Report SSL3O2
FATIGUE BENDING TESTS
AT LOW TEMPERATURE
ON' WELDED SPECIMENS OF
30MM AND 70MM THICKNESS
Deif t, 1986
TU Deift
Technical University Delt t
¡r. H.G. Scholte Ir. Evan Rietbergen
Department of Marine Engineering Ship Structure Laboratory
SUMMARY
As a part of the NIL fracture programme. 30mm and. 70mm
w.eldments were tested under fatigue .be.nding at. low temperature
at the Sh;ips. Structure Laboratory. During, fatigue testing
intermediate ClOD-tests were caTrri'ed out' at intervals of 1: or
2. mm. of fatigue crackp.ropa;gation..
With this way of testing 1173 results on fracture toughness
be'havioúr were gained from onl,y 69 specimens. The resú.Lt's give g.00:d additional i.nformat'io.n tO the' co,nveñtional fracture
toughness testresuits and .' a well defined transition
temperature., . whicì divides thepct entiál range of temperature
under wrking conditions' very sharply in a safe and un9af
LIST OF SYMBOLS
a - crack'length mm
a est - estimated cracklength
a Es - real cracklength mm
B - breadth mm
COD - crack opening displacement. mm
COD-S - COD at the side of the specimen mm
.CTOD .- crack tip opening displacement mm
CTOD 1/3R - CTOD calculated with a center of rotation at 1/3 of the net-section mm CTOD BS . - CTOD calculated according to BS 5762 mm
CTOD Holi.-. CTOD calculated according to the method of Hollstein et al.. mm f req. - frequency Hz
HAZ - hEat affected zone
K stress inténsity fector
KIc - critical stress intensity fáctor in mode i
L -length mm
LT - specimen orientation
n - number of cycles
Pmax - maximum load in COD-test kN
Pmin - maximum fatigue load in fatigue step kN
R - stress ratio
r . -. rotation factor
S - span between up and down load in four point, bending mm
sigma-y yield' stress MPa
T - thickness mm.
W - specimen width min
x - distance from bottom specimen to side COD measuring point mm
z - knife edge height mm
- crack tip opening displacement mm
a - yield stress MPa
CONTENTS 1. I;NTRODLJ.CT1ON SPECIMENS 4 2.1 Material 4 2.2 Welding ... . .
2.3 Geometry and instrumentation
of
the specimens 5TEST EQUIPMENT .
TEST PROCEDURE i
. 7
5 PRESENTATION OF THE TEST RESULTS
. 9
5.1 Sp:ecimen resultS .
. 9
5.2 Results oP 30mm specimens
...
5.3 Results of 70mm specimens
...10
5.4 Comparison
of
30mm and 70mm specimens...11
DISCUSSiON OF THE RESULTS 12
6.. 1 Cal,culat.ion of the COD at the cractip
...12
6..2 InflOence of intermedjatè
COD on final
ClOD-values at fracture
...14
CONCLUSIONS lIERA TURE lABEL I VII FIGUÄE i - 23 1.51. INTRODUCTION
This report comprises th.e results of the fatigue bending tests
at low temperature (fabalt'-test.)'. as carried out
in the Ship
Structures Laboratory of the 'Delft, University of Technology.
The fabalt test programme fOrms part of the NIL-fracture
programme which is the, Outc.h contributIon to an international
fracture toughness programme. That programme aims to achieve
a better definition of material properties with re;ga'rd to the
occura;ri.ce of brittle fracture or plastic collapse of
structures. This is the more' impo'rtant.whereas the approach
wit.h 'regard to the acceptance of defects is cha'nging from the
tendency of absolute absence of defects to tolerated
defect sizes.
With a wide range of different tests to assess material
properties, the NIL-fracture programme tries to get
a
realistic set, of requiremen.ts in connection
an economic, point of vie.w small scale tests are
they should give reliable predic:tions
of
behaviour on large scale.
with special regard to th.e tests
to
reliability . of those
predict material behaviour on larger scale.
In the. NI:Lf,racture programme accent is given to'thecOD.and
J-int.egr'al. Both are frac t ure toughness properties
. that can
be compared' t results of tests carried out
at other
laboratories because the relevant t:est s are standardized. Thé
CTOD,-vaLue.s_ar.eu.g.ed 'toC predict, critical crack izes or loads
for larger construction details by using
the CT.00-de:sign. curve. A disadvantage of the OD-test in
heterogeneous
material is, that only a very small amount. of
material i.s
t est ed. To me ett.h.i.sh an d4c a'p'-a---fat:i-gu ebewdtrí'g t e s t at low'
temperature .(fabal't-tegt) has been proposed by Nibbering
/1/,
/2/ as a complementary and alternative test method.
There are . several ways to perf'orm the fabalt-test. In the
first tests by Nibbering the acçert was on 'wide plate testing.
A serie of small scale specimen gave Similer results with
'which the behaviour of the wide plates could be predicted..
During these small scale bending
tests brittle steps occured.
First they were attributed to the heterogenity
. of the heat
affected zone (HAZ) but on furthe;r
consideration they seemed
to defects. From
preferred, but
the material
to conform ta the work hardened zone cause.d by the fatigue
load. Outside this zone the material toughness Was sufficient
to stop fractures. Thislabo'ratory situation corresponds to
the reality, where ships and offshore constructions are
continuoUsly exposed to fatigue loads.
Later investigation gave similar brittle steps in 25mm SAW
specimens (1:3/). The basic principle in this way of testing
is t'o have the crack grown though..the net-section of the
specimen at a high load level. Fracture will occur at a bad
spot of low fracture toughness as compared ta t'ha rest of the
section. In this
procedure the
load has ta be gradually lower8d in order to expose every crackti.p point of the section t.o the same stress condition.At fracture crack'leng'th and load result in a realistic
critical 'stress intensity factOr' (K) value, for which the
material at that temperature cannt be. used safely. I. case
the specimen remains undamaged until the crack reaches half
the specimen widt:h, then the test is concluded with a static
COD-test. The most important advantages 0f thiS Way of
testing are: - the realistic load history, - no difficult COD
measurements during the test, - no problem to calculate the
COD_value at the crack-tip , '- contihuou:s testing of the.
complete speoimen section (-which s:houl.d give more reliable
results, especially for heterogeneous material compositions
like welds)
A problem is the 'comparison wit!h other more commo,n fracture
toughness teats. Apart from that, however realistic the
resulting :KI.c may be, this value loses its applicability In
the demanded toughness zone.
The idea of fatigue bending at low temperature was adapte.d in
an altered version a.g Fatigue COD by Tanaka et al./4/. His
purpose Was to detect the minimum CTOD-v.alue in a small
bzittle zone of the H-AZ. For this purpose face-cracked
specimens were fatig:ued with a constant high maximum load.
and high A-value. When the applied load was high e:nough for
the specimen to break, the crack-tip value was calculated from
the total measured COO. The high maximum fatigue load causes
blunting of t:h'e c-raokti,p. Therefore too optimistic results
may 'be found.. In a later publication Tanaka proposes
restrictions for the R-values an.d the .K -to avoid this
-2-phenomenon (/5/)'.
More recent
research oP de Soer /6/ which was also directed to
detect the lowest fracture
toughness level in a small
embrittled zone, indicated that the
continuous Fatigue COD
method stili leaves
many interpretation problems to be solved.
More succes could be reached with the method
of intermediate
COD-tests..
The idea of intermediate COD-tests
has been introduced by
Nibbering in /3/ to improve the actual
standard COD-test. As
stated before only a very small amount of the section
is
tasted in the standard test.
This means that the location of
the fatigue cracktip
in heterogeneous Composed material, is
decisive Por the fracture toughness
result of the test. The
principle of intermediate
COD-tests consists of executing a
standard COD-test at various places of the
section up to a
certain ClOD-level. The
intermediate steps are crossed by
applying a fatigue load.
Uñder a relatively high maximum fatigue load there
remains the
en fractures at a bad spot during
procedure. Since the Standard
comparison with the results of
standard COD-tests la stili possible.
possibility that the specim
the fatigue step o? the
COD-test is maintained, a
SPECIMENS
2.1 Material
The specimens o?? the faba'lt,-'tes't were manufacturèd from weÏded
X-joints in the thicknesses 30 and 70mm. The plate màterial
in the NIL fracture programme l's a Fe SlONb steel. To assú're
a. good' comparability of the various test results t.he
manufacturer Qq the steel (Dutch Höogovens) Was asked to
deliver the plate with a material composition as h:omog'efleou.S'
as :possibl'e. 'Table I presents the chemical composition of the plate material with the sp'read in' extreme values. ' The
mechanical prop'ePtieìs ar8 shown in table II. A more extensive
descrïption of thé plate material i.n the NIL-fracture
programme hais been given 'in /7/.
In order 'to 'know the yield strength and tensile strength at
diffa'rent'temperatures, tensile tests under displacement
control were carried out on the weld material at -10' and -70
degrees C (/5/;) . The intermediate values 'were obta;lned' with
t:he a;id of resûlt.s of the. BROS I and II research programme
/9/. F.lg.9 shows t.hè results.
2.2 Welding
The 30mm serieS were taken from four' welded strips made f
three rolled plates (nrs.. 58385-005, 58460-006, 5846Ò-009)
The 70mm. serias ws manufactured from three welded strips from
only one rolled pláte. (nr. 62965-013). Detail's are given in
/11/.
The weldS were 'made by Submerged' ' Arc Welding. For the
rootlayera Ma!nuall,y Arc Welding ' was 'applied. The
prehea.tternperature was 120 degrees C, the lnt'er;passtemperature 150 degree.s C. Finally both 30mm and 70mm welded plates' were
p.ostweld heattreat.ed on 570-590 degrees C for respectively 60
and 150 mInutes. 'Table III a t/m g show1s t;he welding
procedure. for the different welding strips.
-4-2.3 Geometry an,d instrumentation of the specimens
From, the' welded plates 45 specimens of 30mm and 30 specimens
of 70mm were manufat.ured. The specimen geometry is given in
fig2
for the 30mm specimen and in fig.3 for the 70mmspecimen. Both series had a short mechanical notch of resp.
10 and I'S. mm sitUated at the. centre of the weld. This
position was chosen because it is. univocel to define, this in
contrast to the. fusion line or the HAZ. The 70mm specime.n'.has
a B/W=0.S, which equalS. the ratio recommended for th.e BS:
standard test specimen (/12/).. For the 3Ommspecimen B/W was
lowered to 0.33 because otherwise .he. craokgrowthpath wou.ld
have been t'o short to obtain enough measuring point's. The
numbering, of 'the,.. specimen successively consists of: a
weldmerit number;, the orientation of the speclman.( see fig.4).;
a serial number. (e.g.. 8 'LT SL
To measure the COD a clip' gage was used which was. fitted.
between fixed knife edges 'at the cra.ckmouth of the specimen1
'A c.lip.gag.e (MTS) w.ith a range of 3.5 mm w s used for
measuring the. COD at some of tche.3Ornm spec;imen,s., A clip gage
(MTS), with a range of 12 mm.Was.used for the 70mm specimens
and the . greater part of the. 30mm. specimens.
F'ig.5 shows a detail of the i.nstrumentatjôn of the specimen.
In addition to the clip gage a COD-measuring device ' at the
side of. the specimen ca:fl be seen. In fig.5'. also sorne
measurement wires canbe dï'st'inguished which we;re used to
detect, the crac'kleng:th based Upon' th:e potential drop method.
Bat:h .supplernentarymeagurrn,,g appeared t.'o obta.i,n unrelj.abl.e
results and they will not be taken 1ñt.o account in the
discussion of .theres,ults of this investigation.
-5-3. TEST EQUIPMENT.
For the fabalt test programme two vertióal servo-controlled
fatigue test machines were,
used.
A 350 KN machine for the30mm specimens and a i.000kN machine for thè 70mm. specimens
(See, fig.'6,) . The adJustmeit of fatigue load and the execution
of the COD-tests in the first tests of. the 30mm s1pecimen9
:(.nrs. iLl l-5,. 2LT 13-16, OLT
27-36)
weré
carried outmanually. The adjustment during the testing of the 70mm
9ped±mens and the remaining, 30mm series was done by computer
con:trol. The computer was alsp used to gather measurement
data. 0f all COD-tests làa:d-COD plots and time-COD plotswere
made On x-y-recorders, respectively x-t-re,corders.
The experime:nts were carried, out, at low temperatures over' a
rànge from -100 degrees C up to -20 degrees 'C. Two co:o:ling
dév'ices were applied. An alcohól cooling device Was applied.
for the range 0f -20 degrees C to -60 degree C with an
accuracy of about 0.5 degrees C. Lower temperatures were
òbtàin.ed with an accuracy of about 2 degrees C by means of a
nitrogen iñstallation.
-6-4. TEST PROCEOUAE
As stated in the introduction there are several ways to
perform the fabalt-test. First it
j8
possible to adjustcontinuously the maximum fatigue load in such a way that a
constant net-stress at the craòktip is maintained when the
crack moves through the section. This òonforms tO the
procedure of Nibbering and Schalte in /3/, although in theie
tests the maximum load Is only adjusted three times. Tanaka
applied a similar procedure,. However by applying continuous
loading the section point.s are not testéd under equal
circumstances. Therefore süch procedures are only suitable
for detec.ting. the minimum: CTOD iñ a smàll known area.
Moreover this way of testing raise some prolems concerning
the: interpretation of the test results. (see /6/). The
possible. influence of the load his tory, an influence. of. AK and
R on the results and difficulties to calculate the COD
cracktipvalue are the ma1n ones.
Because of these problems and for a better comparison with the
other results in the NIL-fracture programme, the fabalt-test
woe carried out by applying intermediate COD-tests. In that
test th.e load is raised until a prefixed COD-value at the
cracktip jg reached. When the fracture.
toughness of the
material at that place is sufficient to resist that amount of
deformation without cracking, the specimen Is unloaded and the
test je continued by making a next fatigue step C say 2mm) . A
fatigue load is applied thàTtcTOrreqpondg to the h7ilher loads
that occur in practice, so there is po:ssib:ility that
fracture occurs at a bad spot in the material. On the other
hand: the fatigue load should: not influence (too much) the
COD-results. The advantages of thie procedure are clear.
Although there is no continuous testing of the. sectio:n, the
chance to find a bad spot is Increased. The choice of the
prefixed ClOD-value an depend on requirements of
Classification Societies or calculatiöng. When the specimen
has not fractured when the crack has reached half the width
the test Is concluded with a COD-test till fracture. At that
moment the e;peclmen dimensions correspond to those of the BS
5762 /12/. So the result is that of a standard COO-test.
For the 30mm specimens the fatigue step size was set on 1 mm
and for the 70mm specimens on 2 mm These step sizes were
-7-visually perceptible and no other cracklength measurement
method was required. Afterwards often the real cracklength
appeared to be somewhat larger. However because good crack
front marks appeared on the fracture surface (fig.9a),
corresponding to the successive intermediate COD-tests, all
results could be evaluated with the real craciclength.
Cracklength and stepsize are therefore not critical.
The maximum fatigue load has been selected so, that, for that
particular temperature, after every fatigue step the yield
stress was reached in the net-section of the specimen, based
on a linear stress distribution (sigma-y line). This fatigue
load corresponds to the maximum fatigue load permitted to
produce the fatigue notch In the standard specimen according
to BS 5762. In fig.? the maximum fatigue load and
corresponding K-values are shown as a function . of the
craoklength.
With the selected frequency (4 Hz) and stress ratio (A0.3)
every fatigue step needed 1000-2500 cycles. This resulted in
the possibility to perform one fabalt-test every day. It was
fortunate that in this investigation only a slight retardation in crackgrowth was observed at the beginning of eaçh new step.
Although no crackgrowth retardation was noticed , the fatigue
load in the first tests was as high as .75% of the maximum load
of the previous intermediate COD-test, (nrc. 8LT28, 29, 30
and 31)
In the intermediate COD-tests the COD-value which had to be
applied after each fatigue-step had been calculated on the
base of a center of rotation at one third of the net-section
width (r1/3) (see
fig.8) . Later these values have beencorrected with 88 5762. This procedure was necessary because
the CTOD must be continuously calculated during the
experiments in order to to minimize the scatter in applied
intermediate CTOD-values..
-8-5. PRESENTATION OF THE. TESTRESULTS
5. 1 Specimen results
The resulte and data particulars of the fabalt-expe:riments are
collected in report /13/. In the presèn't report several
representativ.e reuita from /13/ have been inserted see fig.9
and 10. The figures 9e. and 10e give : general information,
load, te.stcondltion.s, dimensions etc..; additional remarks; a photograph. of the fracture surfce.; a table with ail tes.t
data. In figures 9 and 10 sorne illustrating graphe have been a:dded. The, first graph shows the load history as a function
of the crackl.ength, and the second ne the CTOO as a function
cf the c:rackie.n'gth.
In the present report all test results are given 'in table IV
-VII for the 30mm specimens and table VIII för the 70mm
specimens. Thfse tables comprise: testtemperature; total
number of cycles; number of COD test at a specific average
int'ermediat:e ClOD level, wlhich is given inthe next columns;
crack.leng.th and load at fracture; moment of fracture; a
critical K-value for the specimens which fractured during
fatigue; CTOO. values at fracture.
For the òalcu,lationof the ClOD-values three different methods are applied:
A linear interpolation between the measured displacement
at the orackmout.h and a center of rotation at one third
0f
thenet-section width (r=1/3 as shown in flg.81.
The compliance method according to BS 5762; 1979, /6/,.
/12/.
The mèthod of Hellstem, Blavel and Ulrich, which is based on a linear Interpolation between the measured .displaòement at
the crackmout'h and the center of rotation. The difference
with a. is the location of the center of rotation, which now
la. given by formula r=O'.48VCTOD. This method' .s'huid give
satisfying results compared to BS 5762 /14/.
Next to the presentation in table IV - VIII the results. have
also plotted In graphs, Which give a complete overview of the
testresults.. Fig.11 gives the results for the 30mm and 70mm specimens based on the assumption r=1/3, which was used during
testing of the specimens. These results corrected wIth 86
-5762,, re p1otted in fig.12
and 13. The various symbols used
in the figures are explained by the
scheme in the left top of
the figure. For some specimen the clip
gage range wá9
insufficient t'o meagur the total COD at
fracture. In that
ca'se the values given in the fig.1i,12
and 13 are based on the
maximum COD which could be reached with
the used clip gage.
An arrow i.ndjcat;es that 'the real
CTOO will be above the
plotted point.
5.2 ResigUe of 30mm specimen.g
To interpret the
results as presented in fig.12 is a rather
complicated matter. Therefore in fig.14 only ClOD
values at
fracture calculated according BG 5762 are given.
In addition
regression lines were calculated tlh:rough the
fracture points
of the various we,ldmentg.
These are plotted in fig.1'S. From
this figure it appears that one weldment (8LTa
series) has a
significant lower fract.uretoughness
as compared to the other
three. weldment,g. The result,g of the
specimens from the other
weldmentg will be Considered as one
group, although the ILl
weldment was somewhat 'better at higher temperatures and lower
at low temperatures.
Only few results are available in the
higher temperat:ure region.
However it seems eviden,t that at
about -40 degreee C the
transition to extensive plastic
deformation occurs. For the 8Lra
weidment this transition
temperature is about 20 degrees C higher.
The caúse of this
difference is not yet clear. The differences in
platematerial
composition and welding
procedures are too small to explain
this behaviour.
5.3 Results of 70mm specimens
Fig.16 ehows the CTOD-values at
fracture for the' 70mm
specimens. In contrast to the 30mm specimens
this figure does
not reveal any signific
difference between the varioUs
weidments However, when testing the 70mm
specimens another
phenomenon appeared Which can
be i.11ustpated when lines
calculated with linear regression are plotted.
The CTOD at
fracture seems to be influenced by the
height of the
intermediate ClOD. The lower line in fig.17 contains all
results while in the upper line the results which might bO
infl:uenced by a high intermediate cîoo have,
been e'xcluded.
The phenomenon will be
paragraph.
5.4 Comparison of 30mm and 70mm specimens
in fig.14 and 16 three different areas C8:fl be distinguished.
There is firSt an area with low temperatures where fracture
during fatigue is- possible. This brittle z-oñe runs upto -70
degrees C for the 30mm specimens end upto -80 degrees C for
tih.e 70mm -ones. This is followed by a second are.a over a
temperature range of about 35 degrees C up to a.n upper limit
of about -40 degrees C. in this area the scatter in the
C-TOO-values i-e high due to a large increase of the upper
values and an almost- .naglectibl-e ncrease of the lower ones.
Finally ove-r .a very' small temperature range we can find a
sudden -disa:ppearance of all lower CT-0D-values-, resulting in -a
well, defined transition temperature. This transition
temperature is about -40 -degrees. C aswe-il for the 30mm
Specimens as for the 70mm specimens and divides the- potential
range of temperature under working conditions very sharply in
a safe and un-Safe region.
-A further look on the second area with increasing scatter in
CTOD-vajues shows a dif-ferènóe in behaviour between the
30mm-and 70mm specimens. Fig.18 shows that the fracture -toughneea
of the 30mm series is considerably -lower than that of the 70mm
-series. An effect of increasing constraint with thic:kness'es
does not appear at -all, Probably this is caused b;y t:h:e
difference In specimen geometry: B/W=0.33 for the 30mm serie-e
and BJW=0.5 for the 70mm se-ries-. Another poss.i.biity is that
the- welding procedure is- more benif'ioial for th.e great-er
thicknesses, of cour-se this is quite haphazard..
'Influence- of the height 0f intermediate CTOD-vaIues- could not
be as -clearly distinguished -for the 30mm specimens as for the
7-Omm ones, altho:ugh also he-re some -bad -results could be
-explained by this phenomenon. This will be discussed in 6.2.
In fig.19 the calculation method using the assumpton r1/3 is
compared to the BS 5762 -for bot-h plate thicknesses.
Especially i-n the -lower toughness region- the diqference j
6. DISCUSSION OF THE
RESULTS
6.lCalc.ulatjon of the COD at the cracktip
One of the problems in applying COD-tests is the calculatjo,n
of the COD cracktip value from the
measured COD at the
crackmouth. De Boer /6/ used the
BS-compliance method and
plotted the load-COO curve of the
actual test on graphs with
load-COO curves for various CTOO-values. This working method
is very
labørjg and difficult
to automatize. TherePore in
this investigation the simple assùmption of a fixed location
of the center of rotatjon at ¿'=1/3 was maintàjned.
The CTOD calculation aÒcord1ng to BS
5762 consists of an
elastic part and a plastic part. The elastic part is
calculated with a standard formula, based on theoretica,1
models, but the factor 2 in the denominator was
evaluated by
experimental data. From the plastic component of the total
COD the plastic one of the ClOD
is! Òa.lculated by taking a
center of rotation of 0.4 of the net-section Width.
For small
CTOD values the plastic part will be small and
the elastic.
part will dominate. Fig.20 gIves the elastic
part as. a
percentage of the total ClOD which
illutrateg
the fast
growing influence, of the
plastic part with increasing ClOD
values over 0.2 mm. The center oP rotation of
the elastic
part is about 0.1. This explains the great
differences In
ClOD-values for the lower region, for the two
calculation
methods 88 5782 and r=113. However, with increasing
toughness
and therefore increasing CTOD-values the contribu:tjon
of the
plastic component becomes larger and larg:er.
Because.th,e SS
5762 assumes a center of rotation at 0.4
of the net-section
width the difference.s
between the CTOD.-v'òlueg calculated with
r=1/3 and BS 5762 become smaller for larger
CTOD-valueg. At
large CTOD-vaJ.ueg r=1/3
becomes conservative compared to BS
5762. It should 'be realized that the center
oP rotation of
the plastic part (r=O.4 is still
subject of discussion
(/15/).
Because earlier investigation of Guyt /14/ indicated: that the
method of Holistein, Ulrich and Blavel gives similar
results
as the SS this method was also taken into
consideration it
gives, a simple formula for the
center of rotation
(r=0.48\flT5)
which makes fast data Processing possible.-Therefore all data have been evaluated using this method. In
fig.21 the CTOD-values are compared on basis of r1/3. The BG
values, are grouped in two separate lines for the 30mm and 70mm
specimens. Probably an influence of the B/W ratio is the
cause of this phenomenon, either in the 96 calculation or at
r=1/3. Using the BG method no influence of a/W ratio could be
determined in contrast to the Holistein et al. method. The
lines for the latter in fig.21 are calculated for the 30mm
specimens. The results 0f the 70mm specimens appeared to
remain in the same hatched region. In fig.21 is indicated how
the curves will shift with the change of the indicated
variables.
The correspondance between the results of the method 0f
Holletein et al. and those 0f the BG is satisfactory up to
CT0D0.5 mm, but CTOD values larger than 0.5 mm are. 0f less
practical interest. Compared to r=1/3 the BG is conservative
up to 0.75 mm for the 30mm specimens and up to 0.9 mm for the
70mm specimens.
In fig.22 the location of the center of rotation as a function
of the CTOO is given for various calculation methods and
experimental data. The experimental data are obtained by
measuring the ClOD directly with advanced measuring techniques
116/, /17/. Compared to these experimental data the simple
assumption
r1/3
is conservative fromCTODO.1
mm. Thecorrespondance between 88 and Holletein and these experimental data is bad up to 0.7 mm.
Although it is not the intention of this investigation to
discuss the 88, apparently great differences appear in the
calculated COD cracktlp values up to 0.5 mm, depending on
calculation method used. As these lower ClOD-values form the
most interesting range for the fabalt-test, maintaining of the
COD-concept remains a handicap in the present fabalt test
procedure, but it is inherent to COD-testing n general.
-6.2 influence of intermediate CTOO on final ClOD-values at fracture
In fig.14 and 16 the results that might be influenced 'by
intermediate COD-tests aré ' marked. with a symbol. The
comparative low values of these results can be explaind b'y
three different effects. . '
Above a certain level of plastic deformatian the
intermediate COD-tests will decrease the fracture toughness at the next measuring points of the net-section to such an extent
that the C.T0D at fracture is 'reduced.
With a higher intermediate CTOD level the probability is
'raised that the cracictip is located at a bad spot with a
fracture toughness j:L8t under that particular intermediate
CTOD level.
HIgher intermediate CT0D-va lues Increase the necessary
numbér of cycles for the additional growth of th.e fá.tigue
crack, resulting in more strain hardening.
That great differences in fracture toughness do occur in one
section is il.luatrated by the result of 8LT37 .(fig.23) .' 'Here
two locations 'of instability can be d:isti.nguished. The first
Praoture at an' intermediate COD test could stop due to load
relaxation and better material quality. ' The latter came
forward when the test was co'ntinue'd and completed with a
standard COO test which resUlted in a good tou:ghness value.
However, with the effect of raised probability in a dominating
role, one shòu,Id expect, that, although a high intermediate
ClOD level 'will causa lower' ClOD values at fracture because
more' bad spots will be detected1 the fracture 'ClOD ' values'
should increase with higher temperatures. As can be noticed
from fig.14 and 16 this is not the case. Particularly the'
fracture ClOD values at -40 degrees C are not 'in line with on
increase in fracture toughness at higher temperature;s. One
has t. conclude that the' influence 0f the' load history and in
pa:rtiòular the height of the foregoing intermediate
CTOD-values contributes to the decrease of fracture toughness
in order to axpla:in this phenomenon. The amount ' of the
contribution of' each particular possibility is difficult to
determine. With the present data lt is n'at possible to
establish which of the three phenomena is dominating.
-7. CONCLUS;IÒNS
At lower temp,e,r'atures, low stress brittle. fracture. ocoured
'during fatigue. The critical t:empera'ture is -70
degrees C for
.30mm specimens and. -80 degrees C for 70mm Specimens.
In a transition, zone from -70 up to -40 degrees C'fracture
toughness slIghtly' increàses, while a great scatter in CTOD
results can be. fou:nd in that' area. Therefore thl,s area n
certainly not be indicated', as. safe from a fracture toughness
point of view.
The transition, from low t.o high fracture toughness, values
takes place in 'a small temperature interval (1.0 degrees C)
Th'i temperature is for both plate thicknesses -40 degrees C
and can be interpreted as a sharp and accurate boùndary
between the safe and unsafe area.
The ' results indicate that the loadhisto'ry, in particular
the level of pea:k.load:.s or intermed:iate CTOD values. inflúences
the CTOD value at fracture. It is not possibl.e yet to give a
quantitative explanation for this phenomenon.
The ClOD' results, in the transitjo:n zone of -70 up to. -40
degrees C are significantly lower' fo,r the 30mm specimens
compared to the 70mm specimens.. HowPar this can be explained
'by differences in
specimen 'geometry and/or influence of the
welding_pjQced.ure is not -et--.e-xami-neth- -'A- further
nvestigation is recommended,.
Calculation of the CT0D values with, the assumption of a
center of rotation at 1./3 of the. net-section width leads to
significantly higher results u.p to CTOD values of about 0.8mm,
compared to the calcul.a'tio, according BS 5762.
-LITERATURE
/1/.N.ibbering,. J..J.W., Lalleman, A.W.,"Lo.w cycle fatigue tests
at low temperature with E.G.-welded plates",, 11W-doc..
/2/
Nibbering, J.J..W. et al.,"Britt.le fat;i.gue in the H.A.Zof E.S.-welded plates subjected to low cycle., fatigue",
11W-doc.
X-67o-72..
/3/ Nibbering, J.J.W., S'cholte, H.G.,"Real.istic testing, of
welds by f'atg..ue' bendi'ng at l.cw temperature", 11W-doc.
x-1014-82.
/4/ Tanaka., K.., Sato, M'., Ishi:kawa;, T...,"Fatigue COD and Short
crack arrest tests", Pa:per 18,
mt.
Conf. on.FractureTougness Testing., The Welding Ipsttu't'e, London. 1982.
/5/ Tanaka, K., Ishilsawa, T.,"DeveÏopme:nt of fatigue CTOD test.
for investigation of brittle regions in welded. joints", Sixth
mt.
Conf. on Frac. (1CF6) New Dahu, India 1984./6/ Boer, R. de,"The detection of local. embri.ttlemen't in
welded structures", final thesis department of Material
Engineering, T.H. Delft, april 1984.
/7/ Kinjet,"Levering van. Fe 510 Nb aan NI.L,/TNO t.b.v.
int.e.rna:tior'aa:l breuktaaih.eid'eonderzoek" PG 84-08 (in Dut.ch)
/8/ Spanjer, W..,, "Tensile tests executed at -10 C and -70 C on
FeSlONb pl,atemateri.a.l and . weld metal", TNO-rep.ort
85M/01i'g./SPA/VLT, PG .85-01 14 January1985..
/9/ Ronge:n.j H.J .M'. , "Ge:g'evens van treIs,pro:even aa:n Fe5lONb",
Mem. 3364106, Pg 85-03, ?S januari 1985 (in Dutch).
/10/ Spànjer, W..,"Tens:i:le tat.s: executed at -10 .0 a.nd -70: C on Fe5lONb base mate.rial",ÏNO-report 84M/10053/SPA1VLT, PG 84-13, 7 September 1984.
/11/ K.onin:g, C,"NIL-bPeruktaa1heidsonderzoek./Nede;rlandS
programma. Uitnameplan en type proefst.ukken", TNO-re,port
/12./ "Methods for
Crack Opening
D'ispi,acemènt Testing", BS
6762British Standards
institution ssi, London
1979./13/ Aletbergen,
E.v.,"Expe:rjment.ai data of fatigúe
bending
tests
at
low
temparatupe".,,
App.endi.xto
report
302, Ship
Structures Laboratory repOrt nr.
302b, Delt 1986.
/14/ Gu.yt.,
J.,"Theo'retjsche. en experimente].e analyse van enlge
aspec:ten. van de COD-proef
eIn haar toepas's:ing",, final
theslis, at
Department of Naval Arc:hitecture
T.H.Delft, 1980 (in
DUtchi.
/15/ Matsoukas, G., Cotterell,
B., Mai, I.W.,"On' the
plastic
rotation
constant
usedin stalndard COO testi",
mt.
iourn.
of Frac.
26,
11984../16/ Inglham, T., Egan,, G.A.,
'EllIott, O., HarrIson,.T.Ö.,'Th
effect
of
geometry
on the Interpretation. of COD test
data",
Prao.
Appl.
of Frac.
Mech.to Press.
Vess.
Tech.,
mIst.
of Mech.
Eng., 'London
1971, p200-208./17/
Veerman,
C.C.,, Muller, T.,"Th,.e
location of the äpparant
rotation axis in notched bend
testing",
EnlgFrac.
M'ech.Table I. Chemical composition of heat and plates. Ladle analysis % X I0 Heat no. C Mn P S Si Ai tot Cu Sn Cr Ni Mo Nb N % .x10 91251 184 H 1323 0113 010 401 056
017005 031
026 002 027 0036 PlatesElement
VÎS
Lower and upper values ScatterC 0.187% 0.173. - 0.193% 0.02% Ñn 1.297% 1.267 - 1323 Oi.05'6% P 0.014% 0.013' - 0.014%. 0.001%. s 1 0.Ó07% 000'6
000%
0,.Ô02% Si b.. 398Z 0.387 - 0.421%. 0.034%Alt
0.048% 0.041 - 0.050% 01.009% Ce 01.4%_O.OTO
-. 0...01L7Z___-0.07
Nb 0.029% 0.026 - 0.031% 0.005% N 0.0053% 0.Ó04:8 - 0.0059% 0001 1%Table II. Mèchanical properties of plates for fabrication of test specimens. Thickness tj Specimens Rolling number Dimensions Re (N/rn2) Rm
(N/2
Elongation (Z) Charpy-V - O J-value ( C) -L (=) V (=) T (=) 30 1LT 58385 6000 1400 30 30 2LT 58385 6000 1400 30 389 567 30.6 89 -40 .371 548 32..5 95 -40 30 8LT 58460 6000 1400 30 391 563 28.6 107 -40 384 570 27.2 97 -40 70 liLT 62968 3000 1400 70 386 550 29.0 7T -40 387 549 27.0 136 -40laboratory report
8424/35/O.N. 35.6.6731 T.N.O. -Apeldoorn
Project-Fracture Mechanics Tests
. Welding Procedure Record
Teetsample Welding process : Welding position: Preheat Interpass temp. : Filling material: - Eeattreatzoent : joint preparation SOC--.... P.S. box 6 øO#A I&den Ihe AOthSdlfidS fspcftO. 841019 i? - 1G plate 30; PeE 355 kT
S.M.A.W. (manual) and S.A.W.
1G
120CC 150°C
S.M.A.W. (manual): Electrode
S.A.W. : Wire
stress relieved Flux
570-590°C/60 min.
noi iarase
constructie
groep by
Kryo i SW 60 P 240 layers as welded-I
O)
-4 o' D. e H H H a'caz
e-QQ. mec wD I,o
ro
f ID-Q.
Cl'i
ID -.-40
3
e ID D 3 to eLayer Electrode Dian. Amp. Volt. R.Ó.L. speed Current
Wire/Flux ma cm
in.
i 1(ryol 31 110 26 12 ac 2 Xryoi 4 165 28 25 - ac 3 SW6O/P240 4500.28
- 50 deep 4-8 SW6O/p240 4 600 32 50 dcep 9 SW6O/P240 4 '0 28 50 deep 10-14 SW6O/P240 4 .00 32 - 50 deep /.fter welding la 1-8 , the weld has been gouched out Untill a dep . . f 5 ma, at side of layer 1.
Octobe 18th 1984
Iaboratozy report
o. 84M/35/O.N. 35.6.6731
died T.N.O.-Apeldoorn
Do. Project-Fracture Mechanics Tests
«t Welding Procedure Record
- Testsample s - welding process * - Welding position: - Preheat s - Interpass temp. s - Filling material: Heattreatment s joint preparation :
,/)J
Octod 18th 1984 d quimy cSsd -7/ Iepcftoo. 841017 2F - 2G plate 30mm FeE 355 kTS.M.A.W. (manual) and S.A.W.
1G
120°C
150°C
S.M.A.W. (manual): Electrode
S.A.W. : Wire
stress relieved Flux
570-590°c/60 min.
- Kryo 1
- SW 60
- P 240
layers as welded
1-9 , the weld has been gouched out ma, at side of layer 1.
-4 a, o. ID H H H o. rs4)
Layer Electrode Diam.
Wire/Flux
Amp. Voit. R.0.L. speed Current
cm sVndn.
I--I
1 Knyol 31 110 26 12 ac 2 Kryol 4 165 28 25 ac 3 SW6O/P240 4-9 SW6O/P240 lo SW6O/P240.4
4 500 600 500 28 -32 28 50 50 50 dc/Ep dc/Ep do/EpCD
11-15 SW6O/P240.4
600 32-
50 do/Ep of 6 After welding i untill a de84M/35/0.N. 35.6.6731
disid T.N.O. -Apeldoorn
dne ProjectFracture Mechanics Tests
bJsct Welding Procedure Record - Testsample - Welding process - Welding position: - Preheat - Xnterpass temp. - Filling material: Eeattreatment joint preparation so.--.-. 1 Kryo1 2 Kryol 3 SW6O/P240 4-10 SW6O/P240 il SW6O/P240 12-16 SW6O/P240 After welding untill a a
r.nty& quality co l departm.nt
°'
Octo.- 18th 1984r.poein 841022
SA - 83
plate 30mm; FeE 355 kT S.M.A.W. (manual) and S.A.W.
1G 120°C
150°C
S.Z4.A.W. (manual): Electrode - Kryo i
S.A.W. : Wire - SW 60
stress relieved Flux - p 240
570-590°C/60 min. WE,DING DATA 12 25 layers as welded 50 50 50 50
r 1-10 , the weld has been gouched out of 6 mm, at side of layer 1. ac ac dc/Ep dclEp dc/Ep dc/Ep cn D (D
w-oc.
I-'. l-'3D
DD D n hit
olo
Il lCD cDL'ro
-43 (j)3 n CD C) 3 CD D 'nrI
n CD 1 CD (n 31 110 26 4 165 28 4 500 28 4 -'0 32 4 5,. 28 4 .00 32constructi e
groep by
laboratory report AA leiden the nel%eflands Layer Electrode Wire/FluxDiam. Amp. Volt. R.O.L. speed Current
laboratory report
r.rno. 84M/35/O.N. 35.6.6731 cSl.n T.WO. -Apeldoorn
Project-Fracture Mechanics Tests Welding Procedure Record
- Testsample - Welding process - Welding position: - Preheat - Interpass temp. - Filling material: - Heattreatinent
pì
t;;
,e,tflD. 841024aC-SD
plate 30mm; FeE 355 kT S.M.A.W. (manual) and S.A.W.1G
120°C
150°c
S.M.A.W. (manual): Electrode
S.A.W. : Wire
stress relieved Flux
570-590°c/60 min.
WELDING DATA
- Kryo i - SW 60
- P 240
After welding layr 110 , the weld has been gouched out untill a dep.1(of 6znzn, at side of layer t.
ori. October
(th 1984
,ntrnI quality control dezrtment aberatoiy .,ctlan
co
-I
o
Layer Electrode Diam. amp. Volt. R.O.L. speed Current
Wire/Flux mm cm cirVmln. 1 Kryol 31 110 26 12 ac 2 Kryol 4 165 28 25 - ac 3 SW6O/P240 4 500 28 50 dcep 4-10 sW60/P240 4
,-00
32 50 dcep 11 SW60/P240 4400
28 50 dcep 12-18 SW6O/P240 600 32 50 dcepcid.zno. 8424/35/O.N. 35.6.6731 cfl.nt T.N.O.-ApeldoOrn - Testsample - Welding process - Welding position: - Preheat - Interpass temp. - Filling material: - Heattreatment Layer Electrode Wire/Flwc 1 ICryol 2 Xxyol 3 SW6O/P240 4-37 SWGO/P240 38 SW6O/P240 39-55 SW6O/P240
.__
loo___._YAfter welding laye untill a dept
Icden. Octob- 18th 1984
repodan. 841171
11 A - 11 B
plate 70mm; FeE 355 kT S.M.A.W. (manual) and S.A.W.
1G
120 oc
150CC
S.M.A.W. (manual): Electrode
S.A.W. : Wire stress relieved F1WC 570-590°C/150 min. a a
aae
cons1uctîe
groep by
- I(ryo i - SW 60 - P 240Diam. Amp. Volt. R.O.L. speed current
ann cm cnVmin. 31 4 4 4
4.
4 110 175 475 ac ac 30 50 dc/Ep 75 32 50 dc/Ep 30 50 dc/Ep 32 50 dc/Ep-37 , the weld has been gouched out 7 mm, at side of layer 1.
00.
.ubjed
Pro3ect-Fracture Xechanics Tests
Welding Procedure Record
layers as welded
joint preparation
jwù AA
* M5e:Iands
label 111f' Welding procedure 70mm specimens 1l;LTb-aeries Bpecifflens
11LT9 -. 11LT18
eider no. cenireot no. eubJ.st ieldegi. Octe cenkot-I
Teatsample i Welding process Welding position Preheat s Interpasa temp. t Filling materials Heattreatinent.i-After welding laye untill a dept 18th 1984 d.Pa1tms,, t. zoeleiwoudeuwee p.o. bee O 2300MIelden the netho,Iande laboratory report 8414/35/O.N. 35.6.6731 T.N.O.-Apeldoorn Project-Fracture Mechanics Thsts
Welding Procedure Record
i Kryo i 31 110 2 Kz''oi 4 175 3 SW60/P240 4 4.75 30 d-39 SW60/P240 4 575 32 40 SW60/P240 4 475 30 41-58 8W60/P240 575 32 ,.ponno. 841172 C l'i - 'D 11
-39 , the weld has nun, at aide of layer
holl landse
con structi e
groep by
Dina. Amp. Volt.. R.O.L. speed Current
mm cm ónVmin.
50 50 50 5°
been gouched out
ac ac da/Ep dc/Ep dc/Ep dò/Ep
plate 70 mInt FeE 355 kT S.M.A..W. (manual) and S.A.W.
1G
120°C
.l5o °C
S.14.A.W. (manual) ElOotrode - KryO i
S.A.W. s Wire 'SW 60.'
stress relieved 'Flux - p '240
570-590°c/ISO' min.
Layer Electrode Wire/Flux
label 111g Welding procedure 70mm specimens 1:1L,Tcse.ries
Speo:imens 1.1LT'i9 = 11LT27
«derlis. ß'4M/35/O.N. 35.6.6731
cUt ?.N.O.-Apeldoorn
conimetee. proèct-Fracture. Mechanics Tests
iu*ct Welding Procedure Record.
leiden. Oct c.nitel leboraleqi
-
'Teatsample t-
WeldIng, process - Welding ponitiont - Preheat Xnterpass temp. i.-
Filling materiali - llèattroatrnont joint preparation Ec -e r 18th 1984 nivel dspestmsn,1, plate 70 mm; FeE 355 )S,.M.A..W. (manual) and S.A.'W.
1G,
120°C
15Ò°C
S.M.A.W. (manual)i Electròde
S. A.W. . t Wire
stress relieved Flux
570-590°C/1:50 mifl.
hòIIandse
constrUctie
groepbv
lepOftilo. 841173 i1 E - 11F - Kryo I - SW 60 - P 240 layers as weldOd-37 , the weld has been gouched out
'mm, at aide of layer i. Diam.
ma
Amp. Volt. R.O.L.
cm speed Current Vm1. 3 l'lO ac 4. 115 ac 4 . 475 .30 50 . ' dc/Ep 4 32 50 dc/Ep 4 47 30 50 dc/Ep.. .4 32 50 do/Ep I. Zootoiwoudseweg p.o. box G 2300 Mielden the nolheilande laboratory report Layer. Electrode wire/Flux i Kryol 2 Xryo.1 3 SW60/'P240 4-37 8W60/P240 38 8W60/P240 39-57' SW6O/P240
After welding lay untill a dept
Tabol IV
RESULTS OF 30mm SPECIMENS WELDMENT itT
Moment of fracture:
E - Fracture at final COD-teat.
I - Fracture at intermediate C0D'temt.
F - Fracture during-fatigue. 1LT7 .30 43888 6 0.16 0.07 0.10 22 0.20 0.12 0.13 44 1.49 E 4.04 4.54 9,74 1LT11 -30 48654 6 0.19 0.10 0.14 21 0.28 0.20 0.21 43B 164 E 0.26 0.22 0.18 ILT1 -40 37412 28 0.16 0.06 0.07 64.1 127 E >0.815>0.85 >1,09 1LT2- -40 45000 26 0.19 0.11 0.12 -44.5 138 E >0.51 >0.50 ->OE.52 1LTIO -40 41063 6 0.14 0.05 0.08 22 0.23 0.14 0.15 44.5 144 E 0.36 0.33 0.30 LLT3 50 50000 5 0 15 0 05 0 09 22 0.19 0.10 0.12 43.8 140. E 0.43 0.38 0.39 ILT9 -50 20157 6 0.15 0:05 0.09 8 0.19 0.10 0.13 29.6 210 I 0.22 0.13 0.15-1LT4 60 31843 19 0 20 0 11 0 14 35 6 113 I 0 17 0 08 0 09 1LT5 -70 16000 9 0.15 0.05 009 21.2 165 F 3229 (0.13) (0.04) (0.06) 1-LT8 -70 16825 12 0.15 0.06 009 27.7 160 F 3166 (0.13) (0.04) (0.07) 1LT6 -80 13463 7 0.15 0.05 0.09 24.8 181 F 3306 (0.13) (0.04) (0.07) Tábel V
-RESULTS 0F 30mm -SPECIMENS WELDHENT 21.2
SPECIMEN TEMPE. NUMBER NUMBER AVERAGE TNTCOD CRACK- LOAD MOMENT K C'FOD- AT PRACTUR
RATURE OF OF -COI) LKN(II AT AT (*
CYCLES TESTS FRACTURE FRACTURE FRACTURE
C r-1/3 RS hou, mm mm mm mm kil r-1/3 SS mm mm-Hou. mm 2LT16 -40 570O1 28 0.21 0.12 0.14 44.1 148 E >0.38 >0.35. >0.32 2LT17 -40 43934 27 -0.21 0.12 0.14 43.1 156 E 1.21 1.29 1.91 2LT23 -40 26522 -6 0.14 0.05 0.09 -6 0.19 0.09 0.12 7 0.28 0.20 0.21 36.0 188 I 0.24 0.16 0.17 2LT24 -40 35703 -6- O-15 0.06 0.10 - -6 0.19 0.10 0.1-3 --13 .0.27 0.19- 0.20- 41,8 161 1 0.23 017 0.15. 2LT-l4 -50 29150 16 0:25 0.15 0.19 32.6 212 E 0.29 0.20- -0.22 2LT22 -50 23615 6 0._15 0.06 0.10 -6 0.19- 0.09 0.13 -6 0.28 - 0.20 - 0.22 34.1 195-1 0.29 0.21 0.22 2LT13 -60. 43609 25 0.20 0.10 0h13 40.7 155 1 0.-19 -0.12 - 011 2LT-15 --60 27551 -17 0.22 0.12 0.16 30.9 220 I 0.22 0.12 0.15 21.T18 -70 29294 27 0.15 0.06 0.08 44.5 132 E 0.20 0,14 0.11 -2LT21 -70 28112 28 0.15 0.06 0.08- 44.9 132 E - 0.25 0.20 0.16 2LT25 -70 32300 28 0.3.6 -0.06 0.09 43.5 139 E 0.33 0.29 0.26 2LT19 -80 26333 28 0.15 0.06 0.08 6-3.9 1.36 E 0.20 0.14- - 0.1-1 21.220 -90 5695 0 - - 13.6 200 F 2556 (0.09) (0.01) (0.04)
SPECIMEN TEMPE- NUMBER NUMBER -AVERAGE INTCOD CRACK-: LOAD AT MOMENT K CTOD AT FRACTUP.
RATURE 0F OF COD LENGTH AT FRACTURE OF
CYCLES TESTS FRACTURE FRACTURE
r-1/3 liS loll. r-1/3 SS- hou.
8LT42 -30 42548 6 014. . 0.05 0.09 6 0.19 0.10 0.12 16 0.24 0.16 0.16 44..7 159 E 1.61 1.77 2.92 8LT43 -40 23028 6 . 0.15 0.06 0.09 6 0.19 0.10 0.13 3 0.28 0.19 0.21 31.5 215 I 0.27 0.18 0.20 8LT40 50 50401 25 0 20 0 11 0 12 43 2 150 I 0 20 0 14 0 11 8LT44 -50 29156 17 0.21 0.11 0.14 32.9 207 II 0.38 0.30 0.33 8LT45 60 24674 14 0 19 0 09 0 12 32 7 212 I 0 19 0 09 0 11 8LT41 70 31175 28 0 15 0 06 0 08 44 3 143 E 0 26 0 21 0 17 Moment of fracture:
E - Fractura mt final COD-teat.
t - Frn.-.turo intur,nedjnto COD-,:oui,.
Frneture during fmtigtio.
Tabal VI
RESULTS OF 3Omm SPECIMENS. WELDMENT 8LTa
SPECIMEN TEMPE- NUMBER NUMBER AVERAGE INTCOD CRACK- WAD MOMENT K CTOD AT FRACTUR RATURE OF OF COD LENGTH AT AT OF
CYCLES TESTS FRACTURE FRACTURE FRACTURE
C r-1/3 SS Hull, min min mm mm kM r-1/3 mm ES mm Noii. mm 8LT37 -20 28208 6 0.19 0.11 0.12 22.3 252 I (6270) 0.19 0.11 0.13 15 0.19 0.11 0.12 45.2 154 E 1.50 1.61 2.66 8LT28 30 9092 3 0 24 0 17 0 20 21 4 260 I 0 28 0 20 0 23 8LT29 -30 30278 26 0.21 0.12 0.13 46.7 130 E 0.25 0.22 0.16 8LT31 -30 20855 13 0.26 0.17 0,20 30.3 233 I 0,24 0.15 017 8LT32 -30 17288 7 0.24 0.15 0.19 22.2 260 I 0.24 0.15 0.18 8LT39 -30 11644 4 0.19 O,.1O 0.14 19.7 248 I 0.18 009 0.13. 8LT30 35 30919 20 0 21 0 12 0 15 35 5 178 I 0 18 0 09 0 10 8LT27 -40 5600 1 17.0 243 I 0.15 0.06 0.10 8LT33 -40 8101. 1 - 16.1 225 I 0.12 0.04 0.08 8LT34- -40 22620 8 . 0.15 0.05 0.09 7 0.19 0.10 0.12 30.9 193 I 0.17 0.08 0.10 8LT35 -50 18132 6 0.15 0.06. 0.09 5 0.20 0.10 . 0.13 27.2. 198 I 0.16 0.07 0.09 8LT36 60 48500 28 0 15 0 06 0 08 44 1 127 E 0 14 0 07 0 06 8LT38 -70 12300.8 . 0.15 0.06 0.10 22.6 187 F 3206 (0.11) (0.02) (0.05) Tabal VII
RESULTS. OF 30mm SPECIMENS WEU)NENT SLTb
SPECIMEN TEMPE- NUMBER NUMBER AVERAGE INTCOD CRACK- LOAD MOMENT K CTOD AT FRACTUR
RATURE 0F OF COD. LENGTH AT AT 0F
CYCLES TESTS. FRACTURE FRACTURE FRACTURE
- - - . r-1/3 SS Hou-. r-1/3 ss hou.
Tabel VIII
RESULTS OF 70mm SPECIMENS
Moment of fractura:
E - Fracture at final COD-teat.
I - Fracture at intermediate COD-teat.
F - Fracture during fatigue.
11LT15 -30 b 55865 6 0.20 0.09 0.15 6 0.30 0.19 0.24 6 0.38 0.29 0.34 62.7 650 E 0.56 0.49 0.60 ÏILT16 -30 b 42611 22 0.20 0.09 0.13 66.3 600 E >1.58 >1.66 >2.20 11LT22 .30 e 51151 6 - 0.20 0.09 0.14 6 0.30 0.19. 0.24 8 0.39 0.29 0.35 63.0 660- E 0.62 0.56 0.70 11LT12 -40 b 62326 5 0.19 0.08 0.14 .5 0.24 0.14 0.18 5 0.29 0.18 0.23 4 0.39 0.29 0.35 60.0 655 1 0.36. 0.26 0.30 11LT13 .40 b 39600 19 0.20 0.09 0.13 62.2 625 >0.95 >0.93 >1.32 11LT19 4O e 40723 6 0.20 .0.09 0.14 6 0.24 0.13 0.17 10 0.29 0.18 0.21 67;3 .550 E 0.82 0.81. 1.00 11LT2O 4O e 40256 6 0.19 0.08 0.14 6 0.29 0.18 0.23 7 0.39 0.29 0.36 61.0 630 I 0.27 0.16 . 11LT23 -40. o 53208 3 0.20 0.10 0.14 3 0.29 0.22. 0.24 5 0.38 0.32 .0.34 64.9 . 650 B 1.97 2.15 3.69 11LT27 -40 o 33203 . 3 0.20 0.09 0.15 3 0.30 0.19 0.24 2 0.39 0.29 0.35 53.2 675 .1 0.26 0.14 0.18 I1LT8 -50. a 32538 6 0.20 0.08 0.14 8 0.35. 0.24 0.30 51.0 785 B 0.36 0.25 0.31 11LT9 -50 a 16 . 0.19 0.08 0.13 60.2 645 E 0.65 0.59 0.76 11LT25 -50 o 30046 6 0.20 0.08 0.16 6 0.30 0.19 0.25 3 0.39 0.29 0.36. 51.5 730 I 0.28. 0.16 0.21 11LT2 .60 a 44722 21 0.24 0.12 0.17 66.3 559 E 0.50 . 0.43 0.52 11LT11 -60 . b 21332 6 0.20 . 0.08 0.i4 5 0.35 0.24 0.31. 42.8 893 .1 0.34 0.23 0.29 11LT21 -60 o 46827 6 0.20. 0.07 0.14 -16 0.29 0.16 0.23 67.8 545 E 0.35 0.25 0.29 11LT24 .60 c 51130 .3 0.19 0.08 0.14 -9 0.30 0.19 0.24 69..9 510 E 0.32 0.23 0.25 11LT26 -60 c 39632 3 0.20 0.09 0.15 IILT6 -70 a 35678 17 0.23 0.12 0.16 67.6 517 E 0.24 0.14 0.15 11LT17 -70 b 32008 . 19 0.19 0.08 0.12 65.9 515 E 0.25 0.14 0.16 t1LTI8 -70 b. 13656 6 O19 0.08 0.13 35.8 713 F (4019) -1ILT4 -80 a 10438 4 0.19 0.07 0.14 30.]. 787 F (0.17) (0.06) (0.11) 11LT5. -80 a 12 0.19 0.08 0.13 49.5 790 E 0.33 0.21 0.27 1ILT14 -80 b 30487 4 0.20 008 0.15 12 0.25 0.13 0.18 57.0 655 ¡ .0.25 0.12 0.17. 1ILT1O -90 b 2616 0 17.5 850 F 3015 1ILT7 -100 a 3800 . 0 19.4 850 F 3166
SPECIMEN TEMPE WELD NUMBER NUMBER AVERAGE INTCOD CRACK- LOAD AT MOMENT K CTOD AT FRACL'UR
RATURE MENT OF 0F COD- LENGTH AT FRACTURE OF
CYCLES TESTS FRACTURE FRACTURE
r-1/3 ES Holst r-1/3 ES Holst
o. 750 700 -60o. MPc 550- 500- 50- 400-j I- - I--150 -100 -50 0 .50
I c
fig. 1 Yie].,d strength an-d ultimate tensIle strength of we:1d rnàt-erial
ob
071
fig.3
Geometry oP 70mm specimen.
w C w E o EI-w-J D.. mc o L." wo EL
'-I
zo
fig.4 Indication of orientation for epecimens- taken out from platee.
S.w nil noti
fig.S Instrumentation of' fabalt-teet specimen.
I
I
I
I
f12.6a lest eqwipment for testIng 30mm specImens.
t4
fig.6b Test equipment foi' tesLing 70mm specimens.
e
I
fig.?
10 20 30 40 50
CRACKLENGTIH a mmi
Maximum load and stress intermsity faötor (K) during fatigue
for fabalt spec:imeriS, based on reachIng, the yield stress at
the cracktiP wt:h a Unear stress distribution over the
fig.8 Calculation of COD c:racktip value èsûming a p]ast'i':c. hinge. loo -90 80 -7o 60 50
-:40
I-ru Q. 'J 4-'n IQ 20 io O pø5Iic binge o CT.O.OE(mm)TH De Ift
TEST DATA: n n n cyclea e61 fa mm mm 8510 9460 10298 11270 12296 13073 13996 14888 15777 16660 17533 18595 19473 20495 21491 22540 24389 25408 26679 28145 28173 30927 32370 34005 35703 33 35.50 34 36.71 35 37.71 36 38.77 37 39.83 38 60.84 39 41.83 COD C0D.5 0.25 0.27 0.27 0.29 0.30 0.30 0.40 0.42 0.43 0.44 0.45 0.47 0.69 0.72 0.73 0.75 0.77 0.80 0.82 0.85 0.88 0.89 0.91 0.95 0.86 mum min 0.06 0.08 0.09 0.10 0.12 0.12 0.19 0.21 0.23 0.24 0.25 0.27 0.44 0.48 0.50 0.53 0.56 0.61 0.64 0.69 0.73 0.78 0.83 0.91 0.85 SPECIMEN PARTICULARS: REMARKS:Fracture at intermediate COD-test.
fi.9a
Tesl data of specimen 2LT24 from /13/.
200 234 208 0.1.5 0.06 0.10 237 202 0.16 0.07 0.11 231 197 0.15 0.06 0.10 225 191 0.15 0.07 0.10 219 186 0.15 0.06 0.10 212 181. 0.15 0.06 0.09 226 175 0.19 0.10 0.13 225 170 0.20 0.10 0.13 222 165 0.19 0.10 0.13 217 1.0 0.19 0.10 0.13 214 155 0.19 0.09 0.12 207 1.51 0.19 0.10 0.12 208 166 0.28 0.19 0.21 205 141 0.28 0.19 0.21. 203 132 0.27 019 021 200 132 0.27 0.19 0.21 195 128 0.27 0.19 0.20 191 123 0.27 0.19 0.20 187 119 0.27 0.19 0.20 182 115 0.27 0.20 0.19 178 111 0.27 0.20 0.19 174 107 0.26 0.20 0.19 170 103 0.26 0.20 0.18 1.66 99 0.26 0.20 0.18 161 0 0.23 0.17 0.15
p p CTOD CTOD CTOD
Illax min 1/3R BS Hou. kN kN tam sum mia
SPEC IMEN: 2 LT 2 4 DATE: 21-11-85 TEMP.: -40 C 29.5 mm 90. mm 150 mm 569 N/mm2 1.6 mm 18.5 mm 0.3 4 Hz B: W: S: si gma - y: z: R: freq: 15 16 17 18 19 20 21. 22 23 24 25 26 27 28 29 30 31. 32 10.00 15.51 16.68 17.72 18.86 20.54 21.53 22.60 23.67 24.77 25.86 26.91 28.06 29.09 30.16 31.11 31.92 33.34 34.35
C. T o D 0.2
H
CTOD-CURVZ 5PECtl1EN NR. 2L724 n---C.rsklongth LmIJfi.9b 'ETOO curve of specimen 2LT'24 from /3/.
/
r
. 1 I' i! I, I.IR 89fig.9ò Load curve o-F' specimen 2LT24 from /13/.
LORD SCOiJENCE OF SPECZÑEÑ NR 2LT24
240 230 -220 2*8 280. *90 180 ¡10 lee -ISO P *40 -¡38 k ¡20 IJIO -laß- w9e -80... 10 -Ge 40 ,30_ 20 10 e S IO IS 20 29 30 39 4e 45, CrckIngh LJ
TH Deift
1iLT.22
TEST DATA:
REMARKS:
Fracture at end COD-test.
n a a COD COD-S cycles est Es mm mm mm mm 0.07 0.09 0.11 0.12 0.15 0.16 0.32 0.34 0.37 0.40 0.43 0.47 0.54 0.60 0.84 0.92 0.84. 1.14 0.7,7 0.00
fig.lOa Tcst dat1
of specimen 11LT22 from :113/.
.10.0 6712 22 23.1 0.33 8227 26 25.2 0.34 9625 26 26.9 0.35 11205 28 29.0 0.37 13204 30 31.2 0.38 14562 32 33.0 0.40 16479 34 35.4 0.62 17628 36 36.9 0.64 19057 38 38.3 0.66 21378 40 40.4 0.69 24385 42 43.2 0.71 26019 44 611.9 0.75 28188 46 66.6 1.03 31167 48 49.1 1.07 36036. 50 51.4 1.12 36880 52 53.6 1.15 60290 54 56.1 1.16 43510 56 58.2 1.25 67167 58 604 1.30 51151 60 63.0 2.19 1' max kN P min kN 850 CTOD l/3R ,mn CTOD RS mm CTOD Hou. mm 924 782 0.20 0.07 0.15 918 '55 0.20 0.08 0.15 897 729 0.20 0.08 0.14 872 703 0.20 0.09 0.14 831 678 0.20 0.09 0.14 808 653 0.20 0.09 0.14 890 629 0.30 0.19 0.24 895 605 0.30 0.19 0.24 893 581 0.30 0.20 0.25 868 558 0.30 0.19 0.24 836 536 0.29 0.19 0.24 820 513 0.30 0.19 0.24 803 492 0.40 0.30 0.37 780 471 0.40 0.30 0.36 753 450 0.39 0.29 0.36 731 430 0.39 0.29 0.35 703 410 0.37 0.27 0.32 681 391 0.39 0.29 0.34 660 372 0.38 0.29 0.34 660 0 0.62 0.56 0.70 SPECIMEN: 11LT22 DATE: 16-8-85 TEMP.: -30 SPECIMEN PARTICULARS: B: 6.9.4 mm W: 140.4 mm S: 210 mm sigma-y: 523 N/min2 z: 3 mm 24 min R: 0.3
freq:
4 Hzn
0.8 L? 0.8 -LS C 0.4_ n 0.3 0.2 0. I-
/r-ii
/
/r
/
e , , I I I I t I $ t II'll
I I I 23.125.220.8 29 31.2 33 3!'3ø.930.a'0.4'3.2'4.94G.G49.ISl.453.65G.l90.2BB.4 83 CraokIin9t,h Lm.nif.ig.iObcTOD curve of specimen i.1,L122 from /13/.
I 3R
-.-H1ea.
flg.lOc Load curve of specimen 11LT2,2 from
/13/.
950 900 eso 800...
LORD SEQUENOE or 0PCDIEN NR. I 1LT22
+ ?S0... 60e... 550ì P 500... k N 458:_ 400 380 300... 250 200 150... 106 50 '0
-IO 20 30 40CtIoNjitLiiJ
50Li 0,6 0,5-0,2 0,1 0.6-0,5 0,4 A V O ILl A V O ZLI
&! 4waIdaaa eucj
I I ftt,,r. th,ri.Q Iatíua-t,st LfIU at C 00-tilt Laa,raq. valuai of m$,r.adat. (700 -0° E E0,3 Ò Ò -0,1 O -80° A V i.,td.nt IILT..1 A V O oildau lILr-bL A V O O witd.il,t lILT-c I
'-L
L---J 1__,_JL---J L_---J L_---J
I liest tempI -70° -60° -50° -40° -35° -30°-Pig.11a Overview of 30mm fabalt test results, ClOD calculation based on r1/3.. 'fractura dormO -faIqu.-t.it frituri it C 00-t.,, avurig. va4uo of mtorm.dlatu (TOO QOZ 065e >O95Ô 4.04 ô1615 è1503 >133 1.9 L__r_J L__.__J L_ L ---:Test temp.(°C1 -70° -60° -5O -40° -30° -20°
fig.11b Overview of 70mm fabalt test results, ClOD calculation
rP (n rP (D U) C rP u) C)
4 o
o
C)O'.
I
o C a' o U 0,2 ZO tri _90080°
'7,' 45b.'
*,
¡
L__T__J7ö°
-oo° 500 Test temperature (°C) L---_35030°
N O. Doc
orn Q.J. 0,5V Q
A V
A V
O wetdrnent 1lT]
O wetdrnent 2LT wetdment 8LT4I ii J
'fracture during s., I I I go o I fatigue-test. i at C.0 -testrr4
o L average valijas o interñiediate c.to.awo
Cfl3 0,4 >0.829 1.268 4,51-b I-a. 0.6, OC
orn.
I-w
I' orrb
D. cn33.
n w V. 'J,,, r D I-I
,O1O
I-I-100C) nAo I-. 7V Û. oA V 9
weidment 11LT-a'A V O
wetdment 11LT-b1AV Q
Owetdment i1LTcJ I I fracture during I I fatigue-test. at C.a-fest'average ,vatues of intermediate C.tD.D.
V
13 a 9 25 12 L_,_JL_.rJ
L_J
7O0.
6O 5Ø0-40°
.Test temperature (°t)
>.0.931
0.81 2i5 4 L..,_JL---J
-I, t-' QQ (J, O (D rlW 'l (DQQ ' ((D (A (n tDt-' (no Pt-.. (D
-.
ESt)
E5th
-
d
Li ('(D3m
CAZ I- rr C-) -4 o o (D C ID (A 2,2- 1,2 1,0 0,8 0,6 - 0.4 - 0,2 o -100 -80° -70° -60°5°
-40° -30° L20° Test temperature ('C) 2.2 o O weIdmenf I LT ie(dmenf 2 LT wewrnent 8 momenP of fracture:: F 3 A16 25 64b io &lbOi4O''
21-9l
AObOi
42b
lest temperature (T) 30mm specimen. (B30rnrn ; W = 90mm)37a
37a -100°-'i'
-80° -k.. 60° -50° -'p° -30° -20° _10°
2,2-QQ
eicLx;O;i3:16;19en23
---ecL.:.;13:16;19en23
-.
-br- OiD orn rl- Ql
m'i
D 1,6
Ô.,
flED U) UI cno -D -.4,'--1,2 -Julo
30
-E1.0 cnO E -Oc -w'--q
o. D rl-0,6o
o
2,0 -o -4-J.
ç:io
P 3 3 '-Joe U) Ql o p.,. 3 ID D U) û al I-' o C I-. a' rl- Ql o- al o C, w (n 2.2weidment liLT-a wetdment il LT -.b
2.0 0 weWme't 1ILT#c niornèñt of fracture: F i .8 1,6 0,6 0.4 0.2 o
è3
130'9
16.9.
0
01511 O2411Ofl"
176
026° 025" 2O O' -10 e -100° -90° -80° _700 -60° _500 -40° -Test temperature ('C) 70mm specimens (B=lOmm W=140mm) rl-O i i i i I I i I I -10O° -90' 80° 70° -60° -50° 400 -30° . _200 100 0° Test temperature ('C)E E
o
ci 2,2 2.0 1.8 1,6 1.4 1,2. 1.0 0,8 0!6 .4 0.2 30mm specimen British Sandertd 70mm specimen 30mm specimen==
7Omm specirneñ r-1/3 o 100° -90° -80°-7o° -°
4Q03°
Test temperatijre 1°C) 20° _100 -4, I-J. 2,2- 2,0 .1.8 OD '-'-O.3"
ml-'i
wO o -I, 1,4 I- (D 1,2 (D QQ ,E1
E U) -U) ' cio.
LI 0,8 06 UI O -4, 0,4 3 o. 0,2 o. D 3 3 -30mm specimen British Stnderd .70mm specimeno---t
i-i I I t 1000 -50° -80° -70° _600 50° _400 -30° _200 -10° 'Test temperature (°C)1ß 0,9 0,8 0, E; E , 0,6
tJ.
4. Q3: 0,2 1/3_7 HOLLSTEIN IlL! 30mm. 8/W.0,33 1 Z:3.14,4,
<V .', British Standard 70mm.f.. '
B/W5.f,',,
J,
dr,
ritish Standard P30mm 8/W! 0.33 Ql 0,2.. 0,3 0,4 0,5 0,6 0.7 . . 0,8 0,9 C.T.OED.J. r= l/3(mm)fig.2l Comparison of ClOD values caìcu1..ted wIth rl/3., ac.dôrdirg
0,4. 1/3 0,3 0,2 0Ji