Flow bifurcation routes to chaos of thermocapillary convection for low Prandtl number fluid in shallow annular pool with surface heat dissipation

被引:19
|
作者
Zhang, Li [1 ,2 ]
Li, You-Rong [1 ]
Wu, Chun-Mei [1 ]
Liu, Qiu-Sheng [3 ]
机构
[1] Chongqing Univ, Key Lab Low Grade Energy Utilizat Technol & Syst, Minist Educ, Coll Power Engn, Chongqing 400044, Peoples R China
[2] Sichuan Int Studies Univ, Chongqing Nanfang Translators Coll, Chongqing 401120, Peoples R China
[3] Chinese Acad Sci, Inst Mech, Key Lab Micrograv, Natl Micrograv Lab, Beijing 100190, Peoples R China
基金
中国国家自然科学基金;
关键词
Flow bifurcation; Thermocapillary convection; Low Prandtl number; Shallow annular pool; Surface heat dissipation; 3-DIMENSIONAL NUMERICAL-SIMULATION; LIQUID LAYERS; BINARY-MIXTURE; BUOYANCY FLOW; INSTABILITY; EVAPORATION; MECHANISMS; TRANSITION; STABILITY; PATTERN;
D O I
10.1016/j.ijthermalsci.2017.11.010
中图分类号
O414.1 [热力学];
学科分类号
摘要
In order to understand clearly the transition characteristics of thermocapillary convection of low Prandtl number fluid in shallow annular pool with surface heat dissipation, some bifurcation routes to chaos of thermocapillary convection have been numerically investigated by using the finite volume method in this paper. The annular pool was filled with the low Prandtl (Pr) number fluid of Pr = 0.011. The range of Biot number is from 0 to 1. Results indicate that the flow bifurcation route of thermocapillary convection depends intensively on surface heat dissipation. When surface heat dissipation is smaller, with the increase of Marangoni number the flow bifurcation sequence of thermocapillary convection is two-dimensional axisymmetric steady flow -> three-dimensional steady flow -> coexisting hydrothermal waves and radial moving waves -> radial moving waves -> chaos. When surface heat dissipation is larger, the bifurcation sequence becomes simple as two-dimensional axisynunetaic steady flow -> hydrothermal waves -> chaos. Furthermore, every bifurcation of thermocapillary convection is always accompanied by the variations of the wave number and the oscillatory frequency. Furthermore, the temperature fluctuation amplitude on the free surface increases gradually with the increase of Marangoni number.
引用
收藏
页码:23 / 33
页数:11
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