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JPH0215018B2 - - Google Patents
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JPH0215018B2 - - Google Patents

Info

Publication number
JPH0215018B2
JPH0215018B2 JP16923282A JP16923282A JPH0215018B2 JP H0215018 B2 JPH0215018 B2 JP H0215018B2 JP 16923282 A JP16923282 A JP 16923282A JP 16923282 A JP16923282 A JP 16923282A JP H0215018 B2 JPH0215018 B2 JP H0215018B2
Authority
JP
Japan
Prior art keywords
magnet
coil
magnetic
thin tube
ultrasonic waves
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
JP16923282A
Other languages
Japanese (ja)
Other versions
JPS5958358A (en
Inventor
Kazuo Morimoto
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.)
Mitsubishi Heavy Industries Ltd
Original Assignee
Mitsubishi Heavy Industries 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 Mitsubishi Heavy Industries Ltd filed Critical Mitsubishi Heavy Industries Ltd
Priority to JP16923282A priority Critical patent/JPS5958358A/en
Publication of JPS5958358A publication Critical patent/JPS5958358A/en
Publication of JPH0215018B2 publication Critical patent/JPH0215018B2/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
    • G01N29/24Probes
    • G01N29/2412Probes using the magnetostrictive properties of the material to be examined, e.g. electromagnetic acoustic transducers [EMAT]

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (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)
  • Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
  • Transducers For Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 この発明は例えば配管等の導電性構造部材を探
傷する探傷装置の電磁音響トランスデユーサに関
する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic acoustic transducer for a flaw detection device that detects flaws in conductive structural members such as piping.

例えば水道配管等の細管に存在する欠陥を超音
波で探傷するには、第1図に示すようなトランス
デユーサを用いて超音波を発生させている。この
トランスデユーサは例えば複数の永久磁石11
a,11b,…を1単位として、それぞれの磁石
11a,11b,…の上下極性が相反するように
配列し、この1単位とする磁石群の周囲に高周波
電流を流すコイル12を巻装して構成している。
For example, in order to detect defects in thin pipes such as water pipes using ultrasonic waves, a transducer as shown in FIG. 1 is used to generate ultrasonic waves. This transducer includes, for example, a plurality of permanent magnets 11
a, 11b, ... are set as one unit, and the magnets 11a, 11b, ... are arranged so that the upper and lower polarities thereof are opposite to each other, and a coil 12 for passing a high-frequency current is wound around the group of magnets forming one unit. It consists of

すなわち第2図に示すように、コイル12に高
周波電流Ihを流すと、このコイル12に接する細
管13には渦電流I1,I2,…が発生するもので、
この渦電流I1,I2,…は磁石11a,11b,…
によりそれぞれ細管13内面に対して垂直で周期
的に変化して生じるようになる磁界B1,B2,…
との相互作用によりローレンツ力F1,F2,…を
発生させる。このローレンツ力F1,F2,…は上
記磁界B1,B2,…の周期と同周期で変化するも
ので、このローレンツカF1,F2,…の方向変化
に対応するように細管13にはSH波と呼ばれる
超音波(板波)が発生する。
That is, as shown in FIG. 2, when a high frequency current Ih is passed through the coil 12, eddy currents I 1 , I 2 , . . . are generated in the thin tube 13 in contact with the coil 12.
These eddy currents I 1 , I 2 ,... are caused by the magnets 11a, 11b,...
As a result, magnetic fields B 1 , B 2 , .
Lorentz forces F 1 , F 2 , ... are generated by the interaction with These Lorentz forces F 1 , F 2 , ... change with the same period as the magnetic fields B 1 , B 2 , ... mentioned above, and the thin tube is 13, ultrasonic waves (plate waves) called SH waves are generated.

つまり細管13に傷等の欠陥が存在する場合、
超音波は傷の存在する位置で反射されるようにな
り、この反射波は上記トランスデユーサにより電
気信号に変換されて検出されるものである。
In other words, if there is a defect such as a scratch on the thin tube 13,
The ultrasonic waves are reflected at the location where the flaw exists, and this reflected wave is converted into an electrical signal by the transducer and detected.

しかし、このように構成されたトランスデユー
サでは、細管13に発生する超音波は主に管軸方
向Xに対して伝播するものであるため、例えば傷
等の欠陥が細管13の円周方向Yに対して存在し
ている場合、超音波は確実に伝播され正確な反射
波を帰還させるようになる。したがつて、これと
は逆に欠陥が管軸方向Xに対して存在している場
合には、超音波を円周方向Yに伝播させることが
困難であるため、上記反射波は正確に帰還されな
い状態となり、充分な探傷感度を得ることができ
ない。
However, in the transducer configured in this way, since the ultrasonic waves generated in the thin tube 13 mainly propagate in the tube axis direction X, defects such as scratches may occur in the thin tube 13 in the circumferential direction Y If there is a difference between the two, the ultrasonic wave will be propagated reliably and the correct reflected wave will be returned. Therefore, on the contrary, if a defect exists in the tube axis direction As a result, sufficient flaw detection sensitivity cannot be obtained.

この発明は上記のような問題点を解決するため
になされたもので、例えば水道配管等の細管を超
音波探傷する際に、探傷される欠陥が管軸方向に
対して存在するような場合でも充分な探傷結出感
度を得ることが可能となる電磁音響トランスデユ
ーサを提供することを目的とする。
This invention was made to solve the above-mentioned problems. For example, when performing ultrasonic flaw detection on thin pipes such as water pipes, even if the flaws to be detected exist in the direction of the pipe axis. The object of the present invention is to provide an electromagnetic acoustic transducer that can obtain sufficient flaw detection sensitivity.

すなわちこの発明に係る電磁音響トランスデユ
ーサは、同一の軸線に対して周囲方向に交互に極
性異ならせ一定ピツチでら旋状に巻回されるよう
に形成した複数の磁石と、この複数の磁石それぞ
れに対応して巻装設定された高周波電流コイルと
を具備したものである。
That is, the electromagnetic acoustic transducer according to the present invention includes a plurality of magnets formed so as to be spirally wound at a constant pitch and having alternately different polarities in the circumferential direction about the same axis, and the plurality of magnets. It is equipped with high frequency current coils which are wound and set in correspondence with each other.

以下図面によりこの発明の一実施例を説明す
る。
An embodiment of the present invention will be described below with reference to the drawings.

第3図はその構成を示すもので、例えば6本の
細長状の磁石帯20a〜20fを、円柱コア21
の周囲表面に対して、隣接する磁石帯20a〜2
0fの磁極がN極、S極と交互に異なるようにし
て同一のピツチTmでら旋状に並ぶように巻回
し、この磁石帯20a〜20fそれぞれの略中心
および各磁石帯と磁石帯との間に、高周波電流コ
イル22を巻装して円柱状の磁石体として一体化
構成する。
FIG. 3 shows its configuration. For example, six elongated magnet bands 20a to 20f are connected to a cylindrical core 21.
With respect to the surrounding surface of the adjacent magnetic strips 20a-2
The magnetic pole of 0f is alternately different from the N pole and the S pole, and is wound so that it is arranged in a spiral shape with the same pitch Tm. A high frequency current coil 22 is wound between them to form an integrated structure as a cylindrical magnet body.

上記円柱コア21に巻回するそれぞれの磁石帯
20a〜20fは、第4図aに示すような細長状
で円柱コア21の周囲表面と直角方向の磁化方向
を有するゴム磁石23を用いるか、または第4図
bに示すような同様の磁化方向を有する小形磁石
24を直列に並べて用いるかして形成するもので
ある。そして、隣接するこれらの磁石帯20a〜
20fの磁化方向は、そのそれぞれが逆方向とな
るように設定する。このようなゴム磁石23もし
くは小形磁石24でなる磁気回路に巻装されるコ
イル22は、第5図に第3図に展開して示すよう
にピツチT0で方向が逆転しており、このコイル
22は、第4図の磁石体の外周表面に巻装され
る。なお、このコイル22の巻装位置は、磁石帯
20a〜20fにおける磁極面の略中央部及び各
磁石帯間である。この巻装したコイル22に対す
る高周波電流Ihは、ピツチT0で流れる方向が逆
転し、且つ磁石帯20a〜20fに巻付けられた
磁石面に沿つてら旋状に流れる。
Each of the magnet bands 20a to 20f wound around the cylindrical core 21 may be a rubber magnet 23 having an elongated shape and having a magnetization direction perpendicular to the peripheral surface of the cylindrical core 21 as shown in FIG. 4a, or It is formed by arranging in series small magnets 24 having the same magnetization direction as shown in FIG. 4b. And these adjacent magnetic bands 20a~
The magnetization directions of 20f are set to be opposite directions. The coil 22 wound around the magnetic circuit made of such a rubber magnet 23 or small magnet 24 has its direction reversed at pitch T 0 as shown in FIG. 5 and expanded in FIG. 22 is wound around the outer peripheral surface of the magnet body shown in FIG. The winding position of this coil 22 is approximately at the center of the magnetic pole face of the magnetic bands 20a to 20f and between each magnetic band. The direction of the high frequency current Ih flowing through the wound coil 22 is reversed at the pitch T0 , and flows in a spiral shape along the magnet surfaces wound around the magnet bands 20a to 20f.

ここでそれぞれの磁石帯20a〜20fのピツ
チTm、およびコイル22の巻装ピツチT0は次式
を満足する間隔に設定する。
Here, the pitch Tm of each of the magnet bands 20a to 20f and the winding pitch T0 of the coil 22 are set to intervals that satisfy the following equation.

Tm=λ/2 T0=λ/4 但しλは発生する超音波の波長である。 Tm=λ/2 T 0 =λ/4 where λ is the wavelength of the generated ultrasonic wave.

すなわちこのように構成される磁気回路におい
て、第6図にその表面の一部分を展開して示すよ
うに、磁気回路の表面周囲には、それぞれの磁石
帯20a〜20dの磁気作用によりピツチT0
方向が90゜変化する磁界B1〜B7が発生するように
なる。
In other words, in a magnetic circuit constructed in this manner, as shown in FIG. 6, a part of its surface is expanded, there is a pitch T 0 around the surface of the magnetic circuit due to the magnetic action of each of the magnet bands 20a to 20d. Magnetic fields B 1 to B 7 whose directions change by 90° are generated.

第7図はこの磁気回路を細管13内に挿入した
場合に、第6図のA−A面に対応した部分の細管
13の斜断面25を示すもので、つまり磁気回路
により加えられた磁界B1〜B7に対してコイル2
2に高周波電流Ihを流すと、斜断面25にはコイ
ル22と平行にして渦電流I1〜I7が発生する。
FIG. 7 shows a diagonal cross section 25 of the thin tube 13 corresponding to plane A-A in FIG. 6 when this magnetic circuit is inserted into the thin tube 13, that is, the magnetic field B applied by the magnetic circuit is shown. Coil 2 for 1 ~ B 7
When a high frequency current Ih is passed through the coil 2, eddy currents I1 to I7 are generated in the oblique section 25 parallel to the coil 22.

この渦電流I1〜I7は磁界B1〜B7との相互作用に
よりピツチT0で方向が90゜変化するローレンツ力
F1〜F7を発生させるもので、このローレンツ力
F1〜F7が2Tm周期で有する破線で示すような方
向性に伴なつて斜断面25にはラム波(板波)が
発生し、第8図に示すように細管13に対してヘ
リカル状に半無限的に伝播されるようになる。
These eddy currents I 1 to I 7 interact with the magnetic fields B 1 to B 7 due to the Lorentz force whose direction changes by 90° at pitch T 0.
This Lorentz force generates F 1 to F 7 .
Lamb waves (plate waves) are generated in the oblique section 25 due to the directionality shown by the broken line that F 1 to F 7 have at a period of 2Tm, and as shown in FIG. will be propagated semi-infinitely.

以上のようにこの発明によれば、同一の軸線に
対して周囲方向に交互に極性を異ならせ一定ピツ
チでら旋状に巻回されるように形成した複数の磁
石と、この複数の磁石それぞれに対応して巻装設
定された高周波電流コイルとを具備するようにし
たので、細管に対してヘリカル状に伝播する超音
波を発生させることができる。すなわち細管の管
軸方向に沿つて超音波が回転して伝播することに
より、例えばひび割れ等の欠陥が細管の円周方向
に存在する場合のみならず、管軸方向に存在する
ような場合でも、超音波は効果的に伝播されて反
射されるようになる。したがつて上記のような欠
陥が細管の如何なる位置に存在しても、充分な探
傷検出感度を得ることが可能となり、細管におけ
る超音波探傷の信頼性は確実に向上するものであ
る。
As described above, according to the present invention, a plurality of magnets are formed so as to be wound in a spiral shape with a constant pitch and have alternately different polarities in the circumferential direction about the same axis, and each of the plurality of magnets is Since the high-frequency current coil is provided with a high-frequency current coil wound in a manner corresponding to the above-mentioned, it is possible to generate ultrasonic waves that propagate helically to the thin tube. In other words, by rotating and propagating ultrasonic waves along the tube axis direction of the thin tube, for example, not only when defects such as cracks exist in the circumferential direction of the thin tube, but also when defects exist in the tube axis direction, Ultrasonic waves are effectively propagated and reflected. Therefore, no matter where the defect as described above exists in the capillary, it is possible to obtain sufficient flaw detection sensitivity, and the reliability of ultrasonic flaw detection in the capillary is surely improved.

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

第1図は従来のトランスデユーサを示す図、第
2図は上記トランスデユーサにより発生する超音
波を説明する図、第3図はこの発明の一実施例に
係る電磁音響トランスデユーサを示す図、第4図
aは上記実施例において磁石として用いることの
できるゴム磁石を示す図、第4図bは上記実施例
において磁石として用いることのできる小形磁石
を示す図、第5図は上記実施例において巻装され
たコイルを展開して示す図、第6図は上記実施例
においてその表面の1部分を展開して示す図、第
7図は上記実施例において発生する超音波を説明
する図、第8図は上記実施例において細管に伝播
される超音波を示す図である。 13……細管、20a〜20f……磁石帯、2
1……円柱コア、22……高周波電流コイル。
FIG. 1 is a diagram showing a conventional transducer, FIG. 2 is a diagram explaining ultrasonic waves generated by the above-mentioned transducer, and FIG. 3 is a diagram showing an electromagnetic acoustic transducer according to an embodiment of the present invention. Fig. 4a shows a rubber magnet that can be used as a magnet in the above embodiment, Fig. 4b shows a small magnet that can be used as a magnet in the above embodiment, and Fig. 5 shows a rubber magnet that can be used as a magnet in the above embodiment. FIG. 6 is an exploded view of a wound coil in the example, FIG. 6 is an expanded view of a part of the surface of the coil in the above example, and FIG. 7 is a diagram illustrating the ultrasonic waves generated in the example above. , FIG. 8 is a diagram showing the ultrasonic waves propagated to the thin tube in the above embodiment. 13...Thin tube, 20a to 20f...Magnetic band, 2
1...Cylindrical core, 22...High frequency current coil.

Claims (1)

【特許請求の範囲】[Claims] 1 円柱コアの外周表面上に、該円柱コアと接す
る面を磁極面とする複数本の細長状磁石帯を、そ
れぞれ隣接する磁石帯の磁極が相異なるようにら
旋状に巻回して磁石体を構成し、前期磁石体の外
周表面上における各磁石帯中心部及び各磁石体間
に、それぞれ電流の流れる方向が相異なるコイル
を巻装したことを特徴とする電磁音響トランスデ
ユーサ。
1 A magnet body is created by winding a plurality of elongated magnet strips on the outer circumferential surface of a cylindrical core in a spiral shape so that the magnetic poles of adjacent magnet strips are different from each other. 1. An electromagnetic acoustic transducer comprising: coils having different current flow directions wound around the center of each magnet band and between each magnet body on the outer peripheral surface of the magnet body.
JP16923282A 1982-09-28 1982-09-28 Electromagnetic acoustic transducer Granted JPS5958358A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16923282A JPS5958358A (en) 1982-09-28 1982-09-28 Electromagnetic acoustic transducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16923282A JPS5958358A (en) 1982-09-28 1982-09-28 Electromagnetic acoustic transducer

Publications (2)

Publication Number Publication Date
JPS5958358A JPS5958358A (en) 1984-04-04
JPH0215018B2 true JPH0215018B2 (en) 1990-04-10

Family

ID=15882676

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16923282A Granted JPS5958358A (en) 1982-09-28 1982-09-28 Electromagnetic acoustic transducer

Country Status (1)

Country Link
JP (1) JPS5958358A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6267447A (en) * 1985-09-20 1987-03-27 Mitsubishi Heavy Ind Ltd Method and apparatus for detecting axial defect of tube
US8653811B2 (en) * 2009-06-26 2014-02-18 Tdw Delaware Inc. Pipeline inspection tool with oblique magnetizer
AT508478B1 (en) * 2009-06-26 2012-01-15 Tdw Delaware Inc SENSORARRAY FOR THE INSPECTION OF THE INTERNAL WALL OF A TUBE
US8319494B2 (en) 2009-06-26 2012-11-27 Tdw Delaware Inc. Pipeline inspection tool with double spiral EMAT sensor array

Also Published As

Publication number Publication date
JPS5958358A (en) 1984-04-04

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