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The Background of Fatigue Limit Ratio of Torsional Fatigue to Rotating Bending Fatigue in ...   295

                                f  Axial direction
                    50
                 x
                  r-  40
                 .-
                  c
                  2  30
                  .I-
                  u)
                  L
                  8  20
                 c
                  u)
                  3 10
                  r
                     0
                        12345678910                     12345678910
                          Axial line number n             Axial line number n
                             (a) S45C                        (b) SC450
                            Fig.9. Local strains in torsional test ( 7  = 18%)


           applied macroscopic strain is 18%. The variation of local strains in torsion is larger than that in
           tension. In S45C steel, local strains are unevenly distributed. That is, most of  them on each
           axial grid line have a  tendency to be distributed only  above andlor below  the average line.
           When the axial grid line exists on the pearlite band, which is harder than ferrite, most of local
           strains on the line are distributed below the average line, and when the axial grid line exists on
           the ferrite band, most of  local strains on the line are distributed above the average line. This
           means that the strain concentrates within the ferrite in S45C steel which has a clear banded
           structure.


           Local deformation and crack initiation in torsional fatigue of  carbon steel with clear-banded
           structure
           Cracks initiated near grain boundaries.  Figure 10 shows the changes of surface state in the
           torsional  fatigue test of  S45C steel. This is an  example of  the  crack initiated near a  grain
           boundary. Figure 1O(a) shows optical micrographs (X 200). In the early stage of stress cycling
           (-0.01Nf  ,Nf: fatigue life),  the long and  narrow shadow, which will  later become a crack,
           already  appears  near the  grain  boundary.  Its  darkness  increases with  increasing number of
           cycles N without increase in its size, and it develops later into a long crack. As is stated above,
           this fatigue process can be divided into two stages, crack initiation and crack propagation.
             Figure lo@) shows the same region observed by scanning electron microscopy. At first, the
           region of the ferrite crystal grain which later becomes a crack (the long and narrow region that
           is white in color) slips. Then the width of the slip band and the extent of disruption increase
           with increasing N. Due to the large deformation on one side of the line, shown by the arrow in
           the figure, the deformation by slip is quite large in spite of high-cycle fatigue. Judging from the
           deformation, it seems that the region becomes more active due to work softening after work
           hardening by slip. On  the other hand, the region near the pearlite side is scarcely deformed.
           Therefore, because of the compensation of deformation, large strains are concentrated near the
           grain boundary between pearlite and ferrite. Consequently, the cracks apparently appear near
           the grain boundary.
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