Three-dimensional thermocapillary–buoyancy flow of silicone oil in a differentially heated annular pool

2007 ◽  
Vol 50 (5-6) ◽  
pp. 872-880 ◽  
Author(s):  
Lan Peng ◽  
You-Rong Li ◽  
Wan-Yuan Shi ◽  
Nobuyuki Imaishi
1999 ◽  
Vol 9 (5) ◽  
pp. 212-218
Author(s):  
Dimiter Hadjistamov

Abstract Model suspension with Aerosil 380 in epoxy resin Araldite GY260 and Aerosil 380 in silicone oil M20000 are compared. The systems with 7.5%, 10% and 12.5% Aerosil 380 in Araldite GY260 show shear thickening flow behavior. A shear induced hydrodynamic force effects at the onset of shear thickening a disorder of the well ordered movement of the Areosil particles in layers. The Areosil particles build-up a pseudo-mixture that lead to a sudden development of a three dimensional structure, i.e. to viscosity incerease. One can assume that the shear thickening can be explained with an order-to-disorder transition. The viscosity increase of the shear thickening region is limited – It can reach topmost the plastic viscosity curve that has to be expected from the beginning. The dilatant system begins in the third straight line section to coincide the viscosity curve of the expected plastic system for the subsequent thixotropic agent concentration.


Author(s):  
Shuangqin Liu ◽  
Douglas A. Gauthier ◽  
Ethan Mandelup ◽  
Robert D. White

In this research, an uncoiled scale gerbil cochlea is designed and fabricated. The cochlea model is an uncoiled, 16 times scale model of the real gerbil cochlea and has only one duct. Both the basilar membrane width and the duct size vary along the length of the device, in analogy to the physiology. The cochlea duct is filled with silicone oil and driven by a modal exciter (shaker) at different frequencies. The movement of the basilar membrane is measured using laser vibrometry at different locations along the basilar membrane. The ratio of the basilar membrane velocity to drive velocity is computed and plotted. The characteristic frequency of the model varies from 7000 Hz at 2 cm from the base of the cochlea to 350 Hz at the 15 cm from the base. Two different viscosities silicone oil, 20 cSt and 500 cSt are used for the basilar membrane movement measurements. A WKB method is applied to the calculation of the basilar membrane movement of the scale cochlea model, in which the fluid motion is fully three dimensional.


Author(s):  
Wanyuan Shi ◽  
Nobuyuki Oshima ◽  
Nobuyuki Imaishi

Thermocapillary convection in a shallow annular pool (depth d = 1 mm) of silicone oil (0.65 cSt, Pr = 6.7), heated from the inner wall, is investigated by numerical simulations. Under a fixed value of temperature difference between the outer and inner walls, surface temperature gradient in the inner heated pool is about 10% higher than that in the outer heated pool. Accordingly, the critical temperature difference for the incipience of HTW (ΔTc = 4.58K) is smaller than that (ΔTc = 5.0K) in the outer heated pool. Numerical simulations indicate that two groups of HTW, propagating in opposite azimuthal directions to each other, coexist and produce interference patterns in the inner heated pool. Rotation of the pool around its axis gives no significant influence on the behavior of HTW in the inner heated pool. The characteristics of HTW are discussed in contrast with those in the outer heated pool.


Crystals ◽  
2019 ◽  
Vol 9 (4) ◽  
pp. 217 ◽  
Author(s):  
Jia-Jia Yu ◽  
Lu Zhang ◽  
Ting Shen ◽  
Li Zhang ◽  
You-Rong Li

A series of three-dimensional numerical simulations were performed to understand the thermal-solutal capillary-buoyancy flow of Ge1-xSix melts during Czochralski crystal growth with a rotating crystal or crucible. The crystal and crucible rotation Reynolds numbers in this work are 0∼3.5 × 103 (0∼4.4 rpm) and 0∼−2.4 × 103 (0∼−1.5 rpm), respectively. Simulation results show that if the thermal capillary Reynolds number is relatively low, the flow will be steady and axisymmetric, even though the crystal or crucible rotates at a constant rate. The critical thermal capillary Reynolds number for the initiation of the three-dimensional oscillatory flow is larger than that of pure fluids. As the crystal or crucible rotation rate increases, the critical thermal capillary Reynolds number first increases and then decreases. The dominant flow pattern after the flow destabilization is azimuthal traveling waves. Furthermore, a reversed evolution from the oscillatory spoke pattern to traveling waves appears in the melt. Once the crystal or crucible rotation rate is relatively large, the traveling waves respectively evolve to rotating waves at the crystal rotation and a spindle-like pattern at the crucible rotation. In addition, the maximum amplitude of solute concentration oscillation on the free surface initially decreases, but finally rises with the crystal or crucible rotation rate increasing.


2004 ◽  
Vol 39 (12) ◽  
pp. 1055-1062 ◽  
Author(s):  
Y. R. Li ◽  
L. Peng ◽  
S. Y. Wu ◽  
N. Imaishi ◽  
D. L. Zeng

2016 ◽  
Vol 23 (06) ◽  
pp. 1650053
Author(s):  
YUANXIN FENG ◽  
CHUHANG ZHANG

By thermal evaporation method, gold (Au) atomic aggregates were fabricated on a silicone oil surface and the aggregation mechanism was investigated. It is found that the apparent surface coverage ([Formula: see text]) of the Au aggregates dropped obviously, from 15% to 12% as the oil temperature (T) increased from 285[Formula: see text]K to 353[Formula: see text]K. Meanwhile, the average width of the aggregates gradually increased from 0.36[Formula: see text][Formula: see text]m to 0.50[Formula: see text][Formula: see text]m, indicating the aggregates combine with each other as T increased. By the atomic force microscopy observation, Au nanoparticles with diameter around 45.0 nm were observed in the aggregates, which were independent with T. Similarly, the average height of the aggregates found remain unchanged at around 10.0[Formula: see text]nm as T increased. The anomalous aggregation mechanism of Au aggregates suggests that a compact microstructure for Au aggregates is preferred at high T rather than three-dimensional (3D) growth, which is quite different from that of Ag aggregates.


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