Argon Injection Optimization in Continuous Slab Casting

Similar documents
Effect of Argon Gas Distribution on Fluid Flow in the Mold Using Time-Averaged k-ε Models

Argon Injection Optimization in Continuous Slab Casting

ANNUAL REPORT UIUC, August 16, Bubble Formation, Breakup and Coalescence in Stopper-rod Nozzle Flow and Effect on Multiphase Mold Flow

CCC Annual Report. UIUC, August 14, Gas Flow Through Upper Tundish Nozzle Refractory and Bubble Size Evolution Inside SEN

Transient Turbulent Flow Simulation with Water Model Validation and Application to Slide Gate Dithering

Asymmetric Multi-phase Fluid Flow and Particle Entrapment in a Continuous Casting Mold

Model of Gas Flow through Upper Tundish Nozzle Refractory and Initial Bubble Size

Numerical Simulations of a Train of Air Bubbles Rising Through Stagnant Water

CCC Annual Report. UIUC, August 19, Particle Capture in Mold including Effect of Subsurface Hooks. Kai Jin

Simulation of Gas Holdup in a Bubble Column with a Draft Tube for Gas Dispersion into an Annulus

Workshop 1: Bubbly Flow in a Rectangular Bubble Column. Multiphase Flow Modeling In ANSYS CFX Release ANSYS, Inc. WS1-1 Release 14.

PHYS 101 Previous Exam Problems

Model of Gas Flow through Porous Refractory Applied to An Upper Tundish Nozzle. Rui Liu and Brian G. Thomas

Metallurgical and Materials Transactions B, Vol. 32B, No. 6, 2001, pp BUBBLE FORMATION DURING HORIZONTAL GAS INJECTION

Submitted to Metallurgical and Materials Transactions B, on May 26, BUBBLE FORMATION DURING HORIZONTAL GAS INJECTION

Air Bubble Defects in Dispensing Nanoimprint Lithography

Old-Exam.Questions-Ch-14 T072 T071

IRONARC; a New Method for Energy Efficient Production of Iron Using Plasma Generators

Chapter 15 Fluid. Density

AIRFLOW GENERATION IN A TUNNEL USING A SACCARDO VENTILATION SYSTEM AGAINST THE BUOYANCY EFFECT PRODUCED BY A FIRE

A Computational Assessment of Gas Jets in a Bubbly Co-Flow 1

MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING 2.06 Fluid Dynamics

Questions. theonlinephysicstutor.com. facebook.com/theonlinephysicstutor. Name: Edexcel Drag Viscosity. Questions. Date: Time: Total marks available:

. In an elevator accelerating upward (A) both the elevator accelerating upward (B) the first is equations are valid

Numerical Investigation of Air Bubbles Evolution and Coalescence from Submerged Orifices Based on OpenFOAM

Numerical Analysis of Two Phase Flow Patterns in Vertical and Horizontal Pipes

ANALYSIS OF HEAT TRANSFER THROUGH EXTERNAL FINS USING CFD TOOL

Applications of Bernoulli s principle. Principle states that areas with faster moving fluids will experience less pressure

Tutorial. BOSfluids. Relief valve

Numerical simulation of an intermediate sized bubble rising in a vertical pipe

Free Surface Flow Simulation with ACUSIM in the Water Industry

Lecture Outline Chapter 15. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Enter your parameter set number (1-27)

This file was downloaded from Telemark Open Research Archive TEORA -

! =! [4 (2) ! n] 16 th Australasian Fluid Mechanics Conference Crown Plaza, Gold Coast, Australia 2-7 December 2007

ON THE EFFECT OF LIFT FORCES IN BUBBLE PLUMES

1. Air is blown through a pipe AB at a rate of 15 litre per minute. The cross-sectional area of broad

Irrigation &Hydraulics Department lb / ft to kg/lit.

Physics P201 D. Baxter/R. Heinz

Types of Forces. Pressure Buoyant Force Friction Normal Force

AP B Fluids Practice Problems. Multiple Choice. Slide 2 / 43. Slide 1 / 43. Slide 4 / 43. Slide 3 / 43. Slide 6 / 43. Slide 5 / 43

Simulation of Free Surface Flows with Surface Tension with ANSYS CFX

Slide 5 / What is the difference between the pressure on the bottom of a pool and the pressure on the water surface? A ρgh B ρg/h C ρ/gh D gh/ρ

MODELING AND SIMULATION OF VALVE COEFFICIENTS AND CAVITATION CHARACTERISTICS IN A BALL VALVE

Chapter 15 Fluids. Copyright 2010 Pearson Education, Inc.

Experimental Studies on the Instabilities of Viscous Fingering in a Hele-Shaw Cell

Homework #10 Due Monday, May Compute the moment of inertia of the objects below.

Modeling Turbulent Entrainment of Air at a Free Surface C.W. Hirt 5/24/12 Flow Science, Inc.

Experimental study on path instability of rising bubbles

Fluid Flow. Link. Flow» P 1 P 2 Figure 1. Flow Model

Instruction Manual. Pipe Friction Training Panel

Student name: + is valid for C =. The vorticity

Energy and mass transfer in gas-liquid reactors.

HiPerMax LuK tooth chain for transmissions Reliable Power Flow in the Drive Train

Study on the Influencing Factors of Gas Mixing Length in Nitrogen Displacement of Gas Pipeline Kun Huang 1,a Yan Xian 2,b Kunrong Shen 3,c

CFD SIMULATIONS IN AN INTERNAL CIRCULATION AIRLIFT OPERATING UNDER HOMOGENEOUS REGIME

Experimental study on the gas tightness of a mined cavern with groundwater

CONSIDERATION OF DENSITY VARIATIONS IN THE DESIGN OF A VENTILATION SYSTEM FOR ROAD TUNNELS

Modelling Shrouded Supersonic Jets in Metallurgical Reactor Vessels

PHYSICAL AND MATHEMATICAL MODELLING INVESTIGATIONS OF THE MECHANISMS OF SPLASH GENERATION IN BATH SMELTING FURNACES

IBERIAN SPH 2015 SPH MODELLING FOR AIR ENTRAINMENT IN WAVE BREAKING

A Physical Model for the Two-phase Flow in a Continuous Casting Mold

Experimental investigation on air entrainment below impinging jets by means of video observations and image processing

SUMMARY OF THE EXPERIMENTAL STUDIES OF COLD HELIUM PROPAGATION ALONG A SCALE MODEL OF THE LHC TUNNEL

REFERENCE GUIDE. Rev. 0 15/09/2016

Investigation on 3-D Wing of commercial Aeroplane with Aerofoil NACA 2415 Using CFD Fluent

Tool Weight Analysis An Engineering Approach to Optimize Pressure Temperature and Spinner Data Acquisition

Air Bubble Departure on a Superhydrophobic Surface

COURSE NUMBER: ME 321 Fluid Mechanics I Fluid statics. Course teacher Dr. M. Mahbubur Razzaque Professor Department of Mechanical Engineering BUET

AIR EJECTOR WITH A DIFFUSER THAT INCLUDES BOUNDARY LAYER SUCTION

Single Phase Pressure Drop and Flow Distribution in Brazed Plate Heat Exchangers

A Discrete, Multiphase Flow Approach to Monopropellant-Based Micropropulsion

Snow load on structures: case studies on cableway masts and measures against snow gliding

Vapour pressure of liquids SURFACE TENSION

Chapter 14 Fluids Mass Density Pressure Pressure in a Static Fluid Pascal's Principle Archimedes' Principle

Pressure Drop of Two-Phase Flow Through Horizontal Channel with Smooth Expansion

U S F O S B u o y a n c y And Hydrodynamic M a s s

EDUCTOR. principle of operation

Section 2 Multiphase Flow, Flowing Well Performance

2 Available: 1390/08/02 Date of returning: 1390/08/17 1. A suction cup is used to support a plate of weight as shown in below Figure. For the conditio

ANSWERS TO QUESTIONS IN THE NOTES AUTUMN 2018

Homework of chapter (3)

The Usage of Propeller Tunnels For Higher Efficiency and Lower Vibration. M. Burak Şamşul

3. A fluid is forced through a pipe of changing cross section as shown. In which section would the pressure of the fluid be a minimum?

Effect of Inlet Clearance Gap on the Performance of an Industrial Centrifugal Blower with Parallel Wall Volute

Ermenek Dam and HEPP: Spillway Test & 3D Numeric-Hydraulic Analysis of Jet Collision

CHAPTER 9 Fluids. Units

STATIONARY SPRINKLER IRRIGATION SYSTEM

Concept of Fluid. Density. Pressure: Pressure in a Fluid. Pascal s principle. Buoyancy. Archimede s Principle. Forces on submerged surfaces

FLUID MECHANICS Time: 1 hour (ECE-301) Max. Marks :30

ROSE-HULMAN INSTITUTE OF TECHNOLOGY Department of Mechanical Engineering. Mini-project 3 Tennis ball launcher

Investigation of momentum exchange term closures for the Eulerian-Eulerian model applied to bubbly flows

DRINKING WATER - LAB EXPERIMENTS LAB EXPERIMENTS. Nanofiltration

DNVGL-CP-0187 Edition March 2016

Liquid -Vapor. Contacting columns

Static Fluids. **All simulations and videos required for this package can be found on my website, here:

Effect of the cross sectional shape of the recirculation channel on expulsion of air bubbles from FDBs used in HDD spindle motors

Chapter 13 Fluids. Copyright 2009 Pearson Education, Inc.

Large-eddy simulation of a turbulent buoyant helium plume

Mild steel. Stainless steel. HPR130XD Auto Gas Revision 2. Nozzle retaining cap. tube. Shield cap 30 A 50 A 80 A 130 A

Transcription:

Argon Injection Optimization in Continuous Slab Casting Tiebiao Shi and Brian G. Thomas Department of Mechanical Engineering University of Illinois at Urbana-Champaign March 25, 2001 University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Objectives Develop multiphase computational model to simulate the 3-D flow pattern of molten steel in the continuous casting mold with argon gas injection. Compare and evaluate differences between steel caster and scale water models. Estimate flow pattern (single roll, double roll, etc.) obtained in steel caster as a function of gas injection rate, steel throughput, mold width, and argon bubble size etc. Recommend practices related to argon gas injection optimization to improve steel product quality, especially as related to flow pattern. University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Bubble Size Investigation Water flow direction 35 mm Helium Double-needle experiment schematic 6.35 mm University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Bubble Size Investigation 80 Bubble Volume Percentage (%) 70 60 50 40 30 20 10 case A (55ipm+13SLPM) case B (35ipm+6.3SLPM) 0 0.5 1 1.5 2 2.5 3 4 6 Bubble Size (mm) University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Bubble size in the water model Case A (55ipm + 13 SLPM/ 11% hot gas)

Bubble size in the water model Case B (35ipm + 6.3 SLPM/ 8.5% hot gas)

Bubble Size Investigation 60 Volume percentage (%) 50 40 30 20 case A (55ipm+ 13 SLPM) case B (35ipm+6.3SLPM) 10 0 0.5 1.5 2.5 3.5 4.5 5.5 6.5 7.5 8.5 9.5 10.5 Bubble size (mm) University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Parameters for water model for Case A (55 ipm+11% hot gas) Normal Conditions Enlarged Slide Gate Mold Width W (mm) x Thickness H (mm) 730 x 80 730 x 80 Mold Height (mm) 950 950 Nozzle Submergence Depth 80 80 (top surface to top of port) Nozzle Inner Diameter (mm) 31 31 Nozzle Port Width (mm) x Height (mm) 31 x 31 31 x 31 Jet Angle 30 down 30 down Inlet Jet Spread Angle 0 0 Water Flow Rate Q w (SLPM) 58.59 (15.5 GPM) 76.06 (20.1 GPM) Equivalent Steel Casting Speed (ipm) 54.03 70.14 V c = Qw 04. W 04. H 04. Gas Flow Rate (SLPM, hot volume) 7.43 (15.8 SCFH) 7.43 (15.8 SCFH) Gas Volume Fraction (%) 11.3 8.9 Inlet Velocity, V x (m/s) 0.571 0.724 Inlet Velocity, V z (m/s) 0.330 0.418 Inlet Turbulent Kinetic Energy, K o (m 2 /s 2 ) 0.044 0.044 Inlet Turbulence Dissipation Rate,ε o (m 2 /s 3 ) 0.999 0.999 Water Density (kg/m 3 ) 1000 1000 Water Viscosity (m 2 /s) 1 10-3 1 10-3 Gas Density (kg/m 3 ) 1.20 1.20 Gas Viscosity (m 2 /s) 1.7 10-5 1.7 10-5 Average Bubble Diameter (mm) 2.590 2.590 Volume Fraction of 0.5 mm Bubble (%) 1.07 1.07 Volume Fraction of 1.5 mm Bubble (%) 4.53 4.53 Volume Fraction of 2.5 mm Bubble (%) 31.15 31.15 Volume Fraction of 3.5 mm Bubble (%) 55.83 55.83 Volume Fraction of 4.5 mm Bubble (%) 7.42 7.42 Breakup Coefficient 0.5 0.5 Coalescence Coefficient 0 0

Parameter for water model for Case B (35 ipm+8.5% hot gas) Normal Conditions Enlarged Slide Gate Mold Width W (mm) x Thickness H (mm) 730 x 80 730 x 80 Mold Height (mm) 950 950 Nozzle Submergence Depth 80 80 Nozzle Inner Diameter (mm) 31 31 Nozzle Port Width (mm) x Height (mm) 31 x 31 31 x 31 Water Flow Rate (SLPM) 37.80 (10.0 GPM) 43.64 (11.54 GPM) Equivalent Steel Casting Speed (ipm) 34.86 40.24 = Qw V c 04. W 04. H 04. Gas Flow Rate (SLPM, hot volume) 3.71 (7.9 SCFH) 3.71 (7.9 SCFH) Gas Volume Fraction (%) 8.9 7.8 Inlet Velocity, V x (m/s) 0.358 0.410 Inlet Velocity, V z (m/s) 0.207 0.237 Inlet Turbulent Kinetic Energy (m 2 /s 2 ) 0.044 0.044 Inlet Turbulence Dissipation Rate (m 2 /s 3 ) 0.999 0.999 Water Density (kg/m 3 ) 1000 1000 Water Viscosity (m 2 /s) 1 10-3 1 10-3 Gas Density (kg/m 3 ) 1.20 1.20 Gas Viscosity (m 2 /s) 1.7 10-5 1.7 10-5 Jet Angle 30 down 30 down Inlet Jet Spread Angle 0 0 Average Bubble Diameter (mm) 2.43 2.43 Volume Fraction of 0.5 mm Bubble (%) 4.43 4.43 Volume Fraction of 1.5 mm Bubble (%) 4.90 4.90 Volume Fraction of 2.5 mm Bubble (%) 10.34 10.34 Volume Fraction of 3.5 mm Bubble (%) 8.73 8.73 Volume Fraction of 4.5 mm Bubble (%) 11.60 11.60 Volume Fraction of 5.5 mm Bubble (%) 12.71 12.71 Volume Fraction of 6.5 mm Bubble (%) 0 0 Volume Fraction of 7.5 mm Bubble (%) 0 0 Volume Fraction of 8.5 mm Bubble (%) 0 0 Volume Fraction of 9.5 mm Bubble (%) 21.83 21.83 Volume Fraction of 10.5 mm Bubble (%) 25.46 25.46 Breakup Coefficient 0.1 0.1 Coalescence Coefficient 0 0

0.4m/s Flow Picture of Water Model Simulation Result 0.4m/s PIV Mesurements Comparison of Velocity at centerplane between PIV measurements, simulation and eyeview (55 ipm+13slpm/11% hot gas)

Flow Picture of Water Model (55ipm +11% gas) 0.4 m/s Liquid Velocity Vectors of Modeling (55ipm+11%gas) Comparison of simulation and eyeviews while adjusting liquid level with 15% increase in flow rate Case A (55 ipm + 13 SLPM/11% hot gas)

0.4m/s 0.4m/s Flow Picture of Water Model Simulation Result PIV Mesurements Comparison of velocity at centerplane between PIV measurements, simulation and eyeview (35 ipm+6.5slpm/8.5% hot gas)

Flow Picture of Water Model (35ipm +8.5% gas) 0.4 m/s Liquid Velocity Vectors of Modeling (35ipm+8.5%gas) Comparison of simulation and eyeviews while adjusting liquid level with 15% increase in flow rate Case B (35 ipm + 6.3 SLPM/8.5% hot gas)

Parameters in the real caster modeling Case A (13 SLPM, 55 ipm) Case B (6.3SLPM /13SLPM, 35 ipm) Mold Width Mold Thickness Nozzle Submergence Depth (top surface to top of port) 1854 mm 228 mm 165 mm Nozzle Bore Inner Diameter 78 mm Nozzle Port Height 78 mm Nozzle Port Width 78mm Vertical Velocity in Nozzle 2.05 m/s 1.31 m/s Nominal Vertical Angle of Port Edges 15 down Inlet Jet Spread Angle 0 Casting Speed, V c 23.2 mm/s 14.8 mm/s Liquid Steel Density, ρ l 7020 kg/m 3 Gas Density, ρ gas 0.27 kg/m 3 Steel Laminar (Molecular) Viscosity, µ o 0.00560 kg/m s Gas Vescosity, µ gas 7.42E-5 Surface Tension Coeff. (Steel-Argon) 1.192 N/m Inlet steel flow rate 0.584 m 3 /min 0.376 m 3 /min Throughput (ton/min) 4.10 2.64 Inlet Gas Flow Rate 13 SLPM 6.3SLPM /13 SLPM Inlet Gas Volume Fraction, f gas 11% 8.5% Average Gas Bubble Diameter, D o 2.59 mm 2.43 mm Gravitational Acceleration, g 9.8 m/s 2 *Blank in second column is the same as the first column.

Conditions: 55 ipm 13 SLPM Gate open 58% Velocity at SEN port Centerplane parallel to SEN port Centerplane perpendicular to SEN port Liquid velocity in the nozzle (Case A)

Conditions: 35 ipm 13 SLPM Gate open 50% Velocity at SEN port Centerplane parallel to SEN port Centerplane perpendicular to SEN port Liquid velocity in the nozzle (Case B)

10e-3% 10 mm below Meniscus Casting conditions: 73" slab 55 ipm 13 SLPM 11% Gas (hot) 1m/s 10e-3% 0.1% 10e-3% 0.01% 10e-3% 10 mm from Inner Wide Face Centerplane between Wide Faces 10 mm from Outer Wide Face Steel flow pattern calculated using CFX with distributed bubble size (2.59mm mean)

10 mm below Meniscus 10e-3% 1% 0.1% 10e-3% 0.1% 10e-3% Casting conditions: 73" slab 35 ipm 6.3 SLPM 8.5% Gas (hot) 1m/s 10 mm from Inner Wide Face Centerplane between Wide Faces 10 mm from Outer Wide Face Steel flow pattern calculated using CFX with distributed bubble size(2.43 mm mean)

10 mm below Meniscus 0.1% 10e-3% Casting conditions: 73" slab 35 ipm 13 SLPM 16.4% Gas (hot) 2% 0.1% 10e-3% 2% 1% 0.1% 10e-3% 0.1% 10e-3% 1m/s 10 mm from InnerWide Face Centerplane between Wide Faces 10 mm from Outer Wide Face Steel Flow pattern calculated using CFX with distributed bubble size(2.43 mm mean)

Conditions: 73" slab, 55ipm, 13 SLPM, 11% Gas (hot)) 0.1% 0.1% 1m/s 10e-3% 0.1% 10e-3% 10e-3% Slice at SEN Port Centerplane betwen SEN and NF 10 mm from Narrow Face Steel flow pattern calculated using CFX with distributed bobble size(2.59 mm mean)

Conditions: 73" slab, 35ipm, 6.3 SLPM, 8.5% Gas (hot)) 0.1% 1% 10e-3% 1m/s 10e-3% 0.1% 1% Slice at SEN Port Centerplane betwen SEN and NF 10 mm from Narrow Face Steel flow pattern calculated using CFX with distributed bobble size(2.43 mm mean)

Conditions: 73" slab, 35ipm, 13 SLPM, 16.4% Gas (hot)) 1m/s 0.1% 10e-3% 0.1% 0.1% 10e-4% 0.1% 10e-3% Slice at SEN Port Centerplane betwen SEN and NF 10 mm from Narrow Face Steel flow pattern calculated using CFX with distributed bobble size(2.43 mm mean)

Flow Pattern Identification (Water Model,Modified from M. Assar, P. Dauby and G. Lawson) Gas (hot) percentage (%) 8 6 4 2 Slab Width 73" 63" 50" 40" 0 1 1.5 2 2.5 3 3.5 4 4.5 5 Throughput (ton/min) University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Flow Pattern Identification 30 (Real Caster) Gas (hot) Volume Percentage (%) 25 20 15 10 5 Complex flow pattern zone for 52" slab Complex flow pattern zone for 73" slab 35ipm+6.3SLPM/73" slab (double roll) 35ipm+13SLPM/73" slab (single roll) 55ipm+13SLPM/73" slab (Complex) 40ipm+16SLPM/52" slab (Complex) 0 1 2 3 4 5 6 Throughput (ton/min) 52" slab 73" slab University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Flow Pattern Identification 50 (Real Caster) Gas (cold) Flow Rate (SLPM) 40 30 20 10 Single roll 40" slab 52" slab 63" slab 73" slab Double roll 0 2 2.5 3 3.5 4 4.5 5 Throughput (ton/min) University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Recommendations Do not inject argon into the lowest pressure locations in the nozzle. These low pressure regions will attract large gas flow rates locally, leading to large gas pockets and potential flow instabilities. Ramp the casting speed back up slowly after a ladle change to minimize unstable transient flow. Change submergence gradually and try to arrange for the deeper submergence depths to occur the wider slabs and shallower for narrow slabs. University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Recommendations Optimal argon injection depends on width, casting speed, and submergence depth. Vary argon injection rate with throughput, width, and submergence depth. Keep argon injection below the levels recommended for stable double roll flow. When casting speed drops severely, cut argon to zero or minimal flow rate. Argon should be needed to prevent nozzle clogging due to air aspiration in these conditions; very little gas is needed to maintain a constant gas percentage; and bubble size might grow severely. University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Further Work Further study is recommended using the mathematical models to quantify the conditions which lead to defects and then to fully quantify the flow patterns which lead to safe conditions through subsequent parametric studies. Further study is also needed of gas flow through the refractory relative to pressure drops in the nozzle in order to understand how the gas exits into the nozzle. University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi

Acknowledgements The authors would like to thank: National Science Foundation. Continuous Casting Consortium (CCC) at UIUC. National Center for Supercomputing Applications (NCSA) at the UIUC. AEA technology for use of the CFX 4.2 program LTV Steel, especially Pierre Dauby and Mohammad Assar, for use of the water model and PIV system and access to PIV and MFC measurements. University of Illinois at Urbana-Champaign Metal Process Simulation Lab Tiebiao Shi