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激光选区熔化Ti-6Al-4V合金纳米压痕蠕变研究
引用本文:董广辉,杨诗婷,姜爱峰,郎风超,田宪会,李继军.激光选区熔化Ti-6Al-4V合金纳米压痕蠕变研究[J].表面技术,2020,49(2):252-259.
作者姓名:董广辉  杨诗婷  姜爱峰  郎风超  田宪会  李继军
作者单位:内蒙古工业大学 理学院,呼和浩特 010051,内蒙古工业大学 理学院,呼和浩特 010051,内蒙古工业大学 理学院,呼和浩特 010051,内蒙古工业大学 理学院,呼和浩特 010051,内蒙古工业大学 理学院,呼和浩特 010051,内蒙古工业大学 理学院,呼和浩特 010051
基金项目:国家自然科学基金(1172013,11562016);内蒙古自然科学基金(2018MS01013);内蒙古工业大学科学研究项目(ZZ201812,ZY201818)
摘    要:目的研究原始态和退火态激光选区熔化Ti-6Al-4V合金的室温压痕蠕变特性。方法利用光学显微镜观察原始态和退火态激光选区熔化Ti-6Al-4V合金的显微组织。基于纳米压痕技术结合恒载荷法,测量原始态和退火态合金在室温下的最大压痕深度、蠕变位移和蠕变速率敏感指数等压痕蠕变参数,并分析两种状态下合金的蠕变机理。结果原始态合金的显微组织几乎全为α相,退火态合金的显微组织为网篮组织。荷载分别为200、300、400 mN时,加载阶段原始态合金的最大压痕深度比退火态合金的最大压痕深度分别提高43%、42%、34%;保载阶段,原始态合金的蠕变位移比退火态合金的蠕变位移分别提高129%、128%、139%。原始态合金的蠕变速率敏感指数m值分别为0.054、0.050、0.046,退火态合金的m值分别为0.041、0.032、0.022,相同荷载下原始态的m值均大于退火态的m值。结论退火处理形成的网篮组织,使退火态合金的蠕变速率敏感指数m值降低,从而使其蠕变抗力增强。原始态和退火态激光选区熔化Ti-6Al-4V合金的蠕变机理均为位错蠕变。

关 键 词:激光选区熔化  纳米压痕  TI-6AL-4V  压痕蠕变  蠕变速率敏感指数m
收稿时间:2019/6/3 0:00:00
修稿时间:2020/2/20 0:00:00

Nanoindentation Creep of Ti-6V-4V Alloy Prepared by Selective Laser Melting
DONG Guang-hui,YANG Shi-ting,JIANG Ai-feng,LANG Feng-chao,TIAN Xian-hui and LI Ji-jun.Nanoindentation Creep of Ti-6V-4V Alloy Prepared by Selective Laser Melting[J].Surface Technology,2020,49(2):252-259.
Authors:DONG Guang-hui  YANG Shi-ting  JIANG Ai-feng  LANG Feng-chao  TIAN Xian-hui and LI Ji-jun
Affiliation:School of Sciences, Inner Mongolia University of Technology, Hohhot 010051, China,School of Sciences, Inner Mongolia University of Technology, Hohhot 010051, China,School of Sciences, Inner Mongolia University of Technology, Hohhot 010051, China,School of Sciences, Inner Mongolia University of Technology, Hohhot 010051, China,School of Sciences, Inner Mongolia University of Technology, Hohhot 010051, China and School of Sciences, Inner Mongolia University of Technology, Hohhot 010051, China
Abstract:The work aims to study the indentation creep properties of Ti-6Al-4V alloy by laser selective melting in the primitive and annealed states.The microstructure of the Ti-6Al-4V alloy by selective laser melting in the primitive state and annealed state was observed by optical microscope and the indentation creep parameters of primitive and annealed alloys at room temperature were measured by nanoindentation technique combined with constant load method,such as maximum indentation depth,creep displacement and creep strain rate sensitivity.Then,the creep mechanism of alloys in two states was analyzed.The microstructure of primitive alloys was almost composed ofαphase,and the microstructure of annealed alloys was basket tissue.When the loads were 200 mN,300 mN and 400 mN respectively,the maximum indentation depth of primitive alloy increased by 43%,42%and 34%compared with that of annealed state alloy at loading stage,and the creep displacement of primitive state alloy increased by 129%,128%and 139%compared with that of annealed state alloy at holding stage;the creep strain rate sensitivity m values corresponding to the primitive state alloys were 0.054,0.050 and 0.046 respectively,and the m values of annealed alloys were 0.041,0.032 and 0.022 respectively.The m value of the primitive state was greater than the m value of the annealed state under the same load.The basket structure formed by annealing reduced the creep rate sensitive index m of the annealed state,thus enhancing the creep resistance.The creep mechanism of Ti-6Al-4V alloy prepared by selective laser melting in the primitive and annealed state is dislocation creep.
Keywords:nanoindentation  laser selective melting  Ti-6Al-4V  indentation creep  creep strain rate sensitivity m
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