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JPS648929B2 - - Google Patents

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Publication number
JPS648929B2
JPS648929B2 JP7054678A JP7054678A JPS648929B2 JP S648929 B2 JPS648929 B2 JP S648929B2 JP 7054678 A JP7054678 A JP 7054678A JP 7054678 A JP7054678 A JP 7054678A JP S648929 B2 JPS648929 B2 JP S648929B2
Authority
JP
Japan
Prior art keywords
magnetic
magnet
sensitive element
magnetically sensitive
magnetized
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
JP7054678A
Other languages
Japanese (ja)
Other versions
JPS54161257A (en
Inventor
Akira Matsushita
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP7054678A priority Critical patent/JPS54161257A/en
Publication of JPS54161257A publication Critical patent/JPS54161257A/en
Publication of JPS648929B2 publication Critical patent/JPS648929B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は各種の機械装置の自動制御系たとえば
自動車の点火装置や回転計あるいは近接スイツチ
など、諸種の分野に応用できるパルス信号発生装
置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a pulse signal generator that can be applied to various fields such as automatic control systems for various mechanical devices, such as automobile ignition systems, tachometers, and proximity switches.

最近、自動車等にマイクロコンピユータを装備
して自動制御することが考えられているが、その
自動制御のためにはエンジンの1回転ごとに多数
の同期信号が必要とされ、しかもそれぞれの信号
がエンジン速度に関係なく常に一定の大きさで確
実に得られることが望まれている。
Recently, it has been considered to equip automobiles with microcomputers for automatic control, but automatic control requires a large number of synchronization signals for each revolution of the engine, and each signal is connected to the engine. It is desirable to always be able to reliably obtain a constant size regardless of speed.

このようなパルスを発生させる手段として、、
従来にも例えば米国特許第3820090号に示された
“Self―Nucleating Magnetic Wire”(自己―核
形成磁気線)と称するもの、あるいは特許公報昭
和52年第13705号のパルス発生装置が知られてい
る。これらには強磁性線が利用されているが、こ
れは強磁性線の全体を軸方向に磁化しておいた外
部磁界が遮断された時点で、線心部の磁化方向の
みが外核の磁力線の帰磁路を形成する方向に自律
的に反転せしめられる。この反転時の磁束変化に
もとずきパルスを発生させようとするものである
が、概して出力が小さく、またパルス発生時点を
正確に制御し難いという欠点があつた。
As a means of generating such pulses,
Conventionally, for example, there has been known a device called "Self-Nucleating Magnetic Wire" shown in US Pat. . Ferromagnetic wires are used for these, but when the external magnetic field that has magnetized the entire ferromagnetic wire in the axial direction is cut off, only the direction of magnetization in the wire core changes to the magnetic field line in the outer core. is autonomously reversed in the direction of forming a return magnetic path. Although attempts are made to generate pulses based on changes in the magnetic flux at the time of reversal, they have the drawbacks that the output is generally small and it is difficult to accurately control the timing of pulse generation.

本発明のパルス信号発生装置は、線軸方向に単
軸磁気異方性を備え、その線心部付近に正方向に
磁化された保磁力の大きい部分を有し、これと隣
接する外周部に外部磁界の作用方向に応じて正ま
たは負方向の何れかに磁化しておくことができる
保磁力の小さい部分を有する複合強磁性体で構成
された感磁要素に対し、検出コイルを捲回した当
該感磁要素の両側に、前記外部磁界として正方向
に作用する比較的強い第1磁石と負方向に作用す
る弱い第2磁石をそれぞれ固定しておき、かつ前
記第1磁石に近接させたときその磁力線が集中す
る磁路となり前記感磁要素に対する磁化作用を減
殺させる磁性可動体を組合わせて成ることを特徴
とするものである。
The pulse signal generator of the present invention has uniaxial magnetic anisotropy in the line axis direction, has a portion near the core of the wire that is magnetized in the positive direction and has a large coercive force, and has an external The detection coil is wound around a magnetically sensitive element made of a composite ferromagnetic material having a portion with a low coercive force that can be magnetized in either the positive or negative direction depending on the direction of action of the magnetic field. A relatively strong first magnet that acts in the positive direction as the external magnetic field and a weak second magnet that acts in the negative direction are respectively fixed on both sides of the magnetic sensing element, and when brought close to the first magnet, the It is characterized by being combined with a magnetic movable body that forms a magnetic path where lines of magnetic force are concentrated and reduces the magnetization effect on the magnetically sensitive element.

まず、本発明の装置に用いられている感磁要素
の概要を説明する。
First, an overview of the magnetically sensitive element used in the device of the present invention will be explained.

たとえば線状の強磁性体にひねり等の外部応力
を加えて処理したものは、線軸方向に単軸磁気異
方性を備え、その線心部付近に比較的保磁力の大
きい部分を有し、これと隣接する外周部に保磁力
の小さい部分をもつ複合強磁性体、すなわち感磁
要素になる。
For example, a wire-shaped ferromagnetic material processed by applying external stress such as twisting has uniaxial magnetic anisotropy in the wire axis direction, and has a relatively large coercive force near the wire core. It becomes a composite ferromagnetic material, that is, a magnetically sensitive element, which has a portion with a small coercive force in the outer peripheral portion adjacent to this.

このような感磁要素に対し、まずその全体を充
分に大きな第1磁界により正方向(例えば線軸に
対し右方向)に配向磁化した後、この第1磁界を
遮断する。次に比較的保磁力の小さい部分のみの
磁化方向を反転させるための弱い第2磁界を作用
させて負方向(左方向)に磁化しておく。この状
態において、再び第1磁界と同一方向の第3磁界
を作用させると、保磁力の小さい部分は、保磁力
の大きい部分の正方向の配向磁気の作用に加勢さ
れて、急速かついつせいに正方向(右方向)に逆
転せしめられる。故にこの時の磁化変化に呼応し
て、その近くに配置した検出コイルに急峻で大き
なパルス起電力を誘発する。
First, the entirety of such a magnetically sensitive element is oriented and magnetized in the positive direction (for example, rightward with respect to the line axis) by a sufficiently large first magnetic field, and then the first magnetic field is interrupted. Next, a weak second magnetic field is applied to reverse the magnetization direction of only the portion where the coercive force is relatively small, so that the portion is magnetized in the negative direction (to the left). In this state, when a third magnetic field in the same direction as the first magnetic field is applied again, the portion with a small coercive force is aided by the action of the positive orientation magnetism of the portion with a large coercive force, and rapidly and suddenly. It is reversed in the forward direction (right direction). Therefore, in response to the magnetization change at this time, a steep and large pulse electromotive force is induced in the detection coil placed nearby.

このようなパルス起電力の誘発原理であるがた
めに、弱い第2磁界の次に強い第3磁界が鎖交し
さえすれば、常に一定値以上の大きさのパルス起
電力を発生することができる。これは複合磁性体
内部において、互いに隣接する磁気層間の磁気的
相互作用によつて惹起された特異な磁気逆転現象
による磁束変化に基づき、その起電力の大きさが
支配されるものであるから、従来の誘導起電力の
ような鎖交磁束の変化割合に依存するものとは全
く異なる特異な誘発パルスである。
Because of this principle of inducing pulsed electromotive force, as long as a weak second magnetic field is linked with a strong third magnetic field, a pulsed electromotive force of a magnitude greater than a certain value can always be generated. can. This is because the magnitude of the electromotive force is controlled based on the magnetic flux change due to a unique magnetic reversal phenomenon caused by the magnetic interaction between adjacent magnetic layers inside the composite magnetic material. This is a unique induced pulse that is completely different from conventional induced electromotive force that depends on the rate of change in flux linkage.

なお、前記第1磁界と第3磁界とは同一のもの
を用いればよいから、実際には感磁要素に対し
て、負方向の第2磁界と正方向の第1磁界とを交
互に作用させるだけで順次パルスを誘発させるこ
とができる。
Note that since the first magnetic field and the third magnetic field may be the same, in reality, the second magnetic field in the negative direction and the first magnetic field in the positive direction are alternately applied to the magnetically sensitive element. It is possible to induce sequential pulses by simply

次に、本発明の実施例を図面について説明す
る。
Next, embodiments of the present invention will be described with reference to the drawings.

第1図、第2図において、1は前述の感磁要素
であり、2はその周りに巻かれた(または近くに
配置された)検出コイルである。また3は感磁要
素1を全体的に正方向へ磁化するための充分に強
い第1磁石、4は感磁要素1の比較的保磁力の小
さい部分のみを負方向に磁化するための弱い第2
磁石で、何れも固定された状態にある。ここにい
う磁石とは一般には永久磁石を指すが、電磁石で
あつてもよい。
In FIGS. 1 and 2, 1 is the aforementioned magnetically sensitive element, and 2 is a detection coil wound around (or placed near) it. Further, 3 is a sufficiently strong first magnet to magnetize the entire magnetically sensitive element 1 in the positive direction, and 4 is a weak first magnet to magnetize only a portion of the magnetically sensitive element 1 with a relatively small coercive force in the negative direction. 2
Both are held in place by magnets. The magnet referred to here generally refers to a permanent magnet, but may also be an electromagnet.

これらの固定側に対し、第1磁石3の磁化作用
を断続的に減殺する磁性可動体5が組合せられて
いる。
A magnetic movable body 5 that intermittently reduces the magnetization effect of the first magnet 3 is combined with these fixed sides.

この磁性可動体5としては、例えば第3図と第
4図に例示したような磁性体より成るロータが用
いられる。第3図に示す磁性可動体5は回転軸6
に多数の空〓部7(以下、磁性体を部分的に欠籬
したスリツト部分などを空〓部と称する)を設け
た磁性体の円板であり、第4図のものは多数の磁
性体の凸体8を放射状に備えた風車状のロータで
ある。
As this magnetic movable body 5, for example, a rotor made of a magnetic material as illustrated in FIGS. 3 and 4 is used. The magnetic movable body 5 shown in FIG.
It is a disk of magnetic material with a large number of hollow parts 7 (hereinafter, slit parts where magnetic material is partially omitted are referred to as hollow parts). It is a windmill-shaped rotor that is provided with convex bodies 8 radially.

次に本装置の作用について述べると、あらかじ
めその全体が正方向に磁化された感磁要素1に対
し、比較的強い第1磁石3に磁性可動体5を近接
させた時、その磁性体部分が磁力線を集中する磁
路となり、従つて感磁要素1に対する磁化作用を
減殺する。このように第1磁石3の作用が遮断さ
れている時は、比較的弱い第2磁石4のみの作用
を受けて比較的保磁力の小さい部分のみが負方向
に磁化されている。
Next, to describe the operation of this device, when the magnetic movable body 5 is brought close to the relatively strong first magnet 3 for the magnetically sensitive element 1 whose entirety has been magnetized in the positive direction, the magnetic body part It becomes a magnetic path that concentrates the lines of magnetic force, and therefore reduces the magnetizing effect on the magnetically sensitive element 1. When the action of the first magnet 3 is cut off in this way, only the relatively weak second magnet 4 acts, and only the portion with a relatively small coercive force is magnetized in the negative direction.

次にロータの回動により磁性可動体5の空〓部
を透過した第1磁石3の磁力線が感磁要素1に作
用すると、この磁界により第2磁石4の磁界が減
殺され、感磁要素1の保磁力の小さい部分の磁化
方向を、前述した如くいつせいかつ急速に正方向
に転位する。従つてこの時、検出コイル2に急峻
なパルス起電力を発生する。故に空〓部7または
凸体8の数を多くすれば、ロータの1回転ごとに
多数のパルスを発生させることができる。
Next, when the magnetic field lines of the first magnet 3 that have passed through the empty space of the magnetic movable body 5 due to rotation of the rotor act on the magnetically sensitive element 1, the magnetic field of the second magnet 4 is attenuated by this magnetic field, and the magnetic field of the second magnet 4 is As described above, the magnetization direction of the portion with a small coercive force is gradually and rapidly shifted to the positive direction. Therefore, at this time, a steep pulse electromotive force is generated in the detection coil 2. Therefore, by increasing the number of hollow portions 7 or convex bodies 8, a large number of pulses can be generated for each rotation of the rotor.

この場合、ロータの回転速度が変動したり、あ
るいは例え超々低速で回動したとしても、前記原
理で述べた理由に基づき常に一定以上の大きさの
パルス起電力を確実に発生させることができる。
In this case, even if the rotational speed of the rotor fluctuates, or even if it rotates at an extremely low speed, it is possible to always reliably generate a pulse electromotive force of a certain magnitude or higher based on the reason described in the above principle.

なお、空〓部7や凸体8の数を増やすような場
合、ロータの機械的強度を補強するために、ロー
タを合成樹脂などでモールドすることもできる。
あるいは強固な非磁性体製のロータの所要部に磁
性体を取付けるようにしてもよい。
Incidentally, when increasing the number of hollow portions 7 and convex bodies 8, the rotor may be molded with synthetic resin or the like in order to reinforce the mechanical strength of the rotor.
Alternatively, a magnetic material may be attached to a required portion of a rotor made of a strong non-magnetic material.

また、以上は第1磁石3の作用を断続させる磁
性可動体5としてロータの例を上げたが、磁性体
を第1磁石3に近接離間するような振動体や往復
運動体であつてもよい。
Furthermore, although the rotor has been used as an example of the magnetic movable body 5 that intermittents the action of the first magnet 3, it may also be a vibrating body or a reciprocating body that moves the magnetic body close to and away from the first magnet 3. .

何れにせよ、第2磁石界発生源4の磁界中に配
置された感磁要素1に対し、第1磁石3の作用を
断続させることによつて、その断続速度の大小に
拘らずほぼ一定の大きさの多数のパルス信号を確
実に得られるという特徴があるので、多数の同期
信号を必要とする各種の自動制御系に利用して極
めて効果的である。
In any case, by intermittent action of the first magnet 3 on the magnetic sensing element 1 disposed in the magnetic field of the second magnetic field generation source 4, the effect is kept almost constant regardless of the magnitude of the intermittent speed. Since it has the feature of being able to reliably obtain a large number of pulse signals of different magnitudes, it is extremely effective for use in various automatic control systems that require a large number of synchronous signals.

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

第1図と第2図は本発明の実施例を示す線図、
第3図と第4図は可動体(ロータ)を例示した平
面図である。 1:感磁要素、2:検出コイル、3:第1磁
石、4:第2磁石、5:磁性可動体、6:回転
軸、7:空〓部、8:凸体。
1 and 2 are diagrams showing embodiments of the present invention,
3 and 4 are plan views illustrating the movable body (rotor). 1: Magnetic sensing element, 2: Detection coil, 3: First magnet, 4: Second magnet, 5: Magnetic movable body, 6: Rotating shaft, 7: Air space, 8: Convex body.

Claims (1)

【特許請求の範囲】[Claims] 1 線軸方向に単軸磁気異方性を備え、その線心
部付近に正方向に磁化された保磁力の大きい部分
を有し、これと隣接する外周部に外部磁界の作用
方向に応じて正または負方向の何れかに磁化して
おくことができる保磁力の小さい部分を有する複
合強磁性体で構成された感磁要素に対し、検出コ
イルを捲回した当該感磁要素の両側に、前記外部
磁界として正方向に作用する比較的強い第1磁石
と負方向に作用する弱い第2磁石をそれぞれ固定
しておき、かつ前記第1磁石に近接させたときそ
の磁力線が集中する磁路となり前記感磁要素に対
する磁化作用を減殺させる磁性可動体を組合わせ
て成ることを特徴とするパルス信号発生装置。
1. It has uniaxial magnetic anisotropy in the direction of the wire axis, has a part near the core of the wire that has a large coercive force that is magnetized in the positive direction, and has a part with a large coercive force that is magnetized in the positive direction on the outer periphery adjacent to this part, and has a positive Alternatively, for a magnetically sensitive element made of a composite ferromagnetic material having a portion with a small coercive force that can be magnetized in either the negative direction, a detection coil is wound on both sides of the magnetically sensitive element. A relatively strong first magnet that acts in the positive direction and a weak second magnet that acts in the negative direction are each fixed as an external magnetic field, and when brought close to the first magnet, a magnetic path is formed in which the lines of magnetic force are concentrated, and the above-mentioned A pulse signal generating device characterized by comprising a combination of a magnetic movable body that reduces the magnetization effect on a magnetically sensitive element.
JP7054678A 1978-06-12 1978-06-12 Pulse signal generator Granted JPS54161257A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7054678A JPS54161257A (en) 1978-06-12 1978-06-12 Pulse signal generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7054678A JPS54161257A (en) 1978-06-12 1978-06-12 Pulse signal generator

Publications (2)

Publication Number Publication Date
JPS54161257A JPS54161257A (en) 1979-12-20
JPS648929B2 true JPS648929B2 (en) 1989-02-15

Family

ID=13434616

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7054678A Granted JPS54161257A (en) 1978-06-12 1978-06-12 Pulse signal generator

Country Status (1)

Country Link
JP (1) JPS54161257A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3352366B2 (en) * 1997-09-17 2002-12-03 株式会社ヒロセチェリープレシジョン Pulse signal generator
US6744153B2 (en) 1998-09-18 2004-06-01 Hirose Electric Co., Ltd. Apparatus for and method of generating a pulse signal
DE10259223B3 (en) * 2002-11-20 2004-02-12 Mehnert, Walter, Dr. Position detector registering rotary- or linear motion, includes excitation magnet, ferromagnetic component, coil and sensor

Also Published As

Publication number Publication date
JPS54161257A (en) 1979-12-20

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