JP5567472B2 - Ultrasonic inspection method and ultrasonic inspection apparatus - Google Patents

Description

  The present invention relates to an ultrasonic inspection method and an ultrasonic inspection apparatus. More specifically, a transmitter and a receiver are arranged on the surface of the object to be inspected across the inspection target part, and an ultrasonic wave transmitted from the transmitter to the object to be inspected and propagated through the object to be inspected is transmitted. The present invention relates to an ultrasonic inspection method and an ultrasonic inspection apparatus for inspecting the thinning of the inspection target part by receiving the signal with the receiver.

  Conventionally, as an ultrasonic inspection method as described above, for example, those described in Patent Documents 1 to 4 are known. The inspection method described in Patent Document 1 is an inspection method using surface waves. Since surface waves are easily affected by surface roughness of the surface of the object to be inspected, accurate inspection may be difficult. Further, for example, in a pipe support structure having a welded portion, there is a portion where inspection is difficult because surface waves propagate through the welded portion and do not propagate to the inspection target portion.

  The method described in Patent Document 2 utilizes a phenomenon in which a creeping wave that is a longitudinal wave is mode-converted into a transverse wave and propagates in the thickness direction of the material to be inspected. Longitudinal waves are continually converted into transverse waves and propagated, so loss due to mode conversion is large and the distance between the probes is limited.

  The method described in Patent Document 3 is a technique based on the double probe method, in which inspection is performed by reducing the signal amplitude due to thinning. Therefore, it is easily influenced by the contact state of the probe, the surface roughness, the size of the thinning, the shape, etc., and accurate inspection is difficult. In addition, the amount of decrease in signal amplitude is corrected from the obtained thinning length, which is complicated.

  Since the method described in Patent Document 4 uses an ultrasonic wave that is a surface pseudo-SV wave different from the surface wave, a strong transverse wave that propagates substantially parallel to the surface is generated. Therefore, it is necessary to use a probe having a large refraction angle close to 90 °, which lacks versatility. The object of the invention of Patent Document 2 is sensitivity correction, and there is no detailed description of the thinning detection.

Japanese Patent No. 4500413 Japanese Patent No. 3842794 Japanese Patent Laid-Open No. 2001-4601 JP 2010-54497 A

  In view of such a conventional situation, an object of the present invention is to provide an ultrasonic inspection method and an ultrasonic inspection apparatus that can easily detect a thinning of an inspection target portion regardless of the state of an object to be inspected. .

In order to achieve the above object, the ultrasonic inspection method according to the present invention is characterized in that a transmitter and a receiver are arranged on the surface of an object to be inspected across the inspection target part, and the transmitter to the object to be inspected is super In the ultrasonic inspection method for inspecting the thinning or the like of the inspection target part by transmitting the sound wave and receiving the ultrasonic wave propagated through the inspection object by the receiver, the surface of the inspection object is at least the A curved surface convex toward the outside of the object to be inspected between the transmitter and the receiver, and the transmitter repeats the reflection of only the curved surface a plurality of times and propagates along a propagation path along the curved surface ( (Hereinafter referred to as “surface propagation transverse wave”), and inspecting the thinning of the inspection target part due to a delay in the reception time of the surface propagation transverse wave by bypassing the thinning etc. is there.

  According to the above configuration, the surface-propagating transverse wave repeatedly reflects only the convex curved surface toward the outside. By repeating the reflection finely on the curved surface, it can propagate along the surface shape, the attenuation due to the surface shape such as the surface roughness can be suppressed, and a clear received signal can be obtained. And since the surface propagation shear wave propagates along the surface shape by repeating fine reflection on the curved surface, it propagates around along the surface such as thinning. Therefore, it is possible to easily detect by observing the delay of the reception time due to bypassing the thinning and the like. Further, since the reflection of only the curved surface is repeatedly propagated, it is possible to prevent the propagation to a place other than the inspection target part due to the welded part or the like.

  The surface propagation transverse wave may be an SV wave. It is not necessary to use a highly viscous contact medium, and inspection can be performed efficiently. The frequency of the surface propagation shear wave is preferably 0.5 MHz or more and 5 MHz or less. The low-frequency transverse wave has a low directivity of the ultrasonic wave, and it is possible to prevent the intensity of the ultrasonic beam at a position away from the central axis of the ultrasonic beam from being significantly reduced compared to the central axis of the beam, thereby making the signal clearer. Can be sent and received.

  In any of the above-described inspection methods, for example, the inspection target part can be inspected in a concealing part in which the surface of the object to be inspected is concealed by another member.

  The transmitter may further generate a transverse wave (hereinafter referred to as a “reflected propagation transverse wave”) that repeatedly propagates between the surface of the object to be inspected and the back surface facing the surface. Since the reflected propagation transverse wave is a transverse wave that repeats reflection between the surface and the back surface of the object to be inspected, it is possible to detect a thinning or the like existing on the back surface side as well as the front surface side. It is also possible to identify whether the surface is thinned by generating the surface propagation transverse wave and the reflected propagation transverse wave simultaneously.

  The receiver and the transmitter are moved along the curved surface, and the reception intensity of the surface propagation transverse wave and / or the reflected propagation transverse wave is displayed on a two-dimensional image with the scanning position and the reception time of the transmitter and the receiver as axes. It is desirable to make it. Thereby, thinning etc. can be evaluated easily and easily on a two-dimensional image.

  The receiver and the transmitter may be arranged to face each other in the curved direction of the curved surface. As a result, the surface-reflected shear wave can be clearly propagated and received, and thinning or the like can be detected more accurately.

  In order to achieve the above object, the ultrasonic inspection apparatus according to the present invention is characterized in that in the ultrasonic inspection apparatus used in any of the above ultrasonic inspection methods, the surface of the object to be inspected is at least The curved surface is convex toward the outside of the object to be inspected between the transmitter and the receiver, and the transmitter generates at least the surface-propagating transverse wave, and bypasses the thinning etc. The object is to inspect the thinning of the inspection target part due to a delay in the reception time of the surface propagation shear wave.

  According to the features of the ultrasonic inspection method and the ultrasonic inspection apparatus according to the present invention, it is possible to easily detect the thinning of the inspection target portion regardless of the state of the inspection object.

  Other objects, configurations, and effects of the present invention will become apparent from the following embodiments of the present invention.

It is the schematic which shows the ultrasonic inspection apparatus which concerns on this invention. It is a figure which shows typically the spreading of the ultrasonic wave which injected from the transmitter. It is a figure which shows typically the path | route of the surface reflected shear wave reflected on an outer peripheral surface. It is a figure which shows an example of A scope image of the propagated transverse wave. It is a figure which shows the correspondence of the external shape of a to-be-inspected object, and the two-dimensional image in the to-be-inspected object. It is a figure which shows typically the path | route of a surface propagation transverse wave and a reflected propagation transverse wave. It is a figure which shows an example of the two-dimensional image at the time of arrange | positioning a probe to the circumferential direction of a steel pipe. It is a figure which shows an example of the two-dimensional image in a trunnion part. It is a figure which shows an example of the two-dimensional image in 6B piping. It is a figure which shows an example of the two-dimensional image in 4B piping. It is a figure which shows an example of the two-dimensional image in a pipe mount contact part.

Next, embodiments of the present invention will be described with reference to the drawings.
As shown in FIG. 1, the ultrasonic inspection apparatus 1 according to the present invention uses a pair of transmitter 2 and receiver 3. The transmitter 2 and the receiver 3 are arranged along the circumferential direction X on the outer peripheral surface 100 a as the surface of the device under test 100 across the inspection target part 101 of the device under test 100. The inspection target portion 101 is, for example, a portion where the surface of the device under test 100 is isolated and concealed from the outside by another member 102 and is a place where it is difficult to bring the transmitter 2 and the receiver 3 close to each other.

  In this embodiment, the device under test 100 is a steel pipe used for piping in a plant or the like. The outer peripheral surface 100 a forms a convex curved surface toward the outside of the steel pipe 100 between the transmitter 2 and the receiver 3. In addition, the inspection target part 101 is a concealment part concealed by a trunnion 102 as another member fixed to the steel pipe 100 via the welded part 103 and the reinforcing plate 104. The trunnion 102 is a pipe support structure that supports the steel pipe 100. Hereinafter, an example in which the thinned portion D of the outer peripheral surface 100a in the concealing portion 101 inside the trunnion 102 is inspected will be described.

  As shown in FIG. 1, the transmitter 2 generates a surface propagation transverse wave TW <b> 1 and a reflected propagation transverse wave TW <b> 2 described later in the steel pipe 100. The receiver 3 receives the surface propagation transverse wave TW1 and the reflected propagation transverse wave TW2 propagated through the steel pipe 100. The transmitter 2 and the receiver 3 are connected to the flaw detector 4 together with the position detector 5. The position detector 5 works with the transmitter 2 and the receiver 3 to detect the spatial positions of the transmitter 2 and the receiver 3. The flaw detector 4 includes a CPU 41, a transmission unit 42, a reception unit 43, a position detection unit 44, a display unit 45, and a signal processing unit 46.

  The transmission unit 42 generates a transmission signal and inputs it to the transmitter 2, inputs the ultrasonic wave propagated through the concealment unit 101 received by the receiver 3 to the reception unit 43, and performs arithmetic processing by the signal processing unit 46 and the CPU 41. In addition, the signal from the position detector 5 is input to the position detection unit 44, and the signal processing unit 46 and the CPU 41 perform arithmetic processing to acquire scanning position data.

  The CPU 41 and the signal processing unit 46 generate a B-scope image as a two-dimensional image from the position signals of the transmitter 2 and the receiver 3 sent from the position detector 5 and the ultrasonic reception signal received by the receiver 3. And displayed on the display unit 45. The scanning of the transmitter 2 and the receiver 3 is not necessarily performed in the axial direction Y of the steel pipe 100, and may be performed in the circumferential direction X. That is, instead of measuring the accurate position from the reflected signal of the thinned portion D, it is sufficient to detect at least the presence or absence of the thinned portion D based on the presence or absence of a changing portion appearing in a two-dimensional image described later.

  Here, the two-dimensional image (B-scope image) is the received signal reception intensity (amplitude) with the horizontal axis representing the position information of the transmitter 2 and the receiver 3 and the ultrasonic propagation time (distance) being the vertical axis. Is displayed. For the display of the reception intensity, for example, a gray scale display, a color tone display, or a display by a height orthogonal to a two-dimensional plane can be used. In addition, the change in the reception time appears as a change in a striped pattern due to grayscale display, for example.

  The transmitter 2 uses an oblique probe 10 that causes a transverse wave to enter the steel pipe 100. As shown in FIG. 2, the oblique angle probe 10 generally includes a vibrator 11 and a wedge 12, and the outer surface 12a of the wedge 12 is processed according to the curvature of the outer peripheral surface 100a. At that time, a contact medium is interposed between the wedge 12 and the outer peripheral surface 100a. As shown in the figure, the longitudinal wave LW excited by the vibrator 11 propagates in the wedge 12 and undergoes mode conversion at the outer peripheral surface 100 a, and a transverse wave TW is generated in the steel pipe 100. This transverse wave TW is an SV wave. By using the SV wave, it is not necessary to use a contact medium having a high viscosity such as an SH wave, and therefore it is possible to efficiently inspect using a contact medium having a low viscosity.

  As shown in FIG. 2, the refraction angle θ at the incident point P, which is the point where the central axis A of the ultrasonic beam transmitted from the transducer 11 is incident on the outer surface 100a (the ultrasonic beam propagating through the steel pipe 100). The angle between the traveling direction and the normal H of the outer surface 100a at the incident point P is preferably 60 ° to 85 °. Within this numerical range, it is possible to efficiently generate both a surface-propagating transverse wave TW1 and a reflected-propagating transverse wave TW2 described later at the same time. In this embodiment, for example, the refraction angle θ of the transmitter 2 is set to 70 °.

  The frequencies of the surface propagation transverse wave TW1 and the reflected propagation transverse wave TW2 are preferably 0.5 MHz or more and 5 MHz or less. Furthermore, it is preferable to set it to 1 MHz or more and 1.5 MHz or less. Within this numerical range, since the directivity of the ultrasonic waves is dull, the intensity of the ultrasonic beam propagating to the outer peripheral surface 100a is less likely to be significantly lower than the beam center axis A, and the signal is obtained more clearly. be able to. In addition, since the low-frequency transverse wave has a long wavelength, it is possible to reduce the influence of the surface roughness of the outer peripheral surface 100a.

  As shown in FIG. 2, the transverse wave TW that has entered the steel pipe 100 propagates around the central axis A of the ultrasonic beam due to the curvature of the outer peripheral surface 100a. Of the transverse wave TW, the transverse wave TWa refracted toward the outer peripheral surface 100a with respect to the central axis A of the ultrasonic beam reaches the outer peripheral surface 100a without reaching the inner peripheral surface 100b of the steel pipe 100. Hereinafter, the transverse wave TWa is referred to as “surface reflected transverse wave”.

  As shown in FIG. 3A, for example, the surface reflected shear wave TWa1 is a transverse wave that is reflected once by the outer circumferential surface 100a between the transmitter 2 and the receiver 3 along the circumferential direction X of the steel pipe 100. The surface reflected transverse wave TWa2 is reflected twice by the outer peripheral surface 100a, and the surface reflected transverse wave TWa3 is reflected by the outer peripheral surface 100a three times. In this way, by repeating the reflection of only the outer peripheral surface 100a (curved surface), the propagation path (distance) of the surface reflected transverse wave TWa increases as the number of reflections increases, and the surface reflected transverse wave TWan shown in FIG. As described above, it can be regarded as being almost equal to the path that is asymptotic to the length of the arc of the steel pipe 100 corresponding to the distance between the transmitter 2 and the receiver 3 and propagates along the outer peripheral surface 100 a of the steel pipe 100.

  Here, FIG. 4 shows an A-scope image with the reception time of the received signal as the vertical axis and the reception intensity as the horizontal axis. In the A scope image, as shown in the figure, a signal S1 of a plurality of surface reflected transverse waves TWa is displayed, and another signal S2 is displayed immediately after the signal S1. This signal S2 can be confirmed from the distance between the transmitter 2 and the receiver 3 to be a signal caused by the surface propagation transverse wave TW1 propagating along the outer peripheral surface 100a of the steel pipe 100. Then, as shown in FIG. 5, the corresponding portions d1 and d2 corresponding to the thinned portions D1 and D2 in the two-dimensional image of the outer shape of the inspection object having the thinned portions D1 and D2 and the surface propagation transverse wave TW1 are well It can be seen that the surface propagation transverse wave TW1 propagates along the surface.

  Further, unlike the surface wave, the surface propagation transverse wave TW1 hardly propagates to the surface of the trunnion 102 via the welded portion 103 in the inspection target portion 101 having the welded portion 103 as shown in FIG. Therefore, it is possible to inspect a portion that is difficult to inspect with the conventional surface wave.

  On the other hand, as shown in FIG. 2, the transverse wave TWb refracted from the central axis A of the ultrasonic beam toward the inner peripheral surface 100 b reaches the inner peripheral surface 100 b without reaching the outer peripheral surface 100 a of the steel pipe 100. The transverse wave TWb is reflected by the inner peripheral surface 100b and reaches the outer peripheral surface 100a. And it similarly reflects on the outer peripheral surface 100a, and reaches | attains the inner peripheral surface 100b again. That is, the transverse wave TWb is a reflected propagation transverse wave TW2 that propagates while repeating reflection alternately between the outer peripheral surface 100a and the inner peripheral surface 100b of the steel pipe 100.

  Since this reflected propagation transverse wave TW2 repeats reflection alternately between the outer peripheral surface 100a and the inner peripheral surface 100b of the steel pipe 100, the propagation path is longer than the propagation path of the previous surface propagation transverse wave TW1. As shown in FIG. 4, a signal group S3 appears after the signal S2 of the surface propagation transverse wave TW1. From the distance between the transmitter 2 and the receiver 3, it can be seen that the signal S3 is a signal caused by the reflected propagation transverse wave TW2.

Next, changes in propagation paths of the surface propagation transverse wave TW1 and the reflected propagation transverse wave TW2 due to the thinned portion D will be described with reference to FIGS.
In a healthy inspected object in which the thinned portion D does not exist, the surface propagation transverse wave TW1 propagates from the transmitter 2 to the receiver 3 along the surface. However, as shown in FIG. 6A, when the thinned portion D exists on the outer peripheral surface 100a of the steel pipe 100, the surface propagation transverse wave TW1 propagates around along the surface of the thinned portion D by diffraction. . Therefore, the propagation time of the surface propagation transverse wave TW1 is longer than that of a healthy steel pipe, and the reception time is delayed. Therefore, as shown in FIG. 7, in the corresponding portion d corresponding to the thinned portion D on the two-dimensional image, a change occurs in the striped pattern of the surface propagation transverse wave TW1 as a change in the two-dimensional image. This change in the striped pattern is deformed into a convex shape in the direction in which the time increases in the direction of the time axis on the two-dimensional image (downward in the figure) due to the delay in the reception time by the thinned portion D. Thus, by observing the change in the striped pattern of the surface propagation transverse wave TW1 on the two-dimensional image, it is possible to easily evaluate the presence / absence and degree of the thinned portion D on the outer peripheral surface 100a side.

  On the other hand, as shown in FIG. 6A, the reflected propagation transverse wave TW2 is reflected by the thinned portion D and propagates along the path indicated by the symbol TW2a. Therefore, the propagation time of the reflected propagation transverse wave TW2 is shorter than the case of propagating the path TW2b in the case of a healthy steel pipe, and the reception time is shortened. Therefore, as shown in FIG. 7, in the corresponding portion d corresponding to the thinned portion D on the two-dimensional image, a change also occurs in the striped pattern of the reflected propagation transverse wave TW2 as a change in the two-dimensional image. This change in the striped pattern is deformed into a convex shape in the direction of time reduction (upward in the figure) in the direction of the time axis on the two-dimensional image due to the shortening of the reception time by the thinned portion D.

  Further, as shown in FIG. 6B, when the thinned portion D is present on the inner peripheral surface 100b of the steel pipe 100, the reflected propagation transverse wave TW2 is reflected by the thinned portion D. The stripe pattern changes at the corresponding portion d corresponding to the thinned portion D on the image. On the other hand, since the surface propagation transverse wave TW1 is not affected by the thinned portion D, the propagation time is the same as that of a healthy steel pipe. Therefore, the surface-propagating transverse wave TW1 has thinning information on the outer surface 100a, and the reflected-propagating transverse wave TW2 has thinning information on both the inner and outer surfaces 100a and 100b. Therefore, by observing the change in the striped pattern of both the surface propagation transverse wave TW1 and the reflected propagation transverse wave TW2 on the two-dimensional image, it is possible to easily identify whether the thinned portion D exists on the front or back of the steel pipe 100. The degree of the thinned portion D can also be evaluated.

  In the inspection, first, the transmitter 2 and the receiver 3 to which the position detector 5 is attached are placed facing the outer peripheral surface 100a of the steel pipe 100 with the concealing portion 101 interposed therebetween. Next, the distance between the probes of the transmitter 2 and the receiver 3 is set to a predetermined value, and scanning is performed in the axial direction Y, for example. The ultrasonic wave propagated through the thick portion of the steel pipe 100 is received by the receiver 3, and the received signal is generated through the signal processing unit 46 and the CPU 41, and displayed on the display unit 45. Then, the thinned portion D in the concealing portion 101 is evaluated by the change in the striped pattern of the surface propagation transverse wave TW1 and the reflected propagation transverse wave TW2 on the two-dimensional image.

  Further, the distance between the probes of the transmitter 2 and the receiver 3 is measured in advance, and a value obtained by dividing the distance by the sound velocity of the transverse wave is obtained, and the value is set as a reference propagation time. And it is also possible to obtain | require the thinning depth t by calculating | requiring a propagation time and the difference with reference | standard propagation time by the above-mentioned scanning. Further, since the thinning value of both the inner and outer surfaces 100a and 100b is added to the reflected propagation transverse wave TW2, the inner circumferential surface is obtained by removing the thinning value of the surface propagation transverse wave TW1 from the thinning value of the reflected propagation transverse wave TW2. It is also possible to obtain the thickness of only 100b.

  FIG. 8 shows an example of a two-dimensional image in an actual trunnion. In the example of the figure, in the portion corresponding to the trunnion, the reflected propagation transverse wave TW2 is attenuated and the stripe pattern does not clearly change, but the presence of the thinned portion D can be confirmed by the surface propagation transverse wave TW1. Thus, by generating the surface propagation transverse wave TW1 and the reflected propagation transverse wave TW2 at the same time, the thinning can be detected easily and reliably. It is also possible to obtain the thinning depth t from the two-dimensional image.

  However, since the first embodiment using the surface propagation transverse wave TW1 reflected and propagated only on the surface of the object to be inspected propagates along the surface shape by repeating fine reflection on the surface of the object to be inspected. It is superior to the second embodiment in that attenuation due to the surface shape can be suppressed and a clear received signal can be obtained.

Finally, mention is made of the possibilities of other embodiments. In the following embodiments, members similar to those in the above embodiment are denoted by the same reference numerals.
In the said embodiment, the thinning part D was demonstrated to the example as thickness reduction. However, the thickness reduction includes not only the thickness of the object to be inspected 100 decreased compared to the thickness of the sound object to be inspected due to corrosion, dents, or the like, but also the increased thickness. Further, in addition to the change in the thickness of the device under test 100, those that are deformed without the change in the thickness of the device under test 100 are also included. The change or deformation of the wall thickness may affect the change of the propagation time of the ultrasonic wave, and can be detected by the two-dimensional image as in the above embodiment.

  In the said embodiment, the steel pipe 100 was demonstrated to the example as a to-be-inspected body. However, the device under test 100 is not limited to a cylindrical body such as a pipe, and may be a container having a certain curvature, an elbow, or a curved plate member. In the above embodiment, the surface of the object to be inspected is described as the outer peripheral surface 100a of the steel pipe 100, and the back surface of the object to be inspected is described as the inner peripheral surface 100b. However, the front surface and the back surface are not limited to the outer surface and the inner surface. The front surface is a flaw detection surface on which the transmitter 2 and the receiver 3 are placed and scanned, and the back surface includes a surface facing the flaw detection surface.

  In the said embodiment, it was set as the concealment part 101 concealed by the trunnion 102 as another member welded to the steel pipe 100 as a test object part. However, the inspection target part 101 is not limited to the concealment part, and as shown in FIGS. 9 and 10, for example, thinning formed in a 4B pipe or a 6B pipe can also be detected. Further, the other member 102 is not limited to the trunnion 102, and may be a dummy support that is welded and fixed to a pipe, for example, a gantry, a hanger, a support, or the like as shown in FIG. Inspection of the portion concealed by these pipe support structures is possible.

  In the above embodiment, the refraction angle θ of the oblique probe 10 is set to 70 °. However, the refraction angle is not limited to the above numerical values and can be set as appropriate. For example, when the object to be inspected is a steel pipe as in the above embodiment, it may be set according to the curvature of the steel pipe 100.

  In the said embodiment, although the wedge 12 was processed according to the curvature, it is not restricted to this, Flat may be sufficient. In such a case, the contact portion between the wedge 12 and the outer peripheral surface 100a is reduced, but the transverse wave propagates with spreading as described above.

  INDUSTRIAL APPLICABILITY The present invention can be used as an ultrasonic inspection method and an inspection apparatus that detect a thinning generated in a pipe, a container, a curved plate material, or the like.

1: Ultrasonic inspection apparatus, 2: Transmitter, 3: Receiver, 4: Flaw detector, 5: Position detector, 10: Oblique probe, 11: Vibrator, 12: Wedge, 12a: Outer surface, 41 : CPU, 42: transmitting unit, 43: receiving unit, 44: position detecting unit, 45: display unit, 46: signal processing unit, 100: steel pipe (inspected object), 100a: outer peripheral surface (curved surface, surface, flaw detection surface) ), 100b: inner peripheral surface (back surface), 101: concealment portion (inspection target portion), 102: trunnion (other member), 103: welded portion, 104: reinforcing plate, A: central axis, D, D1, D2 : Thinning part (thinning etc.), d, d1, d2: corresponding part, H: normal, LW: longitudinal wave, P: incident point, S1, S2, S3: signal, TW: transverse wave, TWa: surface reflection Transverse wave, TW1: surface propagation transverse wave, TW2: reflected propagation transverse wave, X: circumferential direction (curving direction), Y: axial direction

Claims (8)

A transmitter and a receiver are arranged on the surface of the object to be inspected across the inspection target part, and an ultrasonic wave transmitted from the transmitter to the object to be inspected and propagated through the object to be inspected is received by the receiver. An ultrasonic inspection method for inspecting thinning of the inspection target part by receiving,
The surface of the object to be inspected is a curved surface that is convex toward the outside of the object to be inspected at least between the transmitter and the receiver.
The transmitter generates at least a transverse wave propagating along a propagation path along the curved surface (hereinafter referred to as “surface propagation transverse wave”) by repeating the reflection of only the curved surface a plurality of times.
An ultrasonic inspection method for inspecting thinning or the like of the inspection target part due to a delay in reception time of the surface propagation transverse wave by bypassing the thinning or the like. The ultrasonic inspection method according to claim 1, wherein the surface propagation transverse wave is an SV wave. The ultrasonic inspection method according to claim 1 or 2, wherein a frequency of the surface-propagating shear wave is 0.5 MHz or more and 5 MHz or less. The ultrasonic inspection method according to claim 1, wherein the inspection target part is a concealing part in which a surface of the inspection object is concealed by another member. 2. The transmitter further generates a transverse wave (hereinafter referred to as a “reflected propagation transverse wave”) that propagates by repeatedly reflecting between a surface of the object to be inspected and a back surface facing the surface. The ultrasonic inspection method in any one of -4. The receiver and the transmitter are moved along the curved surface, and the reception intensity of the surface propagation transverse wave and / or the reflected propagation shear wave is displayed on a two-dimensional image with the scanning position and reception time of the transmitter and receiver as axes. The ultrasonic inspection method according to any one of claims 1 to 5. The ultrasonic inspection method according to claim 1, wherein the receiver and the transmitter are arranged to face each other in a curved direction of the curved surface. An ultrasonic inspection apparatus used in the ultrasonic inspection method according to claim 1,
The surface of the object to be inspected is a curved surface that is convex toward the outside of the object to be inspected at least between the transmitter and the receiver.
The transmitter generates at least the surface-propagating shear wave,
An ultrasonic inspection apparatus that inspects the thinning of the inspection target part due to a delay in the reception time of the surface-propagating shear wave by bypassing the thinning.