Page 140 - Engineered Interfaces in Fiber Reinforced Composites
P. 140

Chapter 4.  Micromechanics of  stress transfer   123

                             -1
                              E
                              E
                             Y
                             -I
                             Eu
                             s
                              rn
                              C
                              a  -            Increasing On = 6,8,10 GPa
                              C  :{I I I #
                             c
                              E
                              P
                             t
    :                        n   * n
                              t
                             LL
                                 "0     I  0.02  '   0.04   '   0.k   0
                                             Applied strain E
                Fig. 4.18. Variation of mean fiber fragment length, 2L, as a function of applied strain, E, predicted in the
                fully  debonded  interface  model  for  constant  fiber  tensile  strengths  CTTS = 6.0,  8  and  10 GPa.  After
                                             Kim et al. (1993b).



                results in a high applied strain required to initiate the fiber fragmentation. However,
                varying the constant fiber tensile strength does not much influence (2L) at a high
                applied strain.

                4.2.4.4. Comparisons with earlier shear-lag models
                  A  major  improvement  of  the models presented  in  this  section compared  to  the
                earlier models given in  Section 4.2.2 is  that the conditions required  to  satisfy the
                three  different  interfaces,  i.e.  full  bonding,  partial  debonding  and  full  frictional
                bonding, are systematically identified. This gives an idea how the interface condition
                changes with increasing load during the whole course of the fiber fragmentation test.
                It  is  also  shown  that  depending  on  the  relative  properties  at  the  bonded  and
                debonded interfaces, the IFSS at the debonded region increases from the boundary
                of  the  two  regions  toward  the  fiber  ends  as  a  consequence  of  the  differential
                contraction  between  the  fiber  and  matrix.  This  effectively  discourages  debond
                propagation during the fiber fragmentation  process. This response makes  it  most
                unlikely that the interface becomes debonded along the whole fiber length even at a
                very high applied strain in most practical polymer matrix composites.
                  Nevertheless,  there  are also  important  issues which  remain  unresolved  in  this
                model.  Apart  from the  three  different interface  states  discussed above,  there  are
                other  states  of  the  interface  due  to  yielding  of  matrix  material  immediately
                surrounding  the  cylindrical  fiber, and the  combination  of  partial  debonding  and
                partial yielding. Plastic yielding occurs in the matrix instead of interface debonding
                if  the interface  shear bond  strength,  Tb,  is sufficiently higher than the matrix yield
                strength  in  shear,  z,,,   as  in  some  composites  containing  ductile  thermosets/
                thermoplastics and metal matrices. To be able to model this behavior  analytically
                the exact knowledge regarding the effective thickness of the interphase region being
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