Probability weighted fourpoint arc imaging algorithm for timereversed lamb wave damage detection
Shuhao Cao^{1} , Yu Lu^{2} , Hanfei Zhang^{3} , Qingwei Xia^{4} , Yanyan Liu^{5} , Shiwei Ma^{6}
^{1, 2, 3, 4, 5, 6}Shanghai University, Shanghai, China
^{6}Corresponding author
Vibroengineering PROCEDIA, Vol. 22, 2019, p. 2530.
https://doi.org/10.21595/vp.2018.20467
Received 21 December 2018; accepted 28 December 2018; published 15 March 2019
36th International Conference on Vibroengineering in Dubai, United Arab Emirates, March 1517th, 2019
Damage imaging based on scattering signals of ultrasonic Lamb waves in plate structure is considered as one of the most effective ways for structural health monitoring area. To improve location accuracy and reduce the impact of artifacts, a probability weighted fourpoint arc imaging algorithm for time reversal Lamb wave damage detection is proposed in this paper. By taking the defect as a secondary wave source, the fourpoint arc positioning method is used to calculate the propagation time of the signal from transducer to defect. And the amplitude of damage signal corresponding to the time of flight is used for imaging. In order to eliminate the artifacts, a damage probability weighting is combined with fourpoint circular arc imaging algorithm. The effectiveness of the proposed method is experimentally verified in aluminum plate. Experimental results indicate that damage location accuracy and imaging quality has been improved in both singleflaw and doubleflaw samples compared with conventional delayandsum method.
 Use the flight time of Lamb wave scattering signals to image the damages
 Combine the fourpoint arc imaging method and damage index probability imaging together
 Time reversal method is used to refocus energy and increase signaltonoise ratio
 Our algorithm has been verified through the experiment on aluminum plates
Keywords: damage index probability, weighted fourpoint arc location, time reversal.
1. Introduction
Structural health monitoring (SHM) has been a considerable research area for material integrity nondestructive inspecting. In this area, structure interrogation using Lamb wave can be done with transducers fixed on plate surface, which is convenient in practical applications. It is of great significance to quality inspections of industry products, especially in the plate like structure detection [13].
Lamb wave can spread between two surfaces of plate structure and scatter at the flaw. The defect information is acquired from the received signals which are collected by ultrasonic transducers fixed on the plate. Through imaging methods, the defect position is shown after processing the received signals. Wang et al. [4] proposed a delayandsum (DAS) algorithm which effectively imaged the received signals, but it made artifacts in the case of multiple defects. Sohn et al. [5] explored the correlation between the damage condition and the similarity of the reconstruct and excitation signal, and proposed the concept of damage index (DI) to characterize the severity of defect without baseline signal. Zenghua Liu et al. [6] yield a baselinefree detection method combined with the modified damage imaging algorithm based on the time reversal method. Xin Li et al. [7] proposed an acoustic emission source locating method based on time reversal theory by using fourpoint arc location algorithm. The efficiency of this methodology had been verified through experiments, and results showed the enhancement of damage signal energy. But the artifacts can be produced through this method.
In our paper, a new probability weighted algorithm based on the fourpoint arc location method is proposed. The new algorithm has been verified by the experiment, and the position of damage can be shown accurately through time reversal reconstruction signal in the detected area.
2. Principle of fourpoint arc location method
Fourpoint arc location algorithm is an active damage monitoring method [8]. Supposing four transducers are fixed in the four corners of a squire measured area in a plate, if the time of arriving at the receivers is known, the time of arriving at the flaw, ${t}_{s}$, can be calculated by Eq. (1):
where (${x}_{s}$, ${y}_{s}$) is the defect coordinate, (${x}_{1}$, ${y}_{1}$) is the first transducer coordinate, $v$ is the structure wave velocity, and ${t}_{1}$ is the time of the signal arriving at the first transducer. (${x}_{2}$, ${y}_{2}$), (${x}_{3}$, ${y}_{3}$), (${x}_{4}$, ${y}_{4}$), ${t}_{2}$, ${t}_{3}$ and ${t}_{4}$ are similar defined. The flaw position and the time of arrival at the defect can be calculated by solving the equations. The principle of fourpoint arc location method is shown in Fig. 1(a), where A is the damage point. And then, the received signal can get imaged referring to the calculation results as shown in Eq. (2):
where ${S}_{ij}$ is the damage imaging value of the position ($i$, $j$), $N$ is the number of the signal, ${A}_{n}$ is a coefficient for balancing the transducers’ output, ${R}_{ijn}$ is the distance of transducer (${x}_{n}$, ${y}_{n}$) and measure point ($i$, $j$) and ${f}_{v}$ is image resolution. The defect is seen as an acoustic secondary source according to the time ${t}_{s}$. The schematic of the imaging method is presented in Fig. 1(b).
Fig. 1. Illustration of fourpoint arc imaging method
a) Location schematic
b) Imaging principle
3. Proposed method
3.1. Damage index probability imaging
The time reversal method is an application of the acoustic reciprocity principle, which can effectively reconstruct the sound source signal [9]. After the time reversal process, the received signal, should have the same shape with the original one, which is called signal reconstruction.
Referring to the time reversal theory, if certain kinds of defects present, the linear reciprocity property will break down, making the reconstructed signal deviate from the input original signal [5]. Due to this property, the damage index is introduced to quantify the deviation of the two signals [10]. Damage index is calculated by Eq. (3):
where $n$ denotes the $n$th damage sensing path, ${t}_{0}$, ${t}_{1}$ are the signal time of beginning and ending. The defect probability $P$ at a specific position ($x$, $y$) is defined by Eq. (4) as follows:
where ${W}_{n}\left[{R}_{n}\left(x,y\right)\right]$ is the probability distribution. Sheen et al. [11] indicated that the longer distance from damage to sensing path related smaller damage index. The distribution function is:
where $\beta $ is a sensing area parameter of a certain path. In this paper, $\beta =$ 0.05. And:
where ${d}_{An}$ is the distance from ($x$, $y$) to the actuator in the $n$th sensing path. Similarly, ${d}_{Rn}$ is the distance to the receiver. And ${d}_{n}$ is the distance of the actuator and receiver. The distribution function gives the relationship between damage probability and measured position.
3.2. Damage probability weighted fourpoint arc imaging
The fourpoint arc location method has better position accuracy than the damage index weighted method, however the artifacts may produce owing to the algorithm limitation. While the probability method creates no artifacts, but it has limited location capability. In order to make full use of the defect information and acquire better imaging quality, a new weighted algorithm based on the fourpoint arc location method and the damage index probability method is presented. According to Eq. (4)(6), this new weighted imaging algorithm is explained by Eq. (7):
It is not difficult to see that Eq. (7) is the form of probability expectation. And the full summation method is used to obtain the imaging result after each of the expectation term is calculated. Under the influence of the probabilities, image of the measured area is limited by the damage probability distribution, which reduces error of the damage location. The new weighted method combines the advantages of both methods. By adding the part of probability weight, the image quality of the fourpoint arc imaging algorithm is improved and the image value of artifact pixel is reduced. Besides, the defects can be located more accurately.
4. Experiments
4.1. Experimental setup
The experimental system consists of a personal computer, an arbitrary waveform signal generator (Agilent 33520A), an active signal amplifier based on the TI op amp chip OPA657, and a fourchannel oscilloscope (Tektronix DPO5034B). The experimental setup is shown in Fig. 2. The excitation signal is the normalized five period sinusoidal narrowband signal modulated by Hanning window. And the signal frequency is 500 kHz. The signals are excited and received by contacting ultrasonic oblique probes.
The test samples in this experiment are two 6061 aluminum plates, which are singleflaw and doubleflaw respectively. The defects are circle through hole with a diameter of 15 mm. The coordinate origin is the left bottom corner of the plate. As the Fig. 3(a) and Fig. 3(b) shows, the center coordinate of the single flaw is (550, 550) called D1, and the center coordinates of the double flaws are (450, 500) and (550, 550) called D1 and D2 respectively. During the imaging process, the measured area is divided into 400×400 = 160000 grids with the area of 2.5×2.5 mm^{2} for each one.
The transducers are placed as shown in the Fig. 3(c), in order to reduce the influence of boundary reflection. The black blocks denote the transducers, and the links between the blocks are the 10 sensing paths. The positions of the eight probes are ${S}_{1}$(250,250), ${S}_{2}$(500,250), ${S}_{3}$(750,250), ${S}_{4}$(500,750), ${S}_{5}$(750,750), ${S}_{6}$(750,500), ${S}_{7}$(750,250), ${S}_{8}$(500,250).
Fig. 2. Schematic illustration of experimental setup
a) Experimental system
b) Transducers placement
Fig. 3. Diagram of environmental sample plates
a) Single flaw sample
b) Double flaws sample
c) Sensing paths layout
4.2. Experiment processing and results
Using the experimental system above, a series of signal data related to each sensing path is obtained through the time reverse process. Then the damage index shown in Table 1 and Table 2 is calculated by Eq. (3) according to the time reversal signal. The result of the damage probability weighted fourpoint arc method is presented in Fig. 4(a) and Fig. 4(b). Note that white circles denote the defects acquired by the method and black circles indicate the actual defect locations. From the picture, the distance from the center of the defect acquired by the method to the real, D1, is 5 mm for the singleflaw plate; and in the doubleflaw sample, the distances from the algorithm acquired to the real are 17.50 mm for the D1 and 15.81 mm for the D2. Besides, the result of the timereverse delayandsum method is presented in Fig. 5(a) and Fig. 5(b). For single defect, the distance from the acquired to the real D1 is 19.04 mm; for the double damages, the distance from the acquired to the center of D1 and D2 are 29.15 mm and 34.00 mm respectively. From Fig. 5(a) and Fig. 5(b), the damage image is insufficiently precise to clearly find exact positions of the defects especially in doubledefect plate. While from the Fig. 4(a) and Fig. 4(b), the flaw locations are well captured with our new weighted method, and the contrast ratio of Fig. 4(b) is higher than the Fig. 5(b). Both in Fig. 4(a) and Fig. 4(b), the maximum image value pixel can indicate the defect position clearly, and the artifact is reduced in the twodefect case compared with the DAS method.
Table 1. Damage index of single flaw
Paths  ${\mathrm{S}}_{4}{\mathrm{S}}_{7}$  ${\mathrm{S}}_{1}{\mathrm{S}}_{5}$  ${\mathrm{S}}_{1}{\mathrm{S}}_{6}$  ${\mathrm{S}}_{3}{\mathrm{S}}_{6}$  ${\mathrm{S}}_{3}{\mathrm{S}}_{7}$ 
DI  0.1402  0.1336  0.1330  0.1287  0.1242 
Paths  ${\mathrm{S}}_{3}{\mathrm{S}}_{8}$  ${\mathrm{S}}_{2}{\mathrm{S}}_{5}$  ${\mathrm{S}}_{1}{\mathrm{S}}_{4}$  ${\mathrm{S}}_{2}{\mathrm{S}}_{7}$  ${\mathrm{S}}_{5}{\mathrm{S}}_{8}$ 
DI  0.1212  0.1202  0.1189  0.1160  0.1010 
Table 2. Damage index of double flaws
Paths  ${S}_{4}{S}_{7}$  ${S}_{1}{S}_{5}$  ${S}_{3}{S}_{7}$  ${S}_{1}{S}_{4}$  ${S}_{3}{S}_{6}$ 
DI  0.1695  0.1450  0.1429  0.1386  0.1322 
Paths  ${S}_{3}{S}_{8}$  ${S}_{1}{S}_{6}$  ${S}_{2}{S}_{7}$  ${S}_{2}{S}_{5}$  ${S}_{5}{S}_{8}$ 
DI  0.1299  0.1228  0.1192  0.1167  0.1129 
Fig. 4. Imaging results of weighted fourpoint arc method
a) Weighted method in singleflaw sample
b) Weighted method in doubleflaw sample
Fig. 5. Imaging results of das method
a) DAS in singleflaw sample
b) DAS in doubleflaw sample
Fig. 6. Thresholder results of weighted method
a) Weighted method in singleflaw sample
b) Weighted method in doubleflaw sample
The location error of the two imaging methods is presented in Table 3 for comparison purpose. As the data in the table shows, it can be seen that the location accuracy of the weighted fourpoint arc imaging method is higher than the timereversal DAS method. To facilitate observation, the image is intercepted with the threshold of the 70 % peak value. The thresholder image is shown in Fig. 6. The damage location and area detected by imaging generally match the actual damage situation. The error may produce due to the inaccuracy of group velocity, and the damage index measurement of the sensing paths. It can be limited further by more accurate velocity measurement and improved damage probability method.
Table 3. Error of two algorithms
Defects  Single defect  Double defects  
Algorithm  D1  D1  D2 
Weighted 4point arc  5.00 mm  17.50 mm  15.81 mm 
Delayandsum  19.04 mm  29.15 mm  34.00 mm 
5. Conclusions
The proposed method combines the advantages of fourpoint arc location algorithm and the damage index probability method. The time reversal process is done for the purpose of focusing the energy of the scatters, and damage index is acquired by calculating the deviation of reconstruction and original signal. Experimental result shows that the method have better location accuracy and more precise defect imaging area compared with the typical delayandsum method, which validates the efficiency of the proposed method. In future works, the velocity of the wave can be measured better, and the weight method can be also modified to achieve better performance.
Acknowledgements
This work was supported by the National Natural Science Foundation of China with Grant No. 61671285.
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