Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method
In this paper, lattice Boltzmann scheme is used to simulate particle flow in a steady incompressible flow inside a square cavity. Numerical simulations are carried out for Reynolds number of 130, 400 and 860. Comparisons for three different Stokes number of Stokes number, St = 0.06, St = 0.21, St =...
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2011
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ump-269232020-03-19T07:43:08Z http://umpir.ump.edu.my/id/eprint/26923/ Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method N. M. M., Ammar C. S. N., Azwadi M. S., Idris TJ Mechanical engineering and machinery In this paper, lattice Boltzmann scheme is used to simulate particle flow in a steady incompressible flow inside a square cavity. Numerical simulations are carried out for Reynolds number of 130, 400 and 860. Comparisons for three different Stokes number of Stokes number, St = 0.06, St = 0.21, St = 0.41 are carried out under Reynolds Number 400. The governing equation use is the double-population lattice Boltzmann formulation. Two-dimensional nine velocity model is used for the computation of velocity field. The results obtained by using compact visual FORTRAN are compared with the results found in the literature review. Present study found that lattice Boltzmann scheme is able to carry out equivalent results as conventional scheme. AIP Publishing 2011 Conference or Workshop Item PeerReviewed pdf en http://umpir.ump.edu.my/id/eprint/26923/1/Particle%20movement%20in%20shear%20cavity%20flow%20for%20different%20Stokes%20number.pdf N. M. M., Ammar and C. S. N., Azwadi and M. S., Idris (2011) Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method. In: AIP Conference Proceedings: 4th International Meeting of Advances in Thermofluids (IMAT 2011), 3-4 October 2011 , Melaka. pp. 1018-1024., 1440 (1018). ISSN 0094-243X https://doi.org/10.1063/1.4704317 |
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TJ Mechanical engineering and machinery N. M. M., Ammar C. S. N., Azwadi M. S., Idris Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method |
description |
In this paper, lattice Boltzmann scheme is used to simulate particle flow in a steady incompressible flow inside a square cavity. Numerical simulations are carried out for Reynolds number of 130, 400 and 860. Comparisons for three different Stokes number of Stokes number, St = 0.06, St = 0.21, St = 0.41 are carried out under Reynolds Number 400. The governing equation use is the double-population lattice Boltzmann formulation. Two-dimensional nine velocity model is used for the computation of velocity field. The results obtained by using compact visual FORTRAN are compared with the results found in the literature review. Present study found that lattice Boltzmann scheme is able to carry out equivalent results as conventional scheme. |
format |
Conference or Workshop Item |
author |
N. M. M., Ammar C. S. N., Azwadi M. S., Idris |
author_facet |
N. M. M., Ammar C. S. N., Azwadi M. S., Idris |
author_sort |
N. M. M., Ammar |
title |
Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method |
title_short |
Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method |
title_full |
Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method |
title_fullStr |
Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method |
title_full_unstemmed |
Particle movement in shear cavity flow for different Stokes number using lattice Boltzmann method |
title_sort |
particle movement in shear cavity flow for different stokes number using lattice boltzmann method |
publisher |
AIP Publishing |
publishDate |
2011 |
url |
http://umpir.ump.edu.my/id/eprint/26923/ http://umpir.ump.edu.my/id/eprint/26923/ http://umpir.ump.edu.my/id/eprint/26923/1/Particle%20movement%20in%20shear%20cavity%20flow%20for%20different%20Stokes%20number.pdf |
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2023-09-18T22:42:13Z |
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2023-09-18T22:42:13Z |
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1777416990697193472 |