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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Main Authors: Lajos Daróczi, Tarek Yousif Elrasasi, Talaye Arjmandabasi, László Zoltán Tóth, Bence Veres, Dezső László Beke
Format: Article
Language:English
Published: MDPI AG 2021-12-01
Series:Materials
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Online Access:https://www.mdpi.com/1996-1944/15/1/224
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author Lajos Daróczi
Tarek Yousif Elrasasi
Talaye Arjmandabasi
László Zoltán Tóth
Bence Veres
Dezső László Beke
author_facet Lajos Daróczi
Tarek Yousif Elrasasi
Talaye Arjmandabasi
László Zoltán Tóth
Bence Veres
Dezső László Beke
author_sort Lajos Daróczi
collection DOAJ
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 <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>ε</mi></mrow></semantics></math></inline-formula> = 1.45 ± 0.05 (−60 °C) to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>ε</mi></mrow></semantics></math></inline-formula> = 1.20 ± 0.15 (50 °C) at a driving rate of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>ε</mi><mo>=</mo><mn>0.15</mn><mo> </mo><msup><mi mathvariant="normal">s</mi><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow></semantics></math></inline-formula>, and the total acoustic energy decreased by three orders of magnitude with increasing temperature. In addition, the exponent <i>γ</i> in the scaling relation <i>S<sub>AE</sub>~D<sub>AE</sub><sup>γ</sup></i> (<i>S</i><i><sub>AE</sub></i> is the area and <i>D</i><i><sub>AE</sub></i> is the duration) also shows similar temperature dependence (changing from <i>γ</i> = 1.78 ± 0.08 to <i>γ</i> = 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, <i>τ<sub>a</sub></i>, was determined as <i>τ<sub>a</sub></i> ≅ 70 μs.
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spelling doaj.art-cd7e75689ccd4ae5bb413b7a84bffa4b2023-11-23T11:50:03ZengMDPI AGMaterials1996-19442021-12-0115122410.3390/ma15010224Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline SnLajos Daróczi0Tarek Yousif Elrasasi1Talaye Arjmandabasi2László Zoltán Tóth3Bence Veres4Dezső László Beke5Department of Solid State Physics, University of Debrecen, P.O. Box 400, H-4002 Debrecen, HungaryDepartment of Solid State Physics, University of Debrecen, P.O. Box 400, H-4002 Debrecen, HungaryDepartment of Solid State Physics, University of Debrecen, P.O. Box 400, H-4002 Debrecen, HungaryDepartment of Solid State Physics, University of Debrecen, P.O. Box 400, H-4002 Debrecen, HungaryDepartment of Solid State Physics, University of Debrecen, P.O. Box 400, H-4002 Debrecen, HungaryDepartment of Solid State Physics, University of Debrecen, P.O. Box 400, H-4002 Debrecen, HungaryIn 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 <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>ε</mi></mrow></semantics></math></inline-formula> = 1.45 ± 0.05 (−60 °C) to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>ε</mi></mrow></semantics></math></inline-formula> = 1.20 ± 0.15 (50 °C) at a driving rate of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>ε</mi><mo>=</mo><mn>0.15</mn><mo> </mo><msup><mi mathvariant="normal">s</mi><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow></semantics></math></inline-formula>, and the total acoustic energy decreased by three orders of magnitude with increasing temperature. In addition, the exponent <i>γ</i> in the scaling relation <i>S<sub>AE</sub>~D<sub>AE</sub><sup>γ</sup></i> (<i>S</i><i><sub>AE</sub></i> is the area and <i>D</i><i><sub>AE</sub></i> is the duration) also shows similar temperature dependence (changing from <i>γ</i> = 1.78 ± 0.08 to <i>γ</i> = 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, <i>τ<sub>a</sub></i>, was determined as <i>τ<sub>a</sub></i> ≅ 70 μs.https://www.mdpi.com/1996-1944/15/1/224stress/strain measurementsacoustic emissionSnplasticitytwinningdislocation slip
spellingShingle Lajos Daróczi
Tarek Yousif Elrasasi
Talaye Arjmandabasi
László Zoltán Tóth
Bence Veres
Dezső László Beke
Change of Acoustic Emission Characteristics during Temperature Induced Transition from Twinning to Dislocation Slip under Compression in Polycrystalline Sn
Materials
stress/strain measurements
acoustic emission
Sn
plasticity
twinning
dislocation slip
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 stress/strain measurements
acoustic emission
Sn
plasticity
twinning
dislocation slip
url https://www.mdpi.com/1996-1944/15/1/224
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