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In this part, the Khan–Huang–Liang (KHL) constitutive model was extended to account for kinematic hardening characteristic behavior of materials. The extended model is then generalized and used to simulate experimental response of oxygen free high conductivity (OFHC) copper under cyclic shear straining and biaxial tension–torsion (multiaxial ratchetting) experiments presented in Part I (Khan et al., 2007). In addition, a new modification for the non-linear kinematic hardening rule of Karim–Ohno (Abdel-Karim and Ohno, 2000) is proposed to simulate multiaxial ratchetting behaviors. Although, the kinematic hardening contributes the most to the response, it is shown that, the loading rate effect, and a coupled isotropic and kinematic hardening effect should also be considered while simulating the multiaxial ratchetting behavior of OFHC copper. Furthermore, the newly modified kinematic hardening rules is able to fairly well simulate the multiaxial ratchetting experiments under different loading conditions, irrespective of the value of applied axial tensile stress, shear strain amplitude, pre-cyclic hardening and/or loading sequence. 相似文献
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采用化爆加载,以黄铜为飞片、无氧铜为靶板,测量了以抗氢钢(HR2)、重玻璃(SiO2)、铝合金(LY12/LF6)、镁铝合金(MB2)、有机玻璃(PMMA)和空气(Air)为垫块(Anvil)材料中的冲击波速度(上述材料的Hugoniot状态参数C0、λ均为已知),由此确定了无氧铜的等熵卸载路径。结果表明:在冲击态(即初始卸载态)高达219 GPa的压力范围内,无氧铜的等熵卸载过程可用Grüneisen状态方程在ργ=ρ0γ0近似下作很好的描述;各条卸载路径到一个大气压的终态粒子速度US与镜像反演的粒子速度2u的偏差(US-2u)/(2u),随冲击波压力的增加而增大。 相似文献
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A series of experiments has been conducted on oxygen free high conductivity (OFHC) copper hollow cylinders under cyclic free-end torsion and biaxial tension–torsion at large strains. In addition, equations are developed to account for the finite rotation and strains in electrical resistance strain gages. In free-end cyclic torsion experiments with shear strain range equal to 23%, a significant strain in the axial direction is observed and it accumulates with a constant rate cycle by cycle. In the biaxial tension–torsion (multiaxial ratchetting) experiments, in which the primary (constant) axial stress is larger than the initial yield stress of the material, the loading conditions are varied to determine the influence of primary axial stress, cyclic shear strain range, pre-cyclic hardening and loading sequence on multiaxial ratchetting. Some important experimental features are high-lighted and recommended to help modeling efforts later. 相似文献
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采用Hopkinson装置和一种基于一级气体炮的高速冲击拉伸断裂装置,研究了无刻槽高导无氧铜
(OFHC)杆在一系列冲击拉伸速度下的断裂。当冲击拉伸速度大于40m/s时,断裂位置总在冲击拉伸端附
近,此速度被确定为OFHC的实验临界冲击拉伸速度。一种受单轴冲击拉伸荷载的、中心含椭球空穴的样本
体积单元被用于数值模拟所含空穴的增长与失稳的过程。OFHC的J-C与Z-A 本构关系用于描述基体材料
的动态响应。讨论了空穴失稳条件并提出以空穴形状演化为判据,比较了空穴失稳时的样本体积单元平均径
向应变与无刻槽杆的冲击断裂应变。也用这种样本体积单元模型分析了OFHC的实验临界冲击拉伸速度。 相似文献
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高导无氧铜在大变形、不同温度和不同应变率下的流动应力和本构模型 总被引:1,自引:0,他引:1
为了理解高导无氧铜(OFHC Cu)的塑性流动行为,采用Instron液压试验机和分离式Hopkinson压杆,系统地对OFHC Cu进行了温度为77 ~1 000 K,应变率为0.001 ~7 000 s-1,以及真实应变超过80%的单轴压缩试验。结果表明:在0.001 s-1应变率下, OFHC Cu在约500 K呈现动态应变时效现象。随应变率增高,动态应变时效温度区域向更高温度移动,甚至动态应变时效现象消失。在高应变变形区域,相对温度来说,OFHC Cu塑性流动应力对应变率依赖更强。基于位错运动学和动力学概念,考虑位错在高温和高应变率的粘-曳阻力现象,结合试验结果,导出一个基于物理概念的本构模型。此模型可预测从低到高不同应变率不同温度下OFHC Cu的塑性流动应力。通过比较表明,本构模型预测结果与试验结果吻合较好。 相似文献
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为有效测量试件中的应力、应变及应变率,Hopkinson拉伸试验(TSHB)必须作优化分析,所进行的数值模拟涉及试件与杆件等连接对于实验结果的影响.为减小上升前沿、惯性效应且使试件处于一维应力及均匀应力与应变状态,优化的试件具有一定的长度与形状要求.对于高导无氧铜,由准静态试验及不同应变率与温度的优化TSHB试验得到一系列应力-应变曲线,并被拟合确定J-C及Z-A型动态本构模型.利用所确定的动态本构模型数值计算的反射与透射的应变在一定程度上与实验结果一致.文中强调指出,必须采用全过程数值模拟,对TSHB试验进行优化设计,并且对所确定的试件动态本构模型进行代入校核,再现实验结果. 相似文献
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