JPH0194280A - Magnetic sensor for detecting magnetic material - Google Patents

Magnetic sensor for detecting magnetic material

Info

Publication number
JPH0194280A
JPH0194280A JP62252245A JP25224587A JPH0194280A JP H0194280 A JPH0194280 A JP H0194280A JP 62252245 A JP62252245 A JP 62252245A JP 25224587 A JP25224587 A JP 25224587A JP H0194280 A JPH0194280 A JP H0194280A
Authority
JP
Japan
Prior art keywords
magnetic material
coil
frequency
voltage
curve
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
JP62252245A
Other languages
Japanese (ja)
Inventor
Akio Ito
伊藤 昭雄
Takahiro Tsuchiya
貴宏 土屋
Toru Ishii
透 石井
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.)
Mitsui Petrochemical Industries Ltd
NEC Ameniplantex Ltd
Original Assignee
Mitsui Petrochemical Industries Ltd
NEC Ameniplantex 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 Mitsui Petrochemical Industries Ltd, NEC Ameniplantex Ltd filed Critical Mitsui Petrochemical Industries Ltd
Priority to JP62252245A priority Critical patent/JPH0194280A/en
Publication of JPH0194280A publication Critical patent/JPH0194280A/en
Pending legal-status Critical Current

Links

Landscapes

  • Measuring Magnetic Variables (AREA)
  • Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)
  • Geophysics And Detection Of Objects (AREA)

Abstract

PURPOSE:To dispense with the adjustment of a coil interval, to facilitate preparation and to stabilize a detection sensitivity temp. characteristic, by providing a resonance circuit, an oscillator and an voltage detection part. CONSTITUTION:A resonance circuit wherein a coil 1 of a single winding empty core and a resonance frequency adjusting condenser 3 are connected in parallel is connected to the wiring of an oscillator 5 containing a current control resistor 2 and a voltage detector 6 detects the voltage between the terminal of the coil 1 and that of the condenser 3. A curve A shows the frequency characteristic of a magnetic sensor when a magnetic material 4 is absent within a detection distance range and the resonance frequency thereof is f0. A curve B shows a characteristic when the magnetic material 4 enters the detection distance range of the sensor and the resonance frequency f0' at that time becomes lower than f0. A curve C shows a frequency characteristic when iron being a soft magnetic material similar to the magnetic material 4 enters the detection distance range and the resonance f0'' at that time becomes higher than f0. Further, the voltage level of the whole of the curve C is lowered. By utilizing the frequency characteristic changing as mentioned above, the magnetic material and the soft magnetic material can be discriminated.

Description

【発明の詳細な説明】 [産業上の利用分野〕 本発明は磁性材料検知磁気センサ、特に単巻コイルを用
いて励磁及び検知を同一コイル上により行う磁性材料検
知磁気センサに関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magnetic material detection magnetic sensor, and particularly to a magnetic material detection magnetic sensor that uses a single-turn coil and performs excitation and detection on the same coil.

〔従来の技術〕[Conventional technology]

磁性材料を検知する磁気センサには各種の方式が発表さ
れているが、いずれの磁気センサも励磁コイルと検知コ
イルとを別個に装備し、励磁コイルから送信される交流
磁界の乱れを検知コイルに検知させ、これを電気信号に
変換する点で共通している。
Various methods have been announced for magnetic sensors that detect magnetic materials, but all magnetic sensors are equipped with separate excitation coils and detection coils, and the disturbances in the alternating current magnetic field transmitted from the excitation coil are sent to the detection coil. What they have in common is that they detect the signal and convert it into an electrical signal.

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

ところで、この種磁気センサでは励磁コイルと検知コイ
ルとの2つのコイルを別個に装備するものであるため、
磁性材料が磁気センサに近づいたときには、励磁コイル
と検知コイルとの相互作用により磁場の乱れが生じると
いう問題がある。
By the way, since this type of magnetic sensor is equipped with two separate coils, an excitation coil and a detection coil,
When a magnetic material approaches a magnetic sensor, there is a problem in that the interaction between the excitation coil and the detection coil causes disturbance of the magnetic field.

したがって、この影響をなくすためには励磁コイルに大
電力を供給する必要がある。また、このような磁気セン
サを製作するに際し、特に励磁コイルと検知コイルとの
間隔の変化が原因となって感度、温度特性のばらつきが
生じ、励磁コイルと検知コイルとの間隔を微妙に調整す
る必要がある。
Therefore, in order to eliminate this effect, it is necessary to supply a large amount of power to the excitation coil. In addition, when manufacturing such magnetic sensors, variations in sensitivity and temperature characteristics occur due to changes in the spacing between the excitation coil and the detection coil, so it is necessary to delicately adjust the spacing between the excitation coil and the detection coil. There is a need.

しかし、如何に微妙に調整したとしても同一ロット上で
の検知特性のばらつきをなくすことは到底できない。
However, no matter how delicately the adjustment is made, it is impossible to eliminate variations in detection characteristics within the same lot.

本発明の目的は上記の問題点を解消するもので停電力、
同一特性の磁性体検知磁気センサを提供することにある
The purpose of the present invention is to solve the above-mentioned problems.
It is an object of the present invention to provide a magnetic substance detection magnetic sensor having the same characteristics.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は周波数f。を共振周波数とする単巻空芯コイル
を含む共振回路と、励磁周波数f□(fl<f、)を前
記共振回路に印加する発振器と、前記共振回路の端子間
電圧レベルを測定する電圧検出部とを有することを特徴
とする磁性材料検知磁気センサである。
The present invention uses frequency f. a resonant circuit including a single-turn air-core coil having a resonant frequency of , an oscillator that applies an excitation frequency f□ (fl<f,) to the resonant circuit, and a voltage detection unit that measures the voltage level between terminals of the resonant circuit. A magnetic material detection magnetic sensor is characterized by having the following features.

〔原理・作用〕[Principle/effect]

本発明は基本的に磁気センサに用いる1つのコイルの漏
洩磁場に磁性材料が接近したとき、コイルのインダクタ
ンスLが変化を起こすことを利用したものである。
The present invention basically utilizes the fact that when a magnetic material approaches the leakage magnetic field of one coil used in a magnetic sensor, the inductance L of the coil changes.

コイルのインダクタンスLは次式で与えられる。The inductance L of the coil is given by the following equation.

μ:透磁率 N:コイル巻数 A:コイル断面積 Q:磁路長 磁性材料がコイルに接近することによりコイルのμが変
化する。また、コイルのLはその断面積にも比例する。
μ: Magnetic permeability N: Number of coil turns A: Coil cross-sectional area Q: Magnetic path length μ of the coil changes as the magnetic material approaches the coil. Further, L of the coil is also proportional to its cross-sectional area.

この点を利用してコイル断面積を調整することによりセ
ンサの検知感度を調整することも可能となる。
Utilizing this point, it is also possible to adjust the detection sensitivity of the sensor by adjusting the cross-sectional area of the coil.

〔実施例〕〔Example〕

以下に本発明の実施例を図によって説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図に本発明センサの回路図を示す。図において、電
流制御抵抗2を含む発振器5の配線に1本の単巻空芯の
コイル1と共振周波数調整用コンデンサ3とを並列に結
線した共振回路を接続したものである。6はコイル1と
コンデンサ3との端子間電圧を検出する電圧検出器であ
る。
FIG. 1 shows a circuit diagram of the sensor of the present invention. In the figure, a resonant circuit in which a single-turn air-core coil 1 and a resonant frequency adjustment capacitor 3 are connected in parallel is connected to the wiring of an oscillator 5 including a current control resistor 2. A voltage detector 6 detects the voltage between the terminals of the coil 1 and the capacitor 3.

本発明において、コイル1は励磁コイルと磁性材料の検
知コイルとを兼ねるものである。
In the present invention, the coil 1 serves both as an excitation coil and as a detection coil made of magnetic material.

コイル1の漏洩磁場に磁性材料4が接近したとき、その
インダクタンスが変化する。
When the magnetic material 4 approaches the leakage magnetic field of the coil 1, its inductance changes.

第2図において、曲線Aは磁性材料4が検知距離範囲内
にないときの磁気センサの周波数特性を示す。同図から
明らかなようにその共振周波数はfoである。曲線Bは
磁性材料4がセンサの検知距離範囲内に入ったときの特
性である。
In FIG. 2, curve A shows the frequency characteristic of the magnetic sensor when the magnetic material 4 is not within the detection distance range. As is clear from the figure, its resonant frequency is fo. Curve B is the characteristic when the magnetic material 4 is within the detection distance range of the sensor.

=3− 明らかなように、そのときの共振周波数f。′はfoよ
り低下する。磁性材料4がセンサにより接近すると共振
周波数はさらに下がるが、それぞれの共振周波数でのレ
ベルは、曲線A、Bから分かるようにあまり変化しない
。一方磁性材料4と同様な軟磁性材料である鉄が検知距
離範囲内に入ったときの周波数特性を曲線Cで示す。軟
磁性材料では磁性材料を検知したときとは異なり、その
ときの共振周波数f。′はfoより上昇する。しかも曲
線C全体の電圧レベルは低下している。これは鉄により
渦電流損失が起きるためと考えられる。
=3- As is clear, the resonance frequency f at that time. ' is lower than fo. As the magnetic material 4 moves closer to the sensor, the resonant frequency drops further, but the level at each resonant frequency does not change much, as can be seen from curves A and B. On the other hand, a curve C shows the frequency characteristic when iron, which is a soft magnetic material similar to the magnetic material 4, comes within the detection distance range. In the case of soft magnetic materials, the resonance frequency f at that time is different from that when detecting magnetic materials. ' increases from fo. Moreover, the voltage level of the entire curve C is decreasing. This is thought to be due to eddy current loss caused by iron.

このような磁性材料の種類に応じて変化する周波数特性
を利用して磁性材料と軟磁性材料とを識別できる。
Magnetic materials and soft magnetic materials can be distinguished by using frequency characteristics that change depending on the type of magnetic material.

すなわち、本来のコイル1と回路部品2,3とで規定さ
れる共振周波数f。より低い周波数、例えばflに発振
器5の励磁用周波数を固定し、その電圧レベル変化から
識別するものである。磁性材料が接近していないときに
は電圧はP点に相当する。
That is, the resonance frequency f defined by the original coil 1 and the circuit components 2 and 3. The excitation frequency of the oscillator 5 is fixed at a lower frequency, for example, fl, and identification is made from changes in the voltage level. The voltage corresponds to point P when no magnetic material is close.

磁性材料4が接近したときには電圧はQ点に上昇し、軟
磁性材料が接近したときにはR点に低下する。
When the magnetic material 4 approaches, the voltage increases to point Q, and when the soft magnetic material approaches, the voltage decreases to point R.

このように励磁周波数をf。より低く設定することによ
り磁性材料と軟磁性材料とを識別できることが分かる。
In this way, the excitation frequency is set to f. It can be seen that magnetic materials and soft magnetic materials can be distinguished by setting the value lower.

一方、励磁周波数をf。より高く、例えばf2に設定す
ると、その識別は困難となる。
On the other hand, the excitation frequency is f. If it is set higher, for example f2, its identification becomes difficult.

すなわち、磁性材料が接近していなかったときの電圧は
P′点に相当するが、磁性材料や軟磁性材料のいずれも
が接近しても電圧はそれぞれ07点に示されるように低
下してしまう。
In other words, the voltage when no magnetic material approaches corresponds to point P', but even if either magnetic material or soft magnetic material approaches, the voltage drops as shown at point 07. .

また、その電圧低下の様子は磁性材料の接近程度により
異なるので、電圧低下の程度からも磁性材料と軟磁性材
料との識別は困難である。
Further, since the state of the voltage drop differs depending on the degree of proximity of the magnetic materials, it is difficult to distinguish between magnetic materials and soft magnetic materials based on the degree of voltage drop.

以上本発明の実施例を磁性材料と軟磁性材料とに対する
特性の違いを用いて述べたが、本発明はこれに限定され
るものでなく、磁性材料と同様に渦電流損失の少ない不
良感体の磁性材料を用いても軟磁性材料との識別は可能
である。
Although the embodiments of the present invention have been described above using the differences in characteristics between magnetic materials and soft magnetic materials, the present invention is not limited thereto. Even if a magnetic material is used, it is possible to distinguish it from a soft magnetic material.

また、本発明は励磁周波数をf。より下げて用いること
を述べた。その下限は原理的にはないが必要以下下げる
と、実効的な検知感度を低下させることになり好ましく
ない。本発明では下限値を(1−2/Q)fo(但しQ
は共振における尖鋭度)にすることが望ましい。
Further, the present invention sets the excitation frequency to f. I mentioned that it should be used at a lower level. Although there is no lower limit in principle, lowering it below the necessary level is undesirable because it lowers the effective detection sensitivity. In the present invention, the lower limit is (1-2/Q) fo (however, Q
is the sharpness at resonance).

〔発明の効果〕〔Effect of the invention〕

以上詳細に述べたとおり本発明によれば、コイル間隔調
整は不要となり、製作が容易であり、しかも検知感度温
度特性の安定した性能センサを得ることができる効果を
有する。
As described in detail above, according to the present invention, there is no need to adjust the coil spacing, the manufacturing is easy, and a sensor with stable detection sensitivity and temperature characteristics can be obtained.

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

第1図はセンサの基本回路図、第2図は本発明の一実施
例に示す特性図である。 1・・・コイル       2・・・電流制御抵抗3
・・・共振周波数調整コンデンサ 4・・・磁性材料5
・・・発振器       6・・・電圧検出器間 上
   王井石油化学工業株式会社第1図
FIG. 1 is a basic circuit diagram of a sensor, and FIG. 2 is a characteristic diagram showing an embodiment of the present invention. 1...Coil 2...Current control resistor 3
... Resonance frequency adjustment capacitor 4 ... Magnetic material 5
...Oscillator 6...Between voltage detectors Upper Oui Petrochemical Industry Co., Ltd. Figure 1

Claims (1)

【特許請求の範囲】[Claims] (1)周波数f_0を共振周波数とする単巻空芯コイル
を含む共振回路と、励磁周波数f_1(f_1<f_0
)を前記共振回路に印加する発振器と、前記共振回路の
端子間電圧レベルを測定する電圧検出部とを有すること
を特徴とする磁性材料検知磁気センサ。
(1) A resonant circuit including a single-turn air-core coil with a resonant frequency f_0 and an excitation frequency f_1 (f_1<f_0
) to the resonant circuit; and a voltage detection section that measures the voltage level between terminals of the resonant circuit.
JP62252245A 1987-10-06 1987-10-06 Magnetic sensor for detecting magnetic material Pending JPH0194280A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62252245A JPH0194280A (en) 1987-10-06 1987-10-06 Magnetic sensor for detecting magnetic material

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62252245A JPH0194280A (en) 1987-10-06 1987-10-06 Magnetic sensor for detecting magnetic material

Publications (1)

Publication Number Publication Date
JPH0194280A true JPH0194280A (en) 1989-04-12

Family

ID=17234536

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62252245A Pending JPH0194280A (en) 1987-10-06 1987-10-06 Magnetic sensor for detecting magnetic material

Country Status (1)

Country Link
JP (1) JPH0194280A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009014531A (en) * 2007-07-05 2009-01-22 Isao Murakami Different material determination device
CN106996967A (en) * 2017-04-28 2017-08-01 成都奥特森科技有限公司 Magnetic ore deposit grade detection method and detection device
JP6288894B1 (en) * 2017-07-27 2018-03-07 株式会社テクレコ Magnetic ink detection device
JP6844075B1 (en) * 2020-04-16 2021-03-17 三菱電機株式会社 Magnetic particle imaging device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59231562A (en) * 1983-06-14 1984-12-26 Matsushita Electric Ind Co Ltd Magnetic powder detector

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59231562A (en) * 1983-06-14 1984-12-26 Matsushita Electric Ind Co Ltd Magnetic powder detector

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009014531A (en) * 2007-07-05 2009-01-22 Isao Murakami Different material determination device
CN106996967A (en) * 2017-04-28 2017-08-01 成都奥特森科技有限公司 Magnetic ore deposit grade detection method and detection device
CN106996967B (en) * 2017-04-28 2023-08-22 成都哈工智传科技有限公司 Magnetic ore grade detection method and detection equipment
JP6288894B1 (en) * 2017-07-27 2018-03-07 株式会社テクレコ Magnetic ink detection device
JP6844075B1 (en) * 2020-04-16 2021-03-17 三菱電機株式会社 Magnetic particle imaging device
WO2021210135A1 (en) * 2020-04-16 2021-10-21 三菱電機株式会社 Magnetic particle imaging device

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