Ultrasonic Testing of Acoustic and Elastic Properties of 12Cr18Ni10Ti Steel Irradiated with Fast Electrons

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Special steel grades such as ChS-68 and 12Cr18Ni10Ti are used in nuclear power engineering, the space industry, medicine and other important areas of the technical sphere, and during operation are exposed to various types of destructive effects, including radiation load. This paper presents the results of a study of the effect of high-energy electron radiation on the acoustic properties of austenitic stainless-steel grade 12Х18Н10Т. It was experimentally established that after exposure to electrons with an energy of 10 MeV, such parameters as the attenuation coefficient of ultrasound and the propagation velocity of transverse waves and Rayleigh waves change. These changes are due to defect formation and structural modifications of the material caused by radiation exposure. The obtained data allow us to conclude that it is necessary to take into account changes in the acoustic properties of steels when assessing their performance under radiation exposure.

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作者简介

Alexey Vasiliev

Yeltsin Ural Federal University

编辑信件的主要联系方式.
Email: vasilev.a.v98@list.ru
俄罗斯联邦, 19, Mir St., Yekaterinburg, 620002

Dmitry Biryukov

Yeltsin Ural Federal University

Email: bir-70@list.ru
俄罗斯联邦, 19, Mir St., Yekaterinburg, 620002

Vladimir Kostin

Mikheev Institute of Metal Physics of the Ural Branch of the Russian Academy of Sciences

Email: kostin@imp.uran.ru
俄罗斯联邦, 18, S. Kovalevskaya St., Yekaterinburg, 620108

Anatoly Zatsepin

Yeltsin Ural Federal University

Email: a.f.zatsepin@urfu.ru
俄罗斯联邦, 19, Mir St., Yekaterinburg, 620002

参考

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2. Fig. 1. Measurement of velocities and attenuation coefficients of longitudinal waves.

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3. Fig. 2. Measurement points of longitudinal wave parameters for the original (a) and irradiated (b) specimens.

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4. Fig. 3. Schemes of sounding of samples by transverse waves (a) and Rayleigh waves (b).

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5. Fig. 4. Results of Monte Carlo modelling of the interaction of fast electrons (10 MeV) with the material under study (12Cr18Ni10Ti steel): electron trajectories (trajectories of back-reflected electrons that left the sample are marked with red lines) (a); electron path profile (% fraction of retarded electrons at the corresponding depth) (b).

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6. Fig. 5. Attenuation coefficient in the original (a) and irradiated (b) specimens when sonicated with a 2.5 MHz PEP.

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7. Fig. 6. Interface of the programme for calculation of acoustic parameters in the far zone.

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