Knudsen layer theory for high-order lattice Boltzmann models

2007 ◽  
Vol 80 (2) ◽  
pp. 24003 ◽  
Author(s):  
L. Szalmás
Open Physics ◽  
2008 ◽  
Vol 6 (4) ◽  
Author(s):  
Lajos Szalmás

AbstractWe present a new method in order to obtain variable slip coefficient in binary lattice Boltzmann models to simulate gaseous flows. We present the Boundary layer theory. We study both the single-and multi-fluid BGK-type models as well. The boundary slip and the Knudsen layer are analyzed in detail. Benchmark simulations are carried out in order to compare the analytical derivation with the numerical results. Excellent agreement is found between the two analytical formalism and the numerical simulations.


2010 ◽  
Vol 21 (06) ◽  
pp. 769-783 ◽  
Author(s):  
ZHI-WEI TIAN ◽  
SHENG CHEN ◽  
CHU-GUANG ZHENG

In this study, microscale gaseous flows in the transitional regime have been investigated by lattice Boltzmann method (LBM). In the existing microflows LBM models, the Knudsen layer correction function has been introduced into the models. According to the kinetic theory rigorously, we choose a proper expression of correction function, and then determine its adjustable parameter. A substitute high-order boundary conditions treatment is adopted to capture the velocity slip, without any difficulties in computing the high-order velocity derivatives. The numerical results of two typical microflows show that: the present results agree with the analytical solutions better than the existing LBM simulations. Evident improvements can also be found, especially for finite Kn microflows.


2019 ◽  
Vol 99 (6) ◽  
Author(s):  
C. S. From ◽  
E. Sauret ◽  
S. A. Galindo-Torres ◽  
Y. T. Gu

2008 ◽  
Vol 19 (02) ◽  
pp. 249-257 ◽  
Author(s):  
LAJOS SZALMÁS

We present an optimization procedure in high-order lattice Boltzmann models in order to fine-tune the method for micro-channel flows in the transition region. Both the first and second slip coefficients are tunable, and the hydrodynamic and Knudsen layer solutions can be tailored. Very good results are obtained in comparison with the continuous solution for hard sphere molecules. For the first time, we provide an accurate description of Poiseuille flow in the transition region.


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