Finite element analysis of temperature and residual stress profiles of porous cubic Ti-6Al-4V titanium alloy by electron beam melting
Finite element analysis of temperature and residual stress profiles of porous cubic Ti-6Al-4V titanium alloy by electron beam melting作者机构:School of Nuclear Equipment and Nuclear EngineeringYantai UniversityYantai 264005China Institute of Metal ResearchChinese Academy of SciencesShenyang 110016China
出 版 物:《Journal of Materials Science & Technology》 (材料科学技术(英文版))
年 卷 期:2020年第44卷第9期
页 面:191-200页
核心收录:
学科分类:07[理学] 0806[工学-冶金工程] 0817[工学-化学工程与技术] 08[工学] 070104[理学-应用数学] 0805[工学-材料科学与工程(可授工学、理学学位)] 080502[工学-材料学] 0703[理学-化学] 0802[工学-机械工程] 0701[理学-数学] 0702[理学-物理学] 0801[工学-力学(可授工学、理学学位)]
基 金:The work was financially supported by the Natural Science Foundation of Shandong Province,China(No.ZR2019MEM012) the Major Scientific and Technological Innovation Program of Shandong Province,China(No.2019JZZY010325) the Key Research Program of Frontier Sciences,CAS(No.QYZDJ-SSW-JSC031-02) the National Natural Science Foundation of China(No.51871220)
主 题:Electron beam melting Ti-6Al-4V titanium alloy Porous cubic grids Finite element analysis Temperature field Stress field
摘 要:The temperature and stress profiles of porous cubic Ti-6Al-4V titanium alloy grids by additive manufacturing via electron beam melting(EBM)based on finite element(FE)method were ***-dimensional FE models were developed to simulate the single-layer and five-layer girds under annular and lateral *** results showed that the molten pool temperature in five-layer girds was higher than that in single-layer grids owing to the larger mass and higher heat *** energies accumulated by the longer scanning time for annular path than lateral path led to the higher temperature and steeper temperature *** thermal stress drastically fluctuated during EBM process and the residual stress decreased with the increase of powder layer where the largest stress appeared at the first layer along the build *** stress under lateral scanning was slightly larger but relatively more homogeneous distribution than those under annular *** stress distribution showed anisotropy and the maximum Von Mises stress occurred around the central *** stress profiles were explained by the temperature fields and grids structure.