The present application claims priority to Japanese Patent Application No. 2021-181510 filed on Nov. 5, 2021, the entire contents of which are incorporated herein by reference.
The present disclosure relates to a measurement apparatus and a measurement method.
Non-destructive testing refers to a testing technique to examine the state of defects or deterioration inside or on the surface of a sample without destroying the sample. Patent Literature (PTL) 1 describes a technique for nondestructive testing to determine the adhesive strength between layers of a multilayer sample.
Conventional configurations have room for improvement, however, in the measurement accuracy of the adhesive strength between layers.
It is an aim of the present disclosure to provide a measurement apparatus and a measurement method capable of improving the measurement accuracy of the adhesive strength between layers.
A measurement apparatus according to several embodiments includes a controller configured to output an electromagnetic wave from an electromagnetic wave output source toward a sample that has a first layer and a second layer adjacent to each other and is subjected to vibration at a predetermined vibration frequency, receive a reflected wave of the electromagnetic wave from a measurement target portion at an interface between the first layer and the second layer, calculate a frequency or an amplitude of vibration of the measurement target portion based on the reflected wave, and measure an adhesive strength of the measurement target portion based on the frequency or the amplitude of vibration of the measurement target portion calculated based on the reflected wave. In this way, the measurement apparatus can measure the adhesive strength between layers with high accuracy, since the adhesive strength is measured by acquiring the frequency or amplitude of vibration of the measurement target portion while the degree of the adhesive strength at the interface is brought to light by the vibration.
In the measurement apparatus according to an embodiment, the controller is configured to measure the adhesive strength of the measurement target portion based on a frequency spectrum of the vibration of the measurement target portion in a frequency band that includes a different frequency than the vibration frequency. In this way, the measurement apparatus can measure the adhesive strength of the measurement target portion with even higher accuracy by referring to the frequency spectrum of the vibration of the measurement target portion in a frequency band that includes a different frequency than the vibration frequency of the sample.
In the measurement apparatus according to an embodiment, the controller is configured to calculate the frequency or the amplitude of vibration of the measurement target portion by performing a Doppler measurement of the reflected wave. The measurement apparatus can reduce the effect of background noise by using Doppler measurement and can measure the adhesive strength of the measurement target portion with even higher accuracy.
In the measurement apparatus according to an embodiment, the controller is configured to cause a p-polarized laser from a laser light source to be outputted toward the sample at Brewster's angle as the electromagnetic wave. This can exclude the effect of reflected waves from the surface of the sample, and the measurement apparatus can measure the adhesive strength of the measurement target portion with even higher accuracy.
In the measurement apparatus according to an embodiment, the controller is configured to output the electromagnetic wave toward the sample subjected to vibration at a first vibration frequency as the predetermined vibration frequency and calculate a first frequency or a first amplitude, which is the frequency or the amplitude of vibration of the measurement target portion, based on the reflected wave of the electromagnetic wave from the measurement target portion of the sample subjected to vibration at the first vibration frequency, output the electromagnetic wave toward the sample subjected to vibration at a second vibration frequency as the predetermined vibration frequency and calculate a second frequency or a second amplitude, which is the frequency or the amplitude of vibration of the measurement target portion, based on the reflected wave of the electromagnetic wave from the measurement target portion of the sample subjected to vibration at the second vibration frequency, and measure the adhesive strength of the measurement target portion based on at least one of the first frequency and the second frequency, and the first amplitude and the second amplitude. In this way, the measurement apparatus may use the total of the frequency or amplitude of the reflected wave from the sample subjected to vibration at the first vibration frequency and the frequency or amplitude of the reflected wave from the sample subjected to vibration at the second vibration frequency. The measurement apparatus can therefore measure the adhesive strength of the measurement target portion with even higher accuracy.
In the measurement apparatus according to an embodiment, there are a plurality of measurement target portions at the interface between the first layer and the second layer, and the controller is configured to output an electromagnetic wave toward each measurement target portion in a plurality of measurement target portions at the interface between the first layer and the second layer, receive a reflected wave of the electromagnetic wave from each measurement target portion in the plurality of measurement target portions, analyze, for each measurement target portion in the plurality of measurement target portions, the reflected wave from the measurement target portion to calculate a frequency or an amplitude of vibration of the measurement target portion, and measure, for each measurement target portion in the plurality of measurement target portions, an adhesive strength of the measurement target portion based on a comparison between the frequency or the amplitude of vibration of the measurement target portion and an average value of the frequency or the amplitude of vibration of the plurality of measurement target portions. In this way, the measurement apparatus measures the frequency or amplitude of vibration of the plurality of measurement target portions and measures the adhesive strength of a certain measurement target portion based on a comparison with the frequency or the amplitude of vibration of the plurality of measurement target portions. The measurement apparatus can thereby further increase the measurement accuracy.
In the measurement apparatus according to an embodiment, the controller is configured to output an electromagnetic wave of a first frequency from a first electromagnetic wave output source toward the sample, the second layer of the sample being provided with an additive that increases reflectance of the electromagnetic wave of the first frequency. This enables the measurement apparatus to receive reflected waves with high reflection intensity from the second layer and to measure, with even higher accuracy, the adhesive strength of the measurement target portion located at the interface between the first layer and the second layer.
In the measurement apparatus according to an embodiment, the controller is configured to output an electromagnetic wave of a second frequency from a second electromagnetic wave output source toward the sample, the sample further including a third layer that is adjacent to the second layer and is provided with an additive that increases reflectance of the electromagnetic wave of the second frequency, receive a reflected wave of the electromagnetic wave of the second frequency from a measurement target portion at an interface between the second layer and the third layer, calculate a frequency or an amplitude of vibration of the measurement target portion at the interface between the second layer and the third layer based on the reflected wave of the second frequency, and measure an adhesive strength of the measurement target portion at the interface between the second layer and the third layer based on the frequency or the amplitude of vibration of the measurement target portion at the interface between the second layer and the third layer. This enables the measurement apparatus to receive reflected waves with high reflection intensity from the third layer and to measure, with even higher accuracy, the adhesive strength of the measurement target portion located at the interface between the second layer and the third layer.
In the measurement apparatus according to an embodiment, the controller is configured to output, from a third electromagnetic wave output source, an electromagnetic wave of a third frequency that is reflected by a specific foreign object, and determine that the specific foreign object is present in the sample in response to reception of a reflected wave of the electromagnetic wave of the third frequency from the sample. The measurement apparatus can therefore determine whether a foreign object is present in the sample.
A measurement method according to several embodiments is a measurement method of a measurement apparatus, the measurement method including outputting, by a controller, an electromagnetic wave from an electromagnetic wave output source toward a sample that has a first layer and a second layer adjacent to each other and is subjected to vibration at a predetermined vibration frequency, receiving, by the controller, a reflected wave of the electromagnetic wave from a measurement target portion at an interface between the first layer and the second layer, calculating, by the controller, a frequency or an amplitude of vibration of the measurement target portion based on the reflected wave, and measuring, by the controller, an adhesive strength of the measurement target portion based on the frequency or the amplitude of vibration of the measurement target portion calculated based on the reflected wave. In this way, the measurement method can measure the adhesive strength between layers with high accuracy, since the adhesive strength is measured by acquiring the frequency or amplitude of vibration of the measurement target portion while the degree of the adhesive strength at the interface is brought to light by the vibration.
According to an embodiment of the present disclosure, the measurement accuracy of the adhesive strength between layers can be improved.
In the accompanying drawings:
A system according to a Comparative Example described in PTL 1 outputs electromagnetic radiation toward a multilayer sample and analyzes the electromagnetic radiation reflected by or transmitted through the sample to determine the adhesive strength between the layers of the multilayer sample. The system according to the Comparative Example includes a transmitter that outputs electromagnetic radiation toward a sample, a receiver that receives electromagnetic radiation reflected by or transmitted through the sample, and a data collection device. The system according to the Comparative Example determines the adhesive strength between the first layer and the second layer based on the waveform of the electromagnetic radiation reflected by or transmitted through the sample.
However, since the system according to the Comparative Example outputs electromagnetic radiation from the outside toward a stationary sample and determines the adhesive strength based on the waveform of the reflected electromagnetic radiation and the like, it is difficult to accurately distinguish between the cases in which the first layer and second layer are weakly and strongly adhered to each other. Therefore, the system according to the Comparative Example has difficulty in measuring the adhesive strength between the layers of a sample with high accuracy. To address this issue, the present disclosure describes a measurement apparatus and a measurement method capable of measuring the adhesive strength between layers with high accuracy.
Embodiments of the present disclosure are now described with reference to the drawings. Portions having an identical configuration or function in the drawings are labeled with the same reference signs. In the explanation of the embodiments, a redundant description of identical portions may be omitted or simplified as appropriate.
The measurement apparatus according to the present embodiment irradiates electromagnetic waves toward a sample, as a measurement target consisting of multiple layers, while vibrating the sample. From the reflected wave, the measurement apparatus detects the frequency, amplitude, and the like regarding the vibration of the interface at a measurement point and measures the adhesive strength at the interface of the adherend. In this way, the measurement apparatus according to the present embodiment measures the adhesive strength according to the characteristics of the vibration at the measurement point as detected from the reflected wave from the vibrating sample. The measurement apparatus can thereby measure the adhesive strength between layers with high accuracy.
The measurement apparatus 20 includes a measurement apparatus body 12 and a vibrator 15. In the example in
The vibrator 15 is an apparatus that applies vibration to the sample 30 when the measurement apparatus body 12 transmits and receives electromagnetic waves. The vibrator 15 may, for example, apply vibration to the sample 30 by outputting sound waves, including ultrasonic waves. Specifically, the vibrator 15 may, for example, vibrate the sample 30 by outputting sound waves using a phased array or by ablation of the material by a laser. Although
The measurement apparatus body 12 is equipped with movable parts 1 (1a, 1b), an optical part 10, an electrical and electronic part 11, a controller 13, and a data processor 14. The movable parts 1 (1a, 1b) include any movable structure that can improve the portability of the measurement apparatus body 12. For example, the movable parts 1 (1a, 1b) may include a tire attached to the measurement apparatus body 12. The measurement apparatus body 12 can be moved over the surface of the adherend 31 by tires or the like forming the movable parts 1 (1a, 1b). The movable parts 1 (1a, 1b) move the measurement apparatus body 12 to enable scanning of the irradiation position of the electromagnetic waves toward the sample 30.
The optical part 10 irradiates electromagnetic waves toward the sample 30, receives reflected waves from the sample 30, and outputs the reflected waves as an electric signal to the electrical and electronic part 11. As an example, the optical part 10 is described below as including an optical system for measuring the frequency, amplitude, and the like of vibration at the measurement target portion 35 by optical Doppler measurement, but the method for measuring the frequency, amplitude, and the like of vibration is not limited to this case. For example, the measurement apparatus 20 may simply measure the frequency, amplitude, and the like of the vibration from the phase displacement of the reflected waves in a case in which the amplitude of the vibration at the measurement target portion 35 is greater than a predetermined value, or a case in which the frequency of the vibration is greater than a predetermined value. The optical part 10 includes a lens 2, a mirror 3, beam splitters 4 (4a, 4b, 4c), an acousto-optical element (acousto-optics modulator, hereinafter “AOM”) 5, a photoelectric (optical signal/electrical signal, hereinafter “O/E”) converter 6, and a laser light source 7.
In the optical part 10, the laser light source 7 as an electromagnetic wave output source outputs a laser as an electromagnetic wave. The laser light source 7 may be configured by a light-emitting device capable of outputting a laser in a frequency band closer to the frequency band that is highly transmissive with respect to the resin forming the adherend 31. The bandwidth of the laser may, for example, be approximately 0.1 THz to 10 THz or may be microwaves, millimeter waves, or terahertz waves. Hereafter, the frequency of the laser outputted by the laser light source 7 is denoted as f. The signal wave of the laser outputted by the laser light source 7 acts as a carrier wave to transmit information indicating the vibration of the measurement target portion 35 due to the vibrator 15.
The laser outputted from the laser light source 7 is split in two at the beam splitter 4b. One of the lasers split in two at the beam splitter 4b is guided to the AOM 5, and the other laser is guided to the beam splitter 4a. The beam splitters 4 (4a, 4b, 4c) may, for example, be one-way mirrors.
The AOM 5 displaces the frequency f of the laser inputted through the beam splitter 4b to a frequency f+foff. The offset frequency foff is selected from a range of values such that a laser with frequency f+foff passes through the resin forming the adherend 31. The laser with the frequency displaced in the AOM 5 is guided to the beam splitter 4c.
The laser inputted from the AOM 5 to the beam splitter 4c passes through the beam splitter 4c, is focused by the lens 2, and is incident on the adherend 31. The laser incident on the adherend 31 passes through the adherend 31 and is reflected at the measurement target portion 35 in the adhesive 32. Since the sample 30 is subjected to vibration by the vibrator 15, the reflected wave contains a frequency component of f+foff±fd, which reflects the vibration of the measurement target portion 35. Here, fa is the change in frequency of the laser displaced by the vibration of the measurement target portion 35 and is equivalent to the vibration frequency of the measurement target portion 35. The reflected wave reflected at the measurement target portion 35 is focused by the lens 2 and is incident on the beam splitter 4c. In the example in
The reflected wave incident on the beam splitter 4c is reflected at the beam splitter 4c and guided to the mirror 3. The mirror 3 reflects the inputted reflected wave and guides the reflected wave to the beam splitter 4a. The reflected wave that contains the frequency component of f+foff±fd and is guided to the beam splitter 4a passes through the beam splitter 4a and is guided to the O/E converter 6. On the other hand, the laser of frequency f guided from the beam splitter 4b to the beam splitter 4a is reflected at the beam splitter 4a and guided to the O/E converter 6.
The O/E converter 6 converts the inputted optical signal to a photoelectric signal and outputs a current signal. Since the polarity of the laser outputted from the laser light source 7 is inverted upon reflection by the measurement target portion 35, the frequency f component of the reflected wave, which contains the frequency components of f+foff±fd, and the frequency f component of the laser cancel each other out in the O/E converter 6. Therefore, the O/E converter 6 outputs a current signal representing the frequency foff±fd. In the present embodiment, the optical part 10 thus provokes interference between the reflected light, which is subjected to a frequency shift by the vibration of the AOM 5 and the sample 30, and the laser as a reference light outputted from the laser light source 7. The optical part 10 thereby detects a signal pertaining to the vibration of the sample 30 by a heterodyne method. The detection of signals pertaining to the vibration of the sample 30 is not limited to such a heterodyne method. For example, instead of the AOM 5, the mirror 3 may be vibrated at a frequency foff so that the reflected wave from the measurement target portion 35 includes a frequency component varied by foff. The O/E converter 6 outputs a current signal including a frequency component of foff±fd to the electrical and electronic part 11.
The electrical and electronic part 11 analyzes the current signal of frequency foff±fd inputted from the O/E converter 6 of the optical part 10 to calculate the frequency and amplitude of the vibration at the measurement target portion 35. The electrical and electronic part 11 includes an F/V (Frequency/Voltage) converter 8 and a frequency and amplitude calculator 9. The F/V converter 8 outputs a voltage signal corresponding to the frequency foff±fd of the current signal inputted from the O/E converter 6 to the frequency and amplitude calculator 9. The frequency and amplitude calculator 9 calculates the frequency, amplitude, and the like of the vibration at the measurement target portion 35 from the voltage signal inputted from the F/V converter 8.
Specifically, the frequency and amplitude calculator 9 can measure Av by performing frequency modulation (FM) on the current i outputted from the O/E converter 6, calculating the frequency foff+Δv of the current i, and obtaining the difference from the known offset frequency foff. Here, letting t be time, V0 be the amplitude of the speed of the measurement target portion 35 that is vibrating, and λ be the wavelength of the light source, Δv is indicated by Mathematical Expression 1.
As mentioned above, the change in frequency fd is identical to the frequency of the vibration of the measurement target portion 35. Therefore, the frequency and amplitude calculator 9 can determine the frequency fd of the vibration of the measurement target portion 35 based on the frequency of Δv. Furthermore, since the change in frequency Δv is proportional to the moving speed of the measurement target portion 35, the frequency and amplitude calculator 9 can calculate the amplitude of the measurement target portion 35 by integrating Av.
From a plurality of points on the surface of the adherend 31, the measurement apparatus 20 measures the frequency, amplitude, and the like of the vibration in the measurement target portion 35 directly below the points and analyzes the measured data. The data processor 14 of the measurement apparatus body 12 is an arithmetic unit that performs arithmetic processing of such data.
The controller 13 controls the operation of each component of the measurement apparatus 20. For example, the controller 13 may control the operations related to the irradiation of the laser by the laser light source 7, vibration of the vibrator 15, and analysis of the measurement data by the data processor 14. The measurement apparatus 20 may be capable of specifying in advance the range over which the measurement apparatus body 12 scans the adherend 31 in order to measure the frequency, amplitude, and the like of the vibration at a plurality of measurement target portions 35 corresponding to a plurality of points. In the case in which such a scanning range is specified, the controller 13 may control the operation of the movable parts 1 (1a, 1b) to move the measurement apparatus body 12 to each point where measurement is to be performed and may measure the frequency, amplitude, and the like of vibration at the measurement target portion 35 corresponding to each point. The controller 13 includes one or more processors. The “processor” in an embodiment is a general-purpose processor or a dedicated processor specialized for particular processing, but these examples are not limiting. The functions of the measurement apparatus 20 may be achieved by a processor included in the controller 13 executing a program that can be used to cause the measurement system 100 according to the present embodiment to function.
The terminal apparatus 16 is an information processing apparatus that accepts instruction input from a user regarding the operation of the measurement apparatus 20. The terminal apparatus 16 may be achieved by a general-purpose apparatus, such as a personal computer (PC), tablet, or smartphone, or by a dedicated apparatus. Upon receiving an instruction input from the user, the terminal apparatus 16 issues a measurement execution command corresponding to the content of the instruction input and outputs the command to the data processor 14 of the measurement apparatus 20. The data processor 14 outputs the inputted measurement execution command to the controller 13. The controller 13 controls the operation of each component of the measurement apparatus 20, including setting, starting, and stopping the laser light source 7 and the vibrator 15, according to the measurement execution command.
Next, details of the operation of the measurement apparatus 20 are described with reference to
In step S1, the controller 13 controls the laser light source 7 to output a laser.
In step S2, the controller 13 sets the frequency of the vibrator 15 to a preset initial value. For example, the controller 13 may set 10 kHz as the initial value of the frequency of the vibrator 15.
In step S3, the controller 13 initiates the output of vibration by the vibrator 15 according to the set vibration frequency.
In step S4, the controller 13 measures the reflected wave, from the sample 30, of the laser that was outputted from the laser light source 7 and whose frequency was displaced in the AOM 5 to calculate the frequency, amplitude, and the like of the vibration at the measurement target portion 35. For example, as mentioned above, the controller 13 may calculate the frequency, amplitude, and the like of the vibration at the measurement target portion 35 by optical Doppler measurement.
In step S5, the controller 13 transfers data on the calculated frequency, amplitude, and the like of the vibration to the terminal apparatus 16.
In step S6, the controller 13 determines whether the predetermined frequency sweep of the vibrator 15 has been completed at that measurement point. For example, the controller 13 may determine that the sweep has been completed in a case in which measurement based on vibration at 10 kHz, 15 kHz, and 20 kHz frequencies is complete at that measurement point. In a case in which the sweep has been completed (YES in step S6), the controller 13 proceeds to step S8. Otherwise (NO in step S6), the controller 13 proceeds to step S7.
In step S7, the controller 13 updates the frequency of the vibrator 15 to a vibration frequency for which measurement has not yet been performed at that measurement point. After completing the process of step S7, the controller 13 returns to step S3 to continue the process.
In step S8, the controller 13 determines whether all of the surface measurement has been completed, i.e., whether the measurement for each of the predetermined plurality of vibration frequencies has been completed for all of the predetermined measurement points. In a case in which all of the surface measurement has been completed (YES in step S8), the controller 13 proceeds to step S10. Otherwise (NO in step S8), the controller 13 proceeds to step S9.
In step S9, the controller 13 moves the measurement apparatus body 12 to the next measurement point at which measurement has not yet been performed. To move the measurement apparatus body 12, the controller 13 may operate the movable parts 1 (1a, 1b) or may, for example, provide notification via a display of the terminal apparatus 16, by audio output, or the like prompting the user to move the measurement apparatus body 12. After completing the process of step S9, the controller 13 returns to step S2 to continue the process.
In step S10, the controller 13 stops operation of the laser light source 7 and the vibrator 15.
In step S11, the controller 13 analyzes each piece of data obtained by the processes in steps S1 to S9 and measures the adhesive strength at each measurement point. In general, when the sample 30 is subjected to vibration, it is considered that there will be a difference in vibration characteristics, such as the frequency or amplitude, between a measurement target portion 35 that has high adhesive strength and a measurement target portion 35 that has low adhesive strength. For example, in a case in which the adherends 31, 33 are not adhered, the vibration at the interface thereof is expected to be nonlinear vibration different than the vibration of the vibrator 15, due to closings or openings. The controller 13 therefore determines the adhesive strength of a measurement target portion 35 based on the characteristics, such as the frequency or amplitude, of the vibration of the measurement target portion 35. The controller 13 can, for example, determine that the adhesive strength of a certain measurement target portion 35 is weak in a case in which the value of the frequency, amplitude, or the like of the vibration of the measurement target portion 35 is significantly different from the frequency, amplitude, or the like of the vibration of another measurement target portion 35. Specifically, the controller 13 can, for example, acquire the average value and standard deviation σ of the frequency, amplitude, or the like of the vibration of the measurement target portion 35 corresponding to each measurement point and determine that the adhesive strength of a measurement target portion 35 is weak if the value of its frequency, amplitude, or the like is at least a certain value (for example, 2σ) away from the average value. At this time, the controller 13 may mark the measurement target portions 35 whose frequency, amplitude, or other value of vibration is at least a certain value away from the average value for each frequency of the vibrator 15. The controller 13 can then determine that the adhesive strength is weak for a measurement target portion 35 marked for at least one vibration frequency of the vibrator 15. Alternatively, the controller 13 can determine that the adhesive strength is weak for a measurement target portion 35 marked for at least two, or all, vibration frequencies of the vibrator 15.
The measurement apparatus 20 can determine that the adhesive strength of the measurement target portion 35 that vibrates with characteristics that differ significantly from the characteristics of the vibration of the vibrator 15 is weak. For example, the measurement apparatus 20 can determine that the adhesive strength of a measurement target portion 35 for which the difference in frequency or amplitude from the vibration of the vibrator 15 is equal to or greater than a certain value is weak. The measurement apparatus 20 may acquire in advance, and store in a memory apparatus, the relationship between characteristics, such as frequency or amplitude, of the vibration of the measurement target portion 35 and the adhesive strength for each type of sample 30, each measurement environment (including the vibration frequency of the vibrator 15), and the like. In this case, the controller 13 may determine the adhesive strength of the measurement target portion 35 by comparing the measured value of the frequency, amplitude, or the like of vibration of the measurement target portion 35 with the information, stored in the memory apparatus in advance, indicating the relationship between the characteristics and the adhesive strength. The measurement apparatus 20 may, in this case as well, switch the vibration frequency of the vibrator 15 among a plurality of values and detect the frequency and amplitude of the vibration at the measurement target portion 35 for each vibration frequency to further improve the accuracy for determining the adhesive strength. In addition to, or instead of, the frequency and amplitude of the vibration of the measurement target portion 35, the measurement apparatus 20 may use phase information to determine the adhesive strength.
In this way, the controller 13 may acquire a value indicating the adhesive strength at each measurement target portion 35 by, for example, acquiring the difference between a characteristic of vibration at that measurement target portion 35 and a reference vibration characteristic. Such a reference vibration characteristic may, for example, be the average value of a vibration characteristic of other measurement target portions 35, a characteristic of the vibration of the vibrator 15, or a value related to a previously learned characteristic. The measurement target portion 35 for which the difference between the value indicating the adhesive strength and the reference vibration characteristic is at least a certain value (for example, 2σ) may be marked as a portion at which the adhesive strength is weak.
In step S12, the controller 13 displays an image illustrating the measurement results (diagnosis results) on a display of the terminal apparatus 16. For example, the controller 13 may display values indicating the adhesive strength at each measurement point, the marked measurement target portions 35, and the like. After completing the process of step S12, the controller 13 ends the process of the flowchart. Although
As described above, the measurement apparatus 20 vibrates the sample 30 that is the measurement target while irradiating a laser in the microwave, millimeter wave, or terahertz wave band toward the target, thereby transmitting radiation through the adherend 31, and performs Doppler measurement of the reflection from the measurement target portion 35 at the adhesive interface to be observed. This enables highly accurate determination of the adhesive state at the measurement target portion 35. In other words, as in the Comparative Example, it is difficult to determine, in a static state, whether the layers forming the sample 30 are in contact but not adhered. By vibrating the sample 30, the measurement apparatus 20 brings to light the difference between a state of being in contact but not adhered and a state of being in contact and adhered. Closings and openings are generated by vibration, for example, in a case in which the layers forming the sample 30 are in contact but not adhered. This results in complex vibration behavior, and the spectrum of vibration of the measurement target portion 35 will contain various frequency components. The measurement apparatus 20 uses this property for highly accurate measurement of the adhesive strength at the measurement target portion 35.
In a case of irradiating the sample 30 with a laser and determining the adhesive strength at the measurement target portion 35 based on the reflected wave, as described above, the signal of interest is the reflected wave from the adhesive interface, whereas the reflected wave from the interface between the air and the adherend 31 is noise and is preferably eliminated insofar as possible. Therefore, the measurement apparatus 20 may cause p-polarized light to be incident on the adherend 31 at Brewster's angle.
In
The measurement apparatus 20 can thus make the reflected wave from the interface between the air and the adherend 31 zero by irradiating a p-polarized laser toward the adherend 31 at Brewster's angle θB. The measurement apparatus can therefore eliminate the reflected waves that are noise and can measure the adhesive strength of the measurement target portion 35 with high accuracy.
The intensity of the reflected wave may be increased by adding an additive, to the adhesive or the like forming the sample 30, to increase the reflectance of the laser.
In a case in which the refractive indices of the adherend 31 and the adhesive 32 are close to each other, sufficient reflection intensity might not be obtained at the adhesive interface between the adherend 31 and the adhesive 32. Therefore, to obtain a reflected wave with higher intensity from the adhesive interface between the adherend 31 and the adhesive 32, an additive with high reflection intensity with respect to a frequency f1 used in the laser to be irradiated may be added to the adhesive 32, as illustrated in
The measurement apparatus 20 may also use a laser of frequency f3 that has high reflectance with respect to air to detect vibration of an air interface (void 37) as a specific foreign object present in the adhesive 32. Furthermore, the measurement apparatus 20 may include a plurality of laser light sources 7 capable of outputting lasers of such frequencies f1, f2, and f3, and the laser light sources 7 may be switched to measure the reflected waves from the laser of each frequency. This makes it possible to select a specific type of interface inside the sample 30 as the measurement target portion 35 and to measure the adhesive strength thereof.
The vibrator 15 may use an ultrasonic phased array to provide a pinpoint vibration load to the site to be vibrated. This minimizes the influence of vibration generated at sites other than the measurement target portion 35. The measurement apparatus 20 can therefore measure the adhesive strength of a specific measurement target portion 35 with even higher accuracy.
As described above, in a case in which the complex refractive index of the adherend 31 and the adhesive 32 are close, and the interfacial reflection intensity of the measurement target portion 35 is low, the adhesive 32 may be provided with an additive designed to obtain a large reflection at the frequency of the laser to be irradiated. This will increase the intensity of the reflected wave obtained from the surface of the adhesive 32, enabling the measurement apparatus 20 to perform highly accurate measurements. The measurement apparatus 20 may include a plurality of types of laser light sources 7 that emit lasers, and the controller 13 may switch among these laser light sources 7. This enables the measurement apparatus 20 to measure, for example, the adhesive strength at the interface between the adherend 31 and the adhesive 32, the adhesive strength at the interface between the adhesive 32 and the adherend 33, and the presence of voids 37.
In each of the above embodiments, an example has been described in which the sample 30 that is the measurement target has a three-layer structure with the adherend 31, the adhesive 32, and the adherend 33, but as long as the sample 30 that is the measurement target has a plurality of layers, the sample 30 is not limited to such a three-layer structure. For example, the sample 30 may have a two-layer structure with two resins (for example, adherends 31, 33) mechanically bonded together. A sample 30 formed by a resin and a metal anchored together at the nano level, such as NMT® (NMT is a registered trademark in Japan, other countries, or both), may be taken as the measurement target, and the measurement apparatus 20 may use the method of each of the above embodiments to measure the adhesive strength of the anchor joints.
As described above, the controller 13 of the measurement apparatus 20 outputs an electromagnetic wave from the laser light source 7 toward a sample 30 that has a first layer (for example, the adherend 31) and a second layer (for example, the adhesive 32) adjacent to each other and is subjected to vibration at a predetermined vibration frequency by the vibrator 15. The controller 13 receives a reflected wave of the electromagnetic wave from a measurement target portion 35 at the interface between the first layer and the second layer and calculates a frequency or an amplitude of vibration of the measurement target portion 35 based on the reflected wave. The controller 13 measures the adhesive strength of the measurement target portion 35 based on the frequency or the amplitude of the vibration of the measurement target portion 35 calculated based on the reflected wave. In this way, the measurement apparatus 20 can measure the adhesive strength between layers with high accuracy, since the adhesive strength is measured by acquiring the frequency or amplitude of the vibration of the measurement target portion 35 while the degree of the adhesive strength at the interface is brought to light by the vibration.
The controller 13 may also measure the adhesive strength of the measurement target portion 35 based on a frequency spectrum of the vibration of the measurement target portion 35 in a frequency band that includes a different frequency than the vibration frequency. In a case in which the adhesive strength at the interface of a plurality of layers is not sufficient, the measurement target portion 35 will vibrate in an irregular and nonlinear manner due to factors such as a difference in the modulus of elasticity between the layers. As a result, the frequency spectrum of the vibration of the measurement target portion 35 is wider than the frequency of the vibrator 15. The controller 13 can therefore measure the adhesive strength of the measurement target portion 35 with even higher accuracy by referring to the frequency spectrum of the vibration of the measurement target portion 35 in a frequency band that includes a different frequency than the vibration frequency of the vibrator 15.
The controller 13 may also calculate the frequency or the amplitude of vibration of the measurement target portion 35 based on Doppler measurement. In this case, the effect of background noise can be reduced, and the measurement apparatus 20 can measure the adhesive strength of the measurement target portion 35 with even higher accuracy.
The controller 13 may also cause a p-polarized laser to be outputted from the laser light source 7 toward the sample 30 at Brewster's angle as the electromagnetic wave. This can exclude the effect of reflected waves from the surface of the sample 30, and the measurement apparatus 20 can measure the adhesive strength of the measurement target portion 35 with even higher accuracy.
The controller 13 may output the electromagnetic wave toward the sample 30 subjected to vibration at a first vibration frequency as the predetermined vibration frequency. The controller 13 may calculate a first frequency or a first amplitude, which is the frequency or the amplitude of vibration of the measurement target portion 35, based on the reflected wave of the electromagnetic wave from the measurement target portion 35 of the sample 30 subjected to vibration at the first vibration frequency. Furthermore, the controller 13 may output the electromagnetic wave toward the sample 30 subjected to vibration at a second vibration frequency as the predetermined vibration frequency. The controller 13 may calculate a second frequency or a second amplitude, which is the frequency or the amplitude of vibration of the measurement target portion 35, based on the reflected wave of the electromagnetic wave from the measurement target portion 35 of the sample 30 subjected to vibration at the second vibration frequency. The controller 13 may then measure the adhesive strength of the measurement target portion 35 based on at least one of the first frequency and the second frequency, and the first amplitude and the second amplitude. In this way, the measurement apparatus 20 may use the total of the frequency or amplitude of the reflected wave from the sample 30 subjected to vibration at the first vibration frequency and the frequency or amplitude of the reflected wave from the sample 30 subjected to vibration at the second vibration frequency. The measurement apparatus 20 can therefore measure the adhesive strength of the measurement target portion 35 with even higher accuracy.
The controller 13 may output an electromagnetic wave toward each measurement target portion 35 in a plurality of measurement target portions 35 at the interface between the first layer and the second layer and may receive a reflected wave of the electromagnetic wave from each measurement target portion 35 in the plurality of measurement target portions 35. The controller 13 may analyze, for each measurement target portion 35 in the plurality of measurement target portions 35, the reflected wave from the measurement target portion 35 to calculate a frequency or an amplitude of vibration of the measurement target portion 35. The controller 13 may measure, for each measurement target portion 35 in the plurality of measurement target portions 35, an adhesive strength of the measurement target portion 35 based on a comparison between the frequency or the amplitude of the vibration of the measurement target portion 35 and an average value of the frequency or the amplitude of the vibration of the plurality of measurement target portions 35. In this way, the measurement apparatus 20 measures the frequency or amplitude of the vibration of the plurality of measurement target portions 35 and measures the adhesive strength of a certain measurement target portion 35 based on a comparison with the frequency or the amplitude of the vibration of the plurality of measurement target portions 35. The measurement apparatus 20 can thereby further increase the measurement accuracy.
The controller 13 may output an electromagnetic wave of a first frequency f1 from a first electromagnetic wave output source (laser light source 7) toward the sample 30, the second layer of the sample 30 being provided with an additive that increases reflectance of the electromagnetic wave of the first frequency f1. This enables the measurement apparatus 20 to receive reflected waves with high reflection intensity from the second layer and to measure, with even higher accuracy, the adhesive strength of the measurement target portion 35 located at the interface between the first layer and the second layer.
The controller 13 may output an electromagnetic wave of a second frequency f2 from a second electromagnetic wave output source toward the sample 30, the sample 30 further including a third layer (for example, the adherend 33) that is adjacent to the second layer and is provided with an additive that increases reflectance of the electromagnetic wave of the second frequency f2. The controller 13 may receive a reflected wave of the electromagnetic wave of the second frequency f2 from a measurement target portion 35 at the interface between the second layer and the third layer. The controller 13 may calculate a frequency or an amplitude of vibration of the measurement target portion 35 at the interface between the second layer and the third layer based on the reflected wave of the second frequency f2. The controller 13 may measure an adhesive strength of the measurement target portion 35 at the interface between the second layer and the third layer based on the frequency or the amplitude of the vibration of the measurement target portion 35 at the interface between the second layer and the third layer. In this way, the measurement apparatus 20 may irradiate an electromagnetic wave of the second frequency f2 toward the sample 30 that includes the third layer with an additive that increases the reflectance of the electromagnetic wave of the second frequency f2. The measurement apparatus 20 may then measure the adhesive strength of the measurement target portion 35 at the interface between the second layer and the third layer based on the reflected wave. This enables the measurement apparatus 20 to receive reflected waves with high reflection intensity from the third layer and to measure, with high accuracy, the adhesive strength of the measurement target portion 35 located at the interface between the second layer and the third layer.
The controller 13 may output, from a third electromagnetic wave output source, an electromagnetic wave of a third frequency f3 that is reflected by a specific foreign object (for example, the void 37), and determine that the specific foreign object is present in the sample 30 in response to reception of a reflected wave of the electromagnetic wave of the third frequency f3 from the sample 30. The measurement apparatus 20 can therefore determine whether a foreign object is present in the sample 30.
The present disclosure is not limited to the above embodiments. For example, a plurality of blocks described in the block diagrams may be integrated, or a block may be divided. Instead of a plurality of steps described in the flowcharts being executed in chronological order in accordance with the description, the plurality of steps may be executed in parallel or in a different order according to the processing capability of the apparatus that executes each step, or as required. Other modifications can be made without departing from the spirit of the present disclosure.
Number | Date | Country | Kind |
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2021-181510 | Nov 2021 | JP | national |
Filing Document | Filing Date | Country | Kind |
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PCT/JP2022/041248 | 11/4/2022 | WO |