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  • 7/29/2019 Assesment of Interaction Effect Between Two Aligned Surface Cracks in Elbows Subjected to Internal Pressure

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    1 Copyright 2010 by ASME

    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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    2 Copyright 2010 by ASME

    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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    3 Copyright 2010 by ASME

    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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    4 Copyright 2010 by ASME

    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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    5 Copyright 2010 by ASME

    (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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    6 Copyright 2010 by ASME

    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.