JPH0142376B2 - - Google Patents

Info

Publication number
JPH0142376B2
JPH0142376B2 JP57068287A JP6828782A JPH0142376B2 JP H0142376 B2 JPH0142376 B2 JP H0142376B2 JP 57068287 A JP57068287 A JP 57068287A JP 6828782 A JP6828782 A JP 6828782A JP H0142376 B2 JPH0142376 B2 JP H0142376B2
Authority
JP
Japan
Prior art keywords
thin tube
transmitting coil
defect
emat
coil
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
JP57068287A
Other languages
Japanese (ja)
Other versions
JPS58186046A (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 JP57068287A priority Critical patent/JPS58186046A/en
Publication of JPS58186046A publication Critical patent/JPS58186046A/en
Publication of JPH0142376B2 publication Critical patent/JPH0142376B2/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)

Description

【発明の詳細な説明】 本発明は細管の超音波探傷等に用いられる電磁
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 used for ultrasonic flaw detection of thin tubes, etc.

細管内に挿入して超音波探傷を行なう電磁音響
トランスデユーサ(以下EMATと略す)として
は、従来第1図に示す構造のものが知られてい
る。即ち、図中の1…は上下の極性が互に反対と
なるように配列した永久磁石であり、これら永久
磁石1…には例えば5つの永久磁石が1ユニツト
となるようにコイル2…が巻装されて、これによ
りEMAT3が構成されている。なお、図中の4
はEMAT3が挿入される細管である。かかる
EMATの動作を第2を参照して説明する。
EMAT3のコイル2…に高周波を流すと、この
コイル2に近接する細管4に渦電流Iが発生す
る。一方、永久磁石1…から細管4壁面に対して
垂直で周期的な磁束Bが加えられ、前記渦電流I
との相互作用によりローレンツ力Fが発生する。
こうしたローレンツ力Fは磁束周期と同じ周期で
変化し、この力Fにより細管4にSH波と呼ばれ
る超音波(板波)が発生する。なお、超音波の検
出は上述したのと逆プロセスで電気信号に変換し
て行なう。
As an electromagnetic acoustic transducer (hereinafter abbreviated as EMAT) that is inserted into a thin tube to perform ultrasonic flaw detection, one having the structure shown in FIG. 1 is conventionally known. That is, 1 in the figure are permanent magnets arranged so that the upper and lower polarities are opposite to each other, and coils 2 are wound around these permanent magnets 1 so that, for example, five permanent magnets form one unit. This constitutes EMAT3. In addition, 4 in the figure
is the tubule into which EMAT3 is inserted. It takes
The operation of EMAT will be explained with reference to the second example.
When a high frequency is applied to the coil 2 of the EMAT 3, an eddy current I is generated in the thin tube 4 adjacent to the coil 2. On the other hand, a perpendicular and periodic magnetic flux B is applied from the permanent magnet 1 to the wall surface of the thin tube 4, and the eddy current I
Lorentz force F is generated by the interaction with
This Lorentz force F changes at the same period as the magnetic flux period, and this force F generates ultrasonic waves (plate waves) called SH waves in the thin tube 4. Note that the ultrasonic waves are detected by converting them into electrical signals in a reverse process to that described above.

しかしながら、上記構造のEMAT3で発生さ
せた超音波は細管4の軸方向に伝播するため、周
方向の欠陥に対して強く反射されるが、軸方向欠
陥に対しては反射率が低く、欠陥検出が困難とな
る。そこで、周方向に伝播する波を発生させれば
よいが、細管の径がさいと、細管周上を廻つて帰
つてくる超音波の持続時間が長い場合、欠陥信号
がその中に埋もれて検出できない。
However, since the ultrasonic waves generated by the EMAT 3 with the above structure propagate in the axial direction of the thin tube 4, they are strongly reflected against defects in the circumferential direction, but the reflectance is low against defects in the axial direction, and the defect detection becomes difficult. Therefore, it is sufficient to generate a wave that propagates in the circumferential direction, but if the diameter of the capillary is small and the duration of the ultrasonic wave that circulates around the circumference of the capillary and returns is long, the defect signal will be buried in it and detected. Can not.

本発明は上記欠点を解消するためになされたも
ので、径の小さい細管の軸方向欠陥信号のみを取
出すことが可能で、欠陥検出を確実に遂行し得る
電磁音響トランスデユーサを提供しようとするも
のである。
The present invention has been made in order to eliminate the above-mentioned drawbacks, and aims to provide an electromagnetic acoustic transducer that is capable of extracting only axial defect signals of small-diameter thin tubes and that can reliably perform defect detection. It is something.

以下、本発明を第3図示の一実施例に基づいて
詳細に説明する。
Hereinafter, the present invention will be explained in detail based on an embodiment shown in the third diagram.

図中11は磁気回路を形成する永久磁石であ
り、この磁石の極性を示す両端面は細管内壁面に
沿うように曲率をなしている。また、前記磁石1
1の両側面には先端側を細管内壁面に沿うように
曲率とした一対の支持部12a,12bが夫々取
付けられている。そして、一方の支持部12a先
端の曲率面には送信コイル13が該曲率方向に対
して直交する方向に蛇行させて配設されている。
また、他方の支持部12b先端の曲率面には、受
信コイル14が該曲率方向に対して直交する方向
に蛇行させて配設されている。つまり前記送信、
受信のコイル13,14は永久磁石11を中心に
して対称的に配置されている。これらコイル1
3,14は共に発生する超音波の波長λに等しい
周期T0で蛇行され、かつ送信コイル13の長さ
LTと受信コイル14の長さLRは次式のようにな
つている。
In the figure, reference numeral 11 denotes a permanent magnet forming a magnetic circuit, and both end faces of this magnet indicating polarity are curved along the inner wall surface of the thin tube. Moreover, the magnet 1
A pair of support parts 12a and 12b whose distal ends are curved along the inner wall surface of the thin tube are attached to both side surfaces of the support part 1, respectively. A transmitting coil 13 is disposed on a curved surface at the tip of one of the support portions 12a in a meandering manner in a direction perpendicular to the direction of curvature.
Further, on the curved surface of the tip of the other support portion 12b, a receiving coil 14 is arranged in a meandering manner in a direction perpendicular to the direction of curvature. In other words, the above transmission,
The receiving coils 13 and 14 are arranged symmetrically with the permanent magnet 11 at the center. These coils 1
3 and 14 meander with a period T 0 equal to the wavelength λ of the ultrasonic waves generated, and the length of the transmitting coil 13
L T and the length L R of the receiving coil 14 are expressed as follows.

LR=Tp(n+1/2)+LT (但し、n=0、±1、±2…) 次に、本発明のEMATの作用を第4図〜第6
図を参照して説明する。
L R = T p (n + 1/2) + L T (however, n = 0, ±1, ±2...) Next, the action of the EMAT of the present invention is shown in Figures 4 to 6.
This will be explained with reference to the figures.

まず、EMATを細管4内に挿入し、送信コイ
ル13に高周波電流を流すと、該送信コイル13
は細管4の軸方向に蛇行して配置されることにな
るため、送信コイル13に近接する細管4壁間に
渦電流Iが発生する。一方、永久磁石11から細
管4壁面に対してその周方向の磁束Bが加えら
れ、前記渦電流Iとの相互作用によりローレンツ
力Fが発生する。こうしたローレンツ力FはTp
の周期で方向が変化するので、波長λがTpに等
しいラム波と呼ばれる板波が細管4の周方向に発
生する。この板波は送信コイル13が位置する細
管4部分を基点として、時計回り方向に伝播する
ものと、反時計回り方向に伝播するものと、に分
かれる。
First, when EMAT is inserted into the thin tube 4 and a high frequency current is passed through the transmitting coil 13, the transmitting coil 13
are arranged in a meandering manner in the axial direction of the thin tube 4, so that an eddy current I is generated between the walls of the thin tube 4 adjacent to the transmitting coil 13. On the other hand, a magnetic flux B in the circumferential direction is applied from the permanent magnet 11 to the wall surface of the thin tube 4, and a Lorentz force F is generated by interaction with the eddy current I. This Lorentz force F is T p
Since the direction changes with a period of , a plate wave called a Lamb wave with a wavelength λ equal to T p is generated in the circumferential direction of the thin tube 4 . These plate waves are divided into those that propagate in a clockwise direction and those that propagate in a counterclockwise direction with the portion of the thin tube 4 where the transmitting coil 13 is located as a base point.

しかして、細管4に欠陥箇所がない場合は、前
記板波が伝播して送信コイル13と細管4中心に
対して対称的に配置された受信コイル14では、
該受信コイル14の位置関係より、時計回りの板
波に対しては第5図aに示す位相の信号が検出さ
れ、反時計回りの板波に対しては同第5図bに示
す前記波形の1/2周期ずれた位相の信号が検出さ
れる。その結果、2つの板波の合成信号は同第5
図cに示すように互に相殺されエコーとして検出
されない。
Therefore, if there is no defect in the thin tube 4, the plate wave propagates, and in the transmitting coil 13 and the receiving coil 14, which are arranged symmetrically with respect to the center of the thin tube 4,
Based on the positional relationship of the receiving coil 14, a signal with a phase shown in FIG. 5a is detected for a clockwise plate wave, and a signal with a phase shown in FIG. 5b is detected for a counterclockwise plate wave. A signal with a phase shift of 1/2 period is detected. As a result, the composite signal of the two plate waves is
As shown in Figure c, they cancel each other out and are not detected as echoes.

一方、板波が伝播する細管4に欠陥箇所が存在
する場合は、受信コイル14には了第6図aの如
く破線で示す時計回りの板波に一点鎖線で示す欠
陥信号が重畳されて実線で示す信号が検出され、
同第6図bの如く破線で示す反時計回りの板波に
一点鎖線で示す欠陥信号が重畳されて実線で示す
信号が検出される。その結果、受信コイル14で
検出された合成波は同第6図cに示すように欠陥
信号のみ検出される。
On the other hand, if there is a defect in the thin tube 4 through which the plate wave propagates, the receiving coil 14 receives the defect signal shown by the dashed line and is superimposed on the clockwise plate wave shown by the broken line as shown in FIG. The signal indicated by is detected,
As shown in FIG. 6B, the defect signal shown by the dashed line is superimposed on the counterclockwise plate wave shown by the broken line, and the signal shown by the solid line is detected. As a result, only a defective signal is detected in the composite wave detected by the receiving coil 14, as shown in FIG. 6c.

したがつて、欠陥エコーが送信時に発生したエ
コーに重畳して検出が困難な場合でも、欠陥エコ
ーのみ分離することが可能で、確実に欠陥検出を
行なうことができる。また、欠陥エコーが大きく
て、欠陥を通り抜けてくる送信時の時計回りと反
時計回りのエコーのレベルのバランスがくずれて
いる場合には、その差により欠陥の存在を確認で
きる。
Therefore, even if a defective echo is difficult to detect because it is superimposed on an echo generated during transmission, it is possible to separate only the defective echo, and the defect can be detected reliably. Furthermore, if the defect echo is large and the level of the clockwise and counterclockwise echoes transmitted through the defect is unbalanced, the existence of the defect can be confirmed based on the difference.

なお、本発明に係るEMATは、上記実施例に
示す構造のものに限定されず、例えば第7図の構
造のものでも同様の効果を発揮できる。即ち、図
中の15a,15bは磁石用コイル16a,16
bが巻装され、互に対向して配置された馬丁形の
電磁石でである。但し、電磁石に代つて馬丁形の
永久磁石を用いてもよい。そして、一方の電磁石
15aには蛇行した送信コイル13が該電磁石1
5aの極間に介在されるように配設されている。
また、他方の電磁石15bには蛇行した受信コイ
ル14が該電磁石15bの極間に介在されるよう
に配設されている。これらコイル13,14の蛇
行周期、長さは前述した実施例と同様である。こ
のような第7図図示のEMATの電磁石15a,
15b間に第8図に示す如く細管4を配置し、送
信コイル13に高周波電流を流すと、該送信コイ
ル13は細管4外周面の軸方向に蛇行して配置さ
れることになるため、送信コイル13に近接する
細管4壁面に渦電流が発生する。一方、電磁石1
5aから細管4壁面に対してその周方向の磁束が
加えられ、前記渦電流との相互作用によりローレ
ンツ力Fが発生し、第4図図示と同様、送信コイ
ル13が位置する細管4部分を基点として時計回
りに伝播する板波と反時計回りに伝播する板波と
が発生する。こうした時計回りの板波と反時計回
りの板波とを細管4中心に対し送信コイル13と
対称的に配置された電磁石15bの受信コイル1
4で信号検出を行なうことにより、実施例の
EMATと同様欠陥信号のみを検出できる。
It should be noted that the EMAT according to the present invention is not limited to the structure shown in the above embodiment, but can also exhibit the same effect even if it has the structure shown in FIG. 7, for example. That is, 15a and 15b in the figure are magnet coils 16a and 16.
b are horsehair-shaped electromagnets wrapped around each other and placed facing each other. However, a horse-shaped permanent magnet may be used instead of the electromagnet. A meandering transmitting coil 13 is attached to one electromagnet 15a.
It is arranged so as to be interposed between the poles of 5a.
Further, a meandering receiving coil 14 is disposed on the other electromagnet 15b so as to be interposed between the poles of the electromagnet 15b. The meandering period and length of these coils 13 and 14 are the same as in the embodiment described above. The electromagnet 15a of EMAT shown in FIG.
When the thin tube 4 is placed between the tubes 15b and 15b as shown in FIG. 8, and a high frequency current is passed through the transmitting coil 13, the transmitting coil 13 will be arranged in a meandering manner in the axial direction of the outer peripheral surface of the thin tube 4, so that the transmitting Eddy currents are generated on the wall surface of the thin tube 4 close to the coil 13. On the other hand, electromagnet 1
A circumferential magnetic flux is applied from 5a to the wall surface of the thin tube 4, and Lorentz force F is generated by interaction with the eddy current, and as shown in FIG. As a result, a plate wave propagating clockwise and a plate wave propagating counterclockwise are generated. The receiving coil 1 of the electromagnet 15b is arranged symmetrically with the transmitting coil 13 with respect to the center of the thin tube 4, such as clockwise plate waves and counterclockwise plate waves.
By performing signal detection in step 4, the
Like EMAT, it can only detect defect signals.

以上詳述した如く、本発明によれば送信コイ
ル、受信コイルの形状、配置を工夫することによ
り、径の小さい細管に発生させた超音波のうち、
円周上を回つて帰つてきたものを相殺して欠陥信
号のみを取出すことができ、ひいては欠陥検出を
確実に遂行し得る電磁音響トランスデユーサを提
供できる。
As detailed above, according to the present invention, by devising the shape and arrangement of the transmitter coil and the receiver coil, out of the ultrasonic waves generated in the small diameter tube,
It is possible to provide an electromagnetic acoustic transducer that can extract only the defect signal by canceling out the signal that has returned after going around the circumference, and can thereby perform defect detection reliably.

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

第1図は従来のEMATを示す斜視図、第2図
は従来のEMATの作用を示す原理説明図、第3
図は本発明の一実施例を示すEMATの斜視図、
第4図は第3図のEMATの作用を示す原理説明
図、第5図a〜cは夫々板波が伝播する細管に欠
陥箇所がない場合の時計回りの板波の検出信号、
反時計回りの板波の検出信号及び合成信号を示す
波形図、第6図a〜cは夫々板波が伝播する細管
に欠陥箇所がある場合の時計回りの板波の検出信
号、反時計回りの板波の検出信号及び合成した欠
陥信号を示す波形図、第7図は本発明の他の実施
例を示すEMATの斜視図、第8図は第7図の
EMATの作用を示す原理説明図である。 4……細管、11……永久磁石、12a,12
b……支持部、13……送信コイル、14……受
信コイル、15a,15b……電磁石。
Figure 1 is a perspective view showing the conventional EMAT, Figure 2 is a principle explanatory diagram showing the operation of the conventional EMAT, and Figure 3 is a perspective view showing the conventional EMAT.
The figure is a perspective view of EMAT showing one embodiment of the present invention.
Fig. 4 is a principle explanatory diagram showing the operation of the EMAT shown in Fig. 3, and Figs. 5 a to c are detection signals of a clockwise plate wave when there is no defect in the thin tube in which the plate wave propagates, respectively.
Waveform diagrams showing the detection signal and composite signal of a counterclockwise plate wave. Figures 6 a to c are the detection signals of a clockwise plate wave when there is a defect in the thin tube through which the plate wave propagates, respectively, and counterclockwise. FIG. 7 is a perspective view of EMAT showing another embodiment of the present invention, and FIG. 8 is a waveform diagram showing the plate wave detection signal and the combined defect signal.
FIG. 2 is a principle explanatory diagram showing the action of EMAT. 4...Thin tube, 11...Permanent magnet, 12a, 12
b... Support part, 13... Transmission coil, 14... Receiving coil, 15a, 15b... Electromagnet.

Claims (1)

【特許請求の範囲】[Claims] 1 被検体としての細管壁面に沿つて配設された
蛇行状送信コイルと、細管中心に対して前記送信
コイルと対称的な位置に該細管壁面に沿うように
配設され、長さが該送信コイルに比べてn±1/
2(n=0、±1、±2…)周期長いか、もしくは
短い蛇行状受信コイルと、前記各コイルが近接し
ている細管部分に静磁界を与える磁気回路とを具
備したことを特徴とする電磁音響トランスデユー
サ。
1. A meandering transmitting coil disposed along the wall surface of a capillary tube as an object, and a meandering transmitting coil disposed along the wall surface of the capillary tube at a position symmetrical to the transmitting coil with respect to the center of the capillary tube, and having a length equal to that of the transmitting coil. n±1/ compared to coil
2 (n=0, ±1, ±2...) serpentine receiving coils with long or short periods, and a magnetic circuit that applies a static magnetic field to a thin tube portion in which each of the coils is adjacent. An electromagnetic acoustic transducer.
JP57068287A 1982-04-23 1982-04-23 Electromagnetic acoustic transducer Granted JPS58186046A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57068287A JPS58186046A (en) 1982-04-23 1982-04-23 Electromagnetic acoustic transducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57068287A JPS58186046A (en) 1982-04-23 1982-04-23 Electromagnetic acoustic transducer

Publications (2)

Publication Number Publication Date
JPS58186046A JPS58186046A (en) 1983-10-29
JPH0142376B2 true JPH0142376B2 (en) 1989-09-12

Family

ID=13369396

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57068287A Granted JPS58186046A (en) 1982-04-23 1982-04-23 Electromagnetic acoustic transducer

Country Status (1)

Country Link
JP (1) JPS58186046A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0378287B1 (en) * 1989-01-13 1996-06-19 MANNESMANN Aktiengesellschaft Process for detecting flaws in oblong work pieces

Also Published As

Publication number Publication date
JPS58186046A (en) 1983-10-29

Similar Documents

Publication Publication Date Title
US4127035A (en) Electromagnetic transducer
US4471658A (en) Electromagnetic acoustic transducer
US4691572A (en) Transducing device for contactless ultrasonic inspection of pipelines or tubings
JPS60140109A (en) Ultrasonic range finder
CN101813670A (en) Pipeline axial ultrasonic guided wave energy exchange probe
JPH0142376B2 (en)
JP3608423B2 (en) Electromagnetic ultrasonic measurement method and apparatus
JP3673392B2 (en) Electromagnetic ultrasonic flaw detector
KR102203609B1 (en) Electromagnetic acoustic transducer and pipe inspection apparatus comprising the same
JP5305706B2 (en) Electromagnetic ultrasonic probe, ultrasonic flaw detector, and ultrasonic flaw detection method
JP4465420B2 (en) Magnetostrictive ultrasonic element and nondestructive inspection method using the same
JPS6242440B2 (en)
JPS61144566A (en) Electromagnetic acoustic transducer for generating ultrasonic wave
JPH0142375B2 (en)
JPS6080760A (en) Electromagnetic ultrasonic transducer
JPS59228162A (en) Device for inspecting metallic pipe regarding presence of defect by ultrasonic wave
JPH0142377B2 (en)
JPS6333440Y2 (en)
JPH0239252Y2 (en)
JPH0143907B2 (en)
JPH03285160A (en) Remote eddy current flaw detection method
JPH041497Y2 (en)
JPH0143265B2 (en)
JPS6256857A (en) Electromagnetic ultrasonic wave transducer for transverse wave using high frequency magnetic core
JPS63151850A (en) Electromagnetic ultrasound probe device