The effect of interstitial fluid viscosity on particle segregation in a slurry rotating drum

2011 ◽  
Vol 23 (8) ◽  
pp. 083301 ◽  
Author(s):  
S. H. Chou ◽  
C. C. Liao ◽  
S. S. Hsiau
2008 ◽  
Vol 2008.83 (0) ◽  
pp. _10-12_
Author(s):  
Hirotaka YADA ◽  
Yuta EMURA ◽  
Toshihiro KAWAGUTI ◽  
Takuya TSUJI ◽  
Toshitsugu TANAKA

1995 ◽  
Vol 2 (2) ◽  
pp. 113-121
Author(s):  
Hiroshi Ohue ◽  
Genshi Kawashima ◽  
Wen-Jei Yang

The Laser Doppler Velocimetry (LDV) is employed to investigate energy dissipation during a spin-down process inside a rotating drum. The tracer/light sheet method is applied to observe flow patterns in the entire flow field from which the instantaneous, two-dimensional velocity distribution and the formation and subsequent time wise variation of the Ekman boundary layer are determined. Results are synthesized to find the relationship between the Ekman boundary layer and the redistribution of secondary-flow induced angular momentum. The fluid viscosity, drum size and speed of rotation are varied to determine their effects on both the Ekman boundary layer and energy dissipation during spin-down process. The role of Ekman boundary layer in the reduction of rotating fluid motion is determined. Results from the study may be used to develop a method to achieve uniform mixing in an enclosed vessel.


2009 ◽  
Author(s):  
Chun-Chung Liao ◽  
Shu-San Hsiau ◽  
Masami Nakagawa ◽  
Stefan Luding

2021 ◽  
Vol 378 ◽  
pp. 430-440 ◽  
Author(s):  
A.N. Huang ◽  
T.H. Cheng ◽  
W.Y. Hsu ◽  
C.C. Huang ◽  
H.P. Kuo

2001 ◽  
Vol 7 (3) ◽  
pp. 165-171
Author(s):  
Wen-Jei Yang ◽  
Hiroshi Ohue ◽  
Genshi Kawashima

An experimental study is performed to disclose the origin of Ekman flow on the surfaces of a rotating drum resulting from fluid-structure interaction after an impulsive start of motion (referred to as the spin-up process) or an impulsive stop (the spin-down process). Laser Doppler velocimetry (LDV) is employed to determine instantaneous distribution of both the radial and angular velocity components in the flow field inside the rotating drum. From these results, the secondary flow and the time history of the Ekman boundary layer thickness are determined. The tracer/light sheet method is also engaged to enable real-time visualization of flow patterns. Fluid viscosity, drum size and rotational speed are varied to determine their effects on fluid-structure interactions. Results may be applied to cavity flow in rotating machinery.


Author(s):  
K. Hadinoto ◽  
J. Sinclair Curtis

The importance of interstitial fluid effects on particle fluctuating motion in gas-particle or liquid-particle flows with significant particle-particle collisions can be characterized by the ratio of the coefficient of restitution for inelastic particle-particle collisions in a fluid ef to the coefficient of restitution for collisions in a vacuum es. In previous research, the ratio ef/es has been found to depend on the impact Stokes number St, which relates the particle inertia to the viscous force. The value of the impact Stokes number is known to be a function of the particle velocity at impact, the size and density of the particle, and the fluid viscosity. In the present work, the effect of the interstitial fluid on particle fluctuating motion is investigated experimentally using LDV/PDPA in a vertical pipe flow configuration. The influence of the variation in the particle loading and Reynolds number, which affects the particle impact velocity and, hence, ef, is probed using particles of two different densities with comparable sizes. Specifically, the downward flow of 70 micron glass beads (density = 2500 kg/m3) and 60 micron hollow ceramic microspheres (density = 700 kg/m3) is investigated for solids loadings (ratio of solids mass flowrate to gas mass flowrate) from 0.4 to 7 and Reynolds numbers which vary from 6000 to 13,000. For this range of conditions, the values for ef range between 0.65 and 0.94 (0.94 is the value for es for glass beads colliding in a vacuum). Trends in the mean and fluctuating velocities for both the gas and particle phases, as well as the gas turbulence modulation in the presence of particles, are discussed in relation to the degree of influence of the interstitial fluid on the details of the particle motion.


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