摘要
红外锁相热波检测技术在单一的热波激励频率下仅能够检测到一定深度范围内的缺陷,当试样内部缺陷深度的跨度范围过大时,检测人员使用该技术易出现缺陷的漏检和误检。为了克服传统锁相热波检测技术中缺陷检测深度范围受限的缺点,提出了一种多频锁相融合方法。该方法首先根据锁相激励的理论解公式确定最优的热波激励频率和检测次数,再利用双路锁相相关及相位增强技术提取出不同频率下的相位图像,最后使用基于主成分分析的图像融合方法将所有相位图像重构为一幅融合图像。实验对含有不同深度和尺寸缺陷的玻璃纤维复合材料层压板进行检测,检测结果表明基于锁相热激励的多频融合方法相对于在单一热波激励频率下的检测能够扩大缺陷深度的可检测范围,检测图像的质量与其他传统的序列图像处理方法相比有较大的提升。
Objective Defects such as debonding,bulges,pores,pits,delaminations,and inclusions in composites commonly occur during manufacturing and service.These defects not only reduce strength and stiffness but also result in structural failures.Reliable non-destructive testing methods are required for evaluating the quality of composite materials.Lock-in thermography(LIT)is a full-field,non-contact,and non-destructive testing method based on image visualization,providing an efficient approach to assessing defect quality.However,the depth resolution of LIT subsurface defects is limited by the excitation frequency.A single excitation frequency can only detect defects within a specific depth range.Thus,if the range of defect depths within the specimen is extensive,inspectors are susceptible to leakage and misdetection of defects when this technique is employed.To overcome the limitations of traditional LIT,we propose a multi-frequency fused method.This method leverages optimal excitation frequency selection,phase extraction,phase enhancement,and phase image fusion to enhance the depth resolution of defects in composite materials.The defect information at different depths within the sample can be integrated into a single fused phase image by employing the proposed algorithm.Meanwhile,this method facilitates clear delineation of defect edges and accurate measurement of defect sizes.Our approach and findings are expected to make significant contributions to both qualitative and quantitative measurements in the non-destructive testing of composite structures.Methods We put forward a muti-frequency fused LIT method to enhance defect visibility and improve the depth resolution of subsurface defects.This approach consists of four steps:optimal excitation frequency selection,phase extraction,phase enhancement,and image fusion.The optimal thermal wave excitation frequencies and the number of excitation frequencies are initially determined according to the theoretical solution of thermal conduction.The selection of excitation frequencies considers both detection efficiency and quality.Subsequently,the phase images at different frequencies are derived using a correlation algorithm and phase enhancement technique.The phase variable which better reflects the defect information inside the specimen is obtained by transforming the temperature information of the surface during the heating period.The best detection results of defects at different depths within the specimen should be reflected in the phase image corresponding to a specific excitation frequency.Finally,the best detection results of all the defects are integrated into a fused image by adopting a principal component analysis algorithm.Results and Discussions To assess the effectiveness of the proposed method,we conduct an experiment to detect defects of various depths and sizes within glass fiber reinforced polymer(GFRP)laminates.A homemade infrared non-destructive testing system is employed for the experiment.The effectiveness of this method is validated by both qualitative and quantitative analyses,with additional discussion on the influence of experimental parameters.The raw thermal image is shown in Fig.9(a).Only six defects,which range in depth from 1 to 2 mm and in diameter from 10 to 20 mm and are located in the upper-right corner of the GFRP specimen,can be identified in the raw thermal image due to non-uniform heating.Fig.7 illustrates the phase images at different excitation frequencies without enhancement processing.Despite significant improvement in non-uniform heating,the contrast of defects remains low,and their edges are blurred due to simple linear stretching.The enhanced phase images at different excitation frequencies are shown in Fig.8.Enhanced phase images reveal a greater number of defects,although they are distributed across different excitation frequencies due to variations in depth and size.For instance,defects with a depth of 4 mm can only be detected in Figs.8(c)and(d),while those with a depth of 1‒2 mm exhibit higher contrast in Figs.8(a)and(b).This confirms that the optimal frequency for defect detection correlates with the depth of the defects.Fig.9(b)shows the fused image.Fifteen defects are detectable,except for one with a diameter of 5 mm and a depth of 4 mm in the lower-left corner,which results in a detection rate of 94%.Additionally,two thermal excitation methods of long pulse thermography and digital frequency modulated thermal wave imaging are also compared.Figure 10 and Table 1 highlight the superiority of the proposed method from qualitative and quantitative perspectives respectively.Figure 11 and Table 2 compare four different image fusion methods,with the principal component analysis method exhibiting the best performance.To balance computational efficiency and detection effectiveness,Figs.12 and 13 discuss the effect of different thresholds on selecting the optimal excitation frequency.Additionally,the phase difference threshold for this algorithm is determined to be 80%of the peak value.Conclusions We introduce a multi-frequency fusion detection method,which involves optimal excitation frequency selection,phase extraction,phase enhancement,and image fusion to improve the depth resolution of subsurface defects and enhance defect contrast.Phase images at different excitation frequencies are extracted by multiple LIT detection and integrated into a fused image.The fused result exhibits greater defect contrast and clearer defect edges than phase images obtained at a single excitation frequency.Additionally,it encompasses information about defects of varying depths within the specimen,thus minimizing misdetection and defect leakage.Experimental results demonstrate the superior detection performance of the proposed method compared to LPT and DFMTWI.Defects with a depth of 4 mm are observable in a sample with a thickness of 5 mm.Furthermore,the influence of critical parameters in the proposed method,such as threshold values,is discussed.The performance of four data fusion algorithms is also evaluated by employing two quantitative image fusion evaluation metrics.The findings suggest that the principal component analysis method is more suitable for the multi-frequency fusion detection strategy.Finally,we provide practical guidance for non-destructive inspection of composite structures.
作者
魏延杰
肖瑶
Wei Yanjie;Xiao Yao(Department of Engineering Mechanics,Shijiazhuang Tiedao University,Shijiazhuang 050043,Hebei,China;Hebei Research Center of the Basic Discipline Engineering Mechanics,Shijiazhuang Tiedao University,Shijiazhuang 050043,Hebei,China;State Key Laboratory of Mechanical Behavior and System Safety of Traffic Engineering Structures,Shijiazhuang Tiedao University,Shijiazhuang 050043,Hebei,China)
出处
《光学学报》
EI
CAS
CSCD
北大核心
2024年第11期74-84,共11页
Acta Optica Sinica
基金
国家自然科学基金(12372018)。
关键词
无损检测
锁相热像法
复合材料
相位图像
多频融合
non-destructive testing
lock-in thermography
composites
phase image
multi-frequency fusion