Page 148 - Fiber Fracture
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STRENGTH OF GLASS FIBERS                                             133

             smaller-diameter E-glass fibers (5-20  pm), testing in pure tension is the only method
             available at present for measuring intrinsic strengths.
                It  should be  pointed  out  that  the  intrinsic  strength of  a  glass  is  not  a  constant.
             The  intrinsic  strength  values  for  a  given  composition  vary  with  testing  conditions
             (environmental humidity, and temperature).

             Extrinsic Strength, S

                Flaw-controlled strengths are called extrinsic. The strengths of non-pristine fibers are
             extrinsic by definition. Extrinsic strengths show larger COV than can be accounted for
             from fiber diameter variations alone. The additional variation in strength arises from the
             variation in the severity of the most severe flaws in different samples. Gupta (I 987) has
             carried out a detailed analysis of the measured strength distributions by combining the
             variations in fiber diameter and in the flaw-severity statistics.

             Inert Strength, SO

                Strength measured in the absence of fatigue is called the inert strength. Inert strength
             should not be confused with intrinsic strength. Inert refers to absence of fatigue while
             intrinsic refers to absence of flaws. In this paper, the inert strength is denoted by SO.
               In  principle,  inert  strength  can  be  measured  by  using  testing  conditions  which
             minimize fatigue (such as dry environment or vacuum and sufficiently large strain rates
             so that the fatigue reaction does not have time to progress). All these approaches have
             been attempted with varying degrees of success. However, inert strengths are measured
             most conveniently by testing at the liquid Nz temperature (77 K) where the rate of the
             fatigue reaction is sufficiently small to be considered negligible. Several experiments
             have demonstrated that the measured strength at room temperature under conditions of
             high vacuum approaches the measured strength at the liquid nitrogen (LN) temperatures
             (France et al., 1980; Roach, 1986; Smith and Michalske, 1989). In other words, there is
             no significant temperature dependence of the inert strength. The temperature dependence
             from other intrinsic properties such as E is negligible. It follows, therefore, that

                So  = SLN                                                         (4)
             where SLN is the strength measured at the liquid Nz temperature.

             Theoretical Strength, sfh

               The strengths of pristine fibers at the liquid nitrogen temperature, StN, are the highest
             strength values measured for a given composition. One might expect StN in the absence
             of flaws to be equal to the theoretical strength, S,,  of a glass:
                s&I = sa                                                          (5)
             Unfortunately, at present, theoretical estimates of  S,h  do not exist for multicomponent
             compositions (such as E-glass) and  are not  reliable even for  simple one-component
             glasses. For example, estimates of the theoretical strength of silica based on cohesive
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