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128                                   Mechanical Behaviour of  Plastics

                                   Normal stnsro
                                    f   t    t










                                                       hriation of uy
                                                       along x axis (O=O)









                              Fig. 2.66  Stress distribution in vicinity of a crack


               defined as
                                          K  = o(Ru)'/~
                 The stress  intensity factor is a  means of  charactensing the  elastic  stress
               distribution near the crack tip but in itself has no physical reality. It has units
               of MN m-3/2 and should not be confused with the elastic stress concentration
               factor (K,) referred to earlier.
                 In order to extend the applicability of LEFM beyond the case of  a central
               crack in an infinite plate, K is usually expressed in the more general form

                                         K  = Yo(Ru)'/~                    (2. loo)

               where Y is a geometry factor and  'u'  is the half length of  a central crack or
               the full length of  an edge crack.
                 Fig. 2.67 shows some crack configurations of  practical interest and expres-
               sions for K are as follows.
               (a) Central crack of  length 2u  in a sheet of  finite width


                                                                           (2.101)

               (b) Edge cracks in a plate of  finite width


                                                                           (2.102)
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