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铝合金表面变功率CO2激光除漆仿真与实验研究OA

Simulation and Experimental Study on Variable-power CO2 Laser Paint Removal from Aluminum Alloy Surfaces

中文摘要英文摘要

目的 探究变功率(P=10 W、20 W、30 W)对铝合金表面丙烯酸聚氨酯复合漆层CO2 激光清洗的影响规律.方法 建立对应功率条件下单坑与多道面扫描除漆瞬态模型,采用光学显微镜(OM)、扫描电子显微镜(SEM)、能谱仪(EDS)及白光干涉仪(WLI)对比研究仿真及实验结果,并结合高速 ICCD 成像揭示激光除漆机制.结果 单坑烧蚀模拟与实验除漆宽度相符,深度误差小于0.2%;单坑清洗实验截面轮廓随激光功率增加逐步平滑;三种功率单坑表面热应力仿真数值均超过了漆层抗拉强度,但热应力除漆深度不到烧蚀除漆深度的1.1%.多道面扫描除漆深度的仿真与实验结果基本吻合,P=10 W时面漆全部除净,底漆剩余厚度约为 15 µm;当P=20 W和30 W时,复合漆层全部除净,氧化膜先后发生了开裂和大面积熔损崩落现象.多道面扫描清洗表面粗糙度随激光功率增加先减小后增大,三种功率除漆过程均未产生激光诱导等离子体现象.结论 单坑及多道面扫描激光除漆仿真计算均能较为准确地预测实验结果,P=20 W为三种功率中能实现漆层除净的同时,氧化膜保存完整且除漆表面粗糙度最低的功率参数,CO2 激光除漆过程仅包含烧蚀和热应力两种耦合清洗机制.

The maintenance and refurbishment of composite paint layers on civil aircraft skins are critical for flight safety.Traditional chemical stripping and manual grinding methods,however,are characterized by high pollution,labor intensity,and low efficiency.While laser cleaning has emerged as a promising eco-friendly alternative,widely used nanosecond pulsed fiber or Nd:YAG lasers(wavelength:1 064 nm)often cause thermal damage to the substrate due to the high absorption rate of aluminum alloys at near-infrared wavelengths.To address this challenge,the work aims to investigate the efficacy and mechanism of removing acrylic polyurethane composite paints from LY12 aluminum alloy surfaces with a continuous-wave CO2 laser(wavelength:10.6 µm).The CO2 laser is selected for its high selectivity,as organic paint layers exhibit high absorption at this wavelength,whereas the metallic substrate reflects approximately 80%of the energy,theoretically protecting the anodic oxide film. A comprehensive methodology integrating finite element simulation(with COMSOL Multiphysics)and experimental validation was employed.Transient thermal-mechanical coupled models were established for both single-pit ablation and multi-pass area scanning under variable power conditions(10 W,20 W,and 30 W).The simulation assumed an ideal Gaussian beam distribution and considered the temperature-dependent thermal properties of the composite paint layer(total thickness:115 µm).Key process parameters included a scanning speed of 600 mm/s and a 90%overlap rate.Experimental validation was conducted with a T40 CO2 laser,with surface integrity characterized via optical microscopy(OM),scanning electron microscopy(SEM),energy-dispersive spectroscopy(EDS),and white light interferometry(WLI).Additionally,high-speed ICCD imaging was utilized to capture the dynamic plume evolution to elucidate the cleaning mechanism. Simulation results indicated that the calculated ablation crater widths were in good agreement with the experimental data,while the depth increased significantly with power.Notably,the simulation revealed that ablation did not cease immediately upon laser shut-off,and residual heat extended the material removal process by 21-48 µs.Although the calculated thermal stress at the pit center(approx.39.8 MPa)exceeded the paint's tensile strength,the depth of removal attributed to thermal stress was less than 1.1%of the total depth,confirming that gasification ablation was the dominant mechanism. In the multi-pass scanning experiments,the results matched well with the simulation predictions regarding the paint removal depth.At a low power of 10 W,the cleaning was incomplete;while the topcoat was removed,a residual primer layer of approximately 15 µm remained,accompanied by surface deposits of thermally stable β-copper phthalocyanine blue pigment.At a high power of 30 W,the paint was fully removed,but the excessive energy input caused the surface temperature to exceed the melting point of the anodic oxide film(reaching approx.2 399 K in simulation),resulting in severe oxide spallation and increased surface roughness(Sa=1.02 µm). The optimal processing window was identified at 20 W.Under this condition,the composite paint layer was completely removed without damaging the substrate.The anodic oxide film remained intact,exhibiting only minor micro-cracks induced by thermal stress,which did not compromise the substrate's integrity.This parameter yielded the superior surface quality with the lowest roughness(Sa=0.49 µm).Furthermore,comparative ICCD imaging revealed a distinct difference in mechanisms:unlike nanosecond lasers which generated expanding plasma shockwaves,the CO2 laser process produced no plasma,relying solely on a coupling mechanism of dominant ablation and auxiliary thermal stress. In conclusion,this study validates the accuracy of the developed finite element models for predicting CO2 laser cleaning outcomes.The findings demonstrate that optimizing laser power is crucial for achieving selective paint removal,providing a theoretical and experimental foundation for the application of CO2 lasers in high-precision aviation maintenance.

张天刚;刘家邦;丁页峰;张志强;薛鹏;张宏伟

中国民航大学 航空工程学院,天津 300300中国民航大学 航空工程学院,天津 300300中国民航大学 航空工程学院,天津 300300中国民航大学 航空工程学院,天津 300300中国民航大学 工程技术训练中心,天津 300300中国民航大学 工程技术训练中心,天津 300300

矿业与冶金

激光清洗CO2激光器铝合金丙烯酸聚氨酯漆层功率仿真与实验

laser cleaningCO2 laseraluminum alloyacrylic polyurethane paint layerlaser powersimulation and experiment

《表面技术》 2026 (8)

138-149,12

国家自然科学基金(U2033211) National Natural Science Foundation of China(U2033211)

10.16490/j.cnki.issn.1001-3660.2026.08.011

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