Page 56 - Fiber Fracture
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MODELS OF FIBRE FRACTURE                                              41

           a                                                      1      I\     I










            b









                 NUCLEATION                GROWTH                COALESCENCE
            Fig, 6. Nucleation, growth and coalescence of  voids: (a) in the necking zone; (b) near cracks and notches.

           and  perfect fibres, (Fig. 6a) or  in  stress concentrators, near  some cracks  or  notches
           (Fig. 6b); the triaxiality ahead of  the crack tip provides sufficient stress elevation for
           void nucleation, so growth and coalescence of microvoids are usually the critical steps
           in ductile crack growth.
             Modelling ductile fibre failure, using the continuum approach, should consider all
           these  facts.  A  number  of  models  for  estimating  void  nucleation  stress  have  been
           published; among them, those of Argon et al. (1975) and Beremin (1981) are often used.
           The most widely referenced models for growth and coalescence of voids were published
           by  Rice and Tracey (1969) and Gurson (1977). Rice and Tracey considered a single
           void  in  an infinite solid with  a rigid-plastic and  a linear  strain hardening behaviour.
           Gurson analysed plastic flow in a porous medium assuming that the material behaves as
           a continuum and the effect of voids is averaged. The main difference between this model
           and  standard plasticity is that the yield surface in the Gurson model exhibits a weak
           hydrostatic stress dependence. Ductile fractures are assumed to occur as a result of  a
           plastic instability that produces a band of localised deformation. The Gurson model, and
           later improvements (Tvergaard and Needleman, 1984 for example), characterise plastic
           flow  quite well in the early stages of  the ductile fracture process, but  do not provide
           a good description of  the  events that lead to  final failure, because of  not  containing
           discrete voids.  These  shortcomings are  intended  to  be  surmounted by  the  model  of
           Thomason ( 1990), where holes are explicitly considered.
              Once  the  crack  is  nucleated,  crack  growth  can  be  modelled  using  the  above-
           mentioned models, or from a more macroscopic point of view by using the techniques
           of  elasto-plastic fracture mechanics (EPFM) (see, for example, Anderson,  1995, and
           Broberg,  1999). To  the authors’ knowledge, few results are available of  ductile fibre
           failure  based  on  EPFM,  most  probably  because  the  small  size  of  fibre  diameters
           invalidates some of the hypotheses on which this theory is based.
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