Momentum transfer of a Boltzmann-lattice fluid with boundaries

By M. Bouzidi, M. Firdaouss, Pierre Lallemand. 2001

1,238 citations recorded by the source corpus.

Subfields: Aerospace Engineering, Computational Mechanics

View Paper: https://www.semanticscholar.org/paper/f8e397de7f3ea50848dba713a755ac2befb823fb

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Aerospace Engineering

1. Li-Shi Luo
2. Cyrus K. Aidun
3. Dominique d'Humières
4. E. Ding
5. Manfred Krafczyk
6. Jonas Tölke
7. Irina Ginzburg
8. Frederik Verhaeghe

In Computational Mechanics

1. Qing Liu
2. Li-Shi Luo
3. Qing Li
4. Yangyang He
5. Irina Ginzburg
6. Cass T. Miller
7. Qinjun Kang
8. Chong Pan

Citations in the corpus

• Lattice‐Boltzmann simulation of two‐phase flow in porous media (2004, background): “…combines the bounce-back scheme and spatial interpolations of first or second order to realize the locations of boundaries with arbitrary curvatures, can be incorporated for further improvement of numerical stability and a more rapid convergence [Bouzidi et al., 2001; Lallemand and Luo, 2003].”
• Study of Simple Hydrodynamic Solutions with the Two-Relaxation-Times Lattice Boltzmann Scheme (2008, methodology): “Table 1 summarizes the coefficients of the principal M (u) q schemes: bounce-back (BB), several linear interpolations from three populations based LI(α(u))−family: ULI/DLI from [4], YLI from [41], then CLI, MGULI/MGDLI and MGYLI schemes from “magic” linear sub-family MGLI(α(u)) built in [16].”
• Benchmark computations based on Lattice-Boltzmann, Finite Element and Finite Volume Methods for laminar Flows (2006, methodology): “As the benchmark problem discussed in the subsequent sections has also curved boundaries, we utilize the boundary conditions developed in [32,33] for velocity Dirichlet boundaries.”
• Extension of the Lattice-Boltzmann Method for Direct Simulation of Suspended Particles Near Contact (2003, methodology): “( 17 , 18) The model provided by Heelmels et al. (22) is a modified Shell model where it accurately conserves mass and momentum.”
• Lattice-Boltzmann simulations in reconstructed parametrized porous media (2006, methodology): “Furthermore, the simple bounce back scheme has to be replaced by a boundary condition whose convergence behaviour is consistent with the methods bulk behaviour, e.g. Bouzidi et al. (2001).”
• Coupled lattice Boltzmann method and discrete element modelling of particle transport in turbulent fluid flows: Computational issues (2007, background): “Nevertheless, this discrete representation [24] provides a universal approach for any shaped particle; thus arbitrarily shaped particles can be readily handled within the current LB framework.”
• LES of turbulent square jet flow using an MRT lattice Boltzmann model (2006, background): “The no-slip boundary conditions in the LBE is realized by the bounce-back boundary conditions [31,32,22]:”
• Continuous Inertial Focusing and Separation of Particles by Shape (2012, background): “[65] M.”
• Lattice Boltzmann methods for multiphase flow and phase-change heat transfer (2015, methodology): “For isothermal LB models, many boundary treatments have been devised [142, 220-225].”