Simulation of the two-dimensional flow of the initiation channel of the Itaipu hydroelectric power plant by the lattice Boltzmann method

被引:1
作者
Cargnelutti, J. [1 ]
Galina, V. [2 ]
Kaviski, E. [3 ]
Gramani, L. M. [4 ]
Lobeiro, A. M. [5 ]
机构
[1] Univ Tecnol Fed Parana UTFPR, Coordenacao Curso Matemat, Rua Cristo Rei 19, BR-85902490 Toledo, PR, Brazil
[2] Univ Tecnol Fed Parana UTFPR, Dept Matemat, Toledo, PR, Brazil
[3] Univ Fed Parana UFPR, Dept Hidraul & Saneamento, Curitiba, Parana, Brazil
[4] Univ Fed Parana UFPR, Dept Matemat, Curitiba, Parana, Brazil
[5] Univ Tecnol Fed Parana UTFPR, Dept Matemat, Campo Mourao, PR, Brazil
来源
REVISTA INTERNACIONAL DE METODOS NUMERICOS PARA CALCULO Y DISENO EN INGENIERIA | 2018年 / 34卷 / 01期
关键词
Numerical simulation; lattice Boltzmann method; Shallow water equations; Open-channel flow; Submerged obstacles; SHALLOW-WATER FLOWS; MODEL; STABILITY; EQUATIONS;
D O I
10.23967/j.rimni.2017.11.001
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
This paper analyzes the ability of the Lattice Boltzmann method (LBM) with multiple relaxation times (MRT) in the simulation of flow in practical engineering problems. The case study covered refers to the first section of the initiation channel, which is part of the piracema channel, located in the Itaipu Hydroelectric Power Plant. The initiation channel has submerged obstacles distributed from one margin to the other, in order to reduce water velocity and allow the piracema cycle to occur. The governing equations of flow are the shallow water equations, which will be solved through the LBM-MRT. The non-slip bounce-back scheme was used on walls and obstacles, constant discharge at the inlet and fixed depth at the outlet of the channel. Due to the characteristics of the problem to be simulated, a large eddy simulation (LES) technique was incorporated into the computational code, which allows to obtain results that are closer to the actual behavior of the flow. In addition, the stability of the simulation at all points of the mesh is evaluated for each step of time and, together with the property of the consistency of the LBM, the convergence of the solution is obtained. The simulation provides the depth, velocities in the x and y directions, and the magnitude of water vorticity.
引用
收藏
页数:9
相关论文
共 43 条
[1]  
[Anonymous], THESIS
[2]   THE LATTICE BOLTZMANN-EQUATION - THEORY AND APPLICATIONS [J].
BENZI, R ;
SUCCI, S ;
VERGASSOLA, M .
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 1992, 222 (03) :145-197
[3]   Hybrid lattice Boltzmann finite difference simulation of mixed convection flows in a lid-driven square cavity [J].
Bettaibi, Soufiene ;
Kuznik, Frederic ;
Sediki, Ezeddine .
PHYSICS LETTERS A, 2014, 378 (32-33) :2429-2435
[4]   Lattice Boltzmann method for fluid flows [J].
Chen, S ;
Doolen, GD .
ANNUAL REVIEW OF FLUID MECHANICS, 1998, 30 :329-364
[5]   Asymmetric lattice Boltzmann model for shallow water flows [J].
Chopard, B. ;
Pham, V. T. ;
Lefevre, L. .
COMPUTERS & FLUIDS, 2013, 88 :225-231
[6]  
d'Humieres D., 1992, Prog. Astronaut. Aeronaut, V159, P450
[7]   A central moments-based lattice Boltzmann scheme for shallow water equations [J].
De Rosis, Alessandro .
COMPUTER METHODS IN APPLIED MECHANICS AND ENGINEERING, 2017, 319 :379-392
[8]   Hybrid lattice Boltzmann method on overlapping grids [J].
Di Ilio, G. ;
Chiappini, D. ;
Ubertini, S. ;
Bella, G. ;
Succi, S. .
PHYSICAL REVIEW E, 2017, 95 (01)
[9]  
doAmaral F. R., 2015, THESIS
[10]  
Friedrich M. F., 2007, 17 S BRAS REC HIDR S