# Thin Copper Plate Defect Detection Based on Lamb Wave Generated by Pulsed Laser in Combination with Laser Heterodyne Interference Technique

Xinhao Wang, Zhaojiong Zhu, Guqing Guo, Xiaocong Sun, Ting Gong, Yali

Tian, Yueting Zhou, Xuanbing Qiu, Xiaohu He, Huiqin Chen, et al.

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Xinhao Wang, Zhaojiong Zhu, Guqing Guo, Xiaocong Sun, Ting Gong, et al. Thin Copper Plate Defect Detection Based on Lamb Wave Generated by Pulsed Laser in Combination with Laser Heterodyne Interference Technique. Sensors, 2024, 24 (10), pp.3103. 10.3390/s24103103. hal-04781921

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Article

# Thin Copper Plate Defect Detection Based on Lamb Wave Generated by Pulsed Laser in Combination with Laser Heterodyne Interference Technique

Xinhao Wang<fnref n="1" />, Zhaojiong Zhu<fnref n="2" />, Guqing Guo<fnref n="2" />, Xiaocong Sun<fnref n="2" /> ID, Ting Gong<fnref n="2" />, Yali Tian<fnref n="2" />, Yueting Zhou<fnref n="2" />, Xuanbing Qiu<fnref n="2" /> ID, Xiaohu He<fnref n="2" />, Huiqin Chen<fnref n="1" />, Christa Fittschen<fnref n="3" /> ID and Chuanliang Li<fnref n="2" />,* ID

**Abstract:** Thin copper plate is widely used in architecture, transportation, heavy equipment, and integrated circuit substrates due to its unique properties. However, it is challenging to identify surface defects in copper strips arising from various manufacturing stages without direct contact. A laser ultrasonic inspection system was developed based on the Lamb wave (LW) produced by a laser pulse. An all-fiber laser heterodyne interferometer is applied for measuring the ultrasonic signal in combination with an automatic scanning system, which makes the system flexible and compact. A 3-D model simulation of an H62 brass specimen was carried out to determine the LW spatial-temporal wavefield by using the COMSOL Multiphysics software. The characteristics of the ultrasonic wavefield were extracted through continuous wavelet transform analysis. This demonstrates that the A₀ mode could be used in defect detection due to its slow speed and vibrational direction. Furthermore, an ultrasonic wave at the center frequency of 370 kHz with maximum energy is suitable for defect detection. In the experiment, the size and location of the defect are determined by the time difference of the transmitted wave and reflected wave, respectively. The relative error of the defect position is 0.14% by averaging six different receiving spots. The width of the defect is linear to the time difference of the transmitted wave. The goodness of fit can reach 0.989, and it is in good agreement with the simulated one. The experimental error is less than 0.395 mm for a 5 mm width of defect. Therefore, this validates that the technique can be potentially utilized in the remote defect detection of thin copper plates.

**Keywords:** laser ultrasonic; laser heterodyne interferometer; Lamb wave; thin copper plate; continuous wavelet transform

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**Citation:** Wang, X.; Zhu, Z.; Guo, G.; Sun, X.; Gong, T.; Tian, Y.; Zhou, Y.; Qiu, X.; He, X.; Chen, H.; et al. Thin Copper Plate Defect Detection Based on Lamb Wave Generated by Pulsed Laser in Combination with Laser Heterodyne Interference Technique. *Sensors* **2024**, *24*, 3103. https://doi.org/10.3390/s24103103

Academic Editor: Mohammad Noori

Received: 4 April 2024

Revised: 7 May 2024

Accepted: 8 May 2024

Published: 14 May 2024

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**Copyright:** © 2024 by the authors.
Licensee MDPI, Basel, Switzerland.
This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).

## 1. Introduction

Currently, thin copper plates, renowned for their remarkable thermal and electrical conductivity, excellent ductility, and inherent resistance to corrosion, are indispensable in various fields such as construction, automotive manufacturing, electrical components, and marine applications, showcasing their crucial role in modern technology and industry [1-4]. However, the copper plate may exhibit slight surface imperfections generated during the manufacturing process [5]. Timely detection of these tiny or micro defects could prevent their progression into larger structural and mechanical integrity issues. Therefore, it is

<footnote n="1">1 School of Materials Science and Engineering, Taiyuan University of Science and Technology, Taiyuan 030024, China; b20201491011@stu.tyust.edu.cn (X.W.); chenhuiqin@tyust.edu.cn (H.C.)</footnote>

<footnote n="2">2 Shanxi Province Engineering Research Center of Precision Measurement and Online Detection Equipment, Shanxi Center of Technology Innovation for Light Manipulations and Applications, School of Applied Science, Taiyuan University of Science and Technology, Taiyuan 030024, China; zhuzhaojiong@stu.tyust.edu.cn (Z.Z.); guqingguo@tyust.edu.cn (G.G.); sunxiacong@tyust.edu.cn (X.S.); gongting@tyust.edu.cn (T.G.); tianyali@tyust.edu.cn (Y.T.); zyt@tyust.edu.cn (Y.Z.); qiuxb@tyust.edu.cn (X.Q.); xiaohuhe@tyust.edu.cn (X.H.)</footnote>

<footnote n="3">3 CNRS, UMR 8522-PC2A—Physicohimie des Processus de Combustion et de l'Atmosphere, Université Lille, F-59000 Lille, France; christa.fittschen@univ-lille.fr</footnote>

<footnote>* Correspondence: li_chuanliang@126.com</footnote>
significant to develop real-time quantitative measurement and assessment of micro defects
on the surface of copper strips [6].

Several non-destructive testing techniques have been established, including penetrant testing, eddy current testing, ultrasonic testing, radiographic testing, and magnetic particle inspection. Nonetheless, there are certain limitations for these methods [7–11]. For instance, penetrant testing is affected by surface roughness and is not suitable for porous materials. Eddy current testing is sensitive to magnetic permeability changes, making it effective only for conductive materials and not effective for defects parallel to the surface. Ultrasonic testing principally relies on contact transducers and is improper for in-situ harsh environments. Radiographic testing is expensive and inefficient for cracks with special orientation. Magnetic particle inspection fails to detect low-permeability materials or deeply situated defects in casting and requires a sample with a smooth surface. Compared to these methods, laser ultrasonic testing possesses a lot of advantages, including non-contact operation, a high-frequency bandwidth, the ability to generate multi-mode ultrasound, independence from the electronic or magnetic properties of the testing materials, and a flexible laser shape for excitation [12–15]. Consequently, laser ultrasonic testing is increasingly utilized for determining the properties and identifying defects of materials.

A Lamb wave (LW) is a guided wave that travels through thin plates, with charac-
teristics such as low attenuation and the capability to cover substantial distances [16–18].
The generation of LWs can be categorized into two primary techniques: direct-contact
methods [19–23] and non-contact ones [24–28]. There are various approaches for receiving
LW signals. Yu et al. utilized piezoelectric wafer active sensors to both generate and
receive LWs propagating within a plate-like structure [29]. Paul Wilcox et al. employed
electromagnetic acoustic transducers to produce and collect LWs in steel and aluminum
plates with thicknesses from 5 to 10 mm [30]. Air-coupled sensors are also utilized to excite
and receive LWs in composite plates to achieve the baseline-free delamination inspection
technique of composite plates [31]. The fiber Bragg grating sensor is renowned for its
high sensitivity in detecting LWs [32]. However, these techniques require the detector and
sample to be in close proximity or in direct contact for receiving the LW. This would restrict
their applicability in remote or harsh environments. To address this constraint, Naoki
Hosoya et al. employed a scanning laser Doppler vibrometer to detect LWs induced via
laser on an aluminum plate [33]. Additionally, a two-wave mixing interferometer was used
to detect ultrasound and characterize the grain-size defect distribution of aluminum [34].

The primary methods for processing LW signals involve time-domain, frequency-
domain, and time-frequency domain analysis. The time-domain method is characterized
by its simplicity and intuitiveness, but it is susceptible to environmental interference and de-
mands a strict experimental condition. Frequency-domain analysis is a straightforward and
effective method, particularly for dealing with extensively damaged specimens. However,
a LW as a transient signal exhibits dispersion characteristics and displays non-stationary
features. Consequently, it is crucial to understand the frequency-domain characteristics of
the LW signal at different times for defect detection. Furthermore, time-frequency domain
analysis has been proposed to retrieve more accurate and comprehensive information. The
time-frequency domain method frequently utilizes techniques such as short-time Fourier
transform (STFT), wavelet transform, Hilbert-Huang transform (HHT), Wigner-Ville Distri-
bution (WVD) and Cohen Class Distributions [35–38]. STFT exhibits limited time resolution
due to its fixed window width. A broader window enhances frequency resolution but
diminishes time resolution, while a narrower window improves time resolution at the
expense of frequency resolution [39]. Although the HHT shows promise as a valuable tool
for extracting features from non-stationary signals, it encounters challenges in system iden-
tification due to the generation of spurious modes and susceptibility to mode mixing [40].
Conversely, the computational complexity of the WVD renders it impractical for large
datasets due to its complexity [38]. Cohen Class Distributions may introduce cross-term
interference, particularly problematic when analyzing multi-component signals [38]. Com-
paratively, the continuous wavelet transform (CWT) offers excellent resolution in both the
time and frequency domains. Utilizing the complex Morlet wavelet provides the precise measurement of frequency localization for signals with both fast and slow oscillations. This adaptability is achieved through a flexible window that narrows for high frequencies and widens for a low-frequency [41].

This work presents a laser ultrasonic inspection system based on an all-fiber heterodyne interferometer. A 3-D model of an H62 brass specimen was simulated by COMSOL Multiphysics software (version 6.0). In the simulation, a LW was generated by a pulsed laser, and the transmitted and reflected wave signals were investigated by the spatial-temporal wavefield. The CWT was employed to seek the optimum frequency of the LW with maximum energy. In the experiment, the displacement of receiving spots was observed with a time resolution of 1 ns. A comparison test was carried out for both a defect-free sample and a defect sample. The frequency component at 370 kHz was extracted to discern the defects. Both the location and width of defects were determined through the time difference of the reflected and transmitted signals, respectively.

## 2. Finite Element Method

### 2.1. Material Parameters

A three-dimensional model for ultrasonic wave inspection was established using the simulation software COMSOL Multiphysics. The simulation of the ultrasonic wave was generated by a pulsed laser on a specimen corresponding to the LW. The simulating sample was copper, characterized as a linear elastic material with the same size as the testing specimen.

The copper plate specimen has dimensions of 250 mm × 250 mm × 0.5 mm. To simulate surface defects on the copper plate, a groove is machined on the surface, as depicted in Figure 1. For comparisons, a defect-free copper plate is labeled as P1, and a copper plate with a defect is designated as P2 with grooves of 20 mm × 2 mm × 0.2 mm. The laser focal point is fixed in the experiment, while the receiving spot moves in parallel with a step size of 2 mm. The distance from the laser focus to the receiving spot increases from 20 mm to 100 mm. The material properties are listed in Table 1.

<figure><img src="image_4.png" /><figcaption>Figure 1. The tested copper plate. (a) Defect-free sample P1. (b) Defect sample P2.</figcaption></figure>
<table><caption>**Table 1.** Elastic parameters of H62 brass.</caption><thead><tr><td>Material</td><td>Mass Density (kg/m³)</td><td>Young's Modulus (GPa)</td><td>Poisson's Ratio</td></tr></thead><tbody><tr><td>H62 brass</td><td>8390</td><td>105</td><td>0.346</td></tr></tbody></table>

Low reflection boundary conditions are implemented to mitigate the boundary reflection and ensure accurate wave propagation modeling. This approach minimizes wave reflection at boundaries, allowing for the isolation and analysis of the primary surface. The pulsed laser excitation is treated as a boundary condition loaded on the surface of the material. This boundary condition includes both the thermal effect of the laser and the temporal and spatial distribution functions of the laser pulse. The thermal effect is simulated via heat equation [42–44].

## 2.2. Displacement Field Analysis

As shown in Figure 2, the number of oscillations in the wavefield signal over time rises with increasing laser focus-receiving spot distance. This observation indicates the separation of frequency components and the emergence of distinct propagation patterns. The broad frequency spectrum of the laser-generated LW leads to distinct propagation patterns dependent on the excitation-reception distance. At close proximity, the limited propagation distance results in overlapping frequency components, forming a composite vibration pattern. Nonetheless, the various frequency components begin to separate gradually with the distance increase between excitation and reception points, revealing their unique propagation characteristics.

<figure><img src="image_5.png" /><figcaption>**Figure 2.** Laser LW spatial-temporal wavefield. (a) Defect-free copper plate P1. (b) Defect copper plate P2.</figcaption></figure>

LW signals exhibit a distinct frequency-dependent propagation pattern. At a given location, high frequency components arrive first, followed by the lower-frequency components carrying more energy. This sequential arrival stems from the inherent composition of laser-generated LW signals, which are primarily low-frequency. Additionally, the perpendicular orientation of the receiving beam to the plate enhances its sensitivity to out-of-plane LW displacements, further increasing the prominence of low frequency $A_0$ mode components in the received signal [45]. The observed wavefield signal characterizes low energy and fast wave speed for high-frequency components, and high energy and slow wave speed for low-frequency components. It aligns with the theoretical prediction $A_0$ mode varying with frequencies. With comparisons of Figure 2a,b, spatial-temporal wave field signal analysis reveals the distinct reflection and transmission of the incident LW at the
defect site. CWT is implemented to analyze the laser-generated LW signals for further extraction of the defect characteristics.

As shown in Figure 3, a time-frequency analysis is conducted through CWT. The Morlet wavelet is chosen as the mother wavelet. The LW spectrum primarily distributes in the range of 0 to 2 MHz. It is important to note that higher-order modes have not been detected within this frequency range. In Figure 3a, the time-frequency representation demonstrates a strong resemblance to the theoretical curve of the A₀ mode. An energy peak is evident, occurring at 24.5 µs. In Figure 3b, the time-frequency representation is generated by the LW displacement from 0 to 15 µs based on CWT. A distinct signal associated with the S₀ mode displays around 1.5 MHz, which can be found in Figure 3c. The energy with respect to the defect is located at approximately 370 kHz, which corresponds to maximum intensity [28]. It is noteworthy that the time-frequency analysis lacks the precise spatial resolution for defect localization [46].

<figure><img src="image_6.png" /><figcaption>**Figure 3.** Time-frequency graph after CWT at a laser focus-receiving spot distance of 40 mm. (a) Copper plate P1. (b) Copper plate P1 at 0–15 µs. (c) Copper plate P2.</figcaption></figure>

## 2.3. Lamb Wave Dispersion Characteristics

Dispersion curves of H62 brass are shown in Figure 4. The dispersion curves show that at frequency thickness lower than 1 MHz-mm, only the fundamental A₀ and S₀ Lamb modes exist. When frequency thickness goes higher, more LW modes (such as A₁, A₂, S₁ and S₂) appear. The velocities of most modes have a high dependence on frequency. Therefore, in the non-destructive testing of Lamb, small frequency thickness should be used for detection.

<figure><img src="image_7.png" /><figcaption>**Figure 4.** Dispersion curves of the H62 brass. (a) Group velocity dispersion curves. (b) Phase velocity dispersion curves.</figcaption></figure>
### 3. Experiment Setup

As illustrated in Figure 5, the experimental setup consists of the laser ultrasonic generation and detection system, which includes an excited pulse laser, an all-optical fiber heterodyne interferometer for LW detection, and a scanning subsystem. The Nd: YAG laser (Quantel, Ultra, 1064 nm, 6 ns, Les Ulis Cedex, France) irradiates the surface of the H62 brass sample. Simultaneously, the laser controller generates a signal to trigger the oscilloscope and synchronize the laser heterodyne interferometer. For the laser heterodyne interferometer, a continuous wave fiber laser (Precilasers, FL-SF-1550-S, Shanghai, China) is divided into two beams via a fiber beam splitter (1:3). One beam serves as the reference light, passing through the acousto-optic modulator at 80 MHz (Qingjin, G-1550-80-L-B-TAA-A-Y-L, Shanghai, China). The remaining beam (75%) is directed onto the surface of the copper plate, and part of it is reflected back by the sample surface. The reflected beam carrying the ultrasonic signal is collected by a reflective collimator (Thorlabs, RC02APC-P01, NJ, USA) [47,48]. Then, it is transmitted to the optical circulator and combined with the reference laser by a 2 × 1 (50/50) fiber coupler onto a balanced amplified photodetector (Thorlabs, PDB450C-AC). When the two signals are combined, their frequencies mix, and the output beat signals of the photodetector are digitally displayed and stored by the oscilloscope (SIGLENT SDS2504X Plus, Shenzhen, Guangzhou, China). For precise and automated scanning, the collimator is mounted on a 3D-stage equipped with stepper motors. Its position can be adjusted by using a computer.

<figure><img src="image_8.png" /><figcaption>**Figure 5.** Experimental setup of laser ultrasonic generation and detection system.</figcaption></figure>

During the experiment, the laser's single pulse energy is set to 50 mJ. This setting ensure effective excitation of ultrasonic signals through the thermoelastic mechanism and guarantees the integrity of the copper plate [49]. Thirty-two pulses of repetition were averaged at the same location to improve the signal-to-noise ratio. These ultrasonic signals acquired via digital oscilloscope were processed by custom-written MATLAB software (version 2021a). IQ demodulation is used to extract the ultrasonic signal and generate time-resolved surface displacement resulting from the propagation of LWs [50,51]. Subsequently, the displacement was analyzed in both the time and frequency domains. The time resolution can achieve 1 ns. In the experimental samples, five samples with different defect widths were selected, with widths of 2 mm, 4 mm, 5 mm, 6 mm, and 8 mm,
respectively. Their positional dimensions are the same as those shown in Figure 2b. The
distance between the laser focus and the left side of the defect is 50 mm.

4. Results and Discussion

LW time-domain signals are presented in Figure 6. This demonstrates the evident
displacement with respect to the dispersion characteristic [52]. As plotted in Figure 6a, the
displacement amplitude is low between 0 µs and 20 µs. From 20 µs to 100 µs, displacement
amplitude increases gradually. Around 10 µs, the S₀ mode was not observed. The S₀
mode is primarily in in-plane displacement, with minor displacement perpendicular to
the surface. Therefore, it could be measured by laser interferometer. The A₀ mode is
evident from the prominent dispersion observed in Figure 6a. The displacement at a laser
focus-receiving spot distance of 40 mm for plates P1 and P2 is synchronized in Figure 6a,
whereby a noticeable time delay occurs at a laser focus-receiving spot distance of 60 mm in
Figure 6b. This reveals no significant displacement variation on the P2 plate attributed to
the reflection of the defect signal, so it is difficult to recognize defects by LW displacement.
Nevertheless, this does not imply that the reflected signal has not been generated due to a
defect. Further analysis of the LW signal in the time domain is imperative for extracting
the defect signal. Figure 6c,d depicts the LW time-domain signals simulated using FEM. S₀
mode and A₀ mode can be found. These FEM results are consistent with the corresponding
experimental results, thus confirming the accuracy of the experimental findings.

<figure><img src="image_9.png" /><figcaption>**Figure 6.** LW time-domain signal. (a) Experiment results at a laser focus-receiving spot distance of 40 mm. (b) Experiment results at a laser focus-receiving spot distance of 60 mm. (c) FEM simulations at a laser focus-receiving spot distance of 40 mm. (d) FEM simulations at a laser focus-receiving spot distance of 60 mm.</figcaption></figure>
To effectively derive the defect characterization, a frequency of 370 kHz is extracted from the wavelet coefficient spectra of the signals for both the defect-free and defect sample. LW signals are analyzed using CWT, as shown in Figure 7. The direct waves are the same in both P1 and P2 before passing the defect. Therefore, this enables the identification of the location of defect via the presence of the reflected wave. The Hilbert transform is utilized to extract the envelope of the LW. When the envelope amplitude reaches its maximum value, it indicates the time of arrival of Lamb waves at the receiving spot. According to theory, the group velocity of the $A_0$ mode at 370 kHz is 1747.1 m/s in the copper plate. In the experiment, the average velocity of the direct wave is 1756.7 m/s, while the average velocity of the reflected wave is 1759.6 m/s. The velocity error is only 0.94%. Based on the experimental results, the specific location of the defect is identified at 50.08 mm. The propagation distance and defect location are determined through a single frequency. In Figure 7b, the direct wave $A_0$ mode discrepancy is observed in both P1 and P2. This is because of the interaction of the LW and defect, and it induces changes in both their paths and modes. Consequently, the waveforms no longer align or overlap. Therefore, the transmitted signals, compared to the reflection signals of the LW, demand more complex processing. Figure 7c,d depicts the LW signal of 370 kHz extracted by CWT simulated using FEM. These FEM results are consistent with the corresponding experimental results, and they are not affected by noise interference.

<figure><img src="image_10.png" /><figcaption>**Figure 7.** LW signal of 370 kHz extracted by CWT. (a) Experiment results at a laser focus-receiving spot distance of 40 mm. (b) Experiment results at a laser focus-receiving spot distance of 60 mm. (c) FEM simulations at a laser focus-receiving spot distance of 40 mm. (d) FEM simulations at a laser focus-receiving spot distance of 60 mm.</figcaption></figure>

The relative error of the defect measured at various laser focus-receiving spot distances is plotted in Figure 8. It varies for determining the defect wave when the receiving point is close to the defect. Therefore, six measuring points were selected to improve the accuracy,
and the average error is reduced to 0.14%. The minimum error is derived at a distance of 12 mm from the defect, and the largest one is obtained at a distance of 14 mm. This indicates the feasibility of determining the defect location using the reflection signals of the defect.

<figure><img src="image_11.png" /><figcaption>Figure 8. Defect errors at various laser focus-receiving spot distances.</figcaption></figure>

The correlation between defect width and LW transmission time was established through analysis of the LW transmission time across various defects. In Figure 9, various defect widths are depicted, ranging from defect free to widths of 2 mm, 4 mm, 6 mm, and 8 mm. Receiving spots were positioned at intervals of 60 mm, 70 mm, 80 mm, 90 mm, and 100 mm from the laser focus. The time difference of the LW is proportional to the increase in defect width, as displayed in Figure 9. The time differences are the same on different defects regardless of the spatial orientation of the receiving point. It implies that the propagation time of the LW remains uniform across the range of defects.

<figure><img src="image_12.png" /><figcaption>Figure 9. The relationship between LW transmitted signal and defect size. (a) FEM at a laser focus-receiving spot distance of 70 mm. (b) Experiment at a laser focus-receiving spot distance of 70 mm.</figcaption></figure>

The relationships between the LW transmitted signal and defect size are presented in Figure 9. There is a downturn of LW displacement with defect width, causing a delay in received time. This phenomenon is attributed to both energy dissipation of LWs traversing
the defects and a reduction in the velocity of the A₀ mode. Additionally, the waveform of the LW passing through the defect undergoes changes and causes the time fluctuations of the received signal. A linear fitting analysis was conducted to describe the variations in defect width against the time difference. The linear fit, represented in Figure 10, shows the relationship between defect width and time difference. The equations of the fitted line for FEM and experimental ones are denoted, respectively:

$$y = 0.246 x + 0.0474, \qquad (1)$$

$$y = 0.244 x + 0.0723, \qquad (2)$$

<figure><img src="image_13.png" /><figcaption>Figure 10. The relationships between LW transmitted signal and defect size derived by experiments and FEM.</figcaption></figure>

Here, y is the time variation caused by the defect, and x represents the defect width. This can quantitatively characterize defects of different widths based on the equation of the fitted line. With a given detection distance, the defect width can be determined by measuring the travel time of the LW.

A defect width of 5 mm was employed to verify the method. The predicted time difference for a defect width of 5 mm is 1.276 µs according to Equation (1). In the FEM, the time difference is 1.28 µs for a 5 mm defect width. The error is 0.011 mm, corresponding to a relative error of 0.211%. The predicted time variation for a defect width of 5 mm is 1.170 µs according to Equation (2). In the experiment, the actual time difference is 1.196 µs for a 5 mm defect, resulting in a measurement error of 0.395 mm. This demonstrates the feasibility of this method for measurements of defect width.

## 5. Conclusions

A laser ultrasonic defect inspection system was developed in combination with the all-fiber heterodyne interferometer. It could detect LWs with high temporal and spatial resolution. The LW spatial-temporal wavefield of H62 brass was obtained by using the COMSOL Multiphysics software. The A₀ mode with 370 kHz is sensitive to defect detection due to its vibrational direction and maximum energy. The size and location of defects are determined by the time difference of the transmitted wave and reflected wave, respectively. This demonstrates that the average error of defect position is 0.14% through travel time in experiments on six different receiving spots. The width of the defect is linear to the time difference of the transmitted wave, and the error can achieve 0.395 mm for a 5 mm width of defect. The observed results are consistent with those from FEM. Therefore, this validates that the feasibility of the technique can be utilized in the defect detection of thin plates.
**Author Contributions:** Conceptualization, C.L.; methodology, T.G., X.Q. and C.L.; software, X.W., T.G. and X.H.; validation, X.W. and H.C.; formal analysis, Z.Z. and X.S.; investigation, G.G. and X.S.; resources, C.L.; data curation, X.W. and Z.Z.; writing—original draft preparation, X.W.; writing—review and editing, X.W., Y.T., Y.Z., C.F. and C.L.; supervision, G.G., X.Q. and H.C.; project administration, G.G.; funding acquisition, X.S., T.G., Y.T., X.Q. and C.L. All authors have read and agreed to the published version of the manuscript.

**Funding:** The study is supported by the National Key Research and Development Program of China (Number: 2023YFF0718100), National Natural Science Foundation of China (Grant/Award Number: 52076145 and 12304403); special fund for Science and Technology Innovation Teams of Shanxi Province (Number: 202304051001034); Fund Program for the Scientific Activities of Selected Returned Overseas Professionals in Shanxi Province (Number: 20230031); Shanxi Scholarship Council of China (Number: 2023-151); Fundamental Research Program of Shanxi Province (Number: 202303021221147, 202203021222204 and 202303021212224); Dreams Foundation of Jianghuai Advance Technology Center (2023-ZM01C002); Taiyuan University of Science and Technology Scientific Research Initial Funding (20222121), Shanxi Province Scientific Research Initial Funding (20232033), Key Research and Development Program of Shanxi Province of China (202302150101017).

**Institutional Review Board Statement:** Not applicable.

**Informed Consent Statement:** Not applicable.

**Data Availability Statement:** The raw data supporting the conclusion of this article will be made available by the authors, without undue reservation.

**Conflicts of Interest:** The authors declare no conflicts of interest.

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