Dynamic mechanical performance and constitutive model for Zr58Cu12Ni12Al15Nb3 metallic glass

In this study, compression tests under quasi-static and dynamic states and plate impact experiments were performed on Zr58Cu12Ni12Al15Nb3 bulk metallic glass (BMG). The experimental results demonstrated that the BMG specimen fractured catastrophically without noticeable plastic deformation. Therefor...

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Main Authors: Y. Tan, Y.W. Wang, R. An, Q. Fu, Z.Q. Xu, X.W. Cheng, H.W. Cheng
Format: Article
Language:English
Published: Elsevier 2021-07-01
Series:Journal of Materials Research and Technology
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S2238785421005275
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author Y. Tan
Y.W. Wang
R. An
Q. Fu
Z.Q. Xu
X.W. Cheng
H.W. Cheng
author_facet Y. Tan
Y.W. Wang
R. An
Q. Fu
Z.Q. Xu
X.W. Cheng
H.W. Cheng
author_sort Y. Tan
collection DOAJ
description In this study, compression tests under quasi-static and dynamic states and plate impact experiments were performed on Zr58Cu12Ni12Al15Nb3 bulk metallic glass (BMG). The experimental results demonstrated that the BMG specimen fractured catastrophically without noticeable plastic deformation. Therefore, the Johnson-Holmquist II (JH-2) constitutive model was used to describe the mechanical response of the presented alloy. The constitutive parameters of the Zr-based BMG were determined from the experimental results based on the JH-2 constitutive equations. Subsequently, the constitutive model with the presented material parameters was programmed in the commercial finite element analysis software LS-DYNA to simulate the dynamic compression and penetration process. The good agreement between the numerical simulations and experimental results indicates that the obtained JH-2 constitutive parameters are accurate and effective.
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spelling doaj.art-42e6f52409dc4378b17a8af4624a18132022-12-21T19:57:50ZengElsevierJournal of Materials Research and Technology2238-78542021-07-011318661877Dynamic mechanical performance and constitutive model for Zr58Cu12Ni12Al15Nb3 metallic glassY. Tan0Y.W. Wang1R. An2Q. Fu3Z.Q. Xu4X.W. Cheng5H.W. Cheng6School of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081, China; National Key Laboratory of Science and Technology on Materials under Shock and Impact, Beijing 100081, ChinaSchool of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081, China; National Key Laboratory of Science and Technology on Materials under Shock and Impact, Beijing 100081, China; Beijing Institute of Technology Chongqing Innovation Center, Chongqing, 401120, China; Corresponding author.School of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081, China; National Key Laboratory of Science and Technology on Materials under Shock and Impact, Beijing 100081, ChinaSchool of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081, China; National Key Laboratory of Science and Technology on Materials under Shock and Impact, Beijing 100081, ChinaSchool of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081, China; National Key Laboratory of Science and Technology on Materials under Shock and Impact, Beijing 100081, ChinaSchool of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081, China; National Key Laboratory of Science and Technology on Materials under Shock and Impact, Beijing 100081, ChinaSchool of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081, China; National Key Laboratory of Science and Technology on Materials under Shock and Impact, Beijing 100081, ChinaIn this study, compression tests under quasi-static and dynamic states and plate impact experiments were performed on Zr58Cu12Ni12Al15Nb3 bulk metallic glass (BMG). The experimental results demonstrated that the BMG specimen fractured catastrophically without noticeable plastic deformation. Therefore, the Johnson-Holmquist II (JH-2) constitutive model was used to describe the mechanical response of the presented alloy. The constitutive parameters of the Zr-based BMG were determined from the experimental results based on the JH-2 constitutive equations. Subsequently, the constitutive model with the presented material parameters was programmed in the commercial finite element analysis software LS-DYNA to simulate the dynamic compression and penetration process. The good agreement between the numerical simulations and experimental results indicates that the obtained JH-2 constitutive parameters are accurate and effective.http://www.sciencedirect.com/science/article/pii/S2238785421005275Bulk metallic glassJH-2 constitutive modelDamageImpact
spellingShingle Y. Tan
Y.W. Wang
R. An
Q. Fu
Z.Q. Xu
X.W. Cheng
H.W. Cheng
Dynamic mechanical performance and constitutive model for Zr58Cu12Ni12Al15Nb3 metallic glass
Journal of Materials Research and Technology
Bulk metallic glass
JH-2 constitutive model
Damage
Impact
title Dynamic mechanical performance and constitutive model for Zr58Cu12Ni12Al15Nb3 metallic glass
title_full Dynamic mechanical performance and constitutive model for Zr58Cu12Ni12Al15Nb3 metallic glass
title_fullStr Dynamic mechanical performance and constitutive model for Zr58Cu12Ni12Al15Nb3 metallic glass
title_full_unstemmed Dynamic mechanical performance and constitutive model for Zr58Cu12Ni12Al15Nb3 metallic glass
title_short Dynamic mechanical performance and constitutive model for Zr58Cu12Ni12Al15Nb3 metallic glass
title_sort dynamic mechanical performance and constitutive model for zr58cu12ni12al15nb3 metallic glass
topic Bulk metallic glass
JH-2 constitutive model
Damage
Impact
url http://www.sciencedirect.com/science/article/pii/S2238785421005275
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