对竣工的 DED 表面进行多道激光抛光

Arpan Patel, Samantha Webster, Jian Cao, K. Ehmann
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引用次数: 0

摘要

激光抛光(LP)提供了一种快速高效的方法,可对快速成型制造的零件表面进行再熔化,从而改变其几何和物理特性。根据激光参数的不同,重熔后的表面具有不同的特性,与原始表面相比,大部分表面粗糙度较低。在这项研究中,使用了高功率连续光纤激光器来抛光通过粉末喷吹定向能沉积(DED)工艺在钢基体上沉积单层熔覆层而产生的 Inconel 718 表面。抛光在不同的参数设置下进行,即激光功率、光束直径、进给速度或进给量、舱口空间和抛光次数。经过一次和两次抛光后,分析了这些参数对样品横截面表面粗糙度和微观结构特性的影响。样品横截面的光学显微图像显示存在过饱和的 γ 相颗粒、γ′ + γ″ 沉淀、拉维斯相和δ 相针状物。横截面内某些区域的高温梯度和较低凝固速率的共同作用导致了欠冷区域和靠近欠冷区域的未熔化区域的假热处理。用金字塔形的金刚石压头对 IN718 样品横截面上的不同区域进行网格压痕,由于析出物和相变 δ 颗粒的密度不同,导致显微硬度值不同,从而证实了上述结果。
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Multi-pass laser polishing of as-built DED surfaces
Laser polishing (LP) provides a fast and efficient way of re-melting part surfaces manufactured by additive manufacturing to alter both their geometric as well as physical properties. Depending on the laser parameters, remelted surfaces with different properties are achieved, with a majority exhibiting lower surface roughness compared to the original surface. In this study, a high-power continuous fiber laser is used to polish Inconel 718 surfaces produced by depositing a single layer of clads on a steel substrate by the powder-blown directed energy deposition (DED) process. Polishing was performed under different sets of parameters, namely, laser power, beam diameter, feed rate or feed, hatch space, and the number of polishing passes. Their effects on the surface roughness profiles and the microstructural properties of the sample cross-section were analyzed after one and two polishing passes. Optical microscopic images of the sample's cross-sections show the presence of supersaturated γ phase particles, γ′ + γ″ precipitates, Laves phases, and δ phase needles. The combined effect of high-temperature gradients and lower solidification rates in certain regions within the cross-section result in undercooled regions and pseudo heat treatment of unmelted regions close to the undercooled regions. These results are corroborated by indenting the various regions of the IN718 sample cross-section with a pyramidal diamond indenter in the form of a grid, resulting in different micro-hardness values due to different densities of precipitate and phase-transformed δ particles.
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