assesment of interaction effect between two aligned surface cracks in elbows subjected to internal...
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Proceedings of the ASME 2010 Pressure Vessels & Piping Divis ion / K-PVP ConferencePVP2010
July 18-22, 2010, Bellevue, Washington, USA
PVP2010-25604
ASSESMENT OF INTERACTION EFFECT BETWEEN TWO ALIGNED SURFACECRACKS IN ELBOWS SUBJECTED TO INTERNAL PRESSURE
Han-Beom Seo, Jae-Boong Choi and Young-Jin K imSchool of Mechanical Engineering, Sungkyunkwan University
300 Chunchun-dong, J angan-gu, Suwon, Kyonggi-do 440-746, Republic of Korea
Yoon-Suk ChangDepartment of Nuclear Engineering, Kyung Hee University
1 Seochen-dong, Giheung-gu, Yongin, Kyonggi-do 446-701, Republic of Korea
Hyun-Su KimKorea Power Engineering Company, Inc.
360-9 Mabuk-dong, Giheung-gu, Yongin, Kyonggi-do 449-713, Republic of Korea
ABSTRACT
Adjacent multiple cracks can be found in power plant
components such as pressure vessel, piping and so forth. Ifmultiple cracks are detected, it can be affected significant effect
to structure integrity due to high interaction effect of the
multiple cracks. Therefore general fitness-for-service (FFS)
codes and standards propose assessment method for the
multiple cracks. The Section XI of ASME Code suggests crack
coalescence method for multiple cracks. It employs the
approach combining neighbored cracks as single crack if the
distance between them is close. In some cases, since this
combined rule can be considered as a conservative approach,
more accurate investigation of the interaction effect between
multiple cracks is needed. In this study, the interaction effect
between two aligned coplanar circumferential surface cracks in
elbows subjected to internal pressure was investigated. Sincemost previous studies dealt with only plates or straight pipes,
the present research was centered on cracked elbow. FE (Finite
element) limit analyses were carried out by changing elbow
geometries and crack shapes. Also, applicability of the current
criterion for the multiple cracks was discussed.
INTRODUCTION
During in-service inspection (ISI), several adjacent flaws
are frequently detected in power plant components. If theses
adjacent flaws are located nearly, they can have a significant
effect on structure integrity due to interference of stress field
around crack tip. Accordingly, the adjacent multiple cracks
should be treated in fitness-for-service (FFS) to evaluate
precise structure integrity. Generally, various FFS codes and
standards such as Section XI of ASME Code[1], JSMECode[2], API 579[3] proposed assessment approach for the
adjacent multiple cracks.
The Section XI of ASME Code recommends the crack
coalescence model to estimate structure integrity of multiple
cracks. If the distance between the adjacent cracks is equal to
or less than specific criterion which depends on the crack
depth, they are substituted as a single crack. However, this
coalesced rule is regarded as conservative manner in some
cases. It means that the interaction effect of adjacent cracks is
highly estimated. Several researches are performed to examine
the interaction effect between the adjacent cracks and its
conservatism[4,5]. To evaluate the interaction effect around
adjacent cracks, fracture mechanics assessment methods wereutilized such as linear elastic fracture mechanics, elastic plastic
fracture mechanics and limit load analysis.
In this study, detailed parametric 3-dimensional plastic
limit analyses for two aligned surface cracks in elbows are
carried out. Conservatism of coalesced criterion in the Section
XI of ASME is reviewed and assessment of interaction effect
between multiple coplanar surface cracks in elbow is
investigated.
CONSERVATISM OF COALESCED CRITERION INASME SECTION XI
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In accordance with the Section XI of ASME, when thedistance of adjacent multiple cracks is too close, they are
substituted as equivalent single cracks. To determine the
combined condition, the standard of distance between adjacentcracks (S) and offset distance (H) are defined as follows;
H 13mm (1)S 0.5 max (a1, a2)
where l is the crack length and a is the crack depth as
demonstrated in figure 1. In case of aligned coplanar flaws, theoffset distance is ignored. Only the distance between adjacentcracksis solely remained to determine the combined condition.The size of equivalent single crack was determined as follows;
l = l1+l2+S (2)a = max (a1, a2)
Furthermore, the limit load solution for the elbow with asingle crack (PL) subjected to internal pressure was proposedby Kim et al.[6] as follows;
l1 S l2
a1
a2a
Coalesced
single crack
Fig. 1 Combined rule of the adjacent multiple cracks in ASME
SECTION XI
0.0 0.2 0.4 0.6 0.8 1.00.2
0.4
0.6
0.8
1.0
1.2
Maximum
difference : 37%
Rm/t= 5 , = 0.5
Eq. (3)
FE results (Dual crack)
PL
/PO
a/t
Fig. 2 Comparison of normalized FE limit pressure betweenmultiple cracks and coalesced single crack
min 1.0, 3.9 1.5 1.5L
o
P a
P t
(3)
2
2
3 (1 exp( ( / ))o o
B m
tP
r A B R t R
(4)
0.09
1.19 1 1
0.0013 0.307
rA
t
rB
t
where PO is the un-cracked limit load subjected to internalpressure. The plastic limit pressure with cracked elbow is
normalized to the limit load pressure of un-cracked.Some limitations of the ASME coalesced criterion were
confirmed throughout the preliminary FE analyses. Figure 2shows comparison of the normalized limit loads between dual
cracks by FE results and coalesced single crack by Kimssolution[6]. The single crack was combined by ASMEcriterion. As shown in Fig. 2, when a/tis smaller than 0.5, thedifference between them was approximately 7%. It means thatthe coalesced criterion is useful in given condition. However,
as the increase of the a/t value, the difference increased morethan 37%. It means that the coalesced criterion is tooconservative as crack depth is deeper.
DETAILED FE ANALYSESThe FE limit load analyses were carried to evaluate
interaction effect of multiple cracks. Detailed procedure was
described in the following sub-sections.
Geometry
Figure 3 demonstrates the geometry condition of elbow inthe present work. The piping system was conducted as
attaching the two straight pipes at the end of 90 elbow. Notethat the length of straight pipe is three times of outer radius ofpipe. Herein, RB is the bend radius andL is the length ofstraight pipes. Several variables are chosen to perform the FEanalyses for multiple cracks and coalesced single crack. Figure
4 demonstrates the shapes of crack were employed in thepresent work. Multiple crack depth, angle and length aredenoted as a, , and l. Also, single crack angle and length aredenoted as S andlS. The relevant range of these variables wasconsidered. Values ofRm/t as 5 and 10, four values of a/t
ranging from 0.25 to 1, three values of / from 0.167 to 0.5and two values ofRB/Rm as 2 and 4 are selected. Furthermore,both of coplanar cracks which have identical geometry wereconsidered. The distance between multiple cracks is taken into
account as a1/2 preferentially in the present work.
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RB
Extrados
Intrados
Crack
L
Fig. 3 Schematic illustration of 90elbow with a crack
a a
S
t
Rm Ro
l l
as
ls=l+S+ls
t
Rm Ro
(a) (b)Fig. 4 Geometry and dimensions for (a) circumferential
coplanar aligned surface cracks and (b) circumferentialcoalesced single surface crack
Analysis Method
Figure 5 shows typical FE models used in this study. Sincethe geometry of cracked elbows has a symmetric characteristic,
a half model was generated. To avoid incompressibilityproblem, iso-parametric reduced twenty-node quadratic brick
element (C3D20R in ABAQUS element library) wasutilized[7]. Approximately 11,000 nodes and 48,000 elementswere used to build the model. To verify the model, the FE
results of single crack and Eq. (3) was compared in figure 6.Note the geometry and dimension of adjacent dual cracks andcoalesced single crack in figure 4. As a result, the maximumdifference was less than 7% as depicted in the figure. It shows
that applicability of the employed FE model. Internal pressurewas applied to inner surface of elbow and crack face. Also,
(a) Elbow with single surface crack
(b)Elbow with multiple surface cracksFig. 5 Typical FE models employed in the present study
tension load is added at the end of attached straight pipe forconsidering end effect[8]. Material was assumed to obeyelastic-perfectly plastic approximation in the FE analyses.
Material properties is defined; Youngs modulus as 182.7GPa,Poissons ratio as 0.3 and yield strength as 194MPa,respectively. ABAQUS RIKS option was utilized to obtainreliable estimate for the load carry capacity of structure innonlinear analysis.
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0.0 0.2 0.4 0.6 0.8 1.00.6
0.7
0.8
0.9
1.0
1.1
1.2R
m/t= 5, = 0.167
Eq. (3)
FE results (Single crack)
PL
/PO
a/t
Fig. 6 Verification of solution for single surface cracked elbow
Analysis Results
In the preliminary study, the conservatism of coalesced
criterion of ASME code was confirmed in figure 2. To verifymore precisely this conservatism, limit pressure betweenmultiple cracks and coalesced single crack is compared in
figure 7. Here, limit pressure of multiple cracks by FEA(PLM) isnormalized to that of single crack by Kims solution(PLS)[6].
This figure shows that most of PLM/PLS values are higher than1. and increasingly higher as crack depth and length are deeperand longer. It represents that ASME criterion for multiple
cracks is too conservative.To investigate detailed interaction effect of limit pressure
for multiple cracks, the variation of normalized FE limitpressures for adjacent surface crack with a/tand/ is shown
in Fig. 8 and Fig. 9, respectively. Also, limit pressure ofcracked elbow is normalized to that of un-cracked elbow. WhenS=a/2, effects of geometric variables on interaction effect formultiple cracks were exposed;
0.0 0.2 0.4 0.6 0.8 1.00.8
1.0
1.2
1.4
1.6
1.8
2.0
= 0.167,Rm/t
= 0.167,Rm/t
= 0.333,Rm/t
= 0.333,Rm/t
= 0.5,Rm/t
= 0.5,Rm/t
PLM
/PLS
a/t Fig. 7 Comparison of limit pressure between multiple cracks
and coalesced single crack
0.0 0.2 0.4 0.6 0.8 1.00.2
0.4
0.6
0.8
1.0
1.2
Eq. (3) = 0.167
Rm/tR
B/R
m
Rm/t=5R
B/R
m
Rm/t=10R
B/R
m
Rm/t=10R
B/R
m
PL
/PO
a/t
t
Rm
(a)/= 0.167
t
Rm
0.0 0.2 0.4 0.6 0.8 1.00.2
0.4
0.6
0.8
1.0
1.2
Eq. (3) = 0.333
Rm/tR
B/R
m
Rm/t=5R
B/R
m
Rm/t=10R
B/R
m
Rm/t=10R
B/R
m
PL
/PO
a/t (b)/= 0.333
0.0 0.2 0.4 0.6 0.8 1.00.2
0.4
0.6
0.8
1.0
1.2
= 0.5Eq. (3)R
m/tR
B/R
O
Rm/t=5R
B/R
O
Rm/t=10R
B/R
O
Rm/t=10R
B/R
O
PL
/
P
O
a/t
t
Rm
(c) /= 0.5
Fig. 8 Variation of normalized limit pressures with different a/t
for adjacent multiple surface cracks in elbow
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(i) Normalized limit pressure for adjacent multiple crackswas almost unaffected byRB/Rm. In all cases, the differences of
limit pressure between RB/Rm=2 andRB/Rm=4 was below 3%
regardless of anther variables.(ii) In the case of part through-wall cracks, the normalized
limit pressure for multiple cracks had no change aroundPL/PO=1 even though crack length and depth have somewhathigh value. In the Fig. 8, the normalized limit pressure forcoalesced single crack linearly decreased if the crack depth andcrack length have high value. However, FE results weremaintained constant aroundPL/PO=1 to a/t=0.85. Also, in the
Fig. 9 (a) and Fig. 9 (b), FE results were maintained constantaround PL/PO=1 to /=0.5. It demonstrated that combinedcriterion highly estimate the interaction effect of the adjacentcracks. Only in the case of a/t, / is sufficiently small, a/t issmaller than 0.5 or/ is smaller than 0.167, FE results and the
normalized limit pressure for coalesced single crack had a goodagreement with Eq. (3) and ASME coalesced criterion isproper. At this time, these differences are less than 8%.
(iii) In the case of through-wall crack, the interaction effectfor adjacent multiple cracks is affected by Rm/t. Note that a/t=1
indicates the trough-wall crack. In case of part through-wallcrack (a/t
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0.0 0.2 0.4 0.6 0.8 1.00.2
0.4
0.6
0.8
1.0
1.2R
m/t= 5 ,R
B/R
m= 2
Eq. (5)
/
/
/
PL
/PO
a/t
Increasing,
/= 0.167,0.333,0.5
(a) R
m
/t=5
Increasing,
/= 0.167,0.333,0.5
0.0 0.2 0.4 0.6 0.8 1.00.2
0.4
0.6
0.8
1.0
1.2R
m/t= 10 ,R
B/R
m= 2
Eq. (5)
/
/
/
PL
/PO
a/t (b)Rm/t=10
Fig. 10 Comparison of FE limit pressure with Eq.(5) for surface
crack
CONCLUDING REMARKSIn this paper, through the FE limit analysis, the
conservatism of coalesced rule recommended by the Section XI
of ASME was investigated in some geometric shape. DetailedFE analyses were performed to evaluate interaction effectincluding multiple cracks in elbow by evaluating thenormalized failure pressure. The conservatism of Section XI ofASME criterion for adjacent multiple cracks was investigatedand prediction of limit pressure for multiple cracks was
proposed. However, since the research only focused on theS=a/2 case, it has still some remained weakness. Thus, theadditional research which is related with variable S will benecessary as well as that effect of crack size should beconsidered.
0.0 0.1 0.2 0.3 0.4 0.50.2
0.4
0.6
0.8
1.0
1.2
Eq. (5)
Rm/t= 5
Rm/t= 10
a/t= 1 , RB
/Rm= 2
PL
/PO
Increasing,
Rm/t = 5, 10
Fig. 11 Comparison of FE limit pressure with Eq.(5) forthrough-wall crack
REFERENCES[1] ASME, 2004, "Rules for In-Service Inspection of Nuclear
Power Plant Components, ASME Sec. XI, Division 1,
IWA-3000.[2] JSME, 2004, "Rules on Fitness-for-Service for Nuclear
Power Plants, S NA1-2004.[3] American Petroleum Institute, 2007, "Fitness-for-Service,
API 579-1/ASME FFS-1.
[4] Park Y-W, Song M-H, Lee J-H, Moon S-I and Kim Y-J,2002, "Investigation on the interaction effect of twoparallel axial through-wall cracks existing in steamgenerator tube, Nuclear Engineering and Design, Vol.214,pp. 13-23.
[5] Hasegawa, K., Saito, K., Iwamatsu, F.and Miyazaki, K.,2007, "Prediction of fully plastic failure stresses for pipeswith multiple circumferential flaws, PVP2007-26011, SanAntonio, Texas.
[6] Hong S-P, Kim J-H and Kim Y-J, 2009, "Limit pressures of
90elbows with circumferential surface cracks,Engineering Fracture Mechanics, Vol. 76, pp. 2202-2216.
[7]. ABAQUS version 6.7, 2008, " User`s Manual, Inc. andDassault Systems.
[8] Yahiori, K., Moffat D-M and Moreton, D-M, 2000, "Pipingelbows with cracks Part 1 : a parametric study of theinfluence of crack size on limit loads due to pressure and
opening bending, J. Strain Analysis, Vol. 35(1), pp. 35-46.