JP3268219B2 - Eddy current detector - Google Patents

Eddy current detector

Info

Publication number
JP3268219B2
JP3268219B2 JP32038396A JP32038396A JP3268219B2 JP 3268219 B2 JP3268219 B2 JP 3268219B2 JP 32038396 A JP32038396 A JP 32038396A JP 32038396 A JP32038396 A JP 32038396A JP 3268219 B2 JP3268219 B2 JP 3268219B2
Authority
JP
Japan
Prior art keywords
eddy current
magnetic field
magnetic core
flaw detector
subject
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 - Fee Related
Application number
JP32038396A
Other languages
Japanese (ja)
Other versions
JPH10160709A (en
Inventor
保夫 荒木
優 谷口
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 JP32038396A priority Critical patent/JP3268219B2/en
Publication of JPH10160709A publication Critical patent/JPH10160709A/en
Application granted granted Critical
Publication of JP3268219B2 publication Critical patent/JP3268219B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

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

【0001】[0001]

【発明の属する技術分野】本発明は、金属平板等の被検
体の健全性を確認するために、被検体に渦電流を励起し
て欠陥などの異常検出を行う渦電流探傷子に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an eddy current flaw detector for detecting an abnormality such as a defect by exciting an eddy current in an object to check the soundness of the object such as a metal plate.

【0002】[0002]

【従来の技術】一般に渦電流探傷装置は、金属平板など
の金属体中の欠陥の有無を判定し、その健全性を確認す
るために使用されている。従来の渦電流探傷装置は、図
4に示すように励磁コイル101,検出コイル102,
磁心103で構成される探傷子100、及び表示画面1
21を有する探傷器120からなり、探傷子100と探
傷器120とが接続ケーブル130によって接続されて
いる。なお、磁心103は検出感度を高くするために、
磁界を通しやすい強磁性体で形成される。
2. Description of the Related Art Generally, an eddy current flaw detector is used to determine the presence or absence of a defect in a metal body such as a metal flat plate and to confirm its soundness. As shown in FIG. 4, a conventional eddy current flaw detector includes an excitation coil 101, a detection coil 102,
Flaw detector 100 composed of magnetic core 103 and display screen 1
The flaw detector 120 includes the flaw detector 100 and the flaw detector 120 connected by a connection cable 130. Note that the magnetic core 103 is used to increase the detection sensitivity.
It is formed of a ferromagnetic material that easily passes a magnetic field.

【0003】110は金属板などの金属体からなる被検
体、111は被検体110中の表面欠陥、131は励磁
コイル101が発生する磁界、132は励磁コイル10
1が発生する磁界131によって被検体110中に励起
される渦電流、133は渦電流132によって発生する
磁界である。
Reference numeral 110 denotes an object made of a metal body such as a metal plate; 111, a surface defect in the object 110; 131, a magnetic field generated by the exciting coil 101;
An eddy current 133 excited in the subject 110 by the magnetic field 131 generated by the reference numeral 1 is a magnetic field generated by the eddy current 132.

【0004】この渦電流探傷装置の電気的な接続状態を
示す図5を参照して説明すると、励磁コイル101は、
発振器141から一定の大きさ(振幅)、一定周波数の
交流電流が供給されることによって磁界131を発生
し、この磁界131が被検体110と鎖交することによ
り、被検体110に渦電流132が誘起される。この渦
電流132は、被検体110が健全な場合(欠陥が存在
しない場合)、励磁コイル101と同心円上に発生す
る。この渦電流132によっても磁界133が誘起さ
れ、励磁コイル101が発生する磁界131に影響す
る。
Referring to FIG. 5, which shows an electrical connection state of the eddy current flaw detector, an exciting coil 101 is
An alternating current having a constant magnitude (amplitude) and a constant frequency is supplied from the oscillator 141 to generate a magnetic field 131, and the magnetic field 131 links with the subject 110, thereby causing an eddy current 132 in the subject 110. Induced. The eddy current 132 is generated concentrically with the exciting coil 101 when the subject 110 is healthy (when there is no defect). The eddy current 132 also induces a magnetic field 133, which affects the magnetic field 131 generated by the exciting coil 101.

【0005】検出コイル102には、励磁コイル131
の発生する磁界131に渦電流132による磁界133
が影響されたものが鎖交し、交流電圧が誘起される。励
磁コイル101が発生する磁界131は常に一定に保た
れているため、検出コイル102に誘起される電圧の変
化分に着目することによって、被検体110の異常(欠
陥の存在等)を感知することができる。
The detection coil 102 includes an excitation coil 131
Generated by an eddy current 132
Are affected, and an AC voltage is induced. Since the magnetic field 131 generated by the excitation coil 101 is always kept constant, it is possible to detect an abnormality (existence of a defect or the like) of the subject 110 by focusing on a change in the voltage induced in the detection coil 102. Can be.

【0006】探傷器120の内部には各種の信号処理回
路が存在しており、この信号処理回路によって、検出コ
イル102に誘起する電圧の変化だけを抽出して表示画
面121に波形として表示する。
Various signal processing circuits are present inside the flaw detector 120. The signal processing circuit extracts only a change in voltage induced in the detection coil 102 and displays the change on the display screen 121 as a waveform.

【0007】被検体110に欠陥が存在する場合、渦電
流132の流れ方が欠陥のない場合に対して変化する。
この時、渦電流132による磁界133も欠陥のない場
合に対して変化するため、検出コイル102に誘起され
る電圧も変化する。この電圧の変化を探傷器120の表
示画面121で観察し、欠陥の有無を判断することがで
きる。
When a defect exists in the object 110, the flow of the eddy current 132 changes with respect to the case where there is no defect.
At this time, since the magnetic field 133 due to the eddy current 132 also changes with respect to the case where there is no defect, the voltage induced in the detection coil 102 also changes. This change in voltage can be observed on the display screen 121 of the flaw detector 120 to determine the presence or absence of a defect.

【0008】実際には、探傷子100を被検体110に
沿って移動させながら、この時の探傷器120の表示画
面121の波形を観察する。このように、渦電流探傷で
は、探傷子100を被検体110の表面上で移動させな
がら、その時の探傷器120の表示画面121に現れる
波形を観察することによって、欠陥の有無などを判断で
き、被検体110の健全性を知ることができる。
In practice, the waveform of the display screen 121 of the flaw detector 120 at this time is observed while moving the flaw detector 100 along the subject 110. As described above, in the eddy current detection, the presence or absence of a defect can be determined by observing the waveform that appears on the display screen 121 of the flaw detector 120 at that time while moving the flaw detector 100 on the surface of the subject 110, The health of the subject 110 can be known.

【0009】[0009]

【発明が解決しようとする課題】上記した従来の探傷子
を使用した場合、図6に示すように、励磁コイル101
が発生するほとんど全ての磁界(被検体110の表面部
を通過する磁界135及び被検体110の裏面部を通過
する磁界136など)及びこれらの磁界により誘起され
る全ての渦電流による磁界の影響を検出コイル102が
受ける。
When the above-described conventional flaw detector is used, as shown in FIG.
Of the magnetic field generated by the magnetic field (the magnetic field 135 passing through the front surface of the subject 110 and the magnetic field 136 passing through the back surface of the subject 110) and the influence of the magnetic field due to all eddy currents induced by these magnetic fields. The detection coil 102 receives it.

【0010】ここで、方向が同一の磁束(磁界)は互い
に反発する作用があるため、励磁コイル101が発生す
る磁界135,136は比較的広く拡がり、被検体11
0に誘起される渦電流も広く分布する。被検体110に
存在する欠陥等の異常により検出コイル102に生じる
電圧振幅は、その異常部分が被検体110中に流れる渦
電流のどれだけの量と作用するかによって決まる。従来
のように被検体110に流れる渦電流が広く分布する場
合、渦電流の密度が低いため被検体110中に存在する
小さな欠陥112と作用する渦電流の量は小さくなる。
この現象は、特に小さな欠陥112が探傷子の裏側に存
在する場合、顕著に現れる。
Here, since the magnetic fluxes (magnetic fields) having the same direction have a repulsive action, the magnetic fields 135 and 136 generated by the exciting coil 101 spread relatively widely.
Eddy currents induced at zero are also widely distributed. The voltage amplitude generated in the detection coil 102 due to an abnormality such as a defect existing in the object 110 is determined by the amount and the amount of the eddy current flowing in the object 110 at the abnormal portion. When the eddy current flowing through the subject 110 is widely distributed as in the related art, the density of the eddy current is low, and the amount of the eddy current acting on the small defect 112 existing in the subject 110 becomes small.
This phenomenon is particularly noticeable when a small defect 112 exists on the back side of the probe.

【0011】従って、大きい欠陥を走査したときは、図
7(a)に示すように、探傷器120の表示画面121
には大きな波形122が現れるが、小さい欠陥を走査し
たときには、図7(b)に示すように、表示画面121
には小さな波形124しか現れ無い。すなわち、従来の
渦電流探傷子では小さな欠陥に対する検出性能が低いと
いう問題があった。本発明の目的は、小さな欠陥に対す
る検出性能の向上を図った渦電流探傷子を提供すること
にある。
Therefore, when a large defect is scanned, the display screen 121 of the flaw detector 120 is scanned as shown in FIG.
Shows a large waveform 122, but when a small defect is scanned, as shown in FIG.
, Only a small waveform 124 appears. That is, the conventional eddy current flaw detector has a problem that the detection performance for a small defect is low. An object of the present invention is to provide an eddy current flaw detector with improved detection performance for small defects.

【0012】[0012]

【課題を解決するための手段】上記課題を解決するため
に、本発明は励磁コイル及び検出コイルが巻装される磁
心の形状を改良することによって、被検体に作用する磁
界の分散を少なくし、かつこの磁界によって生じる渦電
流による磁界が集中的に検出コイルに作用するようにし
たものである。
SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, the present invention reduces the dispersion of a magnetic field acting on a subject by improving the shape of a magnetic core around which an exciting coil and a detecting coil are wound. In addition, a magnetic field due to an eddy current generated by the magnetic field acts on the detection coil intensively.

【0013】すなわち、本発明の渦電流探傷子は、強磁
性体から形成され、円板状磁心部上に中心磁心部,内部
円筒状磁心部,外部円筒状磁極部を同軸的に設けてなる
磁心材と、前記内部円筒状磁心部の外周に設けられ、被
検体に渦電流を誘起させるための励磁コイルと、前記中
心磁心部の外周に設けられ、前記被検体に誘起された渦
電流の変化を検出する検出コイルとを具備してなること
を特徴とする。なお、前記中心磁心部は、棒状でも筒状
でもよい。
That is, the eddy current flaw detector of the present invention is formed of a ferromagnetic material, and is provided with a central magnetic core, an inner cylindrical magnetic core, and an outer cylindrical magnetic pole coaxially on a disk-shaped magnetic core. A magnetic core material, provided on the outer periphery of the inner cylindrical magnetic core portion, an excitation coil for inducing an eddy current in the subject, and provided on the outer periphery of the center magnetic core portion, of the eddy current induced in the subject. And a detection coil for detecting a change. The center core may be rod-shaped or cylindrical.

【0014】このように構成された本発明の渦電流探傷
子においては、励磁コイルによって発生する磁界は、中
心磁心部及び内部円筒状磁心部を経由して被検体に作用
し、渦電流を生じさせる。一方、検出コイルには中心磁
心部の内部を通過する磁界のみが作用し、この磁界が被
検体に生じる渦電流による磁界の影響受けた際の変化に
よって電圧が誘起される。
In the thus constructed eddy current flaw detector of the present invention, the magnetic field generated by the excitation coil acts on the subject via the central magnetic core and the inner cylindrical magnetic core to generate an eddy current. Let it. On the other hand, only a magnetic field that passes through the center core acts on the detection coil, and a voltage is induced by a change when the magnetic field is affected by the magnetic field due to the eddy current generated in the subject.

【0015】内部円筒状磁心部を経由する磁界及び中心
磁心部を経由する磁界は、被検体に作用する領域ではほ
ぼ同一方向であり、同一方向に生じる磁界は互いに反発
するため、中心磁心部を経由する磁界は内部円筒状磁心
部を経由する磁界により反発されて中心磁心部のより中
心部に集中する。このため、中心磁心部を経由する磁界
によって被検体中に誘起される渦電流は中心部に集中
し、この部分に欠陥が有れば、欠陥と作用する渦電流の
比率が高くなる。また、この渦電流による磁界の変化
は、中心磁心部の外周に設けられた検出コイルによって
効率よく検出される。従って、小さい欠陥でも良好に感
知することができる。
The magnetic field passing through the inner cylindrical magnetic core portion and the magnetic field passing through the central magnetic core portion are substantially in the same direction in the region acting on the subject, and the magnetic fields generated in the same direction repel each other. The magnetic field passing through is repelled by the magnetic field passing through the inner cylindrical magnetic core, and is concentrated at a more central portion of the central magnetic core. For this reason, the eddy current induced in the subject by the magnetic field passing through the central magnetic core portion is concentrated in the central portion, and if there is a defect in this portion, the ratio of the eddy current acting on the defect increases. Further, the change in the magnetic field due to the eddy current is efficiently detected by the detection coil provided on the outer periphery of the central magnetic core. Therefore, even a small defect can be detected well.

【0016】[0016]

【発明の実施の形態】本発明の実施の形態を以下に図面
を参照して説明する。図1は本発明の一実施形態に係わ
る渦電流探傷子の構成を示す図である。図1(a)は渦
電流探傷子の断面図、図1(b)は図1(a)のA側か
らみた平面図、図1(c)は図1(a)のB側からみた
平面図である。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a diagram showing a configuration of an eddy current flaw detector according to one embodiment of the present invention. 1A is a cross-sectional view of the eddy current flaw detector, FIG. 1B is a plan view of FIG. 1A from the A side, and FIG. 1C is a plan view of FIG. 1A from the B side. FIG.

【0017】円形の円板状磁心部11上に中心磁心部1
2と内部円筒状磁心部13と外部円筒状磁極部14とが
同軸上に設置され、磁心材10を構成している。円板状
磁心部11,中心磁心部12,内部円筒状磁心部13及
び外部円筒状磁極部14は、磁界をよく通す強磁性体で
形成されている。
The center magnetic core 1 is placed on the circular disc-shaped magnetic core 11.
2, the inner cylindrical magnetic core 13 and the outer cylindrical magnetic pole 14 are coaxially arranged to form the magnetic core material 10. The disk-shaped magnetic core 11, the central magnetic core 12, the inner cylindrical magnetic core 13, and the outer cylindrical magnetic pole 14 are made of a ferromagnetic material that passes a magnetic field well.

【0018】内部円筒状磁心部13の外周に線材が巻き
付けられて励磁コイル20が構成されている。また、中
心磁心部12の外周に線材が巻き付けられて検出コイル
21が構成されている。励磁コイル20及び検出コイル
21を構成する線材の端は、円板状磁心部11に設けら
れた穴15から磁心材10の外部に取り出され、従来の
探傷子と同様にケーブルを介して探傷器(不図示)に接
続されている。
A wire is wound around the outer periphery of the inner cylindrical magnetic core 13 to form the exciting coil 20. The detection coil 21 is formed by winding a wire around the outer periphery of the center magnetic core portion 12. The ends of the wires constituting the excitation coil 20 and the detection coil 21 are taken out of the magnetic core material 10 from the holes 15 provided in the disc-shaped magnetic core portion 11 and are connected to the flaw detector through a cable in the same manner as a conventional flaw detector. (Not shown).

【0019】次に、本実施形態の動作について図2を用
いて説明する。励磁コイル20に、探傷器内の発振器か
ら一定の大きさ(振幅)、一定周波数の交流電流が供給
されることによって交流磁界を発生する。この場合、中
心磁心部12−外部空間(空気,被検体)−外部円筒状
磁極部14−円板状磁心部11−中心磁心部12を経由
する磁束による磁界(以下、中央磁界という)40と、
内部円筒状磁心部13−外部空間(空気,被検体)−外
部円筒状磁極部14−円板状磁心部11−内部円筒状磁
心部13を経由する磁束による磁界(以下、周辺磁界と
いう)41が形成される。ここで、中心磁心部12の内
部に生じる磁界は、中央磁界40とほぼ同じものであ
る。
Next, the operation of this embodiment will be described with reference to FIG. An alternating magnetic field is generated by supplying an alternating current of a constant magnitude (amplitude) and a constant frequency to the exciting coil 20 from an oscillator in the flaw detector. In this case, a magnetic field (hereinafter, referred to as a central magnetic field) 40 due to a magnetic flux passing through the central magnetic core portion 12-the outer space (air, the subject)-the external cylindrical magnetic pole portion 14-the disk-shaped magnetic core portion 11-the central magnetic core portion 12. ,
A magnetic field (hereinafter, referred to as a peripheral magnetic field) 41 due to magnetic flux passing through the inner cylindrical magnetic core 13-the outer space (air, the subject)-the outer cylindrical magnetic pole 14-the disk-shaped magnetic core 11-the inner cylindrical magnetic core 13. Is formed. Here, the magnetic field generated inside the central magnetic core 12 is substantially the same as the central magnetic field 40.

【0020】図2に示すように、中心磁心部12と被検
体30との間(以下、中央空間という)での中央磁界4
0と内部円筒状磁心部13と被検体30との空間(以
下、周辺空間という)での周辺磁界41とは、ほぼ同一
方向を向いている。同一方向の磁界は常に反発しあうの
で、中央空間での中央磁界40と周辺空間での周辺磁界
41とは、互いに反発しあう。従って、中央空間での中
央磁界40はより中央部へ集中し、周辺空間での周辺磁
界41はより外周部へ拡散する。
As shown in FIG. 2, a central magnetic field 4 between the central magnetic core 12 and the subject 30 (hereinafter, referred to as a central space).
The peripheral magnetic field 41 in the space between the zero, the inner cylindrical magnetic core portion 13 and the subject 30 (hereinafter referred to as the peripheral space) is oriented in substantially the same direction. Since the magnetic fields in the same direction always repel each other, the central magnetic field 40 in the central space and the peripheral magnetic field 41 in the peripheral space repel each other. Therefore, the central magnetic field 40 in the central space is more concentrated on the central portion, and the peripheral magnetic field 41 in the peripheral space is more diffused on the outer peripheral portion.

【0021】一方、中央磁界40によって被検体30に
渦電流が誘起される。この渦電流は、中心磁心部12の
下方に集中し、その密度が高くなるので、渦電流によっ
て誘起される磁界の大きさも大きくなる。そして、中央
磁界40によって誘起された渦電流が欠陥の存在によっ
て変化した場合、渦電流の変化は中央磁界40に影響を
与える。
On the other hand, an eddy current is induced in the subject 30 by the central magnetic field 40. The eddy current is concentrated below the central magnetic core portion 12 and its density increases, so that the magnitude of the magnetic field induced by the eddy current also increases. When the eddy current induced by the central magnetic field 40 changes due to the presence of a defect, the change in the eddy current affects the central magnetic field 40.

【0022】コイルを貫く磁束が時間的に変化する場合
にコイルに電圧が誘起されるが、本実施形態の探傷子の
検出コイル21は中心磁心部12に巻き線されているた
め、検出コイル21は中心磁心部12の内部の磁界変
化、つまり中央磁界40の変化を感知する。
When the magnetic flux passing through the coil changes with time, a voltage is induced in the coil. However, since the detection coil 21 of the flaw detector of this embodiment is wound around the central magnetic core 12, the detection coil 21 Detects a change in the magnetic field inside the central magnetic core 12, that is, a change in the central magnetic field 40.

【0023】被検体30に欠陥のない場合、渦電流は定
常状態にあり、渦電流による磁界は変化しないので、中
央磁界40に影響を与えない。そして、渦電流が欠陥の
存在によって変化した場合、渦電流による磁界が中央磁
界40に影響を与え、この中央磁界40の変化、つまり
中心磁心部12中の磁界変化によって検出コイル21に
誘起される電圧は変化する。そして、検出コイル21の
誘起電圧が探傷器によって信号処理されて、欠陥による
信号波形が探傷器の画面に表示され、探傷が可能とな
る。
When the object 30 has no defect, the eddy current is in a steady state and the magnetic field due to the eddy current does not change, so that the central magnetic field 40 is not affected. When the eddy current changes due to the presence of a defect, the magnetic field due to the eddy current affects the central magnetic field 40, and the change in the central magnetic field 40, that is, the magnetic field change in the central magnetic core 12, induces the detection coil 21. The voltage changes. Then, the induced voltage of the detection coil 21 is signal-processed by the flaw detector, a signal waveform due to the defect is displayed on the screen of the flaw detector, and flaw detection becomes possible.

【0024】このように、本実施形態の渦電流探傷子に
よれば、被検体30に生じる渦電流は中心磁心部12の
下方の中心部に集中することにより、渦電流により発生
する磁界が大きくなり、かつこの渦電流による磁界は中
央磁界40、つまり検出コイル21が巻かれた中心磁心
部12の内部磁界にのみ集中的に影響を与えるので、大
きい欠陥だけでなく、小さい欠陥も感度よく感知するこ
とができる。
As described above, according to the eddy current flaw detector of the present embodiment, the eddy current generated in the subject 30 is concentrated in the central portion below the central magnetic core portion 12, so that the magnetic field generated by the eddy current is large. In addition, since the magnetic field due to the eddy current intensively affects only the central magnetic field 40, that is, the internal magnetic field of the center core portion 12 around which the detection coil 21 is wound, not only large defects but also small defects can be detected with high sensitivity. can do.

【0025】従って、次のステップで必要な修理等を正
確に行うことができ、修理期間の短縮、ひいては各種機
器の耐用年数が増大することになる。被検体に欠陥が存
在したときの信号波形を図3に示す。図3(a)は欠陥
が大きいときの信号波形で、図3(b)は欠陥が小さい
ときの信号波形である。図から分かるように、小さい欠
陥の波形52も大きい欠陥の波形51と同様な振幅波形
が得られている。
Therefore, necessary repairs and the like can be accurately performed in the next step, so that the repair period is shortened, and the service life of various devices is increased. FIG. 3 shows a signal waveform when a defect exists in the subject. FIG. 3A shows a signal waveform when the defect is large, and FIG. 3B shows a signal waveform when the defect is small. As can be seen from the figure, the waveform 52 of the small defect has the same amplitude waveform as the waveform 51 of the large defect.

【0026】本発明は上記実施形態に限定されるもので
はない。例えば、上記実施形態では平板形状の被検体に
ついて述べたが、被検体の形は平板に限られるものでは
なく、パイプ形状,管形状,棒状など種々の被検体に適
用することができる。
The present invention is not limited to the above embodiment. For example, in the above-described embodiment, a flat-shaped object has been described. However, the shape of the object is not limited to a flat plate, and the present invention can be applied to various objects such as a pipe, a tube, and a rod.

【0027】また、磁心材は、円板状磁心部,中心磁心
部,内部円筒状磁心部,外部円筒状磁極部を一体成形し
たものでもよいし、こられの部材を別々に形成して接合
したものでもよい。
The magnetic core material may be formed by integrally molding a disc-shaped magnetic core, a central magnetic core, an inner cylindrical magnetic core, and an outer cylindrical magnetic pole, or these members may be formed separately and joined. May be done.

【0028】また、中心磁心部は棒状に限らず、細い円
筒状のものであってもよい。その他、本発明はその要旨
を逸脱しない範囲で、種々変形して実施することが可能
である。
The center magnetic core is not limited to the rod shape, but may be a thin cylindrical shape. In addition, the present invention can be variously modified and implemented without departing from the gist thereof.

【0029】[0029]

【発明の効果】以上説明したように本発明の渦電流探傷
子によれば、円板状磁心部上に中心磁心部,内部円筒状
磁心部,外部円筒状磁極部を同軸的に設けて強磁性体か
らなる磁心材を形成し、内部円筒状磁心部の外周に励磁
コイル、中心磁心部の外周に検出コイルをそれぞれ設け
ることにより、被検体に生じる渦電流を中心部に集中さ
せ、かつ渦電流による磁界の変化を効率的に検出するこ
とが可能となり、、大きい欠陥だけでなく、小さい欠陥
も感度よく感知することができる。
As described above, according to the eddy current flaw detector of the present invention, the center magnetic core, the inner cylindrical magnetic core, and the outer cylindrical magnetic pole are coaxially provided on the disk-shaped magnetic core. By forming a magnetic core material made of a magnetic material and providing an excitation coil on the outer periphery of the inner cylindrical magnetic core and a detection coil on the outer periphery of the center core, eddy currents generated in the subject are concentrated at the center and It is possible to efficiently detect the change in the magnetic field due to the current, and it is possible to detect not only a large defect but also a small defect with high sensitivity.

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

【図1】本発明の一実施形態に係わる渦電流探傷子の構
成を示す図。
FIG. 1 is a diagram showing a configuration of an eddy current flaw detector according to one embodiment of the present invention.

【図2】図1の渦電流探傷子の発生する磁界の様子を示
す図。
FIG. 2 is a diagram showing a state of a magnetic field generated by the eddy current flaw detector of FIG. 1;

【図3】図1の渦電流探傷子を用いた場合の表示波形を
示す図。
FIG. 3 is a view showing a display waveform when the eddy current flaw detector of FIG. 1 is used.

【図4】従来の渦電流探傷装置の構成を示す図。FIG. 4 is a diagram showing a configuration of a conventional eddy current flaw detector.

【図5】探傷子の電磁気的な作用を示す図。FIG. 5 is a diagram showing an electromagnetic action of the flaw detector.

【図6】従来の探傷子の磁界の様子を説明する図FIG. 6 is a diagram illustrating a state of a magnetic field of a conventional flaw detector.

【図7】従来の探傷子による表示波形例を示す図。FIG. 7 is a diagram showing an example of a display waveform by a conventional flaw detector.

【符号の説明】[Explanation of symbols]

10 磁心材 11 円板状磁心部 12 中心磁心部 13 内部円筒状磁心部 14 外部円筒状磁極部 15 コイル巻線を通す穴 20 励磁コイル 21 検出コイル 30 被検体 40 中央磁界 41 周辺磁界 DESCRIPTION OF SYMBOLS 10 Magnetic core material 11 Disc-shaped magnetic core part 12 Center magnetic core part 13 Inner cylindrical magnetic core part 14 External cylindrical magnetic pole part 15 Hole through which a coil winding 20 Excitation coil 21 Detector coil 30 Subject 40 Central magnetic field 41 Peripheral magnetic field

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭61−137057(JP,A) 特開 平5−10924(JP,A) 特開 平8−211025(JP,A) 特開 平7−286992(JP,A) (58)調査した分野(Int.Cl.7,DB名) G01N 27/72 - 27/90 G01R 33/00 - 33/18 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-61-137057 (JP, A) JP-A-5-10924 (JP, A) JP-A-8-211025 (JP, A) JP-A-7-107 286992 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) G01N 27/72-27/90 G01R 33/00-33/18

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】強磁性体から形成され、円板状磁心部上に
中心磁心部,内部円筒状磁心部,外部円筒状磁極部を同
軸的に設けてなる磁心材と、 前記内部円筒状磁心部の外周に設けられ、被検体に渦電
流を誘起させるための励磁コイルと、 前記中心磁心部の外周に設けられ、前記被検体に誘起さ
れた渦電流の変化を検出する検出コイルとを具備してな
ることを特徴とする渦電流探傷子。
1. A core material formed of a ferromagnetic material and having a center core, an inner cylindrical core, and an outer cylindrical magnetic pole coaxially provided on a disk-shaped core, and the inner cylindrical core. An excitation coil provided on the outer periphery of the portion for inducing an eddy current in the subject; and a detection coil provided on the outer periphery of the center core portion and detecting a change in the eddy current induced in the subject. An eddy current flaw detector characterized by the following.
JP32038396A 1996-11-29 1996-11-29 Eddy current detector Expired - Fee Related JP3268219B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32038396A JP3268219B2 (en) 1996-11-29 1996-11-29 Eddy current detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32038396A JP3268219B2 (en) 1996-11-29 1996-11-29 Eddy current detector

Publications (2)

Publication Number Publication Date
JPH10160709A JPH10160709A (en) 1998-06-19
JP3268219B2 true JP3268219B2 (en) 2002-03-25

Family

ID=18120867

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32038396A Expired - Fee Related JP3268219B2 (en) 1996-11-29 1996-11-29 Eddy current detector

Country Status (1)

Country Link
JP (1) JP3268219B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005148049A (en) * 2003-10-23 2005-06-09 Yokohama Rubber Co Ltd:The Method and device for detecting foreign matter in tire, tire inspection device, tire molding machine, and tire uniformity machine
JP2008032575A (en) * 2006-07-29 2008-02-14 Nippon Hihakai Kensa Kk Eddy current measuring probe and flaw detection device using it
JP5259511B2 (en) * 2008-07-09 2013-08-07 株式会社東芝 Remote field eddy current testing probe

Also Published As

Publication number Publication date
JPH10160709A (en) 1998-06-19

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