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Effect of Carbon on Microstructure oc C-Mn Steel
Transcript of Effect of Carbon on Microstructure oc C-Mn Steel
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8/19/2019 Effect of Carbon on Microstructure oc C-Mn Steel
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The Effect of Carbon on the
Microstructure and Properties of C-Mn
Al l -Weld Metal Deposi ts
Carbon promotes acicular ferrite, at the expe nse of grain
boundary polygonal ferrite, and causes grain refinement of
the reheated regions
BY G. M. EVANS
SYNOPSIS. The effect of
0.05
to 0.15%
carbon on the microstructure and prop
ert ies of shielded metal arc welds con
taining 0.6 to 1.8% M n has bee n investi
ga ted .
It was found that carbon pro
moted acicular ferri te, at the expense of
grain boundary polygonal ferri te, and
caused grain refinement of the reheated
regions. The hardness of the deposits
increased,
and the tensi le properties
were defined by equations of the form:
a = a + b (C) + c (Mn) 4- d (C • Mn).
With regard to impact properties, i t
was fou nd tha t carbon t i l ted the Charpy-
V curves and substantia l ly reduced the
degree o f sca t te r ing . Opt imum tough
ness was achieved at a manganese level
of 1.4% when the carbon content was in
the intermediate range, i.e., 0.07 to
0.09%.
In t roduc t ion
Previous wo rk (Ref. 1), con duc ted as
part o f a jo in t p rogram wi th in Sub-Com
mission HA of the Inter national In stitute of
We lding, established, for low carb on
deposits, that manganese increasingly
refines weld metal microstructures and
gives rise to optimum impact properties
at a conc entrat ion of ab out 1.5%.
The present wo rk is a continu ation of
the p rog ram . Its main aim is to ascertain
whether the opt imum wi th regard to
manganese is displaced, depending on
the carbon level of the deposit.
Paper selected as an alternate for the 64th
AWS Annual Convention, Philadelphia, Penn
sylvania,
April
24-29,
1983.
G. M. EVANS is with Welding Industries Oerli
ko n Buehrle Ltd., Zurich,
Switzerland.
Experimental Procedure
Electrodes
Low hydrogen, i ron powder type e lec
t r o d e s - co d e d A , B, C a nd D-were
prepared as in previous work (Ref. 1).
The manganese content of the coverings
was varied to yie ld deposited metals
conta ining 0.6, 1.0, 1.4 and 1.8% M n ,
respectively.
At each of these manganese levels
different amounts of graphite were add
ed to the coatings to produce four nom
inal levels of carbon in the deposited
m e t a l s - n a m e l y ,
0.045, 0.065, 0.095 and
0.145% C. The core wire diameter of the
16 batches of experimental e lectrodes
thus prepared was 4 mm (0.16 in.), and
the coating factor (D/d) was 1.68.
Weld Preparation
The jo int geometry was that specif ied
in ISO 2560. Wel ding was do ne in the f lat
posit ion, and three weld beads per layer
we re d eposited (Ref. 1). The total num
ber of runs required to f i l l the individual
jo ints was 27. Direct c urrent (e lectrode
posi t ive) was employed, the amperage
being 170 A, the voltage 21 V, and the
heat- input was nomina lly 1 k j / m m (25
kj/ in.). The interpass temperature was
standardized at 200°C (392°F).
Mechanical Testing
Two subsize weld metal tensi le speci
mens were machined and tested for each
of the different deposits. Also, approxi
mately 35 Charpy-V notch specimens
were struck to obtain a fu l l transit ion
curve. The impact specimens were in the
as-we lded cond i t ion . On the o ther hand,
the tensi le specimens underwent hydro
gen removal treatment at 250°C (482°F)
for 14 hours (h).
Results
Chemical Composition
The chemical analyses of the weld
metal deposits are given in Table 1. The
composit ions were essentia l ly on target,
the nominal values for carbon being
0.045, 0.065, 0.095 and 0.145% at each
of the four manganese levels previously
(Ref. 1) designated as A, B, C and D. The
sil icon contents were relatively well bal
anced, the increase with increasing car
bo n being sl ight. Of note is the fact that
both su l fu r and phosphorus were low
throughout .
Metallographic Examination
General. Transverse sections were
prepared, and detai led examination was
carried out on the top weld beads and on
the adjacent super cri t ical ly heat-affected
zones as described previously (Ref. 1).
To i l lustrate the changes due to car
b o n ,
as obse rved in the l ight m icrosc ope,
typical micrographs for the extremes are
shown in Figs. 1-4 for the 1.4% Mn
level.
As-Deposi ted W eld Me ta l . The top
weld bead of each of the test weldments
was examined at the Welding Insti tute,
U.K., and the microstructural compo
nents were quantif ied according to the
scheme proposed by Abson and Do lby
(Ref. 2) and by Pargeter (Ref. 3).
Point counting was carried out at
X500, and the consti tuents were identi
f ied as fo l lows:
• Grain boun dary ferri te.
• Polygonal ferri te.
• Ferrite wi th aligned M-A-C.
• Acicular ferr ite.
WE LDIN G RESEARCH SUPPLEMENT
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Table 1—Weld
Average
con ten t ,
0.045
Metal Chemical Compositions and Tensile Properties
designation
A
B
C
D
C
0.045
0.044
0.044
0.045
M n
0.65
0.98
1.32
1.72
Compos i t i on ,
Si
0.30
0.32
0.32
0.30
%
S
0.006
0.006
0.006
0.006
P
0.008
0.008
0.007
0.008
N/mm
2
*
406
432
451
488
Tensile properti
OR,
N / m m *
462
481
512
549
es
(a)
EL,
%
35.4
35.8
32.0
29.6
R.A., %
78.8
78.8
78.8
76.0
0.065
0.095
A
B
C
D
A
B
C
D
0.059
0.063
0.066
0.070
0.099
0.098
0.096
0.093
0.60
1.00
1.35
1.77
0.65
1.05
1.29
1.65
0.33
0.35
0.37
0.33
0.35
0.32
0.30
0.33
0.007
0.006
0.005
0.006
0.008
0.007
0.007
0.007
0,008
0.008
0.007
0.008
0.009
0.009
0.009
0.007
407
451
469
511
433
477
506
535
483
516
545
588
512
546
576
602
31.2
32.4
29.2
28.4
31.8
30.0
30.8
27.8
80.6
80.6
78.8
77.9
78.8
78.8
77.9
74.0
0.145
A
B
C
D
0.147
0.152
0.148
0.141
0 63
1 00
1 40
1 76
0 40
0 41
0 38
0 36
0 008
0 007
0 007
0 006
0 007
0 007
0 007
0 007
480
517
536
606
569
605
636
691
32 8
27 4
27 4
25 6
76 0
75 0
75 7
71 9
(a) o
E
= yield stress; •
-•
.... v A y ' - X ' ' ••
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the prior austenite grain boundaries
decreased and thus enhanced the etch ing
response. The grain interiors tran sform ed
to a fine acicular structure, and the
changes were essentially a reflection of
those occurring in the as-deposited weld
metal.
Compar ison o f the two photomicro
graphs in Fig. 4 shows that grain refine
ment also occurred in the f ine grained
reheated regions. The results of linear
intercepts made at X630 are plotted in
Fig. 7. The effects of carbon and manga
nese were found to be approximately
equivalent over the experimental ranges
investigated. The microstructure became
more duplex with increasing carbon as
shown in Fig. 4, and the second phases
tended to separate, to an increasingly
greater extent, a long the primary segre
gation bands. The form and structure of
the second phase particles were revealed
by deep etching in a mixture of bromine
an d
me thano l ,
fo l lowed by examinat ion
in the SEM at X5000 magnif ication. The
phases were identified, by the British
Steel Corporation, as:
• Cemen tite f i lms.
: ® ^ A
&
Fig. 4 - Photomicrographs of fine grained
regions, 1.4 Mn. A-0.045 C; B-0.145
C. X630 (reduced 38 on reproduction)
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CARBON IN WELD
• Effect of carbon on the microstructure of weld metals obtained using electrodes A ,
B,
C, and D with Mn in coverings varied to yield deposit
containing
Mn as follows: electrode A-0.6 Mn, electrode B- 1.0 Mn, electrode
C-1.4
Mn and electrode D- 1.8 Mn
WELDING RESEARCH SUPPLEMENT 1315-s
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• Marten site / austenite (M / A).
• Bainite / Fine pea rlite (B / P).
The vo lume f ract ions were found to
increase with increasing carbon content
as shown in Figs. 8 and 9 for the 0.6 and
1.4% M n levels, respe ctively.
Hardness Testing
Average hardness values, obtained for
the last weld bead to be deposited in
each case, are plotted in Fig. 10. The
trends are essentially linear, the increase
over the range for manganese being 50
DP N (i.e., VHN) compared to approxi
mately 30 DPN (i.e., VHN) for the experi
mental range of carbon contents.
Hardness traverses along the center
l ine of deposits welded with electrode C,
at the two extremes of carbon, are plot
ted in Fig. 11 ; the difference of 30 DPN
(Le., VHN), as enc ounte red for the to p
beads, is reflected thr ough out most of
the we ldments.
Mechanical Properties
Tensile Results. The tensile test results
are prese nted in Table 1 . The yield
strengths and the ultimate tensile
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FINE GRAINED REGION
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CARBON IN WELD , .
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7 — Effect o f carbon on the grain intercept in the fine grained region
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Fig. 8 Effect of carbon
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on percentage microphases in fine
grained regions, 0.6 Mn
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martensite/austenite,
bain-
ite/pearlite)
316-s |
N O V E M B E R 1 9 8 3
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strengths are plot ted against carbon con
tent in Figs. 12 and 13, respe ctively. O n
assuming the tensile properties to be
linearly related to both carbon and
man
ganese, the fol lowing regressions were
obta ined:
1. For yield strength ( in N/mm
2
) :
o-
E
= 335 4- 439 C 4- 60
M n 4- 361 C • M n (1)
2. For ult imate tensile streng th (in N /
m m
2
):
O-R = 379 4- 754 C 4- 63
M n
4-
337 C • M n (2)
Impact Results. Charpy-V impact
curves, obtained from the average of the
scatter bands, are plotted in Fig. 14. It is
seen that the upper shelf was depressed
by the addit ion of carbon, whereas the
lower shelf tended to be raised.
On reconsider ing the absorbed energy
as a function of manganese (Fig. 15), the
opt imum composi t ion for the t rans i t ion
range was found to occur at about 1.4%
M n ,
independent ly of the carbon level of
the deposits.
The relat ive ef fects of carbon and
manganese on lateral shift are depicted in
Fig.
16. Here the Charpy-V temperatures
corresp onding to an arbit rary level of 100
) are plot ted against composit ion. At the
low manganese level (A), carbon was
found to be marginally benef icial, where
as at the high level (D) carbon was
deleter ious. For the intermediate manga
nese content (C), opt imum toughness
was achieved at an intermediate carbon
content of 0 .09%. Compar ison of the
tw o graphs in Fig. 16 show s, for the
specific ranges, that manganese had a far
greater influence on lateral shift than
carbon.
An addit ional feature to the t i l t ing of
the average Charpy-V curves was the
observed fact that the degree of scatter
ing decreased as the carbon content
increased.
The phenomenon is i l lustrated
in Fig. 17 for the two extremes of carbon
at the 1.4% Mn level. The situat ion for the
low carbon level is seen to be undesir
able,
the transition being extremely steep
and such that ful l bi-modal f racture
occur red at -40°C (-40°F).
Discussion
It is generally accepted (Refs. 4-6) that
the addit ion of carbon to low strength
ferrit ic weld metal causes the yield and
tensile strengths to increase and ductility
to decrease. Furthermore, the hardness
increases an d, at a constant g rain size, the
yield-to-tensile strength ratio decreases.
The role of dif ferent al loying elements is
known to be complex; carbon in isola
t ion ,
for example, behaves dif ferent ly
o
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5 K g L o a d .
TO P B E A D
0 0 5
0-10 0-15
C A R B O N IN W E L D . \
.
Fig. 10—Effect of carbon on hardness of
as-deposited weld metal at different mang a
nese levels as follows: A—0 .6 , B—1.0 ,
C-1.4 andD-
1.8
0 5 10 15
D I S T A N C E F R O M T O P S U R F A C E O F P L A T E , m m .
Fig.
11.-Effect
of carbon on yield stress at different manga nese levels as follows:
A-0.6 ,
B-
1.0 ,
C- 1.4 and D-
1.8
7 0 0
7 0 0
0O5
0-10 0-15
C A R B O N IN W E L D , wt .%.
Fig. 12 — Effect of carbon on yield stress at different manga nese levels as
follows: A -0.6 , B- 1.0 , C- 1.4 andD- 1.8
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than when in the presence of manga
nese, silicon and oxygen (Ref. 7).
The present metal lographic studies
have shown tha t the microstructure o f
as-deposited we ld metal is mo dif ied by
the add i t ion o f carb on. On a macroscale ,
the main observation was that the prior
austenite grain width decreased, due
possibly to a change in the solidification
sub-structure . Carbon was more e f fec
tive in this respect than manganese, and it
is presumed that the relative effects on
dendrite spacing are different.
On a microsca le , carbon was found to
increase the amount of acicular ferrite at
the expense of the proeutectoid ferri te
occurring at the boundaries of the colum
nar grains. For an increm ent of 0 .1 % C,
however, the overa l l change in micro-
structure was far less than that encoun
tered when varying the manganese
con
tent over the range from 0.6 to 1.8%. On
the other hand, increasing carbon did
lead to the precipitat ion of increasing
amounts of carbide with in the acicular
ferri te.
The microstructure of the reheated
zones was also modif ied by the addit ion
of carbon. In the case of the coarse
grained regions, the ferri te envelopes
tended to be el iminated, and in the f ine
grained regions the grain size decreased
appreciably. The degree of grain refine
ment induced by the increase in carbon
was essentially the same as that encoun
tered for the experimental range of man
ganese contents. As expected, the
amount of second phase carbides in the
fine grained regions increased as the
carbon level was raised.
The tensi le properties achieved in the
present instance varied linearly with
respect to both carbon and manganese,
the regression equations being in the
form:
a
= a + b (C) 4- c (Mn) 4- d (C • Mn).
Interaction occurred as indicated by
the lines in Figs. 12 and 13 which are not
parallel. This is as expected, since it is
known, fo r wrought mater ia ls, tha t bo th
elements have an effect on sol id solution
hardening, grain size and the percentage
amount of pearlite (Ref. 8).
The present data serve to confirm the
statement made by Heuschkel (Ref. 9)
that, for all practical purposes, there is
little error in assuming 0.04 to 0.14%
250
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318-s
| NOVEM BER 1983
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8/19/2019 Effect of Carbon on Microstructure oc C-Mn Steel
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carbon increases yield strength in a linear
manner. Straight line relationships have
been obtained previously for manga
nese, the specif ic constants being depen
dent on process variables, such as inter
pass temper ature (Ref. 10) and heat-input
(Ref. 11).
The add i t ion o f carbon to the we ld
deposits modif ied the shape of the Char
py-V curves by lowering the upper shelf
energy values and making the transit ion
between the duct i le and the br i t t le mode
of fracture more gradual. Thus, with
increasing hardenability, the critical inclu
sion distance decreased and the second
phases increasingly served as sites for
micro-vo id coa lescence.
Allen,
et al.
(Ref. 12), have suggested
that carbide f i lms contribute to the
change in slope of the transit ion curves.
A lso , den Ouden, e f al. (Ref. 7), proposed
that f lattening occurs to a greater extent
when carbon is p resent together w i th a
certa in amount o f oxygen. At the lower
end of the transit ion range, carbon was
beneficia l to an extent that depended on
manganese; also, the detrimental inf lu
ence of carbides on cleavage (Ref. 12)
was evident ly compensated fo r by the
reduction in grain size. The overall situa
t ion was such tha t the opt imum wi th
regard to manganese remained at
approximately 1.4%, independent of the
carbon content — Fig. 15. This finding is
contrary to that expected and indicates
that d i lut ion wit h a high carbon base
materia l cannot be compensated for by
lowering the manganese level.
Mo ll and Stout (Ref. 13) and den O u
d e n ,
et al.
(Ref. 7), have shown that
commercia l we ldments have comparab le
if not bette r transit ion characterist ics than
deposi ts syn thesized f rom pure raw
materia ls. In addit ion, Sagan and Camp
bell (Ref. 4) refer to an instance where a
low ca rbon co ntent is by no means
desirable. In that case, an extra low car
bon E7018 e lectrode, p roduced wi th an
ingot- i ron core wire , gave a room
tem
perature upper shelf value in excess of
360 | but was inferior to a commercial
p roduct a t -20°C
(-4°F).
The require
ment, therefore, is for an intermediate
carbon level so that the up per shelf is not
depressed too much while st i l l t i l t ing the
curve sufficiently and limiting the scatter
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Fig. 15 — Effect of mangan ese on energy absorbed at different temperatures for different carbon levels
WELDING RESEARCH SUPPLEMENT
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A S W E L D E D
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IN
W E L D .
Fig.
16 —
Effects of carbon and m anganese on
test temperatures correspond ing to
1001
F o r E 7 0 1 8 e l e c t r o d e s , w h i c h h a v e
b e e n p e r m i t t e d t o y i e l d u p t o 1 .6 % M n
s i n ce t h e i n t r o d u c t i o n o f A W S A 5 . 1 - 7 8
(Ref . 14) , t he mo st su i t ab le range sugge st
e d b y t h e r e su l ts o f t h e p r e s e n t w o r k i s
b e t w e e n a p p r o x i m a t e l y 0 . 0 7 a n d 0 . 0 9 %
c a r b o n .
C o n c l u s i o n
F o r I SO 2 5 6 0 t yp e d e p o s i t e d m e t a l ,
w e l d e d w i t h b a s ic i r o n p o w d e r e l e c
t r o d e s o f a sp e c i f i c s la g b a se t yp e , t h e
f o l l o w i n g o c c u r r e d o n i n c r e a s i n g t h e c a r
b o n c o n t e n t :
1. T h e a v e r a g e w i d t h o f t h e p r i o r
a u s t e n i t e g r a i n s d e c r e a se d .
2 . T h e a m o u n t o f a c i cu l a r f e r r i t e
i n c r e a se d a t t h e e xp e n se o f t h e p r o
e u t e c t o i d f e r r i t e .
3 . Th e aspe ct ra t i o o f t h e ac i cu la r
f e r r i t e ch a n g e d , i n c r e a s i n g t h e a m o u n t o f
c a r b i d e f o r m e d b e t w e e n t h e l a t h s .
4 . G r a i n r e f i n e m e n t o c c u r r e d in t h e
h i g h t e m p e r a t u r e r e h e a t e d r e g i o n s .
5 . G r a i n r e f i n e m e n t o c c u r r e d in t h e
l o w t e m p e r a t u r e r e h e a t e d r e g i o n s .
6 . I n c r e a s i n g a m o u n t s o f se co n d
p h a se s w e r e p r e c i p i t a t e d i n t h e f i n e
g r a i n e d r e g i o n s .
7 . T h e h a r d n e ss i n c r e a se d .
8 . Th e y ie ld a nd tens i l e s t r eng ths
i n c r e a se d li n e a r l y , b o t h p a r a m e t e r s b e i n g
d e f i n e d b y e q u a t i o n s o f t h e f o r m :
/ D U
2 0 0
-
^150
LU
z
100
G
U J
CQ
a
O
co
50
<
0
I I
T
i
0-045
C
\
i l
•v j l l l l
I I
1-4%Mn
i
i
^ J P
jL*
N
0-147%C
-
i
|
A.W.
I I
- 3 0
- 2 0
E
a
- 1 0
- 1 0 0
- 8 0
- 60
- 4 0 - 2 0 0 2 0
TEST TEMPERATURE
,°C
.
4 0
0
Fig. 17 —Charpy
V-notch
impact curves showing scatter bands for low an d high carbon levels at
1.4
Mn