JPH0521502B2 - - Google Patents

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Publication number
JPH0521502B2
JPH0521502B2 JP61183020A JP18302086A JPH0521502B2 JP H0521502 B2 JPH0521502 B2 JP H0521502B2 JP 61183020 A JP61183020 A JP 61183020A JP 18302086 A JP18302086 A JP 18302086A JP H0521502 B2 JPH0521502 B2 JP H0521502B2
Authority
JP
Japan
Prior art keywords
ultrasonic
curved
transducer
probe
curvature
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
JP61183020A
Other languages
Japanese (ja)
Other versions
JPS6338157A (en
Inventor
Kenichi Tanimoto
Hirotsugu Tanaka
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
Mitsubishi Electric Corp
Original Assignee
Doryokuro Kakunenryo Kaihatsu Jigyodan
Mitsubishi Electric Corp
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, Mitsubishi Electric Corp filed Critical Doryokuro Kakunenryo Kaihatsu Jigyodan
Priority to JP61183020A priority Critical patent/JPS6338157A/en
Publication of JPS6338157A publication Critical patent/JPS6338157A/en
Publication of JPH0521502B2 publication Critical patent/JPH0521502B2/ja
Granted legal-status Critical Current

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

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は既設配管に発生する欠陥を管材の軸
方向に超音波を送受信することにより超音波探傷
試験を行なう超音波探触子に関するものである。
[Detailed Description of the Invention] [Field of Industrial Application] This invention relates to an ultrasonic probe that performs an ultrasonic flaw detection test to detect defects occurring in existing piping by transmitting and receiving ultrasonic waves in the axial direction of the pipe material. be.

〔従来の技術〕[Conventional technology]

第4図は例えば超音波探傷法(昭和49年日刊工
業新聞社発行)に示された従来の超音波探触子を
示す断面図であり、第4図aは斜角探触子の正面
断面図、第4図bは斜角探触子の横断面図であ
る。
Figure 4 is a cross-sectional view of a conventional ultrasonic probe shown in, for example, Ultrasonic Flaw Detection Method (published by Nikkan Kogyo Shimbun, 1972), and Figure 4a is a front cross-section of an angle probe. Figure 4b is a cross-sectional view of the angle probe.

図において、1は超音波の送受信を行なうため
の平板形の振動子、2は上記振動子1の固定と、
上記振動子1から発生する縦波超音波を横波超音
波にモード変換させるためのプラスチツク製の
楔、3は不要な超音波を吸収する吸音材、4は探
触子ケース、5は管材等の試験体、6は超音波の
伝播効率を高めるための探触媒体、イは縦波超音
波、ロは横波超音波である。
In the figure, 1 is a flat plate-shaped transducer for transmitting and receiving ultrasonic waves, 2 is a plate-shaped transducer for fixing the transducer 1,
A plastic wedge is used to convert the longitudinal ultrasound generated from the transducer 1 into a transverse ultrasound, 3 is a sound absorbing material that absorbs unnecessary ultrasound, 4 is a probe case, and 5 is a tube material, etc. The test specimen 6 is a probe for increasing the propagation efficiency of ultrasonic waves, A is a longitudinal wave ultrasonic wave, and B is a transverse wave ultrasonic wave.

従来の超音波探触子は上記のように構成されて
おり、振動子1から発生した縦波超音波イは、楔
2内を伝播し、上記楔2と試験体5との境界面で
スネルの法則により横波超音波ロに変換されて試
験体5の前方へ伝播し、上記試験体5中の欠陥又
は不連続部分で反射し、再び逆経路で振動子1に
縦波超音波イが受信される。
A conventional ultrasonic probe is constructed as described above, and the longitudinal ultrasonic wave A generated from the transducer 1 propagates within the wedge 2 and forms a Snell at the interface between the wedge 2 and the test specimen 5. According to the law, the transverse wave is converted into a transverse ultrasonic wave B, propagates forward of the test object 5, is reflected by a defect or discontinuous part in the test object 5, and is received by the transducer 1 again on the reverse path as a longitudinal wave ultrasonic wave A. be done.

この時に、従来の超音波探触子では探触子ケー
ス4の中に振動子1が1個具備されているだけで
あるため、試験体5の管周方向に対応する方向の
超音波ビーム幅が狭く、上記試験体5の管周方向
全周にわたつて検査を行なう場合には、超音波探
触子の走査回数が極めて多くなり、検査時間の短
縮を計れない状況にあつた。
At this time, since the conventional ultrasonic probe has only one transducer 1 in the probe case 4, the ultrasonic beam width in the direction corresponding to the circumferential direction of the test specimen 5 is If the test specimen 5 was to be inspected over its entire circumference in the tube circumferential direction, the number of scans of the ultrasonic probe would be extremely large, making it impossible to reduce the inspection time.

〔発明が解決しようとする問題点〕 上記のように振動子1が1個だけ具備されてい
る超音波探触子では試験体5の管周方向に対応す
る超音波ビーム幅が狭いために、検査時間が多く
なる問題点があつた。
[Problems to be Solved by the Invention] As described above, in the ultrasonic probe equipped with only one transducer 1, the ultrasonic beam width corresponding to the circumferential direction of the test specimen 5 is narrow. There was a problem that the inspection time was increased.

また、上記問題点を解決させるために、試験体
5の管周方向に従来の超音波探触子を複数個配置
させたとしても、従来の超音波探触子の振動子1
は平板形状であるために超音波ビーム幅が狭く、
お互いの超音波探触子間に超音波ビーム幅がオー
バラツプしない領域が生じ、上記の場合において
も検査時間の短縮はあまり期待できないという問
題点があつた。
In addition, in order to solve the above problem, even if a plurality of conventional ultrasonic probes are arranged in the circumferential direction of the test specimen 5, the transducer 1 of the conventional ultrasonic probe
Because it has a flat plate shape, the ultrasonic beam width is narrow;
There is a problem in that there is a region where the ultrasound beam widths do not overlap between the ultrasound probes, and even in the above case, shortening of the inspection time cannot be expected much.

この発明は上記問題点を解決するためになされ
たもので、複数個の振動子間の超音波ビーム幅を
確実にオーバラツプさせ、1個の超音波探触子に
おける超音波ビーム幅が試験体の管周方向で120°
以上の領域を確保できる超音波探触子を得ること
を目的とする。
This invention was made to solve the above problems, and it ensures that the ultrasonic beam widths of multiple transducers overlap, so that the ultrasonic beam width of one ultrasonic probe is the same as that of the test specimen. 120° in circumferential direction
The purpose is to obtain an ultrasonic probe that can secure the above area.

〔問題点を解決するための手段〕[Means for solving problems]

この発明による超音波探触子は、超音波が拡散
するような曲面振動子を試験体の管周方向に所定
の角度で複数個配置させたものである。
The ultrasonic probe according to the present invention has a plurality of curved transducers that diffuse ultrasonic waves arranged at a predetermined angle in the circumferential direction of a test specimen.

〔作用〕[Effect]

この発明においては、曲面振動子から発生する
超音波ビームの拡がりが、隣接する曲面振動子か
ら発生する超音波ビームと完全にオーバラツプす
るように振動子の寸法と曲率半径と、振動子の配
置角度とを選択し、かつ、1個の超音波探触子に
おける総合した超音波ビーム幅が試験体の管周方
向で120°以上の領域を確保できる数の曲面振動子
を備えているために、検査時間を大幅に短縮でき
ることになる。
In this invention, the dimensions and radius of curvature of the transducer and the arrangement angle of the transducer are determined so that the spread of the ultrasound beam generated from the curved transducer completely overlaps with the ultrasound beam generated from the adjacent curved transducer. In addition, it is equipped with a number of curved transducers that can ensure an area where the total ultrasonic beam width of one ultrasonic probe is 120 degrees or more in the circumferential direction of the test specimen. This will greatly reduce inspection time.

〔実施例〕〔Example〕

第1図はこの発明の一実施例を示す超音波探触
子の断面図であり、第1図aは斜角探触子の正面
断面図、第1図bは斜角探触子の横断面図であ
る。
FIG. 1 is a sectional view of an ultrasonic probe showing an embodiment of the present invention, FIG. 1a is a front sectional view of the angle probe, and FIG. 1b is a cross-sectional view of the angle probe. It is a front view.

図において、1a〜1dは超音波が拡散するよ
うな曲率を有する曲面振動子、2は上記曲面振動
子の曲率半径と同等の曲率半径を有するプラスチ
ツク製の楔、3は不要な超音波を吸収する吸音
材、4は探触子ケース、5は管材等の試験体、6
は接触媒体、7は楔2と試験体5とのすき間を保
持させるシユー、イは縦波超音波、ロは横波超音
波、Aは曲面振動子1a〜1bのお互いの配置角
度である。
In the figure, 1a to 1d are curved transducers with curvatures that allow ultrasound to diffuse; 2 is a plastic wedge with a radius of curvature equivalent to that of the curved transducer; 3 is a wedge that absorbs unnecessary ultrasound waves. 4 is a probe case, 5 is a test piece such as a pipe material, 6 is a sound absorbing material to be
7 is a contact medium, 7 is a shoe for maintaining the gap between the wedge 2 and the test specimen 5, A is a longitudinal wave ultrasonic wave, B is a transverse wave ultrasonic wave, and A is a mutual arrangement angle of the curved surface transducers 1a to 1b.

第2図はこの発明による超音波探触子で形成さ
れる超音波ビーム幅を示す図である。
FIG. 2 is a diagram showing the width of an ultrasonic beam formed by the ultrasonic probe according to the present invention.

図において、ハは曲面振動子1aで形成される
超音波ビーム幅、ニは曲面振動子1bで形成され
る超音波ビーム幅、ホは曲面振動子1cで形成さ
れる超音波ビーム幅、ヘは曲面振動子1dで形成
される超音波ビーム幅、Hは超音波信号の振幅、
θは試験体5の管周方向角度である。
In the figure, C is the ultrasonic beam width formed by the curved transducer 1a, D is the ultrasonic beam width formed by the curved transducer 1b, E is the ultrasonic beam width formed by the curved transducer 1c, and F is the ultrasonic beam width formed by the curved transducer 1c. The width of the ultrasound beam formed by the curved transducer 1d, H is the amplitude of the ultrasound signal,
θ is the circumferential angle of the test specimen 5.

第3図は試験体の外径寸法に対して、曲面振動
子の寸法、曲率半径、配置角度の相関を示す図で
ある。
FIG. 3 is a diagram showing the correlation between the dimensions, radius of curvature, and arrangement angle of the curved vibrator with respect to the outer diameter dimension of the test specimen.

図において、1a,1bは曲面振動子、2は
楔、5は試験体、Aは曲面振動子1aの配置角
度、Lは曲面振動子1aの寸法、l1は試験体5表
面における曲面振動子1a中心からの超音波のビ
ーム幅、l2は試験体5内表面における曲面振動子
1a中心からの超音波ビーム幅、Rは曲面振動子
1aの曲率半径、θ1は曲面振動子1aから放射さ
れる超音波の角度、θ2は試験体5表面におけるビ
ーム幅l1と法線QOとのなす角度、θ3は試験体5
への超音波の入射角度、θ4は試験体5中での超音
波の屈折角度である。
In the figure, 1a and 1b are curved oscillators, 2 is a wedge, 5 is a specimen, A is the arrangement angle of the curved oscillator 1a, L is the dimension of the curved oscillator 1a, and l 1 is the curved oscillator on the surface of the specimen 5. 1a is the ultrasonic beam width from the center of the curved surface transducer 1a, l2 is the ultrasound beam width from the center of the curved surface transducer 1a on the inner surface of the test object 5, R is the radius of curvature of the curved surface transducer 1a, and θ1 is the radiation from the curved surface transducer 1a. θ 2 is the angle between the beam width l 1 on the surface of the specimen 5 and the normal QO, and θ 3 is the angle of the ultrasonic wave generated on the surface of the specimen 5.
θ 4 is the angle of refraction of the ultrasonic wave in the specimen 5.

ここで、曲面振動子1aの寸法Lは欠陥出能の
低下を防止するために20mm以下にすることが望ま
しい。また、超音波探触子1ブロツクでの超音波
のカバー範囲は、超音波探触子と試験体5との着
脱の容易性から180°以下が望ましく、かつ360°を
整数で割り切れる値がデータ処理上望ましく、多
くは120°が一つの目安となる。
Here, the dimension L of the curved surface vibrator 1a is desirably 20 mm or less in order to prevent a decrease in defect production ability. In addition, the ultrasonic coverage range of one block of the ultrasonic probe is preferably 180 degrees or less for ease of attachment and detachment between the ultrasonic probe and the test specimen 5, and the data should be such that 360 degrees is divisible by an integer. It is desirable for processing, and in most cases 120° is one guideline.

さらに、曲面振動子1aの曲率半径Rは楔2内
を超音波が伝播する距離の最小値と最大値の差が
楔2内の波長で1/4〜1/2程度になるようにするこ
とにより超音波が急激に拡散し、欠陥検出能を低
下させるのを防止できる。
Furthermore, the radius of curvature R of the curved transducer 1a should be such that the difference between the minimum and maximum distances of the ultrasonic waves propagating within the wedge 2 is approximately 1/4 to 1/2 of the wavelength within the wedge 2. This can prevent ultrasonic waves from rapidly diffusing and reducing defect detection ability.

上記前提条件のもとで、曲面振動子1aの寸法
L、曲面振動子1aの曲率半径R、曲面振動子1
aの配置角度Aは以下の関係により求めることが
できる。
Under the above preconditions, the dimension L of the curved surface vibrator 1a, the radius of curvature R of the curved surface vibrator 1a, the curved surface vibrator 1
The arrangement angle A of a can be determined from the following relationship.

W=t/cosθS ……(1) l2=sinθ1×(R+Δl) ……(2) θ2=sin-1(l1/D/2) ……(3) θ3=θ1+θ2 ……(4) θ4=sin-1(V2/V1×sinθ3) ……(5) l2≒l1+tan(θ4−θ2)×W ……(6) A=2×sin-1(l2/D/2−t) ……(7) n≧/A ……(8) 但し、仮定条件として λ/4≦R2−(L/2)2≦λ/2 ……(9) なお(1)〜(9)式において t:試験体の厚さ Δl:楔の長さ V1:楔の縦波音速 V2:試験体の横波音速 n:曲面振動子の数 :探触子1ブロツク当たりのカバー範囲 θS:試験体中の横波屈折角 D:試験体の外径寸法 W:試験体中の0.5スキツプ距離 λ:楔中の波長 を表わす。 W=t/cosθ S ...(1) l 2 = sinθ 1 × (R+Δl) ...(2) θ 2 = sin -1 (l 1 /D/2) ...(3) θ 312 ...(4) θ 4 = sin -1 (V 2 /V 1 × sin θ 3 ) ... (5) l 2 ≒ l 1 + tan (θ 4 - θ 2 ) × W ... (6) A = 2 ×sin -1 (l 2 /D/2-t) ……(7) n≧/A ……(8) However, the assumption is that λ/4≦R 2 −(L/2) 2 ≦λ/2 ...(9) In equations (1) to (9), t: Thickness of the test specimen Δl: Length of the wedge V 1 : Longitudinal sound velocity of the wedge V 2 : Transverse sound velocity of the test specimen n: Curved surface vibrator length Number: Coverage range per probe block θ S : Shear wave refraction angle in the specimen D: Outer diameter of the specimen W: 0.5 skip distance in the specimen λ: Represents the wavelength in the wedge.

この一実施例では試験体5の外径60.5mmの時に
曲面振動子1a〜1dの寸法Lを18mmとし、上記
曲面振動子1a〜1dの曲率半径Rを150mmとし、
配置角度Aを30°に選択することにより、4個の
曲面振動子1a〜1dで試験体5の管周約120°に
わたつて超音波を送受信することを可能とした。
In this example, when the outer diameter of the test body 5 is 60.5 mm, the dimension L of the curved surface vibrators 1a to 1d is 18 mm, the radius of curvature R of the curved surface vibrators 1a to 1d is 150 mm,
By selecting the arrangement angle A to be 30°, it was possible to transmit and receive ultrasonic waves over a tube circumference of about 120° of the test specimen 5 using the four curved transducers 1a to 1d.

すなわち、上記のように構成された超音波探触
子においては、超音波の送受を行なう曲面振動子
1a〜1dから発生した縦波超音波イは楔2の中
を拡散しながら伝播し、さらにスネルの法則によ
り試験体5の外径曲率に対応して管周方向に横波
超音波ロとしてさらに拡散伝播することになる。
従つて、試験体5の外径寸法に応じて、曲面振動
子1a〜1dの寸法Lと、上記曲面振動子1a〜
1dの曲率半径Rと、上記曲面振動子1a〜1d
の配置角度Aを(7)〜(9)式により決定することによ
り、より少ない曲面振動子1a〜1dの数で、試
験体5の管周方向の広範囲にわたつて超音波を送
受信することが可能となる。また、当然ながら、
お互いの曲面振動子1a〜1d間の超音波ビーム
幅ハ〜ニは−3dB以内の振幅で完全にオーバラツ
プさせることも容易に可能となる。
That is, in the ultrasonic probe configured as described above, the longitudinal ultrasonic waves A generated from the curved transducers 1a to 1d that transmit and receive ultrasonic waves propagate while being diffused in the wedge 2, and further According to Snell's law, the transverse ultrasonic waves are further diffused and propagated in the tube circumferential direction in accordance with the outer diameter curvature of the test specimen 5.
Therefore, the dimension L of the curved surface vibrators 1a to 1d and the curved surface vibrators 1a to 1d are determined according to the outer diameter dimension of the test body 5.
The radius of curvature R of 1d and the curved surface vibrators 1a to 1d
By determining the arrangement angle A using equations (7) to (9), ultrasonic waves can be transmitted and received over a wide range in the circumferential direction of the test specimen 5 with a smaller number of curved transducers 1a to 1d. It becomes possible. Also, of course,
The ultrasonic beam widths H to D between the curved surface transducers 1a to 1d can easily be completely overlapped with amplitudes within -3 dB.

また、プラスチツク製の楔2の曲面振動子1a
〜1dが当接させる面には、上記曲面振動子1a
〜1dの曲率半径と同等の曲率半径を有し、か
つ、試験体5と対向する面は、上記試験体5の外
径に対して所定のすき間を加えた量だけの曲率半
径を有している。つまり、試験体5の外径公差、
真円度等を考慮した場合に、楔2と試験体5との
接触面積が大きくなるために、上記楔2と試験体
5の外表面との間にはシユー7を用いることによ
り所定のすき間を設け、上記すき間に接触媒体を
供給することにより音響結合不良を防止するよう
にしてある。
In addition, the curved surface vibrator 1a of the plastic wedge 2
The curved surface vibrator 1a is placed on the surface that 1d contacts.
~1d, and the surface facing the specimen 5 has a radius of curvature equal to the outer diameter of the specimen 5 plus a predetermined gap. There is. In other words, the outer diameter tolerance of the test specimen 5,
In order to increase the contact area between the wedge 2 and the test piece 5 when roundness etc. are taken into consideration, a shoe 7 is used between the wedge 2 and the outer surface of the test piece 5 to create a predetermined gap. is provided, and a contact medium is supplied to the gap to prevent poor acoustic coupling.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明したように、超音波拡散形
の曲面振動子を、試験体の管周方向に対応する楔
上に所定の角度で複数個配置することにより、試
験体の管周方向における検査範囲を広くできるの
で、検査時間を大幅に短縮できる効果がある。
As explained above, this invention enables inspection in the circumferential direction of a test specimen by arranging a plurality of ultrasonic diffusion type curved surface transducers at a predetermined angle on a wedge corresponding to the circumferential direction of the test specimen. Since the range can be widened, the inspection time can be significantly shortened.

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

第1図はこの発明による超音波探触子の断面図
で、第1図aは正面断面図、第1図bは横断面
図、第2図はこの発明による超音波探触子の超音
波ビーム幅を示す図、第3図は曲面振動子の寸
法、曲率半径、配置角度の相関を示す図、第4図
は従来の超音波探触子の断面図で、第4図aは正
面断面図、第4図bは横断面図である。 図において、1は平板の振動子、1a〜1dは
曲面振動子、2は楔、3は吸音材、4は探触子ケ
ース、5は試験体、イは縦波超音波、ロは横波超
音波、ハ〜ニは超音波ビーム幅、Aは曲面振動子
の配置角度である。なお、各図中同一符号は同
一、または相当部分を示す。
FIG. 1 is a cross-sectional view of an ultrasonic probe according to the present invention, FIG. 1 a is a front cross-sectional view, FIG. 1 b is a cross-sectional view, and FIG. Figure 3 is a diagram showing the beam width, Figure 3 is a diagram showing the correlation between dimensions, radius of curvature, and arrangement angle of the curved transducer, Figure 4 is a cross-sectional view of a conventional ultrasound probe, and Figure 4a is a front cross-section. Figure 4b is a cross-sectional view. In the figure, 1 is a flat plate transducer, 1a to 1d are curved transducers, 2 is a wedge, 3 is a sound absorbing material, 4 is a probe case, 5 is a test specimen, A is a longitudinal wave ultrasound wave, and B is a transverse wave ultrasound wave. In the sound wave, H~D is the ultrasonic beam width, and A is the arrangement angle of the curved transducer. Note that the same reference numerals in each figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 1 管材の軸方向に超音波を送受信する斜角探触
子において、上記管材の管周方向に、所定の配置
角度で複数個配置した超音波拡散形の曲面振動子
と、上記曲面振動子と管材との間には、上記曲面
振動子が当接する面には上記曲面振動子の曲率半
径と同等の曲率半径を有し、かつ管材外表面に対
向する面には、上記管材外径の曲率に相当する曲
率を有したプラスチツク製の楔とを具備したこと
を特徴とする超音波探触子。
1. In an angle probe that transmits and receives ultrasonic waves in the axial direction of a tube material, a plurality of ultrasonic diffusion type curved transducers arranged at a predetermined arrangement angle in the circumferential direction of the tube material, and the curved surface transducer and The surface with which the curved surface vibrator comes into contact with the tube material has a radius of curvature equivalent to the radius of curvature of the curved surface vibrator, and the surface facing the outer surface of the tube material has a curvature radius equal to the outer diameter of the tube material. An ultrasonic probe comprising a plastic wedge having a curvature corresponding to .
JP61183020A 1986-08-04 1986-08-04 Ultrasonic probe Granted JPS6338157A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61183020A JPS6338157A (en) 1986-08-04 1986-08-04 Ultrasonic probe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61183020A JPS6338157A (en) 1986-08-04 1986-08-04 Ultrasonic probe

Publications (2)

Publication Number Publication Date
JPS6338157A JPS6338157A (en) 1988-02-18
JPH0521502B2 true JPH0521502B2 (en) 1993-03-24

Family

ID=16128335

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61183020A Granted JPS6338157A (en) 1986-08-04 1986-08-04 Ultrasonic probe

Country Status (1)

Country Link
JP (1) JPS6338157A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2020056724A (en) * 2018-10-03 2020-04-09 三菱日立パワーシステムズ株式会社 Ultrasonic inspection device and ultrasonic inspection method

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0664027B2 (en) * 1988-08-23 1994-08-22 川崎製鉄株式会社 Angle beam inspection head for pipes and angle beam inspection device for pipes using the same
JP5730183B2 (en) * 2011-12-14 2015-06-03 三菱重工業株式会社 Ultrasonic flaw detector
EP3701257B1 (en) * 2017-10-27 2024-03-20 Westinghouse Electric Company Llc Apparatus and method for improved corrosion thinning detection

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2020056724A (en) * 2018-10-03 2020-04-09 三菱日立パワーシステムズ株式会社 Ultrasonic inspection device and ultrasonic inspection method

Also Published As

Publication number Publication date
JPS6338157A (en) 1988-02-18

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