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406                c! AUBIN, R QUXEGEBEUR AND S. DEGAUALY


                               700
                               650
                               600
                               550
                               500
                                                 -Monotonic   tension
                               450
                                                  + Tensioncompression
                               400
                               350                +  Torsion
                               300                0  Proportiona145°


                                  0    0.002   0.004   0.006   0.008


             Fig. 5. Cyclic stress-strain responses at the stabilized or quasi-stabilized cycles for proportional
             loading paths.




             Cyclic hardening-softening behaviour under non-proportional loading
             A series of tests using four non-proportional loading paths were performed (see Fig, 3). An
                                                                                 y')
             example  of  the  response  obtained in  the  different planes,  (CJ, & 7) , (E',  y'/&),   ' (7,  ,
             (a,&'),  is given in  Fig.  6  for  the  hourglass path.  At  each cycle, the  radii  and  the  centre
             positions of the smallest circles circumscribed around the responses in the plane (c, & 7) and
                       (  4
             in the plane  E',  y'  &  are calculated. These radii are called equivalent stress amplitude and

             equivalent plastic strain amplitude respectively.
               Cyclic hardening-softening curves at a strain amplitude of 0.5 % for the seven loading paths
             tested, proportional and non-proportional, are given in Fig. 7. Whatever the loading path, the
             cycling leads to quasi-stabilization after a phase of hardening followed by a low softening.
             Figure 8 shows the cyclic stress-strain responses in terms of equivalent stress amplitude versus
             equivalent plastic strain amplitude at the stabilized cycles. At a same strain amplitude, for non-
             proportional loading paths, the duplex stainless steel hardens much more than for proportional
             paths.  This cyclic hardening, called extra-hardening, depends on the strain amplitude and on
             the loading path. For a circle path, at the strain amplitude 0.2 %,  there is no extra-hardening,
             because  the plastic strain is  about zero. On  the contrary, at the strain amplitude 0.5 %,  the
             stabilized stress is 20 % higher (or 120 MPa higher) than the one for the proportional path. In
             comparison, on an austenitic stainless steel type AIS1 316L at the same strain amplitude, the
             circle path induces an extra-hardening of 70 % (or 225 MPa) [lo-141. The hardening effect due
             to loading path, in absolute and in relative values, is lower for duplex stainless steel than for
              austenitic stainless steel. For the duplex stainless steel, three groups can be defined among the
             tested loading paths according to the increasing degree of hardening: (i) tension-compression,
              torsion and proportional 45'  paths; (ii) clover path, (iii) circle, square and hourglass paths.
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