Numerical Simulation of Effect of Different Initial Morphologies on Melt Hydrodynamics in Laser Polishing of Ti6Al4V

被引:16
作者
Li, Kai [1 ,2 ]
Zhao, Zhenyu [1 ]
Zhou, Houming [2 ]
Zhou, Hao [1 ,2 ]
Yin, Jie [1 ,2 ]
Zhang, Wei [1 ]
Zhou, Guiyao [3 ]
机构
[1] Shenzhen Inst Informat Technol, Sch Intelligent Mfg & Equipment, Shenzhen 518172, Peoples R China
[2] Xiangtan Univ, Sch Mech Engn, Xiangtan 411105, Peoples R China
[3] South China Normal Univ, Guangdong Prov Key Lab Nanophoton Funct Mat & Dev, Guangzhou 510006, Peoples R China
关键词
laser polishing; different surface morphologies; melt hydrodynamics; numerical simulation; SURFACE; PREDICTION; ROUGHNESS; EVOLUTION; ALLOYS; MODEL;
D O I
10.3390/mi12050581
中图分类号
O65 [分析化学];
学科分类号
070302 ; 081704 ;
摘要
As a surface finishing technique for rapid remelting and re-solidification, laser polishing can effectively eliminate the asperities so as to approach the feature size. Nevertheless, the polished surface quality is significantly sensitive to the processing parameters, especially with respect to melt hydrodynamics. In this paper, a transient two-dimensional model was developed to demonstrate the molten flow behavior for different surface morphologies of the Ti6Al4V alloy. It is illustrated that the complex evolution of the melt hydrodynamics involving heat conduction, thermal convection, thermal radiation, melting and solidification during laser polishing. Results show that the uniformity of the distribution of surface peaks and valleys can improve the molten flow stability and obtain better smoothing effect. The high cooling rate of the molten pool resulting in a shortening of the molten lifetime, which prevents the peaks from being removed by capillary and thermocapillary forces. It is revealed that the mechanism of secondary roughness formation on polished surface. Moreover, the double spiral nest Marangoni convection extrudes the molten to the outsides. It results in the formation of expansion and depression, corresponding to nearby the starting position and at the edges of the polished surface. It is further found that the difference between the simulation and experimental depression depths is only about 2 mu m. Correspondingly, the errors are approximately 8.3%, 14.3% and 13.3%, corresponding to Models 1, 2 and 3, respectively. The aforementioned results illustrated that the predicted surface profiles agree reasonably well with the experimentally measured surface height data.
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页数:19
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