on
THE FUNDAMENTAL FACTORS INFLUENCING
THE BEHAVIOR OF WELDED STRUCTURES:
The Effect of Subcritical Heat Treatment on the Transition Temperature of a
Low Carbon Ship Plate Steel
by
E. B. Evans and D. J. Garibotfi
CASE INSTITUTE OF TECHNOLOGY
Transmitted through NATIONAL RESEARCH COUNCIL'S
COMMITTEE ON SHIP STEEL Advisory to
SHIP STRUCTURE COMMITTEE
tAEORATOPJUM VOOR
riL±I
L)lN.)I
Division of Engineering and Industrial Research
National Academy of Sciences National Research Council
Washington, D. C. October30, 1953 SERIAL NO. SSC.61
LAEORATOJUM VOOR
0096
Fifth PROGRESS REPORT (Prolect SR-99)SHIP STRUCTURE COMMITTEE
October 30, 193
Dear Sir:
As part of its research program related to the
improvement of hull structures of snips, the Ship
Struc-ture Committee is sponsoring an investigation on "The
Fundamental Factors Influencing the Behavior of Welded Structures under Conditions of Multiaxial Stress and Variations of Temperature" at the Case Institute of
Technology. Herewith is a copy of the Fifth Progress
Report, SSC-61, of the investigation, entitled "The Fundamental Factors Influencing the Behavior of Welded
Structures: The Effect of Subcritical Heat Treatment
on the Transition Temperature of a Low Carbon Ship Plate
Steel" by E. B. Evans and D. J. Garibotti.
The project is being conducted with the advisory assistance of the Committee on Ship Steel of the National Academy of Sciences-National Research Council.
Any questions, comments, criticism or other matters
pertaining to the Report should be addressed to the
Secre-tary, Ship Structure Committee.
This Report is being distributed to those individuals
and agencies associated with and interested in the work of
the Ship Structure Committee.
Yours sincerely,
K. K. COWART
Rear Admiral, U. S. Coast Guard
Chairman, Ship Structure Committee
MEMBER AGENCIES: ADDRESS CORRESPONDENCE TO:
BUREAU OF SHIPS. DEPT. OF NAVY SECRETARY
MILITARY SEA TRANSPORTATION SERVICE. Dipl. OF NAVY SHIP STRUCTURE COMMITTEE
UNITED STATES CO.ST GUARO. TREASURY DEPT. U. S. COAST GUARO HEADQUARTERS
MARITIME ADMINISTRATION. DEPT. OF COMMERCI WASHINGTON 25. D. C.
FI FTH
Progress Report (Project SR-99)
The Fundarnenal Factors Influencing the Behavior of' Welded Structures: The Effect of' Subcritical Heat Treatment
on the Transition Temperature of a Low Carbon Ship Plate Steel
by
E. B, Evans D JG Garibotti
CASE INSTITUTE OF TECHNOLOGY
uride r
Department of the Navy Bureau of Ships NOBS--i-51+7O
BuShips Project No0 NS_011_076?
for
TAELE OF CONTENTE
i
Table of' Contents . . o 3
i
L Ist of Ftiures 11 kbstract iii Introuuction e e a o e t
e tOCO
i
iaterial t Q o a o o o s s o o o o e e s o o o o 2 Proceciure e s o o o o e o s e e e e o o t o e o 3 Results Hardness Tests s o o o e e o e s o o e o e e 1+ Impact Tests o s s e e e o e o o o e O Ioicrostructtres e o e e 0 0 0 0 5 0 0 5 0 0 11+ DJ_SCU.SS1.Ofl© s o o s o e e o s e e s o e o o o e e e o 15' Corìclusion.s . , Future 1iork . t e t t t o e o o s t o i e o o o o o e e o e s e o o 23 21+ Bibliography . . e Q e o o 25'LIST OF FIGURES
Title Page
l Effect of Various Aging Times and Temperatures on
the Hardness of "C" Steel after Water Quenching from 13000F o a t e a e e e * o o s a e o o o
2 Charpy V-Notch Transition Curves for As-Received
urn - -î
O O a e Q o o Q Q Q Q O Q O e o o o
3 Charpy V-Notch Transition Curves for "C" Steel Suberiticaily heated at 1300°F for
15
Minutes and Air Cooled0 t O O Q O Q O *
+. Charpy V-Notched Transition Curves for "C" Steel
SubcriticaJjy heated at 1300°F for
15
Minutes and Water Quenched0 Aged at RooTemperature for Times Indicated G Q 11
Charpy V-Notched Transition Curves for "C" Steel Subcriticafly Heated at 1300°F for 15
Minutes and Water Quenched0 Aged at 125°F
for Times Indicated . . . 12
Charpy V-Notched Transition Curves for 1tC" Steel Subcritically Heated at 1300°F for
15
Minutes and kater Quenched0 . . 12
7 Charpy V-Notched Transition Curves for "C" Steel Subcritically heated at 13000F for
15
Minutes and Water Quenched0 Aged at 600°F
for Times Indicated . . . O O G O t O 0 13
Summary Curves Shoving Effect of Various Aging
Temperatures and Times on the Transition
Temperature and Hardness of "C" Steel0
Specimens Water Quenched from 13000F before
Aging a o o o o e o o a o o a o o o e e 13
l4icrostructures of As-Received and Various
Quench-Aged Conditions . . 16
Effect of Room Temperature Aging Time on the
Transition Temperature and Hardness of "C"
Steel after Water Quenching from Temperatures
Indicated . . . . 18
11 Solution and Room Temperature Aging Effects on the Hardness and Impact Properties of "C"
Steel . . . , . . . 20
ii
5.
9
AB STRACT
An investigation was made to determine the impact transi-tion temperature and hardness changes attndant to the
quench-aging of Project Steel "C" a semi-killed ship plate steel1
Aging temperatures xtended over the range from 35 to 1100°F
after water quenching from 1300°F0
Both impact and hardness tests revealed that this steel can be severely embrittled by the quench-aging mechanism0 With aging temperatures up to 350°F, characteristic aging curves were obtained, i.e, the peak embrittlement and the time to attain this peak d&reased with increasing aging temperature0 For room temperature aging this peak amounted to a 900F increase
in transition temperature and
25
points increase in Rockwell Bhardness above that of a series air cooled from 1300°F
(unembrit-tied condition)0 Specimens aged above
350°F
overaged so rap-idly that no peak in the aging curve could be detected0Metallographic examination of quench-aged specimens at 2000X showed that a two-stage precipitation reaction was
operative0 At low aging temperatures the precipitate was detected as a mottling of the ferrite grains; at higher aging
temperatures, where an overaged condition was rapidly reached,
the precipitate had grown so as to be resolvable0
It is believed that the quench-aging phenomenon is
re-sponsible for the ittle zone previouslfound in the
sub-critically heated region in weidments of this and similar ship
plate steels. This study suggests that a low temperature post
heat at 65O°F (the solution temperature below which quench-aging effects are absent) would lead to rapid overquench-aging in the brittle zone of ship plate weidments and thus largely eliminate
the embrittlement
INTRODUCTION
This Is the fifth and last progress report on the study of the zone of brittleness located adjacent to welds In
semi-killed steel plates0 The project has been sponsored by the Ship Structure Committee under Department of the Navy, Bureau
of Ships Contract Nob +5+7O and covers the period from
September 1, 1952,
to December31, 1952e
The earlier reporton this phase of the investIgatIon covéred the work from
January 1, 1950, to September 1,
1952
Three ProgressRe-ports, SSC_21+(2), SSC-3i-3 and SSC-5+ summarized the
work on eccentric notch tensile testing of ship plate weld
ments under the same contract over the period from July 1,
l9+7,
to January 1,1950e
In previous work reported (1) lt was shown that sub critically heated C steel* base plate could be embrittled, as a result of weldlng In a zone adjacent to the weld0 This
evidence was obtained with changes in transitIon
temperature
(eccentric notch tensile and Charpy V-notch) and hardness0 The degree of embrittlement increased with IncreasIng (1)
solution temperature in the 1lO0-120C°F range, (2) cooling
rate, and
(3)
room temperature aging time and wasdecreased
by accelerated aging0In view
of the fact that quench-aging is belIevedrespon-sible for the zone of minimum ductility found in ship plate
*The designation !C refers to Steel C In the series of Ship Structure
Committee
Project"
Steels.
-2-weldments** in a region not heated above the lower critical temperature at any time(i), it was considered advisable to
investigate the maximum embrittlement possible in this grade of steel by quench-aging and how to minimize or eliminate it0
To this end, Charpy V-notch impact specimens were solution heat treated at the maximum subcritical temperature (1300°F), water quenched, and then aged for various periods of time in the 35°
to 11000F range. The embrittlement was ev.luated by
transi-tion temperature and hardness changes, supplemented by
microscopic examination.
MATERIAL
The semi-killed, ship plate steel (C Steel) used in the present work was the same 3/1-in. thick, as-rolled plate
(Plate II) which supplied specimens for the earlier work on subcritical heat treatment0 The properties reported for this
steel are as follows:
TABLE I
PROPERTIES 0F C STEEL PLATE Chemical Analysis Carbon 0,2+ Copper 0Q03 Manganese 0.18 Chromium 0.03 Phosphorous 0.012 Molybdenum 00005 Sulfur 0.026 Tin 0.003 Silicon 0.05 Nitrogen 0.009 Aluminum
0016
Vanadium 0,02 Nickel 0.02 Arsenic0001
Mechanical PropertiesYield Point Tensile Strength Elongation
Psi Psi Per cent
j9,000 F7,'fC0 25.5 (8e' gauge)
**At least for weldments made of A and C steels, the two
PROCEDtJBE
Ten impact blanks (0+2O" square) were cut from the as rolled plate so that the long axis of each specimen was
perpendicular to the rolling direction0 These blanks were
used as hardness check specimens after heat treating at 1300°F
for
15
minutes in a neutral chloride salt bath*0 OnespeeL-men was air cooled while the remaining nine were water quenched0 Each of the quenched specimens was then aged for various times
in an appropriate bath of water, oil, or tempering salt at one of the following temperatures: 350, room temperature (800),
125°,
2O0,
2500,350°,
600°, 900°, and 1100°F0 All specimenswere air cooled froni the aging temperatures0
The as-quenched'1 hardness was taken in about five minutes after quenching0 In following the progress of aging, specimens
were removed from the
aging baths for
a time only long enoughfor the hardness tests to be made0
With the hardness checks as a guide, series of Charpy
V-notch impact blanks were taken from the plate
in
the samemanner, quenched from 13000F, and aged for various times at
room temperature, 1250,
35Q0,
and 600°F0 In addition, one series was air cooled from 13000F to give the unembrittled eondition0***The composition of the neutral chloride salt was asfollows:
BaCi2 55% NaC1 22%
ICC1 22% "Dicy" 1%
**The Transition Temperature of this series was approximately
the same as that of the as.received material0 In addition, hardness checks of broken specimens showed no change with
After aging, the specimens were immediately ground to
size and the notch cut perpendicular to the surface of the
plate, with each series being machined and tested within
seven hours after aging0 The impact testing procedure was
the same as given previousiy. As pointed out in the
earlier work, the possibility exists that accelerated aging
can occur in the testing bath0 In establishing the transi-.
tion curves, it was necessary to test as high as 350°F
(specimens were held 10 minutes in the bath to assure tempera-ture uniformity), and thus, accelerated aging in the test
bath may occur in those specimens previously aged at room
temperature and 125°F. Hardness checks made on specimens
from these series before and after breaking indicated that the
hardness was unaffected up to testing temperatures of
175°F0
In view of the fact that the 15' f tJb transition temperature
is to be used as the criterion of embrittlement and in no case did this exceed 175°F, the results would appear to be unaffected
RESULTS Hardness Tests
The Rockwell B hardyìesses obtained after aging in the
35°
to 1100°F range are shown as a function of the aging time in
Fig. L
From an as-quenched hardness of R8?, the hardness of the
specimen aged at room temperature (80°F) remained unchanged
00 95 90 > 85 -J
'A
-J bi 80o
o
loS -4
65 1250 F 2000F 250°F AS QUENCHED FROM 1300°Fï1v+uIo'
AS- RECEIVED 7 6000F 900°F 1100°F 0.0_00 D_D . D.-V.
ALL SPECIMENS AIR COOLED FROM AGING TEMPERATURE/
\ 35°F 80°F 350°F 1 1000 10,000LOG AGING TIME-1HOURS
FIG. i:
EFFECT OF VARIOUS AGING TIMES AND TEMPERATURES ON THE
HARDNESS OF IsOli STEEL AFTER WATER QUENCHING
FROM 1300°F.
x.AIR COOLED
FROM 1300°F o 0.1 IO. lOO
-o-level of RB96 after five days0 Aging at a lower temperature
(35°F)
resulted in a slower rate of increase and a longertime (about 50 days) to reach a slightly higher peak level
of RB9?o
With increasing aging temperatures above room temperature
to 250°F, the hardness increased at an ever increasing rate;
but the peak hardness reached and the time to reach this peak
decreased0 Once the peak had been attained, further aging time caused a decrease in hardness at a rate which increased with aging temperature0
At 350°F and higher the hardness did not rise above that of the as-quenched specimen but fell off at a rate which again
increased with temperature0
A summary of the maximum hardness reached and the time to reach this maximum for the various aging temperatures
employed are given in Table 110 TABLE II
EFFECT OF AGING TEMPERATURE ON THE PEAK HARDNESS REACHED AND TRE TINE TO ATTAIN
THIS PEAK
Aging Peak Hardness Time to Reach
Temperature, °F Reached, RH Peak Hardness
35
9750 days
80
96 5 days125
95
23 hours
200 91 2 hours
250
8815
minutes350
Not higher than as-quenched hardness of RB87
t; 600
900
1100
Note: All specimens water quenched from 1300°F prior to
aging0 Hardness of specimen air cooled from
1300°F
These results show that by aging the hardness can be raised
a maximum of about 10 points above that of the as-quenched
hard-ness (RB87)O In turn the as-quenched hardness was 17 points Rockwell B above that of the air cooled hardness (RE7O)o The maximum cumulative hardness increase due to solution and aging
then amounts to about 27 points REO
Iinact Tests
The impact transition temperatures by three criteria
obtained of the (1) as_received*, (2) air cooled, and
(3)
the various quench-aged conditions are summarized in Table IlL The individual transition curves for each condition are plottedin
Figs0
2--7 with both the energy absorbed and the per centfibrous fracture plotted as the ordinate.
In the following sections of the report, the effects of the various subcritical heat treatments are evaluated with the 15 ft-lb transition temperature as the criterion of embrittle-ment and with the properties of the air cooled series reflecting
the unernbrittled state. The choice of either of the other two
criteria listed would reveal the same general effects0 In comparing the impact properties of the as-received
plate,
Fig0
2, with those of the air cooled series, Fig 3,it Is evident that there is little difference in properties other than about a five ft-lb higher upper level for the air
cooled series0
The transition curves after aging for various times at *Previously reported (1)
CEARPY V-NOTCH TRANSITION TEMPERATURES AND HARDNESSES OF C STEEL AGED AT VARIOUS TEMPERATURES AND TIMES AFTER WATER QUENCHING
FROM 13 00°F
Transition Temperature,
50 Fibrous Rockwell B
Aging Tizne Mid.point* Fracture** 15 Ft_Lbs*** Hardness
As-Received *Tempera ture curve **Temperature temperature ***Temperature
TABLE III
NOTE: Only the aging times for impact specimens aged at
room temperature include the seven hours required for machining and testing0
at midpoint of absorbed energy-test temperature
at midpoint of per cent fibrous fracture-test
curve s
at 15 ft-lbs were absorbed.
118 138
Air Cooled from
100°F
85
85
75
70
118
11+5Aged at oom Temperature
5 minutes
87
7 bourn
175
n S
883 days
i8o
212
158
91F 5 dayz 175 210 160 96 32 days202
230175
96 +5 days 175 96 Eed at125°F
1 i/+ hours 150 200 127 91 7 1/2 hours185
215162
93 21 hours188
218
168
9 3 days 182 208 ged at 50°F 168 915
minutes 133 160115
87
i 3/1+ hours 125160
100
8319
hours122
i1+8gd
at00°
9881
2 minutes 120155
93 83 10 minutes125
15295
81
I-z
w O C.) w Q- 20 4O D I-o
4
1h. 80 u) Do
loo -80FIG. 2
CHARPY V-NOTCH
TRANSITION
CURVES
FOR AS-RECEIVED
"C"
STEEL.
o 20 40 60 80 (n D I00
80
L'. -9-0 80 60 240 TEST TEMPERATURE --' 0 80 60 240 TEST TEMPERATURE ' 320 320 400FIG. 3
CHARPY V-NOTCH
TRANSITION CURVES
FOR "C" STEEL
SUBCRITICALLY
HEATED
AT
300°F FOR
15 MINUTES AND
AIRCOOLED.
50 40 30 20 lo I-O4
a. o,
400 50 40 30 20 lo o s.
.
>
,:
\
,Ip.._.00
SS'./\
-10-room temperature, 1250, 350°, and 600°F, are presented in
Figs0
Lf.7,
respectively0 In all the quench-aged series the upperlevel of the individual absorbed energy-test temperature curves
is lower than that for the air cooled series0 In general, a
greater difference in levels is associated with a greater degree of embrittlement, with the maximum difference being about 12
ft-lb0 The degree of ernbrittlement can be more readily seen
in the summary of the 15' ft-lb transition temperature plotted
as a function of the aging time, top of Fig. 8, for the various
aging temperatures employed0 For comparison purposes the com
parable hardness data are plotted in the bottom of this figure0
For room temperature aging (80°F), it can be seen that after seven hours aging the transition temperature (115°F) is
30°F higher than that of the air cooled series (85°F)0 With
increasing aging time, the transition temperature increases,
reaching a maximum level of 175°F at some time greater than five
days but less than 32 days0 This is an increase of 900F over
the unembrittled state0 Although no data were obtained for aging times less than seven hours (this was the minimum time
for machining and testing), it is not expected that the transition temperature would be appreciably lowered for the shorter aging
times because the hardness increased but one point during the first seven hours of aging0 The aging curve at the shorter
aging times has been interpolated to give an as-quenched9
20 40 60 80 00 20 40 o 60 80 lOO o 20 40 60 80 lOO
FIG. 4.(A-E):
CHARPYFOR "Ce' STEEL 1300° F
FOR 15 AGED AT ROOM INDICATED. 50 4° 30 20 (O o 50 40 30 20 o 50 40 30
VNOTCHED TRANSITION CURVES SUBCRITICALLY HEATED AT MINUTES AND WATER QUENCHED. TEMPERATURE FOR TIMES
o 20 40 60 80 'oc o ,, 20 D o 40 u. 60 FIG. 4 CONTINUED 50 40 30 20 I0 o 5° 40 30 20 Io o
u
(A) - AGED 7 HOURS W1b o-s.
'
/
3-r
(B) AGED -DAYSoo.o
'UtIO O.
. o s IO\
co-o-I---(C) AGED jo 5 O DAYS o.IuIIIIo. o coo I o../
'4,
s.,
0l\
-!
(D) AGED 32 r I DAYS r i o\\
/Sr'
4,. o -(E) AGED 45 DAYS Io o 80 100 -80 o 80 60 240 400 360 400 320 -80 0 80 60 240 TEST TEMPERATURE -TEST TEMPERATURE"-Fa) 0 20 40 60 80 100 O 20 40 60 80 IOU o 20 (n 40 o 60 80 loo o 20 40 60 80 lOO o 50 40 30 20 Io o 50 40 30 20 40 lo o 50 40 FIG. 5: (A-D)
CHARPY V-NOTCHED TRANSITION CURVES
FOR
ICC
STEEL SUBCRITICALLY HEATED AT 1300°F
FOR
15 MINUTES AND WATER QUENCHED. AGED
AT 25°F FOR TIMES INDICATED. loO (A) AGED 15 MIN. (0) AGED o O O -f
--.4-1
o o I 3/4 HRS.± (G) AGED 9 HOS. . oL
o 0O.0-° 20 TEST TEMPERATURE--F Io FIG. 6 (A-c)CHARPY VNOTCHED TRANSITION CURVES
O
FOR "C" STEEL SUBCRITICALLY HEATED AT 1300°F
400
FOR
IS MINUTES AND WATER QUENCHED,
AGED AT 350°F FOR TIMES INDICATED.
t
50 40 30 20 - Io o 50 40 30 20 50 40 30 20 IO o (A) AGED I 1/4 1F'°'0hu1b HOURS°L
._.-'i--i
/2 HOURS o o (B) AGED 7 00O -"aL . $:l
I I St
--O___
I O O 0O 0' (G) AGED 21 . HOURSo-0
0. o Jrv
S .4 's-I
._
s....
o OOO 0 ID) AGED 3 DAYS O.r..O%OO -J. s-S-1..S
_________. .
Oo
-80 O 80 60 240 320 TEST TEMPERATURE -'-F 30 -80 O 80 160 240 320 400 50 40 30 20 20 40 Io 60 80 lOO o 20 40 60 80 60 80 lOO O 2040 w o 60 Q. 80 w loo g-. o gr 20 u. 40 o gr o 20 60 u. 80 00 50 40 30 20 Io o 50 40 30 20 Io o 200 190 80 170 w 160 gr I-. 150 -.1 w I. Q. g-. 140 u-w 'n'-30 C -FA R PV 125°F V- NOTCH
D
120----4 IO --660°F 790--AS RECEIVED OR AIR COOLED FROM
300°F 8oL* 350°F 00 80°F
U)I'
125°F--I AS QUENCED 8O°F 90 y ._- 350°F 85 80 L -AS RECEIVED7Ox.-AIR COOLED FROM 1300°F
-65 60 IO IO,) 1000 10,000 LOG AGING TIME-s'HOURS FIG. 8SUMMARY CURVES SHOWING EFFECT OF
VARIOUS AGING TEMPERATURES AND TIMES ON THE TRANSITION TEMPERATURE AND HARDNESS OF "C" STEEL. SPECIMENS WATER QUENCHED FROM 1300°F BEFORE AGING.
(A) AGED 2 I MIN
I,'
IO o-.00_.o IB) AGED I MIN. ._I_-Ir.l.-___ 0% -80 0 80 60 240 320 400 TEST TMPERATURE-'-°F FIG. T ABCHARPY V-NOTCHED TRANSITION CURVES
FOR "C' STEEL SUBCRITICALLY
HEATED AT 1300°F
FOR
15 MINUTES AND WATER QUENCHED.
AGED
AT 600°F FOR TIMES
The transition temperature--aging time relationship for
125°F aging-- shows that the transition temperature starts to
increase at much shorter times, reaching a peak (168°F) after about 20 hours and remaining at this value at least up to
three days aging time0
For 350°F aging it appears that a slight peak may be
present at an aging time less than 15 minutes, but it probably
would not be much greater than the 115°F transition
tempera-ture obtained after 15 minutes aging because the hardness was
unchanged during this time intervaL Aging beyond 15 minutes
results in a decreasing ernbrittlement with time0
Aging at 600°F for two and ten minutes, respectively, effects a considerable improvement in the impact properties For both cases the transition temperature indicated an
embrit-tiement of but 10°F0
From the general trend of these aging curves, it is to be expected that at aging temperatures higher than 600°F the
impact properties would approach those of the unembrittled state very rapidly However, as will be pointed out in the Discussion, this conclusion only holds for specimens cooled
relatively slowly from the aging temperature; a fast cool from aging temperatures above about 6500 can introduce another
quench-aging cycle0 4i cro structure s
-1 5
quench-aging, a number ot specimens representing various quench
aged conditions were examined at 2000X.
The structure of the as-received condition is shown in Fïg0
9(a)0 No difference in structure was noted in the air cooled
condition; however, Immediately after quenching, a mottled
ferrite was evident which did not appear to change with time
at room temperature0 Fig0 9(b) shows the structure after one
month at room temperature No change in this mottled structure
was revealed after aging at 125°F, even after 23 days at this
temperature, Fig0 9(c).
After aging 15 minutes at 350°F, the mottled ferrite 'was still in evidence; after 21 hours at 350°F, Fig. 9(d), the mottled structure appeared to be more intense.
Upon aging at 600°F for two minutes, a precipitate, evenly distributed throughout the mottled ferrite grains, was
resolvable. An increase in aging time to ten minutes, Fig. 9(e), resulted in better definition of the precipitated particles,
which appeared to be platelets, and an increase in their size.
After aging ten minutes at 1100°F, Fig. 9(f), the precip Itate is no longer evenly distributed throughout the ferrite grains but appears to have coalesced along the grain boundaries
as spheroids.
DI SCUSSION
On the evidence of the hardness properties,
Fig0
1, aging curves were obtained which were characteristic of quench-aging(a)
As-1eceived
(d)
Aged 21 Hours at 30°F
(b)
Aged 30 Day5 at Room Temp er ature
(c) Aged 23 Days at 12°F. 1 s
t m
(e) Aged 10 Minutes at 600°F (f) Aged 10 Minutes at 1100°F Fig. 9:MICR0STRUCTU1ES 0F AS-PECEIVED AND VARIOUS QUENCH-AGED CONDITIONS.
J11 aging treatments preceded
by a water quench fran 1300°F.
2000X,
l7-systems, 10e0, the maximum hardness attained and the time to reach this maximum decreased with increasing aging temperature0
The similar changes observed with the impact transition
temperature, Fig0 8, are believed to be new experimental data0
The only information found on the impact transition temperature changes due to quench-aging in a similar grade of steel was
in the work by Low':6) and was restricted to the room tempera-ture aging effects0 In this paper it was shown that after
quenching from 700°C (1290°F) the transition temperature
in-creased continually over the aging interval of three years0
The total increase amounted to a 110°F rise in Charpy keyhole
transition temperature (10 ft-lb value), with the greatest in-crease occurring in the first ten days aging0 This work was
done with a 1/2-inch hot rolled semi-killed plate containing
0l7% carbon0
In conjunction with the earlier work under this project,
it is now possible to show, Fig0 10, the effect of solution
temperature on the magnitude of the peak transition tempera-ture and hardness reached by room temperatempera-ture aging0 As is
evident, increasing the solution temperature in the 11000 to 1300°F range results in a greater initial (as_quenched!)
hardness and, apparently, a greater initial transition
tempera-ture0 Upon subsequent room temperature aging, the magnitude
of the peak also increases with increasing solution temperature0
E 20 (n
z
110 loo 90 80 loo --V 95 90 70 65 X 60 o CHARPY V-NOTCH u AS RECEIVED RECEIVED -18-85 L D D 80 -I3OO°Fo. 00
F o d00 1100°F 0,1 IO 00 1000 10,000LOG AGING TIME -'- HOURS
FIG. io:
EFFECT OF ROOM TEMPERATURE AGING TIME
ON
THE TRANSITION TEMPERATURE AND HARDNESS
OF 'G" STEEL AFTER WATER QUENCHING FROM
TEMPERATURES
INDICATED.
200 90 80 40 30z
o
i 9
which show that a greater change in properties can be expected with increasing solution temperature (greater degree of super
saturation)
To obtain a quantitative measure of the solid solution and the aging effects as a function of solution temperature
from room temperature to 1300°F, Fig0 il has been prepared0
Here for each property three heat treated conditions are under
considerations (1) air cooled, (2) as-quenched, and
(3)
quenched and aged one month at room ternperature The air cooled datasets the base line for evaluating the two effects because in this condition it is assumed that the solid solution and aging effects are absent*0 The difference between the'as-quenched properties and the base line then yields the effect due to solid solution,
whereas the difference between the as-quenched and
'quench-aged' properties gives the effect due to aging0 The aging e-feet may be altered for aging times greater than one month, but it is believed that the change would be slight, if any, and therefore the effect shown may be considered a maximum0
This figure also shows that below a solution temperature of about 650°F the solid solution and aging effects are nil but that above this temperature both effects increase with increasing
solution temperature0 It is interesting to note that the hard-ness is affected to a greater extent than the transition tempera-ture by the solid solution effect, whereas the reverse is true
*Hardness checks showed no change with time at room
lOO 95 90 85 80 75 70 65 190 180 u-s 170 160 w 150
w
Q. 140 130 20l'o
100 90 80 AS REC,EIVED'Io
AS RECEIVED o -20-HARDNESS > AIR COOLED O AS QUENCHED (WATER) QUENCHED AND AGED AT ROOM TEMPERATUREFOR ONE MONTH.
CHARPY V-NOTCH AGING EFFECT°
\
SOLID SOLUTION/
EFFECT-I
AGING- F-..
EFFECT\ t.L ru-
-w 0 200 400 600 800 1000 1200 400 SOLUTION TEMPERATURE-FIG.
II
SOLUTION
AND ROOM TEMPERATURE AGING
EFFECTS ON
THE HARDNESS AND IMPACT
-21-with aging0 In any case the two effects are interrelated and
governed by the solution temperature which in turn controls
the amount of carbon available for the precipitation reaction0
With cooling rates intermediate to an air cool and water quench, it is to be expected that these two effects will be
minimized due to the lower degree of supersaturation, i0e., less
carbon is retained in solution on the quench0
From the metallographic changes occurring during aging,
it would appear that a two-stage precipitation reaction is
operative. The first stage (evident as a mottling of the fer-rite) was responsible for the greater degree of embrittlement,
while the second stage, in which a resolvable precipitate was detected, was associated with an improvement in properties
corresponding to a rapid overaged'condition0 Although no
attempt was ¡nade at identification, the sequence of micro-structural changes observed appear to be the same as reported recently
(7)
In this paper the metallographic changes occurringduring the quench-aging of an ingot iron (0.026 carbon) were
followed by means of the optical and electron microscopes, and the identification of the two-stage precipitate made with
electron diffraction technique0 The first stage was identified
as the hexagonal E-iron carbide after
l5
hours at 200°C (390°F)0The second stage was associated with a change in the crystal lattice to cementite, (orthorhombic Fe3C), observed after aging
-22-It can now be speculated that in the aging of C steel the formation of the transition lattice (&-iron carbide) is associ-ated with a high degree of embrittlement, while subsequent
formation of the equilibrium phase (cementite) brings about a large improvement in properties, corresponding to the rapid
overagedt condition0
Insofar as microstructural changes are concerned, the brittle zone previously found in the subcritically heated region in ship plate weidments has not been identified with a
precipitation reaction*0 However, due to the complexity of the temperature, time at temperature, and cooling rate condi-tions in multiple pass weldments, it is difficult to determine
the exact quench-aging cycle experienced. It has been shown previously (i) that the cooling rate in the subcritically heated region** is such that the ferrite is not supersaturated to the
maximum possible
as in ater quenched test specimens0Conse-quently, less carbon is available for the subsequent precipita-tion reacprecipita-tion, and the resultant precipitate may not he detected***
In regard to the changes in hardness and transition tempera-ture, the results of this investigation give the maximum possible
*It should be recalled that the demonstrated beneficial ef-fects of increasing preheat (decreasing cooling rate) and postheating (overaging' certainly point to the
quench-aging mechanism0
**The cooling rate at the critical zone was found to be intermediate to water quenched and air cooled impact test specimens0
is not expected that the electron microscope would be
able to detect any precipitation0 In the reference cited
in the Discussion (7), the only advantage of the electron over the light microscope was in better resolution of the
-23-embrittlement of C steel by quench-aging, Fig. 11. Any
treat-ment designed to remove these effects in the base plate should be applicable to weidments made of this and similar grades of
Steele As was shown in Figs0 i and 8, overaging' treatments
served to minimize the ernbrittiement, with the degree of em brittlement decreasing with increasing aging temperature.
However, this finding must be qualified in view of the fact
that the results were based on specimens air cooled from the aging temperatures0 A consideration of Fig. ii shows that
if aging temperatures above 650°F were used, then the pos-sibility exists that another quench-aging cycle could be initiated if a fast cool were employed0
(Low6,
using a different approach, arrived at the same conclusion) There-fore, the postheating of weldments susceptible to quench-aging should be restricted to a maximum of about 650°F when this danger exists. As this investigation showed, aging in this neighborhood (600°F) effected a rapid and considerable improve-ment in the ductility by 'overaging.CONCLUSIONS
In conjunction with previous work on the subcritical
heat treatment of a low carbon ship plate steel (C steel), the
following conclusions seem justified:
i The quench-aging mechanism was responsible for the loss in
2 The severity of the embrittlement incrased with increasing solution temperature from
650°
to 1300 F; no embrittlementwas present when employing solution temperatures less than
650°F0
3 On the evidence of impact transition temperature and
hard-ness changes, characteristic aging curves were obtained,
Le0,
the peak transition temperature and hardness reachedand the time to attain this peak decreased with increasing aging temperature.
Metallographic examination showed that a two-stage
precipita-tion reacprecipita-tion was operative.
5 . low temperature postheat at about
650°F
would do much toeliminate by overaging the zone cf minimum ductility
previously found in the subcritically heated region of weld-ments of this and similar grades of' steel0 Higher postheat temperatures run the danger of introducing another aging
cycle if a fast cool is employed
FUTURE WORK
This report concludes the experimental work done under this
contract. A final report will be prepared summarizing all the work done on (i) the distribution of relative ductility in ship
plate weidments and (2) the subcritical heat treatment of base
-25-BIBLIOGRAPHY
l.E0 B0 Evans, and L0 J. Klingler, "The Effect of Subcritical Heat Treatment on the Transition Temperature of a Low Carbon
Ship Plate Steel", Fourth Progress Report, Ship Structure Committee Serial No0 SSC-60, October 30, 1953.
2 G0 Sachs, L0 J0 Ebert, and A0 W. Dana, Jr0, "The Fundamental
Factors Influencing the Behavior of Welded Structures Under
Conditions of Multiaxial Stress and Variations of
Tempera-ture, Stress Concentration, and Rates of Strain", Navy Department, Bureau of Ships, Contract NObsJ+5+70, Serial
No0 SSC2+, May
10,
l9+93
L0 J.
Klingler, L0 J. Ebert and W M. Baldwin, Jr., Ibid,2, Serial No0 SSC-3+, November 28, l9+9.
+. E0 B. Evans and L. J. Klingler, Ibid 2, Serial No. SSC-5+, October 1+, 1952.
Technical Progress Report of the Ship Structure Committee,
Welding Journal, Vol. 13 (July l98), pp. 377s-38+s0 J. R. Low, Jr., "The Effect of QuenchAging on the Notch
Sensitivity of Steel", Welding Research Supplement, Vol0 17 (May 1952), p. 253s-256so
Anna L0 Tsou, J. Nutting, and J. W Menter, "The
Çuench-Aging of Iron", Journal of the Iron and Steel Institute, Vol. 172, Part 2, October, 1952, pp. 163171.