16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... ·...

17
CCC Annual Report UIUC, August 20, 2014 Department of Mechanical Science & Engineering University of Illinois at Urbana-Champaign Thermal Stress Cracking of Ladle Sliding Gate Plates Hyoung-Jun Lee, Seon-Hyo Kim UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN I L L I N O I S Department of Materials Science & Engineering Pohang University of Science & Technology Brian G. Thomas Doo-Hoa Cheong, Sang-Woo Han, Yong-Hwan Kim Steelmaking Research Group POSCO Technical Research Laboratories University of Illinois at Urbana-Champaign Metals Processing Simulation Lab Hyoung-Jun Lee 2 Research Background (Business Case) A A section A-A Japanese Patent [1] Crack location of reusable ladle plate[2] Longer lifetime of Sliding-Gate is needed JFE and POSCO are developing reusable outer plate technology Research is needed to understand and present cracks in ladle plates

Transcript of 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... ·...

Page 1: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

CCC Annual ReportUIUC, August 20, 2014

Department of Mechanical Science & Engineering

University of Illinois at Urbana-Champaign

Thermal Stress Cracking

of Ladle Sliding Gate PlatesHyoung-Jun Lee, Seon-Hyo Kim

UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN

I L L I N O I S

Department of Materials Science & Engineering

Pohang University of Science & Technology

Brian G. Thomas

Doo-Hoa Cheong, Sang-Woo Han,Yong-Hwan Kim Steelmaking Research Group

POSCO Technical Research Laboratories

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 2

Research Background(Business Case)

A A

section A-A

Japanese Patent [1] Crack location of reusable ladle plate[2]

Longer lifetime of Sliding-Gate is needed JFE and POSCO are developing reusable outer

plate technology Research is needed to understand and present

cracks in ladle plates

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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 3

Research Background(Operation Problems)

ShroudNozzle

Lower Plate

Upper Plate

Ladle Bottom

Why are cracksin sliding-gatea concern?

Schematic of ladle-nozzle system [3]

-Safety Problem (Steel leakage)-Clogging (Air penetration)-Require replacing plate every heat

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 4

Schematic of Ladle-Nozzle Sliding-Gate System (Animation)

Lower plate moves horizontally to control the molten steel flow rate through the nozzle

Springs generate cassette pressure on the ladle plate

Ladle bottom

Uppernozzle

Upper frame

Upper plate

Copperrods

Lowerframe

Connected to hydraulic cylinder

Grease

Lower plate

Sliding frame

Shroudnozzle

Tundishtop

Front view (opening change) Side view (cst. pressure)

Links4 Springs in

each side

6-Bolts

Ceramic sheet

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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 5

Type of Ladle Plate Cracks [4]

Common thru-cracks (every plate breaks in two)

Rare radial crack (~50% of plates)

Top View Bottom View

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 6

Method of Elastic Modulus Calibration by 3-Point Bending Test

Data vs time from bending test at 1200°C, #1

Final load = 6505 NFinal displacement = 1.414 mm

# sec kgf mm

SymmetrySliding platerefractory specimen

Reference pointcoupled to load roll

Support roll

Elastic modulus is adjusted until reaction force on reference point in FEM matches to final load of measurement

Eroll = 206 GPaνroll = 0.3Eref = ??? GPaνref = 0.2

Load roll

Eref = 1.53 GPa

Page 4: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 7

2-D Finite Element Model of3-Point Bending Test

Specimen size : 20*20*80 mmSpan distance : 50 mmRoll diameter : 10 mm

2-D transient modelMesh : 2D plane stressShell thickness : 20 mm

tension

compression1

1

22

Specimen : Hex-solid 13,093Load roll : Hex-solid 614Support roll : Hex-solid 3,100

surf. to surf. contactµref-steel = 0.45

UX, UY = 0

Prescribe displacement (t)Strain rate = 0.5mm/min

Symmetry

X

Y

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 8

3-Point Bending Test Resultsat Different Temperatures

Conditions Replicated Tests1 2 3 4

25 ˚CLoad(N) 2805 2266 1521 1793

Stroke(mm) 0.160 0.117 0.116 0.155

400 ˚CLoad(N) 3474 3630 3205 -

Stroke(mm) 0.909 0.958 0.873 -

800 ˚CLoad(N) 3366 3916 4147 -

Stroke(mm) 0.755 1.085 1.842 -

1200 ˚CLoad(N) 6505 7234 - -

Stroke(mm) 1.414 1.502 - -

1400 ˚CLoad(N) 7005 8165 - -

Stroke(mm) 1.598 1.925 - -

The lowest final load at different temperature test is input to 2-D simulation

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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 9

Load vs. DisplacementMeasurement/Prediction

0.0 0.4 0.8 1.2 1.60

2000

4000

6000

8000

Load

(N

)

Displacement (mm)

25 Degree C - predicted 400 Degree C - predicted 800 Degree C - predicted 1200 Degree C - predicted 1400 Degree C - predicted 25 Degree C - measured 400 Degree C - measured 800 Degree C - measured 1200 Degree C - measured 1400 Degree C - measured

1521 N

3205 N3366 N

6505 N

7005 N

Failure load

Measured and predicted final load/displacement are matched

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 10

Physical Property of Ladle Plate [5](Chosun Refractories Co. Ltd.)

Model CSN-601N, Alumina-Carbon BrickPhysical Properties Value

Apparent Porosity 5~8 %

Bulk Density 3,100~3,200 kg/m3

Cold Crushing Strength 147.15 ≤ MPa

Modulus of Rupture at 1,400˚C 12.74 ≤ MPa

Thermal Expansion at 1,400˚C 0.8~1.0 %

Chemical Composition

Al2O3 72 ~ 76 %

ZrO2 4 ~ 6 %

C 10 ~ 13 %

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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 11

Analytical Solutions of 3-Point Bending Test

Elastic modulusLoad, P

b

h

L

3

3max4static

PLE

bh δ

Max. bending stress

max

My

I

M : Bending momentZ : Modulus of sectionI : Inertia of momenty : Distance between centerline

and top or bottom

max 3 2

342 2

12

PLh PL

bh bh

max

M

Z

IZ

y

3

12

bhI

y

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 12

Elastic Modulus and Critical Tensile Strength Results

Apparent decrease in E with increasing temperature is likely due to creep during test (when temperature exceeds glass transition temperature of ceramic)

Predicted critical tensile strength is taken from FEM simulation at center-bottom of test piece (tension area)

0 400 800 12000

1

2

3

4

5

6

7

Ela

stic

Mod

ulus

(G

Pa)

Temperature (degree C)

2D Finite-element model for E Analytical equation to estimate E

0 400 800 12000

10

20

30

40

50

60

70

Crit

ical

Ten

sile

Str

engt

h (M

Pa)

Temperature (degree C)

Predicted max. tensile stress Analytical max. bending stress

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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 13

0 400 800 1200 1600600

800

1000

1200

1400

Spe

cific

hea

t, C

p (J

/kg-

K)

Temperature (degree C)

Thermal Property Measurements (CSN-601N, Chosun Refractories)

y=-603*exp(-x/560)+1396

Conductivity, k (W/m·K) = density, ρ (kg/m3) * diffusivity, κ (m2/sec) * specific heat, CP (J/kg·K)

0 400 800 1200 1600

1

2

3

4

Diff

usiv

ity (

10-6 m

2 /sec

)

Temperature (degree C)

y=3*exp(-x/263)+1.21

measured

Diffusivity Measurement – KICET (Laser Flash, NETZSCH, LFA457)

Specific Heat Measurement – Ajou Univ. (Differential Scanning Calorimeter, NETZSCH, DSC200F3)

[6]

Density, measured by displacement method – POSCO = 3147.5 kg/m3

Alumina-carbon brick (C=30wt%)

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 14

Thermal Conductivity & Thermal Expansion Coefficient Evaluation

[6] [6]

Alumina-carbon brick (C=10wt%)

Alumina-carbon brickof POSCO ladle plate

Magnesia brick

High-alumina brick (corundum type)

Alumina-carbon brickof POSCO ladle plate

Alumina-carbon brick(C=10wt%)

0 400 800 12000.0

0.4

0.8

1.2

1.6

Temperature (degree C)

The

rmal

Exp

ansi

on (

%)

Measured thermal properties are well matched to reference data[6]

Thermal Expansion Coefficient Measurement – POSCO (Dilatometer, NETZSCH, DIL402C)

0 400 800 1200 16000

2

4

6

8

10

The

rmal

Con

duct

ivity

(W

/m-K

)

Temperature (degree C)

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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 15

Ladle-Nozzle Sliding-Gate Components& Cassette Pressure Calculation

Upperframe

Sliding frame

Upper plate

Lower plateSteel band

Ceramic sheet

Settingblock

Cu sliding rods

*Lower frame is omitted

YX

Z

Stopblock

Bolted under ladle bottom

Spring force = 10,000 kgfCu rod area = 0.035 x 0.890 m

210,000 [kgf] 9.81 [m/s ] 11.57 [MPa]

0.035 [m] 0.890 [m] 2

Sym. model

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 16

Ladle-Nozzle Sliding-GateDomain / Finite Element Mesh

Top view

Front view

Right view

Calculation time : 1.5 hrs. (heat transfer), 30 hrs. (stress)

XY

Z

PartsElements

Hexahedral Wedge

Upper plate - 47,764

Upper band 288 -

Upper ceramic sheet - 901

Upper stop block 3,226 -

Upper setting block 2,520 -

Upper frame 147,983 -

Lower plate - 47,764

Lower band 288 -

Lower ceramic sheet - 901

Lower stop block - 2,495

Lower setting block 1,793 -

Sliding frame 51,328 -

Sliding frame Cu rod 632

Lower frame Cu rod 720

Total elements 308,603

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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 17

Properties forLadle-Nozzle Sliding-Gate Model

Property Value

Refractory(Plate)

Density ρref 3147.5 kg/m3

Elastic modulus Eref Prescribed PaPoisson’s ratio νref 0.2 -Thermal conductivity kref Prescribed W/m·KSpecific heat Cp,ref Prescribed J/kg·°CExpansion coefficient αref Prescribed °C-1

Emissivity [7] εref 0.92 -

Steel(Band,

Cassette)[7]

Density ρsteel 7860 kg/m3

Elastic modulus Esteel 206 х 109 PaPoisson’s ratio νsteel 0.3 -Thermal conductivity ksteel 48.6 W/m·KSpecific heat Cp,steel 418.6 J/kg·°CExpansion coefficient αsteel 1.78 х 10-5 °C-1

Emissivity εsteel 0.75 -

Friction coefficient

Steel-Steel [8] μsteel-steel 0.3 -Steel-Refractory [7] μsteel-ref 0.45 -Refractory-Refractory [7] μref-ref 0.1 -

Stefan-Boltzmann constant σ 5.669 х 10-8 W/m2·K4

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 18

Variables and Boundary Conditions for Ladle Sliding-Gate Model

Preheating Refining Casting

Opening Ratio [4] - 100 0 70 %

Duration Time [4] t 210 160 33 min.

Initial Temperature Tinitial 25 - - °C

Internal Sink Temperature Ti750 [9]

(Gas)340 [10](Ladle filler)

1600(Molten Steel)

°C

Internal Convection Heat Transfer Coefficient (Forced) [9] hi 65.24 8.82 28.7 x 103 W/m2·K

External Ambient

Temperature[9]

Inside of Cassette area To,in 200 200 270 °C

Outside of Cassette area To,out 100 100 120 °C

External Convection Heat Transfer Coefficient (Free) [9] ho 8.82 8.82 8.82 W/m2·K

Lower plate movementwith 25 mm/min.

Surface pressure 10,000 kgfat Cu sliding rod

Page 10: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 19

Thermal Behavior (Movie)

Preheating(750˚C, 210min)

Refining(340˚C, 160min)

Casting(1600˚C, 33min)

1000% 070% End of heat

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 20

Temperature & Hoop Stress Histories at Locations where Cracks are Observed

12 3

4 Inner bore

XY Z

0 100 200 300 400

-2

0

2

4

6

8 1, x-stress 2. x-stress 3, y-stress 4, y-stress

Hoo

p S

tres

s (M

Pa)

Time (min)

0

400

800

1200

1600 inner bore 1 2 3 4

Tem

p. (

degr

ee C

)

Preheating Refining Casting

Zoom-innext slide

Compression preload(spring loading against the link)

Tension

Compression

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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 21

Temperature & Hoop Stress Histories during Casting (Log Scale on x-axis)

12 3

4 Inner bore

XY Z

Max.differenceat #1

Max.differenceat #2, 3, 4

Casting start Casting end

Tension

Compression1E-3 0.01 0.1 1 10

0

2

4

6

8 1, x-stress 2, x-stress 3, y-stress 4, y-stress

Hoo

p S

tres

s (M

Pa)

Time from Casting (min)

0

400

800

1200

1600 inner bore 1 2 3 4

Tem

p. (

degr

ee C

)

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 22

Common Through-thickness Crack Formation Mechanism

X

Y

Growthdirection

Temp.[°C] Stress [MPa]

Crack initiates on outer surface max. (P1 at 5min) Crack grows towards inner bore

260˚C Max at P1:Crack starts

Section view of 10 mm below lower plate top surface, after 5 min of casting

1600˚C

Temp. StressX

StressY

StressZ

Slide frame

Steel band

Stopblock

Settingblock

Lower plate

Critical tensile strength ;~16 MPa at 260˚C

8.6 MPa

Page 12: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 23

Rare Radial Crack Formation Mechanism

230˚C

Not connected to inner bore

Temp. StressX

StressY

StressX

Temp.[°C]

Stress [MPa]X

YView of lower plate, after 0.5 min of casting

StressY

Growth direction

Max at P2,3,4:Crack starts

1600˚C

1600˚C

Temp.

Bottom view Top view

Max. load is generated at 0.5 min of casting Crack starts on convex (colder) lump part of upper or lower plate

Slide frame

Steel band

Stopblock

Settingblock Temp.

X Y

ZCritical tensile strength ;~15.5 MPa at 230˚C

6.2 MPa

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 24

Mechanical Loading Effects

Z

X

Stress [MPa]

Stress X

Highest temperature causes compression against block

Y

X

Stress Y

Stop blockSetting block

Contact area

Misalignment during assembly leads to concentrated point loads at contact points

Temp.Temp.[°C]

Temp. and stress distribution in plates at the end of casting450˚C

240˚C 230˚C

200˚C 215˚C

Z

X

Stress Y

Temp.

Top view of upper plate at the end of casting

Note: steel band expands away from ceramic, leaving ~5mm gap during casting

5 mm

x10 distortion

Page 13: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 25

Casting Result without Preheating (Worst Case)

Direct casting and cooling is simulated without preheating for worst case

12 3

4 Inner bore

XY Z

CoolingCasting

Compression preload(spring loading against the link)

0 50 100 150 200 250 300-4

-2

0

2

4

6 1, x-stress 2, x-stress 3, y-stress 4, y-stress

Hoo

p S

tres

s (M

Pa)

Time (min)

0

400

800

1200

1600 inner bore 1 2 3 4

Tem

p. (

degr

ee C

)

0.1 1 10

-2

0

2

4

6

Hoo

p S

tres

s (M

Pa)

Time from casting (min)

Zoom-in during casting

Tension

Compression

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 26

Thermal/Mechanical Distortion Affected by Cassette Pressure

Cassette is plastically deformed after several times using for casting according to plant engineer – Deformation shape effects of plate in the plant will be discussed in future work

Casting (1600˚C,33min) Cooling(25˚C, 270min)

End of cooling

Stress histories, x 10 distortion

End of heat

Compression preload

Front view - symmetric plane, XZ(Stress X)

Right mirror view (Stress Y)

Stress X [MPa] Stress Y [MPa]

Page 14: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 27

Future Works

Ladle bottom

DistortionBolt distortion?

Cracks?

Plastic deformation of used cassette in the plant is needed to investigate

Thermal and mechanical distortion of ladle-nozzle system pushes against upper nozzle, creating forces between upper nozzle and ladle bottom refractory

Creep effect in ceramic materials is important for cracking

Uppernozzle

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 28

Reusable Ladle-Nozzle Sliding-GateDomain / Finite Element Mesh

Lower plate innerLower plate outer

XY

Z

PartElements

Hexahedral Wedge

Upper plate - 49,452

Upper band 288 -

Upper Ceramic sheet - 897

Upper stop block 1,729 -

Upper setting block 2,749 -

Upper frame 146,671 -

Lower Plate

Inner - 5,673

Outer - 31,150

Lower band 288 -

Lower ceramic sheet - 897

Lower stop block - 1,729

Lower setting block 2,749 -

Sliding frame 59,164 -

Sliding frame Cu rod 632

Lower frame Cu rod 2,664

Total elements 306,732

Page 15: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 29

Reusable Lower PlateDomain / Finite Element Mesh

Lower plate bottom surface

XY

Z

Lower plate inner

Lower plate outer

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 30

0

500

1000

1500

Tem

p. (

degr

ee C

) inner bore conventional reusable inner reusable outer

Stress [MPa]

Hoop Stress Results Comparison(Conventional / Reusable)

Larger temperature difference between inside and outside surfaces generates larger tensile stress

Tensile stress can be reduced by using outer “reusable” plate

Casting start

ConventionalStress

XStress

X

8.5 MPa

6.45.3

X

Y

Inner crack starts

Outercrack starts

Crack starts

Section view of 10 mm below lower plate top surface, after 5 min of casting

Casting end

Max.difference

TensionCompression

StressY

Reusable

1E-3 0.01 0.1 1 10-2

0

2

4

6

8

Hoo

p S

tres

s (M

Pa)

Time from casting (min)

conventional reusable inner, x-stress reusable outer, x-stress

Growth direction

Growth direction

Growth direction

Page 16: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 31

Stress [MPa]

Reusable Lower Plate Outer Crack Formation Mechanism

Crack locations after once use [2]

X

Y

StressX

StressY

Crack locations are well matched to used plate In addition to same common crack mechanism:

Expansion of inner plate causes tension in reusable outer plate

x20distorted

Top view of reusable lower plate top surface, after 5 min of casting

Growthdirection

Crack starts

Inner expansion

1

2

1E-3 0.01 0.1 1 10-2

0

2

4

6

8

10

Hoo

p st

ress

(M

Pa)

Time from casting (min)

1, x-stress 2, x-stress

TensionCompression

9.4 MPa

5.3 MPa

Casting start Casting end

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 32

Conclusions

Replicated 3-point bending tests measured refractory strengths at different temps.

Thermal expansion of hot inside of plate causes exterior tensile hoop stress and crack growth towards interior: leading to both common through thickness cracks (starting at cold outside of plate) and rare radial cracks (starting at cold outside of lump).

No cracks are predicted (so quantitative models and fracture criteria need more work.

Reusable plate are predicted to reduce tensile hoop stress, but through-thickness crack formation may be unavoidable.

Two different crack mechanisms can form through-thickness cracks in reusable outer plate middle.

Page 17: 16 LEE-HJ Sliding Gate Crackingccc.illinois.edu/s/2014_Presentations/15_LEE-HJ__Sliding... · University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 33

Acknowledgments

• Continuous Casting Consortium Members(ABB, ArcelorMittal, Baosteel, MagnesitaRefractories, Nippon Steel and Sumitomo Metal Corp., Nucor Steel, Postech/ Posco, Severstal, SSAB, Tata Steel, ANSYS/ Fluent)

• Others - Chosun Refractories Co. Ltd.- Daejoo Machinery Co. Ltd.- POSCO Grant # 4.0009576.01

University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Hyoung-Jun Lee • 34

References

[1] Japanese Patent, JP2012-121049A, 2012.6.28

[2] T. Hisanaga, et al., Japanese Journal of Refractories, No.1, pp.26, 2012

[3] J. Choi, POSCO Gwangyang works, Gwangyang, Jeonnam, Korea

[4] D.H. Jeong, et al.. POSCO Technical Research Lab., Pohang, Gyeungbuk, Korea, 2013

[5] Technical Data, Chosun Refractories Co. Ltd., http://www.chosunref.co.kr/home/kor/product/ndata/

[6] T.G. Kyokai, Refractories Handbook, The Technical Association of Refractories, Japan, June, 1998

[7] J.M. Sun, et al., Chosun Refractories Co. Ltd. Research Center, Pohang, Gyeongbuk, Korea, 2010

[8] B.G. Thomas, et al., Iron and steel maker, Vol.25, pp.125, 1998

[9] H.J. Lee, et al., “Thermal Stress Cracking of Sliding Gate Plates”, AISTech proceeding, 2012

[10] S.S. Kim, et al., Journal of Ceramic Society, Vol.38, No.9, pp.829, 2001