YUAN Siyu
,
ZHANG Liwen
,
LIAO Shulun
,
QI Min
,
ZHEN Yu
,
GUO Shuqi
钢铁研究学报(英文版)
An FE model was developed to study thermal behavior during the rod and wire hot continuous rolling process. The FE code MSCMarc was used in the simulation using implicit static arithmetic. The whole rolling process of 30 passes was separated and simulated with several continuous 3D elasticplastic FE models. A rigid pushing body and a data transfer technique were introduced into this model. The online experiments were conducted on 304 stainless steel and GCr15 steel hot continuous rolling process to prove the results of simulation by implicit static FEM. The results show that the temperature results of finite element simulations are in good agreement with experiments, which indicate that the FE model developed in this study is effective and efficient.
关键词:
FE analysis;thermal behavior;hot continuous rolling;3D deformation
张鸿冰
,
倪乐民
,
徐祖耀
金属学报
经 LFG(ΔG~(γ→a))-Mogutnov(ΔG_(Fe)~(γ→a))、徐祖耀(Shu-A)(ΔG~(γ→a))-Orr-Chipman(ΔG_(Fe)~(γ→a))、徐祖耀(Shu-B)(ΔG~(γ→a))-Orr-Chipman(ΔG_(Fe)~(γ→a))组合,均可算得 Fe-Mn-C 合金的 Ms 温度且与实验值十分符合.所得结果经数学处理,得 Fe-Mn-C 系 Ms 与成分的关系为:Ms(K)=817.4-7513.4xc-4141.9x_(Mn)-32083.5x_Cx_(Mn)(LFG)Ms(K)=829.9-7580.5x_C-4166.0x_(Mn)-15727.8x_Cx_(Mn)(SHU-A)Ms(K)=829.2-7276.1x_C-2915.4x_(Mn)-43825.7x_Cx_(Mn)(SHU-B)其线性相关系数均大于0.992.C 和 Mn 浓度均使合金的 Ms 线性地降低,而碳的作用几乎是Mn 的两倍.处理中引入了合金元素交互作用项(x_Cx_(Mn)),表明 C,Mn 相互加剧对 Ms 的影响。随含 C,Mn 量的增加,相变驱动力均单调地增加,而不存在奇异点.Ms 和相变驱动力的计算值均依赖于ΔG_(Fe)~(γ→a)项.
关键词:
Journal of Materials Processing Technology
The crystallization temperatures and other thermal properties have been measured systematically for two ternary Cu-Ni-P and two quaternary Cu-Ni-Sn-P amorphous systems. The dependence of crystallization temperature on the composition for the four alloy systems can not be described basically by the usual used Naka rule. The Gibbs free energy of crystallization can be calculated for the alloy systems with the model proposed by Shu et al. Using the calculated free energy of crystallization, it is still not possible to properly describe all of the crystallization temperatures of the alloy systems. However, it has been found that the correlation between the crystallization temperature and the content of the alloy systems can be reasonably explained by the nucleation and growth rates of a new phase for the classical theory of phase transformation. It has been established that the classical theory of phase transformation can be used to describe the thermal stability of the Cu-based amorphous alloys during their crystallization process. (C) 1999 Published by Elsevier Science S.A. All rights reserved.
关键词:
thermal stability;amorphous alloys;Cu-P based alloy systems;classical;theory of phase transformation;solid-liquid interface;structural model;glasses
盖红星
,
李建军
,
韩军
,
邢艳辉
,
邓军
,
俞波
,
沈光地
,
陈建新
量子电子学报
doi:10.3969/j.issn.1007-5461.2005.01.016
采用Shu Lien Chuang方法计算了AlInGaAs/AlGaAs应变引起价带中重、轻空穴能量变化曲线,在Harrison模型的基础上详细地计算了AlInGaAs/AlGaAs和GaAs/AlGaAs量子阱电子、空穴子能级分布并且进一步研究了这两种材料在不同注入条件下的线性光增益.进一步计算比较可以得出AlInGaAs/AlGaAs应变量子阱光增益特性要优于GaAs/AlGaAs非应变量子阱增益特性,因此AlInGaAs/AlGaAs应变量子阱半导体材料应用于半导体激光器比传统GaAs/AlGaAs材料更具优势.
关键词:
光电子学
,
应变量子阱
,
光增益
,
AlInGaAs
,
半导体激光器
王学滨
稀有金属材料与工程
认为试样表面的变形场出现不连续性不是绝热剪切带出现的标志,而是形变绝热剪切带进一步发展的结果；在计算绝热剪切带内部的峰值温度时应从局部剪切应变中扣除弹性应变,因为弹性应变不会对塑性功有所贡献.以动态扭转的Ti-6Al-4V试样(TA-50)为例,计算了绝热剪切带内部的峰值温度,其被划分为3部分:环境温度、均匀和非均匀变形引起的温度.在两种条件下(从局部剪切应变中扣除弹性应变与否),计算出的峰值温度分别为669和665℃,其在热回复和再结晶的温度范围之内,未达到相变的温度,比Liao及Duffy的理论计算值(630℃)要高.如果剪切应力-局部塑性剪切应变的关系不能完全确定,适当的近似是必要的.
关键词:
Ti-6Al-4V
,
绝热剪切带
,
峰值温度
,
局部塑性剪切应变
,
剪切弹性模量
,
再结晶
王学滨
稀有金属材料与工程
提出了利用梯度塑性理论计算Ti-6Al-4V绝热剪切带的局部剪切应变新方法.绝热剪切带的最大局部塑性剪切应变依赖于临界塑性剪切应变、试样的标定长度、绝热剪切带总厚度、绝热剪切带的平均塑性剪切应变.计算表明,随着绝热剪切带总厚度的增加,绝热剪切带的最大局部塑性剪切应变以非线性方式下降.当绝热剪切带总厚度的取值接近1 mm时,尽管确定临界塑性剪切应变的方法不同,但是,绝热剪切带的最大局部塑性剪切应变的计算值差别很小.当绝热剪切带总厚度取值在0.335～1 mm之间时,绝热剪切带的最大局部塑性剪切应变的计算值位于Liao及Duffy(1998)实验结果的下限(75%)和上限(350%)之间.
关键词:
Ti-6Al-4V
,
绝热剪切带
,
梯度塑性理论
,
局部塑性剪切应变
,
标定长度
王学滨
稀有金属材料与工程
基于曲线的最小二乘拟合方法,计算了Ti-6Al-4V绝热剪切带出现时的临界塑性剪切应变.根据梯度塑性理论,获得了绝热剪切带内部的局部塑性剪切变形分布曲线的理论表达式,用于拟合Liao及Duffy的实验数据.在不同的绝热剪切带宽度取值条件下,估算了绝热剪切带出现时的临界塑性剪切应变.当绝热剪切带的宽度取值在1～2 mm时,计算出的临界塑性剪切应变在0.1～0.47之间.绝热剪切带内部的局部变形分布曲线的理论表达式可以很好地描述流线的非线性特征.当绝热剪切带的宽度取值较大时,绝热剪切带内部的流线的理论结果在两端较弯曲；而当其取值较小时,这些流线比较平直,仅稍微弯曲.
关键词:
Ti-6Al-4V
,
绝热剪切带
,
宽度
,
局部变形分布
,
梯度塑性理论
,
最小二乘拟合方法
王学滨
稀有金属材料与工程
通过引入与Batra及Kim类似的观点,将绝热剪切带宽度定义为绝热剪切带的中心区域的宽度(W5%),在该区域上温度比其峰值小5%,利用Johnson-cook模型及梯度塑性理论分析Ti-6A1-4V绝热剪切带的厚度随环境温度的演变规律.计算表明,随着环境温度的升高,绝热剪切带宽度增加,这与许多实验观测结果一致.当绝热剪切带的总厚度在上限时,绝热剪切带宽度-环境温度曲线是稍微上凹的;但是,当绝热剪切带的总厚度在下限时,绝热剪切带宽度-环境温度曲线基本上是直线,著名的Dodd及Bai模型无法预测这些新现象.关于绝热剪切带宽度的计算结果非常接近于Liao及Duffy的实测结果.在忽略应变硬化的条件下,采用线性软化模型及梯度塑性理论推导w5%的简化解析式,发现环境温度、密度、热容、软化模量、剪切应力的增加使绝热剪切的敏感性降低,而功热转化因子及抗剪强度的降低使绝热剪切的敏感性降低.
关键词:
Ti-6Al-4V
,
绝热剪切带
,
宽度
,
环境温度
,
梯度塑性理论
,
Johnson-Cook模型
,
绝热剪切敏感性
