Upload
pello-uranga
View
114
Download
2
Embed Size (px)
DESCRIPTION
Presentation made at Materials Science and Technology 2008 Conference held in Pittsburgh
Citation preview
Effect of Alloying Additions in the Final Microstructure of Nb-Mo Steels Processed by Thin
Slab Direct Rolling Technologies
P. Uranga, J. Ganzarain, D. Jorge-Badiola and J.M. [email protected]
MS&T’08 ConferenceOctober 6-9, 2008, Pittsburgh, PA
CEIT and TECNUN (University of Navarra)Donostia-San SebastiánBasque Country, Spain
MS&T’08 Conference, Pittsburgh, PA
Introduction
• Multiple alloying combinations for high strength properties
• Thin slab direct rolling metallurgical peculiarities– As-cast coarse grains– Alloying elements in solid solution
• Study of combined effect in softening and precipitation kinetics
• Modeling and microstructural evolution validation for schedule optimization
MS&T’08 Conference, Pittsburgh, PA
Material
• Two Nb-Mo microalloyed steels
• 0.05%C - 0.03%Nb– 0.16% Mo– 0.31% Mo
Steel C Si Mn S Al Mo Nb N
3Nb-Mo16 0.05 0.04 1.58 0.002 0.027 0.16 0.03 0.005
3Nb-Mo31 0.05 0.05 1.57 0.002 0.028 0.31 0.028 0.006
MS&T’08 Conference, Pittsburgh, PA
Deformation SchedulesSoaking:
1350ºC, 15 min
600ºC, slow cooling
Quenching
Tem
pera
ture
Time
He flow
10ºC/s
700ºC, 1hour
First deformation temperatures
Tini = 1100ºC Tini = 1050ºC
ΔT = 50ºC
Quenching temperatures
Tq = 900ºC Tq = 850ºCε1 = ε2 = ε3 = 0.4ε4 = 0.5
1ºC/s
Austenite Microstructureand Modeling
MS&T’08 Conference, Pittsburgh, PA
Austenite Microstructures Prior to Transformation
• Non-recrystallized deformed austenite grains– Tini = 1100ºC: Homogeneous Structures
3Nb-Mo16 3Nb-Mo31
Tin
i = 1
100º
C
MS&T’08 Conference, Pittsburgh, PA
Microstructural Heterogeneities in Austenite. Tini = 1050ºC
• Non-recrystallized deformed Austenite Grains– Tini = 1050ºC: Microstructural Heterogeneities
in Homogeneous Matrix 3Nb-Mo16 3Nb-Mo31
Tin
i = 1
050º
C
MS&T’08 Conference, Pittsburgh, PA
Grain Distribution Modeling• Input:
– Thermomechanical Sequence– Composition– Initial Grain Size Distribution
• Model:– Equations developed for Nb-Mo steels and wide
range of austenite grains:
• Output:– Recrystallized and unrecrystallized grain size
distributions– Mechanism history: drag, precipitation, dynamic rex
[ ]( ){ } 155,0147,00
3
78,1035,0201108,2 ZDNb
c++
⋅= −ε [ ] [ ]( )⎥⎦
⎤⎢⎣
⎡+⎟
⎠⎞
⎜⎝⎛ −⋅⎟
⎠⎞
⎜⎝⎛⋅= −−−
−
MoNbTRT
Dt DoX 09,0185275000exp180000exp1092,9 53,06,511
5,0
15,00 εε &
MS&T’08 Conference, Pittsburgh, PA
Model Predictions
• Austenite grain size distribution prior to transformation– Tini = 1100ºC: Similar distributions for both
steels 3Nb-Mo16 3Nb-Mo31
Tin
i = 1
100º
C
0
0.1
0.2
0.3
0.4
0.5
20 40 60 80 100 120 140 160 180 200
Grain Size (μm)
Aus
teni
te A
rea
Frac
tion Model
Experimental
3Nb-Mo16Tini = 1100ºC
0
0.1
0.2
0.3
0.4
0.5
20 40 60 80 100 120 140 160 180 200
Grain Size (μm)
Aus
teni
te A
rea
Frac
tion
ModelExperimental
3Nb-Mo31Tini = 1100ºC
MS&T’08 Conference, Pittsburgh, PA
Model Predictions
• Austenite grain size distribution prior to transformation– Tini = 1050ºC: Heterogeneity increases as Mo
content increases 3Nb-Mo16 3Nb-Mo31
Tin
i = 1
050º
C
0
0.1
0.2
0.3
0.4
0.5
20 100 180 260 340 420 500 580
Grain Size (μm)
Aus
teni
te A
rea
Frac
tion
ModelExperimental
3Nb-Mo16Tini = 1050ºC
0
0.1
0.2
0.3
0.4
0.5
20 100 180 260 340 420 500 580
Grain Size (μm)
Aus
teni
te A
rea
Frac
tion Model
Experimental
3Nb-Mo31Tini = 1050ºC
MS&T’08 Conference, Pittsburgh, PA
Heterogeneous Structures
• As-cast austenite grain prior to transformation:– Lack of Recrystallization through deformation
passes and interstands– Higher fraction for 3Nb-Mo31
• Bigger maximum grain size– Strain induced Nb(C,N) precipitation interacts
with softening mechanisms mainly in highly strained grains
MS&T’08 Conference, Pittsburgh, PA
Heterogeneity: As-cast Fraction
• Homogeneous Micro: Complete Rex prior to Precipitation• Minimum initial temperature is needed for heterogeneities
to be avoided• Once homogeneity achieved: focus on austenite pancaking
Tini = 1100ºC Tini = 1050ºC
0
0.2
0.4
0.6
0.8
1 2 3 4Interstand
As-
cast
frac
tion
3Nb-Mo313Nb-Mo16
Tini = 1100ºC
0
0.2
0.4
0.6
0.8
1 2 3 4Interstand
As-
cast
frac
tion
3Nb-Mo313Nb-Mo16
Tini = 1050ºC
MS&T’08 Conference, Pittsburgh, PA
Austenite Pancaking: Unrecrystallized Fraction
Tini = 1100ºC Tini = 1050ºC
0
0.2
0.4
0.6
0.8
1
Unr
ecry
stal
lized
Aus
teni
te F
ract
ion Precipitation
Solute Drag
Interstand
3Nb-Mo16
Tini = 1100ºC
3Nb-Mo31
3 41 2 3 41 20
0.2
0.4
0.6
0.8
1
Unr
ecry
stal
lized
Aus
teni
te F
ract
ion Precipitation
Solute Drag
3 4Interstand
3Nb-Mo16
Tini = 1050ºC
3Nb-Mo31
1 2 3 41 2
• Austenite Pancaking: Drag / Precipitation
MS&T’08 Conference, Pittsburgh, PA
Austenite Pancaking: Nb Steel – NbMo Steels
Tini = 1100ºC Tini = 1050ºC
0
0.2
0.4
0.6
0.8
1
Unr
ecry
stal
lized
Aus
teni
te F
ract
ion Precipitation
Solute Drag
Interstand
3Nb-Mo16
Tini = 1100ºC
3Nb-Mo31
3 41 2 3 41 20
0.2
0.4
0.6
0.8
1
Unr
ecry
stal
lized
Aus
teni
te F
ract
ion Precipitation
Solute Drag
3 4Interstand
3Nb-Mo16
Tini = 1050ºC
3Nb-Mo31
1 2 3 41 2
0
0.2
0.4
0.6
0.8
1
Unr
ecry
stal
lized
Aus
teni
te F
ract
ion
PrecipitationSolute Drag
Interstand
Tini = 1100ºC
3 41 2 3 41 2 3 41 2
3Nb-Mo16 3Nb-Mo313Nb
• Mo drag effect accelerates Nb(C,N) precipitation at low deformation T
0
0.2
0.4
0.6
0.8
1
Unr
ecry
stal
lized
Aus
teni
te F
ract
ion
3 4Interstand
3Nb-Mo16
Tini = 1050ºC
3Nb-Mo31
1 2
3Nb
3 41 2 3 41 2
εac = 0.50
εac = 0.43εac = 0.56 εac = 0.73
εac = 0.54εac = 0.95
Transformation
MS&T’08 Conference, Pittsburgh, PA
• For Tini = 1100ºC:– Homogeneous ferrite
Transformed Microstructures Coiling Simulation 700ºC
3Nb-Mo16 3Nb-Mo31
Tin
i = 1
100º
C
Dα = 8.6 μm Dα = 8.7 μm
MS&T’08 Conference, Pittsburgh, PA
• For Tini = 1050ºC:– Homogeneous ferrite with heterogeneous
regions
Transformed Microstructures Coiling Simulation 700ºC
3Nb-Mo16 3Nb-Mo31
Tin
i = 1
050º
C
Dα = 8.4 μm Dα = 8.6 μm
MS&T’08 Conference, Pittsburgh, PA
Microstructural Units EBSD
• Homogenous ferrite microstructures correspond to high angle GB units
Tini = 1100ºC 3N
b-M
o31
MS&T’08 Conference, Pittsburgh, PA
Microstructural Units EBSD• Prior austenite coarse grains transform to
coarse ferrite units or acicular structures: forming low angle GB areas.
Tini = 1050ºC
3Nb-
Mo3
1
MS&T’08 Conference, Pittsburgh, PA
Conclusions• Mo addition to Nb microalloyed steels: important
increase in the delay of static rex kinetics → The refinement of the initial as-cast structure is retarded.
• For homogeneous microstructures: EBSD show that ferrite grains are diversely oriented with high-angle grain boundaries.
• Structures transformed from non-refined as-cast grains form coarse microstructural units, bigger than those observed with the optical microscope. Toughness will be impaired.
• For optimized thermomechanical schedules, Mo affects hardenability. This factor can be useful for the formation of complex microstructures with high strength and toughness levels.
Effect of Alloying Additions in the Final Microstructure of Nb-Mo Steels Processed by Thin
Slab Direct Rolling Technologies
P. Uranga, J. Ganzarain, D. Jorge-Badiola and J.M. [email protected]
MS&T’08 ConferenceOctober 6-9, 2008, Pittsburgh, PA
CEIT and TECNUN (University of Navarra)Donostia-San SebastiánBasque Country, Spain