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The Environment Effect on Fatigue Crack Growth Rates in  7049 Aluminium Alloy at ___   363


           the stress intensity amplitude AK due to premature contact of crack surfaces. Vasudkvan and
           Sadananda claimed, however, that plasticity in the wake of a crack has a minor influence on
           crack closure [33-351  and argued that fatigue propagation in vacuum does show load-ratio
           effects. It has experimentally been observed that da/dN near the threshold up to higher growth
           rates is nearly independent of the R-ratios in a high vacuum [36,37],  which leads to conclude
           that  plasticity does  not  induce  closure. They  found  that  crack  closure  effects were  less
           important when compared with microstructure and environment effects and do not influence
           the overall crack growth behaviour. Thus, crack growth rate data generated in  laboratory
           should not be used to predict crack growth rates in a structure unless one has measured crack
           closure  of  the  structure  in  service,  which  depends  on  the  component  geometry,  load,
           environment, and crack length.
              Since crack closure is usually assumed as one of the major causes for retardation effects,
           the  examination of  the magnitude of  crack closure and  its relative  role  in  crack  growth
           processes is  very  important. The  existence of  plasticity-induced crack  closure  has  been
           severely questioned by Vasudevan and Sadananda [33-351, while asperity-induced closure,
           which  includes roughness due to crack tortuosity, oxide or chemical reaction debris, etc. is
           more accepted. Paris [38] have provided a theoretical justification for modified criteria for
           crack closure. According to Sadananda et al. all methods used to date for measuring crack
           closure, tend to overestimate the crack closure levels. Therefore they proposed a crack closure
           measurement based on the shape of the load-displacement-curve  [39].
             Keeping in mind that the role of environment in the near-threshold regime is strongly more
           significant than any mechanical contributions such as plasticity, roughness, oxide, etc. effects,
           one may conclude according to Vasudevan and Sadananda that AKth decreasing with R is an
           intrinsic fatigue property of the material for that environment.
             Overload effects have  predominantly been  attributed to  either plasticity  induced crack
           closure behind the crack tip, residual stresses ahead of a crack tip, or a combination of both.
           The  mechanisms  such  as  crack  tip  blunting,  crack  deflection,  branching  and  secondary
           cracking, as well as crack tip  strain hardening or residual stresses ahead of the crack tip,
           involve mainly transient conditions at or ahead of the crack tip  [40]. Mechanisms such as
           plasticity-induced  closure  and  roughness-induced closure  operate  behind  the  crack  tip
           indirectly affecting the crack driving force.
             Vasudevan and  Sadananda presented an 'Unified  Approach to Fatigue"  which considers
           closure as a minor factor for crack advance [40]. They modelled fatigue crack propagation for
           a wide variety of materials by  assuming two stress intensity parameters, AK and Kmax, as the
           relevant crack tip driving forces. They showed that  for most  situations, the description in
           terms of AK and Kmx is necessary and sufficient for fatigue crack growth without the need of
           crack closure. According to this Unified Approach to Fatigue, K,,  and AK are two intrinsic
           parameters simultaneously required for quantifying fatigue crack  growth data. These two
           driving forces are intrinsic parameters of each material and are valid for short or long cracks,
           having no  anomalies between these two regimes [41]. The apparent different behaviour of
           short and long cracks is related to residual stresses. They claim that the residual stress cannot
           be crack closure. Crack closure exists only behind the crack tip and is induced by roughness,
           oxides, plastic deformation, etc. Crack tip plasticity can only produce compressive residual
           stresses at the crack tip and not crack closure effects according to Vasudkvan and Sadananda
           as  consequence of  overloads for  instance. The two parameters AK  and  Kmx lead to  two
           intrinsic thresholds that must be simultaneously exceeded for a fatigue crack to grow  [41].
           Crack retardation owing to residual stresses ahead of the crack tip is reported in [42,43]. Ling
           and  Schijve [44]  confirmed that  residual  stresses play  a major role in  the retardation by
           demonstrating that the effects can be eliminated by annealing after the overloads.
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