Page 289 - Handbook of Materials Failure Analysis
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4 Types of Fracture Mechanics Specimens Analyzed in Upper Shelf    285




                                                          dV
                                                    ð
                                        P f ¼ 1 exp    g σ  i I                 (12.8)
                                                     V    V ref
                  where V is the volume of the plastically deformed zone (an essential condition for
                  slip induced nucleation of cleavage micro-cracks) in the component, V ref is the ref-
                                                          3              i
                  erence volume which is usually taken as 0.001 mm . The function g(σ I ) expresses the
                  probability of failure of an infinitesimal volume i (having volume dV) according to
                  the expression
                                                      dV
                                              dP f ¼ g σ  i I                   (12.9)
                                                      V ref
                        i
                  where σ I is the maximum principal stress acting at a material point i in the plastically
                  deformed region having volume dV. According to Beremin’s model [20] (which uses
                  Weibull’s statistics for distribution of defects responsible for triggering cleavage
                                                        i
                  according to Griffith’s theory), the form of g(σ I ) is defined as
                                                       m
                                                      i
                                                i     I
                                                     σ
                                              g σ ¼                            (12.10)
                                                I
                                                     σ u
                  where m and σ u are the Weibull’s shape and size parameters, respectively. Using
                  Equation 12.10 in Equation 12.8, one can obtain the probability of cleavage fracture
                  P f at any given loading as [20]
                                                          m

                                                       σ w
                                          P f ¼ 1 exp                          (12.11)
                                                       σ u
                  where the loading parameter is defined as the Weibull stress σ w and is expressed
                  as [20]
                                                s ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
                                                   n
                                                  X    m V i
                                                m     i
                                            σ w ¼    σ                         (12.12)
                                                      I
                                                  i¼1    V 0
                  In this chapter, Equation 12.11 is used to calculate the probability of cleavage frac-
                  ture of the CT specimen at different loading levels and at different temperatures,
                  where the Weibull stress will be calculated using the stress field ahead of the growing
                  crack using Equation 12.12. The nonlocal Rousselier’s damage model has been used
                  to calculate the crack-tip stress field. The effect of evolution of damage (ductile void
                  volume fraction) on the stress field is taken care of by this model and hence, the effect
                  of prior stable crack growth before initiation of cleavage fracture is modeled implic-
                  itly through this framework.


                  4 TYPES OF FRACTURE MECHANICS SPECIMENS
                  ANALYZED IN UPPER SHELF AND DBTT REGIME
                  The nonlocal formulation of the Rousselier’s damage model was used for simulation
                  of fracture resistance behavior of various types of specimens in the upper-shelf as
                  well as the DBTT regime. There are various advantages of the nonlocal formulation
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