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64                  30 Fibre Reinforced Polymer Composites

                 cannot be  used  to  analyse variations of  mechanical properties with  some important
                 architecture parameters due to the introduction of oversimplified assumptions. On the
                 other  hand,  it  is  almost  impractical to  investigate experimentally the  mechanical
                 properties  of  textile  composites  and  their  dependence  on  the  major  architecture
                 parameters because of their complexity in geometry and spatial organisation. Hence, it
                 is desirable to develop an analytical approach which  is capable of  modelling textile
                 composites  at  a  micro  geometry  level,  and  predicting  effectively  the  mechanical
                 properties and their dependence on major architecture parameters.
                    Finite element analysis (FEA)  is  a  useful  and  versatile  approach  used  by  many
                 researchers to predict mechanical properties of composite materials. A number of FEA
                 models  have  been  developed  to  evaluate  the  effects  of  various  fibre  architecture
                 parameters  on the mechanical properties of textile composites.
                    It is not intended to present or even review in this book all micromechanics methods
                 that have been used or may be potentially useful for characterising 3D fibre reinforced
                 composite materials.  Instead, this book aims to provide a brief description of selected
                 micromechanics modelling methods that have been proved to be useful for predicting
                 the in-plane mechanical properties of 3D composites.


                 4.2 FUNDAMENTALS IN MICROMECHANICS



                 4.2.1  Generalized Hooke’s Law
                 For  an elastic anisotropic material, the generalized Hooke’s law is  the linear stress-
                 strain relation as given by:
                       {d= [ck}                                                     (4.1)
                 where
                       io}=  {Oil   O22   O33   O23   O31   Ol2)7

                            kll  ‘22   ‘33   ‘23   ‘31   ‘I2)T
                             ‘1,   ‘12   ‘I3   ‘I4   ‘15   ‘16
                             ‘21   ‘22   ‘23   ‘24   ‘25   ‘26
                             ‘31   ‘32   ‘33   ‘34   ‘35   ‘36
                             ‘41   ‘42   ‘43   ‘44   ‘45   ‘46
                             ‘51   ‘52   ‘53   ‘54   ‘55   ‘56
                             ‘61   ‘62   ‘63   ‘64   ‘65   ‘66

                 where  oij and   are the stress and strain components, respectively, and  C, are the
                 elastic  stiffness  constants.  The  stiffness  matrix  is  symmetric  from  an  energy
                 consideration. There are 21 independent constants out of the 36 constants.  The above
                 equation can also be written in the form:


                                                                                    (4.3)
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