12 hibbeler mold taper measurements -...
TRANSCRIPT
CCC Annual ReportUIUC, August 14, 2013
Lance C. HibbelerPh.D. Student and Lecturer
Department of Mechanical Science & Engineering
University of Illinois at Urbana-Champaign
Modeling and On-Line Measurements
of Narrow Face Mold Taper
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 2
Introduction
• Narrow face mold taper has been measured online
with inclinometers at Tata Steel IJmuiden
– Funnel-mold thin slab caster
• Modeling of thermomechanical behavior of mold
has been able to match steady-state
measurements of taper
• This work focuses on the behavior of the narrow
face mold during startup
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 3
Funnel Mold Geometry
90136.8 top106 bottom
OuterFlat
InnerCurve
OuterCurve
InnerFlat
InnerCurve
OuterCurve
OuterFlat
260
750
1200 (Variable)
23.4 top8 bottom
All dimensions
in mm
• Cu-Cr-Zr alloy– 350 W/(m·K) thermal conductivity– 8900 kg/m³ mass density– 385 J/(kg·K) specific heat capacity– 117 GPa Young’s modulus, 0.181 Poisson’s ratio
• No coating layers
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 4
Water Channel Geometry
72
90
Hot Face
Therm
ocouple
Hole
Water
Tube
Bolt Hole
21.3
23.7
10.5 20
510
15
35
Hot Face
Wate
r
Channel
Copper Backing Plate
Copper Mold
Bolt
Hole
Sym
metry
Narrow face Wide face
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 5
Waterbox Geometry
• 316 stainless
– 200 GPa Young’s modulus
– 0.3 Poisson’s ratio
All dimensions
in mm
50 50
695
145
685
895
230
212.5 212.5 212.5 212.5 255 260
125
125
125
125
125
125
125
125
75
210
20
20
20
155
50
3030
3072
1100
850
2060
1105
930
1365
50
400
80
Clamping Force
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 6
Finite-Element Mesh
Part Nodes Elements
Wide Face Mold Plate 855,235 4,223,072
Wide Face Water Box 185,534 190,457
Narrow Face Mold Plate 233,931 495,566
Narrow Face Water Box 83,269 239,604
Bolts and Tie Rods 110 55
Total 1,358,081 5,148,754
Thermal DOF = 1,089,166
Mechanical DOF = 4,830,081
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 7
Thermal Boundary Conditions
• Specified heat flux on mold hot faces
• Convection BC on water channels
• All other faces thermally insulated
• Values calculated from CON1D calibrated to plant measurements [Santillana et al., ISIJ Int. 2008]
0
100
200
300
400
500
600
700
800
900
1000
1100
0 1 2 3 4 5 6 7 8 9
Heat Flux (MW/m²)
Dis
tan
ce B
elo
w T
op
of
Mo
ld (
mm
)
WFNF
Meniscus
33 37 41 45 49 53 57
Convection Coefficient (kW/m²·K)
WFNF
Meniscus
32 34 36 38 40 42 44 46
Water Temperature (ºC)
0
100
200
300
400
500
600
700
800
900
1000
1100
Dis
tan
ce B
elo
w T
op
of M
old
(mm
)
WFNF
Meniscus
spk T− ∇ ⋅ = ⋅n q n
( )k T h T T∞
− ∇ ⋅ = −n
0k T− ∇ ⋅ =n
Qmeas = 2.8 MW/m²Qcalc = 2.7 MW/m²
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 8
Mechanical Boundary Conditions
• Ferrostatic pressure on hot faces
• Symmetry on appropriate planes– Wide face mold and waterbox centerline
– Narrow face mold and waterbox centerline
– Tie rod centerlines
• Mechanical contact on mating faces– “Hard” contact algorithm within ABAQUS
– Copper-copper coefficient of static friction µ = 1.0 [-]
– Copper-steel coefficient of static friction µ = 0.5 [-]
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 9
Mold Bolts and Tie Rods
• Bolts modeled as truss elements and prestressed according to plant practice– See [Thomas et al., Iron and
Steelmaker 1998]
• “Distributing coupling constraints” tie bolt ends to surfaces on mold pieces
• Simulated tie rods account for actual tie rods and spring packs
Narrow Face
Waterbox
Narrow
Face Mold
Truss
Element
Reference
Points
Distributing
Coupling
Constraints
Bolt Length (mm)
Cross-Sectional Area (mm²)
Applied Torque (N·m)
Pre-Load (kN)
Pre-Stress (MPa)
Stiffness (MN/m)
NF (Short) 150 181 100 30 168 240
WF Short 87 187 100 30 162 424
WF Long 449 143 100 30 212 63
Upper Tie Rod 1335 1215 -- 40 33 34.8
Lower Tie Rod 1335 1215 -- 70 58 33.4
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 10
Steady-State Simulation Results
• Heat transfer: 12 minutes on 8-core 2.66 GHz Intel Xeon
• Stress analysis: 44.6 days on 8-core 2.66 GHz Intel Xeon
• Marched through pseudo-time to get a solution
50× scaled distortion
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 11
Thermocouple ValidationCorrected for Wire Convection
17
5 m
m125 m
m125 m
m125 m
m125 m
m125 m
m125 m
m125 m
m
239210
212.5 mm212.5 mm212.5 mm
Outer
Flat
Outer
Curve
Inner
Curve
Inner
Flat
W W W
W W W
A A A
A A A
A A A
A A A
A A A
A A A
227258
220209
48--
185173
177154
161163
46--
166150
160148
145154
46--
155150
151130
138144
46--
148154
144140
131145
47--
154152
150154
138150
48--
152151
151144
143151
48--
197194
199185
196186
64--
21
5 m
m1
34
mm
13
4 m
m1
34
mm
13
4 m
m1
34
mm
13
4 m
m
X
Z
Y
ZW
W
W
W
W
W
W
199191
160160
147155
137148
141149
147145
150132
Tcalculated (ºC)
Tmeasured (ºC)
NF WF
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 12
Cooling Near Mold Exit
Hot face heats up as channels curve away
Hot face stays relatively cool with straight water tubes
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 13
Wide Face Temperatures
0
50
100
150
200
250
300
350
400
0 50 100 150 200 250 300 350 400 450 500 550 600 650 700
Distance from Centerline (mm)
Wid
e F
ace H
ot
Face T
em
pera
ture
(°C
) .
Inner Flat Inner Curve Outer Curve Outer Flat
z = 1050 mm
z = 850 mm
z = 650 mm
z = 416 mm
z = 251 mm
z = 152 mm
z = 100 mm
Bolt
Colu
mn
Bolt
Colu
mn B
olt
Colu
mn
Mold
Level
Sensor
Bolt
Colu
mn
Slight 2D heat transfer in funnel region (less than 2 ºC), but change in cooling around bolts is more significant
Large change in cooling near mold
exit
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 14
Wide Face Mold Distortion
50× scaled distortion
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 15
Wide Face Mold Distortion
Out-of-Plane Behavior
Ou
ter
Fla
t
Ou
ter
Cu
rve
Inn
er
Cu
rve
Inn
er
Fla
t
Short
120
98
137
137
299
863
158
181
157
549
137
18
57
52
225
X
Z
Bolt Stress
in MPa
10720219
102
24
13
23
87
13619418565
12815815841
242
277116 81
31
60
79
78
68
54
35
13
7Long
212.5 mm212.5 mm212.5 mm
50 m
m175 m
m125 m
m125 m
m125 m
m125 m
m125 m
m125 m
m125 m
m
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 16
Wide Face Mold Distortion
Out-of-Plane Behavior
-0.5
-0.4
-0.3
-0.2
-0.1
0
0.1
0.2
0.3
0.4
0.5
0 50 100 150 200 250 300 350 400 450 500 550 600 650 700
Distance from Centerline (mm)
Wid
e F
ace H
ot
Face D
isp
lacem
en
t (m
m)
.
Inner Flat Inner Curve Outer Curve Outer Flat
z = 1050 mm
z = 850 mm
z = 650 mm
z = 416 mm
z = 251 mm z = 152 mm
z = 100 mm
Bolt
Colu
mn
Bolt
Colu
mn
Bolt
Colu
mn
Mold
Level
Sensor
Bolt
Colu
mn
SEN
Waterbox
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 17
Wide Face Mold Distortion
Behavior at Centerline
0
100
200
300
400
500
600
700
800
900
1000
1100
0 50 100 150 200 250 300 350 400 450
Temperature (ºC)
Dis
tan
ce B
elo
w T
op
of
Mo
ld (
mm
)
-0.5 -0.4 -0.3 -0.2 -0.1 0 0.1 0.2 0.3 0.4 0.5
Displacement (mm)
Wide Face
Centerline
SEN Waterbox
Temperature Displacement
Meniscus
Bolt
Bolt
Bolt
Bolt
Bolt
Bolt
Bolt
Bolt
Bolt
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 18
Wide Face Mold Distortion
In-Plane Behavior – Towards NF
0.77
0.80
0.81
0.85
0.90
0.44
0.52
0.55
0.59
0.65
0.00
0.00
0.00
0.00
0.00
Short
X
Z
Long
0.000.400.72
0.43
0.38
0.35
0.35
0.38
0.000.410.761.01
0.000.470.941.27
0.44
0.000.320.73 0.58
0.70
0.66
0.66
0.69
0.76
0.89
1.08
1.34
0.77
100× scaled distortion in x-direction
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 19
Wide Face Mold Distortion
• Distorts into a ‘W’ vertically and horizontally
– Largely because of different stiffnesses of bolts
• Distortion follows bolting pattern more than the thermal response
– Short bolts provide most resistance to distortion
• Cold edges constrain against distortion
• Most severe distortion
– Just below meniscus and just above mold exit
– In between bolt columns
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 20
Narrow Face Mold Distortion
0
100
200
300
400
500
600
700
800
900
1000
1100
0 50 100 150 200 250 300 350 400
Temperature (ºC)
Dis
tan
ce B
elo
w T
op
of
Mo
ld (
mm
)
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6
Displacement (mm)
Narrow Face
Centerline
SEN Waterbox
TemperatureDisplacement
Meniscus
Bolt
Bolt
Bolt
Bolt
Bolt
Bolt
Bolt
Bolt
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 21
NF Taper Measurements
0
100
200
300
400
500
600
700
800
900
1000
1100
0 1 2 3 4 5 6 7 8 9 10
Relative Position of Hot Face (mm)
Dis
tan
ce B
elo
w T
op
of
Mo
ld (
mm
)
Sliding NF
Sticking NF
Measured 20.5'
Measured 35.8'0
100
200
300
400
500
600
700
800
900
1000
1100
0 1 2 3 4 5 6 7
Relative Position of Hot Face (mm)
Dis
tan
ce B
elo
w T
op
of
Mo
ld (
mm
)
Sliding NF
Measured 6'
Measured 34'
MeasuredCalculated, sliding NF
Calculated, sticking NF
Top 35.8’ 39.6’ 33.7’
Bottom 20.5’ 14.6’ 19.6’
Measurements during startup
MeasuredCalculated, sliding NF
Top 34’ 33.2’
Bottom 6’ 6.1’
Measurements during steady casting
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 22
Narrow Face Mold Distortion
• Narrow face distorts into roughly-parabolic arc– Typical behavior
– Elongates by 2 mm
• Low bolt operating stresses– No risk of bolt tensile failure
• Small bolt displacement at mold/waterbox interface– 16 mm bolts in 22 mm holes
– No risk of mold overconstraint or bolt shearing failure
• Waterbox hooks provide extra rigidity to assembly– Causes wobble in distortion profile
– Bolts near hooks do not overcome prestress
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 23
Effect of Distortion on NF Taper
• Calculate perimeter of mold as function of distance down the mold
• Contributions from
– Funnel geometry
– Wide face expansion
– Narrow face distortion
– Prevented sliding of
WF relative to rigid NF
• Sliding should be considered during startup and in molds with rigidly positioned NFs
0
100
200
300
400
500
600
700
800
900
1000
-1.50 -1.25 -1.00 -0.75 -0.50 -0.25 0.00 0.25 0.50 0.75 1.00
Perimeter Change (mm)
Dis
tan
ce B
elo
w M
en
iscu
s (
mm
) Total
Nominal
Funnel
Narrow Face
Distortion
Wide Face
Distortion
Interfacial
Sliding
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 24
ConclusionsMold/Waterbox Behavior
• WF distortion complicated because of bolts
• NF distortion typical
• Good design principle: oversize bolt holes in the waterbox to allow transverse movement
• Distortion has a significant effect on taper
– Not linear with distance down the mold
– Room-temperature calculations are insufficient
• More details found in
– Hibbeler et al., Met. Trans. B, 43 (2012) p. 1156.
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 25
1
2
3
4
5
6
7
Startup Transient
0 5 10 15 20 25 30 35 40 45 5020
22
24
26
28
30
32
34
36
Time (s)
Taper
(min
)
Top
Bottom
0 5 10 15 20 25 30 35 40 45 5025
30
35
40
45
50
55
60
65
70
75
Time (s)
TC
(oC
)
1234
5
6
7
• Inclinometer and thermocouple data from a startup provides great validation for exploring mold behavior during a startup
• TC temperature show first-order behavior– Time constant about 5 seconds
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 26
Startup Heat Flux Profile
• Assume that the heat flux profile has a certain shape, , applied over a region from z = ztop to z = zbot.
• Stretch this profile by changing ztop according to filling a rectangular prism and zbot
according to dummy bar movement
• Estimate filling rate: Q = 0.0048 m3/s
• Filling time gives
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University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 27
Startup Heat Flux Profile
A rough first approximation to the startup heat flux
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 28
Startup Thermal Behavior
5 s 10 s 15 s 20 s 30 s 40 s 50 s
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 29
Thermocouple History
• Obviously, heat load BC needs improvement
• Two-stage filling of mold– “Waterfall” until mold level covers nozzle ports
– “Pipe flow” after ports are submerged
0 5 10 15 20 25 30 35 40 45 5025
30
35
40
45
50
55
60
65
70
75
Time (s)
TC
(oC
)
1234
5
6
7
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 30
ConclusionsMold Startup Behavior
• Preliminary study of mold startup provides
reasonable results
– Mechanical simulations to come: try to match taper
measurements
• Heat flux boundary condition needs improvement
– Use plant data (stopper rod position, nozzle geometry,
dummy bar/casting speed history, etc.)
• Inclinometers are a good tool to use for measuring
taper during casting
University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Lance C. Hibbeler • 31
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)
• National Center for Supercomputing Applications (NCSA) at UIUC
• Ronald Schimmel, Gert Abbel, Henk Visser, Dirk van der Plas, and others at Tata Steel IJmuiden