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材料研究学报  2011, Vol. 25 Issue (3): 283-288    
  研究论文 本期目录 | 过刊浏览 |
23Co13Ni11Cr3Mo超高强钢的高温变形行为
黄始全1, 易幼平1, 李蓬川2
1.中南大学机电工程学院 长沙 410083
2.中国第二重型机械集团公司 德阳 618000
High Temperature Deformation Behavior of 23Co13Ni11Cr3Mo Ultrahigh Strength Steel
HUANG Shiquan1, YI Youping1, LI Pengchuan2
1.School of Mechanical and Electrical Engineering, Central South University, Changsha 410083
2.China National Erzhong Group Co., Deyang 618000
引用本文:

黄始全 易幼平 李蓬川. 23Co13Ni11Cr3Mo超高强钢的高温变形行为[J]. 材料研究学报, 2011, 25(3): 283-288.
, . High Temperature Deformation Behavior of 23Co13Ni11Cr3Mo Ultrahigh Strength Steel[J]. Chin J Mater Res, 2011, 25(3): 283-288.

全文: PDF(1091 KB)  
摘要: 在Gleeble 1500热模拟机上进行大变形等温压缩实验, 研究了23Co13Ni11Cr3Mo钢的高温变形行为。结果表明: 流变应力随着变形温度的降低和应变速率的升高而增大, 在高温、低应变速率下动态再结晶软化效应显著, 在温度为1000℃、应变速率为0.001 s-1时流变应力下降29.6%。23Co13Ni11Cr3Mo钢在温度为1000--1100℃、应变速率为0.01--1 s-1范围内锻造,其动态再结晶充分发生, 晶粒细小, 随变形参数波动变化平缓。根据实验结果建立了峰值流变应力模型及稳态晶粒尺寸模型, 其预测值与实验值吻合得比较好。
关键词 金属材料超高强钢23Co13Ni11Cr3Mo动态再结晶晶粒尺寸    
Abstract:High strain isothermal compression tests were carried out in Gleeble 1500 to study high temperature deformation behavior of 23Co13Ni11Cr3Mo ultrahigh strength steel. The results show that flow stress decreases with temperature increasing, while increases with strain rate increasing. DRX softening played an important role at high temperature and low strain rate. Flow stress decreased about 29.6% from peak stress at 1000oC  and 0.001 s−1. The 23Co13Ni11Cr3Mo ultrahigh strength steel is suit to forge at 1000–1100 ! and strain rate 0.01–1 s−1. At these deformation conditions, sufficiect DRX occurred, grain size was small and changed little with temperature or strain rate increasing. Moreover, based on the experiment results, peak stress and steady grain size model were estalblished. The predicted values of this model agreed well with the experiment values.
Key wordsmetallic    ultrahigh strength steel    23Co13Ni11Cr3Mo    dynamic recrystallization    grain size
收稿日期: 2011-03-07     
ZTFLH: 

TG142

 
基金资助:

国家九七三计划资助项目2011CB706802和国家重大专项资助项目2009ZX04005--011。

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