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48                          E LABESSE-JIED  ET AL.




                                            Ta(t)=Z(t)-?                          (7)

                The damage associated with each cycle is calculated by using Miner’s linear rule and the
             material fatigue strength curve expressed in the form of Basquin’s law [7].









                The lifetime is calculated by maximising the damage over all the examined planes. In other
             words, it means that the critical plane enforces its fatigue life to the material.










              EVALUATION OF THE METHOD ON SPECIMENS
              The local approach is assessed on cylindrical and tubular shaft specimens from experiments
              reported in the round-robin program performed by the  SAE in the  80’s  181.  The  shafts are
              submitted to proportional  or  non-proportional strain-controlled tension  and  torsion  loading.
              The strain amplitudes are constant or variable. The random spectra come fi-om measurements
              made on log skidder and agriculture tractor axles and recorded as Markov matrix. Fatigue tests
              are pedormed on shaft  specimens with  different  deterministic  or  random  amplitudes until
              complete fracture. Calculations are carried out according to the local approach flowchart (Fig.
              4). Starting from the deterministic or random strain cycles, the stress states are calculated by
              using a cyclic constitutive law with non-linear kinematical and isotropic hardening. Then, the
              damage  corresponding  to  the  cycles  extracted  by  the  rainflow  method  is  calculated  and
              cumulated. The life corresponding to each strain sequence is then calculated by using the most
              damaged facet.
                The  shafl  is  made  up  of  C45 carbon  steel.  The  mechanical  properties  of  this  steel  are
              summarised in Table 1.


              Table 1. Monotonic and cyclic properties of C45 carbon steel (from [SI)

              OY      K       n       cf7Y    K’      n’      cf’f    Z’f     b
              (MPa)   (M Pa)          (MPa)   (MPa)           (MPa)   (MPa)
              280     1185    0.23    180     1258    0.208   948     505     - 0.092


                Figure 6 gives the comparison between the experiments and calculated lives for all kinds of
              loading: deterministic uniaxial tension, proportional tension-torsion, non proportional tension-
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