JPS5815453A - Rotary signal generator - Google Patents

Rotary signal generator

Info

Publication number
JPS5815453A
JPS5815453A JP56112550A JP11255081A JPS5815453A JP S5815453 A JPS5815453 A JP S5815453A JP 56112550 A JP56112550 A JP 56112550A JP 11255081 A JP11255081 A JP 11255081A JP S5815453 A JPS5815453 A JP S5815453A
Authority
JP
Japan
Prior art keywords
signal generator
electric
coil
poles
permanent magnet
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
JP56112550A
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 JP56112550A priority Critical patent/JPS5815453A/en
Priority to DE19823223308 priority patent/DE3223308A1/en
Priority to US06/399,145 priority patent/US4525670A/en
Publication of JPS5815453A publication Critical patent/JPS5815453A/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
    • G01P1/00Details of instruments
    • G01P1/04Special adaptations of driving means

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)

Abstract

PURPOSE:To obtain a high-durability and precise signal generator even at a low- speed region by a method wherein a magnetic substance is faced to a permanent magnet rotor alternately magnetizing Ns and Ss and a variation in impedance is detected by applying a ripple voltage to coils wound on the magnetic substance. CONSTITUTION:Both leg sections 5a and 5b of an amorphous magnetic substance 5 formed in U-shaped are arranged by facing to a permanent magnet rotor 2 alternately magnetizing N poles and S poles. The space between the leg sections 5a and 5b is equal to the space between the magnetic poles of the rotor 2. Furthermore, two electric coils 6a and 6b are wound on the magnetic substance 5 to alternately apply a ripple voltage to the electric coils 6a, 6b and a variation in the impedance is detected by converting the variation into voltage drop. In this way, a sine-wave rotary signal in which amplitude is always constant and frequency is proportional to the rotating speed of the rotor 2 can be obtained and precise signal detection can be performed even at a low-speed region.

Description

【発明の詳細な説明】 号を発生する信号発生器に関する。[Detailed description of the invention] This invention relates to a signal generator that generates a signal.

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、およびピツク
アソ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、ピツクアソプコイルを用い
るものでは永久磁石ローフ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 pick-up coil to induce a voltage according to changes in magnetic force. Those that use a reed switch have a problem with the durability of the reed contacts, and those that use a pick-up coil have a problem that the induced voltage is low when the rotation speed of the permanent magnet loaf is low, resulting in low responsiveness in the low speed range. .

本発明は永久磁石ロータタイプの、馴久性が高くしかも
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門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 rotation signal generator of the permanent magnet rotor type, which is highly flexible and has high responsiveness in the low speed range. A second object is to provide a rotational signal generator capable of obtaining precisely synchronized pulses.

上記目的を達成するために本発明においては、永久磁石
ロータの回転による磁性体の融束変化を電気コイルで該
コイルのインピーダンス変化に変換し、インピーダンス
を検出してインピーダンス対応の電圧を得る構成とする
。これによれは、可動部は永久6荏石ロータのみである
ので耐久性が高く、また電気コイルのインピーダンスは
永久磁石ロータの回転速度は無関係であるので、速度に
よっては実質」二重圧振幅変動を生しA[いザイン波電
圧が得られる。
In order to achieve the above object, the present invention has a configuration in which a change in fusion flux of a magnetic material due to rotation of a permanent magnet rotor is converted into a change in impedance of the coil by an electric coil, and the impedance is detected to obtain a voltage corresponding to the impedance. do. This has high durability because the only moving part is the permanent magnet rotor, and the impedance of the electric coil is unrelated to the rotational speed of the permanent magnet rotor, so depending on the speed, there is virtually no double pressure amplitude fluctuation. A high sine wave voltage is obtained.

本発明の好ましい実施例においては、磁性体をアモーフ
ァス(amorphous :非晶質)磁性体とする。
In a preferred embodiment of the present invention, the magnetic material is an amorphous magnetic material.

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ぎわめて高く、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簿いた(’
l’) tJ−夕磁束て飽オDしやずく、それに巻回し
た電気−iイルにロータの回転に応じたインダクタンス
変fヒを生じやすい。
Amorphous magnetic materials have to be made by rapidly cooling liquid metal, so they are thin plates, and magnetically, they are ferromagnetic, have high permeability and saturation magnetization, have low coercive force, and are mechanically difficult to break. Extremely strong, with excellent elasticity and resilience. This kind of amorphous magnetic material has been described ('
l') When the magnetic flux is saturated in the evening, the electric coil wound around it is likely to cause an inductance change according to the rotation of the rotor.

機械的には製潰が簡単になり、面1振、 1fiil衝
撃性および反復再現性か高い。
Mechanically, crushing is easier, and it has high per-plane impact resistance, high per-filtration impact resistance, and high repeatability.

第1a図〜第1f図に本発明の一実施例を示す。An embodiment of the present invention is shown in FIGS. 1a to 1f.

第1a図は縦断面図、第11)図(佳1 n −I 1
3線断面図、第1C図はI C−I C線断面図、第1
d図はI D −I I)線断面図、第1C図は底面図
、第1f図は電気回路図である。こね、らの図面におい
て、ロータ1にはリング状の永久磁石2が固着されてい
る。永久磁石2の側周面は、周方向にN−8−N−5−
−−一と12極(S(1風6個、N極6個)に分極磁化
されている。ロータ1は)1−シンク31および32に
それぞれ圧入された軸受41および42で支持されてい
る。この実施例は車輛法度−1イン−リ−とじて用いる
ため、ロータ1の・−ケ;11;12Iは変速機の出力
軸に、他端11〕はスピード゛メータケーブルに結合す
る形状としている。
Figure 1a is a longitudinal sectional view, Figure 11) (1 n - I 1
3 line sectional view, Figure 1C is I C-I C line sectional view, 1st
Figure d is a sectional view taken along the line ID-II), Figure 1C is a bottom view, and Figure 1F is an electric circuit diagram. In the drawings of Kone et al., a ring-shaped permanent magnet 2 is fixed to a rotor 1. The side peripheral surface of the permanent magnet 2 is N-8-N-5- in the circumferential direction.
--It is polarized and magnetized into 1 and 12 poles (S (6 1-pole, 6 N-pole). The rotor 1 is supported by bearings 41 and 42 press-fitted into 1-sinks 31 and 32, respectively. . Since this embodiment is used as a 1-in-1 vehicle, the ends 11 and 12 of the rotor 1 are connected to the output shaft of the transmission, and the other end 11 is connected to the speedometer cable. .

永久磁石2の側周面近傍にtJ字形に曲けたアモーファ
ス磁性体5か配置されており、その脚5aおよび5bの
間隔は、永久磁石2の隣り合5N−8極間隔と同等にさ
れ、各脚に200ターン巻きの電気コイル6aおよび6
bが装着されている。電気コイル6aおよび6hはリー
ド7を介してコネクタ8に接続されている。
An amorphous magnetic body 5 bent in a tJ shape is arranged near the side circumferential surface of the permanent magnet 2, and the spacing between the legs 5a and 5b is equal to the spacing between adjacent 5N-8 poles of the permanent magnet 2. Electric coils 6a and 6 with 200 turns wound around the legs
b is attached. Electric coils 6a and 6h are connected to connector 8 via leads 7.

次に第1f図を参照して電気回路構成を説明すると、9
はスイ゛ノナング回路であり、これは一方の電気コイル
6aの一端に接続されたオープンコレクタタイプのイン
バータI N、1および、他方の電気コイル6bの一端
に接続され、たオープンコレクタタイプのインバータI
N2およびIN3で構成されている。電気コイル6a、
6bの他端は共通接続されて平滑化回路10と共に、限
流抵抗R2を介して定電圧VCCラインに接続されてい
る。
Next, the electric circuit configuration will be explained with reference to Fig. 1f.
is a switching circuit, which consists of an open collector type inverter IN,1 connected to one end of one electric coil 6a, and an open collector type inverter IN,1 connected to one end of the other electric coil 6b.
It consists of N2 and IN3. electric coil 6a,
The other ends of 6b are commonly connected together with the smoothing circuit 10 and connected to a constant voltage VCC line via a current limiting resistor R2.

インバータINIおよびIN2には、この実施例では、
50 Kl(z、 50%チューティのパルスが印加さ
れる。該パルスの高レベル「1」区間ではインバータI
NIが導通して電気コイル6aの一端をアースに接続す
るが、インバータIN2が導通しTN3が非導通となる
のでもう1個の電気コイル6bの一端は開放である。そ
れ故人カバルスの高レベル「1」ではコイル6aに電流
が流れるが、コイル6bには電流が流れない。入カバル
スの低レベル「0」区間ではこの逆となり、コイル6a
には電流が流れずコイル6bに電流が流れる。このよウ
ニ、コイル6aおよび61〕が交圧に導通ずる。
In this embodiment, inverters INI and IN2 include:
A pulse of 50 Kl(z, 50% tutee is applied. In the high level "1" section of this pulse, the inverter I
NI is conductive and one end of the electric coil 6a is connected to the ground, but since the inverter IN2 is conductive and TN3 is non-conductive, one end of the other electric coil 6b is open. Therefore, at the high level "1" of the caballus, current flows through the coil 6a, but no current flows through the coil 6b. In the low level "0" section of the input caballus, this is reversed, and the coil 6a
No current flows through the coil 6b, but current flows through the coil 6b. In this way, the coils 6a and 61] are electrically connected to the alternating pressure.

コイル6aおよび61)は、通電レベルか飽和磁束密度
に達するまでは高いインピーダンスを示すが、飽和磁束
密度相当値を越えると低いインピーダンスを示す。そこ
で、第2a図および第21)図に示すように、アモーフ
ァス(1好性体5の脚5aおよび5bの直下に磁極が位
置するときは、コイル6aおよび6bの通電により磁性
体5が飽和しやすく、コイル6aおよび6bのインピー
ダンスが低くなるが、第2b図に示すように脚5aと5
bの中間に磁極が位置するときには磁性体5が飽和しに
くくコイル6aおよび6bのインピーダンスは高い。
The coils 6a and 61) exhibit high impedance until they reach the energization level or saturation magnetic flux density, but exhibit low impedance once the value equivalent to the saturation magnetic flux density is exceeded. Therefore, as shown in FIGS. 2a and 21), when the magnetic pole is located directly under the legs 5a and 5b of the amorphous body 5, the magnetic body 5 is saturated by the energization of the coils 6a and 6b. The impedance of the coils 6a and 6b is low, but as shown in FIG.
When the magnetic pole is located in the middle of b, the magnetic body 5 is difficult to saturate, and the impedance of the coils 6a and 6b is high.

コイルのインピーダンスが高いときにはその電圧降下が
大きいので平滑化回路10に加わる電圧は高く、コイル
のインピーダンスか低いときにはその電圧降下か小さい
ので平滑化回路10に加わる電圧は低い。これにより、
第1f図に示す電気回路の各部の電圧は、ロータ1の回
転に伴なって第3a図〜第3C図に示す変化を示す。第
3a図は第2a図に示す状態での信号を、第31〕図は
第2b図に示す状態での信号を、また第3C図は第2C
図に示す状態での信号を示す。
When the impedance of the coil is high, the voltage drop is large, so the voltage applied to the smoothing circuit 10 is high; when the impedance of the coil is low, the voltage drop is small, so the voltage applied to the smoothing circuit 10 is low. This results in
The voltages at various parts of the electric circuit shown in FIG. 1F change as shown in FIGS. 3A to 3C as the rotor 1 rotates. Fig. 3a shows the signal in the state shown in Fig. 2a, Fig. 31 shows the signal in the state shown in Fig. 2b, and Fig. 3C shows the signal in the state shown in Fig. 2C.
The signal in the state shown in the figure is shown.

ロータ1の回転により第3a図〜第3C図に示す信号変
化を示すので、結局回路の出力OU ’J’は第4図に
実線で示すサイン波状の変動を示し、その周波数かロー
タ1の回転速度に1対1に対応する。
As the rotor 1 rotates, the signal changes as shown in Figures 3a to 3C, so the circuit output OU 'J' eventually shows a sine wave-like fluctuation as shown by the solid line in Figure 4, and the rotation of the rotor 1 One-to-one correspondence with speed.

しかしながら、振幅VWは一定である。したがって、今
第4図に示す2点鎖線のレベルで出力OUTを2値化す
るとパルスPa旧となり、このパルスPoutはロータ
1の回転速度に比例した周波数となり、この周波数が回
転速度に1対工に対応する。従来の、ピ゛ツクアップコ
イルを用いるものでは、低速度で振幅Vw が小さく、
高速度で太ぎくなるので、特に低速域においてこのよう
な正確なパルスPout以上の通り本発明の・ITt 
”3発生X:+ +:t、開閉接点を用いないので耐久
性か高く、しか・1)1y191(iIIや衝撃に強G
)47III造となり、しかも、発生信シー30)処理
は1゛バ゛j単であって、低速度域でも正確な(11号
が創られる。
However, the amplitude VW is constant. Therefore, if the output OUT is now binarized at the level of the two-dot chain line shown in FIG. corresponds to In conventional devices using a pickup coil, the amplitude Vw is small at low speeds,
Since it becomes thicker at high speeds, the present invention's ・ITt
``3 generation
) 47III structure, and moreover, the generated signal transmission 30) processing is only 1 by 1, and accurate (No. 11) is created even in the low speed range.

【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(〕)縦断面図、第11
〕図はそのI B −I fl線断面図、第1C図(佳
IC−IC線断面図、第1 (1図ばl 11−11)
線断面図、第1e図は底面図であり、第1r図口、TI
L気回路の構成を示す回路図である。第2;1)ツ1.
第21)図および第2C図は永久(磁石2の回11す々
(1」度古アモーファス(I磁性体5の脚5 a 、 
51)のf)″f置関1系とそれにお(−Jる磁性体5
の畠化特性を示す説明1ン1、第3a図、第31)図お
よび第1(0図はそれそ゛れ第22図。 第2b図お3丁び第2C図に示ず状態にお&Jる電気回
路各部の電圧を示す波形図、第・1図はロータ1が回転
しているときの電気回路各部01J Tと、該出力の2
イ直化パルスP(川tを示すタイツ・チャートである。 1:ロータ       2:永久磁石;う1132:
ケーシング  a、 、 42:軸 受5 :アモーフ
ァス磁性体   5a、5b:脚6a、61):電気コ
イ/l/  7..72:リード8 :=1ネクタ  
     9 ニスイツチング回路10:平滑化回路 特開昭58(!’1453  (4)
, FIG. 1a is a vertical cross-sectional view of one embodiment of the present invention (), and FIG.
] The figure is a cross-sectional view taken along the line IB-I fl, and Figure 1C (a cross-sectional view taken along the IC-IC line, Figure 1).
Line sectional view, Figure 1e is a bottom view, Figure 1r opening, TI
FIG. 2 is a circuit diagram showing the configuration of an L air circuit. 2nd; 1) 1.
Figures 21) and 2C show permanent (11 times (1) degrees of old amorphous (I legs 5 a of magnetic body 5) of magnet 2,
51) f)″ f position system 1 and it (-J magnetic material 5
Explanation 1, Figure 3a, Figure 31) and Figure 1 (Figure 0 are respectively Figure 22. Figure 2B, Figure 3, and Figure 2C) A waveform diagram showing the voltage of each part of the circuit, Figure 1 shows the voltage of each part of the electric circuit when the rotor 1 is rotating, and the output 2 of the electric circuit.
A straightening pulse P (This is a tights chart showing the river t. 1: Rotor 2: Permanent magnet; U1132:
Casing a, 42: Bearing 5: Amorphous magnetic material 5a, 5b: Legs 6a, 61): Electric coil/l/7. .. 72: Lead 8 :=1 Nectar
9 Niswitching circuit 10: Smoothing circuit Unexamined Japanese Patent Publication No. 1983 (!'1453 (4)

Claims (1)

【特許請求の範囲】 (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
磁性体、磁性体に巻回された電気コイル。 および、電気コイルに脈動電圧を印加し電気コイルのイ
ンピーダンスを電圧に変換する電気回路を備える回転信
号発生器1、 (2161i性体をコの字形又はU形の磁路を形成する
2脚を有するもの古し、脚のそれぞれに電気コイルを巻
回した前記特許請求の範囲第(1)項記載の回転信号発
生器。 (3)2脚の間隔を永久磁石ロータの隣り合うN極と8
極の距離相当とした前記特許請求の範囲第(2)項記載
の回転信号発生器。 (4)  電気回路は、2組の電気コイルの一方を通電
するとき他方を非通電とし、他方を通電するとき一方を
非通電とするスイッチング手段、および電気コイルと並
列に接続された平滑化回路で構成した前記特許請求の範
囲第(1)項記載の回転信号発生器。 (5)  磁性体をアモーファス磁性体とした前記特許
請求の範囲第(1)項、第(2)項、第(3)項又は第
(4)項記載の回転信号発生器。
[Scope of Claims] (1) A permanent magnet rotor in which north and south poles are formed alternately in the circumferential direction, a magnetic body partially facing the magnetic poles of the permanent magnet rotor, and an electric wire wound around the magnetic body. coil. and a rotation signal generator 1 equipped with an electric circuit that applies a pulsating voltage to an electric coil and converts the impedance of the electric coil into voltage (having two legs that form a U-shaped or U-shaped magnetic path with the 2161i magnetic body) A rotary signal generator according to claim (1), in which an electric coil is wound around each of the legs. (3) The distance between the two legs is set to 8 to
The rotation signal generator according to claim 2, wherein the rotation signal generator is equivalent to the distance between poles. (4) The electric circuit includes a switching means that de-energizes one of the two electric coils when the other is energized and de-energizes the other when the other is energized, and a smoothing circuit connected in parallel with the electric coil. A rotation signal generator according to claim (1), comprising: (5) The rotational signal generator according to claim 1, (2), (3), or (4), wherein the magnetic material is an amorphous magnetic material.
JP56112550A 1981-07-17 1981-07-17 Rotary signal generator Pending JPS5815453A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP56112550A JPS5815453A (en) 1981-07-17 1981-07-17 Rotary signal generator
DE19823223308 DE3223308A1 (en) 1981-07-17 1982-06-22 TURN SIGNALER
US06/399,145 US4525670A (en) 1981-07-17 1982-07-16 Generator for generating a rotational signal in accordance with changing saturation magnetic flux density of a magnetic member

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56112550A JPS5815453A (en) 1981-07-17 1981-07-17 Rotary signal generator

Publications (1)

Publication Number Publication Date
JPS5815453A true JPS5815453A (en) 1983-01-28

Family

ID=14589459

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56112550A Pending JPS5815453A (en) 1981-07-17 1981-07-17 Rotary signal generator

Country Status (1)

Country Link
JP (1) JPS5815453A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6158846A (en) * 1984-08-31 1986-03-26 株式会社竹中工務店 Method of foaming molten slag

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6158846A (en) * 1984-08-31 1986-03-26 株式会社竹中工務店 Method of foaming molten slag
JPH0529619B2 (en) * 1984-08-31 1993-05-06 Takenaka Komuten Co

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