Deformation Behavior of the Zr53.5Cu26.5Ni5Al12Ag3 Bulk Metallic Glass Over a Wide Range of Strain Rate and Temperatures
The stress-strain relations for the Zr53.5Cu26.5Ni5Al12Ag3 bulk metallic glass (BMG) over a broad range of temperatures (room temperature to its supercooled liquid region) and strain rates (10^-4 to 10^-1 s^-1) were established in uniaxial compression using a thermal-mechanical simulation system. Th...
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          | Published in | Journal of materials science & technology Vol. 31; no. 9; pp. 941 - 945 | 
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| Main Authors | , , , | 
| Format | Journal Article | 
| Language | English | 
| Published | 
            Elsevier Ltd
    
        01.09.2015
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| Subjects | |
| Online Access | Get full text | 
| ISSN | 1005-0302 1941-1162  | 
| DOI | 10.1016/j.jmst.2015.06.001 | 
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| Abstract | The stress-strain relations for the Zr53.5Cu26.5Ni5Al12Ag3 bulk metallic glass (BMG) over a broad range of temperatures (room temperature to its supercooled liquid region) and strain rates (10^-4 to 10^-1 s^-1) were established in uniaxial compression using a thermal-mechanical simulation system. The superplastic flow was seen above its glass transition temperature (Tg = 694 K) and strain rates of up to 10^-1 s^-1 from the variation of stress-strain curves. A deformation map of strain rate vs temperature of Zr53.5Cu26.5Ni5Al12Ag3 was obtained, which was mainly composed of homogeneous and inhomogeneous deformation regions, the former featuring either Newtonian or non-Newtonian flow while the latter characterizing linear elastic behavior followed by shear localization, respectively. A phenomenological constitutive equation used to describe a master curve of viscosity with respect to the strain rate was obtained by fitting the experi- mental results, which determines the viscosity of the present alloy at the temperature near and above Tg. The results show the Zr53.5Cu26.5Ni5Al12Ag3 BMG is the subject suitable for net shape forming process at the supercooled liquid region. | 
    
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| AbstractList | The stress–strain relations for the Zr53.5Cu26.5Ni5Al12Ag3 bulk metallic glass (BMG) over a broad range of temperatures (room temperature to its supercooled liquid region) and strain rates (10−4 to 10−1 s−1) were established in uniaxial compression using a thermal-mechanical simulation system. The superplastic flow was seen above its glass transition temperature (Tg = 694 K) and strain rates of up to 10−1 s−1 from the variation of stress–strain curves. A deformation map of strain rate vs temperature of Zr53.5Cu26.5Ni5Al12Ag3 was obtained, which was mainly composed of homogeneous and inhomogeneous deformation regions, the former featuring either Newtonian or non-Newtonian flow while the latter characterizing linear elastic behavior followed by shear localization, respectively. A phenomenological constitutive equation used to describe a master curve of viscosity with respect to the strain rate was obtained by fitting the experimental results, which determines the viscosity of the present alloy at the temperature near and above Tg. The results show the Zr53.5Cu26.5Ni5Al12Ag3 BMG is the subject suitable for net shape forming process at the supercooled liquid region. The stress-strain relations for the Zr53.5Cu26.5Ni5Al12Ag3 bulk metallic glass (BMG) over a broad range of temperatures (room temperature to its supercooled liquid region) and strain rates (10^-4 to 10^-1 s^-1) were established in uniaxial compression using a thermal-mechanical simulation system. The superplastic flow was seen above its glass transition temperature (Tg = 694 K) and strain rates of up to 10^-1 s^-1 from the variation of stress-strain curves. A deformation map of strain rate vs temperature of Zr53.5Cu26.5Ni5Al12Ag3 was obtained, which was mainly composed of homogeneous and inhomogeneous deformation regions, the former featuring either Newtonian or non-Newtonian flow while the latter characterizing linear elastic behavior followed by shear localization, respectively. A phenomenological constitutive equation used to describe a master curve of viscosity with respect to the strain rate was obtained by fitting the experi- mental results, which determines the viscosity of the present alloy at the temperature near and above Tg. The results show the Zr53.5Cu26.5Ni5Al12Ag3 BMG is the subject suitable for net shape forming process at the supercooled liquid region.  | 
    
| Author | Guangcai Ma Zhengwang Zhu ZhengWang Haifeng Zhang | 
    
| AuthorAffiliation | Shenyang National Laboratory for Materials Sdence, Institute of Metal Research, Chinese Academy ofSdences, Shenyang 110016, China Shenyang Kejin Advanced Material Company Limited, Shenyang 110016, China | 
    
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| CitedBy_id | crossref_primary_10_1016_j_jnoncrysol_2018_06_011 crossref_primary_10_1016_j_jmrt_2024_03_037 crossref_primary_10_1016_j_jnoncrysol_2018_12_004 crossref_primary_10_1002_prep_202200063 crossref_primary_10_1007_s40195_019_00882_7 crossref_primary_10_1016_j_msea_2020_139252 crossref_primary_10_1016_j_jnoncrysol_2017_06_011 crossref_primary_10_1039_C9CP02545F crossref_primary_10_1038_srep19530 crossref_primary_10_1111_ffe_14246 crossref_primary_10_1016_j_ijplas_2023_103673 crossref_primary_10_1016_j_jallcom_2024_176608 crossref_primary_10_1016_j_mtcomm_2021_102460 crossref_primary_10_1016_j_jmst_2016_10_012 crossref_primary_10_1007_s11665_022_07467_z crossref_primary_10_1016_j_intermet_2025_108754 crossref_primary_10_1016_j_jmst_2017_01_024 crossref_primary_10_1016_j_msea_2022_143165 crossref_primary_10_1063_5_0059822 crossref_primary_10_1016_j_acme_2018_09_001 crossref_primary_10_1103_PhysRevMaterials_7_105604  | 
    
| Cites_doi | 10.1016/0001-6160(77)90232-2 10.1016/S0921-5093(00)01562-8 10.1016/j.jmst.2014.04.018 10.1016/j.jmst.2014.03.028 10.1016/j.jmst.2013.12.020 10.1016/j.msea.2014.10.051 10.1016/S1369-7021(04)00124-5 10.1016/j.jnoncrysol.2014.12.036 10.1016/S1359-6454(01)00068-4 10.1016/j.actamat.2006.09.012 10.1016/S1359-6454(03)00164-2 10.1016/j.jallcom.2015.03.158 10.1016/S1359-6454(99)00300-6 10.1016/j.scriptamat.2005.09.051 10.1103/PhysRevLett.94.205502 10.1063/1.1827349 10.1557/S0883769400053252  | 
    
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| Notes | 21-1315/TG The stress-strain relations for the Zr53.5Cu26.5Ni5Al12Ag3 bulk metallic glass (BMG) over a broad range of temperatures (room temperature to its supercooled liquid region) and strain rates (10^-4 to 10^-1 s^-1) were established in uniaxial compression using a thermal-mechanical simulation system. The superplastic flow was seen above its glass transition temperature (Tg = 694 K) and strain rates of up to 10^-1 s^-1 from the variation of stress-strain curves. A deformation map of strain rate vs temperature of Zr53.5Cu26.5Ni5Al12Ag3 was obtained, which was mainly composed of homogeneous and inhomogeneous deformation regions, the former featuring either Newtonian or non-Newtonian flow while the latter characterizing linear elastic behavior followed by shear localization, respectively. A phenomenological constitutive equation used to describe a master curve of viscosity with respect to the strain rate was obtained by fitting the experi- mental results, which determines the viscosity of the present alloy at the temperature near and above Tg. The results show the Zr53.5Cu26.5Ni5Al12Ag3 BMG is the subject suitable for net shape forming process at the supercooled liquid region. Bulk metallic glassesViscosityDeformation behaviorCompressionConstitutive equation  | 
    
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| Snippet | The stress-strain relations for the Zr53.5Cu26.5Ni5Al12Ag3 bulk metallic glass (BMG) over a broad range of temperatures (room temperature to its supercooled... The stress–strain relations for the Zr53.5Cu26.5Ni5Al12Ag3 bulk metallic glass (BMG) over a broad range of temperatures (room temperature to its supercooled...  | 
    
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| SubjectTerms | Bulk metallic glasses Compression Constitutive equation Deformation behavior Viscosity 变形行为 大块金属玻璃 宽范围 应力-应变关系 应力-应变曲线 应变率 温度范围 玻璃化转变温度  | 
    
| Title | Deformation Behavior of the Zr53.5Cu26.5Ni5Al12Ag3 Bulk Metallic Glass Over a Wide Range of Strain Rate and Temperatures | 
    
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