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Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved. 1 Benefits of CFD in Modeling Solids Suspension in Stirred Vessels Lanre Oshinowo, André Bakker, Liz Marshall, Ahmad Haidari Fluent Inc., Lebanon, NH, USA Session 174: Computational Fluid Mixing 2000 AIChE Annual Meeting "Exchanging Ideas for Innovation” Los Angeles, California, November 12-17 Paper 174h

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Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.1

Benefits of CFD in Modeling SolidsSuspension in Stirred Vessels

Lanre Oshinowo, André Bakker, Liz Marshall, Ahmad HaidariFluent Inc., Lebanon, NH, USA

Session 174: Computational Fluid Mixing2000 AIChE Annual Meeting

"Exchanging Ideas for Innovation”Los Angeles, California, November 12-17

Paper 174h

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.2

Overview

• Solids suspension processes• Just-suspended speed• Modeling solids suspension using CFD

w Velocity distributionw Solids distribution

• Criteria for scale up

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.3

Suspending Solids

• Mechanical agitation is widely used in process industryoperations involving solid-liquid flows

• The typical process requirement is for the solid phaseto be suspended:w dissolution, reaction, feed uniformity

• The challenge is in understanding the fluid dynamicsin the vessel and relating this knowledge to design

• CFD modeling can provide insight to both themultiphase transport and the design parameters

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.4

Suspending Solids (2)

• The motivation of this study is to:w Elucidate the criteria of minimum suspension speed and

it’s prediction using CFDw Validate the CFD predictions of solids distribution with

experimental dataw Evaluate scale-up criteria for stirred tanks suspending

solids

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.5

Just-Suspended Speed

• NJS is the estimated speed when particle reside on thetank bottom for no longer than 1-2 secondsw Criteria of NJS is subjectivew Experiments typically performed in transparent bottom

vesselsw Acoustic methods have been used to measure the

amount of solids on tank bottom

• What does mean NJS fundamentally?w Is the just-suspended condition adequate?w This does not determine complete dispersion and

particles may be segregated in the bottom of a tall tank

• Is NJS related to the distribution of the solids?

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.6

Example of Just-Suspended Speed• All three systems are operating at NJS (Bakker et al, 1996)

• Designing based on only NJS or on power draw does notnecessarily lead to an optimum design

• The impeller system has to be designed to provide theoptimum flow pattern for the suspension duty

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.7

Estimating Just-Suspended Speed

• Numerous correlation's exist for Njs: Zwietering (1958),Chemineer (Myers et al, 1994), BHR/FMP

• Many recent Njs correlation's have extended theZwietering correlation to include D/T and C/Tw Armenante et al (1998), Penney et al (1999)

• Most correlation's are developed for low viscosityliquids, free-settling solids, low solids loading (<40%),and non-adhesive or non-coagulating solids

• Some of correlation's were developed with a narrowrange of impeller blade styles, sizes and position in thelab scale tank

• The large variability in predicting Njs may or may notbe acceptable

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.8

Power per Unit Volume

• Scale up criteria based on power per unit volume hasdivergent results depending on the correlation used

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.9

Needs from Modeling

• Prediction of NJS

• Solids distributionw Cloud heightw Amount of solids unsuspended

• Scaleup• Other transport phenomena

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.10

Modeling Granular Flows

• Lagrangian models• Drift Flux models• Algebraic Slip Mixture models• Granular Eulerian models

w Granular Viscosity model (Syamlal & O’Brien, 1986)w Exchange coefficient (Di Felice et al, 199)w Restitution Coefficients (Inelastic collisions)w Dispersed Turbulence modeling

• 2D axisymmetric with swirl correction, 3D• Impeller modeling (Implicit and Explicit)

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.11

Modeling NJS

• Should CFD be used to predict NJS ?w Requires optimization of design and operating conditions

Ø Vary D/T, C/T, N

w What mathematical criteria can describe analysis of“particles remaining on the tank bottom for 1-2 seconds”

w Can be expensive (3D, sliding mesh, Granular EulerianMultiphase models)

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.12

Modeling Suspension Distribution

• CFD has most immediate benefit from the prediction ofthe solids distributionw just-suspension distributionw fully-suspended distribution

• Concept of “Quality of Suspension”w Forti et al (2000; 50th Can. Chem. Eng. Conf.)w Degree of suspension σ related to the Froude number

and impeller clearance

ÈUniform suspension: σ < 0.2È Just-suspended condition: 0.2 < σ < 0.8Ê Incomplete suspension: σ > 0.8

( )

ρ∆ρ

=

−=σ ∑ T

Cgd

DNf

CC

n p

n

AV

222

1

11

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.13

Modeling Suspension Distribution

0.0

0.2

0.4

0.6

0.8

1.0

1.2

1.4

0 1000 2000 3000 4000 5000

σ < 0.2 homogeneous0.2< σ <0.8 complete suspension σ > 0.8 decantation

σ

( ){ }TCFrf

Forti et al (2000; 50th Can. Chem. Eng. Conf.)

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.14

Two-Phase Velocity Distribution

• Experimental study by Guiraud et al, “Localmeasurements of …”, Chem. Eng. J.,v.68, p.75 (1997)

• Geometry• 3 blade Mixel prop• D/T = 0.47• C = T/3• N = 5.1 rps• T = H = 0.3 m• w = 5 x 10-3 m• dshaft = 25 x 10-3 m

• Propertiesl Solids

l ρ = 2230 kg/m3

l d50 = 253 µml Cav = 0.5%

l Liquidl ρ = 1000 kg/m3

l µ = 1cp

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.15

Flow Field Distribution

Velocity Magnitude (0 - 0.85 m/s) Solids Volume Fraction (0 - 0.025)

σ = 0.57

N = 306 rpm > NJSz = 160 rpm

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.16

-0.5

-0.4

-0.3

-0.2

-0.1

0

0.1

0.2

0.3

-1 -0.5 0 0.5 1 1.5 2

Axial Position, Z/D

Axi

al V

eloc

ity,

-U

ND

Expt.-solids

Expt.-Cont. Phase

Expt.Liquid only

solids

cont. phase

Liquid-only

Single & Two-Phase Velocity Profiles

r/D = 0.464im

peller

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.17

-0.5

-0.4

-0.3

-0.2

-0.1

0

0.1

0.2

0.3

-1 -0.5 0 0.5 1 1.5 2

Axial Position, Z/D

Axi

al V

elo

city

, -U

/ πN

DExpt.-solidsExpt.-Cont. PhaseExpt.Liquid onlyLiquid-onlycont. phasesolids

Single & Two-Phase Velocity Profiles

r/D = 0.961im

peller

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.18

Axial Solids Concentration Profiles

• Godfrey & Zhu, “Measurement of Particle-LiquidProfiles in Agitated Tanks”, AIChE Symp. Series, No.299, Vol. 90

• Geometry• 4PBT45°• D = T/3• C = T/5• N = 1000, 1600 rpm• T = H = 0.154 m• w = T/10D

• Propertiesl Solids

l ρ = 2480 kg/m3

l d50 = 390µml Liquid

l ρ = 1096 kg/m3

l µ = 1.76 cp

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.19

Axial Solids Concentration Profiles

• Flow fieldw N = 1000 rpm; Avg. vol. conc = 12%, dp = 390 µm

Velocity Magnitude (0 - 0.95 m/s) Solids Volume Fraction (0 - 0.4)

σ = 0.87

NJSChemineer = 780 rpm < N = 1000 rpm < NJS

Zwietering = 1170 rpm

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.20

Effect of Agitation Speed

Average concentration = 12%Particle Size = 390 µm

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

0 1 2 3 4

X

Z

N=1000rpm (Expt.,Godfrey&Zhu)

N=1600rpm (Expt.,Godfrey&Zhu)

N=1000rpm; 2D(80x40)

N=1000rpm; 3D(48x30x70)

N=1600rpm; 2D(160x80)

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.21

Effect of Particle Diameter

Average concentration = 12%Impeller speed = 1000 rpm

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

0 1 2 3 4X

Z

dp=0.39mm (Expt.,Godfrey&Zhu)

dp=0.231mm (Expt.,Godfrey&Zhu)

dp=0.39mm; 2D(80x40)

dp=0.39mm; 3D(48x30x70)

dp=0.231mm; 2D(80x40)

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.22

Cloud Height Analysis

• Suspensionexperiments (Bakkeret al, 1996)w Instantaneous

• CFDw Time-averagedw Cloud height

(volume fraction ofsolids < 0.25%)

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.23

Correlation between StreamLines/Tubes and Cloud Height (1/3)

• N = 1600 rpm• CAV = 12%• dp = 390 µm• NJS

z = 1170 rpml σ = 0.28

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.24

Correlation between StreamLines/Tubes and Cloud Height (2/3)

• N = 1000 rpm• CAV = 12%• dp = 231 µm• NJS

z = 1050 rpml σ = 0.15

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.25

Correlation between StreamLines/Tubes and Cloud Height (3/3)

• N = 1000 rpm• CAV = 12%• dp = 390 µm• NJS

z = 1170 rpml σ = 0.87

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.26

Scale-Up

• Use literature correlation's to predict NJS for differentscales to give ball-park number

• Possible scale up criteriaw NJS, Fr(C/T), ...

• P/V scale up criteria not consistent• Run CFD calculation on design as confirmation

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.27

Scale-Up

• Scale-up Godfrey & Zhu case by factor of 6.5w Zwietering NJS

Ø Scale x 1 = 1170 rpmØ Scale x 6.5 = 236 rpm

w Quality of SuspensionØ Scale x 1, N = 1000 rpm (Godfrey & Zhu), σ = 0.86Ø Scale x 6.5, N = 236 rpm, σ = 0.72

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.28

Scale-Up (2)

Solids Volume Fraction (0 - 0.4)

σ = 0.87 σ = 0.72X 6.5X 1

Animation

Paper 174h. AIChE 2000 Annual Meeting Copyright 2000 Fluent Inc. All rights reserved.29

Conclusions

• CFD can be used to model solids suspension inagitated vessels

• The velocity field and solids distribution compared verywell with experimental data

• Standard deviation of solids volume fraction can beused to confirm the quality of suspension

• Process design and analysis can be rapidly performed:w Scale geometryw Modify tank geometry, baffling and draft tubesw Evaluate agitator performance rapidly