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Mechanical Behaviour of  Plastics                               51

                  A
                  -
              10000
                  -
              lo00
                  -
               100
                  -
                10

                 1-
                  -
               0.1
               0.01 '

                                                         Log (time)   b
                   Fig. 2.9  Typical variation of creep or relaxation moduli with time

           18
           14

           20
           16                   C.C
          ?                      \
          d  l2
           03
           OL








                     Fig. 2.10  Construction of isometric and isochronous graphs

           The creep modulus will vary with time, i.e. decrease as time increases, in a
        manner similar to that shown for the relaxation modulus. The classical variation
        of these moduli is illustrated in Fig. 2.9. On log-log  scales it is observed that
        there is a high  value of  creep or relaxation modulus at  short times. This is
        referred to as the Unrelaxed Modulus and is independent of time. Similarly at
        long times there is a low  value Relaxed Modulus  which is also independent
        of time.
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