Optimizing Weld Repair in Cast Steels
Transcript of Optimizing Weld Repair in Cast Steels
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Optimizing Repair Welding Techniques
in Cast Steels—Part
II
Hz-induced cracking can be prevented by using low
hydrogen practice if the maximum HAZ hardness is below
Re
35, and all steel
castings
should be normalized before repair w elding
BY D. K. A I D U N AND W. F. SAVAGE
of cast
for hydrogen- induced
low- and
h igh-
in simulated repair
It was shown tha t to prevent
is not possible,
of hardness in
be be low
e 35.
Metal lographic examinat ion of these
the
fus ion zone
out
and
including
the
unaffected base
are:
1 Fusion zone
2. Unmixed zone .
3. Coarse-gra ined homo geneou s HAZ.
4 . Fine-grained homogeneous HAZ.
5. Part ial ly t ransformed region.
6. Spheroidized region.
7. Unaffected base metal.
All as-cast heats with carbon contents
0.21 to 0.32 wt-%,
upon
to a 5-second arc t ime, exhib
of about
0 Re in the ne tworks of martensite
the
islands
of
unt ransformed
in the part ial ly t ransformed region.
was a t t r ibuted to the inhomogenei ty
f the as-cast structure. However, for
was
by normalizing the alloy
the we ld ing opera t ion . For cast
of abou t 0.30 wt-%, in addi t ion to
a pos tweld heat t reat
be ad visable.
It is generally recogn ized that four
be met s imultaneously for
to
occur.
can be summar ized as fo l lows:
1 . A me tallurgical requisite. For crack
in g to occur , a crack-sensitive microstruc
ture must
be
present , and,
in
genera l ,
the
susceptibility to hydrogen- induced crack
ing increases with increase in the hard
ness of the m icrost ructure.
2. A chemical requisite. For cracking to
occur , the level of dif fusible hydrogen
present in the crack-suscept ible micro-
structure must exceed a cr it ical concen
trat ion, which decreases sharply as the
yield strength of the microstructure
present increases (Ref. 1).
3.
A
mechanical requisite. A l though
cracking has been show n to init iate at
lower stress levels, it appears that crack
prop aga t ion requires localized stresses of
approx imate ly y ie ld-s t rength magni tude
(Ref. 2).
4 .
An environment requisite. Hydro
gen- induced crack ing has been show n to
result f rom the ext raord inary reduct ion in
the notched-tensile strength
of
steels
caused by the presence of a relatively
small amount of d i f fus ib le hydrog en (Ref.
3). Since this loss in strength in the pres
ence of a notch occurs only in the range
- 1 4 8 to 390°F ( -100 to 200°C), hydro
gen-induced cracking requires that the
weldments be exposed to temperatures
within this range in the presence of the
f irst three requisites.
A l t hough in theory h ydrogen - induced
cracking
can be
p reven ted
by
el iminat ion
of any one of the above requisites, in
pract ice it is usually possible to exert
cont ro l over only the first two. This
results f rom
the
fact that
the
thermally-
D. K. AIDUN
is Assistant
Professor,
Mechanical
an d
Industrial Fngineering
Department, Clark-
so n
University,
Potsdam, New
York;
a nd W F.
SA
VA
GE is Professor
Emeritus,
Rensselaer
Poly
technic Institute,
Troy,
New
York.
induced residual stresses in all but the
simplest of weldment geometr ies are
usually sufficient in magni tude to init iate
cracking if the other requisites are met.
Furthermore, unless stress relief heat
t reatment is per fo rme d af ter weld ing , the
addi t ion of service usually raises the local
ized stresses in the we ldmen t above the
crit ical level for c rack propagat ion.
Because most welded structures expe
rience service in the crack-sensitive t em
perature range, this requisite is usually
met . However , it is possible to take
advantage
of
this requirement
in two
ways:
1 . Postweld soaking. It has been
s h o wn by Adams (Ref. 4) and others that
an immediate postweld soak for 30
minutes (min) to one hour (h) at a temper
ature of above 390°F (200°C) will usually
prevent hydrogen - induced crack ing. This
is at t r ibuted mainly to the reduct ion in the
level of dif fusible hydrogen made possi
b le by the greatly increased diffusivity of
hydrogen at 390°F (200°C). Thus, by the
t ime the we ld m e n t is a l lowed to return to
the crack-sensit ive temperature range,
the residual level of dif fusible hydrogen is
rendered be low the critical lev el for crack
init iation.
2. Cryogenic storage. In conduct ing
laboratory studies, it is convenient to be
able to s tore welded specimens under
condit ions which preclude either loss of
hydrogen or the f o rmat ion of hyd rogen-
induced cracks unt i l controlled experi
ments can be init iated. This has been
s h o wn (Ref. 5) to be possible by transfer
o f the we ldments to l iquid nit rogen
(-320°F) ( -1 95 .8°C boi l ing point ) as
soon as they reach ambient temperature
and stor ing under l iquid nit rogen unt i l the
exper iments begin.
The crit ical hardness level is inf luenced
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Table
1—Chemical
Co mpo sition, Initial Hardness (IH), and Ideal Critical Diam eter (D[) of Heat
32, 27, 1 , and 0
Composition, wt-%
C
Mn
P
S
Si
Ni
Cr
Mo
Cu
Al
IH, Re
D|, in.
32
0.32
1.15
0 017
0.017
0.54
0.13
0.22
0.04
0 078
51
3 17
27
0.31
1.57
0.013
0 013
0 50
0 03
0.14
0 10
0 04
0 054
51
3.51
1
0.21
1.24
0 018
0.031
0 51
0 07
0 20
0 03
0 04
0.11
46
2 05
0
0 26
0 74
0 021
0 028
0 40
0 04
0.31
0.02
0.03
0.075
48
1.61
by the toughness and duct i l i ty of the
microstructure of the weld heat-af fected
zone (HAZ). O f the var ious possible
microconst i tuents, untempered mar tens
ite is the most br it t le and, therefore, the
most suscept ible to hydrogen-induced
cracking.
The other microconst ituents,
listed in order of decreasing susceptibility,
include lower bainite, upper bainite,
pearl i te, spheroidite, and ferr ite.
In general, the toughness and duct i l i ty
both of ind iv idual and par t icu lar combi
nat ions of microconst ituents is decreased
by increasing the carbon content of the
prior austenite. For this reason, the sus
cept ibi l i ty to hydrogen-induced cracking
is direct ly related to the carbon content
of the steel. For a given carbon content,
increasing the percentage of martensite
in the weld heat -af fected zone lowers
the cr i t ica l hydrogen concent rat ion
required to cause hydrogen- induced
cracking.
Carbon is the least expensive of all
alloying elements. Because of this, steel
foundries tend to increase the carbon
content of their steels in order to achieve
higher strength. The increase in carbon
content increases the ideal crit ical diame
ter, D|, more than any other alloying
element; in addition, it also increases the
hardness of any martensite formed.
A few years ago, the railroad industry
began to invest igate the fai lure of cast
com ponen ts such as couplers, yokes, and
knuckles. As a result of this investigation,
i t was concluded that hydrogen- induced
cracking was a contr ibut ing cause of
fai lure. I t seemed l ikely that hydrogen-
induced cracking could result f rom
improper weld ing procedures used in
repairing casting defects in these struc
tures. It was suspected that, in the
absence of suitable control of repair-
welding procedures, crack suscept ible
heat-af fected-zone microstructures could
easily be produced.
Unfortunately, repair welds in steel
cast ings are of ten performed solely for
"cosmetic" reasons to eliminate superf i
cial surface imperfect ions. The rapid
cooling rates, which are associated with
such "cosmet ic" repairs , coupled wi th
inadequate control of sources of hydro
gen such as improper handling and stor
age of consumables, great ly increase the
probabi l i t y of hydrogen- induced crack
ing.
Underbead cracking is one of the most
insidious forms of hydrogen-induced
cracking. This is because it often is lo
cated ent irely beneath the weld and fails
to emerge at the surface where it can be
detected by nondest ruct ive inspect ion.
Unfor tunate ly , the geometry of most
repair welds is such as to make this a
dominant form of hydrogen- induced
cracking in steel castings. If undetected,
such cracks may experience slow crack
growth in service unt i l the cr it ical crack
size is reached and catastrophic fai lure
occurs.
Materials and Specimen
Preparat ion
Four heats of cast steel were used in
this inve st igat ion. Table
I
lists the chem ical
com pos it ion, init ial hardness,
IH
(the
hard
ness of martensite), and ideal crit ical
diameter, D, (based upon 50% martens
ite),
for all four heats.
The four heats, supplied in the form of
cast coupons, had dimensions that were
approx imate ly 10Vi X4V4 X
3
/i in.
(260 X 108 X 19 mm). From these co u
pons, specimens of 10 X 2 X V2 in.
(254 X 50.8 X 13 m m) we re machined
for the hydrogen- induced crack ing test .
The sur face on which the welds were to
be deposi ted was then pol ished wi th 24 0
grit SiC paper and degreased with ace
tone.
Polishing and degreasing are crit ical
and impor tant for the hydrogen- induced
crack ing test when us ing low-hydrogen
welding pract ice. These cleaning opera
t ions mitigate hydrogen absorpt ion in the
weld b y remov ing hydrogenous mater ia ls
from the surface of the specimen.
Procedure
The e lect rode type , hydrog en c ontent ,
heat t reatments, and the heats of steel
used in this part of the investigation are
summarized in Table 2. The level of
dif fusible hydrogen in welds was mea
sured by the RPI silicone-oil extract ion
technique (Ref. 6). Two levels of dif fus
ib le hydrogen were s tudied:
1 . Low-hydrogen pract ice. Af ter re
moval f rom hermetically sealed shipping
containers, the electrodes were trans
ferred immediately to a well-vent i lated
holding oven and maintained at 350°F
(177°C) unt i l just before use. This proce
dure gave an average level dif fusible
hydrogen of a pprox imate ly 3 ppm (3.3
cc/100 g of weld metal).
2.
High-hydrogen pract ice. The elec
t rodes were removed f rom the open
shipping container, dipped in water for
30 s and used immediately. This pract ice
gave an average dif fusible hydrogen level
o f 30 ppm (33.3 cc / 1 00 g o f we ld m et
al).
The 10 X 2 X l/
2
in. (254 X 50.8 X 13
mm) bars were welded using var ious arc
t imes and weld distances with both low
and h igh-hydrogen pract ice. Af ter
coo l
ing to ambient temperature, the
w e l d
ments were immediately loaded in the
varestraint apparatus (Ref. 7) and a 2%
augmented st ra in was then appl ied.
During this process, an acoust ic-emis
s ion t ransducer was mounted on the
specimen surface adjacent to the weld
bead,
as show n schematically in Fig. 1 , to
monitor crack init iat ion and propagat ion.
Table
2—Summary
for Electrodes, Hydrogen Conte nt, Heat Treatments, and Steel Heats Used
in Investigation
Diffusible H2 in welds made with
3/16 in. (4.76) diam. electrodes:
Moist E7018(
a
>
Baked E7018
(b)
Heats 32 , 27, 1 , 0
Heats 32, 27, 1,0
Heat 27
30 ppm
3 ppm
As-received
Normalized at 1750°F (954°C)
Normalized and postweld heat treatment
at 1100
3
F(593°C)
'"'Electrode d ipped in wa te r fo r 30 seconds .
(b)
Electrode s to red con t inuous ly a t 350-F (177
C
C) a f te r remova l f rom sea led con ta ine r .
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Because of the high ductile-britt le transi
t ion temperature (DBTT) of these heats,
the hydrogen-induced cracking could not
be per form ed at l iqu id-n i trogen tem pera
tu re , - 3 2 0 ° F (-196°C).
Specimens were then cut and
mounted for meta l lographic examinat ion
and microhardness measurements.
Hy d r o g e n - I n d u c e d Cr a c k i n g T e s t s
Equations described in an earlier paper
(Part I to this paper — Ref. 8) were used to
select weld ing condi t ions which would
give maximum weld heat -af fected zone
hardness levels ranging from about 25 to
50 Re in the coarse-grained region at the
fus ion boundary. Welds were made in
heats 32, 27, 1 and 0 using the selected
welding procedures to make simulated
repair welds wi th both h igh- and low-
hydrogen pract ice.
The welde d specimens were loaded in
the varestraint test apparatus. The n, af ter
attaching the acoustic-emission transduc
er , they were subjected to a 2% aug
me nted strain for 2 h in orde r to simulate
the mechanical factor by creat ing yie ld-
strength stresses in the outer f ibers of the
specimen.
The acoust ic-emission data provided
qualitat ive informat ion on the init iat ion
and propagat ion of hydrogen- induced
cracking.
However , quant i ta t ive cor re la
t ion between the acoust ic-emission
counts and the severity of cracking was
not found. This was believed at the t ime
to result f rom extraneous noise in and
about the laboratory that caused errone
ous counts. However, for reasons that
are discussed in a later section, this may
be only partially responsible for the lack
of correlat ion.
fjk
1
- < « • •
""31
Fig.
2
— Typical underbead crack
in the coarse
grained region
of
the HAZ
of
a stationary
weld
made on heat 27 using high-hydrogen prac
tice. Arc c urrent - 220 A; arc voltage-25 V;
arc time-5 s; section thickness- 'A in. (12.7
mm); cooling rate at 900°F (482°C)-49°F/s
(27.2°C/s); hardness-52 Re (50 Re pre
dicted).
2 nital, X500 (reduced 46%, on
reproduction)
For welds made using high-hydrogen
pract ice the maximum "safe" hardness
level was found to be about 33 Re.
Welds made wi th condi t ions that
produce hardness levels of less than 35
Re did not exhibit detectable cracks in the
coarse-grained region of the heat-af
fected zone , even w i th 30 ppm of d i f fus
ible hydrogen present.
With low-hydrogen pract ice, no crack
ing was detected in the coarse-grained
region until hardness levels of approxi
mately 45
Re
were p roduced .
Figure 2 shows a typical underbead
crack, which init iated in the
coarse
grained region of the weld heat-af fected
zone .
The microstructure around the
crack is predo mina nt ly martensit ic.
Weld Bead
To Acoust ic
-»
Emission
-T^P—i
Recorder
aug
2 R
SIDE VIEW
1 - Schematic diagram of bending section of the varestraint apparatus and location of acoustic
transducer with respect to weld
:A
X
# •
ftot
®
Fig. 3 — Effect of cooling rate on microstructure
of repair w eld HAZ in heat 1. A -stationary
weld (stationary
arc);
B — linear weld. Welding
conditions: for A and
B — 220 A
arc
current,
25
V a rc voltage,
V2
in. section
thickness;
for A
only-5
s arc time, cooling rate of 39°F/s @
900 F,
51
Re
max.
hardness;
for B
only- 10
ipm travel speed, 2.0 in. weld
length,
18°F/s
cooling rate @ 900 F, 31 Re max. hardness.
2 nital etch, X500 (reduced 35% on repro
duction)
Figure 3 shows weld heat-af fected-
zone microstructures which experienced
maximum cooling rates of 18 and 39°F/s
(10 and 21 .7°C/s ), respect ively, at 900°F
(482
°C).
The structure in Fig. 3A consists
of a mixture of m artensite ( ident if ied by
the let ter M), lower bainite ( ident if ied by
the letter
B
L
)
and up per bainite ( ident if ied
by the let ter Bu).
The measured maximum hardness in
the martensitic regions of the specimen in
Fig.
3A was
Re 51 ,
whereas the calculated
value of IH for this material (heat 1) is only
45
Re.
This means that the carbon
con
tent of the pr ior austenite was probably
inhomogeneous and was higher than the
nominal carbon content in some regions,
thus explaining the higher than expected
maximum hardness. This is entirely possi
ble because the short t ime-at- tempera-
ture could prevent complete
homogen i -
zat ion f rom occur r ing even at tempera
tures just belo w the solidus. The structure
in Fig. 3B consists of upper and lower
bainites with maximum hardness level of
Re 3 1 .
The major dif ference between cast
and wrought steel products l ies in the
nature and severity of the composit ional
heterogenei ty . In both types of product ,
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.*--
E F
«*•
4 £ C 0
fig.
4 — Microstructure
of 5
s stationary
repair weld
in
heat 27 w ith KHN
(50
g
load) hardnesses as
follows:
A- 168;
6 - 2 8 0 ;
C - 4 0 3 ; D-403 p rior pearlite, 197 prior ferrite; £ -6 1 5 prior pearlite, 84
prior ferrite;
F—
163 prior pearlite; C- (n o t stated). Nital etch, X50 (reduced 49% on reproduc
tion)
the init ial solidif ication process is accom
panied by dendrit ic segregat ion with the
dendrite interst ices being enr iched in
those elements which depress the l iquid
us tempe rature of the a l loy. H ow eve r ,
dur ing soaking at high temperature in
preparat ion for hot -work ing, par t ia l
homogenizat ion occurs, and the pat tern
of the residual segregation is altered by
the hot -work ing operat ions. Thus, in the
case of hot-rolled plate products, the
combinat ion of thermal and mechanical
t reatment forms alternat ing bands of
sol
ute-rich and solute-lean material parallel
to the rolled surface.
In the case of steel castings, the p atte rn
of segregat ion is controlled by the
den
drit ic-arm spacing, which increases as the
section thickness increases. Since no
mechanical work in g is involve d, hom oge
nizat ion of cast ings can only be achieved
by dif fusion-controlled thermal t reat
ments. When the dendrite-arm spacings
are large, the increased diffusion dis
tances require longer t imes and higher
temperatures to achieve a reasonable
degree of homogenizat ion. Thus, it is
customary to normalize cast steels prior
to the f inal heat- t reatment operat ions
which are designed to control the
mechanical propert ies of the cast ings.
Figure 4 shows the microstructural
changes from the fusion zone at the lef t
outward to the unaf fected base meta l a t
the r ight. The panoramic view of the
weldment shows seven dist inct types of
microstructures labelled A t h rough C in
Fig.
4 :
A
—
fusion zone. Figure 5 show s the
microstructure of this region as revealed
by a 2% nital etch at X500. The micro-
structure consists of Widmanstatten fer
r ite and f inely laminated pearl i te. The
hardness of this low-carbon weld metal
was only 168 KHN.
B
—
unmixed zone (Ref. 9). The top
section of Fig. 6 shows this zone at X500.
Because mechanical mixing is incomplete
in this zone, the substitutional alloy con
tent approximates that of the base metal.
Carbon, on the other hand, dif fuses so
rapidly that the carbon content is inter
mediate between that of the weld (0.07
wt-%) and that of the base metal (0.31
wt-%). The region consists of bainite,
Widmanstat ten fer r i te and very f ine
pearl i te structures with measured hard
ness of only 280 KHN.
C—homogenized coarsed-grain re
gion. Figure 7 shows the microstructure
of this region at X500. The uniform
response to the etchant within this region
in Fig. 4 indicates it to be reasonably
hom ogen eou s as a result of the high pea k
temperatures experienced in this region.
The micro structure is ful ly martensit ic and
exhibited a hardness of 403 KHN.
D
—
inhomogeneou s fully transformed
region. Within this region the response to
the etchant in Fig. 4 is uneven and the
- >
*
Fig.
5-Region
A in
Fig.
4 at X500 (reduced
46 on reproduction). 2 nital etch
Fig. 6 -
Region
B in Fig. 4 at X500 (reduced
54 on reproduction). 2 nital etch
mott led appearance is indicat ive of inho-
mogeneity. Figure 8 shows a port ion of
this region at X500. The light gray regions
are ful ly martensit ic and exhibited a hard
ness of 403 KHN. The intermediate
regions which consist of a mixture of
e levated- temperature t ransformat ion
products exhibited a hardness of 197
KHN.
Apparent ly region D exper ienced peak
temperatures abo ve the ef fect ive A3 long
enough to complete the t ransformat ion
to austenite but for too short a t ime t o
exper ience homogenizat ion of even the
interstit ial carbon. The austenite grain size
in this region ranges from slightly coars
ened to ful ly ref ined and the hardenabil i
ty var ies accordingly.
E—partially
transformed region (PTR).
This region is character ized by regions of
near ly eutecto id carbon which cor re
spond to the or iginal networks of pearl i te
Fig. 7—Region C in Fig. 4 at
X500
(reduced
52 on reproduction)
Fig.
8 —Region D in
Fig.
4 at X500 (reduced
54 on reproduction). 2 nital etch
Fig.
9-Region
E in
Fig.
4 at X500 (reduced
53 on reproduction). 2 nital etch
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>
• ^
-.
v
*^
• - - % ^
•r tf
%*
jr
-.
S *
(
-
-
E
'
:,
'A
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% . 10-Region F in Fig. 4 at X500 (reduced
46 on reproduction).
2%,
nital etch
• • •
..J .̂
*i* '
*
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1
*
-.
j
-
^
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j
'• 4 0 »
f /g .
11-Region
G in Fig. 4 at X500 (reduced
52 on reproduction). 2 nital etch
in the as-cast microstructure. This region
transforms to high-carbon austenite
whenever the peak temperature exceeds
the ef fect ive
A-i,
and the short t imes-
at- temperature prevent signif icant redis
t r ibut ion of the carbon. Therefore, the
cont inuous
prior-pearlite
ne tworks f o rm
cont inuous networks of h igh-carbon aus
tenite; upon cooling, these have suff icient
hardenabil i ty to t ransform to cont inuous
networks of h igh-carbon mar tens i te . The
hardness of 615 KHN is in the h igh-
carbon martensit ic regions and the low
values of 84 KHN are encou ntered in the
: , ( ,
— m * •
•Ai
:
'.:~3A
Fig.
14—Microstructure of
5 s stationary repair weld in heat 0. Nital etch, X75 (reduced 42 on
reproduction)
untransformed ferr ite islands. Figure 9
show s the loc at ion of E at X500.
F—spheroidized
region. In this region,
the peak temperature exper ienced
be tween the e f f ec t ive Ai and about
900-1000°F (482-538°C). The lamellar
carbides within the pearl i te nodules
spheroidize while the or iginal ferr ite
grains remain unchanged. Figure 10
shows this microstructure at X500. The
average hardness is 163 KHN in the pr ior
pearl i te and about 84 KHN in the pr ior
ferr ite.
C—unaffected base metal. This micro-
structure consists of cont inuous networks
of pearl i te nodules at the dendrite inter
stices as a result of the segregation of
carbon and alloying elements to the last
mater ial to solidify. This means, in ef fect ,
that the as-cast base metal, which has a
nominal carbon content of 0 . 3 1 % , b e
haves l ike a composite mater ial. As a
composite material, it consists of islands
of low carbon fer r i te gra ins (~0.025% C)
complete ly sur rounded by near ly cont in
uous networks of mater ia l wi th carbon
contents ranging f rom approx imate ly
0.5% (the carbon c onten t of l iquid steel at
the per itect ic temperature) to nearly
eu tec to id (~0.8%) composi t ion. F igure
<
o
_i
Q IOOO
Q
CC
<
I
o
o
UNTRANSFORMED
REGION OF
S C ST STRUCTURE
TYPIC L H RDNESS OF
PE RLITE NODULES
FfRJITS : " . » _ _ _ _
_L_
Q
CC
<
I
0 0 050 0 I00 0 I50
DISTANCE FROM FUSION BOUNDARY-inches
Fig. 12 -Results of hardness traverse across regions show n in Fig. 4
11
shows the m icrostruc ture of this zone
at X500. Note that the pearl i te lamina
t ions can be resolved in some areas at
this magnif icat ion.
Figure 12 summarizes the results of a
microhardness traverse across the region
shown in Fig. 4. Attent ion is drawn to the
large spread between the maximum and
minimum hardness values observed in
the part ial ly- t ransformed region. This
ref lects the nonuni form carbon content
of the martensite formed in this region.
Note that the areas of untransformed
ferr ite in this region exhibited hardness
values ranging from 77 to 94 KHN. An
approximate scale of
Re
hardness is
included at the right side of Fig. 12 for
comparison with calculated hardness
data presented ear l ier.
Homogenizat ion Stud ies
The results summa rized in the previous
sect ion clear ly indicate the dangers of
repair welding as-cast steel structures. It is
Fig. 13 — As-cast and normalized heat 0 micro-
structures: A
—
as-cast;
B
—normalized. 2 nital
etch, X250 (reduced 44 on reproduction)
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IOOO
o
o
o
o
m
9 5 0 0 -
cn
a
tr
<
I
a.
o
o
' *
0 0 . 0 5 0
0.100
D I S T A N C E F ROM F US I ON B OU NDA RY - in c h e s
Fig. 15 —Results of hardness traverse across the regions in Fig. 14
Fig. 18 — Tempered martensite in Fig. 17 at
X500
(reduced 52 on reproduction). Nital
etch
Fig. 16 —M icrostructure of 5 s stationary repair weld in normalized heat
27. Nital etch, X75 (reduced 55 on reproduction)
Fig. 17 — Microstructure of 5 s stationary repair weld in normalized heat
27 with postweld tempering at IIOVF (593°C) for 1 h. Nital etch, X75
(reduced 55 on reproduction)
vir tually impossible to choose welding
condi t ions which prov ide cool ing rates
suff icient ly slow to prevent the format ion
of cont inuous networks of crack-sensi
t ive microstructures in the regions which
experience part ial t ransformat ion to aus
tenite.
The hardness levels identif ied in these
regions are far above those shown to be
acceptable for avoid ing hydrogen-
induced crack ing even wi th good low-
hydrogen pract ice. Thus, i t would be
dif f icult , i f not impossible, to make repair
welds in as-cast steels without the risk of
forming microcracks in the high-carbon
mar tens i t ic networks. In fact, hindsight
n ow suggests that the lack of qu ant itat ive
cor re lat ion between the acoust ic-emis
sion studies and ident if iable hydrogen-
induced cracks is at t r ibutable to this phe
nomenon.
Unfortunately, microcracks in these
hard br it t le ne two rks in the part ial ly t rans
formed region can serve as nuclei for
s low crack growth even af ter postweld
heat t reatments. Therefore, i t appears
that the only sure way to avoid this
problem would be to e l iminate the net
works of interdendrit ic pearl i te nodules
by a homoge niz ing t reatment pr ior to
weld ing. Thus, 10 X 4 X V2 in. (254 X
102 X 13 mm) specimens from each heat
we re no rmalize d at 1750°F (954°C) for 2
h.
Figure 13 compares the as-cast and
normalized microstructures at X250. Note
the complete e l iminat ion of the cont inu
ous networks of pearl i te that results f rom
CC
F-
Q.
M
<
n
UJv
5
UJ /
r /
Q.
CO
Q
UJ
r
O UJ
w z
r
0
<
Z.
z>
->
CQ
~ I 0 0 0 ° F
Fig. 19—Schematic of various regions produced in steel casting repair welds: FZ—fusion zone;
UM Z — unmixed zone; PMZ—partially me/ted zone; HAR — homogeneous austenite region; HA Z—
heat-affected zone; CG—coarse grained; E.G.—fine grained; PTR — partially transformed
region
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Figure 14 shows a panorama of a weld
Figure 15 is a plot of the microhardness
se run on the w eld sho wn in Fig.
4. Comparison with Fig. 12 clear ly indi
Although these plots are for welds
1200 KHN in the weld m ade in the
Figures 16 and 17 show microstruc
wi t h and wi th out a postw eld temper
1100°F (593°C) for 1 h. The we ld in
16 was no t t empered and showed
hard
Re. However ,
Re.
Figure 18 shows this
The var ious zones, which are pro
lding of steel castings, are sum marized
gen -induc ed cracking is the p art ially
It is apparent from the above results
of hydro gen- induced crack ing
reases in bo th the alloying con tent and
Conclusions
The following conclusions pertain to
the hydrogen-induced cracking studies of
repair welds in steel castings.
1 .
The metallurgical factor was
con
t rol led by using the method descr ibed
previously to select combinat ions of
weld ing condi t ions which produced both
crack-sensitive and crack-insensitive mi
crostructures in typical case steel speci
mens.
2. The chemical factor was controlled
by modifying the moisture content of the
E7018 electrode coat ings.
3. The mechanical factor was synthe
sized by applying a controlled
aug
mented st ra in to SMA welds deposi ted
on simple rectangular specimens.
4 .
Acoust ic-emission techniques were
employed to monitor the init iat ion and
growth of hydrogen- induced crack ing.
5. The results conf irm the fact that
proper low-hydrogen pract ice is manda
tory for al l repair welding operat ions if
hydrogen-induced cracking in the coarse
grained heat-af fected-zone is to be
avo ided.
6. The suscept ibil i ty to hyd roge n-
induce d cracking is direct ly related to
both the maximum hardness in the heat-
af fected zone and the level of dif fusible
hydrogen .
7. Hydrogen-induced cracking can be
prevented by us ing good low-hydrogen
pract ice if the maximum hardness in the
heat -af fected zone is kept belo w Re 35.
8. Since the maximum hardness in the
heat-affected_ zone is direct ly related to
the carbon content , reduct ion in the
carb on con tent is the simplest way to
improve the weldabil i ty of steel cast
ings.
The following conclusions pertain to
the results of microstructural studies of
repair welds in steel castings:
1 . For cast steel repair welds one can
identify seven distinct regions by a nital
etch.
2. The part ial ly- t ransformed region of
the heat-af fected zone of repair welds in
as-cast steel was found to have the
microstructure most suscept ible to
hydrogen- induced crack ing.
3. Cont inuous n etworks wi th hard
ness levels ranging from 600 to 1200 KHN
(50 to 70 Re) were ident if ied in the
part ial ly- t ransformed region.
4 . The problem in the part ial ly- t rans
formed region ar ises from the interden
drit ic segregation present in the as-cast
material.
5. Normalizing eliminates the problem
in the part ial ly- t ransformed region by
homogenizat ion.
6. All steel castings should be normal
ized before repair welding to minimize
problems in the part ial ly- t ransformed
region.
7. As the alloy content is increased,
postweld-heat t reatment may become
desirable.
Acknowledgments
The authors wish to thank Mr. Dan
Stone and the Associat ion of American
Railroads (AAR) for its f inancial support of
this project .
References
1.
Rogers, H. C. 1956. The influence of
hydrogen on the yield point in iron. Ada Met.
4(2):114-117.
2. Savage, W . F., Nippes, E. F., and Homm a,
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to 376-s.
3. Frohmberg, R. P., Barnett,
W.
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Troiano, A. R. 1955. Delayed failure and
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I.
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