JPS5814059A - Rotation signal generator - Google Patents

Rotation signal generator

Info

Publication number
JPS5814059A
JPS5814059A JP56112553A JP11255381A JPS5814059A JP S5814059 A JPS5814059 A JP S5814059A JP 56112553 A JP56112553 A JP 56112553A JP 11255381 A JP11255381 A JP 11255381A JP S5814059 A JPS5814059 A JP S5814059A
Authority
JP
Japan
Prior art keywords
rotor
permanent magnet
amorphous magnetic
pole
magnetic material
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
JP56112553A
Other languages
Japanese (ja)
Inventor
Seiichi Miyagawa
宮川 誠一
Takeshi Nakane
中根 武司
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.)
Aisin Corp
Original Assignee
Aisin Seiki Co 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 Aisin Seiki Co Ltd filed Critical Aisin Seiki Co Ltd
Priority to JP56112553A priority Critical patent/JPS5814059A/en
Publication of JPS5814059A publication Critical patent/JPS5814059A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • G01P3/42Devices characterised by the use of electric or magnetic means
    • G01P3/44Devices characterised by the use of electric or magnetic means for measuring angular speed
    • G01P3/48Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage
    • G01P3/481Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage of pulse signals
    • G01P3/487Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage of pulse signals delivered by rotating magnets

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Linear Or Angular Velocity Measurement And Their Indicating Devices (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)
  • General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)

Abstract

PURPOSE:To achieve a high durability by arranging an U-shaped amorphous magnetic body forcibly bent in part facing a magnetic pole of a permanent magnetic rotor whose N pole and S pole are alternately formed in the circumferential direction and an electric coil wound thereon. CONSTITUTION:A ring-shaped permanent magnet 2 is fastened on a rotor 1 and magnetized with the side surface thereof circumferentially polarized into 12 poles N-S-N-S... The rotor 1 is supported with bearings 41 and 42 separately forced into casings 31 and 32. In the embodyment thereof used for a wheel velocity sensor, one end 1a of the rotor 1 is connected to a power shaft of a transmission while the other end 1b thereof to a speed meter cable and a U-shaped amorphous magnetic body 5 forcibly bent is arranged near the side surface of the permanent magnet 2. The amorphous magnetic body 5 was previously coated with a flexible insulation resin when it was flat and a coil 6 is wound thereon somewhat coarsely.

Description

【発明の詳細な説明】 本発明は永久磁石ロータの回転に応じた電気信号を発生
する信号発生器に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a signal generator that generates an electrical signal in response to the rotation of a permanent magnet rotor.

この種の信号発生器には、永久磁石の磁力でリードスイ
ッチを閉とするオン・オフタイプのもの、およびピック
アップコイルで磁力変化に応じた電圧を誘起するタイプ
のものがある。リードスイッチを用いるものではリード
接点の耐久性が問題であり、ピックアップコイルを用い
るものでは永久磁石ロータの回転速度が低いと誘起電圧
が低いので低速域での応答性が低いという問題がある。
This type of signal generator includes an on-off type that uses the magnetic force of a permanent magnet to close a reed switch, and a type that uses a pickup coil to induce a voltage according to changes in magnetic force. Those using reed switches have a problem with the durability of the reed contacts, and those using pickup coils have a problem of low responsiveness in the low speed range because the induced voltage is low when the rotation speed of the permanent magnet rotor is low.

本発明は永久磁石ロータタイプの、耐久性が高くしかも
低速域での応答性が高い回転信号発生器を提供すること
を第1の目的とし、パルス化処理が容易で低速域におい
ても回転に正確に同期したパルスを得ることができる回
転信号発生器を提供することを第2の目的とする。
The first object of the present invention is to provide a permanent magnet rotor type rotation signal generator that is highly durable and has high responsiveness in the low speed range, and has easy pulse processing and accurate rotation even in the low speed range. A second object is to provide a rotation signal generator that can obtain pulses synchronized with the rotation signal generator.

上記目的を達成するために本発明においては、ピックア
ップコイルタイプの回転信号発生器においてピックアッ
プコイルのコアを、アモーファス磁性体を曲げ強制した
ものとする。
In order to achieve the above object, in the present invention, in a pickup coil type rotational signal generator, the core of the pickup coil is made of an amorphous magnetic material that is forced to bend.

これによれば、アモーファス磁性体の屈曲側の面には圧
縮力が作用し、伸張側の面に引張力が作用して両面で磁
化保持力が異なり、ライ−ガント効果が現われる。すな
わち、永久磁石ロータの回転によるコア印加磁界の変化
に対してコア磁束の方向転換が屈曲側と伸張側でタイミ
ングが異なり、一方の層における磁束の方向転換時に鋭
い立−トりおよび立下りのパルス電圧が電気コイルに誘
起される。このパルス電圧の尖頭値はロータの回転速度
にほとんど影響されず、また該パルス電圧の周波数は外
部磁界の変化、すなわち永久磁石ロータの回転に完全に
同期している。したがって、低速度域でも定レベルの同
期パルスが得られる。またアモーファス磁性体は、液相
金属を急冷して作らざるを得ないため薄板であり、しか
も磁気的には強磁性であって透磁率および飽和磁化が大
きく、保持力が小さく、機械的には破断強さがきわめて
高く、弾力性および復元性に優れる。このようなアモー
ファス磁性体は薄いためロータ磁束で飽和しやすく、そ
れに巻回した電気コイルにロータの回転に応じたライ−
ガント効果による電圧パルスを生じやすい。機械的には
製造が簡単になり、耐振、耐衝撃性および反復再現性が
高い。
According to this, a compressive force acts on the surface on the bending side of the amorphous magnetic material, and a tensile force acts on the surface on the elongated side, so that the magnetization retention force is different on both sides, and the Leigand effect appears. In other words, in response to changes in the magnetic field applied to the core due to the rotation of the permanent magnet rotor, the timing of the direction change of the core magnetic flux is different between the bending side and the extension side, and when the direction of the magnetic flux changes in one layer, there is a sharp rise and fall. A pulsed voltage is induced in the electrical coil. The peak value of this pulse voltage is almost unaffected by the rotational speed of the rotor, and the frequency of the pulse voltage is completely synchronized with changes in the external magnetic field, ie, with the rotation of the permanent magnet rotor. Therefore, a constant level synchronization pulse can be obtained even in a low speed range. In addition, amorphous magnetic materials must be made by rapidly cooling liquid metal, so they are thin plates, and magnetically they are ferromagnetic, with high permeability and saturation magnetization, low coercive force, and mechanically Extremely high breaking strength, excellent elasticity and restorability. Since such amorphous magnetic material is thin, it is easily saturated by the rotor's magnetic flux, and the electric coil wound around it has a wire that responds to the rotation of the rotor.
Easily generates voltage pulses due to the Gantt effect. Mechanically, it is easy to manufacture and has high vibration and impact resistance and repeatability.

第1a図に本発明の一実施例を示す。第1a図において
、ロータ1にはリング状の永久磁石が固着されている。
FIG. 1a shows an embodiment of the invention. In FIG. 1a, a ring-shaped permanent magnet is fixed to a rotor 1. In FIG.

永久磁石2の側周面は、周方向にN −8−N −8−
−−−と12極(S極6極、N極6極)に分極磁化され
ている。ロータ1はケーシング3Iおよび32にそれぞ
れ圧入された軸受4.および4□で支持されている。こ
の実施例は車輛速度センサとして用いるため、ロータ1
の一端1aは変速機の出力軸に、他端1bはスピードメ
ータケーブルに結合する形状としている。永久磁石2の
側周面近傍にU形に強制したアモーファス磁性体5が配
置されている。
The side peripheral surface of the permanent magnet 2 is N −8−N −8− in the circumferential direction.
--- It is polarized and magnetized into 12 poles (6 S poles, 6 N poles). The rotor 1 is fitted with bearings 4. which are press-fitted into the casings 3I and 32, respectively. and 4□. Since this embodiment is used as a vehicle speed sensor, the rotor 1
One end 1a is connected to the output shaft of the transmission, and the other end 1b is connected to the speedometer cable. An amorphous magnetic body 5 forced into a U-shape is arranged near the side peripheral surface of the permanent magnet 2.

第1b図にアモーファス磁性体5の縦断面(第1a図の
IB−IB)線断面を、第1C図にアモーファス磁性体
5の端部先端の平面を示す。アモーファス磁性体5には
、それが平板状(直線状)のときに、可撓性の絶縁樹脂
が被覆されその上にやや粗く電気コイル6が巻回された
後に更に可撓性の絶縁樹脂が被覆されており、このよう
に電気コイル6を一体にしたアモーファス磁性体5は、
強制枠8のスリット9. 、9□に両端部を通してU字
形に曲げ強制されている。強制枠8は支持台1oに固着
されている。スリット9. 、92の間隔は、永久磁石
2の周方向に相隣り合うN−8極間隔と等しく設定され
ている。このように等しくすることにより、アモーファ
ス磁性体5の先端間に加わる磁界強度が高くなり、ロー
タ1の回転に応じた磁界の変動が太きい。
FIG. 1b shows a longitudinal section of the amorphous magnetic material 5 (IB-IB in FIG. 1a), and FIG. 1C shows a plane of the end of the amorphous magnetic material 5. When the amorphous magnetic material 5 is flat (straight), it is coated with a flexible insulating resin, and after an electric coil 6 is wound somewhat roughly on it, a flexible insulating resin is further coated on the amorphous magnetic material 5. The amorphous magnetic material 5 that is coated and integrated with the electric coil 6 in this way is
Slit 9 in forced frame 8. , 9□ through both ends and forced to bend into a U-shape. The forced frame 8 is fixed to the support stand 1o. Slit 9. , 92 is set equal to the distance between N-8 adjacent poles of the permanent magnet 2 in the circumferential direction. By making them equal in this way, the strength of the magnetic field applied between the tips of the amorphous magnetic body 5 becomes high, and the fluctuation of the magnetic field according to the rotation of the rotor 1 becomes large.

アモーファス磁性体5には、第2a図に示す如く、U字
形の曲げ強制によりその屈曲側の面(内面)に圧縮力C
が、伸張側の面(外面)に引張力Tが常時作用している
。その結果、磁気特性は、第2b図に一点鎖線BHCで
示すように、圧縮力Cが作用している屈曲側の面では飽
和磁束密度が小で保持力が小となり、二点鎖線BHTで
示すように、引張力Tが作用している伸張側の面では飽
和磁束密度が犬で保持力が犬となっている。実線は引張
力も圧縮力も作用していない境界面の磁気特性を示す。
As shown in FIG. 2a, the amorphous magnetic material 5 is forced to bend in a U-shape, and a compressive force C is applied to the surface (inner surface) on the bent side.
However, a tensile force T is always acting on the stretch side surface (outer surface). As a result, the magnetic properties are such that the saturation magnetic flux density is small and the coercive force is small on the bent side surface where the compressive force C is applied, as shown by the dashed-dotted line BHC in Figure 2b, and the magnetic property is shown by the dashed-double line BHT. As shown, on the extension side surface where the tensile force T is applied, the saturation magnetic flux density is equal to 1, and the holding force is equal to 0. The solid line shows the magnetic properties of the interface where neither tensile nor compressive forces are acting.

その結果、今ロータ1が回転して永久磁石2の、アモー
ファス磁性体5に及ぶ磁界が第2c図に示すようにサイ
ン波状に変化すると、外部磁界強度が圧縮応力面の保持
力を越える時点に該面において一瞬に磁束の向きが反転
し、鋭いパルス電圧がコイル6に誘起される(ライ−ガ
ント効果)。
As a result, when the rotor 1 rotates and the magnetic field of the permanent magnet 2 that affects the amorphous magnetic material 5 changes in a sine wave shape as shown in FIG. The direction of the magnetic flux instantaneously reverses in this plane, and a sharp pulse voltage is induced in the coil 6 (Leigand effect).

この、アモーファス磁性体における磁束の反転速度は、
ロータlの回転による磁束の増減速度に対して極端に速
いので、このパルス電圧ピークはロータ1の回転速度に
実質上無関係と見なしうる一定値である。しかし、永久
磁石2の回転速度とアモーファス磁性体5に加わる磁界
の振動とが一対一に対応し、しかも、該磁界の振動の特
定の位相のときのみ鋭い電圧□パルスが誘起されるので
、電圧パルスの周波数はロータ1の回転速度に比例し、
低速域においてもこの比例関係がある。
The reversal speed of magnetic flux in this amorphous magnetic material is
This pulse voltage peak is a constant value that can be considered to be substantially unrelated to the rotational speed of the rotor 1 because it is extremely faster than the rate of increase/decrease in the magnetic flux due to the rotation of the rotor 1. However, there is a one-to-one correspondence between the rotational speed of the permanent magnet 2 and the vibration of the magnetic field applied to the amorphous magnetic body 5, and a sharp voltage □ pulse is induced only at a specific phase of the vibration of the magnetic field. The frequency of the pulse is proportional to the rotation speed of the rotor 1,
This proportional relationship exists even in the low speed range.

したがって、電気コイル6に誘起されるパルスをタイミ
ングパルスとして用いうるし、それを増幅したり、その
パルス又は増幅パルスでモノマルチバイブレークをトリ
ガしてパルス幅を広げたり、あるいはパルス音カウント
して速度を検出したり、広幅処理したパルスを積分して
速度指示アナログ電圧を得るなど、従来公知の信号処理
で所望の処理を施こしうる。
Therefore, the pulse induced in the electric coil 6 can be used as a timing pulse, it can be amplified, the pulse or amplified pulse can be used to trigger a mono-multi-bi-break to widen the pulse width, or the pulse sound can be counted to determine the speed. Desired processing can be performed using conventionally known signal processing, such as detecting or integrating a wide-width processed pulse to obtain a speed indicating analog voltage.

いずれにしても電気コイル6に誘起される電圧バルスは
シャープであり、そのレベルはロータ1の回転速度に実
質上依存、せず、しかもその周波数はロータ1の回転速
度に比例する。したがって低速域において回転同期が正
確であって速度検出が正確となるという利点がある。ま
た、電気接点がなく、機械的には構造が簡単であって、
耐久性がきわめて高い。
In any case, the voltage pulse induced in the electric coil 6 is sharp, its level does not substantially depend on the rotational speed of the rotor 1, and its frequency is proportional to the rotational speed of the rotor 1. Therefore, there is an advantage that rotational synchronization is accurate in the low speed range and speed detection is accurate. In addition, there are no electrical contacts and the structure is mechanically simple.
Extremely durable.

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

第1a図は本発明の一実施例の縦断面図、第1b図はそ
のIB−IB線拡大断面図、第1C図はアモーファス磁
性体5の端部先端の拡大平面図である。第2a図はアモ
ーファス磁性体5の拡大斜視図、第2b図は磁性体5の
磁化特性を示すグラフ、第2C図は磁性体5に加わる磁
界とコイル6に誘起される電圧の相関を示すタイムチャ
ートである。
FIG. 1a is a longitudinal sectional view of one embodiment of the present invention, FIG. 1b is an enlarged sectional view taken along the line IB-IB, and FIG. 1C is an enlarged plan view of the end of the amorphous magnetic material 5. FIG. 2a is an enlarged perspective view of the amorphous magnetic material 5, FIG. 2b is a graph showing the magnetization characteristics of the magnetic material 5, and FIG. 2C is a time chart showing the correlation between the magnetic field applied to the magnetic material 5 and the voltage induced in the coil 6. It is a chart.

Claims (2)

【特許請求の範囲】[Claims] (1)円周方向にN極とS極が交互に形成された永久磁
石ロータ、永久磁石ロータの磁極に一部が対向するU形
もしくは弧状に曲げ強制されたアモーファス磁性体およ
びアモーファス磁性体に巻回された電気コイルを備える
回転信号発生器。
(1) Permanent magnet rotor with N and S poles alternately formed in the circumferential direction, an amorphous magnetic material that is forced to bend into a U shape or an arc shape with a portion facing the magnetic poles of the permanent magnet rotor, and an amorphous magnetic material. Rotary signal generator with a wound electric coil.
(2)  アモーファス磁性体の端部の距離を隣り合5
N極とS極の距離相当として端部先端を永久磁石ロータ
の磁極に対向させた前記特許請求の範囲第(1)項記載
の回転信号発生器。
(2) The distance between the ends of the amorphous magnetic material is 5
The rotation signal generator according to claim 1, wherein the tip of the end portion is opposed to the magnetic pole of the permanent magnet rotor so as to correspond to the distance between the north pole and the south pole.
JP56112553A 1981-07-17 1981-07-17 Rotation signal generator Pending JPS5814059A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56112553A JPS5814059A (en) 1981-07-17 1981-07-17 Rotation signal generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56112553A JPS5814059A (en) 1981-07-17 1981-07-17 Rotation signal generator

Publications (1)

Publication Number Publication Date
JPS5814059A true JPS5814059A (en) 1983-01-26

Family

ID=14589538

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56112553A Pending JPS5814059A (en) 1981-07-17 1981-07-17 Rotation signal generator

Country Status (1)

Country Link
JP (1) JPS5814059A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0325370A (en) * 1989-06-23 1991-02-04 Ofic Co Measuring instrument for traveling speed of automobile

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0325370A (en) * 1989-06-23 1991-02-04 Ofic Co Measuring instrument for traveling speed of automobile

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