PREDETERMINED CONTROL OF OSCILLATORY THERMOCAPILLARY CONVECTION IN A HALF-ZONE LIQUID BRIDGE

Equipment ◽  
2006 ◽  
Author(s):  
S. Uemura ◽  
H. Kawamura
2003 ◽  
Vol 68 (6) ◽  
Author(s):  
V. M. Shevtsova ◽  
D. E. Melnikov ◽  
J. C. Legros

2020 ◽  
Vol 24 (6 Part B) ◽  
pp. 4159-4171
Author(s):  
Shuo Yang ◽  
Rui Ma ◽  
Qiaosheng Deng ◽  
Guofeng Wang ◽  
Yu Gao ◽  
...  

A uniform axial or transverse magnetic field is applied on the silicon oil based ferrofluid of high Prandtl number fluid (Pr ? 111.67), and the effect of magnetic field on the thermocapillary convection is investigated. It is shown that the location of vortex core of thermocapillary convection is mainly near the free surface of liquid bridge due to the inhibition of the axial magnetic field. A velocity stagnation region is formed inside the liquid bridge under the axial magnetic field (B = 0.3-0.5 T). The disturbance of bulk reflux and surface flow is suppressed by the increasing axial magnetic field. There is a dynamic response of free surface deformation to the axial magnetic field, and then the contact angle variation of the free surface at the hot corner is as following, ?hot, B = 0.5 T = 83.34? > ?hot, B = 0.3 T = 72.16? > > ?hot,B = 0.1 T = 54.21? > ?hot, B = 0 T = 43.33?. The results show that temperature distribution near the free surface is less and less affected by thermocapillary convection with the increasing magnetic field, and it presents a characteristic of heat-conduction. In addition, the transverse magnetic field does not realize the fundamental inhibition for thermocapillary convection, but it transfers the influence of thermocapillary convection to the free surface.


2001 ◽  
Vol 44 (19) ◽  
pp. 3765-3774 ◽  
Author(s):  
Zhong Zeng ◽  
Hiroshi Mizuseki ◽  
Kiyoshi Simamura ◽  
Tsuguo Fukuda ◽  
Kazuyuki Higashino ◽  
...  

2016 ◽  
Vol 40 ◽  
pp. 06001
Author(s):  
Ruquan Liang ◽  
Limin Kong ◽  
Fuqiang Yan ◽  
Di Bei ◽  
Shuo Zhang

2014 ◽  
Vol 27 (1) ◽  
pp. 1-10 ◽  
Author(s):  
Shuo Yang ◽  
Ruquan Liang ◽  
Fusheng Yan ◽  
Taiyin Gao ◽  
Yutao Feng

2017 ◽  
Vol 139 (12) ◽  
Author(s):  
Shuo Yang ◽  
Ruquan Liang ◽  
Song Xiao ◽  
Jicheng He ◽  
Shuo Zhang

The influence of airflow shear on the free surface deformation and the flow structure for large Prandtl number fluid (Pr = 111.67) has been analyzed numerically as the parallel airflow shear is induced into the surrounding of liquid bridge from the lower disk or the upper disk. Contrasted with former studies, an improved level set method is adopted to track any tiny deformation of free surface, where the area compensation is carried out to compensate the nonconservation of mass. Present results indicate that the airflow shear can excite flow cells in the isothermal liquid bridge. The airflow shear induced from the upper disk impulses the convex region of free interface as the airflow shear intensity is increased, which may exceed the breaking limit of liquid bridge. The free surface is transformed from the “S”-shape into the “M”-shape as the airflow shear is induced from the lower disk. For the nonisothermal liquid bridge, the flow cell is dominated by the thermocapillary convection at the hot corner if the airflow shear comes from the hot disk, and another reversed flow cell near the cold disk appears. While the shape of free surface depends on the competition between the thermocapillary force and the shear force when the airflow is induced from the cold disk.


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