首页|选区激光熔化镍基合金IN625数值仿真热源模型比较研究

选区激光熔化镍基合金IN625数值仿真热源模型比较研究

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  • 国家科技期刊平台
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热源模型的选取对数值模拟增材制造过程中准确预测温度场分布和熔池形貌至关重要。本文选取面热源模型、体热源模型和双椭圆热源模型进行对比分析。3种热源模型被汇编成用户自定义子程序嵌入Abaqus/Standard 仿真软件中用于镍基高温合金IN625选区激光熔化过程中最高温度和熔池形貌的预测。仿真与实验结果对比表明，双椭圆模型可以较好地预测熔池几何形貌，而体热源模型在预测最高温度值时准确度更好。相比之下，面热源模型在预测最高温度和熔池形貌时准确度最差。研究结果表明，在开展深入研究之前，热源模型的校准修正是提高效率和模拟准确性的前提。
Comparison of Heat Source Model for Numerical Modeling of Selective Laser Melting of IN625 Superalloy
The selection of heat source model is very important to accurately predict the distribution of temperature field and melting pool geometry in the numerical modeling of additive manufacturing process.The surface model,volumetric model and double-ellipsoid model are selected for comparison and analysis.These three heat source models are progarmmed as user-defined subroutines with Abaqus/Standard simulation software to predict the peak temperature and melting pool geometry during selective laser melting(SLM)of IN625.The comparison between simulation and experimental results shows that double-ellipsoid model can predict the melting pool geometry well,while the volumetric model provides comparative peak temperature predictions.In contrast,the surface model exhibits significant deviations in both melting pool geometry and peak temperature.The findings in this research highlight the need for model calibration or modification to enhance efficiency and accuracy before further research can be conducted.

heat source modelnumerical modelingIN625temperaturemelting pool geometry

李斌训、孙玉晶、杜劲、夏岩、苏国胜、张庆

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齐鲁工业大学(山东省科学院)机械工程学院,济南 250353,中国

山东省机械设计研究院,济南 250031,中国

山东大学工程训练中心,济南 250002,中国

热源模型 数值仿真 IN625 温度 熔池形貌

Natural Science Foundation of Shandong ProvinceTalent Research Project of Qilu University of Technology(Shandong Academy of Sciences)National Natural Science Foundation of ChinaNational Natural Science Foundation of China

ZR2021QE2302023RCKY1185227543852205480

2024

10.16356/j.1005?1120.2024.02.004

南京航空航天大学学报(英文版)
南京航空航天大学

南京航空航天大学学报(英文版)

CSTPCD
影响因子：0.279
ISSN：1005-1120
年,卷(期)：2024.41(2)
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