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    International Journal o f Fracture 41: R55-R58 1989. R5 5

    1989

    KluwerAcademic Publishers.Printed n the Netherlands.

    F A T I G U E C R A C K P R O P A G A T I O N I N C O N C R E TE

    Y i W a n g a n d H e n r y J . P e t ro s k i

    D e p a r t m e n t o f C iv i l a n d E n v i r o n m e n t a l E n g i n e e r i n g

    D u k e U n i v e r si t y

    D u r h a m , N o r t h C a r o li n a 2 7 7 0 6 U S A

    t e l: 9 1 9 ) 6 8 4 - 2 4 3 4

    I t is n o w g en e ra l l y r eco g n i ze d th a t a u n i q u e r e la t io n b e t w ee n c rack

    p ro p ag a t i o n r a t e d a / d N an d s t re s s i n t en s i t y f ac t o r r an g e A K ex i s t s fo r a m a t e r i a l ,

    i .e . , in t he no ta t ion of Pa ds e t a l. [1 ]

    d a

    = f ( A K )

    (1)

    F o r m an y en g i n ee r i n g m a t e r i a ls , t h e r e la t i o n o f t en t ak es t h e fo rm [2]

    d a

    = C(zXK)

    d N

    (2)

    w h e re t h e v a l u e s o f C an d n a r e co n s i d e red t o b e m a t e r i a l co n s t an ts .

    N u m e r o u s s tu d i es h a v e b e e n p u b l i s h e d o n p o r t la n d c e m e n t c o n c r e t e f r ac t u r e

    [3 -1 2] . B u t n o a t t em p t h a s b een r ep o r t ed t o r e l a t e t h e c r ack p ro p ag a t i o n r a t e in

    co n c re t e to s t r es s i n t en s i t y f ac t o r r an g e . A t e s t i s b e i n g p rep a red t o o b t a in su ch

    i n fo rm a t i o n an d d e t e rm i n e i f (2 ) ap p l ie s t o co n c re t e .

    A l a rg e f r ac t u re p ro ces s z o n e , a s r ep o r t ed i n co n c re t e f r ac t u re te s ts , i s

    ex p ec t ed ah ea d o f a c r ack t ip , a s su g g es t ed in F i g . 1 . T h i s f a c t m ak es i t

    i n ap p ro p r i a t e t o u se t h e p h y s i ca l c r ack s i z e a i n t h e ca l cu l a t io n o f s t re s s i n t en s i t y

    fac t o r K . I t i s n ece s sa ry to ad d a p o r ti o n o f t h e f r ac t u re p ro ces s z o n e s i z e g t o th e

    p h y s i ca l c r ack l en g t h t o o b t a i n an e f f ec t i v e c r ack s i z e a

    ao = a + g (3)

    W h i l e i t i s p o s s i b le

    to

    num erica l ly eva lu a te ao by as sum ing a s t ress d i s t r ibu t ion in

    t h e f r ac t u re p ro ces s zo n e an d ca l cu l a t e th e zo n e s i ze , t h e s am e g o a l c an b e

    a c h i e v e d u s i n g a c o m p l i a n c e m e t h o d [ 9 ,1 3 ,1 4 ]. T h i s m e t h o d c a n a v o i d th e

    u n ce r t a i n t ie s i n t ro d u ced i n t h e s t r e ss d i s t r ib u t i o n a s su m p t i o n an d p h y s i ca l c r ack

    s iz e m e a s u r e m e n t a n d t h e c o m p u t a t i o n i n v o l v e d i n z o n e s iz e d e t e r m i n a ti o n .

    I n t J o u r n o f r a c t u r e 4 1 1 9 8 9 )

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    R56

    In develop ing the complianc e vs . crack s ize (C,-a) curve, a set of specimen s

    with know n crack s izes wil l be s tatically loaded. The crack mo uth openin g

    displacem ent (CMO D) wil l be plot ted against the appl ied nominal s tess o, as in

    Fig. 2. The inverse of the CMOD -G l ine s lope is the comp liance C~. Since a

    signif icant f racture process zone appears in concrete unde r mode rate G, the

    magn i tude of G needs to be kept low to ensure that the or iginal kno wn crack s ize a

    is not chan ged by the process zone. Plot t ing the data obtained from the test in a

    graph as in Fig. 3, a regression curve can be dev eloped.

    To est imate the ma xim um appl ied a , the s tress dis t r ibut ion in the process

    zone is assumed parabolic and reaching f, at a distance (8+dy) from the physical

    crack tip, whe re f, is the tensile strength, as show n in Fig. 1.- The m aterial be yo nd

    that distance is elastic and the stress profile follows that fr om linear elastic

    fracture mechan ics . The elastic s t ress prof i le is then extended back into the

    process zone by the dot ted l ine. The ver t ical asymptote of the extended curve

    determines the effect ive crack t ip, a t a dis tance 8 f rom the physical crack t ip.

    From these assumptions and Irwin s model [15]

    8 5 K ~ 2

    = t77,

    4)

    where K is the stress intensity factor calculated with effective crack size (a+8).

    Wh en neglect ing the boundary correct ion in the K calculat ion

    5(1 + ~x)

    5)

    wh ere o~ = 8/a. To kee p 8/a < 0.05, (5) gives 8/f, < 0.138. Con side ring the

    assump tions made, i t i s safe to l imit the maxi mu m appl ied nomin al s t ress G to 10

    perce nt o f f ,.

    Center-cracked-spl i t t ing-disk (CCSD) and edge-cracked-four-point-bend-

    ing-bea m (EC BB) specime ns of port land cement concrete , as show n in Fig. 4, are

    being used in the experiments . AS TM Standard E647-88 [16] is used to guide the

    specime n and exper iment designs. To minim ize crack s ize mea surem ent error , an

    increm ental-poly nomia l met hod [16] is used to reduce crack s ize ao and crack

    propag t ion rate dao/dN from raw measu rements .

    REFERENCES

    [1] P.C. Par is , M.P. G omez, and W.E. A nderson,

    The Trend in Engineering

    13

    (1961) 9-14.

    [2] P.C. Paris and F. Erdogan, Journal of Basic Engineering 85 (1963) 528-534.

    [3] M.F. Kaplan,

    Journal of American Concrete Institute

    58 (1961) 591-610.

    [4] O.E.Gjorv, S.I. Sorensen, and A .Arnesen, Cement and Concrete Research

    (1977) 333-344.

    Int Journ of racture 41 1989)

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    R 5 7

    [5] Y.S. Jen q and S.P. Shah, in Application of Fracture Mechanics to Cementi-

    tious Composites

    S.P. Sha h ed.), Mart inus N ijho ff Publishers, Bo ston 1985)

    319-359.

    [6] H. K itagawa , S. Kim , and M. Suyama,

    The 19th Japan Congress on Materials

    Reseach - Nonmetallic Materials 1976) 160-163.

    [7] V.C. Li , in Application o f Fracture Mechanics to Cementitious Composites

    Martinus N ijho ff Pub lishers, Bo ston 1985) 431-449.

    [8] R.P. O jdrov ic and H.J. Petrosk i , Journal of Engineering Mechanics 113 1987)

    1551-1564.

    [9] P.C. Perdikar i s and A.M. Calom ino, Load His tory Effect on the Fracture

    Proper t ies of P la in Concrete , a repor t on NSF Research Grant CEE-83-07937,

    Case Western Univers i ty , Cleveland, Oh io 1986).

    [10] M. W ech aran a and S.P. Shah, Journal o f Structural Division 108 1982)

    1400-1413.

    [11] M.W echarana an d S .P . Shah, Journal of Engineering Mechanics 109 1983)

    1231-1246.

    [12] S.P. Shah and F.J. McGarry,

    Journal of Engineering Mechanics Division

    47

    1971) 1663-1676.

    [13] S.E. Sw artz and C.G. Go ,

    Experimental Mechanics

    24 1984) 129-134.

    [14] S.E. Swartz, K.K. Hu, and G.L. Jones,

    Journal o f Engineering Mechanics

    Division

    EM 4 1978) 789-800.

    15] G.R. Irw in, in

    Mechanical and Metallurgical Behavior of Sheet Material

    Procee dings of 7th S agam ore Ordn ance M ater ia l Research Co nference, Syracuse ,

    NY 1960) IV-63.

    [16] ASTM E647-88, in Annual Book of ASTM Standards 03.01 1988) 714-736,

    2 November 1988

    y

    ft

    \

    \

    \

    a

    C ~ 1 I

    F i g u r e i . S t r e s s d i s t r i b u t i o n i n c o n c r e t e a h e a d o f c r a c k t ip .

    fnt Journ of racture 41 1989)

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    R 5 8

    aV;OD

    Cp

    F i g u r e 2. C o m p l i a n c e e v a l u a t i o n .

    F i g u r e 3. C o m p l i a n c e - c r a c k s i z e

    c u r v e .

    ~ ~

    t t

    F i g u r e 4 . S p e c i m e n s b e i n g u s e d .

    Int Journ of racture

    41 1989)