PSI - Issue 23
M.R. Tyutin et al. / Procedia Structural Integrity 23 (2019) 559–564 M.R.Tyutin , L.R.Botvina, V.P.Levin and I.O.Sinev/ Structural Integrity Procedia 00 (2019) 000 – 000
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caused by the dislocation motion. Thus, the 4 stages of damage changes that are noted earlier (Zharkova, Botvina, and Tyutin 2007) are evident due to the dislocations movement at the beginning of the plastic flow, the appearance of microcracks, their coalescence and the formation of fracture localization zone and macrocrack. The transition from one stage to another causes changes in the parameters of acoustic emission, as well as in the self-magnetic field intensity. A study of the staging of the fracture of austenitic stainless steel by acoustic emission method was also carried out by (Bashkov et.al. 2010), where it was shown that each type of defect (dislocation, micro- and macrocrack) corresponds to a certain AE signals spectrum, analyzing which authors identified fracture stages. Unfortunately, the lack of damage evolution data in specified article makes it difficult to compare the results obtained by Bashkov and the results of this study. A direct correlation of coercive force values with damage, not previously noted in the literature, is established. The study shows that the change in the in eddy current parameter with damage significantly differs in two studied steels. This is probably due to the deformation induced martensite transformation in austenitic steel. It is shown that changes in the rate of accumulation of microcracks in low-carbon steel at tension obey the Kachanov-Rabotnov equation.
Acknowledgements The study was supported by the Russian Science Foundation (project №1 9-19-00674).
References
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