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62                  Mechanics and analysis of composite materials


                dW  dS
                ->-                                                            (3.12)
                 dl   dl
             the crack will propagate,  and the fiber will fail. Substituting Eqs. (3.10) and (3.11)
             into inequality (3.12) we arrive at


                                                                               (3.13)

             The most important result that follows from this condition specifying some critical
             stress,  rrc,  beyond  which  the  fiber  with  a  crack  cannot exist  is  the  fact  that  aC
             depends on the absolute value of the crack length (not on the ratio Z/d).  But for a
             continuous fiber, 21 < d so, the thinner the fiber, the less is the length of the crack
             that can exist in this fiber and the higher  is the critical  stress,  ifc.  More rigorous
             analysis shows that reducing Z  to a in Fig. 3.8 we arrive at SC= ifl.
               Consider for example  glass fibers that  are widely used  as reinforcing  elements
             in  composite  materials  and  have  been  studied  experimentally  to  support  the
             fundamentals of Fracture Mechanics (Griffith, 1920). Theoretical  strength of glass,
             Eq. (3.8), is about 14 GPa, while the actual strength of  1 mm diameter glass fibers
             is  only  about  0.2 GPa, and  for  5 mm  diameter  fibers  this  value  is  much  lower
             (about  0.05 GPa).  The  fact  that  such  low  actual  strength  is  caused  by  surface
             cracks can be readily proved  if the fiber surface is smoothed  by  etching the fiber
             with  acid.  Then,  the  strength  of  5 mm  diameter  fibers  can  be  increased  up  to
             2 GPa.  If  the  fiber  diameter  is  reduced  with  heating  and  stretching  fibers to a
             diameter  about 0.0025 mm,  the  strength  rises  up  to 6 GPa. Theoretical  extrapo-
             lation of the experimental curve, showing dependence of the fiber strength on the
             fiber diameter for very small fiber diameters, yields  8 = 11 GPa, which is close to
             Cl  = 14 GPa.
               Thus,  we  arrive  at the  following  conclusion  clearing  out  the  nature  of  high
             performance of advanced composites and their place among the modern structural
             materials.
               Actual  strength  of  advanced  structural  materials  is  much  lower  than  their
             theoretical strength. This difference is caused by defects of  material microstructure
             (e.g.,  crystalline  structure)  or microcracks  inside the material  and  on its surface.
             Using thin fibers we reduce the influence of cracks and thus increase the strength of
             materials reinforced with these fibers. So, advanced composites comprise a special
             class  of  structural  materials  in  which  we  try  to  utilize  thc  natural  potential
             properties  of  the  material  rather  than  the  possibilities  of  technology  as  we  do
             developing high-strength  alloys.

             3.2.2.  Statistical aspects of Jiber strength

               Fiber strength, being relatively high, is still less than the corresponding theoretical
             strength which means that fibers of advanced composites have microcracks or other
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