JPS60243559A - Flaw-detecting magnetic sensor - Google Patents

Flaw-detecting magnetic sensor

Info

Publication number
JPS60243559A
JPS60243559A JP9941084A JP9941084A JPS60243559A JP S60243559 A JPS60243559 A JP S60243559A JP 9941084 A JP9941084 A JP 9941084A JP 9941084 A JP9941084 A JP 9941084A JP S60243559 A JPS60243559 A JP S60243559A
Authority
JP
Japan
Prior art keywords
rope
detecting
flaw
fluxes
magnetic
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.)
Pending
Application number
JP9941084A
Other languages
Japanese (ja)
Inventor
Mitsugi Abe
阿部 貢
Shinichi Kamewaka
亀若 真一
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.)
IHI Corp
Macome Corp
Original Assignee
IHI Corp
Macome Corp
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 IHI Corp, Macome Corp filed Critical IHI Corp
Priority to JP9941084A priority Critical patent/JPS60243559A/en
Publication of JPS60243559A publication Critical patent/JPS60243559A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N27/00Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
    • G01N27/72Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating magnetic variables
    • G01N27/82Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating magnetic variables for investigating the presence of flaws

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  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Electrochemistry (AREA)
  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Measuring Magnetic Variables (AREA)
  • Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)

Abstract

PURPOSE:To enable continuous and extensive-range detection, by using a linear detecting element. CONSTITUTION:A flaw-detecting apparatus is composed of a permanent magnet 17 for magnetizing a wire rope 16 up to a point nearly of saturation, a detecting head 18 including a detecting element detecting leakage magnetic fluxes from the wire rope and an output circuit, etc., and a magnetic field is constructed with magnet 17, yoke 19 and rope 16. The head 18 is composed of detecting elements 3a, 4a in a ring shape encircling concentrically the rope 16. If a strand constructing the rope 16 is accompanied with break, scar, etc., these flaws change the magnetic permeability of the location, generating leakage magnetic fluxes and the field is displaced with the rope 16 in the x direction. When the elenent 3a detects the fluxes 20, a positive voltage signal is generated on the output end of the circuit and when the element 4a detects them, a negative voltage signal is generated and thus, a discrepancy is detected on the rope. Further, as the elements 3a, 4a encircle the rope 16, noise produced by the leakage fluxes by the twisted construction of the rope and vibration of the rope is uniformalized in the output circuit without propagating to the outside. Thus, easy detection of flaw becomes available.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、ワイヤロープ、鋼板、などの内部欠陥を磁気
探傷するのに有用な探傷用磁気センサに関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magnetic sensor for flaw detection useful for magnetically detecting internal defects in wire ropes, steel plates, and the like.

〔従来の技術〕[Conventional technology]

探傷用センサは、一般に線状または面状に分布する2次
元磁界の変化を検出できる機能が要求されている。しか
し、従来の磁気センサは第11図に示すごとく点状であ
り狭い範囲の磁界(A)を検出するセンサのみが実用化
されているため、探傷の際はこれらの点状センサを複数
個組み合せて使用しなければならなかった。しかし。
Flaw detection sensors are generally required to have the ability to detect changes in a two-dimensional magnetic field distributed linearly or planarly. However, conventional magnetic sensors are point-shaped as shown in Figure 11, and only sensors that detect magnetic fields (A) in a narrow range have been put into practical use. Therefore, when performing flaw detection, it is necessary to combine multiple of these point-shaped sensors. I had to use it. but.

このようにすると各センサの性能の不揃いなどによシ充
分な精度が得られなかったり、制御部の構造が複雑にな
り、探傷装置の価格が高価になる欠点があった。
If this is done, sufficient accuracy may not be obtained due to uneven performance of each sensor, the structure of the control section becomes complicated, and the flaw detection apparatus becomes expensive.

なお、第11図に示す従来のセンサについて説明すると
、符号(α)はコア、(b)は高周波電源。
In addition, to explain the conventional sensor shown in FIG. 11, the code (α) is the core, and (b) is the high frequency power source.

(1)はダイオード(d)、コンデンサ(1)、抵抗q
)などからなるバランス形の出力回路である。コア(α
)を容易に飽和状態まで励磁し且つ漏れ磁束をできるた
け小さくするため、コア(、)はできるたけ小型に且つ
薄形に、さらに閉じた磁路を構成するようにつくられる
。従って外部磁界(g)の検出範囲はもっばらコア(a
)周辺の極く小さい空間(h)(破線で示す)に限定さ
れる。
(1) is a diode (d), a capacitor (1), and a resistor q
), etc., is a balanced output circuit. Core (α
) is made to be as small and thin as possible, and to form a closed magnetic path, in order to easily excite the core (, ) to a saturated state and to minimize leakage flux. Therefore, the detection range of the external magnetic field (g) is mostly the core (a
) is limited to a very small space (h) (indicated by a dashed line) around it.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

本発明は、前述の欠点に鑑み、巌または面状の2次元外
部磁界の磁束変化を検出し得る探傷用磁気センサを提供
する、こ、とにある・〔問題点を解決するための手段〕 上記問題点を解決し得る本発明の探傷用磁気センサは、
磁性体でつくった線状のコアに巻線を施した複数の検出
素子と、前記巻線に高周波電流を供給する高周波電源装
置と、各検出素子・が検出した磁束変化を電圧変化とし
て出力する電気回路とを撫えたものであシ、a状の検出
素子を用いて外部磁界の磁束変化を一度に検出すること
ができるだめ検出精度が高く、かつ、検出素子の数が大
巾に削減されるので、装置を小型軽量に構成できるなど
の利点を肩するものである。
In view of the above-mentioned drawbacks, the present invention is to provide a magnetic sensor for flaw detection capable of detecting magnetic flux changes in a two-dimensional external magnetic field in the form of a rock or a planar shape. [Means for solving the problems] The magnetic sensor for flaw detection of the present invention that can solve the above problems is as follows:
A plurality of detection elements each having a wire wound around a linear core made of a magnetic material, a high frequency power supply device that supplies a high frequency current to the windings, and each detection element outputs the magnetic flux change detected as a voltage change. It is a combination of electric circuits and can detect changes in the magnetic flux of an external magnetic field at once using a-shaped detection elements, resulting in high detection accuracy and a significant reduction in the number of detection elements. Therefore, it has the advantage that the device can be made smaller and lighter.

〔実 施 例〕〔Example〕

以下1本発明の実施例を図面を参照して説明する。第1
図ないし第10図は本発明の一実施例である磁気センサ
の構成、作動説明図、磁気センサを適用したワイヤロー
プ探傷装置を示すもので5本発明の磁気センサは1強磁
性体(例えばパーマロイ線)でつくった細い(直径01
〜0、.5myI)線状のコア(1)の直径が70μm
の巻a (2)を直接一層巻してつくった2個の検出素
子(3) (4)と、−各巻線(2) (2)に約IM
Hzの高周波電流を供給してコアを飽和状態まで励磁す
る高周波電源装置(5)と、各検出素子(3) (4)
が検出した磁束変化を正、負の電圧変化として出力端(
6) ’(7)に出力するバランス式出力回路(8)な
どかちなる。出力回路(8)は図示のごとく抵抗R+%
R2,R3、R4およびコンデンサC1,C2、C3・
ダイオードDI−D2などからなり、外部状況(温度変
化、地磁気の影響など)によって左右されないバランス
機能を有している。
An embodiment of the present invention will be described below with reference to the drawings. 1st
Figures 1 to 10 show the structure, operation explanatory diagram, and wire rope flaw detection device to which the magnetic sensor is applied, which is an embodiment of the present invention. A thin (diameter 01
~0,. 5myI) The diameter of the linear core (1) is 70 μm
Two sensing elements (3) (4) are made by directly winding the winding a (2) in one layer, and - each winding (2) (2) has approximately IM
A high frequency power supply device (5) that supplies a high frequency current of Hz to excite the core to a saturated state, and each detection element (3) (4)
The magnetic flux change detected by the output terminal (
6) It consists of a balanced output circuit (8) which outputs to (7). The output circuit (8) has a resistance R+% as shown in the diagram.
R2, R3, R4 and capacitors C1, C2, C3・
It consists of a diode DI-D2, etc., and has a balance function that is not affected by external conditions (temperature changes, geomagnetic influences, etc.).

次に磁気センサの作動について説明するに、捷ず、コア
(1) (1)を高周波電源装置(5)からの高周波電
流によって励磁すると、磁気表皮効果により最大透磁率
約7000において約5μmというスキンデプス(5k
indepth )となり、コア(1)の極く表面だけ
が励磁され飽和状態になる・従ってコア(1)は数百能
の長い線、あるいは比較的直径の大きい丸棒であっても
コア(1)の表面付近は十分に飽和状態に達する。
Next, to explain the operation of the magnetic sensor, when the core (1) (1) is excited by a high-frequency current from the high-frequency power supply (5) without being separated, a skin with a maximum magnetic permeability of about 7000 and a thickness of about 5 μm due to the magnetic skin effect. Depth (5k
depth ), and only the very surface of the core (1) is excited and becomes saturated. Therefore, even if the core (1) is a long wire of several hundred wires or a round bar with a relatively large diameter, the core (1) reaches a saturation state near the surface.

次に、各巻線(2)のインダクタンス(L)は、(1)
式で表わされる。
Next, the inductance (L) of each winding (2) is (1)
It is expressed by the formula.

L−弁一丑・A(1)式 ここに、Lは自己誘導係数、Φは磁束、Bは磁束密度、
Aはコア(1)の断面積であり、外部磁界が存在しない
ときのコア(1)の磁束密度Bと磁界Hの関係は、第2
図に示すように巻a(2)による励磁磁界(9)によっ
て飽和状態になっており、磁界(9)による磁束密度の
変化は00で示される(破線参照)。この状態において
外部磁界(坦がコア(1)に作用すると、巻線(2)が
発生した励磁磁界(9)による磁束密度の変化(ハ)は
式(1)に従って小さくなる(第6図参照)。この結果
、インダクタンスLの変化を出力回路(8)の電圧変化
として取り出すことができる。従って第1図に示す検出
素子(4)にのみ第4図に示すように外部磁界S、Nが
加わったときの出力電圧■は第5図で示される。また検
出素子(3) (4)を2個用い、差動的に働(ように
1.た本発明の′mαセンサの出力は、検出素子(3)
 (4)に平行に同じように加えられる外部磁界に対し
て出力変化を生じないが、差動的に作用する出力は第6
図に示すように電圧変化として外部に取シ出される。な
お、図中2は外部磁界a均の移動方向を示す。
L-Valve Ichigo・A (1) formula where L is the self-induction coefficient, Φ is the magnetic flux, B is the magnetic flux density,
A is the cross-sectional area of the core (1), and the relationship between the magnetic flux density B of the core (1) and the magnetic field H when there is no external magnetic field is the second
As shown in the figure, it is saturated by the excitation magnetic field (9) from winding a (2), and the change in magnetic flux density due to the magnetic field (9) is indicated by 00 (see the broken line). In this state, when an external magnetic field (field) acts on the core (1), the change in magnetic flux density (c) due to the excitation magnetic field (9) generated by the winding (2) decreases according to equation (1) (see Figure 6). ).As a result, the change in inductance L can be extracted as a voltage change in the output circuit (8).Therefore, as shown in FIG. 4, the external magnetic fields S and N are applied only to the detection element (4) shown in FIG. The output voltage ■ when applied is shown in Figure 5.The output of the 'mα sensor of the present invention using two detection elements (3) and (4) and working differentially (1. Detection element (3)
There is no output change in response to an external magnetic field applied in parallel to (4), but the output that acts differentially is the 6th
As shown in the figure, it is taken out to the outside as a voltage change. Note that 2 in the figure indicates the direction of movement of the external magnetic field a.

第7図ないし第10図に本装置を応用したワイヤロープ
探傷装置の実施例および作動説明図を示す。探傷装置は
ワイヤロープ06を飽和点近くまで磁化させるだめの永
久磁石(171とワイヤロープOejからの漏れ磁束を
検出する検出素子を含む検出ヘッド08)と図示しない
出力回路なとからなり、永久磁石α力とヨーク0つとワ
イヤロープ(4)が磁路を構成する・検出ヘッド(ト)
はワイヤロープα0を同心に取り囲むリング状の検出素
子(3α)(軸)からなり(第9図参照)、出方回路は
第1図に示すものと同様である。
FIGS. 7 to 10 show an embodiment of a wire rope flaw detection device to which the present device is applied and explanatory diagrams of its operation. The flaw detection device consists of a permanent magnet (171 and a detection head 08 including a detection element that detects leakage magnetic flux from the wire rope Oej) that magnetizes the wire rope 06 to near the saturation point, and an output circuit (not shown). α force, 0 yokes, and wire rope (4) constitute a magnetic path ・Detection head (G)
consists of a ring-shaped detection element (3α) (shaft) concentrically surrounding the wire rope α0 (see FIG. 9), and the output circuit is the same as that shown in FIG.

ワイヤロープaOを構成する素線に断線、傷、疲労など
が発生すると、この部分の透磁率が変わり、漏れ磁束−
が発生し、ロープと共にX方向に移動する(矢印k)0
 この漏れ磁束−を検出素子(6α)が検出すると回路
の出力端に正の電圧信号を、また検出素子(4α)が検
出すると負の電圧信号を発生しく第10図参照)、ワイ
ヤロープQ峰の欠陥が検出される。また、検出素子(3
G)(4α)がワイヤロープQQを取シ囲んでいるので
、ロープの撚り構造による漏れ磁束およびワイヤロープ
OQの振動によるノイズは出力回路(8)内で平均化さ
れ、外部に現われることがない。従って欠陥の存在を容
易に検出することができる。
When wires constituting the wire rope aO are broken, scratched, fatigued, etc., the magnetic permeability of this part changes, causing leakage magnetic flux -
occurs and moves in the X direction with the rope (arrow k) 0
When the detection element (6α) detects this leakage magnetic flux, a positive voltage signal is generated at the output end of the circuit, and when the detection element (4α) detects this leakage magnetic flux, a negative voltage signal is generated. defects are detected. In addition, the detection element (3
G) (4α) surrounds the wire rope QQ, so leakage magnetic flux due to the twisted structure of the rope and noise due to vibration of the wire rope OQ are averaged within the output circuit (8) and do not appear externally. . Therefore, the presence of defects can be easily detected.

なお、本発明は前述の実施例にのみ限定されるものでは
なく、本発明の要旨を逸脱しない範囲において種々の変
更を加え得ることは勿論である。
It should be noted that the present invention is not limited only to the above-described embodiments, and it goes without saying that various changes can be made without departing from the gist of the present invention.

〔発明の効果〕〔Effect of the invention〕

以上述べたごとく本発明の探傷用磁気センサは線状検出
素子を用いるので1次の優れた効果を発揮する。
As described above, since the magnetic sensor for flaw detection of the present invention uses a linear detection element, it exhibits an excellent first-order effect.

(1)線状および面状に拡がる磁界の変動を検出できる
(1) Fluctuations in magnetic fields that spread linearly and planarly can be detected.

(11)検出素子に可撓性を持たせることができるため
検出すべき外部磁界の形状に適合した検出ヘッドを構成
することができる。
(11) Since the detection element can be made flexible, it is possible to configure a detection head that matches the shape of the external magnetic field to be detected.

(iiD 従来のように点状の検出素子を複数個組み合
わせて使用せずに、連続して広範囲の検出をすることが
できる・ 翰 第(110項の結果、連続した広範囲の磁束分布を
平均化して検出することができるためシ公比が向上し、
検出結果の判別が容易となり。
(iiD) It is possible to continuously detect a wide range without using a combination of multiple dot-shaped detection elements as in the past. Since it is possible to detect the
Detection results can be easily distinguished.

熟練者に頼る必要がない。No need to rely on experts.

(V) 差動型二次元磁気センサであり、バランス回路
機能により外部状況(温度変化、地磁気の影響)に左右
されない。
(V) It is a differential two-dimensional magnetic sensor, and its balance circuit function makes it unaffected by external conditions (temperature changes, geomagnetic influences).

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

第1図ないし第6図は本発明の実施例および作動原理の
説明図で、第1図は装置の構成を示す結線図、第2図は
外部磁界がない場合のコアのB −H曲線、第6図は外
部磁界が加わった場合のコアのB−H曲線、第4図は一
方の検出素子に作用する外部磁界の分布状況の説明図、
第5図は第4図の状態における励磁磁界と出力電圧の関
係を示す図、第6図は両方の検出素□子に移動する外部
磁界が加わった際の出力電圧を示す図、第7図ないし第
10図は本装置をワイヤロープ探傷に適用した場合の実
施例を示し、第7図は磁化部の切断側面図、第8図は第
7図における■−■方向からの切断側面図、第9図は検
出素子の配置を示す斜視図、第10図はロープ移動方向
と出力電圧の関係を示す図、第11図は従来の磁気セン
サの説明図である。 図中、(1)はコア、(2)は巻線、(3H3α) (
4) (4α)は検出素子、(5)は高周波電源装置、
(8)は出力回路である。 特許出願人 石川島播磨重工業株式会社 特許出願人 株式会社 マコメ研究所 第1図 第2図 第3図 日
1 to 6 are explanatory diagrams of embodiments and operating principles of the present invention, FIG. 1 is a wiring diagram showing the configuration of the device, and FIG. 2 is a B-H curve of the core in the absence of an external magnetic field. Fig. 6 is a B-H curve of the core when an external magnetic field is applied, Fig. 4 is an explanatory diagram of the distribution of the external magnetic field acting on one detection element,
Figure 5 shows the relationship between the excitation magnetic field and the output voltage in the state shown in Figure 4, Figure 6 shows the output voltage when a moving external magnetic field is applied to both sensing elements, and Figure 7 10 to 10 show an embodiment in which this device is applied to wire rope flaw detection, FIG. 7 is a cut side view of the magnetized part, FIG. 8 is a cut side view taken from the ■-■ direction in FIG. 7, FIG. 9 is a perspective view showing the arrangement of detection elements, FIG. 10 is a diagram showing the relationship between the rope moving direction and the output voltage, and FIG. 11 is an explanatory diagram of a conventional magnetic sensor. In the figure, (1) is the core, (2) is the winding, (3H3α) (
4) (4α) is a detection element, (5) is a high frequency power supply device,
(8) is an output circuit. Patent applicant: Ishikawajima-Harima Heavy Industries Co., Ltd. Patent applicant: Makome Research Institute Figure 1 Figure 2 Figure 3 Date

Claims (1)

【特許請求の範囲】[Claims] 旬 磁性体でつくった線状のコアに巻線を施した複数の
検出素子と、前記巻線に高周波電流を供給する高周波電
源装置と、各検出素子が検出した磁束変化を電圧変化と
して出力する電気回路とを備えたことを特徴とする探傷
用磁気センサ。
A plurality of detection elements each having a wire wound around a linear core made of a magnetic material, a high frequency power supply device that supplies high frequency current to the windings, and a magnetic flux change detected by each detection element outputting as a voltage change. A magnetic sensor for flaw detection characterized by being equipped with an electric circuit.
JP9941084A 1984-05-17 1984-05-17 Flaw-detecting magnetic sensor Pending JPS60243559A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9941084A JPS60243559A (en) 1984-05-17 1984-05-17 Flaw-detecting magnetic sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9941084A JPS60243559A (en) 1984-05-17 1984-05-17 Flaw-detecting magnetic sensor

Publications (1)

Publication Number Publication Date
JPS60243559A true JPS60243559A (en) 1985-12-03

Family

ID=14246708

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9941084A Pending JPS60243559A (en) 1984-05-17 1984-05-17 Flaw-detecting magnetic sensor

Country Status (1)

Country Link
JP (1) JPS60243559A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6472052A (en) * 1987-09-14 1989-03-16 Toshiba Shokoki Service Flaw detector for steel tape of elevator
JPH02128945U (en) * 1989-03-30 1990-10-24

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6472052A (en) * 1987-09-14 1989-03-16 Toshiba Shokoki Service Flaw detector for steel tape of elevator
JPH02128945U (en) * 1989-03-30 1990-10-24

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