Page 486 - Biaxial Multiaxial Fatigue and Fracture
P. 486

470                          J.L.7: SANTOS ET AL.


           Approaches for Evaluating Shear Stress Amplitude under Multiaxial Loading
           The definition of the square root of the second invariant of the stress deviator is:

                               1
                         &&{(rXx -6,,)2 +(e,, -crr)2 +(6, -6,)* +6(c,,'   +err2] (9)

           One direct way to calculate the amplitude of   is:







           Eq.(lO)  is  applicable  for  proportional  loading,  where  all  the  stress  components  vary
           proportionally. However, when the stress components vary  non-proportionally (for example,
           with  phase  shift between the  stress components), Eq.(lO)  gives the same result with that of
           proportional loading condition. In fact, the non-proportionality has influence on the shear stress
           amplitude generated by multiaxial loading. Therefore, a new methodology is needed.
              The  longest  chord  approach  is  one  of  the  well-known  approaches  as  summarized  by
           Papadopoulos in  [16], which defines the shear stress amplitude as half of the longest chord of
           the loading path, denoted as D/2. Based on the longest chord approach, an improvement was
           proposed to provide a detailed characterization of the loading path by Deperrois et al in [ 171.
              For combined bending and torsion fatigue problem, the application of Deperrois approach
           can be described as: firstly find the maximum chord of the loading path curve, denoted as 4,
           and then project the loading path curve onto the line perpendicular to D2. This projection is a
           line segment with the length equal to DI. The shear stress amplitude is defined as !-,/=.
                                                                          2
           A weakness of the Deperrois approach is the breakdown for cases with non-unique maximum
           chord. Then a multitude of  lines exist, each one perpendicular to a different maximum chord
            oy) i = 1,2 ... , consequently  a  multitude  of  projections  exist,  inducing  the  breakdown  of
           Deperrois approach.
              To overcome the inconsistency of the longest chord approach, the minimum circumscribed
           circle (MCC) approach was developed by Dang Van  [7] and Papadopoulos [16].  The MCC
           approach defines the shear stress amplitude as the radius of the minimum circle circumscribing
           to  the  loading  path.  However,  the  minimum circumscribed circle  (MCC)  approach  cannot
           differentiate proportional loading path from non-proportional loading path, which means that
            the MCC approach cannot characterize the non-proportional loading effect.
              On  the  basis  of  the  MCC  approach  [7,  161,  a  new  approach,  called  the  minimum
            circumscribed ellipse (MCE) approach [14, 151, was proposed to compute the effective shear
            stress amplitude taking into account the non-proportional loading effect.
              The load traces are represented and analysed in the transformed deviatoric stress space [ 181,
            where each point  represents a value of  fi and the variations of   are shown during a
            loading cycle.  The  schematic  representation of  the  minimum circumscribed ellipse  (MCE)
            approach  and  the  relation  with  the  minimum  circumscribed  circle  (MCC)  approach  are
            illustrated in Fig. 2.
   481   482   483   484   485   486   487   488   489   490   491