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Thirty-nine peer-reviewed papers give you the most recent examine on fatigue and fracture mechanics. subject matters disguise:
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Additional resources for Fatigue and Fracture Mechanics, Volume 37:
Fracture toughness in terms of Jc is shown in Fig. 21͑a͒ for the non-irradiated material. Since cleavage fracture is known to originate at a single point in the material, intensive fractography was carried out, which revealed indeed the existence of isolated locations on the fracture surface from where cleavage fracture spread all over the fracture surface. These locations observed on 25 C͑T͒ specimens tested between −55 and −90° C are compiled in Fig. 21͑b͒. It is clearly seen that their positions, rc, ahead of the crack front vary within a wide range, which indicates that also several amounts of ductile tearing are needed to reach the weak points further ahead of the crack front.
20—Experimental and, with Eqs 35 and 36, estimated initiation values of K for ductile tearing, data from Ref 36. clear that such models can never be used to “predict” fracture toughness; however, they show how the various basic material parameters affect the result, and what could be done to improve the toughness of a speciﬁc material. Material data for validation of the three models can be found in Ref 36. It should be noted that the above derivations done in the framework of linear elastic fracture mechanics could be easily converted to elastic-plastic parameters such as the J-integral.
The aim of the investigation was not to determine the transferability of an R-curve from specimen to component; the aim was rather to check the ability of the ETM to estimate the deformation and fracture behavior of the large scale pipes. A study on internally pressurized cylinders ͓69͔ yielded also promising results. A thin-walled cylinder with a through-crack tested at TWI, Cambridge ͓70͔, was equipped with CTOD gages at both crack tips. The ETM estimates ͑Fig. 37͒ compare reasonably well with the pressure-CTOD record as averaged for both crack tips.
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