Study of Natural Convection in a Triangular Cavity Filled with Water: Application of the Lattice Boltzmann Method
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Study of Natural Convection in a Triangular Cavity Filled with Water: Application of the Lattice Boltzmann Method

Authors: Imen Mejri, Ahmed Mahmoudi, Mohamed A. Abbassi, Ahmed Omri

Abstract:

The Lattice Boltzmann Method (LBM) with double populations is applied to solve the steady-state laminar natural convective heat transfer in a triangular cavity filled with water. The bottom wall is heated, the vertical wall is cooled, and the inclined wall is kept adiabatic. The buoyancy effect was modeled by applying the Boussinesq approximation to the momentum equation. The fluid velocity is determined by D2Q9 LBM and the energy equation is discritized by D2Q4 LBM to compute the temperature field. Comparisons with previously published work are performed and found to be in excellent agreement. Numerical results are obtained for a wide range of parameters: the Rayleigh number from  to  and the inclination angle from 0° to 360°. Flow and thermal fields were exhibited by means of streamlines and isotherms. It is observed that inclination angle can be used as a relevant parameter to control heat transfer in right-angled triangular enclosures.

 

Keywords: Heat transfer, inclination angle, Lattice Boltzmann Method, Nusselt number, Natural convection, Rayleigh number.

Digital Object Identifier (DOI): doi.org/10.5281/zenodo.1090852

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References:


[1] S. Chen and G.D. "Doolen, Lattice Boltzmann method for fluid flows”, Annual Review of Fluid Mechanics, vol. 30, pp.329–64, 1998.
[2] S. V. Patankar, Numerical Heat Transfer and Fluid Flow, Hemisphere, Washington, D.C., 1980
[3] H. N. Dixit, V. Bab, "Simulation of high Rayleigh number natural convection in a square cavity using the lattice Boltzmann method”. Int.J. Heat Mass Transfer, vol. 49, pp.727-39, 2006.
[4] F. J. Higuera, S. Succi, R. Benzi, "Lattice gas dynamics with enhanced collisions”, Europhys. Lett. Vol. 9, pp. 345–349, 1989.
[5] R. Benzi, S. Succi, M. Vergassola, "The lattice Boltzmann equation: theory and applications”, Phys. Rep. vol. 222, pp.145–197, 1992.
[6] S. Succi, The Lattice Boltzmann Equation for Fluid Dynamics and Beyond. Oxford University Press, 2001.
[7] G. McNamara and B. Alder. "Analysis of the lattice Boltzmann treatment of hydrodynamic”, Physica A: Statistical Mechanics and its Applications. Vol. 194, pp. 218–28, 1993.
[8] S. Ostrach, "Natural convection in enclosures”, J. Heat Transfer. vol.110, pp. 1175–1190, 1988.
[9] I. Catton, "Natural convection in enclosures”, Proc. 6th Int. Heat Transfer Conf. vol.6, pp. 13–31, 1978.
[10] B. Gebhart, Y. Jaluria, R.P. Mahajan, B. Sammakia, Buoyancy-induced Flows and Transport. Hemisphere, Washington, 1988.
[11] G. De Vahl Davis, "Natural convection of air in a square cavity: a bench mark numerical solution”, Int. J. Numer. Methods in Fluids, vol. 3, pp. 249–264, 1983.
[12] H. Asan, L. Namli, "Numerical simulation of buoyant flow in a roof of triangular cross section under winter day boundary conditions”, Energy Buildings, vol. 33, pp. 753-757, 2001.
[13] M.M. Rahman, M.M. Billah, A.T.M.M. Rahman, M.A. Kalam, A. Ahsan, "Numerical investigation of heat transfer enhancement of nanofluids in an inclined lid-driven triangular enclosure”, Int. Commun. Heat Mass Transfer. vol. 38, pp. 1360–1367. 2011.
[14] A. Koca, H. F. Oztop, Y. Varol, "The effects of Prandtl number on natural convection in triangular enclosures with localized heating from below”, Int. Commun. Heat Mass Transfer. vol. 34, pp. 511–519, 2007.
[15] A. Omri, "Numerical investigation on optimization of a solar distiller dimensions”, Desalination, vol.206, pp. 373–379, 2007.
[16] A. H. Mahmoudi, I. Pop, M. Shahi,”Effect of magnetic field on natural convection in a triangular enclosure filled with nanofluid”, Int. J. Thermal Sciences, vol. 59, pp. 126-140, 2012.
[17] B. Ghasemi, S.M. Aminossadati, "Mixed convection in a lid-driven triangular enclosure filled with nanofluids”, Int. Commun. Heat Mass Transfer, vol. 37, pp. 1142-1148, 2010.
[18] Y. Varol, "Natural convection in porous triangular enclosure with a centered conducting body”, Int. Commun. Heat Mass Transfer, vol. 38, pp. 368-376, 2011.
[19] Y. C. Ching , H. F. Oztop, M. M. Rahman, M. R. Islam, A. Ahsan, "Finite element simulation of mixed convection heat and mass transfer in a right triangular enclosure”, Int. Commun. Heat Mass Transfer, vol.39, pp. 689-696, 2012.
[20] T. Basak, R. Anandalakshmi, P. Gunda, "Role of entropy generation during convective thermal processing in right-angled triangular enclosures with various wall heatings”, Chemical Engineering Research and Design, vol. 90, pp.1779-1799, 2012.
[21] H. F. Oztop , Y. Varol , A. Koca, M. Firat , "Experimental and numerical analysis of buoyancy-induced flow in inclined triangular enclosures”. Int. Commun. Heat Mass Transfer, vol. 39, pp.1237–1244, 2012.
[22] Y. Gurkan, A. Orhan, "Laminar natural convection in right-angled triangular enclosures heated and cooled on adjacent walls”, Int. J. Heat Mass Transfer, vol. 60, pp. 365–374, 2013.
[23] S. C. Tzeng, J. H. Liou, R. Y . Jou, "Numerical simulation-aided parametric analysis of natural convection in a roof of triangular enclosures”, Heat Transfer Engineering, vol. 26, pp. 69-79, 2005.
[24] V. Akinsete, T. A. Coleman, "Heat transfer by steady laminar free convection in triangular enclosures”, Int. J. Heat Mass Transfer,vol. 25, pp. 991-998, 1982.