CLC number: O359
On-line Access: 2024-08-27
Received: 2023-10-17
Revision Accepted: 2024-05-08
Crosschecked: 0000-00-00
Cited: 4
Clicked: 5149
SHAO Xue-ming, LIN Jian-zhong, YU Zhao-sheng. Sedimentation of a single particle between two parallel walls[J]. Journal of Zhejiang University Science A, 2004, 5(1): 111-116.
@article{title="Sedimentation of a single particle between two parallel walls",
author="SHAO Xue-ming, LIN Jian-zhong, YU Zhao-sheng",
journal="Journal of Zhejiang University Science A",
volume="5",
number="1",
pages="111-116",
year="2004",
publisher="Zhejiang University Press & Springer",
doi="10.1631/jzus.2004.0111"
}
%0 Journal Article
%T Sedimentation of a single particle between two parallel walls
%A SHAO Xue-ming
%A LIN Jian-zhong
%A YU Zhao-sheng
%J Journal of Zhejiang University SCIENCE A
%V 5
%N 1
%P 111-116
%@ 1869-1951
%D 2004
%I Zhejiang University Press & Springer
%DOI 10.1631/jzus.2004.0111
TY - JOUR
T1 - Sedimentation of a single particle between two parallel walls
A1 - SHAO Xue-ming
A1 - LIN Jian-zhong
A1 - YU Zhao-sheng
J0 - Journal of Zhejiang University Science A
VL - 5
IS - 1
SP - 111
EP - 116
%@ 1869-1951
Y1 - 2004
PB - Zhejiang University Press & Springer
ER -
DOI - 10.1631/jzus.2004.0111
Abstract: The sedimentation of a single circular particle between two parallel walls was studied by means of direct numerical simulation (DNS) and experiment. The improved implementation of distributed Lagrange multiplier/fictitious domain method used in our DNS is a promising new way for simulation of particulate flows. The settling behaviors of the particle are presented ranging in Reynolds number from 0 to about 700, which showed that our results for low Reynolds numbers agreed well with that reported before. Nevertheless, for higher Reynolds numbers our results were different from theirs. The long-term mean equilibrium positions in our results were all on the centerline, but not at off-center position as reported before. In order to validate our simulation, experiments were also conducted. The results showed that the sedimenting behavior simulated in this paper agreed well with our experiment result.
[1] Christonpherson, D. G. and Dowson, D., 1959, An example of minimum energy dissipation in viscous flow. Proc. R. Soc., A251:550-564.
[2] Feng, J., Hu, H. H. and Joseph, D. D., 1994. Direct simulation of initial value problems for the motion of solid bodies in a Newtonian fluid, Part 1. Sedimentation. J. Fluid Mech., 261:95-134.
[3] Glowinski, R., Pan, T. W., Hesla, T. I. and Joseph, D.D., 1999. A distributed Lagrange multiplier/fictitious domain methos for particulate flows. Int. J. Multiphase Flow, 25:755-794.
[4] Glowinski, R., Pan, T. W., Hesla, T. I., Joseph, D.D. and Periaux, J., 2001. A fictitious domain approach to the direct numerical simulation of incompressible viscous flow past moving rigid bodies: Application to particulate flow. J. Comp. Phys., 169:363-426.
[5] Hu, H.H., Joseph, D.D. and Crochet, M.J., 1992. Direct simulation of fluid particle motions. Theor. Comp. Fluid Dyn., 3:285-306.
[6] Lin, J.Z., Zhang, W.F. and Wang, Y.L., 2002. Research on the orientation distribution of fibers immersed in a pipe flow. J. Zhejiang Univ. Sci., 3(5):501-506.
[7] Patankar, N.A., 1997. Numerical simulation of particulate two-phase flow. Ph.D. thesis. University of Pennsylvania, Pennsylvania.
[8] Suker, D. and Brauer, H., 1975. Fluiddynamik bei quer angestrmten Zylindern. Wrme-und Stoffuertragung, 8:149-158.
[9] Tachibana, M., 1973. On the behaviour of a sphere in the laminar tube flows. Rheol. Acta, 12:58-69.
[10] Vasseur, P. and Cox, R. G., 1977. The lateral migration of spherical particles sedimenting in a stagnant bounded fluid. J. Fluid Mech., 80:561-591.
Open peer comments: Debate/Discuss/Question/Opinion
<1>