Page 121 - Biaxial Multiaxial Fatigue and Fracture
P. 121

106                G.B. MARQUIS AND 2 K4MAUIIVEN-ROIKOMEN

             features  which  lead  to  fatigue damage.  Small cracks  grow in  a complicated manner that  is
             affected  by  crack  closure,  microstructure and  crack  size.  Linear elastic  fracture  mechanics
             assumes that the stress and strain fields surrounding a crack are uniquely determined by the
             stress intensity factor.  However, continuum mechanics assumptions are not valid for cracks of
             the  size  of  the  microstructure  because,  on  this  scale,  a  polycrystalline material  does  not
             resemble the ideal homogeneous solid.  Closure conditions for small cracks are also different
             since the crack  wake  is  small.  These factors prevent direct modeling with  linear elastic or
             elastic-plastic fracture mechanics.
             Critical plane models

             The so-called critical plane approaches to multiaxial fatigue have evolved from experimental
             observations of the nucleation and growth of cracks during cyclic loading. Models in this class
             attempt. to compute fatigue damage on specific planes within a test specimen or component.  A
             critical  plane  can,  therefore,  be  defined as one or  more planes  within  a  solid  subject to  a
             limiting value of some damage parameter. For example, in some models the limiting damage
             parameter value  is associated with  the maximum alternating shear strain on  a specific plane
             while  other  models  define  as  critical  the  plane  experiencing  the  maximum  value  of  some
             combination of stress and strain components during a load history. The common element in all
             critical plane approaches is that fatigue life is considered to be controlled by the combination
             of stresses and strains acting on a specific critical plane or on a set of critical planes. Socie and
             Marquis have published a review on critical plane and other approaches to multiaxial fatigue
             [I].
               It has been observed that fatigue life will usually be dominated either by crack gowth along
             shear planes or along tensile planes. Crack growth mode will depend on material, stress state,
             environment  and  strain  amplitude.  A  critical  plane  model  will  incorporate  the  dominant
             parameters  governing  either  type  of  crack  growth.  Due  to  the  different  possible  cracking
             modes, shear or tensile dominant, no single damage model should be expected to correlate test
             data for all materials in all life regimes.
               While  critical  plane  models  underscore  the  important  role  of  crack  nucleation  and
             propagation  on  fatigue,  they  do  not  specifically  model  crack  propagation.  Normally  they
             describe the complex crack nucleation and microcrack growth mechanisms in a general sense
             using load or strain values available in  most engineering applications. These stress or strain
             terms are normally those values that are obtained directly from strain gage measurements or
             finite element analysis. Crack growth from an initial size to faiIure is assumed, but for the sake
             of  simplicity most models avoid the integration of  crack a propagation equation. Successful
             models are able to predict both the fatigue life and the dominant failure plane(s).
               Among the early critical plane fatigue damage criteria, the Findley model [2-4] is one of the
             most refined. Findley suggested that the normal stress, On, on a shear plane might have a linear
             influence on the allowable alternating shear stress, A212.





               This model differs from earlier empirical methods [5-71 and methods based on extensions of
             static yield criteria in that it identifies the stress components acting on a specific plane within
   116   117   118   119   120   121   122   123   124   125   126