Nb-16Si-22Ti-2Cr-2Al-2Hf-xFe合金热加工性能研究
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  • 英文篇名:Hot Workability of Nb-16Si-22Ti-2Cr-2Al-2Hf-xFe Alloys
  • 作者:褚楚 ; 徐严谨 ; 侯红亮 ; 骆良顺 ; 苏彦庆 ; 郭景杰 ; 傅恒志
  • 英文作者:Chu Chu;Xu Yanjin;Hou Hongliang;Luo Liangshun;Su Yanqing;Guo Jingjie;Fu Hengzhi;AVIC Manufacturing Technology Institute;Aeronautical Key Laboratory for Plastic Technology;Beijing Key Laboratory for Plastic Technology and Equipment;National Key Laboratory for Precision Hot Processing of Metals, Harbin Institute of Technology;
  • 关键词:功率耗散图 ; 变形失稳图 ; 变形稳定区
  • 英文关键词:power dissipation diagram;;deformation instability diagram;;deformation stability zone
  • 中文刊名:COSE
  • 英文刊名:Rare Metal Materials and Engineering
  • 机构:中国航空制造技术研究院;塑性成形技术航空科技重点实验室;数字化塑性成形技术及装备北京市重点实验室;哈尔滨工业大学金属精密热加工国家级重点实验室;
  • 出版日期:2019-05-15
  • 出版单位:稀有金属材料与工程
  • 年:2019
  • 期:v.48;No.394
  • 基金:国家自然科学基金(51405458)
  • 语种:中文;
  • 页:COSE201905018
  • 页数:7
  • CN:05
  • ISSN:61-1154/TG
  • 分类号:125-131
摘要
通过对真空非自耗电弧炉制备的Nb-16Si-22Ti-2Cr-2Al-2Hf-xFe(x=0, 1,2, 3, 5, at%) 5种铌硅合金的热变形行为进行探索和研究,分别绘制了5种铌硅合金的热加工图,并分析了不同变形参数下合金显微组织的变化,确定了各合金的最佳变形工艺范围,为后续铌硅合金的设计及热加工研究提供了理论依据。合金耗散效率因子η的最大值出现在低应变速率及高温区域;最小值则出现在低温和高应变速率区域。不同Fe含量合金的热加工图中均存在失稳变形区,主要分布区域与低耗散效率因子区重合,同时,失稳区晶粒明显拉长,晶界出现弯曲扭折现象,晶粒大小分布不均匀,发生了局部塑性流动。稳定变形区存在链状的动态再结晶组织,细小的再结晶晶粒沿晶界分布,随着变形温度的升高和应变速率的降低,动态再结晶晶粒的尺寸增大。
        Through the research of hot deformation behavior of Nb-16Si-22Ti-2Cr-2Al-2Hf-xFe(x=0, 1,2,3, 5) alloys, the hot working diagrams of these alloys were made, which would provide a theoretical basis for subsequent design and hot working study of Nb-Si alloys.The maximum dissipative efficiency factor η appears in the region of low strain rate and high temperature; the minimum appears in low temperature and high strain rate region. There are unstable regions in the thermal processing map of the alloys with different Fe contents,mainly distributed in the regions with high strain rate and low temperature, coinciding with the low dissipative efficiency factor regions.The grains in the unstable regions are obviously elongated and the grain boundaries are curved. The grain size is uneven and local plastic flow occurs. The dynamic recrystallization structure exists in the stable deformation zone as well as the fine recrystallized grain is distributed along the grain boundary. With the increase of the deformation temperature and the decrease of the strain rate, the size of the dynamic recrystallization grain increases.
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