Page 196 - Mechanics Analysis Composite Materials
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Chapter 4.  Mechanics of a composite layer      181

           matrix is relatively low, and the second circumstance arises - matrix material with
           low stiffness cannot provide the proper stress diffusion in the vicinity of damaged or
           broken fibers (see Section 3.2.3). As a result, the main material characteristic - its
           longitudinal  tensile  strength  - decreases.  Experimental  results  corresponding  to
           composites with resins 1, 2, 3, and 4 are presented in Fig. 4.50. Thus, significant rise
           in  transverse  elongation  is  accompanied  with  unacceptable  drop in  longitudinal
           strength (see also Chiao,  1979).
             One  of  the  possible  ways  for  synthesizing  composite  materials  with  high
           transverse  elongation  and  high  longitudinal  strength  is  to  combine  two  matrix
           materials  - one  with  high  stiffness to  bind  the  fibers  and  the  other  with  high
           elongation  to  provide  the  proper  transverse  deformability  (Vasiliev  and  Salov,
           1984). The  manufacturing  process  involves two-stage  impregnation.  At  the  first
           stage a fine tow is impregnated with  the high-stiffness epoxy resin (of the type  2
           in Fig.  4.48) and cured. The properties of thus fabricated composite fiber are as
           follows:














                                0'   " " " EZ,%
                                  0   0.2   0.4   0.6   0.8   1   1.2

           Fig. 4.49. Stress-strain curves for transverse tension of unidirectional fiberglass compositeswith different
                        epoxy matrices (numbers on the curves correspond to Fig. 4.48).


                                    F,,MPa
                                    1500

                                    1400

                                    1300

                                    1200

                                    I100
                                    I000
                                       0  2  0  4  0  6  0
           Fig. 4.50. Dependence of the longitudinal strength on the matrix ultimate elongation (numbers on  the
                                 curve correspond to Figs. 4.48 and 4.49).
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