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Multiphase CFD: the use of Optimization models and the
importance of full scale in Multiphase Modelling
JosRoberto Nunhez and Collab orato rsFaculty of Chemical Engineering, UNICAMP
State University of Campinas
E-mail: [email protected]
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JosRoberto Nunh ezFaculty of Chemical Engineering,
UNICAMP State University of Campinas
E-mail: [email protected]
Nicolas SpogisESSS South America ANSYS representative
Email: [email protected]
Design of a high efficiently hydrofoil through the use of
computational fluid dynamics and multi-objective optimization
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Solid SuspensionsGet a Lift
In a project completed at UNICAMP in
Brazil, an optimization procedure was
applied to the design of an impeller to
illustrate how this approach can lead tomore efficient mixing processes (and
why not other processes?) in general.
The suspension of solid particles in a
stirred tank was used to illustrate the
methodology.
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ANSYS Advantage
ANSYS Advantageuses real examples.
How engineers,analysts and designerscan use CFD moreeffectively.
Articles detail howSimulation DrivenProduct Developmentcan reducedevelopment time,prototype testing and
time-to-market; andultimately helpcompanies win the racein product innovation.
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AIChE Journal
AIChE J, V55, issue 7,pp17231735, 2009
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Optimization
Microdigital1983
29 years
PGQE + L-CFD alone
have in their labs 520
cores with aproximatly 30
TFLOPs capacity;
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Optimization
1950 A6000
LIGHTNIN Mixers - 1994
44 years
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Design of a high efficiently hydrofoil:
Pure Axial Flow
Lack of Radial Flow
Torque Reduction Saving Costs
Through the use of: Computational Fluid Dynamics
Multi-Objective Design Optimization
Study Objectives
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Still provide good bottom
mixing when located
2-3 diameters off bottom.
Allows the use of shorter
and smaller diameter shafts
Customer Benefits
Pure Axial Flow
Results in less side force
Lower bending moments
and hence gives
longer life for gear
reducers and shaft seals.
Lack of Radial Flow
Up to 50%
resulting in increase
of the gear reducer life
use of a smaller
gear reducer.
Torque Reduction
Savings in operating costs
combined with first
cost savings
giving the customer
a two-fold benefit.
Saving Costs
Hydrofoil impellers advantages
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CAD and Mesh
Generation
Post Process
CFD Solver
Impeller
Multidisciplinary
Optimization
Impeller optimization steps
Icem Scripts
Batch Scripts
CFX Scripts
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Modeling considerations
Unsteady Navier stokes equations in theirconservation form;
Mass conservation equation;
This work used the Alternate Rotation Model thatsolves numerically the absolute frame velocity
instead of the relative velocity;
The Frozen Rotor model was used in a 120o sector
of the reactor;
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Modeling considerations
The Shear Stress Transport (SST) turbulence modelwas used since it is more accurate and robust for
the prediction of problems involving flow separation;
In order to predict turbulence correctly, it isimportant to have at least a layer of control volumes
capturing the effect of the boundary layer, which is
assessed by the dimensionless variable y+. The
average y+
is about 1 for the SST turbulence model.
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Impeller Process Types
Energy Level Process Type P/V Relation (kW/m)
Low level Weak solid suspensionLow viscosity fluids
0.2 kW/m
Moderately Heat transfer
Gas dispersion
0.6 kW/m
High Level Heavy solid suspension
High gas dispersion
Emulsification
2 kW/m
Higher Level High viscosity fluids
Pasta 4 kW/m
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CalculateNew rotationto keep P/V
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Solve Npsteady state
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Solve P/Vsteady state
Solid Suspensiontransient
Geometry Generation
Mesh Generation
,
Post ProcessNp Nq, Variance, etc
Impeller optimization steps
Input Variables
Output Variables
53.. DN
PNp
35.. NpD
PN
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Input Variables
Parameters Parameter Value
Tank diameter T = 1m
Height of the liquid H= T = 1m
Bottom clearance C=H/4 = 0.25m
H
C
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Input Variables
D/T
R_HD T_HD
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Variable Minimum Value Maximum Value Discrete / Continuum
Impeller diameter 0.4 0.5 Continuum
Root chord 0.1 0.2 Continuum
Tip chord 0.1 0.2 Continuum
Root chord angle 20 degrees(related to rotation axis)
70 degrees(related to rotation axis)
Continuum
Tip chord angle 30 degrees(related to rotation axis)
95 degrees(related to rotation axis)
Continuum
Root profile DAE11, S1223, E387, FX 63-13717 different profiles
Discrete
Tip profile DAE11, S1223, E387, FX 63-137
17 different profiles
Discrete
Input Variables
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Blade ProfilesLow Reynolds Hydrofoil
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Vessel solid concentration
variance
Heavy solid suspension
Pure Axial Flow
Lack of Radial Flow
Pumping effectiveness
Torque Reduction Saving Costs
n
i
i CC
ns
1
22
1
1
p
q
N
N
Pefect
Objective Functions
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A Sobol's algorithm was chosen
to generate an initial population
of 3000 individuals, than 50
individuals was filtered by a D-
Optimal algorithm in order to
reduce the preliminary
investigation computational time.
DOE - Preliminary investigations
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RSM - Response SurfacesSolid Concentration Variance
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RSM - Response SurfacesPumping Effectiveness
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DOEScatter Chart - Preliminary investigations
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Optimization Algorithm
Multi-Objective GeneticAlgorithm (MOGA-II)
MOGAs search method alsohas very interesting aspects:
it allows global solutions to befound
it especially guarantees anactual multi-objectiveoptimization, where the Paretofrontier is defined in the end.
Reproduction operators:
Classical crossover;
Directional crossover;
Mutation;
Selection.
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Pareto Frontier
Dominated Points
Non Dominated Points
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Problems:
Average axial Flow
Average radial flow
High NpTorque
High power consumption
Low solid suspension
Initial Impeller DesignPBT 45
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Solutions:
Pure axial Flow
Lack of radial flow
Low NpTorque
Low power consumption
High solid suspension
Optimized Impeller
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Solutions:Low Hub Separation
Low Tip Vortex
Low Shear
Problems:High Hub Separation
High Tip Vortex
High Shear
Hub and Tip Vortex
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Experimental tests
In the accomplishment of the
experimental tests an agitationsystem was projected that consists:
Vertical Vessel with torospherical
10% bottom;
Sustentation Structure in stainless
steel 316L; Baffles, made use in the interior of
the tank;
SEW Electric Motor - 1,5 kW;
Control panel;
MAGTROL torquimeter TM 300series, accuracy
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Power Number evaluation
6% error
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Solid Suspension
N=290 RPM ->P = 6.09 W N=172 RPM ->P = 6.06 W
N=390 RPM ->P = 10.54 W N=232 RPM ->P = 11.23 W
O
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Optimized Blade Design
S lid S i
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Solid Suspension
O ti i d Bl d D i
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Solid concentration variance wasreduced by 48.5%
Power consumption reduced by84.4%
Pumping effectiveness increasedby 410.2%
When compared to the
performance of a standardpitched blade impeller (45degrees constant Tip ChordAnglePBT45).
Optimized Blade Design
O ti i d Bl d D i P t t 2
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Industrial hydrofoil impellersrequire a higher Power number,compared to the previousimpeller. It should be ideallybetween 0.1 and 0.3
The model was run again using
now another restriction on theoptimization model. We set therestriction Np > 0.2
The model arrived at acompletely different impeller
Optimized Blade DesignPrototype 2Previous impeller
Prototype 2 impeller
O ti i d Bl d D i P t t 2
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Optimized Blade DesignPrototype 2
VELOCITY VELOCITYVECTOR PLOT
O ti i d Bl d D i P t t 2
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Optimized Blade DesignPrototype 2
SOLIDSCONCENTRATION
STREAMLINES
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The Importance of Using Three-Phase 3-D Models in
a Real Scale Simulation of Industrial FCC Risers.
University of Campinas
School of Chemical Engineering
Gabriela Cantarelli Lopes
Email: [email protected]
Leonardo Machado da Rosa
Milton Mori
Email: [email protected]
Waldir Pedro Martignoni
Jos Roberto Nunhez
Email: [email protected]
P bli h d
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Introduction
Published papers
FCC P
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IntroductionWhat is the FCC process and how does it work?
part of the petroleum refining:
FCC Process
Crude oil Distillationresiduum
FCC
converts the heavy fractions into more valuablelighter fractions
FCC P
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Introduction
it is necessary because of the increase on the oil
demand and prices along with the decline of the oil
fields;
large profits result from any further improvement
either in the process, or in the equipments.
Why is the FCC process so important to the refineries?
FCC Process
FCC P
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Introduction
FCC Process
Riser reactor
The need for improvement in the FCC
process calls for advances in:
feed injection technology;
highly active catalysts;
geometric configurations.
FCC Process
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Introduction
Experiments Numerical studies
CFD
Multiphase flows
better understanding of the phenomena;
allows the investigation of ways to
improve the performance of the FCC
process.
FCC Process
FCC Process
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FCC Process
Literature review
models present
varying degrees of
simplifications and
assumptions.
Complete physical model of the FCC riser
reactor (Source: Gao et al., 2001)
Research Objective
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Research Objective
3-Dimensional:test of different geometries
2-Phase 3-Phase
CFD simulations using a sophisticated modeling.
Modeling and Simulation
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Modeling and Simulation
Eulerian - Eulerian - Lagrangian approach;
solidgas liquid
Modeling and Simulation
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Modeling and Simulation
EulerianEulerian:
continuous
Conservation Equations: momentum, mass and energy
3-Phase Model
Momentum transfer: Guidaspow drag model;
Heat transfer: Ranz-Marshall correlation;Turbulence: Reynolds stress model (RSM);
Particle fluctuations: KTGF.
M d li d Si l ti
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Modeling and Simulation
3-Phase Model
Lagrangian:
discrete
droplet is calculated individually
Trajectory: Gravity + Drag force (Morsi-Alexander);
Heat transfer (gas and droplet) : Ranz-Marshall;
Mass transfer (gas and droplet): difference of concentration.
Modeling and Simulation
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Modeling and Simulation
Reactions
4-Lump Model:
The set of cracking reactions are simplified
Modeling and Simulation
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Modeling and Simulation
Setup
Solver: ANSYS FLUENT 12.0;
User-defined functions for heterogeneous
kinetics;
Hexaedrical meshes: 1 million volumes;
Transient simulation: 15 sec. of flow;
16 partitions solved in parallel.
Modeling and Simulation
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Modeling and Simulation
Geometries
L-shape T-shape
Previous studies in cold
setup:
Smooth exits:less
turbulence and solidbackmixing. High wear
by friction.
Abrupt exits:less
maintenance.
Modeling and Simulation
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Modeling and Simulation
Geometries
Modeling and Simulation
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Cases
gas
+
solid
+
liquid
gas
+
solid
Case 2
gas
+
solid
+
liquid
Case 1 Case 3
Modeling and Simulation
Modeling and Simulation
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Modeling and Simulation
Operating conditions
Feed (oil mass flux) 20 kg/s
Catalyst-to-oil ratio 7 kg/kg
Steam 7 wt%
Feed oil temperature 500 K
Catalyst inlet
temperature
900 K (2-
Phase)
960 K (3-Phase)
Droplet diameter 0.1 mm
Results
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Flow characteristics
Average cross-section values
Results
Results
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Results
Vaporization
Max. res. time: 0.2 seconds(Gao et al., 2001)
Results
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Results
Exit shape effects
Case 1 (L-shape exit) Case 3 (T-shape exit)
Solid velocity streamlines
Results
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Results
Case 1 (L-shape exit) Case 3 (T-shape exit)
Exit effects
Height = 32m
Results
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Results
Height = 32m
Exit effects
Results
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Results
Exit effects
Results
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(Ali et al.,
1997)
9%
Results
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Acknowledgements
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Acknowledgements
The students and colleagues mentioned in the
presentation of both works;
Petrobras for the funding of the FCC project;
ESSS for the support on the Optimizationproject;
The organizers of the workshop Trends in
Physical and Numerical Modeling for IndustrialMultiphase Flow for the invitation.
Brain storm
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Brain storm
Do you believe the use of optimization models withCFD is a promising way to improve equipments
performance?;
Since turbulence in multiphase flow is hardly
scalable, and both area/volume ratio and shearstress change both in scaling up/down, do you agree
we should aim at simulating equipments at their real
size?
http://www.cenpra.gov.br/ -
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Thank you!
http://www.cenpra.gov.br/