JPS63256847A - Ultrasonic contactor - Google Patents
Ultrasonic contactorInfo
- Publication number
- JPS63256847A JPS63256847A JP9125587A JP9125587A JPS63256847A JP S63256847 A JPS63256847 A JP S63256847A JP 9125587 A JP9125587 A JP 9125587A JP 9125587 A JP9125587 A JP 9125587A JP S63256847 A JPS63256847 A JP S63256847A
- Authority
- JP
- Japan
- Prior art keywords
- sound pressure
- ultrasonic
- wedge
- pressure intensity
- ultrasonic 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
Links
Landscapes
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、棒材、線材等の表皮下に存在する欠陥、介
在物等を超音波斜角探傷によシ検出する超音波探触子に
関するものである。[Detailed Description of the Invention] [Field of Industrial Application] The present invention provides an ultrasonic probe for detecting defects, inclusions, etc. existing under the skin of bars, wires, etc. using ultrasonic angle flaw detection. It is related to.
第2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装置す図である
。FIG. 2 is a diagram of a conventional ultrasonic probe device shown in, for example, Ultrasonic Flaw Detection Method (published by Nikkan Kogyo Shimbun in 1972).
第2(8)(a)は超音波探触子の断面図、第2図(b
)は従来の超音波探触子による探傷波形図である。2(8)(a) is a cross-sectional view of the ultrasonic probe, FIG. 2(b)
) is a flaw detection waveform chart using a conventional ultrasonic probe.
図において(1)は超音波探触子、(2)は超音波全送
受する振動子、(3)はプラスチック製の楔、(4)は
水。In the figure, (1) is an ultrasonic probe, (2) is a transducer that transmits and receives all ultrasonic waves, (3) is a plastic wedge, and (4) is water.
油等から成る音響結合材、(5)は音圧強度の強いメイ
ンロープ、 +61H音圧強度の弱いメインロープ。Acoustic coupling material made of oil etc. (5) is main rope with strong sound pressure strength, +61H main rope with weak sound pressure strength.
(7)は被検材、αは被検材(7)に対する超音波の入
射角度、Cは被検材(7)の中心、(8)は探傷ゲート
、Bは音圧強度の弱いメインロープ(6)による底面エ
コー、GVi超音波探触子(1)と被検材(7)とのギ
ャップ。(7) is the material to be tested, α is the incident angle of the ultrasonic wave to the material to be tested (7), C is the center of the material to be tested (7), (8) is the flaw detection gate, and B is the main rope with weak sound pressure intensity. Bottom echo according to (6), gap between GVi ultrasonic probe (1) and test material (7).
Tは送信パルスである。T is the transmit pulse.
従来の超音波探触子装置は上記のように構成されており
、被検材(7)の表皮下部分をできるだけ未探1易領域
部分を少なくして探傷検査を行うために。The conventional ultrasonic probe device is configured as described above, in order to perform flaw detection in the subepidermal area of the material to be inspected (7) while minimizing the unexplored area.
斜角探傷法が使用されるのが一般的である。斜角探傷法
は、被検材(7)の中心c1通る法線に対して所定の角
度αで超音波を入射させると、スネルの法則により入射
角度αに対応した屈折角が与えられるものである。The angle angle flaw detection method is generally used. In the angle angle flaw detection method, when an ultrasonic wave is incident at a predetermined angle α to the normal line passing through the center c1 of the test material (7), a refraction angle corresponding to the incident angle α is given according to Snell's law. be.
振動子(2)から放射される超音波ビームには音圧強度
の強いメインローブ(5)と音圧強度の弱いメインロー
ブ(6)が存在する。The ultrasonic beam emitted from the transducer (2) has a main lobe (5) with a strong sound pressure intensity and a main lobe (6) with a weak sound pressure intensity.
特に、被検材(7)が九捧材の場合には、振動子(2)
の端部から発生する音圧強度の弱いメインローブ(6)
が、被検材(7)に入射する点は被検材(7)の中心か
らずれるために、特に音圧強度の最大点より後方では超
音波の入射角度が著しく小さくなり、縦波超音波として
被検材(7)の中心C付近を伝播することがめる。In particular, when the material to be inspected (7) is a nine-piece material, the vibrator (2)
Main lobe (6) with weak sound pressure intensity generated from the end of
However, since the point of incidence on the material to be tested (7) is shifted from the center of the material to be tested (7), the angle of incidence of the ultrasonic wave becomes significantly smaller, especially behind the point of maximum sound pressure intensity, and the longitudinal wave ultrasound It can be seen that the signal propagates near the center C of the test material (7).
上記条件は被検材(7)の外形寸法が小さいほど顕著と
なる。The above conditions become more pronounced as the outer dimensions of the test material (7) become smaller.
上記に示すように音圧強度の弱いメインローブ(6)成
分が被検材(7)の中心Cに向ってほぼ垂直に入射する
と、縦波超音波として被検材(7)中を伝播することに
なる。一方、音圧強度の強いメインローブ(5)は被検
材(7)中を横波で伝播するように入射角度αが設定さ
れている超音波探触子では、送信・(ルスT以降の時間
は全て被検材(7)の横波音速で超音波の伝播時間が設
定、あるいは計算されているため、音圧強度の弱いメイ
ンローブ(6)成分による縦波超音波が底面エコーBと
して、音圧強度の強いメインローブ(51の横波超音波
が被検材(7)の側面に1パウンドする時間より若干短
い時間で発生するため、常にノイズ成分として探傷ゲー
ト(8)に読み込まれ、 S/N比を悪化させる問題が
あった。As shown above, when the main lobe (6) component with low sound pressure intensity is incident almost perpendicularly toward the center C of the test material (7), it propagates through the test material (7) as a longitudinal ultrasonic wave. It turns out. On the other hand, in an ultrasonic probe in which the incident angle α is set so that the main lobe (5) with strong sound pressure intensity propagates through the test material (7) as a transverse wave, The propagation time of the ultrasonic wave is set or calculated based on the transverse sound velocity of the test material (7), so the longitudinal ultrasonic wave due to the main lobe (6) component with weak sound pressure intensity becomes the bottom echo B and the sound Because the main lobe (51) with strong compressive strength is generated in a slightly shorter time than the time it takes for one pound of transverse ultrasonic waves to hit the side of the material to be inspected (7), it is always read into the flaw detection gate (8) as a noise component, and the S/ There was a problem of deteriorating the N ratio.
この発明は上記問題点全解決するためになされたもので
、音圧強度の弱いメインローブを被検材中に入射させな
いでS/N比の良い超音波探触子装置を得ることを目的
とする。This invention was made to solve all of the above problems, and its purpose is to obtain an ultrasonic probe device with a good S/N ratio without allowing the main lobe, which has a weak sound pressure intensity, to enter the test material. do.
この発明による超音波探触子は、楔の音響結合体と接す
る面上において、音圧強度が最大となる点より後方面で
、音圧強度の最大点より一10dB以下の音圧の全面に
わたり、超音波の反射体を具備させたものである。The ultrasonic probe according to the present invention has a sound pressure of 10 dB or less from the maximum point of the sound pressure intensity over the entire surface on the surface of the wedge in contact with the acoustic coupler, on the rear side of the point where the sound pressure intensity is maximum. , which is equipped with an ultrasonic reflector.
この発明においては、楔の音響結合体と接する面上にお
いて、音圧強度が最大となる点より後方面で、音圧強度
の最大点より一10dB以下の音圧の全面にわたり超音
波の反射体を具備させているため、振動子の端部から発
生する音圧強度の弱いメインローブは被検材には入射し
なくなる。したがって、探傷波形図においても、探傷ゲ
ート中に縦波超音波によるノイズ成分は発生しない超音
波探触子となり得る。In this invention, on the surface of the wedge in contact with the acoustic coupler, on the rear surface from the point where the sound pressure intensity is maximum, an ultrasonic reflector is provided over the entire surface of the sound pressure of 10 dB or less from the maximum point of the sound pressure intensity. , the main lobe of low sound pressure intensity generated from the end of the vibrator does not enter the specimen. Therefore, even in the flaw detection waveform diagram, it is possible to obtain an ultrasonic probe in which no noise component due to longitudinal ultrasonic waves is generated during the flaw detection gate.
第1図はこの発明の一実施例を示す超音波探触子を示す
図である。FIG. 1 is a diagram showing an ultrasonic probe showing an embodiment of the present invention.
第1図(a)は超音波探触子の断面図、第1図(b)は
この発明の超音波探触子による探傷波形図である。FIG. 1(a) is a cross-sectional view of an ultrasonic probe, and FIG. 1(b) is a flaw detection waveform diagram by the ultrasonic probe of the present invention.
図においてfil Vi超音波探触子、(2)は振動子
、(3)は楔、(4)は音響結合材、(5)は音圧強度
の強いメインローブ、 f61H音圧強度の弱いメイン
ローブ、(7)は被検材、(8)は探傷ゲー1−.(9
1はこの発明によるコルク材等から成る反射体、αは被
検材(7)への超音波入射角度、Cは被検材(7)の中
心、Tは送信パルス、Gは超音波探触子(1)と被検材
(7)とのギャップである。In the figure, fil Vi ultrasonic probe, (2) is the transducer, (3) is the wedge, (4) is the acoustic coupling material, (5) is the main lobe with strong sound pressure intensity, and f61H is the main lobe with weak sound pressure intensity. Lobe, (7) is the material to be tested, (8) is the flaw detection game 1-. (9
1 is a reflector made of cork material or the like according to the present invention, α is the angle of incidence of ultrasonic waves on the test material (7), C is the center of the test material (7), T is the transmission pulse, and G is the ultrasonic probe. This is the gap between the child (1) and the material to be tested (7).
上記のように構成された超音波探触子においては、振動
子(2)から放射された超音波の音圧強度の強いメイン
ローブ(5)、および音圧強度の弱いメインローブ(6
)は楔(3)中を伝播し、音圧強度の強いメインローブ
(5)は被検材(7)の表面へと伝播される。In the ultrasonic probe configured as described above, the ultrasonic waves emitted from the transducer (2) have a main lobe (5) with a strong sound pressure intensity, and a main lobe (6) with a weak sound pressure intensity.
) is propagated through the wedge (3), and the main lobe (5) with high sound pressure intensity is propagated to the surface of the test material (7).
一方、音圧強度の弱いメインローブ(6)は楔(3)に
設けられた反射体(9)に到達し、検(3)内に反射さ
れる。On the other hand, the main lobe (6) with low sound pressure intensity reaches the reflector (9) provided on the wedge (3) and is reflected into the detector (3).
又、被検材(7)の表面へ伝播した音圧強度の強いメイ
ンローブ(5)は被検材(7)の中に所定の角度で入射
し、横波超音波として伝播するだけでめるため被検材(
7)の中心6Cに向って伝播する縦波超音波は存在しな
くなる。その結果、探傷波形図においても、送信パルス
T以降の探傷ゲート(8)内には縦波超音波によるノイ
ズエコーは発生しないことになる。In addition, the main lobe (5) with strong sound pressure intensity propagated to the surface of the test material (7) enters the test material (7) at a predetermined angle and can be determined simply by propagating as a transverse ultrasonic wave. Therefore, the material to be tested (
7) The longitudinal ultrasonic wave propagating toward the center 6C no longer exists. As a result, in the flaw detection waveform diagram, no noise echoes due to longitudinal ultrasonic waves are generated within the flaw detection gate (8) after the transmission pulse T.
ここで反射体(9)全具備させる範囲を音圧強度の最大
点から一10dB以下の全範囲としているのは。The reason why the reflector (9) is provided in its entirety is the entire range of 10 dB or less from the maximum point of sound pressure intensity.
−6〜−8dB程度の範囲では被検材(7)中を伝播す
る横波超音波の強度が弱くなる欠点を有しているからで
ある。又、−10dBより近い範囲では9反射体(9)
の効果があまり現われないために両者のバランスを考慮
して一10dBより低い音圧の全範囲としている。This is because a range of about -6 to -8 dB has the disadvantage that the intensity of transverse ultrasonic waves propagating through the test material (7) becomes weak. Also, in the range closer than -10dB, 9 reflectors (9)
Since this effect does not appear much, the entire sound pressure range is set to be lower than -10 dB in consideration of the balance between the two.
この発明は以上説明したように、外形形状が円筒状の被
検材において、上記被検材の円周方向に斜めに超音波を
入射させる超音波探触子において。As explained above, the present invention is directed to an ultrasonic probe for a test material having a cylindrical external shape, in which ultrasonic waves are incident obliquely in the circumferential direction of the test material.
楔の音響結合体と接する面上において、音圧強度が最大
となる点より後方面で、音圧強度が最大となる点より一
10dB以下の音圧の全面にわたり、超音波の反射体を
具備させたことにより、音圧強度の弱いメインロープが
被検材の中心部分に向って垂直に入射することを防止す
る事が可能となる。On the surface of the wedge in contact with the acoustic coupler, an ultrasonic reflector is provided on the rear surface of the point where the sound pressure intensity is maximum, covering the entire surface with a sound pressure of 10 dB or less from the point where the sound pressure intensity is maximum. By doing so, it is possible to prevent the main rope, which has a weak sound pressure strength, from entering perpendicularly toward the center of the test material.
その結果、被検相中で縦波超音波が発生しないため、送
信パルス以降の探傷ゲート内にノイズ成分となるエコー
は発生せず、 S/N比の良い超音波探触子を供給でき
る効果がある。As a result, no longitudinal ultrasonic waves are generated in the test phase, so no echoes that become noise components are generated within the flaw detection gate after the transmitted pulse, making it possible to supply an ultrasonic probe with a good S/N ratio. There is.
第1図(a)ijこの発明による超音波探触子の断面図
、第1図(b)viこの発明による超音波探触子による
探陽波形図、第2図(a)は従来の超音波探触子の断面
図、第2図(b)は従来の超音波探触子による探傷波形
図である。
図において+11は超音波探触子、(2)は撮動子、(
3)は]始(4)は音響結合材、(5)は音圧強度の強
いメインロープ、(6)は音圧強度の弱いサイドロープ
、(7)は被検材、(9)は反射体である。
尚、各図中同一符号(1同−又は相当部分を示している
。Figure 1 (a) ij is a sectional view of the ultrasonic probe according to the present invention, Figure 1 (b) vi is a detection waveform diagram of the ultrasonic probe according to the present invention, and Figure 2 (a) is a cross-sectional view of the ultrasonic probe according to the present invention. The cross-sectional view of the sonic probe, FIG. 2(b), is a flaw detection waveform diagram by a conventional ultrasonic probe. In the figure, +11 is an ultrasound probe, (2) is an imager, (
3) is] the beginning (4) is the acoustic coupling material, (5) is the main rope with strong sound pressure strength, (6) is the side rope with low sound pressure strength, (7) is the test material, and (9) is the reflective material. It is the body. In addition, the same reference numerals (1 and - or equivalent parts are shown in each figure).
Claims (1)
斜めに超音波を入射させ、かつ、上記被検材と超音波探
触子との間のギャップが2〜3mm以下で使用される超
音波探触子において、振動子の被検材と対向する面に、
アクリル樹脂等のプラスチック製楔を有し、上記楔の音
響結合体が接する面上において、音圧強度が最大となる
点より後方面で音圧強度の最大点より−10dB以下の
音圧の全面にわたり超音波の反射体を具備させた事を特
徴とする超音波探触子。The outer shape of the test material is cylindrical, the ultrasonic wave is incident obliquely in the circumferential direction of the test material, and the gap between the test material and the ultrasonic probe is 2 to 3 mm or less. In ultrasonic probes used in
It has a wedge made of plastic such as acrylic resin, and on the surface of the wedge in contact with the acoustic coupler, the entire surface of the sound pressure is -10 dB or less from the point of maximum sound pressure intensity on the rear side from the point of maximum sound pressure intensity. An ultrasonic probe characterized by being equipped with an ultrasonic reflector.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62091255A JP2630393B2 (en) | 1987-04-14 | 1987-04-14 | Ultrasonic flaw detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62091255A JP2630393B2 (en) | 1987-04-14 | 1987-04-14 | Ultrasonic flaw detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63256847A true JPS63256847A (en) | 1988-10-24 |
| JP2630393B2 JP2630393B2 (en) | 1997-07-16 |
Family
ID=14021317
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62091255A Expired - Lifetime JP2630393B2 (en) | 1987-04-14 | 1987-04-14 | Ultrasonic flaw detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2630393B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5094108A (en) * | 1990-09-28 | 1992-03-10 | Korea Standards Research Institute | Ultrasonic contact transducer for point-focussing surface waves |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3457191B2 (en) | 1998-11-06 | 2003-10-14 | 三菱電機株式会社 | Ultrasonic flaw detector and ultrasonic flaw detection method |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56116664U (en) * | 1980-02-06 | 1981-09-07 | ||
| JPS5794800A (en) * | 1980-12-05 | 1982-06-12 | Nippon Denso Co | Sound horn |
| JPS598153U (en) * | 1982-07-09 | 1984-01-19 | 三菱電機株式会社 | ultrasonic probe |
| JPS6075047A (en) * | 1983-09-30 | 1985-04-27 | 株式会社島津製作所 | Probe for ultrasonic diagnosis |
-
1987
- 1987-04-14 JP JP62091255A patent/JP2630393B2/en not_active Expired - Lifetime
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56116664U (en) * | 1980-02-06 | 1981-09-07 | ||
| JPS5794800A (en) * | 1980-12-05 | 1982-06-12 | Nippon Denso Co | Sound horn |
| JPS598153U (en) * | 1982-07-09 | 1984-01-19 | 三菱電機株式会社 | ultrasonic probe |
| JPS6075047A (en) * | 1983-09-30 | 1985-04-27 | 株式会社島津製作所 | Probe for ultrasonic diagnosis |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5094108A (en) * | 1990-09-28 | 1992-03-10 | Korea Standards Research Institute | Ultrasonic contact transducer for point-focussing surface waves |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2630393B2 (en) | 1997-07-16 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |