Page 223 - Fiber Fracture
P. 223

208                                                           H.U.  Riinzi

                       7




                     t3

                     -

                     v1
                     Y
                     -
                     0
                     Z-1



                       -5

                                           lO'OOO/T   [ K']
                Fig. 24. Arrhenius plot for 50 prn diameter Au wires of  4N purity. The 4 lines  correspond to  normalized
                yield stress values  R of  0.08,0.48, 0.77 and 0.86.

                  In  most thermally activated relaxation and  diffusion processes, the evolution pro-
                gresses with time expressed in units of a characteristic temperature-dependent time that
                elapsed since the beginning of the process. If  we apply this argument to the evolution
                of  the  yield  stress and  assume the  temperature dependence to  follow an  Arrhenius
                law,  we  can  express  the  actual  annealing  time  t  at  temperature  T  by  an  effective
                temperature-compensated annealing time 0


                Here Q is an effective activation energy which is to be determined from the slope of the
                Arrhenius plot
                  In(t)  vs  1/T

                for a given yield stress. For convenience, the yield stress is given in normalized units

                   R = (R0.2 - R,)/(Ro  - Rea)
                where Ro  and R,  are the yield stresses at the beginning and after very long annealing
                times. Fig. 24  shows the Arrhenius plot for 50  km diameter Au  wires of  4N punty.
                The four lines correspond to normalized yield stress values R  of 0.08, 0.48, 0.77  and
                0.86. They give an effective activation energy of  1.16 & 0.10 eV which is roughly in
                between the activation energies for auto-diffusion (1.8 eV) and for vacancy migration
                (0.84 eV). A value below the activation energy of auto-diffusion is to be expected, since
                strong modifications of  the yield stress already occur during restoration. Here vacancy
                migration is important and optical micrographs are thus not visibly changed.
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