JPS5965211A - Frequency generator - Google Patents

Frequency generator

Info

Publication number
JPS5965211A
JPS5965211A JP17520482A JP17520482A JPS5965211A JP S5965211 A JPS5965211 A JP S5965211A JP 17520482 A JP17520482 A JP 17520482A JP 17520482 A JP17520482 A JP 17520482A JP S5965211 A JPS5965211 A JP S5965211A
Authority
JP
Japan
Prior art keywords
units
frequency generator
magnetic field
rotation
divided
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
JP17520482A
Other languages
Japanese (ja)
Inventor
Tsunehiro Maruo
丸尾 恒弘
Tsumoru Matsumoto
松本 積
Hiroyuki Hara
原 啓之
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.)
Sony Corp
Original Assignee
Sony 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 Sony Corp filed Critical Sony Corp
Priority to JP17520482A priority Critical patent/JPS5965211A/en
Publication of JPS5965211A publication Critical patent/JPS5965211A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/12Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means
    • G01D5/14Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage
    • G01D5/142Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage using Hall-effect devices
    • G01D5/145Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage using Hall-effect devices influenced by the relative movement between the Hall device and magnetic fields

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)

Abstract

PURPOSE:To make it possible to obtain a highly accurate frequency generator, by applying a rotary magnetic field, which is synchronized with the rotation of a rotary body, to magnetoresistance elements made of ferromagnetic metal, which are divided into a plurality of units in axial symmetry or point symmertry and formed in a bent line pattern in each unit. CONSTITUTION:Magnetoresistance element units made of ferromagnetic metal PA-PH, which are symmetrically divided into 8 equal parts, are alternately arranged at angles of 30 deg. and 60 deg.. Output terminals Out 1 and Out 4 are connected by jumper wires J 1 and J 4 so as to form a bridge structure. A voltage applying terminal is V and a grounding terminal is G. Since a rotating magnetic field is applied to magnetism sensitive elements in synchronization with the rotation of a rotary body, the outputs having a constant phase difference is generated. All the outer configurations of the units are in congruence, and the arrangement of the units are in point symmetry or axial symmetry. Therefore, the uniform magnetic field is applied to the units. Uniform sine outputs are obtained from the output terminals of the magnetism sensitive elements. When a phase modulation detecting method is used as interpolation, a highly accurate frequency generator can be obtained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は周波数発電器、特に強磁性全編薄膜の磁気抵抗
効果ン利用した磁気抵抗素子を用いた高精度の周波数発
電器に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a frequency generator, and more particularly to a high-precision frequency generator using a magnetoresistive element utilizing the magnetoresistive effect of a ferromagnetic full-length thin film.

背景技術とその間順点 従来の周波数発電器は第1図又は第2図に示す如く円形
の多極着磁しであるPGリングlと対向してホール素子
等の感磁素子2Y配設し、F G IJソングンブラシ
レスモータのロータのような回転体と同期して回転させ
るよう圧して、その磁界変化ビ感磁素子2によって検出
して周波数信号7得ていた。
BACKGROUND TECHNOLOGY AND ITS POINTS In a conventional frequency generator, as shown in FIG. 1 or 2, a magnetically sensitive element 2Y such as a Hall element is arranged opposite to a circular multi-pole magnetized PG ring l. A frequency signal 7 was obtained by applying pressure to rotate in synchronization with a rotating body such as the rotor of a FGIJ Songun brushless motor, and detecting the change in the magnetic field with a magnetic sensing element 2.

しかしこのような従来装61の構成によると。However, according to the configuration of such conventional device 61.

F Gリングlの着磁のピンチむら、その外周のぶれ等
により正しく回転をできなかったり、或いは小型化又は
出力周波数を増大しようとしてもFGリング自体に制約
され物理的に困難であった。出力周波数を増大T乙には
公知の内挿法を用いることにより可能であるが、そのた
めには歪の少ない正弦波出力を得ることが前提であり、
fI’ G IJングを用いる従来装置ではそれは困難
であった。また小型化しようと丁れば必然的[k’ G
 IJングの着磁極数ン減少せざるン得なかった。
Due to pinch unevenness in the magnetization of the FG ring l, wobbling of its outer periphery, etc., it may not be possible to rotate correctly, or attempts to downsize or increase the output frequency are physically difficult due to constraints imposed by the FG ring itself. It is possible to increase the output frequency by using a known interpolation method, but this requires obtaining a sine wave output with little distortion.
This has been difficult with conventional devices using fI' G IJ. Also, if you try to make it smaller, it is inevitable [k' G
The number of magnetized poles of the IJ ring had to be reduced.

発明の目的 本発明の目的は上述した従来装置の欠点を除去した+R
i I+’7度かつ小型化可能で、出力の内挿法として
位相変調検出力法を採用することができる周波数発′屯
器に提供するにある。
OBJECTS OF THE INVENTION The purpose of the present invention is to eliminate the drawbacks of the above-mentioned conventional devices.
The object of the present invention is to provide a frequency oscillator which is 7 degrees i I+', can be made compact, and can employ a phase modulation detection power method as an output interpolation method.

発明の概要 本発明は上記目的を達成するため、線対称又は点対称な
枚数のユニットに分割され、かつ各ユニット内で折線パ
ターンに形成された強磁性金稿磁気抵抗素子から成り、
各ユニット間の隣接する磁気抵抗素子の折線パターンが
所定角度と坂で配列された感磁素子に、回転体の回転に
同期した回転うに構成したことを特徴とする。
SUMMARY OF THE INVENTION In order to achieve the above object, the present invention comprises a ferromagnetic metal magnetoresistive element divided into a line-symmetric or point-symmetric number of units and formed in a broken line pattern within each unit,
It is characterized in that the magnetic sensing elements in which the folded line patterns of adjacent magnetoresistive elements between each unit are arranged at a predetermined angle and slope are configured to rotate in synchronization with the rotation of a rotating body.

実施例 以下まず本発明に使用する感磁素子を説明すると、第3
図において、A〜14は対称[8等分された強磁性金目
磁気抵抗素子ユニットで、各ユニット間の磁気抵抗素子
を構成″fる隣接する折線パターンPA−PHは図示の
如(交互に30°、60°の角度を以て配列されている
Examples Below First, the magnetic sensing element used in the present invention will be explained.
In the figure, A to 14 are symmetrical ferromagnetic metal magnetoresistive element units divided into eight equal parts, and adjacent broken line patterns PA-PH constitute the magnetoresistive element between each unit as shown in the figure (alternately 30 They are arranged at angles of 60° and 60°.

OUT□〜(JUT4は出力端子、■及びGは電圧印加
端子及び接地端子であり、例えば出力端子otJTi間
及びOUT 4間馨ジャンパー線Jl及びJ4で接続し
、ブリッジ構成とする。
OUT□~(JUT4 is an output terminal, ■ and G are a voltage application terminal and a ground terminal. For example, the output terminals otJTi and OUT4 are connected by jumper wires Jl and J4 to form a bridge configuration.

第4図は第3図の感磁素子の等価回路であり、各端子の
出力電圧をv1〜v4と丁れば該素子に対″″fる印2
11I TjB 界f) ”/2 回転4jj K J
2’B = VI  V2 =に’VCCsin2θ及
びl□ = VB  V4 == K’VCCsin 
(2θ−杓π)なる互いに120°位相の異なる2相出
力を得ることができる。従ってこれら2つの信号ダB*
00から回路的に更に互いに120°位相の異なる信号
を作ることは容易であり、かくして1個の感磁素子から
3相の位置検出信号を得ることができる。
Fig. 4 is an equivalent circuit of the magnetically sensitive element shown in Fig. 3, and if the output voltages of each terminal are divided by v1 to v4, then the element will have a pair of ``f'' mark 2.
11I TjB field f) ”/2 rotation 4jj K J
2'B = VI V2 = 'VCCsin2θ and l□ = VB V4 == K'VCCsin
It is possible to obtain two-phase outputs having a phase difference of 120° from each other (2θ - π). Therefore, these two signals DaB*
00, it is easy to generate signals having a phase difference of 120 degrees from each other using a circuit, and thus three-phase position detection signals can be obtained from one magneto-sensitive element.

第5図は本発明に特に好適な感磁素子の他の例で、各ユ
ニット間の隣接する折線パターンが図示の如(45°の
角度ン以て配列されている。この素子も第6図に示す如
くブリクジに構成して出力v5〜V8ン取り出すとすれ
ば、 g6D=V5  V6−K V(:Cs in 20D
B = V7− VB = KVoCsin (2θ−
−i)の如<90°位相の異なる2相出力OD、グEン
得ることができる。
FIG. 5 shows another example of a magnetic sensing element particularly suitable for the present invention, in which the adjacent fold line patterns between each unit are arranged at an angle of 45° as shown in the figure. This element is also shown in FIG. If we configure the bridge as shown in the figure and take out the output v5 to V8, g6D=V5 V6-K V(:Cs in 20D
B = V7- VB = KVoCsin (2θ-
-i) It is possible to obtain two-phase outputs OD and GEN having different phases by <90°.

第7図(a)、 lblは本発明の一実施例で、3は例
えば第5図に示す感磁素子を内蔵したパッケージ・4は
2極着磁した磁石、5は支持体である。支持体5はモー
クロの回転軸7に装着され、該支持体上に磁石4が配設
され、これに対向して感磁素子パッケージ3が設けられ
ている。
In FIG. 7(a), lbl is an embodiment of the present invention, 3 is a package incorporating a magnetic sensing element shown in FIG. 5, 4 is a bipolar magnetized magnet, and 5 is a support. The support body 5 is attached to the rotary shaft 7 of the mokuro, a magnet 4 is disposed on the support body, and a magnetically sensitive element package 3 is disposed opposite to the magnet 4.

磁石4は第8図(a) 、 (b)に示す如く2個の棒
磁石M、、M2とし、該磁石間に感磁素子パンケージ3
を設けてもよい。
The magnets 4 are two bar magnets M, M2 as shown in FIGS.
may be provided.

或いは第9図(a) 、 (b)に示すように回転体8
の外壁内に2極着磁したリング状磁石9を装着し、該磁
石内に感磁素子パンケージ3を設けてもよい。
Alternatively, as shown in FIGS. 9(a) and 9(b), the rotating body 8
A two-pole magnetized ring-shaped magnet 9 may be mounted inside the outer wall of the magnet, and the magnetically sensitive element pancage 3 may be provided within the magnet.

上述のように構成子れば、回転体の回転に同期して回転
磁界が感磁素子に印加されるので、第10図に示すよう
な906位相の異なる出力j’l *  5152が発
生する。
With the configuration described above, a rotating magnetic field is applied to the magneto-sensitive element in synchronization with the rotation of the rotating body, so that outputs j'l*5152 having 906 different phases as shown in FIG. 10 are generated.

而して本発明に使用する感磁素子は前述したようにその
ユニットの外形が全て合同であり、しかも各ユニットの
配置は点対称又はIvI!対称であるため、各ユニット
に均一な磁場が作用する。従って感磁素子パンケージ3
の各出力端子からは均一な正弦波出力が得られ、しかも
物に感磁素子として第5図に示す如く各ユニット内の折
線パターンが45°を成子ものを使用丁れば、発生する
2つの出力は906の位相差を有しているので、内挿法
として公仰の位相変調検出法(例えば、特開昭57−5
14号、特開昭57−30909号等参照)を用いるこ
とができ、これにより高精度周波数発*aが得られる。
As mentioned above, all of the units of the magnetic sensing element used in the present invention have the same external shape, and the arrangement of each unit is point symmetrical or IvI! Because of the symmetry, a uniform magnetic field acts on each unit. Therefore, the magnetic sensing element pan cage 3
A uniform sine wave output can be obtained from each output terminal of the unit, and if a magnetically sensitive element is used as a magnetically sensitive element in each unit, as shown in Fig. 5, the two generated Since the output has a phase difference of 906, the phase modulation detection method (for example, JP-A-57-5
14, Japanese Unexamined Patent Publication No. 57-30909, etc.) can be used, thereby obtaining high-precision frequency oscillation*a.

即ち、前記第1相及び第2相出力2+  42は夫夫下
記のように表示される。
That is, the first and second phase outputs 2+42 are displayed as shown below.

11 =: E6 sinωt $2 == EO5in(GJt + 90 ) =E
OC03(c)を但しEoは直流で’2は回転体の角速
度である。
11 =: E6 sinωt $2 == EO5in(GJt + 90) =E
OC03(c), where Eo is a direct current and '2 is the angular velocity of the rotating body.

上記出力11+12Y位相変調検出方法による内挿回路
に与えると、該回路では%961*j’2は下記のよう
に変調される。
When the above output 11+12Y phase modulation detection method is applied to the interpolation circuit, %961*j'2 is modulated as follows.

el == (E□sinωot ) sinωte2
 = (EO5in(ωot+90°))CO5ωt−
(E□ cosGJOt ) cosωを但しω0は交
流の角速度である。
el == (E□sinωot) sinωte2
= (EO5in(ωot+90°))CO5ωt-
(E□cosGJOt) cosω, where ω0 is the angular velocity of alternating current.

両変調出力el+e2Y加算すると、 C3= el + C4= H□ sinω□tsin
ωt −4−E□ cosωOt cosω二EOl 
cos (ωO−ω)1) となりC3の位相は(ω0−ω)に依存したものとなる
ので、C3の位相を知ることにより回転体の角速度ω、
従って回転体の周波数ン仰ることができる。
Adding both modulation outputs el + e2Y, C3 = el + C4 = H□ sinω□tsin
ωt −4−E□ cosωOt cosω2EOl
cos (ωO-ω)1), and the phase of C3 depends on (ω0-ω), so by knowing the phase of C3, the angular velocity ω of the rotating body,
Therefore, the frequency of the rotating body can be determined.

発明の詳細 な説明した所から明らかなように本発明によれば、下記
のような優れた効果が得られる。
As is clear from the detailed description of the invention, according to the present invention, the following excellent effects can be obtained.

(イ) 出力の内挿法として位f目変調検出方法を用い
ることができるので高精度の周波数発電器が得られ7)
(b) Since the f-th modulation detection method can be used as the output interpolation method, a highly accurate frequency generator can be obtained7)
.

(口j 各素子ユニットを対称形に配置した感磁素子を
用いているので、各素子ユニットには均一な回転磁場が
作用し、従って均一かつ歪の少ない正弦波出力が得られ
る。
(J) Since magnetic sensing elements are used in which each element unit is arranged symmetrically, a uniform rotating magnetic field acts on each element unit, and therefore a uniform sine wave output with less distortion can be obtained.

p−を多くの菓子ユニットヶ1つのチップに集約してな
る感磁素子ユニットに対向して配設された小型の2極着
磁した磁石を回転させるように構成子ればよいので、装
置全体が大巾に小型化しうる。
Since all that is needed is a component that rotates a small two-pole magnetized magnet placed opposite to a magnetically sensitive element unit which is made up of many confectionery units integrated into a single chip, the entire device is It can be downsized to a large extent.

【  に) 2極N磁の磁石を使用子れば、その周波数
発電器パッケージに対する取付精度を厳しくしなくても
、均一な回転磁場を得ることができる。
[2] If a 2-pole N magnet is used, a uniform rotating magnetic field can be obtained without strict mounting accuracy to the frequency generator package.

(ホ) 磁石単体としての部品精度ン厳しくしな(ても
均一な回転磁場が得られる。
(E) A uniform rotating magnetic field can be obtained even if the precision of the parts as a single magnet is not strict.

(へ)、J−型かつ軽量の周tll数発電器が実現でき
る。
(f) A J-type and lightweight generator with a number of cycles can be realized.

従ってこの周波数発電器をサーボ系に使用すればそのサ
ーボ系の帯域ケ高くとることが可能となるノテ、サーボ
系駆動用モータにトルクリンゲルがあっても、そのサー
ボ系において除去し得る。
Therefore, if this frequency generator is used in a servo system, the band of the servo system can be increased.Even if there is a torque ringer in the servo system drive motor, it can be eliminated in the servo system.

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

第1図及び第2図は従来の周波数発電器l示す概略図、
第3図(al、 (blは本発明に使71される感磁素
子の一例を示す概略図、第4図はイーの尋価回路図、第
5図(al、 lblは本発明に使用される感磁素子の
他の例を示す概略図、第6図はその等価回路図、第7図
(a)、 fb)は本発明の一実施例Z示す概略図、第
8図fan、 (b)及び第9図(al、 (b)は夫
々本発明の他の実施例〉示す概略図、第1θ図は第5図
の感磁素子の出力波形図である。 3・・・g磁素子パッケージ、4−・・磁石、5・・・
支持体、6・・・モータ。 ポ3図 奉4図 第5図 (0)v 第5図 (b) 乍7図 (G)            (b)某8図
1 and 2 are schematic diagrams showing a conventional frequency generator,
Figure 3 (al, (bl) is a schematic diagram showing an example of a magnetic sensing element used in the present invention, Figure 4 is a circuit diagram of Yi's circuit diagram, Figure 5 (al, (bl) is a schematic diagram showing an example of a magnetic sensing element used in the present invention. FIG. 6 is a schematic diagram showing another example of a magneto-sensitive element, FIG. 6 is an equivalent circuit diagram thereof, FIG. ) and FIGS. 9(a and 9b) are schematic diagrams showing other embodiments of the present invention, respectively, and FIG. 1θ is an output waveform diagram of the magnetic sensing element in FIG. Package, 4-... Magnet, 5...
Support body, 6... motor. Figure 3 Figure 4 Figure 5 (0) v Figure 5 (b) Figure 7 (G) (b) Certain Figure 8

Claims (1)

【特許請求の範囲】 (υ 線対称又は点対称な複数のユニットに分割され、
かつ各ユニット内で折線パターンに形成された強磁性金
民磁気抵抗素子から成り、各ユニツト量の隣接する磁気
抵抗素子の折線パターンが所定角度を以て配列された感
磁素子と、該素子に回転体の回転に同期して回転磁場を
印加する手段とを備えたことン特漱とする周波数発電器
。 (2)前記素子が8ユニツトに分割され、前記各折線パ
ターンの角度が互いに45ヲなし、かつ90’の角度ン
な丁ユニットを一組として、4組のユニットの出力乞ブ
リッジに接続したことを特徴とする特許請求の範囲第f
i1項記載の周波数発電器。 (3)  前記手段が回転体の回転に同期して回転する
ようになってい7:+2極着磁の磁石を有することン特
倣とする特許請求の範囲第+1)項記載の周波数発電器
。 (4)  前記感磁素子の出カン位相変調検出方法によ
る内挿するように構成したことを特徴とする特許請求の
範囲第+13項及び第(2)項記載の周波数発電器。
[Claims] (υ Divided into a plurality of line-symmetric or point-symmetric units,
Each unit consists of a ferromagnetic metal magnetoresistive element formed in a broken line pattern, and a magnetic sensing element in which the broken line pattern of adjacent magnetic resistance elements of each unit is arranged at a predetermined angle, and a rotating body attached to the element. and means for applying a rotating magnetic field in synchronization with the rotation of the frequency generator. (2) The element is divided into 8 units, and each of the folded line patterns has an angle of 45 degrees with respect to each other, and a set of units having an angle of 90' is connected to the output bridge of 4 sets of units. Claim f characterized by
The frequency generator according to item i1. (3) The frequency generator according to claim 1, wherein the means is adapted to rotate in synchronization with the rotation of a rotary body, and has a magnet with +2 pole magnetization. (4) The frequency generator according to claim 13 and claim 2, characterized in that the frequency generator is configured to perform interpolation using an output phase modulation detection method of the magnetic sensing element.
JP17520482A 1982-10-05 1982-10-05 Frequency generator Pending JPS5965211A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17520482A JPS5965211A (en) 1982-10-05 1982-10-05 Frequency generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17520482A JPS5965211A (en) 1982-10-05 1982-10-05 Frequency generator

Publications (1)

Publication Number Publication Date
JPS5965211A true JPS5965211A (en) 1984-04-13

Family

ID=15992110

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17520482A Pending JPS5965211A (en) 1982-10-05 1982-10-05 Frequency generator

Country Status (1)

Country Link
JP (1) JPS5965211A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1256778A1 (en) * 2001-05-08 2002-11-13 Dr. Fritz Faulhaber GmbH &amp; Co. KG Feinmechanische Werkstätten Angle sensor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1256778A1 (en) * 2001-05-08 2002-11-13 Dr. Fritz Faulhaber GmbH &amp; Co. KG Feinmechanische Werkstätten Angle sensor

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