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Vol.25 No.2 LI Xincheng et al: Effect of Nanophase on the Nucleation…228
DOI 10.1007/s11595-010-2228-8
Effect of Nanophase on the Nucleation of
Intragranular Ferrite in Microalloyed Steel
LI Xincheng1
, WANG Xinyu2
,FENG Xiaotian1
(1. Advanced Forming Technology Institute, Jiangsu University, Zhenjiang 212013, China;
2. School of Material Science and Engineering, Jiangsu University, Zhenjiang 212013, China)
Abstract: MnS, MnS+V(C, N) complex precipitates in micro-alloyed ultra-fine grained steels
were precisely analyzed to investigate the grain refining mechanism. The experimental results shows
that MnS, MnS+V(C, N) precipitates provide nucleation center for Intra-granular ferrite (IGF), so that
refined grain remarkably. Moreover, substructures such as grain boundary, sub-boundary, distortion
band, dislocation and dislocation cell in austenite increased as the deformation energy led by heavy
deformation at low temperature (deformation temperature≤800 ℃, deformation quantity≥50%). As
a result, V(C, N) nanophase precipitated at these substructures, which pinned and stabilized sub-
structures. The substructures rotated and transformed into ultra-fine ferrite. 20 nm-50 nm were the best
grain size range of V(C, N) as it provided nucleating center for intragranular ferrite. The grain size of
V(C, N) were less than 30 nm in the microalloyed steels that with volume ratio of ultra-fine ferrite more
than 80% and grain size less than 4 μm.
Key words: intra-granular ferrite (IGF); vanadium; MnS; nanophase; substructure
1 Introduction
For a long term, there were few studies on structure
refinement effect of nanophase such as V(C, N) and MnS
in steels. The extremely rigorous constraint on this study
was mainly because the carbonitride of microalloy ele-
ments in steel is very few, MnS and other nanophase
(grain size less than 100 nm) is regarded as harmful in-
clusions that has not been caused attention of its effect on
grain refine in microalloyed steel and high-accuracy
method to detect the morph and location of these pre-
cipitates is lacked. Studies on this aspect are only about
niobium and titanium micoalloyed steel[1-3]
, so far a sys-
tematic research on the nucleating effect and grain re-
fining mechanism of V(C, N) particles in V-microalloyed
steel is rarely seen. The recent work shows that V(C, N),
MnS and other nanophase have very significant structure
refinement and nucleating promotion effect on intra-
granular ferrite in V-microalloyed steel. In order to ex-
plore the nucleating effects of nanophases on structure
refinement as well as its refining mechanism, it’s neces-
sary to go deep into observation and analysis on structure
pattern and precipitation phase in metallographic, TEM
micrograph and complex photos of vanadium microal-
loyed steels (ultra-fine grain steel), then grain refinement
can be explored, so as to lay a theoretical foundation of
ultra-fine grain steel prototype preparation and industrial
production.
2 Experimental
The test steels used mid-component of Q235 as ba-
sic ingredient and a pinch of vanadium were added into it.
Specific chemical compositions are shown in Table 1
(Steel A in Table 1 was used as contrast steel). A 25 kg
vacuum inductance furnace was used to smelt the test
steels. The ingot was forged into a φ14 mm cylinder
specimen, and then it was machined to form aφ8 mm×
12.4 mm compression specimen. The phase transforma-
tion point Ar3 was measured by Foremaster Digital full
automatic phase transformation machine and metal-
lographic analysis apparatus under the condition of
holding 5 min at 1200 ℃, the heating and cooling rate
was 10 ℃/s. Table 1 shows Thermo-Calc calculations of
the equilibrium phase transition point Ae3 in steels mi-
croalloyed with vanadium.
©Wuhan University of Technology and Springer-VerlagBerlin Heidelberg2010
(Received: Nov.25, 2008; Accepted: May 18, 2009)
李李李LI Xincheng( ): Prof.; Ph D; E-mail:lixincheng@ujs.edu.cn
Funded by the National Natural Science Foundation of China (50475125)
and the Universities Natural Science Fund Key Project of Jiangsu Province
(04KJA430021)
Journal of Wuhan University of Technology-Mater. Sci. Ed. Apr.2010 229
Table 1 The Ae3, Ar3 and chemical composition of the test steels/%
Single-pass compression test were proceeded on a Glee-
ble-2000 thermal simulator. Specimens were austenitized at
1200 ℃for 5 min to make sufficient solutionizing of vana-
dium, followed by cooling at cooling rate of 10 ℃/s and then
deformed throughout undercooled austenite range. Deforma-
tion temperature(T) were 800 ℃(Ae3)-750 ℃(Ar3), deforma-
tion amount(ε) were30%, 50%, 60% and 70%, respectively,
and the rate of deformation were 50 s
-1
.The influences of
static recovery and recrystallization on ferrites were eliminated
by water quenching to room temperature immediately after
deformation.
Microstructure observation was performed by a
scanning and transmission electron microscope (SEM
and TEM), respectively. For SEM observations, 2%-4%
nital was used for etching. TEM thin foil specimens
were prepared by mechanical thinning followed by
twin-jet reduction method. TEM observation was per-
formed by using a JEM-2010 UHR electron microscope.
MnS and V(C, N) particles and structure components in
microstructure were analyzed by a SISC-IAS8.0 image
analysis software. There are few particles which sizes
are greater than 100 nm, so the particles less than 100
nm are regarded as nanaphase. The average sizes of
particles that make up 60% of the precipitation were
used as the grain size of nanophase, ensuring that it was
representative.
3 Results and Discussion
3.1 Nucleation promote effect of MnS and
MnS + V(C, N) on IGF
MDCSobral and GMiyamoto’s work[3,4]
shown that
use metallic oxide as nucleating center, MnS+V(C, N)
complex precipitate can promote the nucleation of intra-
granular ferrite idiomorphs on it. Fig.1 (a) and (b) are
respectively micrograph and EDS of intragranular ferrite
formed on single MnS phase of the non-vanadium test
steel A in Table 1. Fig.1 (c) shows that intragranular
ferrites nucleate on precipitates which are presumably
incoherent MnS+V(C, N). EDS measurement (Fig.1 (d))
reveals that this complex precipitate is V(C, N) precipi-
tated on incoherent MnS in austenite.
Random selected 62 incoherent MnS in austenite of
test steel B and C in Table 1 were investigated to explore
the nucleating effect of MnS and MnS+V(C, N) com-
plex precipitates on intragranular ferrite. Table 2 shows
analyzing result of IGF nucleating rate on MnS and MnS+
V(C, N) precipitates.
Results in Table 2 show that intragranular ferrite
nucleating rate of MnS+V(C, N) complex precipitates is
higher than that of single MnS obviously. These results
show that the nucleating mechanisms of MnS and MnS+
V(C, N) on intragranular ferrite are difference. Manga-
nese is austenite stabilizer; manganese-poor area exists
around MnS increased driving force of γ/α transfor-
mation, thus promote ferrite nucleate on MnS and then
growing into intragranular ferrite. However, compared
with epitaxial growth ferrite on MnS+V(C, N) complex
precipitates, the promotion effect on form new phase of
constitutional supercooling caused by manganese-poor is
very small. Fig.2 shows EDS measurement of
un-nucleated MnS in austenite. It reveals that their exist
higher ferrite peak in MnS. So it can be inferred that this
kind of precipitate constitute by (MnFe)S which belongs
to atypical MnS precipitates. The constitutional super-
cooling degree around (MnFe)S can not satisfy the re-
quest of form new precipitate.
Steel C Si Mn S P V N Ae3/℃ Ar3/℃
A
B
C
0.086
0.091
0.089
0.16
0.18
0.20
0.57
0.56
0.58
0.007
0.005
0.006
0.011
0.0089
0.0094
—
0.064
0.14
0.0032
0.0031
0.0063
862
866
873
718
705
695
Table 2 IGF nucleating rate on MnS and MnS+V(C, N) in test steel B and C
MnS/
MnS+V(C,N)
Nucleated MnS/
analyzed MnS
Nucleated MnS+V(C, N)/
analyzed MnS+V(C, N)
Nucleating rate of MnS
Nucleating rate of
MnS+V(C, N)
22/40 14/22 33/40 63.6% 82.5%
Fig.1 TEM and EDS of MnS and MnS+V(C, N)
Vol.25 No.2 LI Xincheng et al: Effect of Nanophase on the Nucleation…230
Statistical analysis on MnS precipitates show that it
also has relationship with the size of MnS whether MnS
could be a nucleating center for intragranular ferrite. The
present work observed that the MnS precipitates size
greater than 100 nm cannot be nucleating center of IGF,
those IGF nucleating centers are all belongs to nanophase
(size less than 100 nm). This is because the differences of
precipitation temperature affect grain size of MnS as well
as the probability to be nucleating center of intragranular
ferrite. The solubility product[9]
of MnS in δ and γ
shows in formula (1) and formula (2).
(1)
(2)
Precipitation temperature (1200 ℃-1390 ℃) of
MnS can be inferred from formula (1) and (2). It means
MnS precipitate in austenite after γ/α transformation.
Most of MnS precipitate on grain boundary of austenite
and growing into large grains (200 nm-300 nm) rapidly,
which not belongs to nanophase. It can not satisfy the
request nanophase grain sizes of intragranular ferrite
nucleating center.
The Refs.[9,10] revealed that the diffusion of man-
ganese was controlling factor for precipitate growth of
MnS, which is because the diffusion coefficient of
manganese in γ is much smaller than sulphur. Diffu-
sion speed of manganese get slow following the decrease
of temperature. The residual manganese and sulfur con-
tents will nucleate on oxide inclusions or high-energy
deformation band formed in austenite granular. At this
point, MnS has no growing tendency. The sizes of MnS
are very tiny, many are the circular nanometer, and it may
become IGF nucleating center.
3.2 Effects of deformed austenite and V(C,
N) on IGF
By analyzing the test steel B in Table 1, the results
shows that partial of ultra-refined ferrite formed in
V-microalloyed steel are caused by heterogeneous nu-
cleation effect of deformation enhanced precipitates in
austenite on intragranular ferrite. A noticeable phe-
nomenon shows that new secondary nucleating ferrite
which have no correlations with precipitates were ob-
served that exist around ultra-refined ferrite nucleated by
precipitates (shows in Fig.3). Actually, the amount and
volume ratio of precipitates are obviously inadequate if
only consider ferrite grains nucleated by precipitates to
make up whole microstructure of ultra-refined steels. The
experimental results inferred that whole microstructure
consists of secondary nucleating ferrite and ultra-refined
ferrites formed by ferrite (second nucleation) dynamic
recrystallization and other unknown grain refining
mechanism.
3.2.1 Effect of deformed austenite fragmentation on IGF
That can be presumed that unknown grain refining
mechanism have relationship with structure evolution of
deformation austenite. High density dislocation relaxa-
tion caused by deformation in austenite made the poly-
gonization of austenite grain, thus refined the grain size
furthermore. There were cellular structures which were
divided by the dense dislocated walls formed in the aus-
tenite. Deformed austenite grains were divided into sub-
grains which has the minimum misorientation by dislo-
cated walls. As deformation carried on, γ/α trans-
formation in austenite subgrains continued, and the aus-
tenite grains were refined. The more deformation of
specimens, the thinner of austenite grains and subgrains.
For that, the size of ferrite grains decreased obviously.
The misorientation of austenite subgrains caused by ro-
tation of austenite grain in the process of deformation
increased as the increasing of deformation amount. In
subsequent process of quenching, ferrite grains were
refined furthermore for there was orientation relation-
ship[11]
between the ferrite and the austenite matrix.
lg[Mn][S] 9090 / 2.929 ( 215 / 0.097)
[Mn] 0.07[Si]
T T= − + − − +
−
lg[Mn][S] 105900 / 4.2489 0.07[Si]T= − + −
Fig.2 EDS of un-nucleated MnS in austenite
Fig.3 Microstructure of test steel B in Table 1
Journal of Wuhan University of Technology-Mater. Sci. Ed. Apr.2010 231
Fig.4 shows the shape of cellular structures in aus-
tenite grains of test steel B in table 1 after 30% and 70%
compression deformation respectively at 750 ℃. Fig.4 (a)
shows that the size of cellular structure was uneven and
its shape varied not only massive but also strip, it inferred
that the deformations of austenite grains were severe
inequality. Its microstructure also exists a very serious
phenomenon of mixed crystal, grain size of ferrite were
uneven (2-9 μm), volume ratio of ultra-fine ferrite was
only 10%. Cellular structures in Fig.4 (b) are small and uni-
form, ferrite grain size was only 2.4 μm in its microstructure
anda volume ratio of ultra-fine ferrite was morethan 80%.
3.2.2 Effects of V(C, N) precipitated in austenite on IGF
Precipitation occurred in the grain boundary, the
sub-grain boundaries, dislocation lines, and the disloca-
tion cell wall of austenite in the process of deformation
enhanced transformation. This is because there exist
higher energy than average free energy on austenite ma-
trix at those defects. In addition, the micro-alloy solute
and C, N solute atoms themselves easy-to-segregate at
these defects, and thus in favor of forming nucleating
center for micro-alloy carbon and nitrogen compounds in
these places. Fig.5 shows the shape of precipitation in the
grain boundary, the sub-grain boundaries, dislocation
lines, the dislocation cell wall and α phase of test steel
B and C in Table 1 after 60% compression deformation.
Fig.4 Microstructure of B test steel in Table 1 after
30% and 70% deformation at 800 ℃
Fig.5 Microstructure of precipitation in different defects of test steel B and C after different deformation (50%-70%) at 750℃
Vol.25 No.2 LI Xincheng et al: Effect of Nanophase on the Nucleation…232
Fig.5 (a) shows acicular ferrite precipitated in the
grain boundary of austenite. Such ferrites had fuzzy in-
terface, non-axis and irregular-shaped grains, its grain
size were tinier than common transformation ferrite. It
split the original austenite grains, and then limited the
growth of transformation ferrite. As a result, the
pre-generated acicular ferrite had a significant promoting
effect on obtaining fine-grained ferrite in the continuous
cooling process.
Fig.5 (f) shows that two kinds of precipitation were
observed in the same austenite grain. A was intragranular
ferrite precipitate in grain boundary and grown into
transgranular (grain inner). B was precipitation in dislo-
cation cell wall which stabilized the strip dislocation cell
wall where it was precipitated. As sub-structures of aus-
tenite recovery and transformed into ultra-fine grains,
disperse precipitation of nanophase can prevent the
coarsening of ferrite grain.
V(C, N) precipitated in defects of the grain bound-
ary, the sub-grain boundaries, dislocation lines, and the
dislocation cell wall had its special pinning effects on
refine grains. Austenite sub-structure were spun by V(C,
N) precipitates and limited to grown up after it trans-
formed into ferrite. Fig.6 shows that V(C, N) precipitates
have significant spinning effects.
It can be inferred from Fig.6 that the size of trans-
formation ferrite in three test steels were very tiny (less
than or equal 4 μm). Arguably the coarsening driving
force should be very large, but the experimental results
shown that the coarsening ratio of ferrite grain in test
steel C was sluggish. Growing from 2.8 μm to 4 μm
holding for 300 seconds, its growth rate G was about
0.004 μm/s. But at the same experiment condition, the
size of ferrite grain in non-vanadium test steel A was
growing from 3.8μm to 7.4 μm, its growth rate G was
about 0.012 μm/s, about 3 times than test steel C. The
growth rate of test steel B between it of test steel A and C.
As shown in Fig.6, the higher the amount of vanadium,
the more stable of the size of transformation ferrite. The
significant differences of grain growing trend between tree
test steels were due to the differences of micro-precipitation
mechanism of vanadium content in steels.
MNiikura[12]
discussed the effect of microalloy
element vanadium in steel by the first-principles of
quantum mechanics. The segregation energy of vana-
dium on fcc ferrite grain boundary was about 2.35 eV, as
well as its impurity formation energy in crystal was about
0.96 eV. Therefore in the austenite, vanadium can present
in the crystal boundary may also exist in transgranular,
and occupy the crystal boundary. That was, regarded
from energy point, adding vanadium will increase the
number of austenitic grain boundary and at the same time
reduce the grain size. Vanadium existed in the crystals
will cause changes of stress field; it can serve as a new
nucleating center for austenite. If Vanadium existed in
the grain boundary, it had a strong interaction with other
atoms around it. This was an effective way to prevent the
migration of sub-grain boundary and grain boundary and
inhibit growing of grains. V(C, N) could be a
non-spontaneous nucleating center for intragranular fer-
rite and play a very important role on grain refinement.
In summary, the ultra-fine ferrite grains in
V-microalloyed steels were mainly formed due to com-
bined effect of fragment of deformed austenite, the pin-
ning of V(C, N) nanophase on substructure, intragranular
nucleation and secondary nucleation(show in Fig.7).
Moreover, in order to investigate the appropriate particle
size of V(C, N) that can provide nucleation center for
intra-granular ferrite, a model of α nucleated on V(C,
N) interface was established(shows in Fig.8).
The free energy △G can be obtained by formula (3):
(3)
where, ΔGV is the transformation kinetics of unit volume,
r the radius ofα.
Fig.9 shows the relations between △G and r cal-
culated by formula(3). It can be inferred from Fig.9 that
the smallest nucleation energy △G was on the interface
of V(C, N). So the nucleation position for intra-granular
ferrite should be V(C, N) nanophase.
Differentiate on r in formula (3), then can obtain the
critical nucleation energy △Gcrit and criticalradius rcrit ofα.
3 2
4 ( ) / 3 4 ( )VG r G f r fγαθ σ θΔ = π Δ ⋅ + π ⋅
( )=(1 cos )(2+cos )/4f θ θ θ−
cosX Xγ α γασ σ σ θ− = ⋅
Fig.6 Ferrite grain size of test steel A, B and C holding for
different times after 70% deformation at 750 ℃
Fig.7 Formation of ultra-fine ferrite due to combined effect of fragment of deformed austenite, pinning of nanophase on substructure,
intragranular nucleation and secondary nucleation
Journal of Wuhan University of Technology-Mater. Sci. Ed. Apr.2010 233
(4)
(5)
The critical diameter of V(C, N) is:
(6)
By the above analysis, V(C, N) particle must have an
appropriate size to become nucleation center for in-
tra-granular ferrite. The size of V(C, N) particle changes
along with the change of △GV. Fig.10 shows the relationship
between the size of V(C, N) precipitates, the volume ratio of
ultra-fine ferrite and the grain size of ultra-fine ferrite in test
steel B and C in Table 1. For greatest display the grain re-
finement function of microalloyed contents, the size of V(C,
N) shouldbe controlledunder 100 nm. It canbe inferredfrom
Fig.10 that 20 nm-50 nm were the best size range. The grain
size of V(C, N) were less than 30 nm in the microalloyed
steels that with volume ratio of ultra-fine ferrite grater than
80% and grain size less than 4 μm.
4 Conclusions
a) In the experiment condition of present work, MnS,
in the traditional sense was a kind of harmful inclusions
in steels, could be transformed into beneficial inclusions.
It provided nucleating center for V(C, N) and intra-
granular ferrite, so that refined grains remarkably.
b) The experimental results strongly indicate that the
grain refining mechanism of MnS and MnS+V(C, N)
complex precipitates were its intercrystalline and secon-
dary nucleation can increase nucleating center for intra-
granular ferrite. Moreover, substructure such as grain
boundary, sub-boundary, distortion band, dislocation and
dislocation cell wall in austenite increased as the defor-
mation energy leaded in by heavy deformation at low
temperature. As a result, V(C, N) nanophase precipitated
at these substructures, which pinned and stabilized sub-
structure, thus refined ferrite grains furthermore.
c) The nucleating energy of IGF was the smallest on
V(C, N) phase interface. 20 nm-50 nm were the best
grain size range of V(C, N) as it provide nucleating center
for intragranular ferrite.
d) It was shown that there exist a linear relationship
between the size of precipitates and the grain size of fer-
rite. The grain size of V(C, N) were less than 30 nm in the
microalloyed steels that with volume ratio of ultra-fine
ferrite more than 80% and grain size less than 4 μm.
References
[1] C Carlos, G C Francisca, G M Carlos. The Role of Inclusions
and Austenite Grain Size on Intragranular Nucleation of
Ferrite in Medium Carbon Microalloyed Steels[J]. Materials
Transactions, 2004, 8(45): 2678-2685
[2] O Yasuya. Microstructural Evolution with Precipitation of
Carbides in Steels[C]. ISIJ International, 2001, 6(41): 554-565
[3] M Sobral, P RMei,HJ Kestenback. Effect ofCarbonitride Particles
Formed in Austenite on the Strength of Microalloyed Steels [J].
Materials Scienceand Engineering, 2004, 2(367):317-321
[4] G Miyamoto, T Shinyoshi, J Yamaguchi. Crystallography of
Intragranular Ferrite Formed on (MnS+V(C, N)) Complex Pre-
cipitate in Austenite[J]. Scripta Materialia, 2003, 2(48): 371-377
[5] K He, D V Edmonds. Formation of Acicular Ferrite and
Influence of Vanadium Alloying[J]. Material Science and
Technology, 2002, 3(18): 289-296
[6] CRDong, HP Ren, TZJin. Micro-alloy Quenched and Tempered
Steel[M]. Beijing:Metallurgical IndustryPress, 2000 (in Chinese)
[7] K T Park, Y S Kim, D H Shin. Microstructural Stability of
Ultrafine Grained Low-carbon Steel Containing Vanadium
Fabricated by Intense Plastic Straining[J]. Metallurgical and
Materials Transactions A, 2001, 9(32): 2373-2381
[8] H Dong. Fundamental Research Report on 800MPa Grade
High-Strength Low-Alloy Steel[R]. Beijing: China Iron &
Steel Research Institute Group, 2003. 7 (in Chinese)
[9] H Yu, Y L Kang, Z Z Zhao. Morphology and Precipitation
Kinetics of MnS in Low-carbon Steel During Thin Slab
Continuous Casting Process[J]. Journal of Iron and Steel
Research, International, 2006, 9(13): 30-36
[10] Y Ueshima, Y Sawada, S Mizoguchi. Precipitation behavior
of MnS during δ/γ Transformation in Fe-Si Alloys[J].
Metal.Trans. A, 1989, 20A: 1375
[11] P J Hurley, B C Muddle, P D Hodgson. Nucleation Sites for
Ultrafine Ferrite Produced by Deformation of Austenite
during Single-pass Strip Rolling[J]. Metallurgical and Ma-
terials Transactions, 2001, 6(32): 1507-1515
[12] M Niikura, M Fujioka, Y Adachi. New Concepts for Ultra
Refinement of Grain Size in Super Metal Project[J]. J. Mater.
Proc. Tech., 2001, 117: 341-346
3 2
crit 4 ( ) (1 cos )(2 cos ) / 3( )VG Gγασ θ θΔ = π − + Δ
crit 2 / Vr Gγασ= − Δ
crit crit2 4 / Vd r Gγασ= ⋅ = − Δ
Fig.8 Model ofαucleated on V(C, N) interface
Fig.9 Relations between ΔG and radius ofα
Fig.10 The relationship between the size of precipitates, the vol-
ume ratio of ultra-fine ferrite and the grain size of ultra-fine
ferrite in test steel B and C in Table 1

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Effect of Nanophase Precipitates on Nucleation of Ferrite in Microalloyed Steel

  • 1. Vol.25 No.2 LI Xincheng et al: Effect of Nanophase on the Nucleation…228 DOI 10.1007/s11595-010-2228-8 Effect of Nanophase on the Nucleation of Intragranular Ferrite in Microalloyed Steel LI Xincheng1 , WANG Xinyu2 ,FENG Xiaotian1 (1. Advanced Forming Technology Institute, Jiangsu University, Zhenjiang 212013, China; 2. School of Material Science and Engineering, Jiangsu University, Zhenjiang 212013, China) Abstract: MnS, MnS+V(C, N) complex precipitates in micro-alloyed ultra-fine grained steels were precisely analyzed to investigate the grain refining mechanism. The experimental results shows that MnS, MnS+V(C, N) precipitates provide nucleation center for Intra-granular ferrite (IGF), so that refined grain remarkably. Moreover, substructures such as grain boundary, sub-boundary, distortion band, dislocation and dislocation cell in austenite increased as the deformation energy led by heavy deformation at low temperature (deformation temperature≤800 ℃, deformation quantity≥50%). As a result, V(C, N) nanophase precipitated at these substructures, which pinned and stabilized sub- structures. The substructures rotated and transformed into ultra-fine ferrite. 20 nm-50 nm were the best grain size range of V(C, N) as it provided nucleating center for intragranular ferrite. The grain size of V(C, N) were less than 30 nm in the microalloyed steels that with volume ratio of ultra-fine ferrite more than 80% and grain size less than 4 μm. Key words: intra-granular ferrite (IGF); vanadium; MnS; nanophase; substructure 1 Introduction For a long term, there were few studies on structure refinement effect of nanophase such as V(C, N) and MnS in steels. The extremely rigorous constraint on this study was mainly because the carbonitride of microalloy ele- ments in steel is very few, MnS and other nanophase (grain size less than 100 nm) is regarded as harmful in- clusions that has not been caused attention of its effect on grain refine in microalloyed steel and high-accuracy method to detect the morph and location of these pre- cipitates is lacked. Studies on this aspect are only about niobium and titanium micoalloyed steel[1-3] , so far a sys- tematic research on the nucleating effect and grain re- fining mechanism of V(C, N) particles in V-microalloyed steel is rarely seen. The recent work shows that V(C, N), MnS and other nanophase have very significant structure refinement and nucleating promotion effect on intra- granular ferrite in V-microalloyed steel. In order to ex- plore the nucleating effects of nanophases on structure refinement as well as its refining mechanism, it’s neces- sary to go deep into observation and analysis on structure pattern and precipitation phase in metallographic, TEM micrograph and complex photos of vanadium microal- loyed steels (ultra-fine grain steel), then grain refinement can be explored, so as to lay a theoretical foundation of ultra-fine grain steel prototype preparation and industrial production. 2 Experimental The test steels used mid-component of Q235 as ba- sic ingredient and a pinch of vanadium were added into it. Specific chemical compositions are shown in Table 1 (Steel A in Table 1 was used as contrast steel). A 25 kg vacuum inductance furnace was used to smelt the test steels. The ingot was forged into a φ14 mm cylinder specimen, and then it was machined to form aφ8 mm× 12.4 mm compression specimen. The phase transforma- tion point Ar3 was measured by Foremaster Digital full automatic phase transformation machine and metal- lographic analysis apparatus under the condition of holding 5 min at 1200 ℃, the heating and cooling rate was 10 ℃/s. Table 1 shows Thermo-Calc calculations of the equilibrium phase transition point Ae3 in steels mi- croalloyed with vanadium. ©Wuhan University of Technology and Springer-VerlagBerlin Heidelberg2010 (Received: Nov.25, 2008; Accepted: May 18, 2009) 李李李LI Xincheng( ): Prof.; Ph D; E-mail:lixincheng@ujs.edu.cn Funded by the National Natural Science Foundation of China (50475125) and the Universities Natural Science Fund Key Project of Jiangsu Province (04KJA430021)
  • 2. Journal of Wuhan University of Technology-Mater. Sci. Ed. Apr.2010 229 Table 1 The Ae3, Ar3 and chemical composition of the test steels/% Single-pass compression test were proceeded on a Glee- ble-2000 thermal simulator. Specimens were austenitized at 1200 ℃for 5 min to make sufficient solutionizing of vana- dium, followed by cooling at cooling rate of 10 ℃/s and then deformed throughout undercooled austenite range. Deforma- tion temperature(T) were 800 ℃(Ae3)-750 ℃(Ar3), deforma- tion amount(ε) were30%, 50%, 60% and 70%, respectively, and the rate of deformation were 50 s -1 .The influences of static recovery and recrystallization on ferrites were eliminated by water quenching to room temperature immediately after deformation. Microstructure observation was performed by a scanning and transmission electron microscope (SEM and TEM), respectively. For SEM observations, 2%-4% nital was used for etching. TEM thin foil specimens were prepared by mechanical thinning followed by twin-jet reduction method. TEM observation was per- formed by using a JEM-2010 UHR electron microscope. MnS and V(C, N) particles and structure components in microstructure were analyzed by a SISC-IAS8.0 image analysis software. There are few particles which sizes are greater than 100 nm, so the particles less than 100 nm are regarded as nanaphase. The average sizes of particles that make up 60% of the precipitation were used as the grain size of nanophase, ensuring that it was representative. 3 Results and Discussion 3.1 Nucleation promote effect of MnS and MnS + V(C, N) on IGF MDCSobral and GMiyamoto’s work[3,4] shown that use metallic oxide as nucleating center, MnS+V(C, N) complex precipitate can promote the nucleation of intra- granular ferrite idiomorphs on it. Fig.1 (a) and (b) are respectively micrograph and EDS of intragranular ferrite formed on single MnS phase of the non-vanadium test steel A in Table 1. Fig.1 (c) shows that intragranular ferrites nucleate on precipitates which are presumably incoherent MnS+V(C, N). EDS measurement (Fig.1 (d)) reveals that this complex precipitate is V(C, N) precipi- tated on incoherent MnS in austenite. Random selected 62 incoherent MnS in austenite of test steel B and C in Table 1 were investigated to explore the nucleating effect of MnS and MnS+V(C, N) com- plex precipitates on intragranular ferrite. Table 2 shows analyzing result of IGF nucleating rate on MnS and MnS+ V(C, N) precipitates. Results in Table 2 show that intragranular ferrite nucleating rate of MnS+V(C, N) complex precipitates is higher than that of single MnS obviously. These results show that the nucleating mechanisms of MnS and MnS+ V(C, N) on intragranular ferrite are difference. Manga- nese is austenite stabilizer; manganese-poor area exists around MnS increased driving force of γ/α transfor- mation, thus promote ferrite nucleate on MnS and then growing into intragranular ferrite. However, compared with epitaxial growth ferrite on MnS+V(C, N) complex precipitates, the promotion effect on form new phase of constitutional supercooling caused by manganese-poor is very small. Fig.2 shows EDS measurement of un-nucleated MnS in austenite. It reveals that their exist higher ferrite peak in MnS. So it can be inferred that this kind of precipitate constitute by (MnFe)S which belongs to atypical MnS precipitates. The constitutional super- cooling degree around (MnFe)S can not satisfy the re- quest of form new precipitate. Steel C Si Mn S P V N Ae3/℃ Ar3/℃ A B C 0.086 0.091 0.089 0.16 0.18 0.20 0.57 0.56 0.58 0.007 0.005 0.006 0.011 0.0089 0.0094 — 0.064 0.14 0.0032 0.0031 0.0063 862 866 873 718 705 695 Table 2 IGF nucleating rate on MnS and MnS+V(C, N) in test steel B and C MnS/ MnS+V(C,N) Nucleated MnS/ analyzed MnS Nucleated MnS+V(C, N)/ analyzed MnS+V(C, N) Nucleating rate of MnS Nucleating rate of MnS+V(C, N) 22/40 14/22 33/40 63.6% 82.5% Fig.1 TEM and EDS of MnS and MnS+V(C, N)
  • 3. Vol.25 No.2 LI Xincheng et al: Effect of Nanophase on the Nucleation…230 Statistical analysis on MnS precipitates show that it also has relationship with the size of MnS whether MnS could be a nucleating center for intragranular ferrite. The present work observed that the MnS precipitates size greater than 100 nm cannot be nucleating center of IGF, those IGF nucleating centers are all belongs to nanophase (size less than 100 nm). This is because the differences of precipitation temperature affect grain size of MnS as well as the probability to be nucleating center of intragranular ferrite. The solubility product[9] of MnS in δ and γ shows in formula (1) and formula (2). (1) (2) Precipitation temperature (1200 ℃-1390 ℃) of MnS can be inferred from formula (1) and (2). It means MnS precipitate in austenite after γ/α transformation. Most of MnS precipitate on grain boundary of austenite and growing into large grains (200 nm-300 nm) rapidly, which not belongs to nanophase. It can not satisfy the request nanophase grain sizes of intragranular ferrite nucleating center. The Refs.[9,10] revealed that the diffusion of man- ganese was controlling factor for precipitate growth of MnS, which is because the diffusion coefficient of manganese in γ is much smaller than sulphur. Diffu- sion speed of manganese get slow following the decrease of temperature. The residual manganese and sulfur con- tents will nucleate on oxide inclusions or high-energy deformation band formed in austenite granular. At this point, MnS has no growing tendency. The sizes of MnS are very tiny, many are the circular nanometer, and it may become IGF nucleating center. 3.2 Effects of deformed austenite and V(C, N) on IGF By analyzing the test steel B in Table 1, the results shows that partial of ultra-refined ferrite formed in V-microalloyed steel are caused by heterogeneous nu- cleation effect of deformation enhanced precipitates in austenite on intragranular ferrite. A noticeable phe- nomenon shows that new secondary nucleating ferrite which have no correlations with precipitates were ob- served that exist around ultra-refined ferrite nucleated by precipitates (shows in Fig.3). Actually, the amount and volume ratio of precipitates are obviously inadequate if only consider ferrite grains nucleated by precipitates to make up whole microstructure of ultra-refined steels. The experimental results inferred that whole microstructure consists of secondary nucleating ferrite and ultra-refined ferrites formed by ferrite (second nucleation) dynamic recrystallization and other unknown grain refining mechanism. 3.2.1 Effect of deformed austenite fragmentation on IGF That can be presumed that unknown grain refining mechanism have relationship with structure evolution of deformation austenite. High density dislocation relaxa- tion caused by deformation in austenite made the poly- gonization of austenite grain, thus refined the grain size furthermore. There were cellular structures which were divided by the dense dislocated walls formed in the aus- tenite. Deformed austenite grains were divided into sub- grains which has the minimum misorientation by dislo- cated walls. As deformation carried on, γ/α trans- formation in austenite subgrains continued, and the aus- tenite grains were refined. The more deformation of specimens, the thinner of austenite grains and subgrains. For that, the size of ferrite grains decreased obviously. The misorientation of austenite subgrains caused by ro- tation of austenite grain in the process of deformation increased as the increasing of deformation amount. In subsequent process of quenching, ferrite grains were refined furthermore for there was orientation relation- ship[11] between the ferrite and the austenite matrix. lg[Mn][S] 9090 / 2.929 ( 215 / 0.097) [Mn] 0.07[Si] T T= − + − − + − lg[Mn][S] 105900 / 4.2489 0.07[Si]T= − + − Fig.2 EDS of un-nucleated MnS in austenite Fig.3 Microstructure of test steel B in Table 1
  • 4. Journal of Wuhan University of Technology-Mater. Sci. Ed. Apr.2010 231 Fig.4 shows the shape of cellular structures in aus- tenite grains of test steel B in table 1 after 30% and 70% compression deformation respectively at 750 ℃. Fig.4 (a) shows that the size of cellular structure was uneven and its shape varied not only massive but also strip, it inferred that the deformations of austenite grains were severe inequality. Its microstructure also exists a very serious phenomenon of mixed crystal, grain size of ferrite were uneven (2-9 μm), volume ratio of ultra-fine ferrite was only 10%. Cellular structures in Fig.4 (b) are small and uni- form, ferrite grain size was only 2.4 μm in its microstructure anda volume ratio of ultra-fine ferrite was morethan 80%. 3.2.2 Effects of V(C, N) precipitated in austenite on IGF Precipitation occurred in the grain boundary, the sub-grain boundaries, dislocation lines, and the disloca- tion cell wall of austenite in the process of deformation enhanced transformation. This is because there exist higher energy than average free energy on austenite ma- trix at those defects. In addition, the micro-alloy solute and C, N solute atoms themselves easy-to-segregate at these defects, and thus in favor of forming nucleating center for micro-alloy carbon and nitrogen compounds in these places. Fig.5 shows the shape of precipitation in the grain boundary, the sub-grain boundaries, dislocation lines, the dislocation cell wall and α phase of test steel B and C in Table 1 after 60% compression deformation. Fig.4 Microstructure of B test steel in Table 1 after 30% and 70% deformation at 800 ℃ Fig.5 Microstructure of precipitation in different defects of test steel B and C after different deformation (50%-70%) at 750℃
  • 5. Vol.25 No.2 LI Xincheng et al: Effect of Nanophase on the Nucleation…232 Fig.5 (a) shows acicular ferrite precipitated in the grain boundary of austenite. Such ferrites had fuzzy in- terface, non-axis and irregular-shaped grains, its grain size were tinier than common transformation ferrite. It split the original austenite grains, and then limited the growth of transformation ferrite. As a result, the pre-generated acicular ferrite had a significant promoting effect on obtaining fine-grained ferrite in the continuous cooling process. Fig.5 (f) shows that two kinds of precipitation were observed in the same austenite grain. A was intragranular ferrite precipitate in grain boundary and grown into transgranular (grain inner). B was precipitation in dislo- cation cell wall which stabilized the strip dislocation cell wall where it was precipitated. As sub-structures of aus- tenite recovery and transformed into ultra-fine grains, disperse precipitation of nanophase can prevent the coarsening of ferrite grain. V(C, N) precipitated in defects of the grain bound- ary, the sub-grain boundaries, dislocation lines, and the dislocation cell wall had its special pinning effects on refine grains. Austenite sub-structure were spun by V(C, N) precipitates and limited to grown up after it trans- formed into ferrite. Fig.6 shows that V(C, N) precipitates have significant spinning effects. It can be inferred from Fig.6 that the size of trans- formation ferrite in three test steels were very tiny (less than or equal 4 μm). Arguably the coarsening driving force should be very large, but the experimental results shown that the coarsening ratio of ferrite grain in test steel C was sluggish. Growing from 2.8 μm to 4 μm holding for 300 seconds, its growth rate G was about 0.004 μm/s. But at the same experiment condition, the size of ferrite grain in non-vanadium test steel A was growing from 3.8μm to 7.4 μm, its growth rate G was about 0.012 μm/s, about 3 times than test steel C. The growth rate of test steel B between it of test steel A and C. As shown in Fig.6, the higher the amount of vanadium, the more stable of the size of transformation ferrite. The significant differences of grain growing trend between tree test steels were due to the differences of micro-precipitation mechanism of vanadium content in steels. MNiikura[12] discussed the effect of microalloy element vanadium in steel by the first-principles of quantum mechanics. The segregation energy of vana- dium on fcc ferrite grain boundary was about 2.35 eV, as well as its impurity formation energy in crystal was about 0.96 eV. Therefore in the austenite, vanadium can present in the crystal boundary may also exist in transgranular, and occupy the crystal boundary. That was, regarded from energy point, adding vanadium will increase the number of austenitic grain boundary and at the same time reduce the grain size. Vanadium existed in the crystals will cause changes of stress field; it can serve as a new nucleating center for austenite. If Vanadium existed in the grain boundary, it had a strong interaction with other atoms around it. This was an effective way to prevent the migration of sub-grain boundary and grain boundary and inhibit growing of grains. V(C, N) could be a non-spontaneous nucleating center for intragranular fer- rite and play a very important role on grain refinement. In summary, the ultra-fine ferrite grains in V-microalloyed steels were mainly formed due to com- bined effect of fragment of deformed austenite, the pin- ning of V(C, N) nanophase on substructure, intragranular nucleation and secondary nucleation(show in Fig.7). Moreover, in order to investigate the appropriate particle size of V(C, N) that can provide nucleation center for intra-granular ferrite, a model of α nucleated on V(C, N) interface was established(shows in Fig.8). The free energy △G can be obtained by formula (3): (3) where, ΔGV is the transformation kinetics of unit volume, r the radius ofα. Fig.9 shows the relations between △G and r cal- culated by formula(3). It can be inferred from Fig.9 that the smallest nucleation energy △G was on the interface of V(C, N). So the nucleation position for intra-granular ferrite should be V(C, N) nanophase. Differentiate on r in formula (3), then can obtain the critical nucleation energy △Gcrit and criticalradius rcrit ofα. 3 2 4 ( ) / 3 4 ( )VG r G f r fγαθ σ θΔ = π Δ ⋅ + π ⋅ ( )=(1 cos )(2+cos )/4f θ θ θ− cosX Xγ α γασ σ σ θ− = ⋅ Fig.6 Ferrite grain size of test steel A, B and C holding for different times after 70% deformation at 750 ℃ Fig.7 Formation of ultra-fine ferrite due to combined effect of fragment of deformed austenite, pinning of nanophase on substructure, intragranular nucleation and secondary nucleation
  • 6. Journal of Wuhan University of Technology-Mater. Sci. Ed. Apr.2010 233 (4) (5) The critical diameter of V(C, N) is: (6) By the above analysis, V(C, N) particle must have an appropriate size to become nucleation center for in- tra-granular ferrite. The size of V(C, N) particle changes along with the change of △GV. Fig.10 shows the relationship between the size of V(C, N) precipitates, the volume ratio of ultra-fine ferrite and the grain size of ultra-fine ferrite in test steel B and C in Table 1. For greatest display the grain re- finement function of microalloyed contents, the size of V(C, N) shouldbe controlledunder 100 nm. It canbe inferredfrom Fig.10 that 20 nm-50 nm were the best size range. The grain size of V(C, N) were less than 30 nm in the microalloyed steels that with volume ratio of ultra-fine ferrite grater than 80% and grain size less than 4 μm. 4 Conclusions a) In the experiment condition of present work, MnS, in the traditional sense was a kind of harmful inclusions in steels, could be transformed into beneficial inclusions. It provided nucleating center for V(C, N) and intra- granular ferrite, so that refined grains remarkably. b) The experimental results strongly indicate that the grain refining mechanism of MnS and MnS+V(C, N) complex precipitates were its intercrystalline and secon- dary nucleation can increase nucleating center for intra- granular ferrite. Moreover, substructure such as grain boundary, sub-boundary, distortion band, dislocation and dislocation cell wall in austenite increased as the defor- mation energy leaded in by heavy deformation at low temperature. As a result, V(C, N) nanophase precipitated at these substructures, which pinned and stabilized sub- structure, thus refined ferrite grains furthermore. c) The nucleating energy of IGF was the smallest on V(C, N) phase interface. 20 nm-50 nm were the best grain size range of V(C, N) as it provide nucleating center for intragranular ferrite. d) It was shown that there exist a linear relationship between the size of precipitates and the grain size of fer- rite. The grain size of V(C, N) were less than 30 nm in the microalloyed steels that with volume ratio of ultra-fine ferrite more than 80% and grain size less than 4 μm. References [1] C Carlos, G C Francisca, G M Carlos. The Role of Inclusions and Austenite Grain Size on Intragranular Nucleation of Ferrite in Medium Carbon Microalloyed Steels[J]. Materials Transactions, 2004, 8(45): 2678-2685 [2] O Yasuya. Microstructural Evolution with Precipitation of Carbides in Steels[C]. ISIJ International, 2001, 6(41): 554-565 [3] M Sobral, P RMei,HJ Kestenback. Effect ofCarbonitride Particles Formed in Austenite on the Strength of Microalloyed Steels [J]. Materials Scienceand Engineering, 2004, 2(367):317-321 [4] G Miyamoto, T Shinyoshi, J Yamaguchi. Crystallography of Intragranular Ferrite Formed on (MnS+V(C, N)) Complex Pre- cipitate in Austenite[J]. Scripta Materialia, 2003, 2(48): 371-377 [5] K He, D V Edmonds. Formation of Acicular Ferrite and Influence of Vanadium Alloying[J]. Material Science and Technology, 2002, 3(18): 289-296 [6] CRDong, HP Ren, TZJin. Micro-alloy Quenched and Tempered Steel[M]. Beijing:Metallurgical IndustryPress, 2000 (in Chinese) [7] K T Park, Y S Kim, D H Shin. Microstructural Stability of Ultrafine Grained Low-carbon Steel Containing Vanadium Fabricated by Intense Plastic Straining[J]. Metallurgical and Materials Transactions A, 2001, 9(32): 2373-2381 [8] H Dong. Fundamental Research Report on 800MPa Grade High-Strength Low-Alloy Steel[R]. Beijing: China Iron & Steel Research Institute Group, 2003. 7 (in Chinese) [9] H Yu, Y L Kang, Z Z Zhao. Morphology and Precipitation Kinetics of MnS in Low-carbon Steel During Thin Slab Continuous Casting Process[J]. Journal of Iron and Steel Research, International, 2006, 9(13): 30-36 [10] Y Ueshima, Y Sawada, S Mizoguchi. Precipitation behavior of MnS during δ/γ Transformation in Fe-Si Alloys[J]. Metal.Trans. A, 1989, 20A: 1375 [11] P J Hurley, B C Muddle, P D Hodgson. Nucleation Sites for Ultrafine Ferrite Produced by Deformation of Austenite during Single-pass Strip Rolling[J]. Metallurgical and Ma- terials Transactions, 2001, 6(32): 1507-1515 [12] M Niikura, M Fujioka, Y Adachi. New Concepts for Ultra Refinement of Grain Size in Super Metal Project[J]. J. Mater. Proc. Tech., 2001, 117: 341-346 3 2 crit 4 ( ) (1 cos )(2 cos ) / 3( )VG Gγασ θ θΔ = π − + Δ crit 2 / Vr Gγασ= − Δ crit crit2 4 / Vd r Gγασ= ⋅ = − Δ Fig.8 Model ofαucleated on V(C, N) interface Fig.9 Relations between ΔG and radius ofα Fig.10 The relationship between the size of precipitates, the vol- ume ratio of ultra-fine ferrite and the grain size of ultra-fine ferrite in test steel B and C in Table 1