Pattern selection for convective flow in a liquid bridge subjected to remote thermal action

被引:5
作者
Gaponenko, Y. [1 ]
Yano, T. [2 ]
Nishino, K. [3 ]
Matsumoto, S. [4 ]
Shevtsova, V. [5 ,6 ]
机构
[1] Univ Libre Bruxelles ULB, Micrograv Res Ctr, CP-165-62,50 Ave FD Roosevelt, B-1050 Brussels, Belgium
[2] Kanagawa Univ, Dept Mech Engn, 3-27-1 Rokkakubashi,Kanagawa Ku, Yokohama, Kanagawa 2218686, Japan
[3] Yokohama Natl Univ, Dept Mech Engn, 9-5 Tokiwadai,Hodogaya Ku, Yokohama, Kanagawa 2408501, Japan
[4] Japan Aerosp Explorat Agcy, 2-1-1 Sengen, Tsukuba, Ibaraki 3058505, Japan
[5] Mondragon Univ, Mech & Mfg Dept, Loramendi 4,Apdo 23, Arrasate Mondragon 20500, Spain
[6] Basque Fdn Sci, Bilbao, Spain
关键词
3-DIMENSIONAL NUMERICAL-SIMULATION; OSCILLATORY THERMOCAPILLARY FLOW; HEAT-TRANSFER; INSTABILITY; STABILITY; FLUID; ONSET;
D O I
10.1063/5.0101901
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
The stability of thermocapillary/buoyant flows is affected by a remote thermal source. We present a nonlinear two-phase computational study of convection in a liquid bridge that develops under the action of Marangoni and buoyancy forces as well as under the influence of distant thermal disturbances. The gas phase (air) occupies a typical annular container holding a liquid bridge (n-decane, Pr = 14), and the disturbances are locally imposed in the form of hot/cold spots on the outer wall of the container. The hydrothermal wave instability and pattern selection have been explored for two temperature differences delta T by varying the intensity of thermal source H-f over a wide range. Not far from the critical point, in all the cases, the instability emerges in the form of a standing wave, but the azimuthal wavenumber depends on whether the external perturbation is caused by cooling (m = 2) or by heating (m = 1). Further into supercritical area, 45% above the threshold, in the region with thermal perturbations - 200 < H-f < 50 , the flow pattern comprises, but is not limited to, a hydrothermal traveling wave with the azimuthal wavenumber m = 2. For hotter perturbations, the instability develops either in the form of traveling or standing waves, depending on H-f, with the prevailing mode m = 1, but with a strong presence of other modes. Published under an exclusive license by AIP Publishing.
引用
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页数:12
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