JPS58166258A - Ultrasonic microscopic lens - Google Patents

Ultrasonic microscopic lens

Info

Publication number
JPS58166258A
JPS58166258A JP57049899A JP4989982A JPS58166258A JP S58166258 A JPS58166258 A JP S58166258A JP 57049899 A JP57049899 A JP 57049899A JP 4989982 A JP4989982 A JP 4989982A JP S58166258 A JPS58166258 A JP S58166258A
Authority
JP
Japan
Prior art keywords
lens
forward end
face
recess
single crystal
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
JP57049899A
Other languages
Japanese (ja)
Other versions
JPH0365495B2 (en
Inventor
Ichiji Yamanaka
一司 山中
Satoshi Nagai
聰 永井
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.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
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 Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP57049899A priority Critical patent/JPS58166258A/en
Publication of JPS58166258A publication Critical patent/JPS58166258A/en
Publication of JPH0365495B2 publication Critical patent/JPH0365495B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/22Details, e.g. general constructional or apparatus details
    • G01N29/221Arrangements for directing or focusing the acoustical waves

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)

Abstract

PURPOSE:To perform easily nondestructive inspection of a relatively thick layer, by providing a recess of a circular conical shape on the forward end face of a cylinder consisting of single crystal alumina or fused quartz and focusing a refracted converging beam on the segment on the central line of said circular cone. CONSTITUTION:An acoustic lens 1 is produced by tapering 2, the outside circumference on the forward end of a cylinder consisting of single crystal alumina (sapphire) or fused quartz (quartz glass), providing a conic recess at the center of said forward end face and forming a conical surface 4. According to such ultrasonic microscopic lens of this invention, beams can be focused on the segment in an object; therefore, the nondestructive inspection of relatively thick layer is easily executed. The construction thereof is extremely simple and the easy working of the lens is possible.

Description

【発明の詳細な説明】 本発明は、材料の非破壊検査等に好適な超音波顕微鏡レ
ンズに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic microscope lens suitable for non-destructive testing of materials.

最近、超音波顕微鏡が開発され、これによって固体表面
下のミクロン程度の大きさの微小欠陥を非破壊検査する
ことが可能になった。この超音波顕微鏡は、超音波ビー
ムをレンズで絞ることにより小さなスポットとし、これ
によって試料の表面上を走査しながら反射強度を各場所
ごとに記録し、2次元的に走査した結果をディスプレイ
に表示するものであり、弾性波に対する応答性の違いに
よシ機械的性質に対応した表示画面を得ることができる
Recently, ultrasonic microscopes have been developed, which have made it possible to non-destructively inspect minute defects on the order of microns beneath the surface of solids. This ultrasonic microscope uses a lens to focus the ultrasonic beam into a small spot, which scans the surface of the sample while recording the reflected intensity at each location, and displays the two-dimensional scanning results on a display. Therefore, it is possible to obtain a display screen that corresponds to mechanical properties due to the difference in response to elastic waves.

しかるに、現在用いられている超音波顕微鏡レンズは凹
球面レンズであって、これにより超音波ビームを焦点に
収束させているため、レンズと対象物体との間の距離を
一定にすると、焦点の位置によって決まる特定の深さの
層の観察に限られることになる。つまり、焦点深度が小
さい。
However, the currently used ultrasound microscope lenses are concave spherical lenses that converge the ultrasound beam to a focal point, so if the distance between the lens and the target object is constant, the focal position Observation is limited to a layer at a specific depth determined by In other words, the depth of focus is small.

これに対し、一般的な工業製品の非破壊検査では、欠陥
の正確な位置の検出よりも欠陥の有無を検出すればよい
という場合が少なくない。このような非破壊検査に既存
の超音波顕微鏡を用い、厚い層を全体的に観察しようと
すると、レンズと物体表面の間の距離を何通りかに変え
て多数枚のスライス像を撮る必要がある。これは、厚い
層を少ない労力で能率的に非破壊検査しようとする場合
に望ましいことではない。
On the other hand, in general non-destructive testing of industrial products, it is often sufficient to detect the presence or absence of a defect rather than the exact position of the defect. When attempting to observe a thick layer in its entirety using an existing ultrasound microscope for such nondestructive testing, it is necessary to take multiple slice images by changing the distance between the lens and the object surface in several ways. be. This is undesirable when trying to efficiently non-destructively test thick layers with little effort.

斜上に鑑み、本発明は、焦点深度の大きい超音波顕微鏡
レンズを開発し、1回の撮像で比較的厚い層の非破壊検
査を完了できるようにすることを目的とするものである
In view of the above, the present invention aims to develop an ultrasonic microscope lens with a large depth of focus, so that non-destructive testing of relatively thick layers can be completed with one imaging.

かかる目的を達成するため、本発明の超音波顕微鏡レン
ズは、単結晶アルミナ又は溶解石英からなる円筒の先端
面に円錐状の凹みを設けて、屈折した収束ビームにその
円錐の中心線上の線分上に焦点を結ばせるための円錐面
を形成し、上記円筒の先端面に対向する基端面に圧電薄
膜を設けることにより構成される。
In order to achieve such an object, the ultrasonic microscope lens of the present invention has a conical recess on the tip surface of a cylinder made of single-crystal alumina or fused silica, so that the refracted convergent beam has a line segment on the center line of the cone. It is constructed by forming a conical surface for focusing upward, and providing a piezoelectric thin film on the base end surface opposite to the distal end surface of the cylinder.

而して、かかる構成によれば、円錐面において屈折した
収束ビームが上記線分上において焦点を結ぶだめ、焦点
深度の大きい超音波顕微鏡レンズを得ることができる。
According to this configuration, since the convergent beam refracted at the conical surface is focused on the line segment, an ultrasonic microscope lens with a large depth of focus can be obtained.

以下に図面を参照して本発明の実施例について詳述する
Embodiments of the present invention will be described in detail below with reference to the drawings.

第1図に示す音響レンズ1は、単結晶アルミナ(サファ
イヤ)又は溶融石英(石英ガラス)からなる円筒の先端
外周をテーパ面2とし、かつその先端面の中心に円錐状
の凹み3を設け、円錐面4を形成したものである。円錐
状の凹み3の内部には、エポキシ樹脂やブチルゴム等か
らなる吸音体5を埋設するが、その位置は円錐状凹み3
の頂点からその凹み3の深さの略1/3までであり、即
ち第1図において円錐状凹み3の頂点Bからの長さDE
=1/3ACを直径とすると位置までである。
The acoustic lens 1 shown in FIG. 1 is a cylinder made of single crystal alumina (sapphire) or fused silica (quartz glass), with a tapered surface 2 on the outer periphery of the tip, and a conical recess 3 in the center of the tip surface. A conical surface 4 is formed. A sound absorbing material 5 made of epoxy resin, butyl rubber, etc. is buried inside the conical recess 3, and its position is within the conical recess 3.
from the apex of the conical recess 3 to approximately 1/3 of the depth of the recess 3, that is, the length DE from the apex B of the conical recess 3 in FIG.
If = 1/3 AC is the diameter, it is up to the position.

一方、上記円筒における基端面、即ち円錐状凹み3を設
けた側と反対の側の端面には、接地電極6、圧電薄膜7
、信号電極8を蒸着し、これをケース9に固定して、通
常の超音波顕微鏡に既存のレンズと同様に取付けて使用
する。
On the other hand, a ground electrode 6 and a piezoelectric thin film 7 are provided on the base end surface of the cylinder, that is, the end surface on the opposite side to the side where the conical recess 3 is provided.
, a signal electrode 8 is vapor-deposited, this is fixed to a case 9, and it is used by attaching it to an ordinary ultrasound microscope in the same way as an existing lens.

上記構成を有する超音波顕微鏡レンズにおいては、第2
図に示すように、圧電薄膜で励起された平行超音波ビー
ムλA −C’Cが円錐面4(二よって一定の角度で屈
折し、収束ビームAP −L)H,、E+(〜CQに変
換される。      ・ 従って、レンズの内側から出る収束ビーム、1)14及
びERが対象物体10上の点Rで焦点を結ぶようにそれ
らを配置すれば、レンズにおいて上記ビームDR及びE
Rよりも外側から出る収束ビームが物体10の表面で屈
折し、物体10内において円錐面の中心線上の線分RS
の上で焦点を結ぶことになり、線分RS上に微少欠陥が
ある場合には、それが鋭く絞られたビームで照射される
ため、反射波が生じて検出されることになる。吸音体5
は、不必要なビームや乱反射したビームを吸収させるた
めのものである。
In the ultrasonic microscope lens having the above configuration, the second
As shown in the figure, the parallel ultrasound beam λA -C'C excited by the piezoelectric thin film is refracted at a certain angle by the conical surface 4 (2) and converted into a convergent beam AP -L)H,,E+(~CQ).・Therefore, if the convergent beams 1) 14 and ER coming out from inside the lens are arranged so that they are focused at a point R on the target object 10, then at the lens the beams DR and E
A convergent beam emitted from outside R is refracted at the surface of the object 10, and within the object 10 a line segment RS on the center line of the conical surface is formed.
If there is a minute defect on the line segment RS, it will be irradiated with a sharply focused beam, and a reflected wave will be generated and detected. Sound absorber 5
is for absorbing unnecessary beams and diffusely reflected beams.

なお、第2図に示す角度αは、 を満たすか、これよりもやや大きくするのが望ましい。Note that the angle α shown in Fig. 2 is It is desirable to satisfy or slightly larger than this.

ここで、vA 、 Vc 、 Vl、は、それぞれレン
ズ中での縦波音速、カップラーとして用いる液体中の音
速、及び検査する物体中の縦波音速である。角度αをこ
のように選ぶと、物体内には波長の短い横波のみが励起
されて波長の長い縦波が励起されず、その結果、分解能
が高められる。
Here, vA, Vc, and Vl are the longitudinal sound speed in the lens, the sound speed in the liquid used as a coupler, and the longitudinal sound speed in the object to be inspected, respectively. When the angle α is selected in this way, only transverse waves with short wavelengths are excited in the object, and longitudinal waves with long wavelengths are not excited, and as a result, resolution is improved.

このような本発明の超音波顕微鏡レンズによれば、対象
物体内における線分上に焦点を結ばせることができるた
め、比較的厚い層の非破壊検査を簡単に実施することが
でき、しかもその構造が非常に簡単で、加工も極めて容
易に行うことができる。
According to the ultrasonic microscope lens of the present invention, since it is possible to focus on a line segment within a target object, non-destructive inspection of a relatively thick layer can be easily performed. It has a very simple structure and can be processed very easily.

また、プラスチックを用いた低周波用の探触子は提案さ
れているが、プラスチックでは吸収が大きく、高周波化
に限界があって、分解能も高々0.1mm程度にしかな
らないが、本発明では単結晶アルミナや溶融石英という
吸収の小さい材料を用いるので、比較的容易に高周波化
を行い、ミクロン程度の分解能を得ることができる。
Additionally, low-frequency probes made of plastic have been proposed, but plastic has large absorption, limits the ability to use high frequencies, and has a resolution of only about 0.1 mm. Since materials with low absorption such as crystalline alumina and fused silica are used, it is relatively easy to increase the frequency and obtain resolution on the order of microns.

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

第1図は本発明の超音波顕微鏡レンズの実施例を示す断
面図、第2図はその作用説明図である。 3・・・円錐状凹み、   4・・・円錐面、7・・・
圧電薄膜。
FIG. 1 is a sectional view showing an embodiment of the ultrasonic microscope lens of the present invention, and FIG. 2 is an explanatory view of its operation. 3... Conical recess, 4... Conical surface, 7...
Piezoelectric thin film.

Claims (1)

【特許請求の範囲】[Claims] 1、 単結晶アルミナ又は溶融石英からなる円筒の先端
面に円錐状の凹みを設けて、屈折した収束ビームにその
円錐の中心線上の線分上に焦点を結ばせるための円錐面
を形成し、上記円筒の先端面に対向する基端面に圧電薄
膜を設けたことを特徴とする超音波顕微鏡レンズ。
1. A conical recess is provided on the tip surface of a cylinder made of single crystal alumina or fused silica to form a conical surface for focusing the refracted convergent beam on a line segment on the center line of the cone; An ultrasonic microscope lens characterized in that a piezoelectric thin film is provided on the proximal end face opposite to the distal end face of the cylinder.
JP57049899A 1982-03-27 1982-03-27 Ultrasonic microscopic lens Granted JPS58166258A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57049899A JPS58166258A (en) 1982-03-27 1982-03-27 Ultrasonic microscopic lens

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57049899A JPS58166258A (en) 1982-03-27 1982-03-27 Ultrasonic microscopic lens

Publications (2)

Publication Number Publication Date
JPS58166258A true JPS58166258A (en) 1983-10-01
JPH0365495B2 JPH0365495B2 (en) 1991-10-14

Family

ID=12843860

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57049899A Granted JPS58166258A (en) 1982-03-27 1982-03-27 Ultrasonic microscopic lens

Country Status (1)

Country Link
JP (1) JPS58166258A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6179158A (en) * 1984-09-27 1986-04-22 Toppan Printing Co Ltd Ultrasonic microscope lens
JPH03113362A (en) * 1989-09-16 1991-05-14 Wild Leitz Gmbh Conical ultrasonic wave deflector
CN113092381A (en) * 2021-02-25 2021-07-09 南昌大学 Acousto-optic coupling prism suitable for large depth-of-field detection of photoacoustic microimaging

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6179158A (en) * 1984-09-27 1986-04-22 Toppan Printing Co Ltd Ultrasonic microscope lens
JPH03113362A (en) * 1989-09-16 1991-05-14 Wild Leitz Gmbh Conical ultrasonic wave deflector
CN113092381A (en) * 2021-02-25 2021-07-09 南昌大学 Acousto-optic coupling prism suitable for large depth-of-field detection of photoacoustic microimaging

Also Published As

Publication number Publication date
JPH0365495B2 (en) 1991-10-14

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