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JPS623900B2 - - Google Patents
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JPS623900B2 - - Google Patents

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Publication number
JPS623900B2
JPS623900B2 JP54096958A JP9695879A JPS623900B2 JP S623900 B2 JPS623900 B2 JP S623900B2 JP 54096958 A JP54096958 A JP 54096958A JP 9695879 A JP9695879 A JP 9695879A JP S623900 B2 JPS623900 B2 JP S623900B2
Authority
JP
Japan
Prior art keywords
transducer
magnetic field
permanent magnet
inspected
thickness
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
Application number
JP54096958A
Other languages
Japanese (ja)
Other versions
JPS5621058A (en
Inventor
Toshihiro Mori
Nobutada Sugaya
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.)
JFE Engineering Corp
Original Assignee
Nippon Kokan Ltd
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 Nippon Kokan Ltd filed Critical Nippon Kokan Ltd
Priority to JP9695879A priority Critical patent/JPS5621058A/en
Publication of JPS5621058A publication Critical patent/JPS5621058A/en
Publication of JPS623900B2 publication Critical patent/JPS623900B2/ja
Granted legal-status Critical Current

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  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Transducers For Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 この発明は鋼材、特に連続鋳造工程等での熱間
素材の探傷に用いて有用な電磁超音波探傷用トラ
ンスジユーサに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a transducer for electromagnetic ultrasonic flaw detection that is useful for flaw detection of steel materials, particularly hot materials in continuous casting processes.

従来、電磁超音波探傷用トランスジユーサとし
て、ヨーク形の電磁石あるいは永久磁石を用いて
磁束を絞り、磁石の先端部にコイルを置いて被検
査材表面に渦電流を発生させ、渦電流と磁界の相
互作用によるローレンツ力によつて被検査材内に
超音波エネルギーを投入するようにしたものが知
られている。その基本構成を示すと第1図のとお
りである。図に示したように、いま、コイル2に
ある方向の電流を流すと被検査材3の表面部に渦
電流Iが発生し、これと磁石1による磁界Hとの
相互作用により被検査材3の表面部にローレンツ
力Fが働く。従つてコイル2に交流電流を流すこ
とによつて、第1図の場合、振動方向と伝播方向
が一致する縦波の超音波が被検査材3に投入され
ることになる。
Conventionally, as a transducer for electromagnetic ultrasonic flaw detection, a yoke-shaped electromagnet or a permanent magnet is used to narrow the magnetic flux, and a coil is placed at the tip of the magnet to generate eddy currents on the surface of the material to be inspected. A method is known in which ultrasonic energy is input into the material to be inspected using the Lorentz force caused by the interaction between the two. The basic configuration is shown in Figure 1. As shown in the figure, when a current in a certain direction is passed through the coil 2, an eddy current I is generated on the surface of the inspected material 3, and due to the interaction between this and the magnetic field H generated by the magnet 1, the inspected material Lorentz force F acts on the surface of . Therefore, by passing an alternating current through the coil 2, in the case of FIG. 1, longitudinal ultrasonic waves whose vibration direction and propagation direction coincide are applied to the inspected material 3.

被検査材3に投入された超音波は、被検査材3
中に欠陥があるとそこで反射されて戻つてくる。
そこに戻つてくる超音波を、投入の場合と逆の変
換過程により検出コイルで検出することにより探
傷が行われる。この場合検出コイルは、第1図の
励磁用コイル2をそのまま用いることもできる
し、これと別個に用意してもよい。
The ultrasonic waves applied to the material to be inspected 3
If there is a defect inside, it will be reflected back.
Flaw detection is performed by detecting the returning ultrasonic waves with a detection coil through a conversion process that is the reverse of the input process. In this case, as the detection coil, the excitation coil 2 shown in FIG. 1 can be used as is, or it can be prepared separately.

電磁超音波用トランスジユーサによる投入エネ
ルギを増大させるためには、発生磁界を強力にす
ることが必要である。しかしそのためには、第1
図の構成ではヨークが極めて大きなものとなり、
実用上からはある程度の規模に止めざるを得な
い。従つて投入エネルギも限定され、高感度を得
ることが難しい。
In order to increase the input energy by an electromagnetic ultrasound transducer, it is necessary to make the generated magnetic field stronger. However, in order to do so, the first
In the configuration shown in the figure, the yoke is extremely large,
From a practical standpoint, it has no choice but to be limited to a certain scale. Therefore, input energy is also limited, making it difficult to obtain high sensitivity.

このような問題を解決するものとして、磁界を
被検査材の表面近傍に局在させて全体の静磁エネ
ルギを小さくすることで、小形のマグネツトで大
きなバイアス磁界を発生するようにした新しい電
磁超音波トランスジユーサが最近提案された。そ
の基本構成は、厚み方向に磁化した複数枚の永久
磁石板を高透磁率磁性材で挾んで交互に極性が逆
になるように厚み方向に配列してなる磁界発生機
構と、その端部近傍に前記永久磁石板の配列に沿
つて蛇行するように配置した波型状コイルとから
なる。
To solve these problems, we have developed a new electromagnetic superstructure that allows a small magnet to generate a large bias magnetic field by localizing the magnetic field near the surface of the material under test and reducing the overall magnetostatic energy. Sonic transducers have recently been proposed. The basic structure consists of a magnetic field generation mechanism in which multiple permanent magnet plates magnetized in the thickness direction are sandwiched between high permeability magnetic materials and arranged in the thickness direction so that the polarity is alternately reversed, and and a wave-shaped coil arranged in a meandering manner along the arrangement of the permanent magnet plates.

ところで、連続鋳造工程等での熱間素材の探傷
をこのような電磁超音波トランスジユーサで行う
場合には、冷間での場合と異なつていくつかの配
慮が必要となる。特に重要な点は、トランスジユ
ーサと被検査材との間の空隙距離を十分大きく、
例えば5mm程度とらなければならないことであ
る。その理由は、熱間素材の場合表面の凹凸が激
しいこと、トランスジユーサを冷却構造としてト
ランスジユーサの端面と被検査材の間の空隙に冷
却媒体を流さなければならないこと、等にある。
そして、このような空隙距離を保ちながら、大き
い超音波エネルギを投入して熱間素材で問題とな
る15mm×15mm程度以上の欠陥を高感度に検出する
ことが要求される。
By the way, when performing flaw detection on a hot material in a continuous casting process or the like using such an electromagnetic ultrasonic transducer, several considerations are required, unlike when testing in a cold process. It is especially important to make the gap distance between the transducer and the material under test sufficiently large.
For example, it must be about 5 mm. The reasons for this are that hot materials have severe surface irregularities, and that the transducer has a cooling structure in which a cooling medium must flow into the gap between the end face of the transducer and the material to be inspected.
While maintaining such a gap distance, it is required to input a large amount of ultrasonic energy to detect defects of approximately 15 mm x 15 mm or larger, which are a problem in hot materials, with high sensitivity.

この発明は上記の点に鑑みてなされたもので、
被検査材表面部の広い面積に均一で強力な磁界を
形成することができる磁界発生機構と波型状コイ
ルとの組合せを用い、特に熱間素材の欠陥検出を
効果的に行うことを可能とした電磁超音波用トラ
ンスジユーサを提供するものである。
This invention was made in view of the above points,
By using a combination of a magnetic field generation mechanism that can form a uniform and strong magnetic field over a wide area of the surface of the material to be inspected, and a corrugated coil, it is possible to effectively detect defects, especially in hot materials. The present invention provides an electromagnetic ultrasonic transducer.

この発明に係る電磁超音波探傷用トランスジユ
ーサは、厚み方向に磁化した複数枚の永久磁石板
を、高透磁率磁性材で挾んで交互に極性が逆にな
るように厚み方向に配列してなる磁界発生機構を
有し、この磁界発生機構の端部近傍に前記永久磁
石板の配列に沿つて蛇行する波型状コイルを配置
して構成され、かつ上記磁界発生機構の有効面積
を2.5〜3.5インチ角に設定したことを特徴とす
る。この場合、以下に詳述するように、波型状コ
イルと永久磁石板との配置関係を選ぶことによつ
て、被検査材に励起する超音波を縦波とするか横
波とするかあるいは表面波とするかを選ぶことが
できる。
The electromagnetic ultrasonic flaw detection transducer according to the present invention includes a plurality of permanent magnet plates magnetized in the thickness direction, sandwiched between high permeability magnetic materials and arranged in the thickness direction so that the polarities are alternately reversed. The magnetic field generating mechanism has a magnetic field generating mechanism configured by arranging a wave-shaped coil that meanders along the arrangement of the permanent magnet plates near the end of the magnetic field generating mechanism, and the effective area of the magnetic field generating mechanism is 2.5 to 2.5 mm. It is characterized by being set at 3.5 inches square. In this case, as detailed below, by selecting the arrangement relationship between the corrugated coil and the permanent magnet plate, it is possible to select whether the ultrasonic waves excited in the material to be inspected are longitudinal waves, transverse waves, or surface waves. You can choose between waves.

この発明の一実施例の縦波用兼表面波用トラン
スジユーサを第2図〜第4図を参照して説明す
る。これらの図から明らかなように、厚み方向に
磁化した複数枚の永久磁石板11(11,11
,11……………)を、高透磁率磁性材12
(12,12,12……………)で挾んで
交互に極性が逆になるように厚み方向に配列して
磁界発生機構を構成している。渦電流を発生させ
る波型状コイル13は、この例では、第3図に示
したように永久磁石板11の端面直下のみをはう
ように蛇行させて配設している。14は被検査材
である。磁界発生機構の有効面積は2.5〜3.5イン
チ角とする。
A longitudinal wave and surface wave transducer according to an embodiment of the present invention will be described with reference to FIGS. 2 to 4. As is clear from these figures, a plurality of permanent magnet plates 11 (11 1 , 11
2 , 11 3 ……………), high permeability magnetic material 12
(12 1 , 12 2 , 12 3 . . . ) are arranged in the thickness direction so that the polarity is alternately reversed to form a magnetic field generation mechanism. In this example, the wave-shaped coil 13 that generates an eddy current is arranged in a meandering manner so as to creep only directly under the end face of the permanent magnet plate 11, as shown in FIG. 14 is a material to be inspected. The effective area of the magnetic field generation mechanism shall be 2.5 to 3.5 inches square.

第4図は模式的な縦断面図であり、これを用い
て被検査材14への超音波エネルギ投入の様子を
説明すると、いま、波型状コイル13に第3図に
矢印で示した方向の電流を流したとき被検査材1
4表面の永久磁石板11直下の各部に図示極性の
渦電流Iが発生する。この渦電流Iと永久磁石板
11直下の水平方向の磁界Hとの相互作用によ
り、被検査材14表面部には図示極性のローレン
ツ力Fが働く。従つて、波型状コイル13に交流
電流を流すことによつて、振動方向と伝播方向が
共に垂直方向である縦波の超音波が被検査材14
に励起されることになる。
FIG. 4 is a schematic vertical cross-sectional view, and to explain how ultrasonic energy is applied to the inspected material 14 using this, the wave-shaped coil 13 is now directed in the direction indicated by the arrow in FIG. 3. When a current of 1 is applied to the inspected material 1
Eddy currents I having the polarities shown are generated in each part directly under the permanent magnet plate 11 on the fourth surface. Due to the interaction between this eddy current I and the horizontal magnetic field H directly below the permanent magnet plate 11, a Lorentz force F of the illustrated polarity acts on the surface of the inspected material 14. Therefore, by passing an alternating current through the wave-shaped coil 13, longitudinal ultrasonic waves whose vibration direction and propagation direction are both perpendicular to the inspected material 14 are transmitted.
It will be excited by

この場合、主要な超音波は縦波であるが、被検
査材14の表面部にできる磁界の垂直方向成分と
上記渦電流との相互作用も若干存在するため、表
面波も同時に励起される。
In this case, the main ultrasonic waves are longitudinal waves, but since there is some interaction between the vertical component of the magnetic field generated on the surface of the material to be inspected and the eddy current, surface waves are also excited at the same time.

このようにして被検査材14中に超音波を励起
し、その超音波の欠陥部からの反射波を上述した
超音波励起と逆の変換過程をたどつて例えば波型
状コイル13により検出することで探傷が行われ
る。勿論、波型状コイル13とは別にこれと対に
した検出用コイルを配設してもよい。
In this way, ultrasonic waves are excited in the inspected material 14, and the reflected waves of the ultrasonic waves from the defective parts are detected by, for example, the corrugated coil 13 by following the conversion process reverse to the above-mentioned ultrasonic excitation. This is how flaw detection is performed. Of course, a detection coil paired with the wave-shaped coil 13 may be provided separately from the wave-shaped coil 13.

この実施例によれば、その磁界発生機構の構成
上、均一で強力な磁界が得られ、これと波型状コ
イルにより誘導する渦電流との相互作用によつ
て、均一でかつ広い探傷面を得ることができる。
またトランスジユーサの有効面積の拡大に伴つ
て、トランスジユーサと被検査材との間の距離を
従来に比べて十分大きくとつて高感度に欠陥検出
を行うことが可能である。
According to this embodiment, due to the configuration of the magnetic field generation mechanism, a uniform and strong magnetic field can be obtained, and the interaction between this and the eddy current induced by the corrugated coil allows a uniform and wide flaw detection surface to be obtained. Obtainable.
Furthermore, as the effective area of the transducer increases, the distance between the transducer and the material to be inspected can be made sufficiently larger than in the past, and defects can be detected with high sensitivity.

実験によれば、トランスジユーサの有効面積を
1.0インチ角に設計したときの空隙距離と出力電
圧の関係は第5図に示す如くでありまた次の実験
によれば有効面積を2.5インチ角〜3.5インチ角に
設計したとき、トランスジユーサと被検査材との
間の空隙距離を5mmとして15mm×15mmの大きさの
欠陥を十分高感度に検出することができた。有効
面積を余り大きくとると、小さい欠陥を検出する
ことができなくなり、また有効面積を小さくする
とトランスジユーサと被検査材との間の空隙距離
を大きく設定することができず、トランスジユー
サを冷却構造として熱間素材の欠陥検出を効果的
に行うことができない。以上の関係を図示すると
第6図のようになり、有効面積を2.5〜3.5インチ
角とすることが、熱間素材の探傷にとつて好まし
いことが判る。
Experiments have shown that the effective area of the transducer is
The relationship between the air gap distance and the output voltage when designed to be 1.0 inches square is as shown in Figure 5, and according to the following experiment, when the effective area is designed to be 2.5 inches square to 3.5 inches square, the transducer and A defect with a size of 15 mm x 15 mm was able to be detected with sufficiently high sensitivity when the gap distance between the test material and the material to be inspected was 5 mm. If the effective area is set too large, small defects cannot be detected, and if the effective area is set too small, the gap distance between the transducer and the material to be inspected cannot be set large, making it difficult to detect the transducer. As a cooling structure, it is not possible to effectively detect defects in hot materials. The above relationship is illustrated in FIG. 6, and it can be seen that it is preferable for the effective area to be 2.5 to 3.5 inches square for flaw detection of hot materials.

第7図〜第9図はこの発明の更に別の実施例の
要部構成を示している。これらの実施例は磁界発
生機構の両面に波型状コイル13,13′を配置
して両面トランスジユーサを構成したものであ
る。即ち第7図の実施例は、下面を縦波用とし上
面を横波用とした両面トランスジユーサである。
第8図の実施例は第7図における永久磁石板11
の厚みを2倍にしたもので、縦波が約2倍に強化
されることが実験の結果判つている。他方、第9
図は逆に第7図における高透磁率磁性板12の厚
みを2倍にしたもので横波が約2倍に強化される
ことが判つている。
FIGS. 7 to 9 show the main structure of still another embodiment of the present invention. In these embodiments, wave-shaped coils 13, 13' are arranged on both sides of the magnetic field generating mechanism to constitute a double-sided transducer. That is, the embodiment shown in FIG. 7 is a double-sided transducer in which the lower surface is used for longitudinal waves and the upper surface is used for transverse waves.
The embodiment of FIG. 8 is the permanent magnet plate 11 in FIG.
Experiments have shown that by doubling the thickness of the material, longitudinal waves are approximately doubled. On the other hand, the ninth
On the contrary, the figure shows a case in which the thickness of the high permeability magnetic plate 12 in FIG. 7 is doubled, and it has been found that transverse waves are strengthened approximately twice as much.

以上、実施例を挙げて説明したように、この発
明に係る電磁超音波探傷用トランスジユーサによ
れば、被検査材に対して均一で強力な磁界を与え
る磁界発生機構と波型状コイルとの組合せによつ
て有効面積を2.5〜3.5インチ角に設定すること
で、均一でかつ広い探傷面を得ることができ、ま
た有効面積の拡大により、被検査材との間の距離
を大きくとつて熱間素材についても十分高感度に
欠陥検出を行うことができる。
As described above with reference to the embodiments, the transducer for electromagnetic ultrasonic flaw detection according to the present invention has a magnetic field generation mechanism that applies a uniform and strong magnetic field to the inspected material, and a corrugated coil. By setting the effective area to 2.5 to 3.5 inches square by the combination of Defects can be detected with sufficiently high sensitivity even in hot materials.

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

第1図は従来の電磁超音波用トランスジユーサ
の代表例を示す図、第2図はこの発明の一実施例
の電磁超音波用トランスジユーサを示す斜視図、
第3図はその波型状コイルの配設パターンを示す
図、第4図は同じく動作を説明するための模式的
縦断面図、第5図は空隙距離と出力電圧の関係を
示す図、第6図は同じく有効面積と検出能力の関
係を示す図、第7図〜第9図は両面用としたトラ
ンスジユーサの実施例の要部構成を示す図であ
る。 11(11,11,11……………)…
…永久磁石板、12(12,12,12
…………)……高透磁率磁性材、13,13′…
…波型状コイル、14……被検査材。
FIG. 1 is a diagram showing a typical example of a conventional electromagnetic ultrasonic transducer, and FIG. 2 is a perspective view showing an electromagnetic ultrasonic transducer according to an embodiment of the present invention.
FIG. 3 is a diagram showing the arrangement pattern of the wave-shaped coil, FIG. 4 is a schematic longitudinal cross-sectional view for explaining the operation, FIG. FIG. 6 is a diagram similarly showing the relationship between the effective area and the detection capability, and FIGS. 7 to 9 are diagrams showing the main part configuration of an embodiment of the transducer for both sides. 11 (11 1 , 11 2 , 11 3 ……………)…
...Permanent magnet plate, 12 (12 1 , 12 2 , 12 3 ...
………)……High permeability magnetic material, 13,13′…
... Wave-shaped coil, 14 ... Material to be inspected.

Claims (1)

【特許請求の範囲】 1 厚み方向に磁化した複数枚の永久磁石板を、
高透磁率磁性材で挾んで交互に極性が逆になるよ
うに厚み方向に配列してなる磁界発生機構と、こ
の磁界発生機構の端部近傍に配置され前記永久磁
石板の配列に沿つて蛇行する波型状コイルとを備
え、前記磁界発生機構の有効面積を2.5〜3.5イン
チ角に設定したことを特徴とする電磁超音波探傷
用トランスジユーサ。 2 永久磁石板の厚みを高透磁率磁性材の厚みの
1.5〜2.5倍にしたことを特徴とする特許請求の範
囲第1項記載の電磁超音波探傷用トランスジユー
サ。 3 高透磁率磁性材の厚みを永久磁石板の厚みの
1.5〜2.5倍にしたことを特徴とする特許請求の範
囲第1項記載の電磁超音波探傷用トランスジユー
サ。
[Claims] 1. A plurality of permanent magnet plates magnetized in the thickness direction,
A magnetic field generating mechanism arranged in the thickness direction so that the polarity is alternately reversed while being sandwiched between high permeability magnetic materials, and a magnetic field generating mechanism arranged near the end of the magnetic field generating mechanism and meandering along the arrangement of the permanent magnet plates. A transducer for electromagnetic ultrasonic flaw detection, characterized in that the effective area of the magnetic field generation mechanism is set to 2.5 to 3.5 inches square. 2 Set the thickness of the permanent magnet plate to the thickness of the high permeability magnetic material.
The transducer for electromagnetic ultrasonic flaw detection according to claim 1, wherein the transducer is 1.5 to 2.5 times larger. 3 The thickness of the high permeability magnetic material is the thickness of the permanent magnet plate.
The transducer for electromagnetic ultrasonic flaw detection according to claim 1, wherein the transducer is 1.5 to 2.5 times larger.
JP9695879A 1979-07-30 1979-07-30 Transducer for electromagnetic supersonic wave flaw detection Granted JPS5621058A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9695879A JPS5621058A (en) 1979-07-30 1979-07-30 Transducer for electromagnetic supersonic wave flaw detection

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9695879A JPS5621058A (en) 1979-07-30 1979-07-30 Transducer for electromagnetic supersonic wave flaw detection

Publications (2)

Publication Number Publication Date
JPS5621058A JPS5621058A (en) 1981-02-27
JPS623900B2 true JPS623900B2 (en) 1987-01-27

Family

ID=14178766

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9695879A Granted JPS5621058A (en) 1979-07-30 1979-07-30 Transducer for electromagnetic supersonic wave flaw detection

Country Status (1)

Country Link
JP (1) JPS5621058A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0293394U (en) * 1988-12-28 1990-07-25

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58116662U (en) * 1982-02-02 1983-08-09 三菱重工業株式会社 electromagnetic acoustic transducer
US4471658A (en) * 1981-09-22 1984-09-18 Mitsubishi Jukogyo Kabushiki Kaisha Electromagnetic acoustic transducer
JPS5995453A (en) * 1982-11-24 1984-06-01 Mitsubishi Heavy Ind Ltd Electromagnetic ultrasonic transducer
US5608164A (en) * 1995-07-27 1997-03-04 The Babcock & Wilcox Company Electromagnetic acoustic transducer (EMAT) for ultrasonic inspection of liquids in containers
US6122969A (en) 1998-08-24 2000-09-26 Mcdermott Technology, Inc. Main bang recovery EMAT
US6192760B1 (en) 1999-08-19 2001-02-27 Mcdermott Technology, Inc. EMAT transmit/receive switch
GB201419219D0 (en) * 2014-10-29 2014-12-10 Imp Innovations Ltd Electromagnetic accoustic transducer

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0293394U (en) * 1988-12-28 1990-07-25

Also Published As

Publication number Publication date
JPS5621058A (en) 1981-02-27

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