JP2011214891A - Array ultrasonic flaw detector - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide an array ultrasonic flaw detector capable of improving the SN ratio by reducing the surface echoes relative to flaw echoes, when performing automatic flaw detection which uses array probe.SOLUTION: The array ultrasonic flaw detector includes the array probe (10), having a plurality of excitation elements driven by receiving an excitation signal for having a test body irradiated with an ultrasonic beam via a contact medium, receiving an ultrasonic wave reflected by the test body surface and an acoustic discontinuous part inside the test body through the contact medium, and converting the ultrasonic waves into an electrical signal; and a transceiver (20) for driving the array probe, by transmitting the excitation signal and performing flaw detection of the test body by receiving the electric signal. When an excitation signal is transmitted or an electrical signal is received, the transceiver does not excite several elements or a single element on the center among the excitation elements in a covering range required for flaw detection of the test body, but will transmit the excitation signal to partially excited elements corresponding to several elements or a single element on both ends, and receives an electrical signal that is converted by the partially excited elements.

Description

  The present invention relates to ultrasonic flaw detection for nondestructively inspecting flaws generated in a solid, and more particularly to an array ultrasonic flaw detection apparatus with an improved S / N ratio.

  First, a description will be given of an example of a search method using a conventional automatic flaw detector using a case where a test object is a round bar. FIG. 4 is an explanatory view of vertical flaw detection when performing round bar automatic flaw detection in a conventional automatic flaw detection apparatus, and FIG. 5 is an explanatory diagram of oblique angle flaw detection when performing round bar automatic flaw detection in a conventional automatic flaw detection apparatus. (For example, see Non-Patent Document 1). 4 and 5, a vertical probe 11 and an oblique probe 12 used for automatic flaw detection of the round bar 1 are shown. Incidentally, two oblique angle probes 12 in FIG. 5 are arranged and are shown as 12a and 12b, respectively.

  As shown in FIG. 4, the round bar automatic flaw detection uses the vertical probe 11 to inject the ultrasonic beam vertically into the round bar 1 to detect the inside of the round bar 1. Alternatively, as shown in FIG. 5, an ultrasonic beam is obliquely incident on the round bar 1 using the oblique angle probes 12a and 12b, and the surface layer portion of the round bar 1 is detected. At this time, although not illustrated, the round bar 1 is filled with a liquid such as water as a contact medium.

  In the conventional round bar automatic flaw detection, the entire surface flaw detection is performed by rotating a probe around the round bar. In contrast to this method, in recent years, there is an automatic flaw detector of a type in which an array probe is arranged around and the excitation position of the ultrasonic beam is rotated instead of rotating the probe (see, for example, Patent Document 1). ).

  This Patent Document 1 discloses an apparatus in which an array probe is arranged around a round bar to detect a flaw on a surface layer portion, and an ultrasonic beam is incident obliquely. This corresponds to the oblique flaw detection shown in FIG. Naturally, the vertical flaw detection shown in FIG. 4 can also be realized by arranging the array probe around the round bar.

  FIG. 6 is an explanatory diagram of vertical flaw detection by a conventional array ultrasonic flaw detector. The conventional array ultrasonic flaw detector shown in FIG. 6 has an array probe 10 and a transmitter / receiver 20. By arranging the array probe 10 around the round bar 1, the center of the round bar 1 is arranged. This shows a situation where the flaw 2 in FIG.

  Here, the array probe 10 has a plurality of excitation elements that are driven by receiving external excitation signals. Furthermore, the array probe 10 irradiates an ultrasonic beam toward the round bar 1 as a test body through a contact medium such as water, and is reflected by the surface of the test body and the acoustic discontinuity inside the test body. The received ultrasonic wave is received through the contact medium and converted into an electrical signal.

  On the other hand, the transmitter / receiver 20 drives the array probe 10 by transmitting an excitation signal, and receives the electrical signal converted by the array probe 10 as a response to the round probe as a test specimen. Perform 1 flaw detection.

  FIG. 6 shows three states (a) to (c) over time. FIG. 6A shows a state in which the element on the left side of the array probe 10 is excited to detect a flaw. Similarly, FIG. 6B shows a state in which an element located near the center of the array probe 10 is excited and flawed, and FIG. 6C shows an element located on the right side of the array probe 10. Shows a state where the flaw is excited and the flaw is detected.

  By continuously performing these states (a) to (c), the excitation position rotates around the round bar, which is an alternative to the rotation of the probe. The number of excitation elements is determined so as to satisfy the beam width required by the system. The range covered by the number of excitation elements is referred to herein as the cover range. The distance and speed for moving the excitation position vary depending on the system.

JP 2009-150679 A

Japan Nondestructive Inspection Association, “New Nondestructive Inspection Handbook” p 972, Nikkan Kogyo Shimbun (1992)

However, the prior art has the following problems.
In conventional array ultrasonic flaw detectors, when vertical flaw detection is performed, the degradation of the signal-to-noise ratio due to surface echoes reflected from the round bar surface entering the flaw detection gate has been a problem. Here, the signal component S is a flaw echo, and the noise component N is a tail of the surface echo. In order to improve the S / N ratio, it is necessary to reduce the surface echo relative to the scratch echo, and it is desired to improve the performance of the array ultrasonic flaw detector by improving the S / N ratio.

  The present invention has been made to solve the above-described problems. When performing an automatic flaw detection using an array probe, the surface echo is reduced relative to the flaw echo, and the SN ratio is reduced. It is an object of the present invention to obtain an array ultrasonic flaw detector that improves the above.

  An array ultrasonic flaw detector according to the present invention has a plurality of excitation elements that are driven by receiving an excitation signal, irradiates an ultrasonic beam toward a test body via a contact medium, An array probe that receives an ultrasonic wave reflected by an acoustic discontinuity inside the test body through a contact medium and converts it into an electrical signal, and transmits an excitation signal to drive the array probe. In an array ultrasonic flaw detector having a transceiver for receiving a test signal by receiving an electrical signal converted by the array probe, the transmitter / receiver is a test object flaw among a plurality of excitation elements. When an excitation element in the cover range that satisfies the beam width required for the transmission is specified and an excitation signal is transmitted and an electrical signal is received, the middle number of the excitation elements in the cover range or a single element Several elements at both ends. There are those sending the excitation signal to the partial excitation element corresponding to a single element, it receives the electrical signal converted by the partial excitation element.

  According to the array ultrasonic flaw detector according to the present invention, when performing automatic flaw detection using an array probe by not exciting several elements or a single element in the middle of the cover range in the array probe, It is possible to obtain an array ultrasonic flaw detector in which the surface echo is reduced relative to the flaw echo and the SN ratio is improved.

It is explanatory drawing of the vertical flaw detection by the array ultrasonic flaw detector in Embodiment 1 of this invention. It is explanatory drawing regarding the SN ratio improvement of the array ultrasonic flaw detector in Embodiment 1 of this invention. It is the figure which showed the simulation result of the surface echo and the flaw echo in Embodiment 1 of this invention. It is explanatory drawing of the vertical flaw detection at the time of performing the round bar automatic flaw detection in the conventional automatic flaw detector. It is explanatory drawing of the angle flaw detection at the time of performing the round bar automatic flaw detection in the conventional automatic flaw detector. It is explanatory drawing of the vertical flaw detection by the conventional array ultrasonic flaw detector.

  Hereinafter, preferred embodiments of an array ultrasonic flaw detector according to the present invention will be described with reference to the drawings.

Embodiment 1 FIG.
FIG. 1 is an explanatory diagram of vertical flaw detection by the array ultrasonic flaw detector according to Embodiment 1 of the present invention. FIG. 1 corresponds to FIG. 6 describing the conventional method, and the method of exciting the array probe 10 is different.

  First, the configuration of the array ultrasonic flaw detector according to the first embodiment will be described with reference to FIG. The array ultrasonic flaw detection apparatus according to the first embodiment shown in FIG. 1 includes an array probe 10 and a transmitter / receiver 20 and detects a flaw 2 at the center of a round bar 1 to be flaw detected. . Here, it is assumed that the round bar 1 and the array probe 10 have a curvature in the same direction. That is, it is not bent in the direction perpendicular to the paper surface shown in FIG. 1, and the center of curvature is on the lower side of FIG.

  The transceiver 20 electrically excites the array probe 10 and processes electrical signals from the array probe 10. In FIG. 1, the three states (a) to (c) with the passage of time are shown, as in FIG. 6 describing the conventional method.

  Next, the operation of the array ultrasonic flaw detector according to the first embodiment will be described. The transceiver 20 transmits an electrical excitation signal to the array probe 10. The transmitter / receiver 20 according to the conventional method described with reference to FIG. 6 transmits the excitation signal to the array elements within the cover range. On the other hand, the transmitter / receiver 20 in the present invention has the same cover range, but does not excite a few elements or a single element in the middle, and transmits an excitation signal that excites several elements or a single element at both ends. To do.

  An ultrasonic beam is emitted from the element partially excited in this way, and the ultrasonic beam is irradiated to the flaw 2 at the center of the round bar 1. Then, the ultrasonic wave reflected by the flaw 2 at the center of the round bar 1 traces the propagation path in the reverse direction and is received by the array probe 10.

  Even at the time of reception, reception is performed by ignoring several elements or a single element in the middle of the elements within the cover range. As shown in FIGS. 1A to 1C, the excitation position rotates around the round bar 1 by continuously performing such excitation and reception as shown in FIGS. This is an alternative to rotating the child.

Next, the reason why the SN ratio of vertical flaw detection is improved in the array ultrasonic flaw detector according to the present invention will be described. FIG. 2 is an explanatory diagram relating to the improvement of the SN ratio of the array ultrasonic flaw detector according to Embodiment 1 of the present invention. As described with reference to FIG. 1, the technical feature of the present invention is not to excite a few elements or a single element in the middle of the cover range. Therefore, the elements on the left side are array A, and the elements on the right side are array B, with elements not excited. In this case, the status of sending and receiving is
(Case 1) Transmission / reception by array A (Case 2) Transmission / reception by array B (Case 3) Transmission by array A, reception by array B (Case 4) Transmission by array B, reception by array A Can do.

  In (Case 1) and (Case 2), the echo is received in the same way, not the surface echo, so there is no difference between the two echoes. However, (Case 3) and (Case 4) are different in both echoes. Thus, taking the case of (Case 3) as an example, the difference between both echoes will be described with reference to FIG.

  First, reception of a flaw echo will be described with reference to FIG. The ultrasonic beam excited by the array A propagates toward the center of the round bar 1 with the main component at the center of the sound axis, and is reflected by the flaw 2 at the center of the round bar 1. Since the flaw 2 at the center of the round bar 1 is small, the reflected wave propagates in all directions, and there is no directivity. Therefore, the array B can be sufficiently received, and the flaw echo is received by the array B with a large amplitude as in the case of the array A.

  On the other hand, the fact that the surface echo is different will be described with reference to FIG. The ultrasonic beam excited by the array A is reflected by the surface of the round bar 1, but the main component at the center of the sound axis does not propagate in the direction of the array B. On the other hand, the component propagated at a slightly different angle from the sound axis is reflected on the surface of the round bar 1, received by the array B, and becomes a surface echo. Since the component propagated in a slightly different direction from the sound axis has a smaller beam intensity than the main component at the center of the sound axis, the amplitude is relatively smaller than that of the flaw echo.

  In (Case 4), since transmission / reception is only reversed from (Case 3), similarly, the amplitude of the surface echo is relatively smaller than that of the flaw echo. Accordingly, even when considered as a whole of (Case 3) and (Case 4), the amplitude of the surface echo is smaller than that of the flaw echo. Here, since the surface echo is a noise component and the flaw echo is a signal component, the S / N ratio is improved as a result.

  In order to confirm that the surface echo is relatively smaller than the scratch echo unless the middle or single element in the middle of the cover is excited, the echo was obtained by simulation. FIG. 3 is a diagram showing simulation results of surface echoes and flaw echoes in the first embodiment of the present invention.

The response characteristic of the array probe 10 is a broadband with a frequency of 7 MHz, and the round bar 1 has a diameter of 20 mm. The coverage of the array probe 10 is 16 channels,
(Pattern 1) Transmission / reception of all 16 channels (Pattern 2) FIG. 3 shows the results of obtaining echoes in two patterns of transmission / reception ignoring the middle 6 channels out of 16 channels.

  FIG. 3A shows surface echoes and flaw echoes. FIG. 3B shows an enlarged vertical axis of FIG. 3A because it is difficult to compare flaw echoes only with FIG. 3A.

  In FIG. 3, the echo indicated by the solid line is the echo received when all 16 channels are transmitted and received (pattern 1). The echo indicated by the dotted line is an echo received when transmission / reception is performed while ignoring the middle 6 channels out of 16 channels (pattern 2).

  As shown in FIG. 3B, when comparing the amplitude of the solid line according to (Pattern 1) and the amplitude of the dotted line according to (Pattern 2), the surface echoes are transmitted and received while ignoring the middle 6 channels. The amplitude of the echo is −13, 9 dB. On the other hand, when the flaw echo is compared with the amplitude of the solid line by (Pattern 1) and the amplitude of the dotted line by (Pattern 2), the amplitude of the flaw echo is only -8.2 dB. In this way, it is confirmed that the amplitude of the surface echo is relatively small compared with the amplitude of the flaw echo when the middle few elements or a single element in the cover range is not excited (pattern 2). did it.

  In an actual system, the tailing of the surface echo in the flaw detection gate becomes a noise component. If the surface echo itself is reduced, the noise component due to such tailing is also reduced. Therefore, the S / N ratio can be improved by not exciting several elements or a single element in the middle of the cover range.

  Although the simulation result in FIG. 3 shows a case where transmission / reception is performed while ignoring the middle 6 channels of the 16 channels, such excitation conditions are not always optimal. It is considered that the optimum condition varies depending on the diameter and frequency of the round bar 1. Therefore, the transmitter / receiver 20 has a function of changing the excitation condition according to the diameter and frequency of the round bar 1 and can perform optimum flaw detection according to the diameter and frequency of the round bar 1.

  In addition, although Embodiment 1 mentioned above demonstrated the case where a test body is the round bar 1, this invention is not limited to a round bar. It can also be applied to flaw detection on test specimens such as pipes and billets. In this case, the curvature of the acoustic radiation surface of the array probe 10 need not be the same as that of the test body.

  As described above, according to the first embodiment, by performing automatic flaw detection without exciting several elements or a single element in the middle of the cover range in the array probe, the amplitude of the surface echo is reduced. It can be reduced relative to the amplitude. As a result, an array ultrasonic flaw detector with an improved SN ratio can be realized.

  10 array probe, 20 transceiver.

Claims (3)

A plurality of excitation elements driven by receiving an excitation signal, irradiating the test body with an ultrasonic beam via a contact medium, and an acoustic discontinuity in the surface of the test body and in the test body An array probe that receives the ultrasonic waves reflected at the contact medium through the contact medium and converts them into electrical signals;
An array ultrasonic flaw detector comprising: a transmitter / receiver that transmits the excitation signal, drives the array probe, and receives the electric signal converted by the array probe to flaw the specimen. In the device
The transmitter / receiver specifies an excitation element in a cover range that satisfies a beam width required for flaw detection of the specimen, and transmits the excitation signal and receives the electrical signal among the plurality of excitation elements. When performing the above, the excitation signal within the cover range is not excited in the middle several elements or single elements, and the excitation signal is sent to the partial excitation elements corresponding to several elements or single elements at both ends. An array ultrasonic flaw detector characterized by transmitting and receiving the electric signal converted by the partial excitation element. The array ultrasonic flaw detector according to claim 1,
The array ultrasonic flaw detector is characterized in that the transmitter / receiver has a function of changing the excitation condition according to the characteristics and frequency of the specimen and transmitting the excitation signal. The array ultrasonic flaw detector according to claim 1 or 2,
The array probe is configured so that an acoustic radiation surface facing the test body has the same curvature as that of the test body.

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