Size effect during dynamic shear tests with hat-shaped specimens

The failure mechanism and size effect during the quasi-static and dynamic shear tests of hat-shaped specimens were investigated in this study. Three types of specimens with different shear ring thicknesses (800, 400, and 50 μm) were designed. Quasi-static tests were carried out using an electronic u...

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Main Authors: Lan Yan, Anna Jiang, Zhibin Wang, Feng Jiang, Fuzeng Wang, Xian Wu, Yong Zhang
Format: Article
Language:English
Published: Elsevier 2023-11-01
Series:Journal of Materials Research and Technology
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S2238785423025899
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author Lan Yan
Anna Jiang
Zhibin Wang
Feng Jiang
Fuzeng Wang
Xian Wu
Yong Zhang
author_facet Lan Yan
Anna Jiang
Zhibin Wang
Feng Jiang
Fuzeng Wang
Xian Wu
Yong Zhang
author_sort Lan Yan
collection DOAJ
description The failure mechanism and size effect during the quasi-static and dynamic shear tests of hat-shaped specimens were investigated in this study. Three types of specimens with different shear ring thicknesses (800, 400, and 50 μm) were designed. Quasi-static tests were carried out using an electronic universal testing machine, while dynamic impact tests were carried out using split Hopkinson pressure bar (SHPB) tests. The adiabatic temperature rises with different strain rates, and the shear ring thickness was calculated. We found that the adiabatic temperature rises of the specimens with shear ring thicknesses of 800 and 400 μm were much larger than those of the specimens with shear ring thicknesses of 50 μm. The failure surfaces after the SHPB test were investigated via scanning electron microscopy, and the failure surfaces after the SHPB test could be divided into three zones: tensile, shear, and impact zones. The effect of the shear ring thickness and impact speed on the failure surface morphology was discussed. The typical shear stress–strain curves could be divided into three sections: elastic, plastic rise, and plastic plateau sections. Subsequently, a modified Johnson–Cook constitutive model was employed to fit the shear stress–strain results, and the fitted curves showed good agreement with the tested curves.
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spelling doaj.art-8f13851e9e3248cfa1c71c6f2469aded2024-02-21T05:26:27ZengElsevierJournal of Materials Research and Technology2238-78542023-11-012732313242Size effect during dynamic shear tests with hat-shaped specimensLan Yan0Anna Jiang1Zhibin Wang2Feng Jiang3Fuzeng Wang4Xian Wu5Yong Zhang6College of Mechanical Engineering and Automation, Huaqiao University, Xiamen 361011, ChinaCollege of Mechanical Engineering and Automation, Huaqiao University, Xiamen 361011, ChinaShanxi Diesel Industry Limited Responsibility Company, Datong 037036, ChinaInstitute of Manufacturing Engineering, Huaqiao University, Xiamen 361021, China; Corresponding author.Institute of Manufacturing Engineering, Huaqiao University, Xiamen 361021, ChinaCollege of Mechanical Engineering and Automation, Huaqiao University, Xiamen 361011, ChinaCollege of Mechanical Engineering and Automation, Huaqiao University, Xiamen 361011, ChinaThe failure mechanism and size effect during the quasi-static and dynamic shear tests of hat-shaped specimens were investigated in this study. Three types of specimens with different shear ring thicknesses (800, 400, and 50 μm) were designed. Quasi-static tests were carried out using an electronic universal testing machine, while dynamic impact tests were carried out using split Hopkinson pressure bar (SHPB) tests. The adiabatic temperature rises with different strain rates, and the shear ring thickness was calculated. We found that the adiabatic temperature rises of the specimens with shear ring thicknesses of 800 and 400 μm were much larger than those of the specimens with shear ring thicknesses of 50 μm. The failure surfaces after the SHPB test were investigated via scanning electron microscopy, and the failure surfaces after the SHPB test could be divided into three zones: tensile, shear, and impact zones. The effect of the shear ring thickness and impact speed on the failure surface morphology was discussed. The typical shear stress–strain curves could be divided into three sections: elastic, plastic rise, and plastic plateau sections. Subsequently, a modified Johnson–Cook constitutive model was employed to fit the shear stress–strain results, and the fitted curves showed good agreement with the tested curves.http://www.sciencedirect.com/science/article/pii/S2238785423025899Hat-shaped specimenSize effectFailure mechanismSplit Hopkinson pressure barModified Johnson–Cook constitutive model
spellingShingle Lan Yan
Anna Jiang
Zhibin Wang
Feng Jiang
Fuzeng Wang
Xian Wu
Yong Zhang
Size effect during dynamic shear tests with hat-shaped specimens
Journal of Materials Research and Technology
Hat-shaped specimen
Size effect
Failure mechanism
Split Hopkinson pressure bar
Modified Johnson–Cook constitutive model
title Size effect during dynamic shear tests with hat-shaped specimens
title_full Size effect during dynamic shear tests with hat-shaped specimens
title_fullStr Size effect during dynamic shear tests with hat-shaped specimens
title_full_unstemmed Size effect during dynamic shear tests with hat-shaped specimens
title_short Size effect during dynamic shear tests with hat-shaped specimens
title_sort size effect during dynamic shear tests with hat shaped specimens
topic Hat-shaped specimen
Size effect
Failure mechanism
Split Hopkinson pressure bar
Modified Johnson–Cook constitutive model
url http://www.sciencedirect.com/science/article/pii/S2238785423025899
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AT zhibinwang sizeeffectduringdynamicsheartestswithhatshapedspecimens
AT fengjiang sizeeffectduringdynamicsheartestswithhatshapedspecimens
AT fuzengwang sizeeffectduringdynamicsheartestswithhatshapedspecimens
AT xianwu sizeeffectduringdynamicsheartestswithhatshapedspecimens
AT yongzhang sizeeffectduringdynamicsheartestswithhatshapedspecimens