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JPS5922180B2 - Defect position locating device using AE signal - Google Patents
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JPS5922180B2 - Defect position locating device using AE signal - Google Patents

Defect position locating device using AE signal

Info

Publication number
JPS5922180B2
JPS5922180B2 JP50109644A JP10964475A JPS5922180B2 JP S5922180 B2 JPS5922180 B2 JP S5922180B2 JP 50109644 A JP50109644 A JP 50109644A JP 10964475 A JP10964475 A JP 10964475A JP S5922180 B2 JPS5922180 B2 JP S5922180B2
Authority
JP
Japan
Prior art keywords
signal
time difference
defect position
measured
converters
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP50109644A
Other languages
Japanese (ja)
Other versions
JPS5233786A (en
Inventor
幸 五十嵐
久隆 安藤
直己 角田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Doryokuro Kakunenryo Kaihatsu Jigyodan
Original Assignee
Doryokuro Kakunenryo Kaihatsu Jigyodan
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Doryokuro Kakunenryo Kaihatsu Jigyodan filed Critical Doryokuro Kakunenryo Kaihatsu Jigyodan
Priority to JP50109644A priority Critical patent/JPS5922180B2/en
Publication of JPS5233786A publication Critical patent/JPS5233786A/en
Publication of JPS5922180B2 publication Critical patent/JPS5922180B2/en
Expired legal-status Critical Current

Links

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  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 この発明は、被測定物から発生するAE信号(アコース
ティック・工ミッション信号)を検出し、被測定物中の
欠陥位置を標定する装置の改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement of an apparatus for detecting an AE signal (acoustic/machining signal) generated from an object to be measured and locating a defect position in the object to be measured.

固体材料に対立が作用すると、欠陥箇所からAE信号が
放出され、固体材料中を伝播する。
When a conflict acts on a solid material, an AE signal is emitted from the defect location and propagates through the solid material.

かかる現象を応用して、原子炉圧力容器や一次冷却系配
管などの構造物の稼動中に生ずる各種欠陥の進展を監視
すると共に、それらの健全性を常時診断し、それらの構
造物の安全性を確保することができる。従来のAE信号
を用いた欠陥位置標定技術は、被測定物に貼設した一組
のAE信号変換子によつてAE信号を検出し、このAE
信号の立上り部において一定のスレッショルド電圧を越
えた時点を基準として両AE信号変換子に到達した時間
差を測定し、被測定物におけるAE信号伝播速度との関
係からAE信号の発生を算出している。ところで、被測
定物が原子炉容器や一次冷却系配管などの構造物のよう
に大きな場合には、AE信号の伝播距離が長くなり、こ
のため伝播してきたAE信号はその振幅が減衰するばか
りでなく、縦波、横波等二つ以上の波に分離してしまう
。このように波形のくすれたAE信号について、スレッ
ショルド電圧を越えた時点を基準とする従来の方法では
、スレッショルド電圧の設定が難かしく、伝播速度の早
い縦波がスレッショルド電圧を越える場合、伝播速度の
遅い横波がスレッショルド電圧を越える場合が不規則に
生じ測定精度が低下する欠点があつた。この発明の目的
は、上記の如き従来技術の欠点を解消し、測定誤差の小
さいAE信号による欠陥位置標定装置を得ることにある
By applying this phenomenon, we can monitor the progress of various defects that occur during the operation of structures such as reactor pressure vessels and primary cooling system piping, and constantly diagnose their health to ensure the safety of these structures. can be ensured. Conventional defect position locating technology using AE signals detects the AE signal with a set of AE signal converters attached to the object to be measured.
The time difference between the two AE signal converters is measured based on the point at which the signal exceeds a certain threshold voltage at the rising edge of the signal, and the generation of the AE signal is calculated from the relationship with the AE signal propagation speed in the object under test. . By the way, when the object to be measured is a large structure such as a nuclear reactor vessel or primary cooling system piping, the propagation distance of the AE signal becomes long, and as a result, the amplitude of the propagated AE signal is only attenuated. Instead, it separates into two or more waves such as longitudinal waves and transverse waves. For AE signals with such dull waveforms, it is difficult to set the threshold voltage using the conventional method that uses the point at which the threshold voltage is exceeded as a reference, and when a longitudinal wave with a fast propagation speed exceeds the threshold voltage, the propagation speed The problem was that the slow transverse waves of the waveforms irregularly exceeded the threshold voltage, reducing measurement accuracy. SUMMARY OF THE INVENTION An object of the present invention is to eliminate the drawbacks of the prior art as described above and to provide a defect position locating device using an AE signal with small measurement errors.

この発明は、一組のAE信号変換子を有し、該変換子か
らのAE信号を夫々ピークホールド回路に導入し、予め
決められた一定時間ピークホールドした信号を時間差測
定回路に導き前記ピークホールド信号の立下り位置を基
準として時間差を求めるようにすると共に、前記AE信
号を到達順位弁別回路に導き、前記時間差測定回路から
の信号と前記到達順位弁別回路からの信号により欠陥位
置を標定するようにしたAE信号による欠陥位置標定装
置である。
The present invention has a set of AE signal converters, introduces the AE signals from the converters into respective peak hold circuits, and guides the peak-held signal for a predetermined fixed period of time to a time difference measuring circuit. The time difference is determined using the fall position of the signal as a reference, and the AE signal is guided to the arrival order discrimination circuit, and the defect position is located by the signal from the time difference measurement circuit and the signal from the arrival order discrimination circuit. This is a defect position locating device using AE signals.

以下図面に基づきこの発明について詳述する。The present invention will be explained in detail below based on the drawings.

第1図はこの発明の一実施例に係る装置のプロツク図で
あり、被測定物が1次元構造物の場合について適用した
例である。被測定物1の両端適宜箇所に一対のAE信号
変換子2a,2bが貼設されている。各AE信号変換子
2a,2bからの出力は夫々アンプ/フイルタ3a,3
b及びピークホールド回路4a,4bに接続された後、
時間差測定回路5に導かれ、更に信号位置計算装置6へ
送られる。また、前記アンプ/フイルタ3a,3bから
の出力は到達順位弁別回路7に送られ、更に前記の信号
位置計算装置6へ送られる。次にこの装置の動作につい
て説明する。
FIG. 1 is a block diagram of an apparatus according to an embodiment of the present invention, and is an example applied to a case where the object to be measured is a one-dimensional structure. A pair of AE signal converters 2a and 2b are pasted at appropriate locations on both ends of the object to be measured 1. The output from each AE signal converter 2a, 2b is output to an amplifier/filter 3a, 3, respectively.
After being connected to b and peak hold circuits 4a and 4b,
The signal is guided to a time difference measuring circuit 5 and further sent to a signal position calculation device 6. Further, the outputs from the amplifier/filters 3a and 3b are sent to the arrival rank discrimination circuit 7, and further sent to the signal position calculation device 6. Next, the operation of this device will be explained.

被測定物1のD点(AE信号変換子2a寄りの点)に欠
陥があるものと仮定する。被測定物1に外力が加わると
、欠陥DからAE信号が発生し、被測定物中を伝播する
。この機械的AE信号はAE信号変換子2a,2bによ
り奄気信号に変換される。AE信号変換子2a,2bか
らの出力を示すと夫夫第2図A,bの如くであり、欠陥
Dは変換子2a寄りにあるので、変換子2aの方に早く
AE信号が現われ、また欠陥Dと変換子2bとの距離は
長いので、変換子2bに現われるAE信号は伝播速度の
早い縦波成分と伝播速度の遅い横波成分に分離している
。このようにして得られた信号は夫々アンプ/フイルタ
3a,3bに送られる。アンプ部によつて適宜増幅し、
フイルタ部によつて環境雑音の比較的多い低周波成分を
減衰させ、AE信号のS/N比を向上させている。かく
して得られたAE信号はピークホールド回路4a,4b
に送られる。ビークホールドした信号波形を第2図C,
dに示す。点線はAE信号である。ピークホールド回路
は、入力信号の最も高いレベルを一定時間だけ保持する
ものであり、保持時間の最適値は被測定物の大きさによ
つても異なる。第2図dのようにAE信号が長距離伝播
し二つ以上の波に分離しても常に横波成分で検知しうる
ように、保持時間は縦波成分と横波成分との最大時間差
より大としておく。このようにして得られたピークホー
ルド信号の立下り部を測定の基準とし、時間差測定回路
5で時間差信号第2図eを作り、両AE信号変換子に到
達したAE信号の時間差を測定するのである。この時間
差の測定は、例えば第2図eに示す時間差信号をゲート
信号とし、一定周波数で発振する発振器からの出力を制
御し、パルスカウンタにより計数するようにすればよい
。次に、到達順位弁別回路7は、AE信号がどちらの変
換子に先に到達したかを判別するもので、これによつて
欠陥が変換子2a寄りにあるか変換子2b寄りにあるか
を判別することができる。到達時間差に関する情報と到
達順位に関する情報は信号位置計算装置6へ送られ、A
E信号伝播速度との関係からAE信号の発生位置を計算
する。また、AE信号の直前、直後にたまたま雑音が入
つた場合には誤動作することも予想されるが、長時間の
測定を行い、データを累積することによつて雑音による
誤差を統計的に排除することができる。なお、この実施
例}ま被測定物が1次元構造物の場合について適用した
例であるが、3〜4個のAE信号変換子を設置すること
によつて、2次元構造物等についても同様に欠陥位置を
標定しうることは言うまでもない。この発明(ま上記の
ように、AE信号のピーク電圧位置を基準として一組の
AE信号変換子に到達するAE信号の到達時間差の測定
を行うよう構成しているので、被測定物が大きくAE信
号の伝播距離が長大となり、波形のくずれを生ずるよう
な場合においても正確な到達時間差を測定することがで
き、したがつて欠陥位置標定の誤差を低減させることが
できる。
It is assumed that there is a defect at point D of the object to be measured 1 (a point close to the AE signal converter 2a). When an external force is applied to the object to be measured 1, an AE signal is generated from the defect D and propagates through the object to be measured. This mechanical AE signal is converted into an energy signal by AE signal converters 2a and 2b. The outputs from the AE signal converters 2a and 2b are shown in Figure 2 A and b, and since the defect D is closer to the converter 2a, the AE signal appears earlier in the converter 2a, and Since the distance between the defect D and the transducer 2b is long, the AE signal appearing on the transducer 2b is separated into a longitudinal wave component with a fast propagation speed and a transverse wave component with a slow propagation speed. The signals thus obtained are sent to amplifier/filters 3a and 3b, respectively. Amplify as appropriate by the amplifier section,
The filter section attenuates relatively large low frequency components of environmental noise, improving the S/N ratio of the AE signal. The AE signal thus obtained is sent to peak hold circuits 4a and 4b.
sent to. The peak held signal waveform is shown in Figure 2C,
Shown in d. The dotted line is the AE signal. A peak hold circuit holds the highest level of an input signal for a certain period of time, and the optimum value of the holding time varies depending on the size of the object to be measured. The retention time is set to be larger than the maximum time difference between the longitudinal wave component and the transverse wave component so that even if the AE signal propagates over a long distance and separates into two or more waves as shown in Figure 2d, the transverse wave component can always be detected. put. Using the falling part of the peak hold signal obtained in this way as a reference for measurement, the time difference measurement circuit 5 generates a time difference signal e in Figure 2, and measures the time difference between the AE signals that have reached both AE signal converters. be. This time difference can be measured by using, for example, the time difference signal shown in FIG. 2e as a gate signal, controlling the output from an oscillator that oscillates at a constant frequency, and counting by a pulse counter. Next, the arrival order discrimination circuit 7 determines which transducer the AE signal reached first, and thereby determines whether the defect is closer to the transducer 2a or 2b. can be determined. Information regarding the arrival time difference and information regarding the arrival order are sent to the signal position calculation device 6,
The generation position of the AE signal is calculated from the relationship with the E signal propagation velocity. Additionally, malfunctions can be expected if noise happens to occur immediately before or after the AE signal, but errors due to noise can be statistically eliminated by performing long-term measurements and accumulating data. be able to. Although this example is applied to a case where the object to be measured is a one-dimensional structure, the same can be applied to a two-dimensional structure by installing three to four AE signal converters. Needless to say, it is possible to locate the defect position. This invention (as mentioned above, since it is configured to measure the arrival time difference of the AE signals reaching a set of AE signal converters using the peak voltage position of the AE signals as a reference, it is possible to Even when the signal propagation distance is long and the waveform is distorted, the arrival time difference can be measured accurately, and errors in defect position location can therefore be reduced.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の−実施例に係る欠陥位置標定装置の
プロツク図、第2図a−eは第1図に示す装置の動作波
形図である。 1・・・・・・被測定鋤、2a,2b・・・・・・AE
信号変換子、4a,4b・・・・・・ピークホールド回
路、5・・・・・・時間差測定回路、7・・・・・到達
順位弁別回路。
FIG. 1 is a block diagram of a defect position locating device according to an embodiment of the present invention, and FIGS. 2 a to 2 e are operational waveform diagrams of the device shown in FIG. 1. 1...Plow to be measured, 2a, 2b...AE
Signal converter, 4a, 4b... Peak hold circuit, 5... Time difference measuring circuit, 7... Arrival rank discrimination circuit.

Claims (1)

【特許請求の範囲】[Claims] 1 一組のAE信号変換子を有し、該変換子からのAE
信号を夫々ピークホールド回路に導入し、予め決められ
た一定時間ピークホールドした信号を時間差測定回路に
導き前記ピークホールド信号の立下り位置を基準として
時間差を求めるようにすると共に、前記AE信号を到達
順位弁別回路に導き、前記時間差測定回路からの信号と
前記到達順位弁別回路からの信号により欠陥位置を標定
するようにしたことを特徴とするAE信号による欠陥位
置標定装置。
1 has a set of AE signal converters, and the AE from the converters
Each signal is introduced into a peak hold circuit, and the signal whose peak is held for a predetermined period of time is led to a time difference measuring circuit, where the time difference is determined based on the falling position of the peak hold signal, and the AE signal is reached. A defect position locating device using an AE signal, characterized in that the defect position is guided to a rank discriminating circuit, and the defect position is located by a signal from the time difference measuring circuit and a signal from the arrival rank discriminating circuit.
JP50109644A 1975-09-10 1975-09-10 Defect position locating device using AE signal Expired JPS5922180B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP50109644A JPS5922180B2 (en) 1975-09-10 1975-09-10 Defect position locating device using AE signal

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP50109644A JPS5922180B2 (en) 1975-09-10 1975-09-10 Defect position locating device using AE signal

Publications (2)

Publication Number Publication Date
JPS5233786A JPS5233786A (en) 1977-03-15
JPS5922180B2 true JPS5922180B2 (en) 1984-05-24

Family

ID=14515496

Family Applications (1)

Application Number Title Priority Date Filing Date
JP50109644A Expired JPS5922180B2 (en) 1975-09-10 1975-09-10 Defect position locating device using AE signal

Country Status (1)

Country Link
JP (1) JPS5922180B2 (en)

Also Published As

Publication number Publication date
JPS5233786A (en) 1977-03-15

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