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Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn

In this study, acoustic emission (AE) measurements on polycrystalline tin as a function of temperature at different driving rates under compression were carried out. It is shown that there is a definite difference between the acoustic emission characteristics belonging to twinning (low temperatures)...

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Autores principales: Daróczi, Lajos, Elrasasi, Tarek Yousif, Arjmandabasi, Talaye, Tóth, László Zoltán, Veres, Bence, Beke, Dezső László
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8745864/
https://www.ncbi.nlm.nih.gov/pubmed/35009370
http://dx.doi.org/10.3390/ma15010224
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author Daróczi, Lajos
Elrasasi, Tarek Yousif
Arjmandabasi, Talaye
Tóth, László Zoltán
Veres, Bence
Beke, Dezső László
author_facet Daróczi, Lajos
Elrasasi, Tarek Yousif
Arjmandabasi, Talaye
Tóth, László Zoltán
Veres, Bence
Beke, Dezső László
author_sort Daróczi, Lajos
collection PubMed
description In this study, acoustic emission (AE) measurements on polycrystalline tin as a function of temperature at different driving rates under compression were carried out. It is shown that there is a definite difference between the acoustic emission characteristics belonging to twinning (low temperatures) as well as to dislocation slip (high temperatures). The stress averaged values of the exponents of the energy probability density functions decreased from [Formula: see text] = 1.45 ± 0.05 (−60 °C) to [Formula: see text] = 1.20 ± 0.15 (50 °C) at a driving rate of [Formula: see text] , and the total acoustic energy decreased by three orders of magnitude with increasing temperature. In addition, the exponent γ in the scaling relation S(AE)~D(AE)(γ) (S(AE) is the area and D(AE) is the duration) also shows similar temperature dependence (changing from γ = 1.78 ± 0.08 to γ = 1.35 ± 0.05), illustrating that the avalanche statistics belong to two different microscopic deformation mechanisms. The power law scaling relations were also analyzed, taking into account that the detected signal is always the convolution of the source signal and the transfer function of the system. It was obtained that approximate values of the power exponents can be obtained from the parts of the above functions, belonging to large values of parameters. At short duration times, the attenuation effect of the AE detection system dominates the time dependence, from which the characteristic attenuation time, τ(a), was determined as τ(a) ≅ 70 μs.
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spelling pubmed-87458642022-01-11 Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn Daróczi, Lajos Elrasasi, Tarek Yousif Arjmandabasi, Talaye Tóth, László Zoltán Veres, Bence Beke, Dezső László Materials (Basel) Article In this study, acoustic emission (AE) measurements on polycrystalline tin as a function of temperature at different driving rates under compression were carried out. It is shown that there is a definite difference between the acoustic emission characteristics belonging to twinning (low temperatures) as well as to dislocation slip (high temperatures). The stress averaged values of the exponents of the energy probability density functions decreased from [Formula: see text] = 1.45 ± 0.05 (−60 °C) to [Formula: see text] = 1.20 ± 0.15 (50 °C) at a driving rate of [Formula: see text] , and the total acoustic energy decreased by three orders of magnitude with increasing temperature. In addition, the exponent γ in the scaling relation S(AE)~D(AE)(γ) (S(AE) is the area and D(AE) is the duration) also shows similar temperature dependence (changing from γ = 1.78 ± 0.08 to γ = 1.35 ± 0.05), illustrating that the avalanche statistics belong to two different microscopic deformation mechanisms. The power law scaling relations were also analyzed, taking into account that the detected signal is always the convolution of the source signal and the transfer function of the system. It was obtained that approximate values of the power exponents can be obtained from the parts of the above functions, belonging to large values of parameters. At short duration times, the attenuation effect of the AE detection system dominates the time dependence, from which the characteristic attenuation time, τ(a), was determined as τ(a) ≅ 70 μs. MDPI 2021-12-28 /pmc/articles/PMC8745864/ /pubmed/35009370 http://dx.doi.org/10.3390/ma15010224 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Daróczi, Lajos
Elrasasi, Tarek Yousif
Arjmandabasi, Talaye
Tóth, László Zoltán
Veres, Bence
Beke, Dezső László
Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn
title Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn
title_full Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn
title_fullStr Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn
title_full_unstemmed Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn
title_short Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn
title_sort change of acoustic emission characteristics during temperature induced transition from twinning to dislocation slip under compression in polycrystalline sn
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8745864/
https://www.ncbi.nlm.nih.gov/pubmed/35009370
http://dx.doi.org/10.3390/ma15010224
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