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Uniaxial Magnetic Pulse Tension of TiNi Alloy with Experimental Strain Rate Evaluation. / Ostropiko, E.; Magazinov, S.; Krivosheev, S.

в: Experimental Mechanics, Том 62, № 6, 07.2022, стр. 1027-1036.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

Harvard

Ostropiko, E, Magazinov, S & Krivosheev, S 2022, 'Uniaxial Magnetic Pulse Tension of TiNi Alloy with Experimental Strain Rate Evaluation', Experimental Mechanics, Том. 62, № 6, стр. 1027-1036. https://doi.org/10.1007/s11340-022-00864-4

APA

Vancouver

Author

Ostropiko, E. ; Magazinov, S. ; Krivosheev, S. / Uniaxial Magnetic Pulse Tension of TiNi Alloy with Experimental Strain Rate Evaluation. в: Experimental Mechanics. 2022 ; Том 62, № 6. стр. 1027-1036.

BibTeX

@article{068713a1a10d4e57b071c23289b3ba99,
title = "Uniaxial Magnetic Pulse Tension of TiNi Alloy with Experimental Strain Rate Evaluation",
abstract = "Background: Magnetic pulse methods are known since the 80 s and have become widespread for revealing the patterns of fracture processes. The magnetic pulse method can be modified for uniaxial high strain rate tension and be used to investigate the mechanical and functional properties of materials. Objective: The paper shows capabilities of the magnetic pulse method modified for uniaxial high strain rate tension, the scheme of experimental estimation of strain accumulation time and reveals the influence on the basic functional properties of the TiNi shape memory alloy. Method: The special shaped TiNi alloy specimens were deformed in tension mode using the modified magnetic pulse method. The one-way shape memory effects were measured and compared with ones after quasi-static tension. We used COMSOL Multiphysics to evaluate possible heating of the specimens during tests. Results: The technique resulted in a wide range of plastic strain rates from 2000s−1 to 10000 s−1, depending on the specimen{\textquoteright}s mass and residual strain. COMSOL Multiphysics simulation did not show the presence of induced currents or heating in the working parts of the specimens during the tests. The shape memory effect after magnetic pulse tension was lost compared to the shape memory effect after quasi-static deformation. Conclusions: The method allows obtaining various strain rates at the same residual strains without changing in the loading system or dimensions of the working parts of the specimens. The shape memory effect depends on the time for pre-strain accumulation: the shorter the time, the less the shape memory effect upon subsequent heating.",
keywords = "High strain rate, Magnetic pulse tension, Shape memory effect, TiNi alloy",
author = "E. Ostropiko and S. Magazinov and S. Krivosheev",
note = "Publisher Copyright: {\textcopyright} 2022, Society for Experimental Mechanics.",
year = "2022",
month = jul,
doi = "10.1007/s11340-022-00864-4",
language = "English",
volume = "62",
pages = "1027--1036",
journal = "Experimental Mechanics",
issn = "0014-4851",
publisher = "Springer Nature",
number = "6",

}

RIS

TY - JOUR

T1 - Uniaxial Magnetic Pulse Tension of TiNi Alloy with Experimental Strain Rate Evaluation

AU - Ostropiko, E.

AU - Magazinov, S.

AU - Krivosheev, S.

N1 - Publisher Copyright: © 2022, Society for Experimental Mechanics.

PY - 2022/7

Y1 - 2022/7

N2 - Background: Magnetic pulse methods are known since the 80 s and have become widespread for revealing the patterns of fracture processes. The magnetic pulse method can be modified for uniaxial high strain rate tension and be used to investigate the mechanical and functional properties of materials. Objective: The paper shows capabilities of the magnetic pulse method modified for uniaxial high strain rate tension, the scheme of experimental estimation of strain accumulation time and reveals the influence on the basic functional properties of the TiNi shape memory alloy. Method: The special shaped TiNi alloy specimens were deformed in tension mode using the modified magnetic pulse method. The one-way shape memory effects were measured and compared with ones after quasi-static tension. We used COMSOL Multiphysics to evaluate possible heating of the specimens during tests. Results: The technique resulted in a wide range of plastic strain rates from 2000s−1 to 10000 s−1, depending on the specimen’s mass and residual strain. COMSOL Multiphysics simulation did not show the presence of induced currents or heating in the working parts of the specimens during the tests. The shape memory effect after magnetic pulse tension was lost compared to the shape memory effect after quasi-static deformation. Conclusions: The method allows obtaining various strain rates at the same residual strains without changing in the loading system or dimensions of the working parts of the specimens. The shape memory effect depends on the time for pre-strain accumulation: the shorter the time, the less the shape memory effect upon subsequent heating.

AB - Background: Magnetic pulse methods are known since the 80 s and have become widespread for revealing the patterns of fracture processes. The magnetic pulse method can be modified for uniaxial high strain rate tension and be used to investigate the mechanical and functional properties of materials. Objective: The paper shows capabilities of the magnetic pulse method modified for uniaxial high strain rate tension, the scheme of experimental estimation of strain accumulation time and reveals the influence on the basic functional properties of the TiNi shape memory alloy. Method: The special shaped TiNi alloy specimens were deformed in tension mode using the modified magnetic pulse method. The one-way shape memory effects were measured and compared with ones after quasi-static tension. We used COMSOL Multiphysics to evaluate possible heating of the specimens during tests. Results: The technique resulted in a wide range of plastic strain rates from 2000s−1 to 10000 s−1, depending on the specimen’s mass and residual strain. COMSOL Multiphysics simulation did not show the presence of induced currents or heating in the working parts of the specimens during the tests. The shape memory effect after magnetic pulse tension was lost compared to the shape memory effect after quasi-static deformation. Conclusions: The method allows obtaining various strain rates at the same residual strains without changing in the loading system or dimensions of the working parts of the specimens. The shape memory effect depends on the time for pre-strain accumulation: the shorter the time, the less the shape memory effect upon subsequent heating.

KW - High strain rate

KW - Magnetic pulse tension

KW - Shape memory effect

KW - TiNi alloy

UR - http://www.scopus.com/inward/record.url?scp=85130119630&partnerID=8YFLogxK

UR - https://www.mendeley.com/catalogue/b40cfa7a-ac30-3c8c-86d1-771a84bd1b55/

U2 - 10.1007/s11340-022-00864-4

DO - 10.1007/s11340-022-00864-4

M3 - Article

AN - SCOPUS:85130119630

VL - 62

SP - 1027

EP - 1036

JO - Experimental Mechanics

JF - Experimental Mechanics

SN - 0014-4851

IS - 6

ER -

ID: 96788922