Effect of Acoustic Streaming on Heat Transfer of Porous Composite Phase Change Material by Using Lattice Boltzmann Simulation

被引:2
作者
Li, Xiangxuan [1 ]
Li, Xinyi [1 ]
Cui, Wei [1 ]
Ma, Ting [1 ]
Lu, Lin [2 ]
Wang, Qiuwang [1 ]
机构
[1] Xi An Jiao Tong Univ, Key Lab Thermofluid Sci & Engn, MOE, Xian 710049, Shaanxi, Peoples R China
[2] Hong Kong Polytech Univ, Dept Bldg Serv Engn, Hong Kong 999077, Peoples R China
来源
JOURNAL OF HEAT TRANSFER-TRANSACTIONS OF THE ASME | 2021年 / 143卷 / 09期
基金
中国国家自然科学基金;
关键词
lattice Boltzmann method; phase change material; acoustic streaming; porous composite; melting process; PARAFFIN/EXPANDED GRAPHITE COMPOSITE; DOUBLE-DIFFUSIVE CONVECTION; NATURAL-CONVECTION; NUMERICAL-SIMULATION; MECHANICAL VIBRATION; ULTRASOUND; RADIATION; MEDIA; FLOW;
D O I
10.1115/1.4051506
中图分类号
O414.1 [热力学];
学科分类号
摘要
In this paper, the lattice Boltzmann (LB) method was used to simulate the flow and heat transfer process in porous composite phase change material (PCM) with acoustic streaming, 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 the flow field, temperature field, liquid fraction field, and average Nusselt number at the 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 strengthened 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 a more remarkable inhibiting effect on average liquid fraction, decreasing by 1.11%, 5.09%, and 20.1% at the amplitude of acoustic streaming delta rho* = 0.005, 0.01, 0.02, respectively. The average temperature and average liquid fraction show no obvious differences with the increasing of the wavelength of the acoustic streaming.
引用
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页数:12
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