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Mechanical Behaviour of Plastics                               137

                 related to the stress intensity factor K by the following equation
                                             da
                                             -=  CIK"                        (2.1 14)
                                             dt
                 where C1  and rn  are material constants.
                   Now using equation (2.100) we may  write




                   If  the material contains defects of  size (hi) fai-dre occurs w...en  these
                                                          and
                 reach a size (h,) then the time to failure, tf, may  be obtained by integrating
                 the above equation.




                   Although equations (2.1 12), (2.1 13) and (2.1 15) can be useful they must not
                 be used indiscriminately. For example, they are seldom accurate at short times
                 but this is not a major wony since such short-time failures are usually not of
                 practical interest. At long times there can also be inaccurate due to the embrit-
                 tlement problem referred to earlier. In practice therefore it is generally advisable
                 to use the equations in combination with safety factors as recommended by the
                 appropriate National Standard.

                 2.20.2  Crazing in Plastics
                 When  a  tensile  stress is  applied to  an  amorphous (glassy) plastic,  such  as
                 polystyrene, crazes may be observed to occur before fracture. Crazes are like
                 cracks in the sense that they are wedge shaped and form perpendicular to the
                 applied stress. However, they  may  be  differentiated from cracks by  the fact
                 that they  contain polymeric material which  is stretched in  a highly oriented
                 manner perpendicular to the plane of the craze, i.e. parallel to the applied stress
                 direction. Another major distinguishing feature is that unlike cracks, they are
                 able  to  bear  stress. Under static loading, the  strain at  which  crazes  start to
                 form, decreases as the applied stress decreases. In constant strain rate testing
                 the crazes always start to form at a well defined stress level. Of course, as with
                 all aspects of  the behaviour of  plastics other factors such as temperature will
                 influence the levels of  stress and strain involved. Even a relatively low stress
                 may induce crazing after a period of time, although in some glassy plastics there
                 is a lower stress limit below which crazes will never occur. This is clearly an
                 important stress for design considerations. However, the presence of  certain
                 liquids (organic solvents) can initiate crazing at stresses far below this lower
                 stress limit. This phenomenon of  solvent crazing has been the cause of  many
                 service failures because it is usually impossible to foresee every environment
                 in which a plastic article will be used.
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