2021 TAKEO GC CUP...Title 2021 TAKEO GC CUP Created Date 1/25/2021 4:42:18 PM
Ryuichi IWATA1 Takeo KAJISHIMATakeo KAJISHIMA11...
Transcript of Ryuichi IWATA1 Takeo KAJISHIMATakeo KAJISHIMA11...
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Ryuichi IWATA1Takeo KAJISHIMA1Takeo KAJISHIMA1Shintaro TAKEUCHI 2
1 Osaka university2 The university of Tokyo
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ex. Three-phase fluidized bed, flotation, air lift
Microscopic
Interface phenomena– Bubble deformation, surface tension
Three-phase flows include
Microscopic,– Particle rotation, vortex shedding
– Interface phenomena– Collective behavior Mesoscopic
◎ Multi-fluid model (Tomiyama1994)◎ Euler/Lagrange Calculations ( Bourloutski, Sommerfeld 2002) ◎Turbulent structure (Kitagawa 2000)◎Front Tracking-DEM coupling
h d (A l d 2005)
(Kitagawa 2000) (Annaland 2005)
method (Annaland 2005)
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– Fluid-Solid Interaction: Immersed boundary method of body force type (Kajishima 2001)
– Gas-Liquid Interface Capturing: Volume of fluid method – Cartesian coordinate system– Finite difference method – Dispersed-phases described by volumetric fraction
in each computational cell.
Multiple bubbles and particle interaction
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• Fluids-Solid Interaction :– Clusterization of 1024-particle system (Kajishima and co-workers, 2001,2002)– Hindered settling in 105-particle system (Hidaka and co-workers, 2006)
Particle of arbitrarily (time dependent) geometry (Yuki and co workers 2007)– Particle of arbitrarily (time dependent) geometry (Yuki and co-workers 2007)
gg
Particle distribution Induced vortices Sedimentation Deformable particles
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Unified velocity field
The equation of continuity and N-S equation based on one-fluid formulation
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Interaction force
Momentum and angler momentum equations
No leakage of momentum
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Basic equationsBasic equations0.10 0.300.00
1.000.820.22
1.00 1.000.61
Interface reconstruction
Mixed Youngs-centered method(by Aulisa 2007)(by Aulisa, 2007)
Advection scheme Split Lagrangian-explicit scheme (by Gueyffier 1999)(by Gueyffier 1999)
Surface tension Continuum Surface Force Model
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Start
Set up
Time increment
Start
Fluids interface
Advection term,Viscous term
VOF StepFluids interfacecapturing phaseAdvection of VOF
VOF Step
Prediction of fluid velocity
Degitize interface(volumetoric fraction)
Interactionphase
Momentum exchange
Solve momentum eq. Solid phaseIBM Step
Solve poisson eq.C ti St
Update of displacement
Correction Step
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37.8D
D
w t
Periodic
12.6
D
Inle
t flo
w
Out
let
Re=200
x
y 6.3D Periodic
N i l diti
Computational domainSt
Numerical conditions
Re
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axis
n out
let
on
rm in
let
cond
ition
nvec
tive
ow
con
ditioa
b
Fixed particleU
nifo
rflo
w c
Con
flow
Ellipticity
Free slip condition
p y
Reynolds number y
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L w
Dp
Re=100, Dp/Dx=10
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Numerical conditionsgas
liquid
Free slip condition
particle
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A floating object A floating object g jg j
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IB-VOF coupling method for three-phase flow◦ Validated by comparison with other solutions◦ Applicability for non-spherical objects◦ Capability for large scale simulation involving multiple◦ Capability for large-scale simulation involving multiple
dispersed-phases