JPS6338157A - Ultrasonic probe - Google Patents

Ultrasonic probe

Info

Publication number
JPS6338157A
JPS6338157A JP61183020A JP18302086A JPS6338157A JP S6338157 A JPS6338157 A JP S6338157A JP 61183020 A JP61183020 A JP 61183020A JP 18302086 A JP18302086 A JP 18302086A JP S6338157 A JPS6338157 A JP S6338157A
Authority
JP
Japan
Prior art keywords
ultrasonic
curved
curvature
vibrators
probe
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.)
Granted
Application number
JP61183020A
Other languages
Japanese (ja)
Other versions
JPH0521502B2 (en
Inventor
Kenichi Tanimoto
谷本 健一
Hirotsugu Tanaka
洋次 田中
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.)
Mitsubishi Electric Corp
Power Reactor and Nuclear Fuel Development Corp
Original Assignee
Mitsubishi Electric Corp
Power Reactor and Nuclear Fuel Development 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 Mitsubishi Electric Corp, Power Reactor and Nuclear Fuel Development Corp filed Critical Mitsubishi Electric Corp
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)

Abstract

PURPOSE:To shorten an inspection time greatly by arranging plural curved- surface vibrators which diffuse ultrasonic waves at specific angles in the tube direction of a body to be tested. CONSTITUTION:The size and radius of curvature of the curved-surface vibrators and the arrangement angles A of the vibrators are so selected that spreads of ultrasonic wave beams generated by the vibrators 1a and 1c overlap with ultrasonic wave beams generated by adjacent curved-surface vibrators 1b and 1d. Then, many curved-surface vibrators enough for the width of an ultrasonic wave beam on one ultrasonic probe to secure an area of more than a specific angle in the tube periphery direction of the body 5 to be tested are provided to widen the inspection range, thereby shortening the inspection time greatly.

Description

【発明の詳細な説明】 〔成業上の利用分野〕 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深傷試暎を行なう超
音波探触子に関するものである。
[Detailed Description of the Invention] [Field of Commercial Application] This invention relates to an ultrasonic probe that detects defects occurring in existing piping by transmitting and receiving ultrasonic waves in the axial direction of the pipe material. It is related to.

〔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−1
ir聞社発行)に示された従来の超音波探触子を示す断
面図であシ、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 shows, for example, the ultrasonic flaw detection method (1971 Nikkan Kogyo-1).
Fig. 4(a) is a front sectional view of an angle probe;
FIG. 4(b) 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。
In the figure, (1) is a flat plate-shaped transducer for transmitting and receiving ultrasonic waves, and (2) is the fixing of the transducer (1).

上記振動子(11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ック製の楔。
A plastic wedge for mode converting the longitudinal ultrasonic waves generated from the transducer (11) into transverse ultrasonic waves.

(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接触媒体、イは縦波超音波。
(3) is a sound absorbing material that absorbs unnecessary ultrasonic waves, (4) is a probe case, (5) is a test piece such as a pipe material, and (6) is a contact medium to increase the propagation efficiency of ultrasonic waves. is longitudinal ultrasound.

口は横波超音波である。The mouth is transverse ultrasound.

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(11から発生した縦波超音波イは、楔(2)内を
伝播し、上記俣(2)と試験体(5)との境界面でスネ
ルの法則によシ横波超音波口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fl)に縦波超音波
イが受信される。
The conventional ultrasonic probe is constructed as described above, and the longitudinal ultrasonic wave A generated from the transducer (11) propagates within the wedge (2) and connects the above-mentioned mat (2) and the test specimen (5). ) at the interface with the specimen (5) where the transverse wave is converted into an ultrasonic wave according to Snell's law.
The longitudinal wave ultrasonic wave A propagates forward, is reflected by a defect or a discontinuous part in the test object (5), and is again received by the transducer fl) on the reverse path.

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(11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
っ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っ
た。
At this time, with conventional ultrasound probes, the probe case (4)
Since only one transducer (11) is provided in the tube, the ultrasonic beam width in the direction corresponding to the circumferential direction of the test specimen (5) is narrow; When inspecting the entire circumference, the number of scans of the ultrasonic probe becomes extremely large, making it impossible to reduce the inspection time.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

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
あった。
As mentioned above, in the case of an ultrasonic probe equipped with only one transducer (1), the ultrasonic beam width corresponding to the circumferential direction of the test specimen (5) is narrow, resulting in a long inspection time. There was a point.

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+11は平板形状で
あるために超音波ビーム幅が狭く。
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 +11 of the conventional ultrasonic probe is a flat plate. Due to its shape, the ultrasound beam width is narrow.

お互いの超音波探触子間に超音波ビーム幅がオーバラッ
プしない領域が生じ、上記の場合においても検量時間の
短縮はあまり期待できないという問題点があった。
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, the calibration time cannot be expected to be reduced 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
ップさせ、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fc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 in order to solve the above problems, and it is possible to ensure that the ultrasonic beam widths of multiple transducers overlap, so that the ultrasonic beam width of one ultrasonic probe is An object of the present invention is to obtain an ultrasonic probe that can secure an area fc of 120° or more in the tube circumferential direction.

〔問題点を解決するだめの手段〕[Failure to solve the problem]

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1曲面振動子から発生する超音波ビ
ームの拡がりが2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ップするように憑動子の寸法
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 are adjusted so that the spread of the ultrasonic beam generated from one curved transducer completely overlaps the ultrasonic beam generated from two adjacent curved transducers. Select the placement angle, and 1
Since the ultrasonic probe is equipped with a number of curved transducers that can secure an area where the total ultrasonic beam width of the ultrasonic probe is 120 degrees or more in the circumferential direction of the test specimen, inspection time can be significantly shortened. Become.

〔実施例」 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p、第1図(a)は斜角探触子の正面M面図、第
1図(b)は斜角探触子の横断面図である。
[Embodiment] Fig. 1 is a sectional view of an ultrasonic probe showing an embodiment of the present invention, and Fig. 1(a) is a front M view of an angle probe. b) is a cross-sectional view of the angle probe.

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ック製
の楔、(3)は不要な超音波を吸収する吸音材。
In the figure, (1a) to (1d) are curved transducers having a curvature that allows ultrasonic waves to diffuse; (2) is a plastic wedge having a radius of curvature equivalent to that of the curved transducer; (3) ) is a sound-absorbing material that absorbs unnecessary ultrasonic waves.

(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ュー、イは縦波超音波1口は横波超
音波。
(4) is the probe case, (5) is the specimen such as pipe material, (6
) is the contact medium, (7) is the shoe that maintains the gap between the wedge (2) and the test specimen (5), A is the longitudinal wave ultrasonic wave, and one mouth is the transverse wave ultrasonic wave.

人は曲面振動子(1a)〜(1b)のお互いの配置角度
である。
Person is the angle at which the curved surface vibrators (1a) to (1b) are arranged with respect to each other.

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、二は曲面振動子(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、へは曲面振動子(1d)で形成される超音
波ビーム幅、Hは超音波信号の振幅。
In the figure, C is the ultrasonic beam width formed by the curved transducer (1a), 2 is the ultrasonic beam width formed by the curved transducer (1b), and E is the ultrasonic beam width formed by the curved transducer (1C). The sound wave beam width is the ultrasound beam width formed by the curved surface transducer (1d), and H is the amplitude of the ultrasound signal.

θは試験体(5)の管周方向角度である。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2曲面振動子の寸法
7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 of the bicurved vibrator, the radius of curvature, and the arrangement angle with respect to the outer diameter of the test piece.

図において=  (1a) 、 (1b)は曲面f5i
動子、(2)は楔。
In the figure, = (1a), (1b) is the curved surface f5i
Doko, (2) is a wedge.

(5)は試験体2人は曲面振動子(1a)の配置角度、
Lは曲面振動子(1a)の寸法、I!1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、12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、  IL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11と法線QOとのなす角度、θ5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。
(5) is the arrangement angle of the curved surface vibrator (1a) for the two test subjects;
L is the dimension of the curved surface vibrator (1a), I! 1 is the test specimen (5)
The ultrasonic beam width from the center of the curved transducer (1a) on the surface, 12 is the ultrasonic beam width from the center of the curved transducer (1a) on the inner surface of the specimen (5), and IL is the ultrasonic beam width from the center of the curved transducer (1a) on the inner surface of the specimen (5). The radius of curvature, θ1 is the angle of the ultrasonic wave emitted from the curved transducer (1a), θ2 is the angle between the beam width 11 on the surface of the specimen (5) and the normal QO, and θ5 is the angle of the ultrasonic wave to the specimen (5) The incident angle of ultrasonic waves, θ4 is the test specimen (5)
This is the refraction angle of the ultrasonic wave inside.

ここで2曲面振動子(1a)の寸法りは欠陥検出能の低
下を防止するために20y+i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)との層脱の容易性
から180°以下が望ましく、かっ360°を整数で割
シ切れる直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, it is desirable that the dimensions of the two-curved vibrator (1a) be 20y+i or less in order to prevent a decrease in defect detection ability. In addition, the ultrasonic coverage range of one block of the ultrasonic probe is desirably 180° or less in order to facilitate delamination between the ultrasonic probe and the test specimen (5), which is calculated by dividing 360° by an integer. In terms of data processing, it is desirable that the angle is straight, and in most cases 120° is a standard.

さらに1曲面撮動子(1a)の曲率半径孔は楔(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1/4〜1A程度になるようにすることに
よシ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 hole of the one-curved camera element (1a) has a difference between the minimum value and the maximum value of the distance that the ultrasonic wave propagates within the wedge (2).
By setting the wavelength within ) to about 1/4 to 1 A, it is possible to prevent the ultrasonic waves from rapidly diffusing and reducing the defect detection ability.

上記前提条件のもとで1曲面振動子(1a)の寸法り2
曲面振動子(1a)の曲率半径孔2曲面振動子(1a)
の配置角要人は以下の関係によ)求めることができる。
Under the above preconditions, the dimensions of one curved surface vibrator (1a) are 2
Curvature radius of curved surface vibrator (1a) 2 curved surface vibrator (1a)
The placement angle of key figures can be found by the following relationship.

w = t/■θ8       ・・・・・・・・・
・・・・・・(11/1 ”dnθ1×(R+Δl) 
   ・・・・・・・・・・・・・・・(2)−j  
/j         ・・・・・・・・・・・・・・
・(3)θr噛(1) θ5=o1+o2        ・・・・・・・・・
・・・・・・(4)!!2 # 11 + to (θ
4−02)×W ・・・・・・・・・・・・・・・(6
)−11!2 人= 2 X * (−)    ・・・・・・・・・
・・・・・・(7)D/2−t n≧ヱ       ・・・・・・・・・・・・・・・
(8)人 但し、仮定条件として λ    L2 λ −<R2−(−)<−   ・・・・・・・・・・・・
・・・(9)なお(1)〜(9)式において t:試験体の厚さ Δl!:楔の長さ vl:楔の縦波音速 v2:試験体の横波音速 n:曲面振動子の数 ψ:探触子1ブロック当た)のカバー範囲θ11:試験
体中の横波屈折角 り2試験体の外径寸法 W:試験体中の0.5スキップ距離 λ:楔中の波長 を表わす。
w = t/■θ8 ・・・・・・・・・
・・・・・・(11/1”dnθ1×(R+Δl)
・・・・・・・・・・・・・・・(2)-j
/j ・・・・・・・・・・・・・・・
・(3) θr bite (1) θ5=o1+o2 ・・・・・・・・・
・・・・・・(4)! ! 2 #11 + to (θ
4-02)×W ・・・・・・・・・・・・・・・(6
)-11!2 people = 2 X * (-) ・・・・・・・・・
・・・・・・(7) D/2-t n≧ヱ ・・・・・・・・・・・・・・・
(8) Person However, as an assumption condition, λ L2 λ −<R2−(−)<− ・・・・・・・・・・・・・・・
...(9) In equations (1) to (9), t: thickness Δl of the test piece! : Wedge length vl: Longitudinal wave sound velocity in the wedge v2: Transverse wave sound speed in the test piece n: Number of curved surface oscillators ψ: Coverage range (per probe 1 block) θ11: Shear wave refraction angle in the test piece 2 Outer diameter dimension W of the test piece: 0.5 skip distance λ in the test piece: Represents the wavelength in the wedge.

この一実施例では試験体(5)の外径60.5朋の時に
曲面振動子(1a)〜(1d)の寸法りを18m舅とし
、上記曲面振動子(1a)〜(1d)の曲率半径孔を1
50窯とし、配置角要人を30″に選択することにより
、4個の曲面撮動子(1a)〜(1d)で試験体(5)
の管周約120°にわたっ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 specimen (5) is 60.5 mm, the dimensions of the curved surface vibrators (1a) to (1d) are set to 18 m, and the curvature of the curved surface vibrators (1a) to (1d) is Radius hole 1
By selecting the 50" kiln and the arrangement angle of 30", the test specimen (5) was created using four curved surface sensors (1a) to (1d).
This made it possible to transmit and receive ultrasonic waves over approximately 120 degrees of tube circumference.

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)〜(1
d)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シ試験体(5)
の外径曲率に対応して管周方向に横波超音波口としてさ
らに拡散伝播することになる。
That is, in the ultrasonic probe configured as described above, curved transducers (1a) to (1) that transmit and receive ultrasonic waves are used.
The longitudinal ultrasonic wave A generated from d) propagates while diffusing inside the wedge (2), and further passes through the test specimen (5) according to Snell's law.
According to the outer diameter curvature of the transverse wave, the ultrasonic wave is further diffused and propagated in the tube circumferential direction as a transverse wave aperture.

従って、試験体(5)の外径寸法に応じて2曲面振動子
(1a)〜(1d)の寸法りと、上記曲面振動子(1a
)〜(1d)の曲率半径孔と、上記曲面振動子(1a)
〜(1d)の配置角要人を(7)〜(9)式により決定
することにより、よシ少ない曲面振動子(1a)〜(1
d)の数で、試験体(5)の管周方向の広範囲にわたっ
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。
Therefore, the dimensions of the two curved surface vibrators (1a) to (1d) and the curved surface vibrator (1a) are determined according to the outer diameter dimension of the test specimen (5).
) to (1d) and the curved surface vibrator (1a).
By determining the key placement angles of ~(1d) using equations (7)~(9), fewer curved surface oscillators (1a)~(1) can be obtained.
With the number d), it becomes possible to transmit and receive ultrasonic waves over a wide range in the circumferential direction of the test specimen (5). Also, of course.

お互いの曲面振動子(1a)〜(1d)間の超音波ビー
ム幅ヒ→〜に)は−3dB以内の振幅で完全にオーバラ
ップさせることも容易に可能となる。
It is also easily possible to completely overlap the ultrasonic beam widths between the curved surface transducers (1a) to (1d) with amplitudes within -3 dB.

また、プラスチック製の楔(2)の曲面振動子(1a)
〜(1d)が当接される面には、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
In addition, a curved vibrator (1a) made of a plastic wedge (2)
The curved surface vibrator (1a)
) to (1d), and has a radius of curvature equivalent to that of (1d).

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
表面との間にはシュー(7)を用いることによシ所定の
すき間を設け、上記すき間に接触媒体を供給することに
よシ音響結合不良を防止するようにしである。
The surface facing the test body (5) has a radius of curvature equal to the outer diameter of the test body (5) plus a predetermined gap. In other words, when considering the outer diameter tolerance, roundness, etc. of the test piece (5), the contact area between the wedge (2) and the test piece (5) becomes large. A shoe (7) is used to provide a predetermined gap between the housing and the outer surface of the housing (5), 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止に所定の角度
で複数個配置することによシ、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, the present invention is capable of transmitting energy in the circumferential direction of the test specimen by arranging a plurality of ultrasonic diffusion type curved surface transducers at a predetermined angle on the wedges corresponding to the circumferential direction of the test specimen. Since the inspection range can be widened, the inspection time can be significantly shortened.

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

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。 M2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2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(−)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)〜(1
d)は曲面振動子、(2)は侯、(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2
口は横波超音波、(ハ)〜に)は超音波ビーム1−2人
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 the ultrasonic probe according to the present invention.
FIG. 1(a) is a front cross-sectional view, and FIG. 1(b) is a cross-sectional view. Figure M2 is a diagram showing the ultrasonic beam width of the ultrasound probe according to the present invention, Figure 3 is a diagram showing the correlation between the dimensions of the curved transducer, the radius of curvature, and the arrangement angle, and Figure 4 is a diagram showing the relationship between the dimensions of the curved transducer, the radius of curvature, and the arrangement angle. 4(-) is a front sectional view, and FIG. 4<b) is a cross-sectional view of the feeler. In the figure, (1) is a flat plate vibrator, (1a) to (1
d) is a curved vibrator, (2) is a sound absorber, (3) is a sound absorbing material, (4
) is the probe case, (5) is the specimen, A is the longitudinal ultrasound 2
The opening is the transverse wave ultrasound, and (c) ~ 2) is the ultrasonic beam 1-2 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] 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ック製の楔とを具備したことを
特徴とする超音波探触子。
An angle probe that transmits and receives ultrasonic waves in the axial direction of a tube material includes: 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 transducer and the tube material. The surface on which the curved surface vibrator comes into contact 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 has a radius of curvature equal to the outer diameter of the tube material. An ultrasonic probe comprising a plastic wedge having a corresponding curvature.
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 true JPS6338157A (en) 1988-02-18
JPH0521502B2 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 (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0257973A (en) * 1988-08-23 1990-02-27 Kawasaki Steel Corp Angle beam flaw detecting head for pipe and angle beam flaw detecting apparatus using said head
JP2013124891A (en) * 2011-12-14 2013-06-24 Mitsubishi Heavy Ind Ltd Ultrasonic flaw inspection device
JP2021501320A (en) * 2017-10-27 2021-01-14 ウエスチングハウス・エレクトリック・カンパニー・エルエルシー Improved corrosion thinning detectors and methods

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6815360B2 (en) * 2018-10-03 2021-01-20 三菱パワー株式会社 Ultrasonic inspection equipment and ultrasonic inspection method

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0257973A (en) * 1988-08-23 1990-02-27 Kawasaki Steel Corp Angle beam flaw detecting head for pipe and angle beam flaw detecting apparatus using said head
JP2013124891A (en) * 2011-12-14 2013-06-24 Mitsubishi Heavy Ind Ltd Ultrasonic flaw inspection device
JP2021501320A (en) * 2017-10-27 2021-01-14 ウエスチングハウス・エレクトリック・カンパニー・エルエルシー Improved corrosion thinning detectors and methods

Also Published As

Publication number Publication date
JPH0521502B2 (en) 1993-03-24

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