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1656_C009.fm  Page 400  Monday, May 23, 2005  3:58 PM





                       400                                Fracture Mechanics: Fundamentals and Applications


                       panel is given by

                                                           ba          P  n+1
                                                 J = αε σ o  W  ha W n , )    P              (9.32)
                                                               (/
                                                        o
                                                  pl
                                                              1
                                                                       o
                       where, in the case of the center-cracked panel, a is the half crack length and W is the half width.
                       This modification was made in order to reduce the sensitivity of h  to the crack length/width ratio.
                                                                            1
                          The elastic J is equal to G(a ), the energy release rate for an effective crack length, which is
                                                 eff
                       based on a modified Irwin plastic zone correction:
                                                    a
                                                                           I
                                               a  =+      1     1    n −  1     K   2      (9.33)
                                                          PP ) βπ
                                                eff
                                                       1 + (/  o  2    n +  1   σ o 
                       where b = 2 for plane stress and b = 6 for plane strain conditions. Equation (9.33) is a first-order
                       correction, in which  a  is computed from the elastic  K , rather than  K ; thus iteration is not
                                         eff
                                                                                  eff
                                                                      I
                       necessary. This is an empirical adjustment that was applied in order to match the J values from
                       the estimation procedure with corresponding values from rigorous elastic-plastic finite element
                       analysis. This correction has a relatively small effect on computed J values.
                          The CTOD can be estimated from a computed J value as follows:
                                                                 J
                                                          δ = d n  σ o                           (9.34)
                       where d  is a dimensionless constant that depends on flow properties [27]. Figure 3.18 shows plots
                             n
                       of d  for both plane stress and plane strain. Equation (9.34) must be regarded as approximate in
                          n
                       the elastic-plastic and fully plastic regimes, because the J-CTOD relationship is geometry dependent
                       in large-scale yielding.


                         EXAMPLE 9.1

                         Consider a single-edge-notched tensile panel with W = 1 m, B = 25 mm, and a = 125 mm. Calculate
                         J vs. applied load assuming plane stress conditions. Neglect the plastic zone correction.
                         Given: s o  = 414 MPa, n = 10, a = 1.0, E = 207,000 MPa, e o  = s o /E = 0.002
                         Solution: From Table A9.13, the reference load for this configuration is given by`

                                                         P  o  .  o  b  B= 1 072ησ

                         where

                                                    a
                                             η =  + 1     2  −  a  =  0 867 for  = ab /  125/  = 875  0 143
                                                                             .
                                                           .
                                                      b
                                                    b
                         Solving for P o  gives
                                                          P o  = 8.42 MN
                         For a/W = 0.125 and n = 10, h 1  = 4.14 (from Table A9.13). Thus the fully plastic J is given by


                                                            0
                                                                  1
                                       J pl  = ( . )( . 0 002 )(414 000kPa )  (.875 m )( .125 m )  (.414 )     P     11
                                           1 0
                                                     ,
                                                                 . 10 m       .842 MN 
                                         =    × . 2 486 10  −8 P 11
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