Page 111 - Engineered Interfaces in Fiber Reinforced Composites
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94                Engineered interfaces in fiber reinforced composites

                    that the load-bearing capability of  a composite depends on the efficiency of stress
                    transfer, which is largely controlled by the nature of bonding at the interface region,
                    in addition to the mechanical properties of the fiber and matrix.
                      Theoretical analysis of  interfacial debonding has  received  significant attention
                    especially for the fiber pull-out test. The condition of interface debonding has been
                    defined by  two distinct approaches: the shear strength criterion and the fracture
                    mechanics approach. In the shear strength criterion, when the interface shear stress
                    (IFSS)  reaches  the  interface shear  bond  strength,  Zb, debonding  occurs.  In  the
                    fracture mechanics approach, extension of a  debond crack requires the potential
                    energy  release  rate  of  the  composite constituents  to  reach  a  critical value,  the
                    interface fracture toughness, Gi,. In these two debond criteria, both  Zb  and Gi,  are
                    assumed  to  be  material  constants,  the  characteristic interface  properties  to  be
                    determined in experiments.
                      Recognizing the  significance of  stress concentration  at  the  fiber  broken  ends,
                    many  researchers have  inclined  to  employ  numerical  methods,  particularly  FE
                    analysis where  the  effects  of  specific end  geometry  as  well  as  different  matrix
                    behavior at the interface region can be properly evaluated. The use of FE method
                    allows a more accurate description of the interactions between neighboring fibers
                    and the IFSS fields near the singularity as demonstrated in the fiber fragmentation
                    test (MacLaughlin and Barker, 1972; Termonia, 1987, 1992; Fan and Hsu, 1992a, b;
                    Daabin et al., 1992; Daoust et al., 1993; Ho and Drzal, 1995a, b), the fiber pull-out
                    test (Atkinson et al., 1982; Wu and Claypool, 1991; Marotzke,  1993, 1994; Povirk
                    and Needleman, 1993; Kim et al., 1994a, b) and microindentation test (Grande et al.,
                    1988; Tsai, 1990; Kallas et al.,  1992; Mital et al.,  1993; Meda et al.,  1993; Ho and
                    Drzal,  1996). The stress recovery around the fiber ends after fiber breaks is also
                    taken into account (Curtin,  1991) to describe the fragmentation distribution as a
                    function of the fiber’s underlying statistical strength and the interface bond strength.
                      In this chapter, the roles of the interface are discussed with regard to the efficiency
                    of stress transfer in various loading geometry of the three most popular single fiber
                    microcomposite tests, namely the fiber fragmentation test, the fiber pull-out test and
                    the  fiber  push-out  test.  Among  many  different failure mechanisms that  may  be
                    operative  at  the  interface  region,  universally  considered  in  this  chapter  as  a
                    predominant failure mode is the debonding along the fiber-matrix  interface. Except
                    for the fiber fragmentation test, only the fracture mechanics approach is employed
                    to define the debond process. Much of the discussion here is based on the theoretical
                    consideration of the micromechanics analysis using a shear lag model of the single
                    fiber composite and other models extended therefrom.



                    4.2.  Fiber fragmentation test

                    4.2.1. Introduction
                      Cox (1952) first considered a shear-lag model where an elastic fiber is embedded in
                    an elastic matrix which is subjected to uniaxial tension. Perfect bonding is assumed
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