JPH09257763A - Array ultrasonic flaw detection method and apparatus therefor - Google Patents

Array ultrasonic flaw detection method and apparatus therefor

Info

Publication number
JPH09257763A
JPH09257763A JP8066151A JP6615196A JPH09257763A JP H09257763 A JPH09257763 A JP H09257763A JP 8066151 A JP8066151 A JP 8066151A JP 6615196 A JP6615196 A JP 6615196A JP H09257763 A JPH09257763 A JP H09257763A
Authority
JP
Japan
Prior art keywords
array
scanning
peak
calculator
sensitivity distribution
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.)
Pending
Application number
JP8066151A
Other languages
Japanese (ja)
Inventor
Tomonori Masuda
智紀 増田
Kazuhiro Ito
一博 伊藤
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.)
Tokyo Gas Co Ltd
Original Assignee
Tokyo Gas Co Ltd
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 Tokyo Gas Co Ltd filed Critical Tokyo Gas Co Ltd
Priority to JP8066151A priority Critical patent/JPH09257763A/en
Publication of JPH09257763A publication Critical patent/JPH09257763A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/04Wave modes and trajectories
    • G01N2291/044Internal reflections (echoes), e.g. on walls or defects

Abstract

PROBLEM TO BE SOLVED: To accurately measure the dimension of a reflecting object (flaw) by calculating the max. scanning quantity wherein the peak of the receiving sensitivity distribution between the elements of an array probe is received within the range of the definite distance from the center of a transmission element group. SOLUTION: An array probe 1 is set to a flaw detection place and elements are electronically driven in the arranging direction of them while timing is controlled by an array controller 3. The scanning distance of the probe 1 at this time is calculated by a scanning quantity calculator 4. The ultrasonic waves transmitted from the elements are reflected by a reflecting object and the reflected waves therefrom are received by the respective elements. The receiving sensitivities of the respective elements and the distribution state thereof are calculated by a sensitivity distribution calculator 5. A peak detector 6 calculates the peak of this distribution state. A flaw length calculator 7 calculates the max. scanning quantity wherein the peak of the receiving sensitivity distribution is received within the range of the definite distance from the center of a transmission element group from the scanning quantity and peak calculated by the scanning quantity calculator 4 and the peak detector 6 to calculate the length of the reflecting object (flaw) from the calculated value.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、配列した複数の微
細な素子を有するアレイ探触子を用いて例えば溶接箇所
の探傷を行う方法及びその装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method and an apparatus for detecting flaws in, for example, a welded portion by using an array probe having a plurality of arrayed fine elements.

【0002】[0002]

【従来の技術】従来のアレイ超音波探傷法としては、次
のような方法が知られている。 a.図8(a)(b)に示すように配列した複数の微細
な素子2…を有するアレイ探触子1を用いて、その駆動
するタイミングを変え、あるいは駆動する素子2…のセ
ットを切り替え、さらにそれらの組み合わせによって超
音波の電子的な走査、偏向、集束を可能とする技術であ
って、(a′)は電子偏向、(b′)は電子集束の状態
を示すものである。
2. Description of the Related Art The following method is known as a conventional array ultrasonic flaw detection method. a. By using the array probe 1 having a plurality of fine elements 2 arranged as shown in FIGS. 8A and 8B, the driving timing is changed or the set of elements 2 to be driven is switched, Further, it is a technique that enables electronic scanning, deflection and focusing of ultrasonic waves by a combination thereof, where (a ') shows electron deflection and (b') shows electron focusing.

【0003】b.図8(a)(b)に示すアレイ探触子
1の各素子2…から発信した信号であって、反射体(き
ず)から反射した信号を各素子2…で夫々独立に受信を
行い、その素子2…間の受信感度分布、及び受信時間分
布から反射体(きず)の形状を推定する技術(例えば特
願平7−140928号発明)。
B. The signals transmitted from the elements 2 of the array probe 1 shown in FIGS. 8A and 8B, which are reflected from the reflectors (scratches), are individually received by the elements 2. A technique for estimating the shape of a reflector (scratch) from the reception sensitivity distribution between the elements 2 ... And the reception time distribution (for example, Japanese Patent Application No. 7-140928).

【0004】c.図9(a)(b)は従来の探触子1a
を機械的に走査(移動)させて行うきず長さの測定方法
を示すもので、例えば(a)において、溶接部Aに存在
するきずの場合、発見したきずに対して予めそのエコー
高さが最大となる位置Pを見つけてその位置から溶接線
方向に探触子1aを走査し、(b)に示すように、一定
の感度を超える範囲の長さ、あるいは最大エコー高さの
半分以上のエコー高さhとなる範囲の長さlをきずの長
さとする方法(JISZ 3060−1996,日本建
築学会基準−1989)である。
C. 9A and 9B show a conventional probe 1a.
Fig. 2 shows a method for measuring a flaw length by mechanically scanning (moving) the, for example, in the case of a flaw existing in the welded portion A in (a), the echo height of the flaw found in advance is After finding the maximum position P and scanning the probe 1a from that position in the welding line direction, as shown in (b), the length of the range exceeding a certain sensitivity, or a half or more of the maximum echo height is detected. This is a method (JISZ 3060-1996, Architectural Institute of Japan Standard-1989) in which the length l in the range of the echo height h is used as the flaw length.

【0005】[0005]

【発明が解決しようとする課題】しかし、上記従来例に
おいては、次のような欠点がある。 a.aの場合、アレイであることのメリットを送信にの
み活用しているために、きずのサイジング等では従来の
超音波探傷法と同様に、受信エコーの感度を主に用いて
いる。しかし、その感度の閾値に対する理論的な説明は
あまりされておらず、経験的に決められている側面があ
り、信頼性が低い。
However, the above conventional example has the following disadvantages. a. In the case of a, since the advantage of being an array is utilized only for transmission, the sensitivity of the reception echo is mainly used in flaw sizing and the like as in the conventional ultrasonic flaw detection method. However, there is not much theoretical explanation for the threshold value of the sensitivity, and there are aspects that are empirically determined, and the reliability is low.

【0006】b.bの場合、受信にもアレイであること
のメリットを用いているが、きず寸法と素子寸法やA/
Dコンバータの性能等の影響により精度向上範囲に限界
がある。
B. In the case of b, the merit of being an array is used for reception as well, but the flaw size and element size and A /
The accuracy improvement range is limited due to the performance of the D converter.

【0007】c.cの場合、2種類の方法とも比較的正
しい値を示すことは知られてはいるが、理論的な根拠に
は欠ける。
C. In the case of c, it is known that the two methods show relatively correct values, but the theoretical basis is not sufficient.

【0008】[0008]

【課題を解決するための手段】本発明は、アレイ探触子
を用いて行う探傷法において、正確に反射体の寸法(素
子配列方向長さ)を求めることができる方法とその装置
を得るのが目的であって、その構成は次のとおりであ
る。
The present invention provides a method and apparatus for accurately determining the size of a reflector (length in the element array direction) in a flaw detection method using an array probe. The purpose is to have the following structure.

【0009】1.アレイ探触子を素子の配列方向に走査
することにより素子間の受信感度分布とこの分布のピー
クを検出し、前記ピークが送信素子群の中心から一定の
距離に収まる最大走査量を求めてこの値から反射体の寸
法を評価するアレイ超音波探傷法。
1. By scanning the array probe in the array direction of the elements, the receiving sensitivity distribution between the elements and the peak of this distribution are detected, and the maximum scanning amount at which the peak is within a certain distance from the center of the transmitting element group is obtained. Array ultrasonic testing method to evaluate the size of the reflector from the value.

【0010】2.アレイ探触子を駆動すると共に、駆動
する素子群の組み合せを変更することでアレイ探触子を
素子の配列方向に電子的に走査させるアレイコントロー
ラと、前記アレイコントローラがアレイ探触子を走査さ
せた距離を求める走査量計算器と、前記アレイ探触子で
受信された超音波の受信感度分布をチャンネルごとに求
める受信感度分布計算器と、前記受信感度分布計算器で
計算された受信感度分布のピークを求めるピーク検出器
と、前記走査量計算器で求めた走査量及びピーク検出器
で求めた受信感度分布のピークが送信素子群の中心から
一定の距離に収まる最大走査量を求め、この値から反射
体の寸法を求めるきず長さ計算器と、から成るアレイ超
音波探傷装置。
[0010] 2. An array controller that electronically scans the array probe in the array direction of the elements by changing the combination of the driven element groups while driving the array probe, and the array controller that scans the array probe A scanning amount calculator for obtaining the distance, a reception sensitivity distribution calculator for obtaining the reception sensitivity distribution of the ultrasonic waves received by the array probe for each channel, and a reception sensitivity distribution calculated by the reception sensitivity distribution calculator Of the peak detector for obtaining the peak of, the scanning amount obtained by the scanning amount calculator and the peak of the reception sensitivity distribution obtained by the peak detector are obtained at the maximum scanning amount within a fixed distance from the center of the transmitting element group, An array ultrasonic flaw detector comprising a flaw length calculator for obtaining the size of a reflector from a value.

【0011】3.アレイ探触子を駆動するアレイコント
ローラと、前記アレイ探触子を素子の配列方向に機械的
に走査させる走査装置と、前記走査装置がアレイ探触子
を走査させた距離を求める走査量計算器と、前記アレイ
探触子で受信された超音波の受信感度分布をチャンネル
ごとに求める受信感度分布計算器と、前記受信感度分布
計算器で計算された受信感度分布のピークを求めるピー
ク検出器と、前記走査量計算器で求めた走査量及びピー
ク検出器で求めた受信感度分布のピークが送信素子群の
中心から一定の距離に収まる最大走査量を求め、この値
から反射体の寸法を求めるきず長さ計算器と、から成る
アレイ超音波探傷装置。
3. An array controller that drives the array probe, a scanning device that mechanically scans the array probe in an element array direction, and a scanning amount calculator that determines a distance over which the scanning device scans the array probe. A reception sensitivity distribution calculator that obtains the reception sensitivity distribution of the ultrasonic waves received by the array probe for each channel, and a peak detector that obtains the peak of the reception sensitivity distribution calculated by the reception sensitivity distribution calculator , The maximum scanning amount in which the scanning amount obtained by the scanning amount calculator and the peak of the receiving sensitivity distribution obtained by the peak detector are within a certain distance from the center of the transmitting element group, and the dimension of the reflector is obtained from this value. An array ultrasonic flaw detector consisting of a flaw length calculator.

【0012】4.アレイ探触子を駆動すると共に、駆動
する素子群の組み合せを変更することでアレイ探触子を
素子の配列方向に電子的に走査させるアレイコントロー
ラと、前記アレイ探触子を素子の配列方向に機械的に走
査させる走査装置と、前記アレイコントローラ及び走査
装置がアレイ探触子を走査させた距離を求める走査量計
算器と、前記アレイ探触子で受信された超音波の受信感
度分布をチャンネルごとに求める受信感度分布計算器
と、前記受信感度分布計算器で計算された受信感度分布
のピークを求めるピーク検出器と、前記走査量計算器で
求めた走査量及びピーク検出器で求めた受信感度分布の
ピークが送信素子群の中心から一定の距離に収まる最大
走査量を求め、この値から反射体の寸法を求めるきず長
さ計算器と、から成るアレイ超音波探傷装置。
4. An array controller that electronically scans the array probe in the element array direction by changing the combination of the driven element groups while driving the array probe, and the array probe in the element array direction. A scanning device that mechanically scans, a scanning amount calculator that obtains the array controller and the scanning distance of the array probe by the scanning device, and a channel for receiving the sensitivity distribution of the ultrasonic waves received by the array probe. Reception sensitivity distribution calculator to be obtained for each, a peak detector to obtain the peak of the reception sensitivity distribution calculated by the reception sensitivity distribution calculator, the scanning amount obtained by the scanning amount calculator and the reception obtained by the peak detector An array ultrasonic probe that consists of a flaw length calculator that finds the maximum scanning amount at which the peak of the sensitivity distribution falls within a certain distance from the center of the transmitting element group and finds the size of the reflector from this value. Apparatus.

【0013】[0013]

【作用】探傷を行う場合、探傷箇所にアレイ探触子をセ
ットし、アレイコントローラによりタイミングを制御し
ながら素子をその配列方向に電子的に駆動する。又は、
アレイ探触子自体を走査装置により機械的に1mmずつ
移動させると共に、アレイコントローラにより素子を駆
動する。又は、素子の駆動タイミングを電子的に制御
し、同時にアレイ探触子を機械的に移動させる。このと
きの素子又は(及び)アレイ探触子の走査距離は走査量
計算器で求められる。素子から送信された超音波は、反
射体で反射し、この反射波は夫々の素子で受信される。
そして、受信された反射波は、受信感度分布計算器によ
り夫々の素子の受信感度とこの分布状態が計算される。
ピーク検出器は、前記分布状態のピークを求める。きず
長さ計算器は、走査量計算器及びピーク検出器で求めた
走査量とピークから、受信感度分布のピークが送信素子
群の中心から一定の距離に収まる最大の走査量を求め、
この値から反射体(きず)の長さを求める。
When performing flaw detection, the array probe is set at the flaw detection position, and the elements are electronically driven in the array direction while controlling the timing by the array controller. Or
The array probe itself is mechanically moved by 1 mm by the scanning device, and the elements are driven by the array controller. Alternatively, the drive timing of the element is electronically controlled, and at the same time, the array probe is mechanically moved. The scanning distance of the element or (and) array probe at this time is calculated by the scanning amount calculator. The ultrasonic waves transmitted from the elements are reflected by the reflector, and the reflected waves are received by the respective elements.
Then, the reception sensitivity distribution calculator calculates the reception sensitivities of the respective elements and the distribution state of the received reflected waves.
The peak detector finds the peak of the distribution state. The flaw length calculator, from the scanning amount and peak obtained by the scanning amount calculator and the peak detector, obtains the maximum scanning amount at which the peak of the receiving sensitivity distribution is within a certain distance from the center of the transmitting element group,
The length of the reflector (scratch) is obtained from this value.

【0014】[0014]

【発明の実施の形態】本発明において使用されるアレイ
探触子の構成を図1(a)(b)及び図2(a)(b)
に示す。図1において、1は素子2…を横方向に配列し
たアレイ探触子、図2において、1は素子2…を縦方向
に配列したアレイ探触子であって、図1及び図2の各
(a)において、矢印は超音波の送信方向である。この
図1及び図2に示したアレイ探触子1は、素子2…の配
列方向に向かって素子2…を電子的又は機械的に駆動し
て走査、又はアレイ探触子1自体の走査(移動)が可能
である。
BEST MODE FOR CARRYING OUT THE INVENTION The structure of an array probe used in the present invention is shown in FIGS. 1 (a) (b) and 2 (a) (b).
Shown in 1 is an array probe in which elements 2 are arranged in a horizontal direction, and in FIG. 2, 1 is an array probe in which elements 2 are arranged in a vertical direction. In (a), the arrow indicates the ultrasonic wave transmission direction. The array probe 1 shown in FIGS. 1 and 2 scans by electrically or mechanically driving the elements 2 ... In the array direction of the elements 2 ,. It is possible to move).

【0015】[実施例1]図3は電子走査方式のアレイ
超音波探傷装置であって、請求項1及び2の発明の実施
例を示し、符号の1はアレイ探触子、3はアレイコント
ローラであって、前記アレイ探触子1、素子2…を同時
に又は群ごとに又は時間差をおいて電子的に駆動する。
[Embodiment 1] FIG. 3 is an electronic scanning type array ultrasonic flaw detector, showing an embodiment of the invention of claims 1 and 2, wherein reference numeral 1 is an array probe and 3 is an array controller. The array probe 1, the elements 2, ... Are electronically driven at the same time or for each group or with a time lag.

【0016】4は走査量計算器であって、アレイ探触子
1(素子2)が走査した距離を計算する。5は受信感度
分布計算器であって、アレイ探触子1内の素子2…を同
時に駆動したときの各素子2…の受信感度の分布を計算
する。6はピーク検出器であって、前記受信感度分布計
算器5で計算された受信感度分布のピークを検出する。
Reference numeral 4 denotes a scanning amount calculator, which calculates the distance scanned by the array probe 1 (element 2). A receiver sensitivity distribution calculator 5 calculates the receiver sensitivity distribution of each element 2 ... When the elements 2 ... In the array probe 1 are simultaneously driven. A peak detector 6 detects a peak of the reception sensitivity distribution calculated by the reception sensitivity distribution calculator 5.

【0017】7はきず長さ計算器であって、走査量計算
器4で計算された走査量及びピーク検出器6で検出され
たピークから、送信素子群の中心から一定の距離に収ま
る最大の走査量を求める。この値からきずの長さを求め
る。
Reference numeral 7 denotes a flaw length calculator, which has a maximum distance within a certain distance from the center of the transmitting element group from the scanning amount calculated by the scanning amount calculator 4 and the peak detected by the peak detector 6. Find the scanning amount. Find the length of the flaw from this value.

【0018】[実施例2]図4は機械走査方式のアレイ
超音波探傷装置であって、請求項1及び3の発明の実施
例を示し、走査装置8は、機械的にアレイ探触子1を走
査し、この走査装置8で走査した量を走査量計算器4に
より計算する。きずの長さの計算は実施例1と同様にし
て行う。
[Embodiment 2] FIG. 4 shows a mechanical scanning type array ultrasonic flaw detector, which is an embodiment of the invention of claims 1 and 3, wherein the scanning device 8 mechanically operates the array probe 1. Is scanned, and the amount scanned by the scanning device 8 is calculated by the scanning amount calculator 4. The flaw length is calculated in the same manner as in the first embodiment.

【0019】[実施例3]図5は電子走査方式(実施例
1)と機械走査方式(実施例2)とを併用して行うアレ
イ超音波探傷装置であって、アレイ探触子1内の素子2
…の駆動をアレイコントローラ3で電子的に行い、同時
に走査装置8でアレイ探触子1を移動させ、この双方の
走査量を走査量計算器4で計算する。きずの長さの計算
は実施例1と同様にして行う。
[Embodiment 3] FIG. 5 shows an array ultrasonic flaw detector using both the electronic scanning method (Embodiment 1) and the mechanical scanning method (Embodiment 2). Element 2
.. are electronically driven by the array controller 3, and at the same time the array probe 1 is moved by the scanning device 8, and the scanning amounts of both of them are calculated by the scanning amount calculator 4. The flaw length is calculated in the same manner as in the first embodiment.

【0020】図6(a)(b)は、アレイ探触子1を反
射体xに沿って走査させたときの送信音場の変化を示す
説明図である。この図から素子2…の中心から音場が徐
々に移動していることが判る。
FIGS. 6A and 6B are explanatory views showing changes in the transmitted sound field when the array probe 1 is scanned along the reflector x. From this figure, it can be seen that the sound field gradually moves from the center of the elements 2.

【0021】図7(a)(b)は図1に示したアレイ探
触子(以下「Aタイプ」と称す)と図2に示したアレイ
探触子(以下「Bタイプ」と称す)による受信感度分布
の変化を調べた際のデータである。このように、アレイ
探触子1を走査させながらデータをとり、このデータか
らきずの長さを求める。例えば、Aタイプのアレイ探触
子1による貫通縦スリットの探傷では、6mmのスリッ
トの中心とアレイ探触子1の中心とを合わせ、そこから
アレイ探触子1を横方向に1mmずつ移動させ(a)、
Bタイプのアレイ探触子1によるスリットの探傷では、
2mmのスリットによるエコーが、5番目の素子で最大
になる位置にアレイ探触子1を配置し、前後に1mmづ
つ移動させた(b)。Aタイプの場合には、感度分布が
ほぼ一定の値を示す範囲位置が徐々に移動しているのが
わかる。移動量が4mmになるとこの範囲が中心に該当
する素子(5番又は6番)から外れる。これにより、ス
リット幅が6mmであることがわかる。またBタイプの
場合は移動量が3mmになると感度分布の極大が中心に
該当する素子5番又は6番から外れる。これを数1によ
りスリットに換算すると、高さが1.7mmとなる。
7A and 7B show the array probe shown in FIG. 1 (hereinafter referred to as "A type") and the array probe shown in FIG. 2 (hereinafter referred to as "B type"). This is the data when the change in the reception sensitivity distribution is investigated. In this way, data is taken while scanning the array probe 1, and the length of the flaw is obtained from this data. For example, in flaw detection of a through vertical slit by the A type array probe 1, the center of the 6 mm slit is aligned with the center of the array probe 1, and the array probe 1 is moved laterally by 1 mm from there. (A),
In the flaw detection of the slit by the B type array probe 1,
The array probe 1 was arranged at a position where the echo by the slit of 2 mm was maximized at the fifth element, and the array probe 1 was moved back and forth by 1 mm (b). In the case of the A type, it can be seen that the range position where the sensitivity distribution shows a substantially constant value is gradually moving. When the amount of movement is 4 mm, this range deviates from the corresponding element (No. 5 or No. 6). This shows that the slit width is 6 mm. Further, in the case of the B type, when the movement amount becomes 3 mm, the maximum of the sensitivity distribution deviates from the element No. 5 or 6 corresponding to the center. When this is converted into a slit by the formula 1, the height becomes 1.7 mm.

【0022】[0022]

【式1】 ただしh:スリット高さ(mm)、d:探触子移動量
(mm)、θ1 鋼中屈折角、θ2 :アクリル中屈折角。
(Equation 1) However, h: slit height (mm), d: probe movement amount (mm), θ 1 steel refraction angle, θ 2 : acrylic refraction angle.

【0023】[0023]

【発明の効果】本発明は以上のように、アレイ探触子を
走査させ、この走査量と受信感度分布のピークが送信素
子群の中心から一定の距離に収まる量を反射体(きず)
の寸法(長さ)として評価するようにした。この結果、
分布形状は送信音場と反射体との相対的関係により決ま
るために、その変化の理論的説明も可能であり、従来技
術で述べたcの反射体の長さの測定方法に対して信頼性
の向上が可能である。また、従来技術で述べたbの反射
体の形状の推定の方法に対しても機械的走査や電子走査
により、分解能やサイジングに対して素子寸法などの機
器の能力の限界の影響を少なくすることが可能である。
As described above, according to the present invention, the array probe is scanned, and the amount of this scanning amount and the peak of the receiving sensitivity distribution are within a certain distance from the center of the transmitting element group.
Was evaluated as the dimension (length). As a result,
Since the distribution shape is determined by the relative relationship between the transmitted sound field and the reflector, it is possible to theoretically explain the change, and it is reliable with respect to the method of measuring the reflector length of c described in the prior art. Can be improved. In addition, in the method of estimating the shape of the reflector described in b) in the prior art, mechanical scanning or electronic scanning should be used to reduce the influence of the limit of the device capability such as the element size on the resolution and sizing. Is possible.

【図面の簡単な説明】[Brief description of drawings]

【図1】横方向に素子を配列したアレイ探触子の説明
図。
FIG. 1 is an explanatory diagram of an array probe in which elements are arranged in a lateral direction.

【図2】縦方向に素子を配列したアレイ探触子の説明
図。
FIG. 2 is an explanatory diagram of an array probe in which elements are arranged in a vertical direction.

【図3】電子走査方式の探傷装置の説明図。FIG. 3 is an explanatory diagram of an electronic scanning flaw detector.

【図4】機械走査方式の探傷装置の説明図。FIG. 4 is an explanatory view of a mechanical scanning type flaw detection device.

【図5】電子走査方式と機械走査方式を組み合わせた探
傷装置の説明図。
FIG. 5 is an explanatory diagram of a flaw detection device that combines an electronic scanning method and a mechanical scanning method.

【図6】送信音場の移動の説明図。FIG. 6 is an explanatory diagram of movement of a transmission sound field.

【図7】探傷試験において、探傷スリット幅と受信感度
分布の関係の説明図。
FIG. 7 is an explanatory diagram of a relationship between a flaw detection slit width and a reception sensitivity distribution in a flaw detection test.

【図8】従来技術において、駆動タイミング或いはセッ
トを変えて行う従来の探傷方法の説明図。
FIG. 8 is an explanatory diagram of a conventional flaw detection method performed by changing a drive timing or a set in a conventional technique.

【図9】従来技術において、オシロスコープに表示され
た反射波のピークの説明と、きずの長さ及びアレイ探触
子を走査させたときの反射波のピークの変化、及びこの
変化分布からきずの長さを求める方法の説明図。
FIG. 9 is a view for explaining a peak of a reflected wave displayed on an oscilloscope in the related art, a change in the peak of the reflected wave when a flaw length and an array probe are scanned, and a change distribution of this flaw. Explanatory drawing of the method of calculating | requiring length.

【符号の説明】[Explanation of symbols]

1 アレイ探触子 2… 素子 3 アレイコントローラ 4 走査量計算器 5 受信感度分布計算器 6 ピーク検出器 7 きず長さ計算器 8 走査装置 1 array probe 2 ... element 3 array controller 4 scanning amount calculator 5 reception sensitivity distribution calculator 6 peak detector 7 flaw length calculator 8 scanning device

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 アレイ探触子を素子の配列方向に走査す
ることにより素子間の受信感度分布とこの分布のピーク
を検出し、前記ピークが送信素子群の中心から一定の距
離に収まる最大走査量を求めてこの値から反射体の寸法
を評価するアレイ超音波探傷法。
1. A maximum scanning in which a receiving sensitivity distribution between elements and a peak of this distribution are detected by scanning an array probe in an element array direction, and the peak is within a certain distance from the center of a transmitting element group. An array ultrasonic flaw detection method that obtains the quantity and evaluates the dimensions of the reflector from this value.
【請求項2】 アレイ探触子を駆動すると共に、駆動す
る素子群の組み合せを変更することでアレイ探触子を素
子の配列方向に電子的に走査させるコントローラと、 前記アレイコントローラがアレイ探触子を走査させた距
離を求める走査量計算器と、 前記アレイ探触子で受信された超音波の受信感度分布を
チャンネルごとに求める受信感度分布計算器と、 前記受信感度分布計算器で計算された受信感度分布のピ
ークを求めるピーク検出器と、 前記走査量計算器で求めた走査量及びピーク検出器で求
めた受信感度分布のピークが送信素子群の中心から一定
の距離に収まる最大走査量を求め、この値から反射体の
寸法を求めるきず長さ計算器と、 から成るアレイ超音波探傷装置。
2. A controller for driving the array probe and electronically scanning the array probe in the element arrangement direction by changing the combination of driven element groups, and the array controller A scanning amount calculator for obtaining the distance at which the probe is scanned, a reception sensitivity distribution calculator for obtaining the reception sensitivity distribution of the ultrasonic waves received by the array probe for each channel, and the reception sensitivity distribution calculator for calculating And a peak detector for obtaining the peak of the receiving sensitivity distribution, and the maximum scanning amount for which the scanning amount obtained by the scanning amount calculator and the peak of the receiving sensitivity distribution obtained by the peak detector are within a certain distance from the center of the transmitting element group. An array ultrasonic flaw detector consisting of a flaw length calculator and a reflector length calculator.
【請求項3】 アレイ探触子を駆動するアレイコントロ
ーラと、 前記アレイ探触子を素子の配列方向に機械的に走査させ
る走査装置と、 前記走査装置がアレイ探触子を走査させた距離を求める
走査量計算器と、 前記アレイ探触子で受信された超音波の受信感度分布を
チャンネルごとに求める受信感度分布計算器と、 前記受信感度分布計算器で計算された受信感度分布のピ
ークを求めるピーク検出器と、 前記走査量計算器で求めた走査量及びピーク検出器で求
めた受信感度分布のピークが送信素子群の中心から一定
の距離に収まる最大走査量を求め、この値から反射体の
寸法を求めるきず長さ計算器と、 から成るアレイ超音波探傷装置。
3. An array controller that drives the array probe, a scanning device that mechanically scans the array probe in the direction in which the elements are arranged, and a distance that the scanning device scans the array probe. A scanning amount calculator to be obtained, a reception sensitivity distribution calculator for obtaining the reception sensitivity distribution of the ultrasonic waves received by the array probe for each channel, and a peak of the reception sensitivity distribution calculated by the reception sensitivity distribution calculator The peak detector to be obtained and the scanning amount obtained by the scanning amount calculator and the maximum scanning amount at which the peak of the reception sensitivity distribution obtained by the peak detector falls within a certain distance from the center of the transmitting element group, are reflected from this value. An array ultrasonic flaw detector consisting of a flaw length calculator that determines the body size.
【請求項4】 アレイ探触子を駆動すると共に、駆動す
る素子群の組み合せを変更することでアレイ探触子を素
子の配列方向に電子的に走査させるアレイコントローラ
と、 前記アレイ探触子を素子の配列方向に機械的に走査させ
る走査装置と、 前記アレイコントローラ及び走査装置がアレイ探触子を
走査させた距離を求める走査量計算器と、 前記アレイ探触子で受信された超音波の受信感度分布を
チャンネルごとに求める受信感度分布計算器と、 前記受信感度分布計算器で計算された受信感度分布のピ
ークを求めるピーク検出器と、 前記走査量計算器で求めた走査量及びピーク検出器で求
めた受信感度分布のピークが送信素子群の中心から一定
の距離に収まる最大走査量を求め、この値から反射体の
寸法を求めるきず長さ計算器と、 から成るアレイ超音波探傷装置。
4. An array controller for driving an array probe and electronically scanning the array probe in an element array direction by changing a combination of driven element groups, and the array probe. A scanning device that mechanically scans in the array direction of the elements, a scanning amount calculator that obtains a distance over which the array controller and the scanning device scan the array probe, and an ultrasonic wave received by the array probe. A receiving sensitivity distribution calculator that obtains a receiving sensitivity distribution for each channel, a peak detector that obtains a peak of the receiving sensitivity distribution calculated by the receiving sensitivity distribution calculator, and a scanning amount and peak detection that are obtained by the scanning amount calculator The peak length of the receiver sensitivity distribution obtained by the detector is found at the maximum scanning distance within a certain distance from the center of the transmitter element group, and the size of the reflector is obtained from this value. Array ultrasonic flaw detector.
JP8066151A 1996-03-22 1996-03-22 Array ultrasonic flaw detection method and apparatus therefor Pending JPH09257763A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8066151A JPH09257763A (en) 1996-03-22 1996-03-22 Array ultrasonic flaw detection method and apparatus therefor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8066151A JPH09257763A (en) 1996-03-22 1996-03-22 Array ultrasonic flaw detection method and apparatus therefor

Publications (1)

Publication Number Publication Date
JPH09257763A true JPH09257763A (en) 1997-10-03

Family

ID=13307588

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8066151A Pending JPH09257763A (en) 1996-03-22 1996-03-22 Array ultrasonic flaw detection method and apparatus therefor

Country Status (1)

Country Link
JP (1) JPH09257763A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005156305A (en) * 2003-11-25 2005-06-16 Daido Steel Co Ltd Evaluation method of internal defect

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005156305A (en) * 2003-11-25 2005-06-16 Daido Steel Co Ltd Evaluation method of internal defect

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