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Discrete effects on the forcing term for the lattice Boltzmann modeling of steady hydrodynamics

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Fig.  1. Schematic representation of  studied channel flow problems: (a)  porous  flow  with  wall injection,  (b)  rotating Poiseuille flow
Fig. 2. Velocity  profiles in  the  porous channel  flow  with wall  injection simulated with LBM-TRT for N  y =  2  h  / δ x  =  32 computational  cells  and   =  3  /  8  ,  comparing  two force  schemes and their  respective analytical solutions, given  b
Fig. 3. Mesh convergence analysis in the porous channel flow with wall injection simulated with the LBM-TRT scheme using   = 3  /  8 and Ma  = 0
Fig. 6. Velocity profiles in the rotating channel Poiseuille flow simulated with LBM-TRT for N  y  =  2  h  / δ x  =  32 computational cells and   =  3  /  16 using two force schemes  (with A  =  0  and A  =  1  ) versus the analytical solutions given by  Eq
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