Page 123 - Plastics Engineering
P. 123

106                                  Mechanical Behaviour of Plastics

                        equation (2.63) permits the problem of  intermittent loading to be analysed in
                        a  relatively  straightforward manner  thus  avoiding uneconomical overdesign
                        which would result if the recovery during the rest periods was ignored.
                          From  equation (2.63)  and  the  definition  of  Fractional  Recovery,  F,,  the
                        residual strain is given by
                                         &r(t) = &c(T) - Fr  *  &c(T)




                          If there have been N cycles of creep and recovery the accumulated residual
                        strain would be
                                                  x=N
                                      &,(t) = EC(T)   [ (F) ?I - ( y - 1) '1
                                                  x=l
                        where  tp is  the  period  of  each cycle and  thus  the  time  for  which the  total
                        accumulated strain is being calculated is t = t,N.
                          Note also that the total accumulated strain after the load application for the
                        (N + 1)th time will be the creep strain for the load-on period ie cC(T) plus the
                        residual strain s,(t).

                                                                  -
                        ie       (&N+l)max  = &c(T) { 1 + x=N  [(F)" (y - l)n]}      (2.65)
                                                      x=  I
                          Tests have shown that when total strain is plotted against the logarithm of
                        the total creep time (ie NT or total experimental time minus the recovery time)
                        there is a linear relationship. This straight line includes the strain at the end of
                        the first creep period and thus one calculation, for say the  10th cycle allows
                        the line to be drawn. The total creep strain under intermittent loading can then
                        be estimated for any combinations of  loading/unloading times.
                          In  many  design calculations it is necessary to have the  creep modulus in
                        order to estimate deflections etc from standard formulae. In the steady loading
                        situation this  is  straightforward and  the  method  is  illustrated in  the Exam-
                        ples (2.1)-(2.5).  For the intermittent loading case the modulus of the material
                        is effectively increased due to the apparent stiffening of  the material caused
                        by  the recovery during the rest periods. For example, if  a constant stress of
                        17.5 MN/m2 was applied to acetal (see Fig. 2.51) for 9600 hours then the total
                        creep strain after this time would be 2%. This would give a 2% secant modulus
                        of  17.5/0.02 = 875 MN/m2. If, however, this stress was applied intermittently
                        for 6 hours on and  18 hours off, then the total creep strain after 400 cycles
                        (equivalent to a total time of 9600 hours) would only be  1.4%. This would be
                        equivalent to a stress of  13 MN/m2 being applied continuously for 9600 hours
                        and so the effective creep modulus would be 13/0.014 = 929 MN/m2.
   118   119   120   121   122   123   124   125   126   127   128