Page 283 - Engineered Interfaces in Fiber Reinforced Composites
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?21  ;;=:  /
                   264                Engineered interfaces in $ber reinforced composites


                                 I \              C3        *  k1= 0.2
                                                    I-

                                                    -I
                                                            x  h1=  2.0













                                                                /- /I






                                 -I   4.8   0.6   0.4   0.2   0   0.2   0.4   0.6   0.8   I
                                                       a
                    Fig. 6.20. Ratio of the strain energy release rates, GL/GT, plotted as a function of the material parameter,
                                a, for a doubly deflected interface crack. After Gupta et at. (1993).
                    6.4.2.2.  Maximum stress criterion
                      A  criterion  has  been  developed  based  on  the  tensile  normal  stress  and  the
                    anisotropic  tensile strength  on arbitrary  planes  about the crack tip.  It is assumed
                    that the crack grows along the plane on which the stress ratio is maximum (Buczck
                    and Herakovich,  1985). A maximum stress criterion is also proposed (Gupta et al.,
                    1993) for a crack which deflects along the interface
                                                                                      (6.27)

                    where  0; and  0; are  the  interface  (longitudinal  splitting)  and  fiber  (transverse
                    fracture) strengths, and ~~(0') and oU(9O0) are the stresses at the interface and in
                    the fiber, respectively, as determined by the method of singularity integral equations
                    (Erdogan,  1972). Taking  into account  the  elastic  anisotropy, Gupta et  al. (1993)
                    introduced  the  anisotropy  parameters  1 and  p  which  depend  on  the  elastic
                    compliances Sij as follows:
                                                                                      (6.28)

                                                                                      (6.29)
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