Page 240 - Biaxial Multiaxial Fatigue and Fracture
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224                      C. GAIER AND H. DANNBAUER

               The theory applied in FEMFAT differs in some aspects from classical approaches like the
             nominal stress concept or  the  local one  and can be characterized by the  terms  ,,influence
             parameter method“, “concept of synthetic S/N-curves” or “local stress concept”. As basic input
             data S/N-curves of unnotched specimens are used and modified locally at each node of the FE-
             mesh to obtain computed component S/N-curve at critical spots. Several influence parameters
             can  be  considered  as  e.g.  stress-gradient  to  take  into  account  notch  effects,  mean-stress
             influence,  surface roughness,  surface treatments,  temperature,  technological  size,  etc.  Also
             mean-stress rearrangements caused by plastic deformations are taken  into account. The user
             can choose between several analysis methods for the quantification  of the influence parameters,
             e.g.  methods which  are  fixed by  German guiding rules  from  the  Research  Committee  for
             Mechanical  Engineering  FKM  (“Forschungskuratorium Maschinenbau”)  [ 71 and  such  ones
             which have been developed by ECS (“Engineering Center Steyr”) [ 1-61.
                For proportional loads, which scale the magnitude of local stress states, but which do not
             change the orientation of the principal axes, classical damage hypotheses like the maximum
             principal stress hypothesis for brittle materials or the distortion energy (von Mises) criterion for
             ductile ones can be applied in the high cycle fatigue domain. These hypotheses deliver results
             with sufficient accuracy for the technical practice.
                The  situation  is  different  for  complex  load  situations, when  non-correlating  stochastic
             external loads are applied to components with complicated shapes. The principal axes of local
             stress tensors will change their orientations with time. For very special load combinations these
             axes can even rotate, while the magnitude of the maximum principal stress remains almost
             constant. A widely accepted and applied method to deal with such general load situations is the
             critical plane approach (e.g.  [8-131). At the critical spot of the component it is assumed, that the
             plane is responsible (“critical”)  for fatigue failure, for which the accumulated damage exceeds a
              critical limit at first (theoretically 1). A still open question remains, how to combine the critical
             plane method with classical rainflow counting procedures in a general way, for the assessment
             of  triaxial  stress  states  and  for  different material  behaviours (brittle/ductile).  A  method  is
             developed using a similar nomenclature for basic stress quantities as in [ 121 and [ 131.


             THEORETICAL BACKGROUND

              In fatigue science closed hysteresis loops in the local stress-strain-path have been recognized to
             be responsible for local damages of the material. This has been realized for uniaxial stress or
              strain states with constant directions. A procedure for counting such closed hyteresis loops is
             the well known rainflow counting method (Matsuishi and Endo [ 141, see Fig. 1).
                In reality the situation is much more complicated: Stresses and strains are symmetric tensors
              of second order in the 3D-space, where cycle counting methods cannot be applied directly. The
              stress  tensor must be reduced by two steps to obtain scalar quantities, for which a rainflow
              counting of amplitudes and mean values can be  applied (Fig. 2): The first step is the well
              known transformation into a plane, which is specified by its unit normal vector n:







              A  time  dependent  stress  vector  Sn(t) is  obtained,  consisting  of  three  independent  stress
              components  &At), S,,&)  and S,,&).
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