JP3121430B2 - Ultrasonic flaw detection method and ultrasonic probe - Google Patents

Ultrasonic flaw detection method and ultrasonic probe

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Publication number
JP3121430B2
JP3121430B2 JP04099914A JP9991492A JP3121430B2 JP 3121430 B2 JP3121430 B2 JP 3121430B2 JP 04099914 A JP04099914 A JP 04099914A JP 9991492 A JP9991492 A JP 9991492A JP 3121430 B2 JP3121430 B2 JP 3121430B2
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JP
Japan
Prior art keywords
medium
ultrasonic
wave
ultrasonic probe
vibrator
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
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JP04099914A
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Japanese (ja)
Other versions
JPH0643139A (en
Inventor
利彦 阿部
忠宏 野村
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Tokyo Keiki Inc
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Tokyo Keiki Inc
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Publication of JPH0643139A publication Critical patent/JPH0643139A/en
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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、超音波集束ビームを発
生し、被検材内の欠陥検出に用いられる超音波探触子に
関し、特に横波を利用して超音波ビーム集束特性を改良
した超音波探触子に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an ultrasonic probe which generates an ultrasonic focused beam and is used for detecting a defect in a test material, and more particularly to an improved ultrasonic beam focusing characteristic using a transverse wave. It relates to an ultrasonic probe.

【0002】[0002]

【従来の技術】従来、この種の超音波探触子としては、
例えば図4に示すようなものがある。
2. Description of the Related Art Conventionally, as an ultrasonic probe of this kind,
For example, there is one as shown in FIG.

【0003】この超音波探触子においては、超音波集束
ビームを発生するため、振動子41の片面には発生した
超音波を減衰させるダンパー42が、また他方の超音波
放射面には、発生した超音波をビーム成形するため、音
響レンズ43が配設されている。
In this ultrasonic probe, to generate an ultrasonic focused beam, a damper 42 for attenuating the generated ultrasonic wave is provided on one side of a vibrator 41, and a damper 42 is provided on the other ultrasonic wave emitting surface. An acoustic lens 43 is provided for beam forming the ultrasonic waves.

【0004】超音波探触子は発生した超音波を伝達する
音響結合剤である媒質I内へ浸漬して、音響レンズ43
と媒質I(音響結合剤)2を介して、媒質II(被検材)
3へ向けて、超音波の送波を行い、さらに、受波も逆方
向に同じパスを通って行われる。
The ultrasonic probe is immersed in a medium I, which is an acoustic coupling agent for transmitting generated ultrasonic waves, and
And medium I (acoustic coupling agent) 2 and medium II (test material)
The ultrasonic wave is transmitted toward 3, and the reception is also performed in the opposite direction through the same path.

【0005】振動子41からの超音波は縦波であり、音
響レンズ43を介して媒質I2から媒質II3へ入射する
とき超音波は屈折して、被検材内にて縦波超音波による
集束ビームを形成して焦点位置に集束される。
[0005] The ultrasonic wave from the transducer 41 is a longitudinal wave. When the ultrasonic wave enters the medium II3 from the medium I2 via the acoustic lens 43, the ultrasonic wave is refracted and focused by the longitudinal ultrasonic wave in the test material. The beam is formed and focused at the focal position.

【0006】被検材内欠陥などからの反射波は上記集束
ビームを介して振動子にて受波される。
[0006] A reflected wave from a defect in the test material is received by the vibrator through the focused beam.

【0007】[0007]

【発明が解決しようとする課題】このような従来の超音
波探触子にあっては、媒質I2内に浸漬された振動子か
らは、音響レンズを介して被検材の媒質II3へ向け縦波
超音波が放射される。
In such a conventional ultrasonic probe, a vibrator immersed in a medium I2 vertically extends through an acoustic lens toward a medium II3 of a test material. Wave ultrasonic waves are emitted.

【0008】縦波超音波の媒質I2から媒質II3への入
射角は縦波臨界角より小さいので、被検材内には縦波超
音波が発生して両媒質の臨界面において下記のとおり屈
折する。
[0008] Since the incident angle of the longitudinal wave ultrasonic wave from the medium I2 to the medium II3 is smaller than the longitudinal wave critical angle, longitudinal wave ultrasonic waves are generated in the test material and refracted at the critical surface of both media as follows. I do.

【0009】[0009]

【数1】sin θ1/sin θ2=Cw/Ce θ1…入射角、θ2…屈折角、Cw…媒質I2の音速、Ce
…媒質II3の音速である。そして、たとえば、媒質I2
を水、媒質II3をエポキシ樹脂とする。
## EQU1 ## sin θ1 / sin θ2 = Cw / Ce θ1: incident angle, θ2: refraction angle, Cw: sound velocity of medium I2, Ce
... The sound velocity of the medium II3. Then, for example, the medium I2
Is water and the medium II3 is an epoxy resin.

【0010】入射角θ1が変わると両者の音速比により
被検材内では焦点化せず、分散配置となるので、先鋭な
集束ビームが形成できない。従って分解能が低下し、被
検材内の微小欠陥の検出、例えばICパッケージの割れ
や内部におけるチップの剥離などの欠陥の検出が不可能
になる。
If the incident angle .theta.1 changes, a focused beam is not formed in the test material due to the sound velocity ratio between the two, and the beam is dispersed, so that a sharp focused beam cannot be formed. Therefore, the resolution is reduced, and it becomes impossible to detect a minute defect in the test material, for example, a defect such as a crack in an IC package or a peeling of a chip inside.

【0011】先鋭な集束ビームを形成するため超音波の
周波数を高くすると、被検材内での超音波の伝搬損失が
増加して受波信号のレベルが低下し、微小欠陥の検出が
困難になる。
If the frequency of the ultrasonic wave is increased to form a sharp focused beam, the propagation loss of the ultrasonic wave in the test material increases, the level of the received signal decreases, and it becomes difficult to detect minute defects. Become.

【0012】また先鋭ビーム形成のため音響レンズの開
口を大きくすると、縦波超音波の入射角θ1が広い範囲
に亙り変わるので、縦波と同時に横波が発生して両者が
干渉し、安定した動作が得られないという問題点があっ
た。
When the aperture of the acoustic lens is enlarged to form a sharp beam, the incident angle θ1 of the longitudinal ultrasonic wave changes over a wide range, so that a longitudinal wave and a transverse wave are generated at the same time, and the two interfere with each other, resulting in stable operation. There was a problem that was not obtained.

【0013】本発明の目的は、横波超音波を用いて、媒
質Iを介して媒質IIにおいて集束しうる超音波の送波を
行う超音波探傷方法を提供することである。
An object of the present invention is to provide an ultrasonic flaw detection method for transmitting ultrasonic waves that can be focused on a medium II via a medium I by using transverse ultrasonic waves.

【0014】[0014]

【課題を解決するための手段】上記課題を解決するた
め、本発明は、媒質Iを介して媒質IIへ向けて超音波を
送波する超音波探触子を用いた超音波探傷方法におい
て、 互いに平行する2つの平面で中空球を裁断したとき
にできる円環状の1の振動子から放射された超音波を、
縦波臨界角より大きな角度で媒質IIへ斜めに入射させる
こと、 媒質II内部に発生した横波を、屈折後、焦点位置
に焦束させることを特徴とする超音波探傷方法を提供す
る。
Means for Solving the Problems To solve the above problems,
Therefore, the present invention provides a method of transmitting ultrasonic waves through a medium I to a medium II.
Ultrasonic flaw detection method using transmitting ultrasonic probe
And cut a hollow sphere in two planes parallel to each other
The ultrasonic waves radiated from one ring-shaped vibrator
Obliquely incident on medium II at an angle greater than the longitudinal wave critical angle
That, after refraction of the transverse wave generated inside the medium II, the focal position
To provide an ultrasonic flaw detection method characterized by focusing on
You.

【0015】[0015]

【作用】媒質Iを介して媒質IIへ向けて超音波の送波を
行う超音波探触子を用いた超音波探傷方法において、振
動子から放射された超音波を、縦波臨界角より大きな角
度にて媒質IIへ斜めに入射させるため、媒質II内部に横
波が発生する。発生した横波を屈折後、円環状に入射さ
せて焦点位置に集束させるため、超音波は集束されて先
鋭ビームとなり、所定位置に集束度の高い焦点が形成さ
れる。振動子と媒質IIの相対位置を変えると媒質II内の
焦点位置が調整できる。
According to the ultrasonic flaw detection method using an ultrasonic probe for transmitting ultrasonic waves toward the medium II via the medium I, the ultrasonic waves radiated from the vibrator are set to be larger than the longitudinal wave critical angle. Since the light is obliquely incident on the medium II at an angle, a transverse wave is generated inside the medium II. After the generated transverse wave is refracted and then incident in an annular shape and focused at the focal position, the ultrasonic wave is focused and becomes a sharp beam, and a focal point with a high degree of convergence is formed at a predetermined position. By changing the relative position between the oscillator and the medium II, the focal position in the medium II can be adjusted.

【0016】[0016]

【実施例】以下、本発明を図面に基づいて説明する。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below with reference to the drawings.

【0017】図1は、本発明の一実施例を示す図であ
る。図2は図1の上面図である。図5は、本発明の振動
子の一実施例の外観を示す説明図である。まず構成を説
明すると、1は振動子(PZT,チタン酸鉛,メタニオ
ブ酸鉛,PVDF等を材料とする)、2は音響結合剤と
しての媒質I、3は被検材である媒質II、5は焦点を示
している。振動子1は圧電セラミック材よりなり中空球
を互いに平行する2つの面にて裁断して、円環状をなし
ている。振動子1は媒質I2即ち音響結合剤としての例
えば水中に浸漬され、円環状をなす球面から所定の入射
角即ち縦波臨界角より大きな入射角にて、披検材として
の媒質II3へ超音波を放射し、媒質II3内の所定位置に
集束ビームの焦点が形成されるように、媒質II3に対し
て配置される。図5に示すように、振動子1から出る音
の伝搬路に関して、それぞれの、焦点までの伝搬時間が
同じになるように振動子1の曲率を設定している。
FIG. 1 is a diagram showing an embodiment of the present invention. FIG. 2 is a top view of FIG. FIG. 5 is an explanatory diagram showing the appearance of one embodiment of the vibrator of the present invention. First, the configuration will be described. 1 is a vibrator (made of PZT, lead titanate, lead metaniobate, PVDF, etc.), 2 is a medium I as an acoustic coupling agent, 3 is a medium II as a test material, 5 Indicates a focus. The vibrator 1 is made of a piezoelectric ceramic material and cuts a hollow sphere at two surfaces parallel to each other to form an annular shape. The vibrator 1 is immersed in a medium I2, that is, for example, water as an acoustic coupling agent, and is ultrasonically transmitted from a circular spherical surface to a medium II3 as a test material at a predetermined incident angle, that is, an incident angle larger than the longitudinal wave critical angle. And is disposed with respect to the medium II3 such that a focus of the focused beam is formed at a predetermined position in the medium II3. As shown in FIG. 5, the curvature of the vibrator 1 is set so that the propagation times of the sound emitted from the vibrator 1 to the focal point are the same.

【0018】次に、上記の実施例の作用を説明する。図
3は斜め入射による縦波と横波の強度分布図であり、水
浸法により水中の振動子1から媒質II3へ入射角を変え
て縦波を放射したときの、媒質II3内に発生する縦波と
横波の往復通過率をそれぞれTD ,TS として、示した
ものである。往復通過率をTiとすると、
Next, the operation of the above embodiment will be described. FIG. 3 is an intensity distribution diagram of longitudinal waves and transverse waves due to oblique incidence. A longitudinal wave generated in the medium II3 when a longitudinal wave is radiated from the vibrator 1 in the water to the medium II3 by changing the incident angle by the water immersion method. The reciprocal passage rates of the wave and the shear wave are shown as T D and T S , respectively. If the round trip rate is Ti,

【0019】[0019]

【数2】Ti =P′/P0 , P0 …入射波,
P′…反射波である。
[Equation 2] Ti = P '/ P0 , P0 … Incident wave,
P ': reflected wave.

【0020】入射角が縦波臨界角より、小さい範囲では
横波も一部発生するが、縦波の往復通過率が大きく縦波
が支配的である。入射角が増加して縦波臨界角を超え、
横波臨界角までの範囲においては横波のみが現われる。
入射角は横波の往復通過率が最大値から約90%(約1
dBだけ最大値から下がった範囲である。入射角で言う
と、例えば、媒質Iが水、媒質IIがエポキシの場合にお
いては、41度から52度の範囲の音波を出力するよう
に、振動子1の曲率を決定する。これより広い範囲の音
波を出力するようにすると、縦波が生じる可能性が有る
からである)までの値となるように中空球の裁断位置を
選定し、振動子の形状を決定する。振動子1と媒質II3
との相対位置を調節して媒質II3内における集束ビーム
が形成する焦点位置が調整できる。
In the range where the incident angle is smaller than the critical angle of the longitudinal wave, a part of the transverse wave is also generated, but the longitudinal wave has a large reciprocal passage rate and the longitudinal wave is dominant. Incident angle increases and exceeds longitudinal wave critical angle,
In the range up to the shear wave critical angle, only the shear wave appears.
The incident angle is about 90% (about 1%)
This is a range that is lower than the maximum value by dB. In terms of the incident angle, for example, when the medium I is water and the medium II is epoxy, the curvature of the vibrator 1 is determined so as to output a sound wave in the range of 41 to 52 degrees. This is because if a sound wave in a wider range is output, a longitudinal wave may be generated), the cutting position of the hollow sphere is selected, and the shape of the vibrator is determined. Transducer 1 and medium II3
Can be adjusted to adjust the focal position formed by the focused beam in the medium II3.

【0021】媒質I2に水、媒質II3にエポキシ樹脂を
用いたとき屈折率は1に近く、且つ横波の往復通過率が
適正な値となるよう振動子の形状を決定すると、超音波
周波数を高くしたり、開口寸法を大きくすることなく著
しく先鋭な集束ビームが形成され集束度を上げることが
できる。
When water is used for the medium I2 and epoxy resin is used for the medium II3, the refractive index is close to 1 and the shape of the vibrator is determined so that the reciprocal transmissivity of the transverse wave becomes an appropriate value. And a sharply focused beam is formed without increasing the aperture size, thereby increasing the degree of convergence.

【0022】従って媒質II3内の微小欠陥などから十分
なレベルの反射信号が得られて感度が向上する。更に互
いに隣接する欠陥などの識別が容易になり、分解能も向
上できる。従ってプラスチック材よりなるICパッケー
ジに発生した割れや内部におけるチップの剥離などが高
分解能にて検知できる。
Therefore, a sufficient level of reflected signal can be obtained from a minute defect in the medium II3, and the sensitivity is improved. Further, it is easy to identify defects adjacent to each other, and the resolution can be improved. Therefore, cracks generated in an IC package made of a plastic material and peeling of a chip inside can be detected with high resolution.

【0023】以上説明してきたように、本発明によれ
ば、以下に列挙する効果が得られる。
As described above, according to the present invention, the following effects can be obtained.

【0024】球面を円環状にそなえた振動子から、縦波
臨界角より大きな入射角にて媒質IIへ超音波を放射す
るよう相互に配置しているので、媒質IIの中では横波
超音波のみで集束度の高い焦点を形成できるため高感度
が得られる。
Since the ultrasonic waves are radiated from the vibrator having a spherical surface to the medium II at an incident angle larger than the longitudinal wave critical angle, only the transverse ultrasonic waves are included in the medium II. Can form a focus with a high degree of convergence, so that high sensitivity can be obtained.

【0025】さらに、同一周波数ならば縦波超音波より
約1/2短い波長の横波超音波を使用するため減衰の少
ない低い周波数でも高い分解能が得られる(一般に超音
波は周波数の2乗で減衰が大きくなる)。
Further, if the frequency is the same, a high resolution can be obtained even at a low frequency with a small attenuation since a transverse wave ultrasonic wave having a wavelength shorter than that of the longitudinal wave ultrasonic wave is used by about half. Becomes larger).

【0026】この結果、探触子は感度ならびに分解能が
向上し微小欠陥が検出できる。
As a result, the probe has improved sensitivity and resolution, and can detect minute defects.

【0027】[0027]

【発明の効果】以上説明してきたように、本発明によれ
ば、横波超音波を用いて、媒質Iを介して媒質IIにおい
て集束しうる超音波の送波を行う超音波探傷方法を提供
できる。
As described above, according to the present invention, it is possible to provide an ultrasonic flaw detection method for transmitting ultrasonic waves that can be focused on the medium II via the medium I using the transverse ultrasonic waves. .

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

【図1】本発明の振動子の一実施例を示す断面図。FIG. 1 is a sectional view showing an embodiment of a vibrator according to the present invention.

【図2】本発明の振動子の上面図。FIG. 2 is a top view of the vibrator of the present invention.

【図3】斜め入射による縦波と横波の強度分布のグラ
フ。
FIG. 3 is a graph showing the intensity distribution of longitudinal waves and transverse waves due to oblique incidence.

【図4】従来の超音波探触子の断面図。FIG. 4 is a cross-sectional view of a conventional ultrasonic probe.

【図5】本発明の振動子の一実施例における音の伝搬路
の説明図。
FIG. 5 is an explanatory diagram of a sound propagation path in one embodiment of the vibrator of the present invention.

【図6】本発明の振動子の一実施例の外観を示す説明
図。
FIG. 6 is an explanatory view showing the appearance of one embodiment of the vibrator of the present invention.

【符号の説明】[Explanation of symbols]

1…振動子 41…振動子 42…ダンパ 43…音響レンズ DESCRIPTION OF SYMBOLS 1 ... vibrator 41 ... vibrator 42 ... damper 43 ... acoustic lens

───────────────────────────────────────────────────── フロントページの続き 審査官 神谷 直慈 (56)参考文献 特開 昭59−157560(JP,A) 特開 昭61−286747(JP,A) 実開 昭62−140450(JP,U) (58)調査した分野(Int.Cl.7,DB名) G01N 29/00 - 29/28 ────────────────────────────────────────────────── ─── Continuation of the front page Examiner Naoji Kamiya (56) References JP-A-59-157560 (JP, A) JP-A-61-286747 (JP, A) Jikai Sho 62-140450 (JP, U) (58) Field surveyed (Int. Cl. 7 , DB name) G01N 29/00-29/28

Claims (4)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】媒質Iを介して媒質IIへ向けて超音波を送
波する超音波探触子を用いた超音波探傷方法において、互いに平行する2つの平面で中空球を裁断したときにで
きる円環状の1の 振動子から放射された超音波を縦波
臨界角より大きな角度で媒質IIへ斜めに入射させるこ
と、 媒質II内部に発生した横波を、屈折後、焦点位置に焦束
させること特徴とする超音波探傷方法。
In an ultrasonic flaw detection method using an ultrasonic probe for transmitting ultrasonic waves toward a medium II via a medium I, when a hollow sphere is cut on two planes parallel to each other.
The ultrasonic wave radiated from one vibrating ring is obliquely incident on the medium II at an angle larger than the critical angle of the longitudinal wave. The transverse wave generated inside the medium II is focused at the focal point after refraction. ultrasonic flaw detection method characterized by be.
【請求項2】媒質Iを介して媒質IIに向けて超音波を送
波する超音波探触子であって、縦波臨界角より大きな角度で前記超音波が円環状に媒質
IIへ斜めに入射するように、 球面を互いに平行な2つの
平面裁断したときにできる円環状の位置に、1の振動
子を有することを特徴とする超音波探触子。
2. An ultrasonic probe for transmitting an ultrasonic wave toward a medium II via a medium I , wherein the ultrasonic wave is formed in an annular shape at an angle larger than a longitudinal critical angle.
An ultrasonic probe having one vibrator at an annular position formed when a spherical surface is cut by two planes parallel to each other so as to be obliquely incident on II .
【請求項3】媒質Iを介して媒質IIに向けて超音波を送
波する超音波探触子であって、縦波臨界角より大きな角度で前記超音波が円環状に媒質
IIへ斜めに入射するように 、中空球を互いに平行な2つ
の平面裁断したときにできる円環状の1の振動子を有
することを特徴とする超音波探触子。
3. An ultrasonic probe for transmitting an ultrasonic wave toward a medium II via a medium I , wherein the ultrasonic wave is formed into an annular shape at an angle larger than a longitudinal wave critical angle.
To be incident obliquely to II, the ultrasonic probe and having a first vibrator annular capable when cut hollow sphere with two parallel planes to each other.
【請求項4】請求項2または3記載の超音波探触子であ
って、 当該超音波探触子は、超音波の受波の機能を有すること
を特徴とする超音波探触子。
4. The ultrasonic probe according to claim 2 , wherein said ultrasonic probe has a function of receiving an ultrasonic wave.
JP04099914A 1992-04-20 1992-04-20 Ultrasonic flaw detection method and ultrasonic probe Expired - Lifetime JP3121430B2 (en)

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Application Number Priority Date Filing Date Title
JP04099914A JP3121430B2 (en) 1992-04-20 1992-04-20 Ultrasonic flaw detection method and ultrasonic probe

Publications (2)

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JPH0643139A JPH0643139A (en) 1994-02-18
JP3121430B2 true JP3121430B2 (en) 2000-12-25

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7175599B2 (en) * 2003-04-17 2007-02-13 Brigham And Women's Hospital, Inc. Shear mode diagnostic ultrasound
US7344509B2 (en) * 2003-04-17 2008-03-18 Kullervo Hynynen Shear mode therapeutic ultrasound
CA2712540C (en) * 2005-08-26 2015-12-08 Masaki Yamano Ultrasonic probe, ultrasonic testing equipment, ultrasonic testing method, and manufacturing method of seamless pipe or tube
JP5645428B2 (en) * 2010-03-04 2014-12-24 三菱重工業株式会社 Ultrasonic flaw detection method

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