朱春英, 付涛涛, 高习群, 等. Numerical Simulation of Concentration Field on Liquid Side around Bubble during Rising and Coalescing Process in Non-Newtonian Fluid[J]. 中国化学工程学报(英文版), 2011,19(5):799-807.
ZHU Chunying, FU Taotao, GAO Xiqun, MA Youguang. Numerical Simulation of Concentration Field on Liquid Side around Bubble during Rising and Coalescing Process in Non-Newtonian Fluid[J]. , 2011, 19(5): 799-807.
朱春英, 付涛涛, 高习群, 等. Numerical Simulation of Concentration Field on Liquid Side around Bubble during Rising and Coalescing Process in Non-Newtonian Fluid[J]. 中国化学工程学报(英文版), 2011,19(5):799-807.DOI: 10.1016/S1004-9541(11)60059-1.
ZHU Chunying, FU Taotao, GAO Xiqun, MA Youguang. Numerical Simulation of Concentration Field on Liquid Side around Bubble during Rising and Coalescing Process in Non-Newtonian Fluid[J]. , 2011, 19(5): 799-807.DOI: 10.1016/S1004-9541(11)60059-1.
Numerical Simulation of Concentration Field on Liquid Side around Bubble during Rising and Coalescing Process in Non-Newtonian Fluid
On the basis of Navier-Stockes equation and convection-diffusion equation
combined with surface ten-sion and penetration models
the equations of moment and mass transfer between bubble and the ambient non-Newtonian liquid were established. The formation of a single bubble from a submersed nozzle of 1.0 mm di-ameter and the mass transfer from an artificially fixed bubble into the ambient liquid were simulated by the volume-of-fluid (VOF) method. Good agreement between simulation results and experimental data confirmed the validity of the numerical method. Furthermore
the concentration distribution around rising bubbles in shear thinning non-Newtonian fluid was simulated. When the process of a single ellipsoidal bubble with the bubble deformation rate below 2.0 rises
the concentration distribution is a singletail in the bubble’s wake
but it is fractal when the bubble deformation rate is greater than 2.0. For the overtaking of two in-line rising bubbles
the concentration distribution area between two bubbles broadens gradually and then coalescence occurs. The bifurcation of concentration distribution appears in the rear of the resultant bubble.
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相关作者
Nikolaos A. Avgerinos
Dionissios P. Margaris
Li Xinyu
Song Yiwen
Teng Shenglong
Zeng Dewang
Xu Jingxin
Zhang Jing
相关机构
Department of Mechanical Engineering and Aeronautics, Fluid Mechanics Laboratory, University of Patras,- Patras
Key Laboratory of Energy Thermal Conversion and Control of Ministry of Education, School of Energy and Environment, Southeast University
State Key Laboratory of Low-carbon Smart Coal-fired Power Generation and Ultra-clean Emission, China Energy Science and Technology Research Institute Co.,Ltd.
School of Chemical Engineering and Technology, Tianjin University
School of Mechanical and Power Engineering, Shenyang University of Chemical Technology