Computational Performance of Disparate Lattice Boltzmann Scenarios under Unsteady Thermal Convection Flow and Heat Transfer Simulation

The present work highlights the capacity of disparate lattice Boltzmann strategies in simulating natural convection and heat transfer phenomena during the unsteady period of the flow. Within the framework of Bhatnagar-Gross-Krook collision operator, diverse lattice Boltzmann schemes emerged from two different embodiments of discrete Boltzmann expression and three distinct forcing models. Subsequently, computational performance of disparate lattice Boltzmann strategies was tested upon two different thermo-hydrodynamics configurations, namely the natural convection in a differentially-heated cavity and the Rayleigh-Bènard convection. For the purposes of exhibition and validation, the steady-state conditions of both physical systems were compared with the established numerical results from the classical computational techniques. Excellent agreements were observed for both thermo-hydrodynamics cases. Numerical results of both physical systems demonstrate the existence of considerable discrepancy in the computational characteristics of different lattice Boltzmann strategies during the unsteady period of the simulation. The corresponding disparity diminished gradually as the simulation proceeded towards a steady-state condition, where the computational profiles became almost equivalent. Variation in the discrete lattice Boltzmann expressions was identified as the primary factor that engenders the prevailed heterogeneity in the computational behaviour. Meanwhile, the contribution of distinct forcing models to the emergence of such diversity was found to be inconsequential. The findings of the present study contribute to the ventures to alleviate contemporary issues regarding proper selection of lattice Boltzmann schemes in modelling fluid flow and heat transfer phenomena.

[1]  Pei Xiang Yu,et al.  Compact computations based on a stream-function-velocity formulation of two-dimensional steady laminar natural convection in a square cavity. , 2012, Physical review. E, Statistical, nonlinear, and soft matter physics.

[2]  Wenwen Liu,et al.  A New Multiple-relaxation-time Lattice Boltzmann Method for Natural Convection , 2013, J. Sci. Comput..

[3]  Steven A. Orszag,et al.  Numerical simulation of thermal convection in a two-dimensional finite box , 1989, Journal of Fluid Mechanics.

[4]  Xiaoyi He,et al.  Thermodynamic Foundations of Kinetic Theory and Lattice Boltzmann Models for Multiphase Flows , 2002 .

[5]  Ahmed Mezrhab,et al.  Double MRT thermal lattice Boltzmann method for simulating convective flows , 2010 .

[6]  L. Luo,et al.  Theory of the lattice Boltzmann method: From the Boltzmann equation to the lattice Boltzmann equation , 1997 .

[7]  Ahmed Mezrhab,et al.  New thermal MRT lattice Boltzmann method for simulations of convective flows , 2016 .

[8]  V. Babu,et al.  Simulation of high Rayleigh number natural convection in a square cavity using the lattice Boltzmann method , 2006 .

[9]  Luo Li-Shi,et al.  Theory of the lattice Boltzmann method: Lattice Boltzmann models for non-ideal gases , 2001 .

[10]  Taieb Lili,et al.  NUMERICAL SIMULATION OF TWO-DIMENSIONAL RAYLEIGH–BÉNARD CONVECTION IN AN ENCLOSURE , 2008 .

[11]  Martin Crapper,et al.  h‐adaptive finite element solution of high Rayleigh number thermally driven cavity problem , 2000 .

[12]  Abdulmajeed A. Mohamad,et al.  A critical evaluation of force term in lattice Boltzmann method, natural convection problem , 2010 .

[13]  Shiyi Chen,et al.  A Novel Thermal Model for the Lattice Boltzmann Method in Incompressible Limit , 1998 .

[14]  Song Zheng,et al.  Analysis of force treatment in lattice Boltzmann equation method , 2019, International Journal of Heat and Mass Transfer.

[15]  Zhaoli Guo,et al.  Lattice Boltzmann model for incompressible flows through porous media. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[16]  Viriato Semiao,et al.  First- and second-order forcing expansions in a lattice Boltzmann method reproducing isothermal hydrodynamics in artificial compressibility form , 2012, Journal of Fluid Mechanics.

[17]  Benoît Trouette,et al.  Lattice Boltzmann simulations of a time-dependent natural convection problem , 2013, Comput. Math. Appl..

[18]  S Succi,et al.  Three ways to lattice Boltzmann: a unified time-marching picture. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.

[19]  Xiaowen Shan,et al.  SIMULATION OF RAYLEIGH-BENARD CONVECTION USING A LATTICE BOLTZMANN METHOD , 1997 .

[20]  B. Shi,et al.  Discrete lattice effects on the forcing term in the lattice Boltzmann method. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[21]  G. D. Davis Natural convection of air in a square cavity: A bench mark numerical solution , 1983 .

[22]  Q. Zou,et al.  On pressure and velocity boundary conditions for the lattice Boltzmann BGK model , 1995, comp-gas/9611001.

[23]  S. Syrjälä Higher Order Penalty-Galerkin Finite Element Approach to Laminar Natural Convection in a Square Cavity , 1996 .

[24]  Gerasim V. Krivovichev,et al.  Stability analysis of body force action models used in the single-relaxation-time single-phase lattice Boltzmann method , 2019, Appl. Math. Comput..

[25]  C. Shu,et al.  SIMULATION OF NATURAL CONVECTION IN A SQUARE CAVITY BY TAYLOR SERIES EXPANSION- AND LEAST SQUARES-BASED LATTICE BOLTZMANN METHOD , 2002 .

[26]  D. A. Medvedev,et al.  On equations of state in a lattice Boltzmann method , 2009, Comput. Math. Appl..