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The chemistry, manufacture, and tensile behavior of polyamide fibers  413

           12.6   Failure mechanisms in polyamide fibers


           The ambition of the field of fracture mechanics is to provide an understanding of how
           flaws ultimately govern the behavior of materials. The theoretical cohesive stress of a
           material is derived by determining the amount of force required to separate individual
           atoms for a prescribed interatomic separation distance (Anderson, 1995). Since the
           cohesive stress indicates the value at which atoms separate, it is an adequate measure
           of the theoretical strength limitation for a given material. Termonia and Smith
           (Dismore and Statton, 1966) have developed a Monte-Carlo approach to assess the
           theoretical tensile behavior of polymeric fibers, in which they quantified the effects
           of inhomogeneities among atoms on ultimate tensile strength.
              Lim et al. (1989) confirmed that the theoretical strength of a polyamide fiber is
           based on the force between the carbon-carbon bonds and the molecular cross-
           sectional area. For PA 66 and PA 6 fibers, the theoretical strength is 28.3 GPa (Lim
           et al., 1989; Tobolsky and Mark, 1971).
              In polymer systems, the processes of plasticity and fracture are normally indepen-
           dent (Anderson, 1995; Dowling, 1999). Nevertheless, molecular weight and molecular
           structure are the main determinants in the rupture behavior of polymer systems. Becht
           et al. (1971) considered that fracture in polyamide fibers from an atomistic viewpoint
           occurs mainly by chain scission. They determined that the deformation occurs mainly
           in the amorphous regions of the polymer, and normally results in free radical produc-
           tion that is detectable by electron spin resonance. Ward and Hadley (1993) assumed
           that there exist crystalline bridges that connect adjacent crystalline blocks and are a
           key factor in determining the axial stiffness of a semicrystalline polymer. Chain frac-
           ture in oriented polymers was examined using electron paramagnetic resonance to
           detect the free radicals produced. Infrared spectroscopy is another method commonly
           used in the analysis of polymer fracture. This method seeks to identify aldehyde end
           groups in polymers, which suggests chain scission. Kausch (Ward and Hadley, 1993;
           Kausch, 1987) has investigated such studies and provided a synopsis of the results.
           These findings are concomitant with flaw theory (Andrews, 1968) in polymers, which
           expresses that stress concentrations at the crack tip produce dilatation, which aids in
           the production of corrosive molecules. Additionally, Bershtein et al (Warwicker,
           1971) confirmed from an extensive investigational procedure on thin polyamide sam-
           ples that molecular weight and structure can be altered under a combination of stress
           conditions.
              All of these studies are good from a molecular perspective, but are inadequate for
           solving real-world fracture mechanics problems.
              Analogous to the results for yield phenomena in PA 66 fibers, the fracture perfor-
           mance is affected by hydrostatic pressure, to a great extent. Kausch et al. (1973)
           concluded that in PA 66, the fracture stress increases with pressure. This conjecture
           is based on concepts in simple mechanics theory, in which the hydrostatic pressure in-
           vokes a state of dilatation due to changes in volume of the sample. The direction of the
           propagation path in polyamide fibers can be described as meandering and random in
           nature, as compared to other structural materials (see Fig. 12.38). The path is strictly
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