Page 77 - Fiber Fracture
P. 77

62                                                           J.W.S. Hearle
















               Fig. 4.  (a)  Light-degraded  nylon.  (b,c)  High-speed  break  of  nylon  from  pendulum  impact.  For  further
               explanation, see Fig. 1.


               increase in stress on the unbroken side causes additional plastic yielding and the crack
               opens into a V-notch, Fig. 3b. When this has grown to a critical size, catastrophic failure
               occurs over the remaining cross-section, Fig. 3c. Tests on polyester film marked with a
               grid show that the additional elongation represented by the open end of the V-notch is
               accommodated in the unbroken material by a band of shear, Fig. 3d, which would extend
              back by  many fibre diameters. Plastic deformation over a large volume of  the whole
              circular specimen is a challenge to the theoreticians of fracture mechanics.
                 There are variant forms. The initial flaw may be a small point, a line perpendicular
              to the fibre axis, or an angled line, and this changes the detail of  the break, Fig. 3e.
              Occasionally, breaks start from opposite sides of  the fibre, giving two V-notch zones
              and  a  central  catastrophic region.  Breaks  normally  start  from  the  fibre surface, but
              occasionally from an internal flaw, when the V-notch becomes a double cone, Fig. 3f.
              A variant on this form occurs in light-degraded nylon. Voids form round the delustrant,
              titanium dioxide particles, and multiple breaks start from these voids to give a turreted
              appearance, Fig. 4a.

              High-speed Breaks


                 As the rate of  extension is increased, the V-notch region gets smaller, Fig. 4b, and
              the catastrophic region gets larger. At ballistic rates, the change is  complete and the
              break appears as a mushroom, Fig. 4c. This is explained as being due to a change from
               isothermal to adiabatic conditions. Heat generated by the rapid plastic flow causes the
              material to melt, or at least soften. The elastic energy stored in the fibre remote from the
              break zone causes snap-back when break occurs. When snap-back stops, the softened
              material collapses into the mushroom cap.

              Granular Breaks

                 Cellulosic and acrylic fibres, which  are spun from solution, show granular breaks,
              which  are  similar to  lower-magnification views  of  the  structure of  a  fibre-reinforced
              composite, Fig. 5a,b. The reasons are similar. The fibres coagulate from solution with
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