金属热处理 ›› 2025, Vol. 50 ›› Issue (2): 29-35.DOI: 10.13251/j.issn.0254-6051.2025.02.005

• 组织与性能 • 上一篇    下一篇

核燃料U-50%Zr合金的组织及热变形行为

李岩峰1,2, 郭洪1,2, 李明阳1,2, 胡秉坤1,2, 刘建成1,2   

  1. 1.中核新型材料研究与应用开发重点实验室, 内蒙古 包头 014035;
    2.中核北方核燃料元件有限公司, 内蒙古 包头 014035
  • 收稿日期:2024-12-06 修回日期:2024-12-17 发布日期:2025-04-10
  • 通讯作者: 郭 洪,正高级工程师,博士,E-mail:hengze2222@vip.qq.com
  • 作者简介:李岩峰(1984—),男,工程师,硕士,主要研究方向为核燃料制造技术,E-mail:66525850@qq.com。
  • 基金资助:
    中核集团集中研发项目(中核科发[2022]160号)

Microstructure and hot deformation behavior of U-50%Zr alloy for nuclear fuel

Li Yanfeng1,2, Guo Hong1,2, Li Mingyang1,2, Hu Bingkun1,2, Liu Jiancheng1,2   

  1. 1. CNNC Key Laboratory on New Materials Research and Application Development, Baotou Inner Mongolia 014035, China;
    2. China North Nuclear Fuel Co., Ltd., Baotou Inner Mongolia 014035, China
  • Received:2024-12-06 Revised:2024-12-17 Published:2025-04-10

摘要: 通过高频感应熔炼制备了核燃料U-50%Zr合金,利用金相显微镜和X射线衍射仪对其组织和物相进行了分析,利用Gleeble-3800热模拟试验机进行不同变形温度(500、550和600 ℃)和应变速率(0.01、0.1和1 s-1)下的热压缩试验,研究其热变形行为。结果表明,除变形温度600 ℃、应变速率为0.01 s-1外,其他变形条件下,U-50%Zr合金表现出明显的加工硬化特征。相同应变速率下,峰值应力随变形温度的升高而降低,特别是在600 ℃时,峰值应力相比于500 ℃和550 ℃降低明显;相同变形温度下,峰值应力随应变速率的增大而升高。U-50%Zr合金经热变形后,组织并未发生相变,均为δ-UZr2相;随热变形温度的升高,晶粒尺寸先基本不变随后增大,500、550 ℃时晶粒尺寸均在250 μm左右,600 ℃时,晶粒尺寸明显长大,达到493 μm。基于峰值应力,通过Arrhenius模型与温度补偿因子Z参数,建立了U-50%Zr合金的本构方程,其热变形激活能Q=694.9 kJ/mol。通过DMM动态材料模型构建了热加工图,并确定了合适的加工区间为:变形温度540 ℃以上,应变速率0.01~1 s-1

关键词: 核燃料U-50%Zr合金, 热压缩变形, 本构方程, 热加工图, 组织

Abstract: U-50%Zr alloy for nuclear fuel was prepared by high-frequency induction melting, and its microstructure and phase constituent were analyzed using metallographic microscope and X-ray diffractometer. The Gleeble-3800 thermal simulation test machine was used to conduct hot compression tests at different deformation temperatures (500, 550 and 600 ℃) and strain rates (0.01 s, 0.1 and 1 s-1) to investigate its hot deformation behavior. The results show that, except for a deformation temperature of 600 ℃ and a strain rate of 0.01 s-1, the U-50%Zr alloy exhibits significant work hardening characteristics under other deformation conditions. At the same strain rate, the peak stress decreases with the increase of deformation temperature, especially at 600 ℃, where the peak stress decreases significantly compared to 500 ℃ and 550 ℃. At the same deformation temperature, the peak stress increases with the increase of strain rate. After hot deformation, no phase transformation occurs in the microstructure, all of which are δ-UZr2 phase. As the hot deformation temperature increases, the grain size of the alloy initially remains basically unchanged and then increases. At 500 ℃ and 550 ℃, the grain size is around 250 μm, and at 600 ℃, the grain size significantly increases to 493 μm. Based on peak stress, the constitutive equation of U-50%Zr alloy is established using the hyperbolic sine function Arrhenius model and temperature compensation factor Z parameter, with a hot deformation activation energy Q=694.9 kJ/mol. A hot working map is constructed using DMM dynamic material model, and the appropriate processing range is determined as follows: deformation temperature above 540 ℃, strain rate between 0.01 s-1 and 1 s-1.

Key words: nuclear fuel U-50%Zr alloy, hot compression deformation, constitutive equation, hot working map, microstructure

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