E.
- Subjects
MAGNETIC fields ,NANOFLUIDS ,LATTICE Boltzmann methods ,MAGNETOHYDRODYNAMICS ,RAYLEIGH number ,NANOPARTICLES - Abstract
Abstract: This work applied the Lattice Boltzmann Method (LBM) to investigate the effect of CuO nanoparticles on natural convection with magnetohydrodynamic (MHD) flow in a square cavity. The left and right vertical walls of the cavity were kept at constant temperatures, and , respectively, with two insulated walls at the top and bottom. A uniform magnetic field was used in a horizontal direction. Results were carried out for different Hartmann numbers ranging from 0–100, Rayleigh numbers from 10
3 –105 and the solid volume fraction from 0 to 0.05. Effects of the solid volume fraction and magnetic field on hydrodynamic and thermal characteristics were investigated and discussed. The averaged Nusselt numbers, on hot wall, streamlines, temperature contours, and the vertical component of velocity for different values of a solid volume fraction, Hartmann and Rayleigh numbers were illustrated. The results indicate that the averaged Nusselt number increases for nanofluids when increasing the solid volume fraction, while, in the presence of a high magnetic field, this effect decreases. [Copyright &y& Elsevier]- Published
- 2012
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7. Lattice Boltzmann simulation of mixed convection heat transfer in eccentric annulus
- Author
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Fattahi, E., Farhadi, M., and Sedighi, K.
- Subjects
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LATTICE Boltzmann methods , *SIMULATION methods & models , *HEAT convection , *HEAT transfer , *TEMPERATURE effect , *NUSSELT number , *COMPARATIVE studies - Abstract
Abstract: Mixed convection heat transfer in eccentric annulus was simulated numerically by lattice Boltzmann model (LBM) based on multi-distribution function double-population approach. The effect of eccentricity on heat transfer at various locations was examined at Ra =104 and σ =2. Velocity and temperature distributions as well as Nusselt number are obtained. The results are validated with published results and shown that multi-distribution function approach can evaluate the velocity and temperature fields in curved moving boundaries with a good accuracy in comparison with the previous studies. The results show that the average Nusselt number increases when the inner cylinder moves downward regardless of the radial position. [Copyright &y& Elsevier]
- Published
- 2011
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8. Lattice Boltzmann simulation of nanofluid in lid-driven cavity
- Author
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Nemati, H., Farhadi, M., Sedighi, K., Fattahi, E., and Darzi, A.A.R.
- Subjects
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LATTICE Boltzmann methods , *NANOFLUIDS , *REYNOLDS number , *HYDRODYNAMICS , *THERMAL conductivity , *VISCOSITY , *SIMULATION methods & models - Abstract
Abstract: Lattice Boltzmann Method is applied to investigate the mixed convection flows utilizing nanofluids in a lid-driven cavity. The fluid in the cavity is a water-based nanofluid containing Cu, Cuo or Al2O3 nanoparticles. The effects of Reynolds number and solid volume fraction for different nanofluids on hydrodynamic and thermal characteristics are investigated. The effective thermal conductivity and viscosity of nanofluid are calculated by Chon and Brinkman models, respectively. The results indicate that the effects of solid volume fraction grow stronger sequentially for Al2O3, Cuo and Cu. In addition the increases of Reynolds number leads to decrease the solid concentration effect. [ABSTRACT FROM AUTHOR]
- Published
- 2010
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