Page 141 - Biaxial Multiaxial Fatigue and Fracture
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126                     R.€? KAUFMAN AND T.H.  TOPPER

















                                                  ‘Alternating
                                      Periodic Overload

             Fig.  1.  Schematic of  crack face interference free conditions. The magnitude of  the periodic
             overload stress is significantly larger than the clamping force stress (spring force stress).

              the  portion  of  the  alternating shearing stress acting  on  the  crack  tips  is  dependent on  the
              magnitude of the Mode 1 periodic overloads and the spring force of the material.
                Fig.  I  shows that  the  application of  a  large enough periodic  Mode I  overload causes an
              interference free condition to result.  The magnitude of the periodic overload affects the amount
              of  the  total  shearing force  acting  at  the  crack tips.  Large  periodic compressive overloads
              compress  the  asperities in  the  crack  wake,  thereby  reducing  crack  closure/interference and
              increase the crack growth rate.  Large periodic tensile overloads (yield point magnitude) leave
              shear cracks fully  open.  Once closure free crack growth  is  achieved, further increasing the
              magnitude of the tensile or compressive applied periodic overload (Mode I) does not decrease
              the fatigue life or increase the crack growth rate.
                Data from  a  test  machine that  uses  internal and external pressure and  axial loading on  a
              tubular specimen to produce a wide range of static compressive and tensile mean stresses normal
              to the maximum alternating shear stress planes is presented in the following.  It is expected that
              tensile mean  stresses normal to one or both maximum shear planes will decrease the frictional
              force or surface interference on the shear plane which will result in a decrease in the fatigue life
              for a given applied alternating shear stress range.  Once the normal static tensile mean stresses
              (Si,,  ) are sufficiently large to fully separate the crack faces, the fatigue life will remain constant
              for larger tensile static mean  stresses (ostaue M~~~). The proposed model  of  the effect of  static
              mean stresses together with alternating shear stress for a given fatigue life is illustrated in Fig. 2.


              Material
              The material used during this program of study was SAE 1045 steel with two Brinell hardness
              numbers (BHN 456 and 203).  The first hardness level, BHN 456, was chosen because its ratio of
              yield strength to fracture strength is high,  and  the onset of ratcheting in load control  is delayed
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