Direct modeling method of acoustic streaming using lattice Boltzmann approach

2021 ◽  
Author(s):  
Jaouad Benhamou ◽  
Mohammed Jami ◽  
Ahmed Mezrhab
Kybernetes ◽  
2004 ◽  
Vol 33 (2) ◽  
pp. 382-389 ◽  
Author(s):  
Wang Yinao ◽  
Chen Zhijie ◽  
Gao Zhiqiang ◽  
Chen Mianyun

2012 ◽  
Vol 31 ◽  
pp. 901-908
Author(s):  
Tianmao Xu ◽  
Yun Zeng ◽  
Lixiang Zhang ◽  
Jing Qian

2002 ◽  
Vol 32 (4) ◽  
pp. 297-309 ◽  
Author(s):  
S. Marino ◽  
A. De Gaetano ◽  
A. Giancaterini ◽  
D. Giordano ◽  
M. Manco ◽  
...  

2013 ◽  
Vol 312 ◽  
pp. 800-804
Author(s):  
Zheng Hao Ge ◽  
Wei Huang ◽  
Zhi Ping Ma ◽  
Yu Bie

To study the globoidal indexing cams parametric design, this paper introduced three kinds of its parametric modeling method.That was offset surfaces method , direct modeling method and "point - curve - surface" method. Then modeled the globoidal indexing cams which had the same parameters and specifications by three parametric methods and Pro/Engineer.Meanwhile, used curvature comb command in Pro/Engineer to conduct the curvature analysis of indexing segment of cam profile. At last, conducted the indexing mechanisms kinematic simulation by ADAMS. From the characteristics of these three parametric methods and the result of cam profiles curvature analysis, this paper explains the reason of jitter acceleration in the simulation results.


2021 ◽  
Author(s):  
Xiangxuan Li ◽  
Xinyi Li ◽  
Wei Cui ◽  
Ting Ma ◽  
Vivien Lu Lin ◽  
...  

Abstract In this paper, lattice Boltzmann method was used to simulate the flow and heat transfer process in porous composite phase change material with acoustic streaming, in order to investigate the mechanism of heat transfer enhancement caused by acoustic streaming. The study focused on the effect of acoustic streaming at different Rayleigh number, Prandtl number, amplitude and wavelength of acoustic streaming on flow field, temperature field, liquid fraction field and average Nusselt number at hot wall.. The results show that acoustic streaming can enhance the fluid flow in the liquid phase region, and reduce the temperature inhomogeneity and inclination of liquid-solid interface front. The natural convection and the forced convection caused by acoustic streaming both get strengthen with the increasing of Rayleigh number, thus the influence of acoustic streaming first slightly rises and then drops. The momentum diffuses slower compared to the heat diffusion with the increasing of Prandtl number, thus the influence of acoustic streaming increases. With the amplitude of acoustic streaming increasing, the effect of acoustic streaming has more remarkable inhibiting effect on average liquid fraction, decreasing by 1.11%, 5.09% and 20.1% at the amplitude of acoustic streaming δρ*=0.005, 0.01, 0.02, respectively. The average temperature and average liquid fraction show no obvious differences with the increasing of wavelength of the acoustic streaming.


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