Page 249 - Plastics Engineering
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232                               Mechanical Behaviour of Composites

                        is complex. However, the  stiffness of  such systems may  be predicted quite
                        accurately using the following simple empirical relationship.

                                              Emdom  = 3E1/8 + 5E2/8                 (3.50)
                          Hull also proposed that the shear modulus and Poisson’s Ratio for a random
                        short fibre composite could be approximated by

                                                Gmdm = gEi 4-  $E2                   (3.51)
                                                         I
                                                             -
                                                Vmdom = - 1                          (3.52)
                                                         2Gr
                          El  and E2  refer to the longitudinal and transverse moduli for aligned fibre
                        composites of  the type shown in (Fig. 3.29). These values can be determined
                        experimentally or using specifically formulated empirical equations. However,
                        if  the fibres are relatively long then  equation (3.5) and (3.13) may  be  used.
                        These give results which are sufficiently accurate for most practical purposes.

                        3.15  Creep Behaviour of Fibre Reinforced Plastics

                        The viscoelastic nature of  the matrix in many fibre reinforced plastics causes
                        their properties to be time and temperature dependent. Under a constant stress
                        they exhibit creep which will be more pronounced as the temperature increases.
                        However, since fibres exhibit negligible creep, the time dependence of the prop-
                        erties of fibre reinforced plastics is very much less than that for the unreinforced
                        matrix.


                        3.16 Strength of Fibre Composites
                        Up to this stage we have considered the deformation behaviour of fibre compos-
                        ites. An equally important topic for the designer is avoidance of failure. If  the
                        definition of  ‘failure’ is  the  attainment of  a  specified deformation then  the
                        earlier analysis may  be used. However, if the Occurrence of  yield or fracture
                        is to be predicted as an  extra safeguard then  it  is necessary to use  another
                        approach.
                          In  an isotropic material subjected to a uniaxial stress, failure of  the latter
                        type is straightforward to predict. The tensile strength of the material 6~ will
                        be known from materials data sheets and it is simply a question of  ensuring
                        that the applied uniaxial stress does not exceed this.
                          If an isotropic material is subjected to multi-axial stresses then the situation is
                        slightly more complex but there are well established procedures for predicting
                        failure. If  a,  and ay are applied it is not simply a question of  ensuring that
                        neither of  these exceed 8~. At  values of  a,  and  ay below 3~ there  can be
                        a plane within the material where the  stress reaches 6~ and this will initiate
                        failure.
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