Page 445 - Aircraft Stuctures for Engineering Student
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426  Stress analysis of aircraft components

                  corresponding to a1 is given by
                                                      A1
                                                  E1  = -                           (10.44)
                                                       I
                  and
                                                    = El&]                          (10.45)

                  where El is the modulus of elasticity of the lamina in the direction of the flament.
                  Also, using the suffixes f and m to designate filament and matrix parameters, we
                  have
                                            af = EfEl,   0,  = E,E~                 (10.46)
                  Further, if A is the total area of cross-section of the lamina in Fig. 10.66, Af is the
                  cross-sectional area of  the filament and A,  the cross-sectional area of  the matrix
                  then, for equilibrium in the direction of the filament
                                             o1A = UfAf + amA,
                  or, substituting for q, af and a,  from Eqs (10.45) and (10.46)
                                           E~E~A EfEfAf + Em€lAm
                                                =
                  so that
                                                                                    (10.47)

                  Writing Af/A  = vf and A,/A  = v,,  Eq. (10.47) becomes
                                              El  = VfEf + VmEm                     (10.48)

                  Equation (10.48) is generally referred to as the law of mixtures.
                    A  similar approach may be  used  to determine the modulus of  elasticity in the
                  transverse direction (Et). In Fig. 10.67 the total extension in the transverse direction
                  is produced by q and is given by
                                               Etlt = Em&  + Eflf




                                         t  t  fUit  t  t
















                  Fig. 10.67  Determination of Et.
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