JPS6048701B2 - Surface wave method ultrasonic flaw detection probe - Google Patents
Surface wave method ultrasonic flaw detection probeInfo
- Publication number
- JPS6048701B2 JPS6048701B2 JP674377A JP674377A JPS6048701B2 JP S6048701 B2 JPS6048701 B2 JP S6048701B2 JP 674377 A JP674377 A JP 674377A JP 674377 A JP674377 A JP 674377A JP S6048701 B2 JPS6048701 B2 JP S6048701B2
- Authority
- JP
- Japan
- Prior art keywords
- probe
- surface wave
- flaw detection
- vibrator
- ultrasonic flaw
- 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
Links
Landscapes
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
Description
【発明の詳細な説明】
本発明は、表面波法超音波探傷において、被検材側底面
に凹状レンズ部(以下凹部と称する。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a concave lens portion (hereinafter referred to as a concave portion) on the bottom surface of a specimen in surface wave method ultrasonic flaw detection.
)を設け、さらに被検材とこの凹部とが形成する空間に
水を供給しながら探傷を行なう探触子に関する。従来の
形状および機構を有する探触子においては、第1図に示
す如く、探触子から発信された超音波は、近距離音波領
域を通過すると、被検材内の表面波伝播方向に対し固有
の角度をなして広がりながら伝播する。), and further relates to a probe that performs flaw detection while supplying water to the space formed by the test material and the recess. In a probe with a conventional shape and mechanism, as shown in Fig. 1, when the ultrasonic waves emitted from the probe pass through the short-range sound wave region, they change in the direction of surface wave propagation within the test material. It propagates while spreading out at a unique angle.
この広がり角は、超音波の波長および振動子の発信方向
に直交する方向に対する射影長さ寸法によつて定まる。
片側の広がり角を指向角θと称し、これは次式により表
わされる。θ■(7晴)゜・・・・・・(1)
ここでλ:波長、D:振動子の寸法
このように従来の探触子では、発信された表面波の伝播
が進むにつれて広がつていくので、S/Nが悪化し、ま
た被検材疵の評価において疵の被検材中の位置の影響に
よる誤差が生じていた。This spread angle is determined by the wavelength of the ultrasonic wave and the projected length dimension of the transducer in a direction perpendicular to the transmission direction.
The spread angle on one side is called the directivity angle θ, which is expressed by the following equation. θ■ (7 days)゜・・・・・・(1) Here, λ: Wavelength, D: Dimension of the transducer In conventional probes, as the emitted surface waves propagate, they spread. As a result, the S/N deteriorates, and errors occur in the evaluation of defects in the material to be inspected due to the influence of the position of the flaw in the material to be inspected.
本発明の目的は、探触子から発信した超音波を被検材内
でほぼ平行に伝播させS/N比が良好で、評価精度の良
い探傷を行なうことのできる探触子を提供することにあ
る。また、本発明の要旨は、探触子の被検材側底面の一
部あるいは全面に設けられた凹状レンズ部と:探触子内
部に設けられた振動子と;探触子外フ表面から前記凹状
レンズ部に貫通する少なくとも1つ以上の給水孔と;を
備えており、前記探触子の凹状レンズ部と被検材とが形
成する空間に水が供給され、かつ前記振動子からの超音
波が被検材内の表面波伝播方向に対してほぼ平行に伝播
する、表面波法超音波探触子である。An object of the present invention is to provide a probe that allows ultrasonic waves emitted from the probe to propagate almost parallel within a material to be inspected, has a good S/N ratio, and can perform flaw detection with high evaluation accuracy. It is in. In addition, the gist of the present invention is that: a concave lens portion provided on a part or the entire surface of the bottom surface of the probe on the side of the sample to be measured; a vibrator provided inside the probe; at least one water supply hole penetrating the concave lens part; water is supplied to the space formed by the concave lens part of the probe and the test material, and water is supplied from the vibrator. This is a surface wave method ultrasonic probe in which ultrasonic waves propagate approximately parallel to the surface wave propagation direction within the test material.
以下、図面を参照して、本発明の実施例を説明する。Embodiments of the present invention will be described below with reference to the drawings.
第2図は、本発明の実施例を説明する概略斜視図である
。FIG. 2 is a schematic perspective view illustrating an embodiment of the present invention.
図において、1は被検材であり、2はその内部に振動子
3を備えた探触子である。振動子3の幅は、探触子2の
幅と等しいか、あるいはそれより小さくする。振動子3
は、その振動の伝播が探触子2の被検材底面へ向かうよ
うに、探触子内部て傾斜をもたせて配置してある。また
、探触子2は、その被検材側底面に凹部4を有している
。この凹部4は、円弧をなしており、その設計例を第7
図に示す。この円弧の半径をrとすると、これは次式に
より算出される。r=(1−C2/C1)b・・・・・
・(2)ここでC,:入射側音速(m/Sec)C。In the figure, 1 is a material to be tested, and 2 is a probe equipped with a vibrator 3 inside. The width of the vibrator 3 is equal to or smaller than the width of the probe 2. Vibrator 3
are arranged with an inclination inside the probe so that the vibrations propagate toward the bottom surface of the sample to be inspected. Further, the probe 2 has a recess 4 on the bottom surface on the side of the test material. This recess 4 has a circular arc shape, and a design example thereof is shown in the seventh example.
As shown in the figure. If the radius of this circular arc is r, it is calculated by the following equation. r=(1-C2/C1)b...
・(2) Here, C: Speed of sound on the incident side (m/Sec)C.
:被検材中の音速(m/Sec)b:焦点を結ぶ位置(
TWL)
第7図に示した実施例では、探触子部材にエポキシ樹脂
を用い、また被検材は鋼材を対象している。: Speed of sound in the material being tested (m/Sec) b: Focusing position (
TWL) In the embodiment shown in FIG. 7, epoxy resin is used for the probe member, and the material to be tested is steel.
そして焦点距離を700wrmと設定する。したがつて
、(2)式において、C1=2700m/SeCNc2
=リ2980rT1/SecNb=70077z771
を代人して、r =ー66閾と求められる。こうして本
実施例では、探触子底面に半径66m77Zの凹部を設
ければ良いことが分かる。探触子の幅が40Tr$Lの
場合には、凹部の高さは約3.5wLに、50Trrm
の場合には約5.577!771になる。な二お、振動
子の幅が探触子の幅より小さい楊合には、探触子の幅全
体に対応して探触子底面に凹部を設けても良ιル、振動
子の幅に対応する長さにわたつて凹部を設け、探触子の
両端部を平坦状に形成しても良い。3
第3図ないし第6図は、本発明の探触子の実施例を示す
図である。Then, the focal length is set to 700wrm. Therefore, in equation (2), C1=2700m/SeCNc2
=Re2980rT1/SecNb=70077z771
As a proxy, r = -66 threshold can be obtained. Thus, it can be seen that in this example, it is sufficient to provide a concave portion with a radius of 66 m77Z on the bottom surface of the probe. When the width of the probe is 40Tr$L, the height of the recess is approximately 3.5wL, and 50Trrm
In the case of , it becomes approximately 5.577!771. In addition, if the width of the transducer is smaller than the width of the probe, it may be possible to provide a recess on the bottom of the probe corresponding to the entire width of the probe. A concave portion may be provided over a corresponding length, and both ends of the probe may be formed flat. 3 FIGS. 3 to 6 are diagrams showing embodiments of the probe of the present invention.
第3図は、給水孔5を探触子2の上面から凹部に貫通す
るように、かつ振動子3の後方に配設した実施例を示し
ている。FIG. 3 shows an embodiment in which the water supply hole 5 is disposed so as to pass through the recess from the top surface of the probe 2 and behind the vibrator 3.
振動子3より発信した超音波は、矢印6の如く伝播する
。第4図は、探触子2の底面に脚部7を設け、前記脚部
の外周面から凹部へ向つて貫通する給水孔5’を備えた
実施例を示している。The ultrasonic waves emitted from the vibrator 3 propagate as indicated by an arrow 6. FIG. 4 shows an embodiment in which a leg portion 7 is provided on the bottom surface of the probe 2, and a water supply hole 5' is provided penetrating from the outer peripheral surface of the leg portion toward the recess.
なお、給水孔5’は、脚部7の片側にのみ配設しても良
い。第5図は、探触子2の前方1,のみに凹部4を設け
、残りの1。部分の底面は平坦状にした場合の実施例例
である。一般には、凹部を底面全体に設けた場合のほう
が、凹部に気泡等が留まらず、エアーパージが容易に行
なえる。第6図は、給水孔5″を探触子2の上面から凹
部4へ貫通し、かつ振動子3’の前方に設けた実施例を
示している。Note that the water supply hole 5' may be provided only on one side of the leg portion 7. In FIG. 5, a recess 4 is provided only in the front 1 of the probe 2, and the remaining 1. This is an example in which the bottom surface of the portion is made flat. Generally, if the recess is provided over the entire bottom surface, air bubbles will not remain in the recess and air purging will be easier. FIG. 6 shows an embodiment in which a water supply hole 5'' passes through the top surface of the probe 2 into the recess 4 and is provided in front of the vibrator 3'.
この場合には、超音波が給水孔5″によつて散乱され、
不感帯が広がるのを防ぐために、振動子3’を2名割し
て配置するようにしている。さて、本発明の探触子によ
れば前述の如く、S/N比が良好になる。In this case, the ultrasonic waves are scattered by the water supply hole 5'',
In order to prevent the dead zone from widening, the vibrator 3' is divided into two people and arranged. Now, according to the probe of the present invention, as described above, the S/N ratio is good.
本発明者の実験では、従来の探触子と比べて、使用周波
数帯域1〜2MHzにおいて少なくとも4〜■旧の向上
が見られた。In experiments conducted by the present inventors, an improvement of at least 4 to 2 times was observed in the operating frequency band of 1 to 2 MHz compared to conventional probes.
第1図は従来の探触子による表面波の伝播状況を説明す
る概略斜視図、第2図は本発明の実施例探触子による表
面波の伝播状況を説明する概略斜視図、第3図ないし第
6図は、本発明の実施例を説明する概略図、第7図は本
発明の探触子凹状レンズ部の設計例を示す概略図である
。
1 ・・・・・・被検材、2・・・・・・探触子、3,
3’・・・・・・振動子、4 ・・・・・・凹状レンズ
部(凹部)、5,5’,5″・・・・・・給水孔、6
・・・・・・超音波伝播方向、7 ・・・・・・脚部、
D・・・・・・振動子の幅、θ・・・・・・指向角。Fig. 1 is a schematic perspective view illustrating the propagation situation of surface waves by a conventional probe, Fig. 2 is a schematic perspective view illustrating the propagation situation of surface waves by the embodiment probe of the present invention, and Fig. 3 6 to 6 are schematic diagrams illustrating embodiments of the present invention, and FIG. 7 is a schematic diagram illustrating a design example of a probe concave lens portion of the present invention. 1...Test material, 2...Probe, 3,
3'... Vibrator, 4... Concave lens portion (concave portion), 5, 5', 5''... Water supply hole, 6
・・・・・・Ultrasonic propagation direction, 7 ・・・・・・Legs,
D...Width of the vibrator, θ...Directivity angle.
Claims (1)
れた凹状レンズ部と;探触子内部に設けられた振動子と
; 探触子外表面から前記凹状レンズ部に貫通する少なくと
も1つ以上の給水孔と;を備えており、前記探触子の凹
状レンズ部と被検材とが形成する空間に水が供給され、
かつ前記振動子からの超音波が、被検材内の表面波伝播
方向に対してほぼ平行に伝播することを特徴とする表面
波法超音波探傷用探触子。[Scope of Claims] 1. A concave lens portion provided on a part or the entire surface of the bottom surface of the probe on the side of the specimen; a vibrator provided inside the probe; at least one water supply hole penetrating the lens portion; water is supplied to the space formed by the concave lens portion of the probe and the test material;
A surface wave method ultrasonic flaw detection probe characterized in that the ultrasonic waves from the vibrator propagate substantially parallel to the surface wave propagation direction within the test material.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP674377A JPS6048701B2 (en) | 1977-01-26 | 1977-01-26 | Surface wave method ultrasonic flaw detection probe |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP674377A JPS6048701B2 (en) | 1977-01-26 | 1977-01-26 | Surface wave method ultrasonic flaw detection probe |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5393084A JPS5393084A (en) | 1978-08-15 |
| JPS6048701B2 true JPS6048701B2 (en) | 1985-10-29 |
Family
ID=11646679
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP674377A Expired JPS6048701B2 (en) | 1977-01-26 | 1977-01-26 | Surface wave method ultrasonic flaw detection probe |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6048701B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6098356A (en) * | 1983-11-02 | 1985-06-01 | Olympus Optical Co Ltd | Water injecting device of acoustic lens for ultrasonic microscope |
| JP2012093246A (en) * | 2010-10-27 | 2012-05-17 | Jfe Steel Corp | Ultrasonic probe and method for detecting defect |
| JP5609540B2 (en) * | 2010-10-27 | 2014-10-22 | Jfeスチール株式会社 | Defect detection method and defect detection apparatus using leaky surface acoustic wave |
-
1977
- 1977-01-26 JP JP674377A patent/JPS6048701B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5393084A (en) | 1978-08-15 |
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