JPH0664027B2 - Angle beam inspection head for pipes and angle beam inspection device for pipes using the same - Google Patents

Angle beam inspection head for pipes and angle beam inspection device for pipes using the same

Info

Publication number
JPH0664027B2
JPH0664027B2 JP63209210A JP20921088A JPH0664027B2 JP H0664027 B2 JPH0664027 B2 JP H0664027B2 JP 63209210 A JP63209210 A JP 63209210A JP 20921088 A JP20921088 A JP 20921088A JP H0664027 B2 JPH0664027 B2 JP H0664027B2
Authority
JP
Japan
Prior art keywords
pipe
probe
bevel
angle
flaw detection
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 - Lifetime
Application number
JP63209210A
Other languages
Japanese (ja)
Other versions
JPH0257973A (en
Inventor
廣章 近藤
Original Assignee
川崎製鉄株式会社
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 川崎製鉄株式会社 filed Critical 川崎製鉄株式会社
Priority to JP63209210A priority Critical patent/JPH0664027B2/en
Publication of JPH0257973A publication Critical patent/JPH0257973A/en
Publication of JPH0664027B2 publication Critical patent/JPH0664027B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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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

Landscapes

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

Description

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

【産業上の利用分野】 本発明は、管用斜角探傷ヘツド及びそれを用いた管用斜
角探傷装置に係り、特に電縫鋼管の溶接部における管軸
方向の欠陥を検出する際に用いるのに好適な、溶接部追
従が不要で、管厚変更時の調整も不要な、管用斜角探傷
ヘツド及びそれを用いた管用斜角探傷装置に関するもの
である。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a bevel flaw detection head for pipes and a bevel flaw detection device for pipes using the same, and is particularly used for detecting defects in a welded portion of an electric resistance welded pipe in a pipe axial direction. The present invention relates to a preferable bevel angle flaw detection head for pipes and a bevel angle flaw detection device for pipes using the same, which does not need to follow the welded portion and need not be adjusted when changing the pipe thickness.

【従来の技術】[Prior art]

一般に、電縫鋼管の溶接部における管軸方向の欠陥を検
出するため、斜角探傷法が用いられている。この方法
は、被検査材(以下、「被検管」という)の検査面に対
し斜めに超音波を入射させ、被検管の欠陥で反射した反
射波から当該検管の内外表面欠陥及び内部欠陥を検出す
るものである。 又、上記電縫鋼管の溶接部全長にわたつて欠陥を検出す
るため、超音波探触子を電縫鋼管の溶接部に対し平行に
走査して、該溶接部に対して超音波ビームを直角に伝播
させる方法が用いられている。 しかるに、上記斜角探傷法においては、超音波ビームが
入射した点から欠陥部までの距離の変動、即ち探触子−
欠陥距離の変動に伴ない、欠陥からのエコー高さが、第
11図に示すように大きく変化することが知られている。
このことは、例えば特開昭55−140148号の第2図や特公
昭57−8420号の第1図に開示されている。 このため、基準エコー高さを定めるのが難しく、探触子
−欠陥距離が変動すると正確な探傷が困難になると言う
問題があり、この問題を緩和するため、次のような方法
が採用されていた。 即ち、第12図は従来例の構成説明図であり、第13図
(A)、(B)及び(C)はそれぞれ第12図のA−A′
断面図、B−B′断面図、及びC−C′断面図である
が、これらの図に示すように、電縫鋼管のような被検管
10の溶接部11の片側にそれぞれ例えば3個ずつの斜角探
触子18a〜18c、18d〜18fを配置し、これらの探触子から
被検管10に入射する超音波ビームが溶接部11の中心にお
いて外面(第13図(A)参照)、中央(第13図(B)参
照)、及び内面(第13図(C)参照)に伝播するように
していた。 更に、例えば特公昭57−8420号に開示されているよう
に、溶接部の捩れ量と被検管の長さを予めプリセツトし
ておき、その後現在位置の長さを逐次検出して、探触子
の溶接部からのずれ量を算出して溶接部の追従を行つた
り、又は、例えば特開昭59−43354号に開示されている
ように、探触子に被検管の周方向に沿つて複数個の送受
信コイルを取付け、これら送受信コイルの受診信号レベ
ルを順次時系列的に判断し、溶接部と探触子の相対位置
を一定の関係に保持して、溶接部の追従を行うようにし
ていた。 しかしながら、上記従来例においては、第1に、探触子
と欠陥の距離が変化すると上述の如くエコー高さが大き
く変化するため、溶接部の追従を行わなければならない
という問題があつた。 又、第2に、被検管の外径や管厚によりピークエコーの
出現位置が異なるという問題があつた。即ち、ピークエ
コーの出現位置Lは、下式(1)のように表わされ、被
検管の外径Dや管厚tの値によつて変動する。このた
め、管厚tに応じて、探触子と溶接部の距離を調整しな
ければならなかつた。 L=N・K・t・tanθr ……(1) ここで、Nは、スキツプ数Sによる係数(N=S/0.
5)、Kは、屈折角θrとt/Dで決まる補正係数であ
る。 又、第3に、探傷装置本体の感度をピークエコーで設定
するために、感度調整作業を行わなければならないとい
う問題もあつた。
Generally, in order to detect defects in a welded portion of an electric resistance welded steel pipe in the pipe axis direction, a bevel flaw detection method is used. This method involves injecting ultrasonic waves obliquely to the inspection surface of the material to be inspected (hereinafter referred to as the "inspection tube"), and the internal and external surface defects of the inspection tube and the inside of the inspection tube are reflected from the reflected waves reflected by the defects of the inspection tube. The defect is detected. Further, in order to detect defects over the entire length of the welded portion of the electric resistance welded steel pipe, the ultrasonic probe is scanned parallel to the welded portion of the electric resistance welded steel pipe, and the ultrasonic beam is perpendicular to the welded portion. The method of propagating to is used. However, in the above-described oblique angle flaw detection method, variation in the distance from the point where the ultrasonic beam is incident to the defect portion, that is, the probe-
As the defect distance changes, the echo height from the defect becomes
It is known that there are large changes as shown in Fig. 11.
This is disclosed, for example, in FIG. 2 of JP-A-55-140148 and FIG. 1 of JP-B-57-8420. For this reason, it is difficult to determine the reference echo height, and there is a problem that accurate flaw detection becomes difficult when the probe-defect distance changes, and in order to mitigate this problem, the following method is adopted. It was That is, FIG. 12 is a structural explanatory view of a conventional example, and FIGS. 13 (A), (B) and (C) are respectively AA ′ of FIG.
It is a sectional view, a BB 'sectional view, and a CC' sectional view, but as shown in these drawings, a test tube such as an electric resistance welded steel tube
For example, three oblique angle probes 18a to 18c and 18d to 18f are arranged on one side of the welded portion 11 of 10 respectively, and an ultrasonic beam incident on the tube 10 to be inspected from these probes is welded to the welded portion 11. At the center of the, the light propagates to the outer surface (see FIG. 13 (A)), the center (see FIG. 13 (B)), and the inner surface (see FIG. 13 (C)). Further, as disclosed in, for example, Japanese Examined Patent Publication No. 57-8420, the twist amount of the weld and the length of the pipe to be inspected are preset, and then the length of the current position is sequentially detected to detect the probe. The displacement of the child from the welded portion is calculated to follow the welded portion, or, for example, as disclosed in JP-A-59-43354, the probe is arranged in the circumferential direction of the tube to be inspected. A plurality of transmission / reception coils are installed along the line, the signal levels of the reception / transmission coils are sequentially determined in time series, and the relative positions of the weld and the probe are held in a fixed relationship to follow the weld. Was doing. However, in the above-mentioned conventional example, firstly, there is a problem that the welding portion must be followed because the echo height greatly changes as described above when the distance between the probe and the defect changes. Secondly, there is a problem that the peak echo appearance position differs depending on the outer diameter and the tube thickness of the test tube. That is, the appearance position L of the peak echo is expressed by the following equation (1) and varies depending on the values of the outer diameter D and the tube thickness t of the test tube. Therefore, the distance between the probe and the welded portion has to be adjusted according to the tube thickness t. L = N · K · t · tan θr (1) Here, N is a coefficient by the skip number S (N = S / 0.
5) and K are correction coefficients determined by the refraction angle θr and t / D. Thirdly, there is also a problem that sensitivity adjustment work must be performed in order to set the sensitivity of the flaw detection apparatus main body by the peak echo.

【発明が達成しようとする課題】[Problems to be achieved by the invention]

本発明は、上述のような問題に鑑みてなされたものであ
り、上記第1乃至第3の問題点が全て解消され、特に電
縫鋼管のような被検管の溶接部における管軸方向の欠陥
を検出するのに好適な管用斜角探傷ヘツド及びそれを用
いた管用斜角探傷装置を提供することを課題とする。
The present invention has been made in view of the above-mentioned problems, and all of the above-described first to third problems are solved, and particularly in the pipe axis direction in the welded portion of the pipe to be inspected such as the electric resistance welded steel pipe. It is an object of the present invention to provide a pipe bevel flaw detection head suitable for detecting a defect and a pipe bevel flaw detection device using the same.

【課題を達成するための手段】[Means for achieving the object]

本発明は、超音波斜角探傷法により、被検管の管軸方向
の欠陥を検査するために用いられる管用斜角探傷ヘツド
において、複数個の斜角探触子を、前記被検管の管周方
向に隙間なく効率的に配置するために、それぞれの該斜
角探触子が垂直探触子と音響くさびとにて構成され、前
記被検管の管周方向における前記音響くさびの断面形状
が、前記被検管側より前記垂直探触子側の幅広の、前記
被検管の外径と前記垂直探触子の幅とによつて決定され
る放射角βの放射角状の形状であつて、更に、前記音響
くさびの断面形状が、前記被検管の管周方向に斜めに超
音波を励振又は受信すべく、管周方向で入射角θiとな
るように傾斜配置される形状であり、前記入射角θiと
直交する前記音響くさびの取り付け面に対して、垂直方
向に超音波を励振又は受信する前記垂直探触子を取り付
けると共に、複数の前記斜角探触子を、前記管周方向に
アレイ状に隙間なく且つ傾斜配置状態で装着する、前記
被検管と同芯円の円弧形状の側板を有し、又、アレイ状
の複数の前記斜角探触子の前後に設けられた、前記被検
管の表面と前記音響くさびとの間のギヤツプを保持し、
該音響くさびの摩耗を防ぐ、耐摩耗性の1対のシユーを
設けることにより、前記課題を解決したものである。 又、本発明は、管用斜角探傷装置において、上記管用斜
角探傷ヘツドを具備して、被検管を探傷することによ
り、前記課題を解決したものである。
The present invention provides a plurality of bevel probes for a pipe bevel flaw detection head for a pipe used for inspecting defects in the pipe axis direction of a subject pipe by an ultrasonic bevel flaw detection method. In order to arrange the angle probes in a circumferential direction of the pipe efficiently without gaps, each of the bevel probes is composed of a vertical probe and an acoustic wedge, and a cross section of the acoustic wedge in the pipe circumferential direction of the test tube. The shape is wider than the test tube side on the vertical probe side, and has a radiation angle shape of a radiation angle β determined by the outer diameter of the test tube and the width of the vertical probe. Further, the acoustic wedge has a cross-sectional shape inclined so as to have an incident angle θi in the tube circumferential direction so as to excite or receive ultrasonic waves obliquely in the tube circumferential direction of the test tube. And excites ultrasonic waves in a direction perpendicular to the mounting surface of the acoustic wedge that is orthogonal to the incident angle θi. An arc shape of a concentric circle with the tube to be inspected, in which the vertical probe for receiving is attached and a plurality of the oblique probes are mounted in an array form in the circumferential direction of the tube without a gap and in an inclined arrangement. A side plate, and is provided in front of and behind the plurality of beveled probes in an array, holding a gear gap between the surface of the tube to be tested and the acoustic wedge,
The above problem is solved by providing a pair of wear-resistant shoes that prevent wear of the acoustic wedge. Further, the present invention solves the above-described problems in a bevel angle flaw detection device for a pipe, which is equipped with the above-mentioned bevel angle flaw detection head for a pipe to detect a test tube.

【作用】[Action]

本発明の管用斜角探傷ヘツドにおいては、第1図及び第
2図、又第3図(A)又は(B)に示す如く、矩形状の
接触面を持つ垂直探触子14と、放射角状の幅を持つ音響
くさび15とからなる、管周方向の幅が例えば数mm以下の
斜角探触子12が、管周状に複数個アレイ状に配置されて
いる。ここで斜角探触子12の数n(図ではn=6)は、
被検管10における最大の1スキツプ距離S以上をカバー
できるように決定することができる。 前記探触子を管周に沿つてアレイ状に配置するため、音
響くさび15の管周方向幅は、例えばβ゜の放射角状に加
工されると共に、探触子が被検管10と同芯円の円弧形状
の側板16a、16bに取り付けられている。 更に、音響くさび15と被検管10の表面とのギヤツプ保持
及び音響くさび15の摩耗防止のために、探触子群の前後
に耐摩耗性のシユー17a、17bが取り付けられている。 従つて、管状材に対する探傷を容易に行うことができ、
後述するように、溶接部追従が不要となり、管厚変更時
の調整も不要となる。
As shown in FIGS. 1 and 2 and FIG. 3A or FIG. 3B, the oblique angle flaw detection head for a pipe according to the present invention has a vertical probe 14 having a rectangular contact surface and a radiation angle. A plurality of beveled probes 12 each having a width in the tube circumferential direction of, for example, several mm or less, which are composed of an acoustic wedge 15 having a circular width, are arranged in an array in the tube circumferential shape. Here, the number n of the bevel probe 12 (n = 6 in the figure) is
It can be determined so that the maximum one skip distance S or more in the test tube 10 can be covered. Since the probes are arranged in an array along the pipe circumference, the width of the acoustic wedge 15 in the pipe circumferential direction is processed into a radial angle of, for example, β °, and the probe is the same as the test pipe 10. It is attached to side plates 16a and 16b having an arc shape of a center circle. Further, wear-resistant shoes 17a and 17b are attached to the front and rear of the probe group in order to hold the gear between the acoustic wedge 15 and the surface of the tube 10 to be tested and prevent the acoustic wedge 15 from being worn. Therefore, it is possible to easily perform flaw detection on the tubular material,
As will be described later, it is not necessary to follow the welded portion, and no adjustment is required when changing the pipe thickness.

【実施例】【Example】

以下、図面を参照して、本発明の実施例を詳細に説明す
る。 本発明に係る鋼管用斜角探傷ヘツドの実施例は、第1図
及び第2図、又第3図(A)、(B)に示すような構成
になつている。 即ち、矩形状の接触面をもつ垂直探触子14と放射角状の
幅(例えば数mm以下)を有する音響くさび15で斜角探触
子12が構成され、該垂直探触子14は音響くさび15に小ね
じ等(図示せず)によつて取付けられている。 一般に、音響くさびに直接振動子を接着させることによ
り、斜角探触子となるが、本実施例における音響くさび
が、後述するように被検管の外径により異なつた放射角
状の断面形状を有する必要がある。このため、本実施例
においては、垂直探触子14に音響くさび15を装着するこ
とにより斜角探触子12としている。 なお、前記垂直探触子14は、ごく一般に用いられている
ものである。例えば、『非破壊試験概論』(社団法人
日本非破壊検査協会 1992)の第39頁に、斜角探触子と
併せて図等を用いて詳しく言及されている、ごく一般的
な垂直探触子を用いることができる。この垂直探触子
は、これに接する試験体表面に対して垂直に、発生され
た超音波を伝搬させる。 前述の『非破壊試験概論』では、前記垂直探触子につい
て、例えば、用いる振動子やダンパ(保持体)について
解説されている。前記垂直探触子には、直流のパルス電
圧を加えて超音波を発生させる振動子が組込まれてい
る。振動子材料には圧電材料が用いられている。その代
表的なものは、水晶とジルコン・チタン酸鉛系磁器(略
称:ジルナマ)とされている。又、例えば、振動子は、
その表面に銀メッキによつて電極を付けられたものであ
り、直流パルス電圧を加えると、振動子は、その厚さで
決まる共振周波数で厚さ方向に伸縮するものである。
又、前記垂直探触子では、振動を早く止めるためのダン
パの役割をする保持体を振動子に貼り付けて、ケースに
納められている。一般に、一つの探触子で送信と受信を
併せて行うことができる。 又、垂直探触子14の接触面と音響くさび15の取り付け面
との間には油等による薄膜(図示せず)が存在し、垂直
探触子14と音響くさび15を音響的に結合させている。一
方、各斜角探触子12の間は、それぞれ音響分割板(図示
せず)で区画されている。 前記音響くさび15は、上述の如く放射角状の幅を有し、
具体的には、被検管(電縫鋼管)10の管周方向の幅がβ
゜の放射角状となつている。 又、音響くさび15へ入射する入射波の音速と被検管10で
屈折する屈折波の音速をそれぞれCi、Crとするとき、該
入射波の入社角θiと屈折波の屈折角θrとの関係は所
謂スネルの法則に従い、下式(2)が成立する。 Cr/sinθr=Ci/sinθi …(2) 従つて、所望の上記屈折角θrを得るため、入射角が上
記入射角θとなるように音響くさび15の形状が形成され
ている。 ところで、音響くさび15は上述の如く放射状の幅を有し
ているが、該幅の放射角β゜は被検管10の外径と垂直探
触子14の幅によつて決定される。音響くさび15の管周方
向の幅を上述の如く放射角β゜に加工することにより、
該音響くさび15を被検管10の管周上に第1図の如くアレ
イ状に配置することが容易になつている。 管周方向に超音波を送受信するための斜角探触子を管周
方向に最も狭間隔で配置するために、斜角探触子におけ
る重要な構成要素である音響くさび15を第1図に示すよ
うな放射角状の幅を持つ形状とする。即ち、以下、主と
して第2図を用いて説明するような、前記被検管10の管
周方向における、前記音響くさび15の断面形状である。 まず、所望のくさび中心長さをlmm及びくさび上面の幅
をωmmとする。又、前記被検管10の外周である円A(半
径=r)のP点に対し、入射角θiにて超音波を入射
させるものとする。このとき、前記第2図の線分Q
′、線分P′P′、線分P′Q、線分Q
で示される前記音響くさび15は、以下のようになる。 音響くさび15の上面のQより±ω/2の点を、それぞ
れ、点Q、点Qとする。Qにより被検管10の外周
である前記円A(半径=r)の点Pへ、入射角Qiで超
音波を入射させるためには、音響くさび15の上面は、線
分Pと直交する線分Qとなる。又、線分P
は、半径r′(=r・sinθi)の仮想上の円B
への接線の延長線上に位置する。又、点Q及び点Q
を各々通る円Bへの接線を引き、それぞれ、線分R
及び線分Rとする。これらの線分R及び
線分Rそれぞれと、円Aとの交点を、それぞれ点
及び点Pとすると、音響くさび15の上面の点Q
から円Aの点Pへの入射角はθiとなる。同様に、音
響くさび15の上面QからQAの点Pへの入射角もθi
となる。 なお、音響くさび15の下面は、線分OPと直交する線分
′P′とし、音響くさび15の被検管10の円周方向
の断面形状を、四角形Q′P′とする。こ
のとき、線分Q′と線分Q′とは、βの角
度を有することになる。又、このβは、近似的に下式で
求めた値となる。即ち、少なくとも前記被検管10の外径
rと前記音響くさび15の幅ω(即ち、前記垂直探触子の
幅)に従って、次式のとおり、このβは求められる。 β≒sin [ω/(r・cosθi+l)] …(3) 更に、第3図(A)、(B)により良く示されているよ
うに、垂直探触子14と音響くさび15からなる上記斜角探
触子12は、被検管10と同芯円の円弧形状を有する側板16
a、16bによつて小ねじ等(図示せず)を介して保持され
ている。この側板16a、16bは、上記斜角探触子12を被検
管10の管周上で容易にアレイ状に保持するために用いら
れている。 又、上記斜角探触子群の前後には、耐摩耗性を有するシ
ユー17a、17bが小ねじ等(図示せず)を介して取り付け
られている。該シユー17a、17bは、音響くさび15の摩耗
を防止すると共に、音響くさび15と被検管10の表面との
間にギヤツプを保持するために用いられている。 なお、第1図及び第3図において、上記斜角探触子12の
数は6個となつているが、本発明はこの数に限定される
ものではなく、この数は、既に説明したように、被検管
10の寸法範囲(最大スキツプ距離)によつて決定され
る。 一方、前記のような鋼管用斜角探傷ヘツドを用いた本発
明の鋼管用斜角探傷装置は、次のような構成になつてい
る。即ち、第1図及び第2図、又第3図を用いて詳述し
た鋼管用斜角探傷ヘツドが、第1図に示す如く、溶接部
11に対し左右1組ずつ対向して設置されて鋼管用斜角探
傷装置が構成されている。 上記鋼管用斜角探傷ヘツドにおける斜角探触子12の励振
方法により、鋼管用斜角探傷装置は全チヤンネル同時励
振方式のものと個別チヤンネル順次励振方式のものに大
別される。 全チヤンネル同時励振方式の鋼管用斜角探傷装置は、鋼
管用斜角探傷ヘツドにおける各斜角探触子12の全チヤン
ネル1〜nを同時に励振させ、各斜角探傷ヘツド毎に左
右交互に励振させて被検管10の溶接部11を探傷するよう
になつている。第4図は、全チヤンネル同時励振方式の
鋼管用斜角探傷装置の従来からのものを示すブロツク図
である。 この鋼管用斜角探傷装置は、合計n個の探触子、即ちN
o.1探触子〜No.n探触子を用いるものである。又、この
ように複数の探触子に対して、1つのパルサPと、1つ
のレシーバRと、1つのゲートユニツトGとを備える。 この全チヤンネル同時励振方式では、1つの前記パルサ
Pにて、同時に、複数の前記探触子全てを励振し、これ
ら全ての探触子から被検査対象となる物体へと超音波を
同時に伝播させるというものである。このように伝播す
る超音波はパルス状であり、極短時間のものである。 この全チヤンネル同時励振方式では、このように短時間
超音波を伝播させた後、直ちに、前記レシーバRは、複
数の前記探触子へと伝播される超音波を受信する。この
レシーバR及び前記ゲートユニツトGにて、被検査対象
の物体中の、例えば検査対象となる疵等にて反射される
超音波を検出するものである。 このような全チヤンネル同時励振方式の鋼管用斜角探傷
装置では、前記第4図にも示されるとおり、複数の探触
子に対して1組のパルサP、レシーバR及びゲートユニ
ツトGのみを用いる構成となつている。従つて、これら
パルサP、レシーバR及びゲートユニツトGの台数が少
ないという点で、鋼管用斜角探傷装置としてその規模の
縮小(小型化等)を図ることが可能である。 又、個別チヤンネル順次励振方式の鋼管用斜角探傷装置
は、鋼管用斜角探傷ヘツドにおける全ての射角探触子12
を受信可能な状態に保持しながら、各射角探触子を例え
ばNo.1からNo.nへ1個ずつ順次励振させて、被検管10の
溶接部11を探傷するようになつている。第5図は、個別
チヤンネル順次励振方式の鋼管用斜角探傷装置の従来か
らのものを示すブロツク図である。 の個別チヤンネル順次励振方式の鋼管用斜角探傷装置
は、合計n個の探触子、即ちNo.1探触子〜No.n探触子を
用いたものである。この個別チヤンネル順次励振方式で
は、各探触子毎に、パルサPとレシーバRとゲートユニ
ツトGとを備えるチヤンネルユニツト、即ちNo.1チヤン
ネルユニツトU1〜No.nチヤンネルユニツトUnを有する。 又、この個別チヤンネル順次励振方式の鋼管用斜角探傷
装置は、メインクロツク発生器32と、クロツク分配器34
とを備える。該クロツク分配器34は、前記メインクロツ
ク発生器32が発生する一定周期のクロツクパルスに従つ
た主励振タイミングで、前述のNo.1探触子からNo.n探触
子を、それぞれに対応する前述のNo.1チヤンネルユニツ
トU1〜No.nチヤンネルユニツトUnが備える前記パルサP
を用いて、順次励振させながら超音波を発生する。これ
ら各探触子が超音波を励振するタイミングを、それぞ
れ、No.1探触子励振タイミング〜No.n探触子励振タイミ
ングとする。 又、この個別チヤンネル順次励振方式の鋼管用斜角探傷
装置では、1つの探触子がその探触子励振タイミングで
超音波を励振する間、他の探触子については、それぞれ
対応するチヤンネルユニツトU1〜Unが備える前記レシー
バR及び前記ゲートユニツトGを用い、被検査対象とな
る物体中の疵等で反射される超音波を受信する。 即ち、配置位置が異なる各探触子から順次超音波を発生
させると共に、超音波を発生させていない、配置位置が
異なる他の複数の探触子にて、疵等に反射した超音波を
受信するというものである。従つて、この個別チヤンネ
ル順次励振方式の鋼管用斜角探傷装置によれば、被検管
等の被検査対象の物体の溶接部における欠陥の存在位置
等を、欠陥エコーのビーム路程から幾何学的に解明する
ことができる。 なお、この個別チヤンネル順次励振方式の鋼管用斜角探
傷装置では、前述の全チヤンネル同時励振方式のものに
比べ、前記パルサPや前記レシーバRや前記ゲートユニ
ツトGを各探触子毎に必要とし、装置の規模が大きくな
つてしまう。 第6図は、上記個別チヤンネル順次励振方式の鋼管用斜
角探傷装置における順次励振のタイミングを示す図であ
る。この図において、斜角探触子の送信は、各斜角探触
子(No.1〜No.n斜角探触子)によつて順次1個づつ行わ
れ、被検管の欠陥からの反射エコーの受信は全ての斜角
探触子によつて行われる。 第7図に示すように、本発明の鋼管用斜角探傷ヘツドを
使用し、外径406.4mm、管厚9.52mmに加工された外面N5
ノツチ(ノツチ探さ0.48mm)の被検管を探傷したとこ
ろ、第8図乃至第10図で示すような結果が得られた。 第8図は、本発明の鋼管用斜角探傷ヘツドを用いて調査
した各探触子毎の距離振幅特性を示す図であり、図中、
(A)〜(C)は各斜角探触子(具体的には、No.2〜N
o.4の各斜角探触子)毎の距離振幅特性を示している。
従来例と同様の第8図(A)〜(C)においては、スキ
ツプ点でピークエコー高さを示し、斜角探触子と欠陥の
距離が変化するとエコー高さが大きく変化することがわ
かる。 一方、第9図は、本発明の鋼管用斜角探傷ヘツドにおけ
る各斜角探触子を全チヤンネル同時励振方式とした場合
の距離振幅特性を示したもので、探触子距離変化に伴う
エコー高さ変化が極めて小さいことがわかる。 又、第10図は、本発明の鋼管用斜角探傷ヘツドにおける
各斜角探触子を個別順次励振方式とした場合の距離振幅
特性の概念を示しているが、各探触子毎の出力の包絡線
を辿ることになるので、全チヤンネル同時励振方式の場
合と同様に、斜角探触子と欠陥の距離が変化してもエコ
ー高さの変化は極めて小さくなつていることがわかる。 なお、前記実施例においては、本発明が鋼管の探傷に適
用されていたが、本発明の適用対象は、これに限定され
ず、管状材一般の探傷にも同様に適用できることは明ら
かである。
Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. An embodiment of the bevel flaw detection head for steel pipes according to the present invention has a structure as shown in FIGS. 1 and 2 and FIGS. 3 (A) and 3 (B). That is, the oblique probe 12 is composed of a vertical probe 14 having a rectangular contact surface and an acoustic wedge 15 having a radial width (for example, several mm or less). It is attached to the wedge 15 by means of machine screws or the like (not shown). Generally, a transducer is directly bonded to the acoustic wedge to form a bevel probe, but the acoustic wedge in the present embodiment has a radial cross-sectional shape that varies depending on the outer diameter of the test tube, as described later. Need to have. Therefore, in this embodiment, the oblique probe 12 is formed by mounting the acoustic wedge 15 on the vertical probe 14. The vertical probe 14 is a generally used one. For example, "Introduction to nondestructive testing" (corporate association
It is possible to use a very general vertical probe, which is mentioned in detail on the 39th page of the Japan Non-Destructive Inspection Association (1992) together with the beveled probe using figures and the like. The vertical probe propagates the generated ultrasonic wave perpendicularly to the surface of the test body in contact with it. In the above-mentioned “Introduction to Non-Destructive Testing”, the vertical probe is explained, for example, the vibrator and damper (holding body) to be used. The vertical probe has a built-in vibrator that applies a DC pulse voltage to generate ultrasonic waves. A piezoelectric material is used as the oscillator material. Typical examples are crystal and zircon / lead titanate porcelain (abbreviation: zirnamama). Also, for example,
An electrode is attached to the surface by silver plating, and when a DC pulse voltage is applied, the vibrator expands and contracts in the thickness direction at a resonance frequency determined by its thickness.
Further, in the above-mentioned vertical probe, a holding body which plays a role of a damper for quickly stopping vibration is attached to the vibrator and housed in a case. In general, one probe can perform both transmission and reception. In addition, a thin film (not shown) made of oil or the like exists between the contact surface of the vertical probe 14 and the mounting surface of the acoustic wedge 15, and the vertical probe 14 and the acoustic wedge 15 are acoustically coupled to each other. ing. On the other hand, each bevel probe 12 is partitioned by an acoustic dividing plate (not shown). The acoustic wedge 15 has a radial width as described above,
Specifically, the width of the test pipe (electric resistance welded steel pipe) 10 in the circumferential direction is β
It has a radial angle of ゜. Further, when the speed of sound of the incident wave incident on the acoustic wedge 15 and the speed of sound of the refracted wave refracted by the test tube 10 are Ci and Cr, respectively, the relationship between the entrance angle θi of the incident wave and the refraction angle θr of the refracted wave The following equation (2) is established according to the so-called Snell's law. Cr / sin θr = Ci / sin θi (2) Therefore, in order to obtain the desired refraction angle θr, the shape of the acoustic wedge 15 is formed so that the incident angle becomes the incident angle θ. By the way, the acoustic wedge 15 has a radial width as described above, and the radiation angle β ° of the width is determined by the outer diameter of the test tube 10 and the width of the vertical probe 14. By processing the width of the acoustic wedge 15 in the pipe circumferential direction to the radiation angle β ° as described above,
It is easy to arrange the acoustic wedges 15 on the circumference of the test tube 10 in an array as shown in FIG. In order to arrange the bevel probe for transmitting and receiving ultrasonic waves in the pipe circumferential direction at the narrowest interval in the pipe circumferential direction, an acoustic wedge 15 which is an important component in the bevel probe is shown in FIG. The shape has a radial width as shown. That is, the cross-sectional shape of the acoustic wedge 15 in the tube circumferential direction of the test tube 10 as described below mainly with reference to FIG. First, the desired center length of the wedge is lmm and the width of the upper surface of the wedge is ωmm. Further, it is assumed that the ultrasonic wave is incident on the point P 0 of the circle A (radius = r) which is the outer circumference of the test tube 10 at the incident angle θi. At this time, the line segment Q 2 P in FIG.
2 ′, line segment P 2 ′ P 1 ′, line segment P 1 ′ Q 1 , line segment Q 1 Q
The acoustic wedge 15 indicated by 2 is as follows. Points ± ω / 2 from Q 0 on the upper surface of the acoustic wedge 15 are set as points Q 1 and Q 2 , respectively. In order to cause an ultrasonic wave to enter the point P 0 of the circle A (radius = r), which is the outer circumference of the test tube 10 by Q 0 , at the incident angle Qi, the upper surface of the acoustic wedge 15 has a line segment P 0 Q It becomes a line segment Q 1 Q 2 orthogonal to 0 . Also, the line segment P
0 Q 0 is an imaginary circle B of radius r ′ (= r · sin θi)
Located on an extension of the tangent to. Also, the points Q 1 and Q 2
Draw a tangent to each through a circle B of each line segment R 1 Q
1 and a line segment R 2 Q 2 . Assuming that the intersection points of the line segment R 1 Q 1 and the line segment R 2 Q 2 with the circle A are point P 1 and point P 2 , respectively, the point Q 1 on the upper surface of the acoustic wedge 15 will be described.
The incident angle from the circle to the point P 1 of the circle A is θi. Similarly, the incident angle from the upper surface Q 2 of the acoustic wedge 15 to the point P 2 of QA is θi.
Becomes The lower surface of the acoustic wedge 15 is a line segment P 1 ′ P 2 ′ orthogonal to the line segment OP 0, and the sectional shape of the acoustic wedge 15 in the circumferential direction of the test tube 10 is a quadrangle Q 1 Q 2 P 2 Let'P 1 '. At this time, the line segment Q 1 P 1 ′ and the line segment Q 2 P 2 ′ have an angle of β. Further, β is a value approximately obtained by the following equation. That is, at least according to the following equation, this β is obtained in accordance with the outer diameter r of the test tube 10 and the width ω of the acoustic wedge 15 (that is, the width of the vertical probe). β ≒ sin - 1 [ω / (r · cosθi + l)] ... (3) Further, FIG. 3 (A), as it is better illustrated in (B), consisting of a vertical probe 14 and the acoustic wedge 15 The bevel probe 12 is a side plate 16 having an arc shape concentric with the tube 10 to be inspected.
It is held by a and 16b via machine screws or the like (not shown). The side plates 16a and 16b are used to easily hold the bevel probe 12 on the circumference of the test tube 10 in an array. In addition, wear-resistant shoes 17a and 17b are attached to the front and rear of the above-mentioned bevel probe group through small screws or the like (not shown). The shoes 17a and 17b are used to prevent wear of the acoustic wedge 15 and to hold a gear gap between the acoustic wedge 15 and the surface of the test tube 10. 1 and 3, the number of the angle probe 12 is six, but the present invention is not limited to this number, and this number is as described above. The test tube
It is determined by 10 dimensional ranges (maximum skip distance). On the other hand, the steel bevel angle flaw detection device of the present invention using the above-described bevel angle flaw detection head for steel pipe has the following configuration. That is, the oblique angle flaw detection head for steel pipes described in detail with reference to FIGS. 1 and 2 and FIG.
A pair of left and right sides are installed opposite to 11 to form a bevel flaw detection device for steel pipes. According to the method of exciting the bevel probe 12 in the above bevel flaw detection head for steel pipes, the bevel flaw detectors for steel pipe are roughly classified into those of the simultaneous excitation type of all channels and those of the sequential excitation type of individual channels. The all-channel simultaneous excitation type bevel flaw detection device for steel pipes simultaneously excites all the channels 1 to n of each bevel probe 12 in the bevel flaw detection head for steel pipe and alternately excites each bevel flaw detection head to the right and left alternately. By doing so, the welded portion 11 of the test tube 10 is detected. FIG. 4 is a block diagram showing a conventional oblique angle flaw detection apparatus for steel pipes of the all-channel simultaneous excitation system. This bevel angle flaw detector for steel pipes has a total of n probes, namely N
o.1 probe ~ No.n probe is used. Further, as described above, one pulsar P, one receiver R, and one gate unit G are provided for a plurality of probes. In this all-channel simultaneous excitation method, one pulsar P simultaneously excites all of the plurality of probes, and ultrasonic waves are simultaneously propagated from all these probes to an object to be inspected. That is. The ultrasonic wave propagating in this way is in the form of a pulse and is for an extremely short time. In this all-channel simultaneous excitation method, after the ultrasonic waves have been propagated in this way for a short time, the receiver R immediately receives the ultrasonic waves propagated to the plurality of probes. The receiver R and the gate unit G detect ultrasonic waves reflected by, for example, a flaw or the like to be inspected in an object to be inspected. In such an oblique angle flaw detector for steel pipes of the simultaneous excitation type, as shown in FIG. 4, only one set of pulsar P, receiver R and gate unit G is used for a plurality of probes. It is composed. Therefore, in view of the small number of the pulsar P, the receiver R, and the gate unit G, it is possible to reduce the scale (size reduction, etc.) of the oblique angle flaw detection device for steel pipes. In addition, the individual-channel sequential-excitation-type bevel flaw detector for steel pipe is used for all the angle-of-angle probes 12 in the bevel flaw detection head for steel pipe.
While maintaining the state of being able to receive the signal, each angle probe is sequentially excited, for example, from No. 1 to No. n one by one, and the welded portion 11 of the tube 10 to be inspected is detected. . FIG. 5 is a block diagram showing a conventional oblique angle flaw detection apparatus for steel pipes of the individual channel sequential excitation system. The individual-channel sequential excitation type oblique angle flaw detection device for steel pipes uses a total of n probes, that is, No. 1 to No. n probes. In this individual channel sequential excitation system, each probe has a channel unit including a pulser P, a receiver R, and a gate unit G, that is, No. 1 channel unit U1 to No. n channel unit Un. Further, this individual channel sequential excitation type oblique angle flaw detection device for steel pipes includes a main clock generator 32 and a clock distributor 34.
With. The clock distributor 34, at the main excitation timing according to the clock pulse of a constant cycle generated by the main clock generator 32, the No. 1 probe to No. n probe described above, respectively corresponding to the above. No. 1 channel unit U1 to No. n The pulsar P provided in the channel unit Un
The ultrasonic wave is generated by sequentially exciting the ultrasonic wave. The timing at which each of these probes excites ultrasonic waves is defined as No. 1 probe excitation timing to No. n probe excitation timing. Further, in this individual channel sequential excitation type oblique angle flaw detection device for steel pipes, while one probe excites ultrasonic waves at the probe excitation timing, the other transducers respectively correspond to corresponding channel unit units. The receiver R and the gate unit G included in U1 to Un are used to receive ultrasonic waves reflected by a flaw or the like in an object to be inspected. That is, ultrasonic waves are sequentially generated from each probe having a different arrangement position, and ultrasonic waves reflected by a flaw or the like are received by a plurality of other probes having different arrangement positions that do not generate ultrasonic waves. Is to do. Therefore, according to the bevel flaw detector for steel pipes of the individual channel sequential excitation method, the existence position of defects in the welded portion of the object to be inspected such as the inspection pipe is geometrically determined from the beam path of the defect echo. Can be clarified. The individual channel sequential excitation type oblique angle flaw detection device for steel pipes requires the pulsar P, the receiver R, and the gate unit G for each probe, as compared with the above-mentioned all-channel simultaneous excitation type. However, the scale of the device becomes large. FIG. 6 is a diagram showing the timing of sequential excitation in the above-mentioned individual channel sequential excitation system steel bevel flaw detector. In this figure, the transmission of the bevel probe is carried out one by one by each bevel probe (No. 1 to No. n bevel probe) one by one. The reception of the reflected echo is performed by all the bevel probes. As shown in FIG. 7, an outer surface N5 machined to an outer diameter of 406.4 mm and a pipe thickness of 9.52 mm using the bevel flaw detection head for steel pipe of the present invention
When a test tube of a notch (notch probe 0.48 mm) was inspected, the results shown in FIGS. 8 to 10 were obtained. FIG. 8 is a diagram showing distance amplitude characteristics for each probe investigated using the bevel flaw detection head for steel pipe of the present invention.
(A) to (C) are bevel probes (specifically, No. 2 to N).
Distance amplitude characteristics for each bevel probe in o.4 are shown.
In FIGS. 8A to 8C similar to the conventional example, the peak echo height is shown at the skip point, and it can be seen that the echo height greatly changes when the distance between the bevel probe and the defect changes. . On the other hand, FIG. 9 shows distance-amplitude characteristics when each bevel probe in the bevel flaw detection head for steel pipes of the present invention is of the all-channel simultaneous excitation system. It can be seen that the height change is extremely small. Further, FIG. 10 shows the concept of distance-amplitude characteristics when each bevel probe in the bevel flaw detection head for steel pipes of the present invention is an individual sequential excitation system, but the output for each probe is shown. Since it follows the envelope curve of, the change in echo height is extremely small even if the distance between the bevel probe and the defect changes, as in the case of the simultaneous excitation method for all channels. Although the present invention is applied to the flaw detection of the steel pipe in the above-mentioned embodiments, the application target of the present invention is not limited to this, and it is apparent that the present invention can be similarly applied to the flaw detection of tubular materials in general.

【発明の効果】【The invention's effect】

以上詳しく説明したような本発明によれば、探触子と欠
陥の距離が変化してもエコー高さは極僅かしか変化せ
ず、前記従来例のような溶接部の追従を行う必要性がな
くなる。又、エコー高さピークが無いので、被検管の外
径や管厚に関係なく、常に一定位置に斜角探触子ヘツド
をセツトすればよく、前記従来例の如く管厚変更時に探
傷器本体の感度調整を行う必要性等もなくなる等の優れ
た効果を有する。
According to the present invention as described above in detail, even if the distance between the probe and the defect changes, the echo height changes only slightly, and it is necessary to follow the welded portion as in the conventional example. Disappear. Moreover, since there is no echo height peak, it is sufficient to always set the bevel probe head at a fixed position regardless of the outer diameter and thickness of the tube to be inspected. It has excellent effects such as eliminating the need for adjusting the sensitivity of the main body.

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

第1図は、本発明に係る管用斜角探傷ヘツド及びそれを
用いた管用斜角探傷装置の構成を示す断面図、 第2図は、本発明に係る前記管用斜角探傷ヘツドの音響
くさびの断面形状を示す断面図、 第3図(A)は、第1図の矢視A方向から見た平面図、 第3図(B)は、第1図矢視B方向から見た平面図、 第4図は、全チヤンネル同時励振方式の鋼管用斜角探傷
装置の従来からのものを示すブロツク図、 第5図は、個別チヤンネル順次励振方式の鋼管用斜角探
傷装置の従来からのものを示すブロツク図、 第6図は、前記個別チヤンネル順次励振方式の鋼管用斜
角探傷装置における順次励振のタイミングを示す線図、 第7図は、本発明の実施例の作用を説明するための断面
図、 第8図(A)、(B)、(C)は、本発明の鋼管用斜角
探傷ヘツドを用いて調査した、各探触子毎の距離振幅特
性の例を示す線図、 第9図は、斜角探触子を全チヤンネル同時励振方式とし
た場合の距離振幅特性の例を示す線図、 第10図は、斜角探触子を個別順次励振方式とした場合の
距離振幅特性の概念を示す線図、 第11図は、従来の斜角探傷法における距離振幅特性の例
を示す線図、 第12図は、従来の鋼管用斜角探傷装置の一例の構成を示
す平面図、 第13図(A)、(B)、(C)は、それぞれ第12図のA
−A′線、B−B′線、C−C′線に沿う断面図であ
る。 10……被検管、11……溶接部、 12……斜角探触子、13……超音波ビーム、 14……垂直探触子、15……音響くさび、 16a、16b……側板、 17a、17b……シユー、 32……メインクロツク発生器、 34……クロツク分配器 P……パルサ、R……レシーバ、 G……ゲートユニツト、 U〜Un……チヤンネルユニツト。
FIG. 1 is a cross-sectional view showing the structure of a pipe bevel flaw detection head for pipes according to the present invention and a pipe bevel flaw detection device using the same, and FIG. 2 is an acoustic wedge of the pipe bevel flaw detection head for pipes according to the present invention. Sectional drawing which shows sectional shape, FIG. 3 (A) is the top view seen from the arrow A direction of FIG. 1, FIG. 3 (B) is the top view seen from the arrow B direction of FIG. 1, FIG. 4 is a block diagram showing a conventional oblique-angle flaw detector for steel pipes of all-channel simultaneous excitation type, and FIG. 5 shows a conventional oblique-angle flaw detector for steel pipes of individual channel sequential excitation type. FIG. 6 is a block diagram showing the same, FIG. 6 is a diagram showing the timing of sequential excitation in the above-described individual channel sequential excitation type oblique angle flaw detection apparatus for steel pipes, and FIG. 7 is a sectional view for explaining the operation of the embodiment of the present invention. FIGS. 8 (A), 8 (B), and 8 (C) are oblique angle flaw detection heads for steel pipes of the present invention. Fig. 9 is a diagram showing an example of distance-amplitude characteristics of each probe investigated by using Fig. 9, and Fig. 9 is a line showing an example of distance-amplitude characteristics when the bevel probe is of the all-channel simultaneous excitation method. Figures and 10 are diagrams showing the concept of distance-amplitude characteristics when the bevel probe is an individual sequential excitation method, and Fig. 11 shows an example of distance-amplitude characteristics in the conventional bevel flaw detection method. Fig. 12 is a plan view showing an example of the configuration of a conventional bevel flaw detector for steel pipes, and Figs. 13 (A), (B), and (C) are A of Fig. 12, respectively.
FIG. 6 is a cross-sectional view taken along line -A ', line BB', and line CC '. 10 …… Inspected tube, 11 …… Welded part, 12 …… Blade probe, 13 …… Ultrasonic beam, 14 …… Vertical probe, 15 …… Acoustic wedge, 16a, 16b …… Side plate, 17a, 17b ... Shew, 32 ... Main clock generator, 34 ... Clock distributor P ... Pulsar, R ... Receiver, G ... Gate unit, U 1 to Un ... Channel unit.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】超音波斜角探傷法により、被検管の管軸方
向の欠陥を検査するために用いられる管用斜角探傷ヘツ
ドにおいて、 複数個の斜角探傷子を、前記被検管の管周方向に隙間な
く効率的に配置するために、それぞれの該斜角探触子が
垂直探触子と音響くさびとにて構成され、前記被検管の
管周方向における前記音響くさびの断面形状が、前記被
検管側より前記垂直探触子側が幅広の、前記被検管の外
径と前記垂直探触子の幅とによつて決定される放射角β
の放射角状の形状であつて、 更に、前記音響くさびの断面形状が、前記被検管の管周
方向に斜めに超音波を励振又は受信すべく、管周方向で
入射角θiとなるように傾斜配置される形状であり、 前記入射角θiと直交する前記音響くさびの取り付け面
に対して、垂直方向に超音波を励振又は受信する前記垂
直探触子を取り付けると共に、 複数の前記斜角探触子を、前記管周方向にアレイ状に隙
間なく且つ傾斜配置状態で装着する、前記被検管と同芯
円の円弧形状の側板を有し、 又、アレイ状の複数の前記斜角探触子の前後に設けられ
た、前記被検管の表面と前記音響くさびとの間のギヤツ
プを保持し、該音響くさびの摩耗を防ぐ、耐摩耗性の1
対のシユーを有することを特徴とする管用斜角探傷ヘツ
ド。
1. A pipe bevel flaw detection head for a pipe used for inspecting a defect in a tube axis direction of a subject pipe by an ultrasonic bevel flaw detection method, comprising: In order to arrange the angle probes in a circumferential direction of the pipe efficiently without gaps, each of the bevel probes is composed of a vertical probe and an acoustic wedge, and a cross section of the acoustic wedge in the pipe circumferential direction of the test tube. A radiation angle β whose shape is determined by the outer diameter of the test tube and the width of the vertical probe, the width of which is wider on the vertical probe side than on the test tube side.
And the cross-sectional shape of the acoustic wedge has an incident angle θi in the tube circumferential direction so as to excite or receive ultrasonic waves obliquely in the tube circumferential direction of the test tube. And a plurality of the slanted angles with which the vertical probe that excites or receives ultrasonic waves in a vertical direction is attached to a mounting surface of the acoustic wedge that is orthogonal to the incident angle θi. The probe is mounted in an array in the circumferential direction of the pipe in a state of no gaps and in a slanted arrangement, and has side plates in an arc shape concentric with the pipe to be inspected. A wear-resistant 1 which is provided before and after the probe, holds a gear gap between the surface of the tube to be inspected and the acoustic wedge, and prevents abrasion of the acoustic wedge.
An oblique angle head for pipes, characterized by having a pair of shoes.
【請求項2】請求項1に記載の管用斜角探傷ヘツドを具
備して、被検管を探傷することを特徴とする管用斜角探
傷装置。
2. A bevel angle flaw detector for a pipe, comprising the bevel angle flaw detection head for a pipe according to claim 1 for flaw detection of a pipe to be inspected.
JP63209210A 1988-08-23 1988-08-23 Angle beam inspection head for pipes and angle beam inspection device for pipes using the same Expired - Lifetime JPH0664027B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63209210A JPH0664027B2 (en) 1988-08-23 1988-08-23 Angle beam inspection head for pipes and angle beam inspection device for pipes using the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63209210A JPH0664027B2 (en) 1988-08-23 1988-08-23 Angle beam inspection head for pipes and angle beam inspection device for pipes using the same

Publications (2)

Publication Number Publication Date
JPH0257973A JPH0257973A (en) 1990-02-27
JPH0664027B2 true JPH0664027B2 (en) 1994-08-22

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Application Number Title Priority Date Filing Date
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Country Link
JP (1) JPH0664027B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102006046327A1 (en) * 2006-09-29 2008-04-10 Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. Ultraschallprüfanordnung
JP2011237208A (en) * 2010-05-07 2011-11-24 Hitachi-Ge Nuclear Energy Ltd Ultrasonic inspection device and ultrasonic inspection method
CN113406213B (en) * 2021-06-29 2022-11-29 西安热工研究院有限公司 Curved surface sound-transmitting wedge design method for circumferential ultrasonic detection of small-diameter pipe

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5667750A (en) * 1979-11-08 1981-06-08 Kawasaki Steel Corp Automatic ultrasonic flaw detecting method
JPS6230951A (en) * 1985-08-02 1987-02-09 Power Reactor & Nuclear Fuel Dev Corp Probe for ultrasonic flaw detector
JPS6338157A (en) * 1986-08-04 1988-02-18 Power Reactor & Nuclear Fuel Dev Corp Ultrasonic probe

Also Published As

Publication number Publication date
JPH0257973A (en) 1990-02-27

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