Defects Inspection in Wires by Nonlinear Ultrasonic-Guided Wave Generated by Electromagnetic Sensors

Steel wires are widely used as raw materials for spring valves in engines. Considering the quality and safety issues of their structure, there is a demand to develop nondestructive inspection approaches to detect initial damages in steel. In this study, nonlinear ultrasonic-guided waves generated by an electromagnetic acoustic transducer (EMAT) were used to inspect the defects in steel wires. As one of the noncontact testing methods, the use of EMAT has significant advantages to decrease the nonlinearity induced by instruments and transducer contact condition. The principles of design and manufacturing of EMAT are first introduced. The fundamental theory of nonlinear guided waves is also briefly discussed in this investigation. Phase-matched guided wave modes were generated and measured by using EMAT. Variations of acoustic nonlinearity corresponding to existing defects in specimens were obtained. A scanning electron microscope (SEM) was used to check the existence of microdefects in specimen. The results indicate that the use of EMAT can be an effective means to generate and measure nonlinear ultrasonic-guided waves for inspection of microdefects.


Introduction
Steel wire rods are used as raw materials for various mechanical components. This research can be applied to the steel wires, raw material of valve springs and have an influence on keeping smooth cycle motion in a gasoline engine. Under periodic fatigue state, failure of spring valves may occur before expectation of fatigue failure. Therefore, we need a reliable method for steel wires that can evaluate microdefects or early stage damage detection. Up to now, for the research work related with this study not so many articles were published. Gao et al. developed nondestructive evaluation (NDE) techniques using magnetic flux for macro defect [1].
The geometric shape of steel wires before processing of valve springs is cylindrical such as rod and solid shaft. Considering shape characteristics, guided waves have been applied to efficiently inspect long specimens such as wire rods. Research on guided ultrasound has been going on for a long time, but it has not progressed actively due to the complexity of theory and the variety of wave modes.
where a is the wave propagation distance and f is a frequency independent function. In addition, the ratio A 2 /A 2 1 with the relative acoustic nonlinear parameter β applied in this research is considered as a measure of acoustic nonlinearity, where A 1 and A 2 are the measured amplitudes of the fundamental and second harmonics.
The relative acoustic nonlinear parameter increases linearly as a function of propagation distance. The cumulative effect of the second harmonic amplitude is a great advantage for detection in experiment. It is found that second harmonic amplitude linearly grows with propagation distance, when there are synchronism and nonzero power flux. If the wave mode chosen satisfies these two conditions, the second harmonic amplitude will be cumulative. Even a series of double frequency wave components will be generated by the driving sources of nonlinearity. In practice, interest is focused on the second harmonic generation with the cumulative effect, since the cumulative second harmonic wave plays a dominant role after second harmonics propagating some distance. Figure 1a,b shows the typical waveform of the received signal and its spectrum. The received time domain signal is processed in the frequency domain with the fast Fourier transform (FFT) to obtain its spectrum. Figure 1b shows the fundamental frequency and the second harmonic.
Appl. Sci. 2020, 10, x 3 of 15 Where a is the wave propagation distance and f is a frequency independent function. In addition, the ratio 2 2 1 / A A with the relative acoustic nonlinear parameter ' β applied in this research is considered as a measure of acoustic nonlinearity, where 1 A and 2 A are the measured amplitudes of the fundamental and second harmonics.
The relative acoustic nonlinear parameter increases linearly as a function of propagation distance. The cumulative effect of the second harmonic amplitude is a great advantage for detection in experiment. It is found that second harmonic amplitude linearly grows with propagation distance, when there are synchronism and nonzero power flux. If the wave mode chosen satisfies these two conditions, the second harmonic amplitude will be cumulative. Even a series of double frequency wave components will be generated by the driving sources of nonlinearity. In practice, interest is focused on the second harmonic generation with the cumulative effect, since the cumulative second harmonic wave plays a dominant role after second harmonics propagating some distance. Figure 1a,b shows the typical waveform of the received signal and its spectrum. The received time domain signal is processed in the frequency domain with the fast Fourier transform (FFT) to obtain its spectrum. Figure 1b shows the fundamental frequency and the second harmonic.  (1) and (2), the normalized nonlinear parameter can be calculated with Equation (2) by using the amplitudes of the fundamental and the second harmonic modes. Figure 2 shows the nonlinear parameters according to the propagation distance. The cumulative effect means that the nonlinearity increases with distance under certain frequency conditions. The double frequency mode which satisfies a specific condition such as the expression shown in the diagram is selected based on the frequency.  (1) and (2), the normalized nonlinear parameter can be calculated with Equation (2) by using the amplitudes of the fundamental and the second harmonic modes. Figure 2 shows the nonlinear parameters according to the propagation distance. The cumulative effect means that the nonlinearity increases with distance under certain frequency conditions. The double frequency mode which satisfies a specific condition such as the expression shown in the diagram is selected based on the frequency. Appl. Sci. 2020, 10, x 4 of 15

EMAT
EMAT is composed of a generating coil for generating an eddy current of the electromagnet and the transmission and a receiving detecting coil. When the probe is approached to the metal specimen, the inside of the specimen is affected by the electromagnet. As Shown in Figure 3, the eddy current is formed on the surface of the specimen by an alternating current flowing in the generating coil inside the probe. Lorentz force is generated between the eddy current and the low power line, and mechanical displacement occurs on the surface of the specimen. This mechanical displacement is called ultrasound. The purpose of this study was to investigate the nonlinearity of materials by inducing an ultrasonic wave in the longitudinal mode in steel wire rod. The permanent magnet was magnetically biased in the axial direction on the specimen. Then, when the coil was wound in the circumferential direction and the current was applied, the longitudinal mode of the guided ultrasonic wave was generated in the cylindrical structure such as the pipe or the wire rod.
EMAT was generated by Lorentz force effect in meander coil. The alternative current induce in the coil and the magnetic field is built in coil by high-power permanent magnet. Here J is eddy currents field and Β is the magnetic field. The Lorentz force is generated by the eddy currents and magnetic field As shown in Figure 4, the geometry used for describing the reception of EMAT is considering various factors. Equation (3) explain the relationship between magnetic field and eddy current. The influence of magnetic field for inducing eddy current is indicated by Equations (4) and (5). Produce a voltage pick up by receiving coil is Equation (6). EMAT does not require a contact medium in flaw detection. As a noncontact method using electromagnetic, it shows higher performance than PZT for

EMAT
EMAT is composed of a generating coil for generating an eddy current of the electromagnet and the transmission and a receiving detecting coil. When the probe is approached to the metal specimen, the inside of the specimen is affected by the electromagnet. As Shown in Figure 3, the eddy current is formed on the surface of the specimen by an alternating current flowing in the generating coil inside the probe. Lorentz force is generated between the eddy current and the low power line, and mechanical displacement occurs on the surface of the specimen. This mechanical displacement is called ultrasound.

EMAT
EMAT is composed of a generating coil for generating an eddy current of the electromagnet and the transmission and a receiving detecting coil. When the probe is approached to the metal specimen, the inside of the specimen is affected by the electromagnet. As Shown in Figure 3, the eddy current is formed on the surface of the specimen by an alternating current flowing in the generating coil inside the probe. Lorentz force is generated between the eddy current and the low power line, and mechanical displacement occurs on the surface of the specimen. This mechanical displacement is called ultrasound. The purpose of this study was to investigate the nonlinearity of materials by inducing an ultrasonic wave in the longitudinal mode in steel wire rod. The permanent magnet was magnetically biased in the axial direction on the specimen. Then, when the coil was wound in the circumferential direction and the current was applied, the longitudinal mode of the guided ultrasonic wave was generated in the cylindrical structure such as the pipe or the wire rod.
EMAT was generated by Lorentz force effect in meander coil. The alternative current induce in the coil and the magnetic field is built in coil by high-power permanent magnet. Here J is eddy currents field and Β is the magnetic field. The Lorentz force is generated by the eddy currents and magnetic field As shown in Figure 4, the geometry used for describing the reception of EMAT is considering various factors. Equation (3) explain the relationship between magnetic field and eddy current. The influence of magnetic field for inducing eddy current is indicated by Equations (4) and (5). Produce a voltage pick up by receiving coil is Equation (6). EMAT does not require a contact medium in flaw detection. As a noncontact method using electromagnetic, it shows higher performance than PZT for The purpose of this study was to investigate the nonlinearity of materials by inducing an ultrasonic wave in the longitudinal mode in steel wire rod. The permanent magnet was magnetically biased in the axial direction on the specimen. Then, when the coil was wound in the circumferential direction and the current was applied, the longitudinal mode of the guided ultrasonic wave was generated in the cylindrical structure such as the pipe or the wire rod.
EMAT was generated by Lorentz force effect in meander coil. The alternative current induce in the coil and the magnetic field is built in coil by high-power permanent magnet. Here J is eddy currents field and B is the magnetic field. The Lorentz force is generated by the eddy currents and magnetic field As shown in Figure 4, the geometry used for describing the reception of EMAT is considering various factors. Equation (3) explain the relationship between magnetic field and eddy current. The influence of magnetic field for inducing eddy current is indicated by Equations (4) and (5). Produce a voltage pick up by receiving coil is Equation (6). EMAT does not require a contact medium in flaw detection. As a noncontact method using electromagnetic, it shows higher performance than PZT for measuring nonlinearity of materials. However, it should be considered that the receiving sensitivity is lower than PZT.
where ν is the velocity of particle vibration, B is the static magnetic field, σ is the conductivity of the test piece, E ed and J ed are the induced electric field and the induced eddy current sheet due to the particle vibration at the depth z ed respectively.
Appl. Sci. 2020, 10, x 5 of 15 measuring nonlinearity of materials. However, it should be considered that the receiving sensitivity is lower than PZT.
where ν is the velocity of particle vibration, Β is the static magnetic field, σ is the conductivity of the test piece, ed Ε and ed J are the induced electric field and the induced eddy current sheet due to the particle vibration at the depth ed z respectively.

Experiments
Three different kinds of specimens with total 9 samples were tested in this investigation. As shown in Figure 5, the size information of the three specimens was the same, but there were differences in material properties and tensile strength. Detailed information of the samples can be found in in Table 1.

Experiments
Three different kinds of specimens with total 9 samples were tested in this investigation. As shown in Figure 5, the size information of the three specimens was the same, but there were differences in material properties and tensile strength. Detailed information of the samples can be found in in Table 1.
Appl. Sci. 2020, 10, x 5 of 15 measuring nonlinearity of materials. However, it should be considered that the receiving sensitivity is lower than PZT.
where ν is the velocity of particle vibration, Β is the static magnetic field, σ is the conductivity of the test piece, ed Ε and ed J are the induced electric field and the induced eddy current sheet due to the particle vibration at the depth ed z respectively.

Experiments
Three different kinds of specimens with total 9 samples were tested in this investigation. As shown in Figure 5, the size information of the three specimens was the same, but there were differences in material properties and tensile strength. Detailed information of the samples can be found in in Table 1.    The frequency and modes were selected by frequency multiply wire thickness ( f × d). Phase matching must be performed through the dispersion curve. The conditions for generation of second harmonic in a cylindrical structure such as wire rod and pipe are as follows [13].
The power flux at the first harmonic should not be 0 in the second harmonic frequency range. ( f n sur f + f n vol 0) Phase and group velocities of the first and second harmonics should be the same through phase matching (k n * = 2k). Figure 6 shows the dispersion diagram of steel wire rod. It can be confirmed that the phase velocity and the group velocity were the same at 4 MHz · mm, which was a double frequency of 2 MHz · mm. Through this phase-matching, we could use a nonlinear guided wave technique. L 1 (f·d = 2 MHz·mm) and L 2 (f·d = 4 MHz·mm) were selected because the resulted of the L 1 and L 2 modes were clearer for the second harmonic component than the other modes. The frequency and modes were selected by frequency multiply wire thickness ( f d × ). Phase matching must be performed through the dispersion curve. The conditions for generation of second harmonic in a cylindrical structure such as wire rod and pipe are as follows [13].   EMAT was designed and manufactured through impedance and LC-matching. Impedance matching means to eliminate the phase difference by minimizing reflection or loss of input power by buffering impedance difference at input and output. Selecting the appropriate inductor and capacitor element values through Equation (7) and choosing the resonance frequency is called LC-matching. EMAT was designed and manufactured through impedance and LC-matching. Impedance matching means to eliminate the phase difference by minimizing reflection or loss of input power by buffering impedance difference at input and output. Selecting the appropriate inductor and capacitor element values through Equation (7) and choosing the resonance frequency is called LC-matching.
The frequency at which the imaginary part becomes 0 in the Equation (7) through matching between the inductor (L) and the capacitor (C) is called a resonance frequency. Figure 7 shows the resonance frequency due to LC-matching of the capacitor and the inductor.
The frequency at which the imaginary part becomes 0 in the Equation (7) through matching between the inductor (L) and the capacitor (C) is called a resonance frequency. Figure 7 shows the resonance frequency due to LC-matching of the capacitor and the inductor.
In order to realize the inductance in the ultrasonic generating coil, a long meander coil was used in a limited space. A resonant circuit was constructed to maximize current flow in the meander coil. Figure 8 shows a meander coil with a wavelength of 0.38 mm.   Figure 9 shows the impedance-matching EMAT transducer used in this study. The EMAT was manufactured at 1 MHz as shown in Figure 10   Experiments were conducted to investigate the behavior of nonlinear induced ultrasound. Figure 11 shows the experimental setup. The RITEC RAM-4000 was used as a tone-burst ultrasonic transmitter and receiver and it was processed by a pitch-catch method. In order to realize the inductance in the ultrasonic generating coil, a long meander coil was used in a limited space. A resonant circuit was constructed to maximize current flow in the meander coil. Figure 8 shows a meander coil with a wavelength of 0.38 mm.

Z R jwL jwC
The frequency at which the imaginary part becomes 0 in the Equation (7) through matching between the inductor (L) and the capacitor (C) is called a resonance frequency. Figure 7 shows the resonance frequency due to LC-matching of the capacitor and the inductor.
In order to realize the inductance in the ultrasonic generating coil, a long meander coil was used in a limited space. A resonant circuit was constructed to maximize current flow in the meander coil. Figure 8 shows a meander coil with a wavelength of 0.38 mm.   c f Practically, 5.82 mm cannot be applied to steel wire with a diameter of 3.2 mm. It can be applied with lower wavelength as / 2, / 4, / 8 λ λ λ . Since 0.38 mm is an approximate value of 1/16 of wavelength, EMAT was fabricated using 0.38-mm meander coil. Experiments were conducted to investigate the behavior of nonlinear induced ultrasound. Figure 11 shows the experimental setup. The RITEC RAM-4000 was used as a tone-burst ultrasonic transmitter and receiver and it was processed by a pitch-catch method.  Figure 9 shows the impedance-matching EMAT transducer used in this study. The EMAT was manufactured at 1 MHz as shown in Figure 10 and excited at 0.625 MHz. The wavelength (λ = 5.82 mm) of 1 MHz can be derived by substituting the desired frequency and longitudinal wave velocity (C L Steel = 5.82 mm/µs) in the steel into Equation (8).
Appl. Sci. 2020, 10, x 8 of 15     Practically, 5.82 mm cannot be applied to steel wire with a diameter of 3.2 mm. It can be applied with lower wavelength as λ/2, λ/4, λ/8. Since 0.38 mm is an approximate value of 1/16 of wavelength, EMAT was fabricated using 0.38-mm meander coil.
Experiments were conducted to investigate the behavior of nonlinear induced ultrasound. Figure 11 shows the experimental setup. The RITEC RAM-4000 was used as a tone-burst ultrasonic transmitter and receiver and it was processed by a pitch-catch method.   In order to obtain the reliability of the experimental results, the same geometric conditions were set, and two kinds of experiments were conducted. As shown in Figure 12, a meander line and permanent magnets were installed on the steel wire rod. As Shown in Figure 13a, the first experiment was divided into four sections of 60 mm each, and the relative nonlinearity of each wire was confirmed. The second experiment was conducted by increasing the propagation distance by 60 mm as shown in Figure 13b. The schematic diagram of each experiment is shown in Figure 13. Experiments were conducted to determine whether defects could be detected through the relative nonlinearity. In order to obtain the reliability of the experimental results, the same geometric conditions were set, and two kinds of experiments were conducted. As shown in Figure 12, a meander line and permanent magnets were installed on the steel wire rod. As Shown in Figure 13a, the first experiment was divided into four sections of 60 mm each, and the relative nonlinearity of each wire was confirmed. The second experiment was conducted by increasing the propagation distance by 60 mm as shown in Figure 13b. The schematic diagram of each experiment is shown in Figure 13. Experiments were conducted to determine whether defects could be detected through the relative nonlinearity.

Results and Discussion
The relative nonlinearity of the fabricated EMAT sensor was measured for each specimen in the longitudinal direction of the steel wire. The relative nonlinearity tendency was studied. As mentioned above, the nonlinear guided wave technique is a technique to diagnose changes in material properties and microdefects by using harmonic components unlike the conventional technique. EMAT shows higher performance than PZT to measure nonlinearity of material because it does not need contact

Results and Discussion
The relative nonlinearity of the fabricated EMAT sensor was measured for each specimen in the longitudinal direction of the steel wire. The relative nonlinearity tendency was studied. As mentioned above, the nonlinear guided wave technique is a technique to diagnose changes in material properties

Results and Discussion
The relative nonlinearity of the fabricated EMAT sensor was measured for each specimen in the longitudinal direction of the steel wire. The relative nonlinearity tendency was studied. As mentioned above, the nonlinear guided wave technique is a technique to diagnose changes in material properties and microdefects by using harmonic components unlike the conventional technique. EMAT shows higher performance than PZT to measure nonlinearity of material because it does not need contact medium and uses electromagnetic in flaw detection. In case of using PZT, the error due to the individual difference of the experimenter cannot be ignored. Therefore, the method using EMAT is very appropriate. Figure 14 shows the signals for linear ultrasonic wave in three specimens. The time domain signal for each specimen can distinguish between the distance and the speed relative to the time, however, microdefects cannot be confirmed. In addition, the analysis of the modes showed that the L 1 mode was well implemented for SWOSC-V and SWOCS-VHV, but SWOSC-VHS was able to confirm that the various modes were mixed. Therefore, the experiment was conducted using a nonlinear guided ultrasonic technique using second harmonic. The fundamental amplitude A1 and second harmonic amplitude A2 amplitude values can be derived by measuring the time domain signal of 60 mm intervals from three specimen for each material and then performing FFT. Substituting the derived A1 and A2 into Equation (2), nonlinear parameters can be obtained for each specimen. Figure 15 is the result of comparing the relative nonlinearity in each zone. In all three specimens of SWOSC-V, the relative nonlinearity increases with The fundamental amplitude A1 and second harmonic amplitude A2 amplitude values can be derived by measuring the time domain signal of 60 mm intervals from three specimen for each material and then performing FFT. Substituting the derived A1 and A2 into Equation (2), nonlinear parameters can be obtained for each specimen. Figure 15 is the result of comparing the relative nonlinearity in each zone. In all three specimens of SWOSC-V, the relative nonlinearity increases with increasing propagation distance. The relative nonlinearity of all three specimens decreases at the propagation distance of 181-240 mm, which can be regarded as the material properties of the specimen. SWOSC-VHV also shows the same tendency of three specimens. However, SWOSC-VHS # 2 has a tendency to be different from the # 1 and # 3 specimens at 61-180 mm propagation distance. Three specimens with the same physical properties should show the same tendency toward in each section. However, since VWOSC-VHS #2 has a different tendency from the VWOSC-VHS #1 and #3 samples, it can be determined that there is some abnormality inside the material.
Appl. Sci. 2020, 10, x 11 of 15 Three specimens with the same physical properties should show the same tendency toward in each section. However, since VWOSC-VHS #2 has a different tendency from the VWOSC-VHS #1 and #3 samples, it can be determined that there is some abnormality inside the material. Because of the tendency to suspect microscopic defects, additional experiments were conducted to ensure the reliability of the experimental data. Figure 16 is the relative nonlinearity with increasing distance, which was an additional experimental result. SWOSC-V and SWOSC-VHS could obtain a tendency for relative nonlinearity change as the distance increased. However, # 3 of SWOSC-VHV showed a large difference in relative nonlinear factor values from # 1 and # 2 at a propagation distance Because of the tendency to suspect microscopic defects, additional experiments were conducted to ensure the reliability of the experimental data. Figure 16 is the relative nonlinearity with increasing distance, which was an additional experimental result. SWOSC-V and SWOSC-VHS could obtain a tendency for relative nonlinearity change as the distance increased. However, # 3 of SWOSC-VHV showed a large difference in relative nonlinear factor values from # 1 and # 2 at a propagation distance of 120 mm, but it was very difficult to be considered as a suspected defect region due to the agreement of the tendency for each specimen. At the propagation distance of 180 mm, SWOSC-VHH # 2 had the same tendency as the previous experimental results. A total of two experiments were used to consider suspected microdefects in SWOSC-VHV # 2 at a propagation distance of 180 mm.
Appl. Sci. 2020, 10, x 12 of 15 of 120 mm, but it was very difficult to be considered as a suspected defect region due to the agreement of the tendency for each specimen. At the propagation distance of 180 mm, SWOSC-VHH # 2 had the same tendency as the previous experimental results. A total of two experiments were used to consider suspected microdefects in SWOSC-VHV # 2 at a propagation distance of 180 mm.     Figure 17b shows a clear difference in the distribution of microdefects compared to Figure 17a. This is consistent with the experimental results and SEM photographs. Therefore, it can be seen that the reliability of the experimental result was secured. Figure 18 shows the result of enlarged the micro defect.
Appl. Sci. 2020, 10, x 13 of 15 is consistent with the experimental results and SEM photographs. Therefore, it can be seen that the reliability of the experimental result was secured. Figure 18 shows the result of enlarged the micro defect.
(a) (b)  The experimental results were not quantitative because the distance between the coils and the specimen changed finely when the reinstallation was repeated after separating the meander coil and the specimen from each other during the experiment. In other words, the lift-off changed. In order to solve this problem, we had to build a proper system to fix the meander coil and the specimen firmly. In addition, since the nonlinearity was very sensitive, the ultrasound path difference may have occurred due to the minute scratches on the surface of the specimen, resulting in energy loss and affecting the damping coefficient. Therefore, it is necessary to acquire precision machined specimens. is consistent with the experimental results and SEM photographs. Therefore, it can be seen that the reliability of the experimental result was secured. Figure 18 shows the result of enlarged the micro defect.
(a) (b)  The experimental results were not quantitative because the distance between the coils and the specimen changed finely when the reinstallation was repeated after separating the meander coil and the specimen from each other during the experiment. In other words, the lift-off changed. In order to solve this problem, we had to build a proper system to fix the meander coil and the specimen firmly. In addition, since the nonlinearity was very sensitive, the ultrasound path difference may have occurred due to the minute scratches on the surface of the specimen, resulting in energy loss and affecting the damping coefficient. Therefore, it is necessary to acquire precision machined specimens. The experimental results were not quantitative because the distance between the coils and the specimen changed finely when the reinstallation was repeated after separating the meander coil and the specimen from each other during the experiment. In other words, the lift-off changed. In order to solve this problem, we had to build a proper system to fix the meander coil and the specimen firmly. In addition, since the nonlinearity was very sensitive, the ultrasound path difference may have occurred due to the minute scratches on the surface of the specimen, resulting in energy loss and affecting the damping coefficient. Therefore, it is necessary to acquire precision machined specimens.

Conclusions
In this study, the nonlinearity tendency of microdefects was investigated by applying guided wave and nonlinear method to steel wire using EMAT. The relative nonlinearity of each specimen is specific for each material. This is considered to be a characteristic of the content of elements constituting the material. Experimental results show that specimens with large errors and specimens without specimens exist. This is considered to be an error due to the distance between the meander coil and the specimen, that is, the lift-off, when the specimen and the coil are separated and remounted. SEM images were taken to verify the reliability of the experimental results. The results were very satisfactory. The possibility of diagnosing microdefects in steel wire production line was confirmed. In order to utilize the nonlinear technique, there is a need to acquire defect-free specimens. We have identified the need for a system that can acquire clear signals. However, there were experimental errors, there is no critical dispute in confirming the tendency for each specimen. It is possible to observe relatively the suspicion of microdefect. It is expected that quantitative evaluation of each specimen will be possible if the parameters of nonlinear factor are removed through a system which can fix the defect-free specimen and lift-off later. In addition, if this research technique is used, it is possible to quickly check noncontact for defects of steel wire rods passing through the inspection line, and to detect fine defects early before processing the steel wire rod to enhance the safety of the material. It was suitable for inspecting the initial fine defects in steel wires before spring processing by utilizing EMAT, a noncontact method without contact medium. The noncontact method is a method capable of minimizing the deformation of the signal that changes depending on the amount or compression state of the contact medium. If the technique is applied to the industrial site, it is judged that it will be possible to test for microdefects quickly and consistently.