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JPH0434684B2 - - Google Patents
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JPH0434684B2 - - Google Patents

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Publication number
JPH0434684B2
JPH0434684B2 JP22359483A JP22359483A JPH0434684B2 JP H0434684 B2 JPH0434684 B2 JP H0434684B2 JP 22359483 A JP22359483 A JP 22359483A JP 22359483 A JP22359483 A JP 22359483A JP H0434684 B2 JPH0434684 B2 JP H0434684B2
Authority
JP
Japan
Prior art keywords
output signal
output
magnetic
magnetically sensitive
waveform
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
JP22359483A
Other languages
Japanese (ja)
Other versions
JPS60114714A (en
Inventor
Jinichi Ito
Hayato Naito
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.)
Nidec Instruments Corp
Original Assignee
Sankyo Seiki Manufacturing 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 Sankyo Seiki Manufacturing Co Ltd filed Critical Sankyo Seiki Manufacturing Co Ltd
Priority to JP22359483A priority Critical patent/JPS60114714A/en
Publication of JPS60114714A publication Critical patent/JPS60114714A/en
Publication of JPH0434684B2 publication Critical patent/JPH0434684B2/ja
Granted 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
    • 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
    • G01D5/244Mechanical 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 characteristics of pulses or pulse trains; generating pulses or pulse trains
    • G01D5/24471Error correction
    • G01D5/24476Signal processing
    • 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
    • G01D5/244Mechanical 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 characteristics of pulses or pulse trains; generating pulses or pulse trains
    • G01D5/24471Error correction
    • G01D5/2448Correction of gain, threshold, offset or phase control

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Signal Processing (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)

Description

【発明の詳細な説明】 本発明は磁気式エンコーダーに関する。[Detailed description of the invention] The present invention relates to magnetic encoders.

従来、磁気式エンコーダーにおいては第1図に
示すように軸1に同軸的に結合されているモータ
等の回転体2の周面に磁性体からなる情報記録媒
体3が設けられ、この情報記録媒体3には予めN
極及びS極が交互に多数着磁されることによつて
情報信号が磁気的に記録されている。磁気抵抗素
子4は情報記録媒体3の周面に近接対向して配置
され、直流電源5により駆動される。この磁気抵
抗素子4は情報記録媒体3からの磁束に感応して
前記情報信号を90゜の位相差をもつて検出する2
組の素子が内設されており、これらの素子の出力
信号が出力端子A,Bより第2図に示すような
sinθ,cosθとして得られる。この出力信号は回転
体2の回転速度や回転角度に関する情報であり、
この情報に基づいて例えば回転体2が制御され
る。
Conventionally, in a magnetic encoder, as shown in FIG. 1, an information recording medium 3 made of a magnetic material is provided on the circumferential surface of a rotating body 2 such as a motor that is coaxially coupled to a shaft 1. 3 in advance
Information signals are magnetically recorded by alternately magnetizing a large number of poles and S poles. The magnetoresistive element 4 is arranged close to and facing the circumferential surface of the information recording medium 3, and is driven by a DC power source 5. This magnetoresistive element 4 senses the magnetic flux from the information recording medium 3 and detects the information signal with a phase difference of 90 degrees.
A set of elements are installed internally, and the output signals of these elements are output from output terminals A and B as shown in Figure 2.
Obtained as sinθ and cosθ. This output signal is information regarding the rotation speed and rotation angle of the rotating body 2,
For example, the rotating body 2 is controlled based on this information.

この磁気式エンコーダーにあつては、組立精度
のばらつきや着磁強度のばらつき等のない理想的
なものである場合には、磁気抵抗素子4を構成す
る2組の素子の各出力信号はそれぞれ第2図の如
く、ある一定値の直線状をなすエンベロープ3
3,34に囲まれた波形36となる。しかし、実
際の磁気式エンコーダでは、組立精度のばらつき
や着磁強度のばらつき等により、磁気抵抗素子4
を構成する2組の素子の各出力信号は第6図の如
く、エンベロープ27,28,29,30が、あ
る一定値の直線ではなくなつて波打つようにな
り、レベル変動が生ずることになる。
In the case of this magnetic encoder, if it is an ideal one with no variations in assembly accuracy or magnetization strength, each output signal of the two sets of elements constituting the magnetoresistive element 4 will be As shown in Figure 2, envelope 3 is a straight line with a certain constant value.
This results in a waveform 36 surrounded by 3 and 34. However, in actual magnetic encoders, due to variations in assembly accuracy and magnetization strength, the magnetoresistive element 4
As shown in FIG. 6, the envelopes 27, 28, 29, and 30 of the output signals of the two sets of elements constituting the circuit are no longer straight lines with a certain constant value, but become wavy, resulting in level fluctuations.

この点を分かり易く説明するために、この磁気
式エンコーダーが第5図の如きエンコーダ21で
あると想定してみる。このエンコーダ21では、
回転体2および情報記録媒体3がその外周面を、
例えば12極に着磁されたロータマグネツト22に
より構成されて回転軸1に一体に取り付けられ、
磁気抵抗素子4を構成する2組の素子が90度位相
をずらして配置された2組の磁気センサα,βか
らなる。今、回転軸1はロータマグネツト22に
第5図の如く偏心して取り付けられているものと
する。
In order to explain this point in an easy-to-understand manner, let us assume that this magnetic encoder is the encoder 21 as shown in FIG. In this encoder 21,
The rotating body 2 and the information recording medium 3 have their outer peripheral surfaces
For example, it is composed of a rotor magnet 22 magnetized with 12 poles and is integrally attached to the rotating shaft 1,
The two sets of elements constituting the magnetoresistive element 4 are composed of two sets of magnetic sensors α and β arranged with a phase shift of 90 degrees. It is now assumed that the rotating shaft 1 is eccentrically attached to the rotor magnet 22 as shown in FIG.

ロータマグネツト22はこの偏心して取り付け
られている回転軸1を中心として矢印方向に回転
する。
The rotor magnet 22 rotates in the direction of the arrow around the eccentrically attached rotating shaft 1.

第6図は磁気センサα,βの出力信号の変化を
表している。ロータマグネツト22が第5図の位
置から1回転する間に、磁気センサαは位相Aか
ら位相Dまで波形24の出力値を示す。また、磁
気センサβは位相Aから位相Dまで波形25の出
力値を示す。
FIG. 6 shows changes in the output signals of the magnetic sensors α and β. While the rotor magnet 22 rotates once from the position shown in FIG. 5, the magnetic sensor α shows the output value of the waveform 24 from phase A to phase D. Further, the magnetic sensor β shows an output value of waveform 25 from phase A to phase D.

ロータマグネツト22が、組立精度のばらつき
により偏心していることから、磁気センサα,β
は第5図の位置(第6図ではAの位置)で最も出
力信号が大きくなり、ロータマグネツト22が第
5図の位置から180度回転した位置関係(第6図
では位相Cの位置)で最も出力が小さくなる。
Since the rotor magnet 22 is eccentric due to variations in assembly accuracy, the magnetic sensors α and β
The output signal is largest at the position shown in Fig. 5 (position A in Fig. 6), and the positional relationship is such that the rotor magnet 22 is rotated 180 degrees from the position shown in Fig. 5 (position C in Fig. 6). The output is the smallest.

なお、磁気センサα,βは、ロータマグネツト
22の回転に伴つて磁極N,Sが交互に前面を通
過するので、波形24,25の如くサインカーブ
を描く。そして、磁気センサαと磁気センサβと
は電気角で90度(ロータマグネツト22の1磁極
分の半分の角度)ずれて配置されているので、そ
れぞれの出力信号波形も、第6図に示される如く
波形24と波形25とは90度ずれた出力信号波形
となる。
The magnetic sensors α and β draw sine curves as waveforms 24 and 25 because the magnetic poles N and S alternately pass in front of them as the rotor magnet 22 rotates. Since the magnetic sensor α and the magnetic sensor β are arranged at an electrical angle of 90 degrees (half the angle of one magnetic pole of the rotor magnet 22), their respective output signal waveforms are also shown in FIG. As shown, waveform 24 and waveform 25 have output signal waveforms shifted by 90 degrees.

磁気センサαの出力信号波形は、ロータマグネ
ツト22の回転軸1が偏心していないなら(理想
状態なら)、第2図の出力信号波形26の如く、
一定した出力信号(エンベロープ33,34が直
線状態)となるが、第5図のように偏心している
場合には、第6図の如く、出力信号波形24が鼓
状のエンベロープ27,28に囲まれた間で変化
することになる。
If the rotating shaft 1 of the rotor magnet 22 is not eccentric (in an ideal state), the output signal waveform of the magnetic sensor α is as shown in the output signal waveform 26 in FIG.
Although the output signal is constant (envelopes 33 and 34 are in a straight line state), if it is eccentric as shown in FIG. 5, the output signal waveform 24 is surrounded by drum-shaped envelopes 27 and 28 as shown in FIG. It will change over time.

磁気センサβの出力信号波形25も鼓状のエン
ベロープ29,30に囲まれた間で変化すること
になる。
The output signal waveform 25 of the magnetic sensor β also changes between the drum-shaped envelopes 29 and 30.

従つて、例えば、第6図の位相Bでの磁気セン
サαの理想状態の出力値は、出力値31よりももう
少し小さくなる。
Therefore, for example, the output value of the magnetic sensor α in the ideal state at phase B in FIG. 6 is a little smaller than the output value 31.

また、磁気センサβの理想状態での出力値は、
出力値32よりももう少し大きくなる。
In addition, the output value of magnetic sensor β in the ideal state is
It will be a little larger than the output value of 32.

このように、磁気センサα,βの出力信号波形
を囲むエンベロープ33,34が組立精度のばら
つきや着磁強度のばらつき等により一定値となら
ずに波打ち、磁気センサα,βの出力信号レベル
に変動が生ずる。
In this way, the envelopes 33 and 34 surrounding the output signal waveforms of the magnetic sensors α and β do not maintain a constant value due to variations in assembly precision and magnetization strength, etc., and wave, causing the output signal levels of the magnetic sensors α and β to vary. Fluctuations occur.

本発明は上記欠点を改善し、出力信号波形を囲
むエンベロープが組立精度のばらつきや情報記録
媒体の着磁強度のばらつき等により波打つたりせ
ずに一定値の直線状に保持するように補償して出
力信号レベルに変動が生ずることを防止すること
ができる磁気式エンコーダーを提供することを目
的とする。
The present invention improves the above-mentioned drawbacks by compensating the envelope surrounding the output signal waveform so that it maintains a constant linear shape without undulating due to variations in assembly accuracy or magnetization strength of the information recording medium. An object of the present invention is to provide a magnetic encoder that can prevent variations in output signal level.

以下図面を参照しながら本発明について実施例
をあげて説明する。
The present invention will be described below by way of examples with reference to the drawings.

第3図は本発明の一実施例を示す。 FIG. 3 shows an embodiment of the invention.

この実施例は前述の磁気式エンコーダーにおい
て出力信号波形を囲むエンベロープが波打つこと
を補償することにより、第2図の如く出力信号波
形を囲むエンベロープが、ある一定値の直線を示
す出力信号を得るようにしたものであり、このこ
とにより、出力信号のレベル変動が無くなる。こ
の実施例では、出力端子A,Bから得られる90゜
の位相差をもつた出力信号電圧(sinθ,cosθ)が
各々2乗演算器6,7により2乗されて加算器8
により加算される。この加算器8の出力電圧は帰
還抵抗9が付いた増幅器10よりなる誤差検出器
によつて基準電圧源11の基準電圧Eと比較さ
れ、その誤差により磁気抵抗素子4が駆動され
る。したがつて加算器8の出力電圧(sin2θ+
cos2θ)が基準電圧Eに等しくなるように磁気抵
抗素子4の感度が制御され、出力信号のレベル変
動が除去される。
This embodiment compensates for the undulation of the envelope surrounding the output signal waveform in the above-mentioned magnetic encoder, so that the envelope surrounding the output signal waveform obtains an output signal that shows a straight line with a certain constant value, as shown in Figure 2. This eliminates level fluctuations in the output signal. In this embodiment, output signal voltages (sin θ, cos θ) having a phase difference of 90° obtained from output terminals A and B are squared by square operators 6 and 7, respectively, and are then squared by an adder 8.
is added by The output voltage of the adder 8 is compared with a reference voltage E of a reference voltage source 11 by an error detector consisting of an amplifier 10 equipped with a feedback resistor 9, and the magnetoresistive element 4 is driven by the error. Therefore, the output voltage of adder 8 (sin 2 θ+
The sensitivity of the magnetoresistive element 4 is controlled so that cos 2 θ) is equal to the reference voltage E, and level fluctuations in the output signal are eliminated.

すなわち、この実施例では、例えば前述した第
1図の如き磁気式エンコーダーが第5図の如き磁
気式エンコーダーである場合、磁気センサα,β
の出力信号波形24,25に、これより少し大き
い値を加減するように補正されることにより、出
力信号波形が第6図の如く、直線状のエンベロー
プ33,34に沿うように補正制御される。磁気
センサα,βの出力信号波形24,25は位相
A,Dの位置では、出力値がもう少し0に近くな
るように(第6図でいうと、波形がもう少し収縮
するように)、また、位相Cの位置では出力値が
もう少し0から遠ざかるように(第6図でいう
と、波形がもう少し上下に膨らむように)制御さ
れる。
That is, in this embodiment, if the magnetic encoder shown in FIG. 1 is the magnetic encoder shown in FIG.
By correcting the output signal waveforms 24 and 25 by adding or subtracting a slightly larger value, the output signal waveforms are corrected and controlled to follow linear envelopes 33 and 34 as shown in FIG. . The output signal waveforms 24 and 25 of the magnetic sensors α and β are set so that the output values are a little closer to 0 at the positions of phases A and D (in the case of FIG. 6, the waveforms are a little more contracted), and At the position of phase C, the output value is controlled so as to move a little further away from 0 (in FIG. 6, the waveform swells up and down a little more).

例えば、磁気センサα,βの出力信号波形2
4,25を位相Bの位置での制御の様子をみる
と、回転軸1がロータマグネツト22に偏心して
取り付けられた場合には、理想状態よりも波形が
上下に収縮した形状になつており、磁気センサ
α,βの出力値の絶対値が理想状態よりも小さな
値の波形31,32となつている。
For example, output signal waveform 2 of magnetic sensors α and β
4 and 25 at the position of phase B, it is found that when the rotary shaft 1 is eccentrically attached to the rotor magnet 22, the waveform becomes vertically contracted compared to the ideal state. , the absolute values of the output values of the magnetic sensors α and β are smaller than the ideal state as waveforms 31 and 32.

従つて、加算器8の出力電圧(sin2+cos2)の
値も小さくなることから、誤差検出器を構成する
増幅器10への入力信号が小さくなるので、この
入力信号を大きくするように、即ち、磁気センサ
α,βの入力電圧を大きくするような制御が働い
て磁気センサα,βの出力信号が大きくなる。そ
の結果、磁気センサα,βの出力信号が理想状態
での出力値に近づく。
Therefore, since the value of the output voltage (sin 2 + cos 2 ) of the adder 8 also becomes smaller, the input signal to the amplifier 10 constituting the error detector becomes smaller. , the output signals of the magnetic sensors α and β are increased by controlling the input voltages of the magnetic sensors α and β to be large. As a result, the output signals of the magnetic sensors α and β approach the output values in the ideal state.

しかし、増幅器10への入力値が磁気センサ
α,βの出力信号24,25の各2乗値の和では
なく、例えば電圧(sin+cos)を増幅器10へ入
力した場合には、増幅器10の入力値が磁気セン
サα,βの出力信号24,25の各2乗値を加算
した値である場合のように一定値になることがな
く、ロータマグネツト22の回転に伴い時々刻々
と増幅器10への入力値が変化するので、まとも
な制御(エンベロープ27,28,29,30を
第6図の鼓状から第2図のような直線状態:理想
状態に近づける制御)はできない。
However, if the input value to the amplifier 10 is not the sum of the square values of the output signals 24 and 25 of the magnetic sensors α and β, but for example a voltage (sin+cos) is input to the amplifier 10, the input value of the amplifier 10 is the sum of the square values of the output signals 24 and 25 of the magnetic sensors α and β, but does not become a constant value, but changes to the amplifier 10 from time to time as the rotor magnet 22 rotates. Since the input values change, proper control (control that brings the envelopes 27, 28, 29, and 30 from the drum-shaped state shown in FIG. 6 to the linear state shown in FIG. 2, which approaches the ideal state) cannot be performed.

このような作用により、ロータマグネツト22
の偏心によるギヤツプのばらつきや着磁むら等に
より、磁気センサα,βの出力信号波形を囲むエ
ンベロープが波打つたりせず、一定値の直線を保
持するように補償して、磁気センサα,βの出力
信号レベルに変動が生ずることを防止することが
できる。出力信号は磁気抵抗素子4の出力端子
A,Bから導出した端子12,13より外部へ出
力されるが、2乗演算器6,7の出力信号を外部
へ出力するようにしてもよい。
Due to this action, the rotor magnet 22
The output signal waveforms of magnetic sensors α and β are compensated so that the envelopes surrounding the output signal waveforms of magnetic sensors α and β do not wave due to variations in the gap caused by the eccentricity of Fluctuations in the output signal level can be prevented. The output signal is outputted to the outside from terminals 12 and 13 derived from the output terminals A and B of the magnetoresistive element 4, but the output signals of the square calculators 6 and 7 may be outputted to the outside.

第4図は媒体の他の実施例を示す。 FIG. 4 shows another embodiment of the medium.

この実施例は上記実施例において2組の素子を
内設した磁気抵抗素子4の代りに別の磁気感応素
子であるホール素子41,42を用いたものであ
る。このホール素子41,42は電気角で90゜の
位相差となる位置に配列され、増幅器10の出力
電流により駆動される。
In this embodiment, Hall elements 41 and 42, which are other magnetic sensing elements, are used in place of the magnetoresistive element 4 in which two sets of elements are installed in the above embodiment. The Hall elements 41 and 42 are arranged at positions having a phase difference of 90 degrees in electrical angle, and are driven by the output current of the amplifier 10.

なお、上記実施例は回転型であるが、リニア型
等にしてもよい。この場合情報記録媒体3は直線
運動をする移動体にその運動方向へ情報信号が記
録されたもの等で置き換えられる。磁気感応素子
は2個使用する場合(磁気抵抗素子4も2個分で
ある)一般に電気角で90゜の奇数倍の位相差とな
る位置に配列されるが、n(≧3)個の磁気感応
素子を使用して電気角で360゜/nの位相差ずつずれ た位置に配列してもよい。この場合はn相の正弦
波をそれぞれx乗したものの和Sが S=oK=1 sinx{θ−360゜(k−1)/n} となるから、n個の磁気感応素子の出力電圧を
各々累乗演算器でx乗して加算器で加算して増幅
器10に入力すればよい。この場合も、上記実施
例と同様に加算器から増幅器10への加算電圧が
一定値になるように磁気感応素子の感度を制御
し、ロータマグネツト22の偏心によるギヤツプ
のばらつきや着磁むら等により、出力信号波形を
囲むエンベロープが波打つたりせずに一定値の直
線を保持するように補償して、出力信号レベルに
変動が生ずることを防止することができる。但し
xは加算器の出力電圧がゼロでない一定値になる
ように設定する必要があるため、偶数に制限され
る。また上記実施例において2個の磁気感応素子
を電気角で120゜の位相差になるように配置し、こ
の2個の磁気感応素子の出力信号を加算して反転
したものと2個の磁気感応素子の出力信号とを外
部へ出力するようにすれば磁気感応素子を2個に
して3相の信号を出力することができる。
Note that although the above embodiment is of a rotary type, it may be of a linear type or the like. In this case, the information recording medium 3 is replaced by a moving body that moves linearly and information signals are recorded in the direction of the movement. When two magnetic sensing elements are used (two magnetic resistance elements 4 are used), they are generally arranged at positions where the phase difference is an odd multiple of 90 degrees in electrical angle, but when n (≧3) magnetic sensing elements are used, Sensing elements may be used and arranged at positions shifted by a phase difference of 360°/n in electrical angle. In this case, the sum S of the n-phase sine waves raised to the x power is S= oK=1 sin x {θ−360°(k−1)/n}, so the The output voltages may each be raised to the power of x using a power calculator, added together using an adder, and then input to the amplifier 10. In this case, as in the above embodiment, the sensitivity of the magnetic sensing element is controlled so that the added voltage from the adder to the amplifier 10 becomes a constant value, and variations in the gap due to eccentricity of the rotor magnet 22, uneven magnetization, etc. Accordingly, it is possible to compensate so that the envelope surrounding the output signal waveform does not wave and maintain a straight line of a constant value, thereby preventing fluctuations in the output signal level. However, x is limited to an even number because it needs to be set so that the output voltage of the adder is a constant value other than zero. In addition, in the above embodiment, two magnetically sensitive elements are arranged with a phase difference of 120 degrees in electrical angle, and the sum and inversion of the output signals of these two magnetically sensitive elements and the output signal of the two magnetically sensitive elements are By outputting the output signal of the element to the outside, three-phase signals can be output using two magnetically sensitive elements.

以上のように本発明による磁気式エンコーダー
にあつては出力信号波形を囲むエンベロープが組
立精度のばらつきや情報記録媒体の着磁強度のば
らつき等により波打つたりせずに一定値の直線状
に保持するように補償し、出力信号レベルに変動
が生ずることを防止することができる。
As described above, in the magnetic encoder according to the present invention, the envelope surrounding the output signal waveform does not wave due to variations in assembly accuracy or variations in the magnetization strength of the information recording medium, and maintains a constant value in a straight line. It is possible to compensate for this and prevent fluctuations in the output signal level.

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

第1図は従来の磁気式エンコーダーを示す斜視
図、第2図は磁気式エンコーダーの理想的な出力
信号波形例を示す波形図、第3図及び第4図は本
発明の各実施例の構成を示す図、第5図は従来の
磁気式エンコーダーの例を示す平面図、第6図は
同磁気式エンコーダーの出力信号波形を示す波形
図である。 6,7……2乗演算器、8……加算器、10…
…誤差検出用増幅器、11……基準電圧源。
FIG. 1 is a perspective view showing a conventional magnetic encoder, FIG. 2 is a waveform diagram showing an example of an ideal output signal waveform of the magnetic encoder, and FIGS. 3 and 4 are configurations of each embodiment of the present invention. FIG. 5 is a plan view showing an example of a conventional magnetic encoder, and FIG. 6 is a waveform diagram showing an output signal waveform of the magnetic encoder. 6, 7...square calculator, 8...adder, 10...
...Error detection amplifier, 11...Reference voltage source.

Claims (1)

【特許請求の範囲】[Claims] 1 情報信号を着磁により記録した情報記録媒体
に磁気感応素子を近接して対向し、この磁気感応
素子と上記情報記録媒体との相対的な移動により
前記情報信号を前記磁気感応素子より得る磁気式
エンコーダーにおいて、前記磁気感応素子を所定
の位相差をもつてn(≧2)個配列し、このn個
の磁気感応素子の各出力信号をn個の累乗演算器
により各々累乗して加算し、この加算した和電圧
が一定値となるように前記磁気感応素子を制御す
る制御手段を設けたことを特徴とする磁気式エン
コーダー。
1 A magnetically sensitive element is placed close to and facing an information recording medium on which an information signal is recorded by magnetization, and the information signal is obtained from the magnetically sensitive element by relative movement between the magnetically sensitive element and the information recording medium. In the equation encoder, n (≧2) magnetically sensitive elements are arranged with a predetermined phase difference, and each output signal of the n magnetically sensitive elements is raised to a power by n power calculators and summed. A magnetic encoder comprising: a control means for controlling the magnetically sensitive element so that the added sum voltage becomes a constant value.
JP22359483A 1983-11-28 1983-11-28 Magnetic encoder Granted JPS60114714A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22359483A JPS60114714A (en) 1983-11-28 1983-11-28 Magnetic encoder

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22359483A JPS60114714A (en) 1983-11-28 1983-11-28 Magnetic encoder

Publications (2)

Publication Number Publication Date
JPS60114714A JPS60114714A (en) 1985-06-21
JPH0434684B2 true JPH0434684B2 (en) 1992-06-08

Family

ID=16800611

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22359483A Granted JPS60114714A (en) 1983-11-28 1983-11-28 Magnetic encoder

Country Status (1)

Country Link
JP (1) JPS60114714A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6312915A (en) * 1986-07-03 1988-01-20 Yamaha Corp Detection signal processing circuit for encoder
US4705969A (en) * 1986-09-19 1987-11-10 National Semiconductor Corporation High accuracy tachometer circuit
JPH01269014A (en) * 1988-04-21 1989-10-26 Japan Servo Co Ltd Temperature compensation circuit for magnetic encoder
JP3312504B2 (en) * 1994-09-30 2002-08-12 ソニー・プレシジョン・テクノロジー株式会社 Position detection device

Also Published As

Publication number Publication date
JPS60114714A (en) 1985-06-21

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