Effects of Numerical Schemes of Contact Angle on Simulating Condensation Heat Transfer in a Subcooled Microcavity by Pseudopotential Lattice Boltzmann Model

被引:0
作者
Wang, Dongmin [1 ]
Lin, Gaoshuai [1 ]
Zhao, Yugang [1 ]
Gao, Ming [1 ]
机构
[1] Univ Shanghai Sci & Technol, Sch Energy & Power Engn, Key Lab Multiphase Flow & Heat Transfer Shanghai P, Shanghai 200093, Peoples R China
基金
中国国家自然科学基金;
关键词
lattice Boltzmann method; condensation; contact angle; ghost fluid layer; fluid density variation near wall; HYDROPHOBIC SURFACES; DROPLETS; DROPWISE; VAPOR; COALESCENCE; TRANSITION; FLOW; GAS;
D O I
10.3390/en16062622
中图分类号
TE [石油、天然气工业]; TK [能源与动力工程];
学科分类号
0807 ; 0820 ;
摘要
Various numerical schemes of contact angle are widely used in pseudopotential lattice Boltzmann model to simulate substrate contact angle in condensation. In this study, effects of numerical schemes of contact angle on condensation nucleation and heat transfer simulation are clarified for the first time. The three numerical schemes are pseudopotential-based contact angle scheme, pseudopotential-based contact angle scheme with a ghost fluid layer constructed on the substrate with weighted average density of surrounding fluid nodes, and the geometric formulation scheme. It is found that the subcooling condition destabilizes algorithm of pseudopotential-based contact angle scheme. However, with a ghost fluid layer constructed on the substrate or using geometric formulation scheme, the algorithm becomes stable. The subcooling condition also decreases the simulated contact angle magnitude compared with that under an isothermal condition. The fluid density variation near a microcavity wall simulated by pseudopotential-based contact angle scheme plays the role of the condensation nucleus and triggers "condensation nucleation". However, with a ghost fluid layer constructed on the substrate or using geometric formulation scheme, the simulated fluid density distribution near the wall is uniform so that no condensation nucleus appears in the microcavity. Thus, "condensation nucleation" cannot occur spontaneously in the microcavity unless a thin liquid film is initialized as a nucleus in the microcavity. The heat flux at the microcavity wall is unphysical during the "condensation nucleation" process, but it becomes reasonable with a liquid film formed in the microcavity. As a whole, it is recommended to use pseudopotential-based contact angle scheme with a ghost fluid layer constructed on the substrate or use the geometric formulation scheme to simulate condensation under subcooling conditions. This study provides guidelines for choosing the desirable numerical schemes of contact angle in condensation simulation by pseudopotential lattice Boltzmann model so that more efficient strategies for condensation heat transfer enhancement can be obtained from numerical simulations.
引用
收藏
页数:16
相关论文
共 37 条
[1]   A MODEL FOR COLLISION PROCESSES IN GASES .1. SMALL AMPLITUDE PROCESSES IN CHARGED AND NEUTRAL ONE-COMPONENT SYSTEMS [J].
BHATNAGAR, PL ;
GROSS, EP ;
KROOK, M .
PHYSICAL REVIEW, 1954, 94 (03) :511-525
[2]   Wetting condition in diffuse interface simulations of contact line motion [J].
Ding, Hang ;
Spelt, Peter D. M. .
PHYSICAL REVIEW E, 2007, 75 (04)
[3]   A review of dropwise condensation: Theory, modeling, experiments, and applications [J].
El Fil, Bachir ;
Kini, Girish ;
Garimella, Srinivas .
INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER, 2020, 160
[4]   Heat Transfer in Unfrozen and Frozen Porous Media: Experimental Measurement and Pore-Scale Modeling [J].
Farahani, Mehrdad Vasheghani ;
Hassanpouryouzband, Aliakbar ;
Yang, Jinhai ;
Tohidi, Bahman .
WATER RESOURCES RESEARCH, 2020, 56 (09)
[5]   A lattice Boltzmann method for simulation of liquid-vapor phase-change heat transfer [J].
Gong, Shuai ;
Cheng, Ping .
INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER, 2012, 55 (17-18) :4923-4927
[6]   Numerical investigation of droplet motion and coalescence by an improved lattice Boltzmann model for phase transitions and multiphase flows [J].
Gong, Shuai ;
Cheng, Ping .
COMPUTERS & FLUIDS, 2012, 53 :93-104
[7]   3D lattice Boltzmann investigation of nucleation sites and dropwise-to-filmwise transition in the presence of a non-condensable gas on a biomimetic surface [J].
Guo, Qing ;
Cheng, Ping .
INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER, 2019, 128 :185-198
[8]   SIMULATION OF CAVITY FLOW BY THE LATTICE BOLTZMANN METHOD [J].
HOU, SL ;
ZOU, Q ;
CHEN, SY ;
DOOLEN, G ;
COGLEY, AC .
JOURNAL OF COMPUTATIONAL PHYSICS, 1995, 118 (02) :329-347
[9]   Contact angle adjustment in equation-of-state-based pseudopotential model [J].
Hu, Anjie ;
Li, Longjian ;
Uddin, Rizwan ;
Liu, Dong .
PHYSICAL REVIEW E, 2016, 93 (05)
[10]   Lattice Boltzmann equation method in electrohydrodynamic problems [J].
Kupershtokh, A. L. ;
Medvedev, D. A. .
JOURNAL OF ELECTROSTATICS, 2006, 64 (7-9) :581-585