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Variabili@ in Fatigue Lives: An Effect of the Elastic Anisotropy of Grains?   33 1


         are  not  centred  on  their  mean  value.  Low  values  of  the  maximum  Schmid  factor  are  not
         excluded, but their probability is very small. The mean value of the Schmid factor is found to
         be  high (<SF>=0.462). Therefore, in  grains for which the Schmid factor is at  its maximum
         (SF=0.5), the Schmid factor is only 8% higher than the mean Schmid factor in the polycrystal.
            In copper, for a given crystalline orientation of the grain, the maximum principal stress can
         be higher by 35 YO than the mean value in the polycrystal, according to the configuration of its
         neighbours. In comparison, for a given stress state in the grain, the resolved shear stress can be
         higher  by  only  8  %  than  the  mean  value  in  the  polycrystal, according  to  the  crystalline
         orientation of the grain. Therefore, in iron and copper, the load percolation network should be
         dominant,  in  the  crack  nucleation  process,  as  compared  with  the  effect  of  the  crystalline
         orientation of the grains. In  aluminium, the two effects appear to be of the same magnitude
         (Table 2).
            In  order to check this assumption the following calculations have been performed. In each
         point of the model (Fig. 9), the maximum resolved shear stress over the twelve slip systems of
         the FCC crystal was calculated as follows, using the stress tensor obtained from the FEM:











                           Aluminium         Copper
                             30              A 40                 37 5
                             31 4                                  47
                             32 8                                 56 5
                             34 3                                  66
                             35 7               64                 75 5
                             37 1               70                 85







         Fig.  9.  (a) Schmid factor intensity maps for copper and aluminium; (b,c) Maximum resolved
         shear stress intensity maps (MPa), over the twelve (1 11)4 10> slip systems of the FCC crystai
         (b) in aluminium, (c) in copper; (d) Half Tresca equivalent stress in copper. The thin sheet is
         subjected to a uniaxial extension E+O.   1 %.


            The  sample is  subjected to a uniaxial extension. If  the material is  isotropic in  its elastic
         domain, T,,,  is equal to the Schmid factor. When the anisotropy of the crystal increases, the
         stress heterogeneity increases within the polycrystal and modifies the value of T,,,.  In order to
         visualize which effect is dominant on the distribution of z,,,   in the polycrystal, the maps for
         zmax are plotted out and compared with the intensity maps of the Schmid factor and with the
         Tresca equivalent stress (divided by a factor of 2), which measures the maximum shear stress.
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