Page 512 - Biaxial Multiaxial Fatigue and Fracture
P. 512

496                        G. SHATIL AND N. ERSOY













             Fig. 8. Experimental crack growth direction (a) specimens A and B; (b) specimen C; and (c)
             specimens D and E.














                      Fig. 9. FEA mesh models for the three anticlastic specimen notch geometries
                      used in the development stage; (a) slot; (b) sphere; and (c) through hole.


             Further development of  the subsurface fatigue model
             The subsurface fatigue model developed in [6] has assumed that the initiation of fatigue cracks
             and the localized damage in ductile materials are associated with the formation of  persistent
             slip bands on a critical plane. In particular, it is assumed that if, for example, the Brown-Miller
             model for case B cracks or the Lohr-Ellison model is used for the fatigue damage, the critical
             plane  is  in  a  direction  through  the  component thickness  and  usually aligned at  45’  to  the
             surface.  It  is  therefore  argued  that,  although  the  surface  strain  dominates  fatigue  crack
             initiation, fatigue life is also associated with a secondary effect due to what may be called the
             ‘subsurface process zone’. This secondary effect is strongly dependent on the geometry of  the
             critical area and could be represented by using values of multiaxial strain parameters, obtained
             from the surface into the material’s thickness from FEA analysis by using a particular critical
             path illustrated in Fig. 1.
               In the following, the subsurface model is further developed from the analysis of a critical
             subsurface path to the use of  a critical subsurface plane. The critical plane model is based on
             the same principles previously used to modify the surface life in the subsurface path model.
             However,  while  in  the  critical  path  model  the  subsurface  strain  increments  were  used  to
             accumulate the damage, in the subsurface plane model a fraction of  the subsurface damage is
             calculated locally for reference points on  the critical plane. This  is conducted by  using the
             strain at these points to calculate a corresponding fatigue life and damage, Di =l/A!.  The total
             fatigue damage is then simply averaged and summed up over the total number of the reference
             points:
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