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Critical Plane-Energy Based Approachfor Assessment of Biaxial Fatigue Damage whem ...   201


            In equation (1) Gij is the stress tensor (both i and j are equal to1,2,3), and the stresses 01  1,
          622, and q3 are principal stresses. Since the thin-walled tubular specimens are in plane stress
          condition, 92=0.
          Principal stresses can be calculated from applied stress amplitudes:

                           o, =om, +[oI sin (e)]                              (34
                             I







          where orn1 and  crn2 are the longitudinal and the  transverse mean  stresses, respectively. The
          angle 8 is the angle during GI cycles of stressing in a block loading history at which the Mohr's
          circles are the largest and has the maximum value of shear strain. Angle 8 varies from 0 to
          2an. Angle I$  corresponds to the phase delay between loads on the longitudinal and transverse
          axes.
                                                                                2
            In Eq (2) G~ is the strain tensor (both i and j are equal to1,2,3) where the strains &ll,  ~  ~ and   ,
          ~33 are principal strains calculated using the elastic-plastic strain constitutive relation (Eq(4)).
          In Eq (4), the first square bracket presents the elastic and the second square presents the plastic
          components of strains:






          where the deviatoric stress Sij is defined as the difference between the tensorial stress oij and
                         1
          hydrostatic stress ( -okk ):
                        3
                                     1
                           s, = 6, --BJ,
                                    3
          where  &,=1   if  i=j
                S,=O   if  i#j
          E is the elastic modulus, ve=O.3 is the elastic Poisson's ratio for the material used in this study
          and Gkk  is the summation of principal stresses. The stress amplitude of the hysteresis loop at
          half-life cycle was  associated with the  stabilized cyclic stress-strain loop. The cyclic stress-
          strain curve can be  described with the  same mathematical expression as for the  monotonic
          stress-strain curve. The relationship between the equivalent cyclic plastic strain  E&  and the
          equivalent cyclic stress 0% obtained from uniaxial stabilized cyclic stress-strain data is:




          The coefficient and the exponent in   (6) are the cyclic strength coefficient, K*=1227 MPa,
          and the cyclic strain hardening exponent, n*=0.36,  respectively.
            Eq  (4) presents  elastic-plastic  deformation and  correlates the  tensorial  cyclic  stress  and
          strain components for  3D state of  stress and strain. A  simple form of  this  equation for the
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