Page 391 - Mechanics Analysis Composite Materials
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376                 Mechanics and analysis of composite materials

             Table 8.2
             Parameters of typical advanced composites.

             Parameter  Fabric-epoxy composites   Unidirectional-epoxy composites   Boron-AI
                      Glass   Carbon   Aramid   Glass   Carbon   Aramid   Boron
             -
             0~/8l    0.99   0.99    0.83    0.022   0.025   0.012   0.054   0.108
             n        0.85   1.0     1.O     0.28    0.I    0.072   0.11    0.7


             with Eqs. (8.32), this means that hl  -Kh2, and the ratio h2/h1 varies from  12.7 for
             glass-epoxy  to 2.04 for  boron+poxy  composites.  Now,  return  to  the discussion
             presented  in  section  4.4.2  from  which  it  follows  that  in  laminated  composites
             transverse stresses 02  reaching their ultimate value, &, cause cracks in the matrix
             which do not result in the failure of the laminate whose strength is controlled by
             fibers. To describe the laminate with cracks in the matrix (naturally, if the cracks are
             admitted for the structure under design), we can use the monotropic model of the
             ply and, hence, results of optimization presented in Section 8.1.
               Consider again the optimality condition Eq. (8.25). As can be seen, this equation
             can be satisfied not only by strains in Eqs. (8.26), but also if we take

                           Y.VJ
                 tan24i = -.                                                   (8.34)
                         Ex  - E,.
             Because the left-hand  side of  this equation  is a  periodic function  with  period  7c,
             Eq. (8.34) determines two angles, Le.


                                                                               (8.35)

             Thus, the optimal laminate consists of two layers, and the fibers in both layers are
             directed along the lines of principal stresses. Assume that the layers are made of the
             same composite material and have the same thickness, i.e. hl  = h2  = h/2, where h is
             the thickness of the laminate. Then, using Eqs. (8.24) and (8.35) we can show that
             BII= B22  and B24  = -BI~for this laminate. After some transformation  involving
             elimination  of  y.!,,.  from  the  first  two  equations  of  Eqs. (8.23)  with  the  aid  of
             Eq. (8.34) and similar transformation of the third equation from which  and E:  are
             eliminated using again Eq. (8.34) we get

                 Nx = (BII  + 814 tan 24)~:+ (B12 - 814tan %)E!,
                 N,,= (~12- B14tan 2414 + (BI  1 +B14 tan 24)~:~
                 Nx?; = (B44 f B14 cot 24)$,.  .

             Upon substitution  of coefficients B,,,  from Eqs. (8.24) we arrive at
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