JPH04110917U - Magnetoelectric conversion type rotation angle detection device - Google Patents
Magnetoelectric conversion type rotation angle detection deviceInfo
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- 230000008859 change Effects 0.000 abstract description 7
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Abstract
(57)【要約】
【目的】 磁電変換素子(センサ)の出力信号を両磁界
方式で波形整形できるようにしてセンサの検知能力を向
上させ、かつ組立てを容易にする。
【構成】 回転子1に装着された着磁リング2にAB相
着磁帯3とZ相着磁帯7を形成する。Z相着磁帯7は1
個の基準磁極と、この両端に繋がる逆極性のバックグラ
ウンドからなる。AB相着磁帯3は極性が異なる複数の
磁極を交互に配している。これらAB相着磁帯3とZ相
着磁帯7との中間にはバックグラウンドと同極性の中間
着磁帯8を設ける。Z相センサ6から出力される電気信
号は基準磁極とバックグラウンドとの境界でのみ変化点
を有する。したがって両方磁界方式で波形整形しても回
転角検知の基準点を容易に認識できる。また両方磁界方
式の波形整形によれば、検知能力が向上してセンサ6と
着磁帯7との間隙調整が容易となる。
(57) [Summary] [Purpose] To improve the detection ability of the sensor and to facilitate its assembly by making it possible to waveform shape the output signal of a magnetoelectric transducer (sensor) using both magnetic field methods. [Structure] An AB phase magnetized zone 3 and a Z phase magnetic zone 7 are formed on a magnetized ring 2 mounted on a rotor 1. Z-phase magnetic belt 7 is 1
It consists of two reference magnetic poles and a background of opposite polarity connected to both ends of the reference magnetic poles. The AB phase polarized magnetic belt 3 has a plurality of magnetic poles having different polarities arranged alternately. An intermediate magnetized zone 8 having the same polarity as the background is provided between the AB phase magnetic zone 3 and the Z phase magnetic zone 7. The electrical signal output from the Z-phase sensor 6 has a change point only at the boundary between the reference magnetic pole and the background. Therefore, even if waveform shaping is performed using both magnetic field methods, the reference point for rotation angle detection can be easily recognized. Further, according to the waveform shaping of the dual magnetic field method, the detection ability is improved and the gap between the sensor 6 and the magnetized belt 7 can be easily adjusted.
Description
【0001】0001
本考案は磁電変換式回転角検知装置に関するものであり、特に、回転角の被検 知物である回転体に施された着磁帯を改良した磁電変換式回転角検知装置に関す るものである。 The present invention relates to a magneto-electric conversion type rotation angle detection device, and is particularly applicable to rotation angle detection devices. Concerning a magneto-electric conversion type rotation angle detection device that improves the well-known magnetized band applied to a rotating body. It is something that
【0002】0002
図5は従来の磁電変換式回転角検知装置の一例を示す斜視図およびその要部拡 大図である。同図において、回転角の被検知物である回転体(図示せず)に装着 される回転子1の端部には所望の着磁を施すための着磁リング2が嵌着されてい る。着磁リング2には、その全周に亘ってN極およびS極が交互に着磁されたA B相着磁帯3と、N極,S極のいずれか一方の極を他方の極で挟む形で着磁リン グ2の一部に着磁されたZ相着磁帯4とが設けられている。 Figure 5 is a perspective view showing an example of a conventional magneto-electric conversion type rotation angle detection device and an enlarged view of its main parts. It's a big picture. In the same figure, it is attached to a rotating body (not shown) that is the object to be detected for the rotation angle. A magnetizing ring 2 is fitted onto the end of the rotor 1 to provide desired magnetization. Ru. The magnetized ring 2 has an A magnet with N and S poles alternately magnetized around its entire circumference. B-phase magnetized belt 3 and a magnetized ring with either N pole or S pole sandwiched between the other pole. A Z-phase magnetized zone 4 is provided in a part of the magnetic field 2.
【0003】 着磁リング2の外周面に対して、所定の間隙を有して磁電変換素子5および6 が配設されている。一方の磁電変換素子5(以下、AB相センサ5という)はA B相着磁帯3と対向する位置に配され、他方の磁電変化素子6(以下、Z相セン サという)はZ相着磁帯4と対向する位置に配されている。0003 Magnetoelectric transducers 5 and 6 are arranged with a predetermined gap on the outer peripheral surface of the magnetized ring 2. is installed. One magnetoelectric conversion element 5 (hereinafter referred to as AB phase sensor 5) is A The other magnetoelectric change element 6 (hereinafter referred to as Z-phase sensor) (referred to as "sa") is arranged at a position facing the Z-phase magnetized belt 4.
【0004】 AB相センサ5は、回転子1が矢印11の方向に回転するのに伴ってAB相着 磁帯3のN極およびS極から交互に磁気作用を受け、正弦波信号を出力する。こ の正弦波信号は図示しない波形整形手段に供給されて矩形波信号に整形され、そ の矩形波信号のパルス数を計数することによって回転子1の回転角を検知するこ とができる。0004 The AB phase sensor 5 detects the AB phase as the rotor 1 rotates in the direction of the arrow 11. It receives magnetic action alternately from the north and south poles of the magnetic belt 3, and outputs a sine wave signal. child The sine wave signal is supplied to a waveform shaping means (not shown) and shaped into a rectangular wave signal. The rotation angle of the rotor 1 can be detected by counting the number of pulses of the square wave signal. I can do that.
【0005】 同様に、Z相センサ6もZ相着磁帯4による磁界の作用で正弦波信号を出力す る。但し、こちらの場合は着磁リングの全周ではなく、一部に着磁されているだ けなので、連続して正弦波信号が出力されるのではない。つまり回転子1の1回 転についてZ相着磁部4とZ相センサ6とが対向する位置においてのみ正弦波信 号が出力されることになる。このように正弦波信号は限定された範囲でのみ出力 されるので、この信号に基づいて回転子1の1回転中における位置を特定でき、 この位置を回転角検知の基準点とすることができる。なお、図5(b)に示した ようにこの従来装置では、Z相着磁帯4はS極をN極で挟む配置にしているが、 その逆にN極をS極で挟むような配置もある。[0005] Similarly, the Z-phase sensor 6 also outputs a sine wave signal due to the effect of the magnetic field from the Z-phase magnetized belt 4. Ru. However, in this case, the magnetized ring is not magnetized all the way around it, but only a part of it is magnetized. Therefore, a sine wave signal is not output continuously. In other words, once for rotor 1 A sine wave signal is generated only at the position where the Z-phase magnetized part 4 and the Z-phase sensor 6 face each other regarding rotation. The number will be output. In this way, the sine wave signal is output only within a limited range. Therefore, based on this signal, the position of the rotor 1 during one rotation can be specified, This position can be used as a reference point for rotation angle detection. In addition, as shown in Fig. 5(b) In this conventional device, the Z-phase magnetized belt 4 is arranged so that the S pole is sandwiched between the N poles. On the other hand, there is also an arrangement in which the north pole is sandwiched between the south poles.
【0006】[0006]
上記した従来の磁電変換式回転角検知装置には、次のような問題点があった。 図6に従来の磁電変換式回転角検知装置で得られるZ相センサ6の出力信号波形 を示す。同図において、正弦波信号SWはN極側のしきい値ThnとS極側のし きい値Thsとに従ってパルス整形され、矩形波信号PWに変換される。このよ うに、N極およびS極の両側にしきい値を設定して波形整形する方式を両磁界方 式と呼ぶ。 The conventional magneto-electric conversion type rotation angle detection device described above has the following problems. Figure 6 shows the output signal waveform of the Z-phase sensor 6 obtained by a conventional magneto-electric conversion type rotation angle detection device. shows. In the figure, the sine wave signal SW has a threshold value Thn on the north pole side and a threshold value Thn on the south pole side. The pulse is shaped according to the threshold Ths and converted into a rectangular wave signal PW. This way In other words, a method for shaping the waveform by setting thresholds on both sides of the N and S poles is applied to both magnetic fields. It's called a ceremony.
【0007】 この両磁界方式では図示のように、Z相着磁帯4によって得られるZ相センサ 6の出力信号の波形には、オフからオンへの変化点がS1,S2の2か所に現れ る。矩形波信号PWの立上がりを検出して回転基準を認識する検知装置では、余 計な変化点S1が現れる矩形波PWでは回転基準の認識が困難となって処理回路 が複雑になるという問題点があった。[0007] In this dual magnetic field method, as shown in the figure, the Z-phase sensor obtained by the Z-phase magnetized belt 4 In the waveform of the output signal of No. 6, two points of change from off to on appear at S1 and S2. Ru. The detection device that detects the rising edge of the rectangular wave signal PW and recognizes the rotation reference In the square wave PW where a sudden change point S1 appears, it becomes difficult to recognize the rotation reference, and the processing circuit The problem was that it became complicated.
【0008】 このような変化点S1が現れないようにするためには、しきい値Thnおよび Thsの双方をS極側に設定するようにすればよい。このようにしきい値を片方 の磁極側に設定して波形整形する方式を片磁界方式と呼ぶ。 この片磁界方式では、正弦波信号SWの幅を有効に使用できないため、Z相セ ンサ6と着磁リング2との間隙調整に高い精度を要求される。また、高精度を維 持できない場合は、Z相着磁帯4の磁力を強くし、正弦波信号SWの振幅を大き くしなければならない。[0008] In order to prevent such a change point S1 from appearing, thresholds Thn and Both Ths may be set to the south pole side. In this way, set the threshold to one side. The method of shaping the waveform by setting it on the magnetic pole side is called the single-field method. In this single magnetic field method, the width of the sine wave signal SW cannot be used effectively, so the Z-phase High precision is required for adjusting the gap between the sensor 6 and the magnetized ring 2. It also maintains high accuracy. If this is not possible, increase the magnetic force of the Z-phase magnetic belt 4 and increase the amplitude of the sine wave signal SW. I have to comb it.
【0009】 前記Z相センサ6と着磁リング2との間隙を正確に調整するには、長い調整時 間が必要となったり調整用の治具が必要となったりする。一方、Z相着磁帯4の 磁力を強くするとAB相着磁帯3に影響が出るため、AB着磁帯3の個々の磁極 を小さくできない、つまり分解能が低下するという問題点も生じる。[0009] In order to accurately adjust the gap between the Z-phase sensor 6 and the magnetized ring 2, it is necessary to This may require additional time or a jig for adjustment. On the other hand, the Z-phase magnetic belt 4 If the magnetic force is strengthened, it will affect the AB phase magnetized zone 3, so the individual magnetic poles of the AB phase magnetic zone 3 will be There also arises the problem that it is not possible to make the image smaller, that is, the resolution is reduced.
【0010】 このように、Z相センサ6の出力波形は両磁界方式で整形する方が利点が多い が、従来の着磁帯では上述のように両磁界方式を使用できないという問題点があ った。0010 In this way, there are many advantages to shaping the output waveform of the Z-phase sensor 6 using both magnetic field methods. However, as mentioned above, conventional magnetized belts have the problem that both magnetic field methods cannot be used. It was.
【0011】 本考案の目的は、前述の問題点を解決し、センサ出力の処理や取付け調整を複 雑にしないでZ相センサ6の出力波形を両磁界方式によって整形できる磁電変換 式回転角検知装置を提供することにある。[0011] The purpose of this invention is to solve the above-mentioned problems and to make it easier to process sensor output and to make installation adjustments easier. Magnetoelectric conversion that allows the output waveform of the Z-phase sensor 6 to be shaped using both magnetic field methods without complication An object of the present invention is to provide a rotation angle detection device based on the above-described method.
【0012】0012
前記の問題点を解決するために、本考案は、1個の基準磁極およびこの基準磁 極の両端に繋がり、かつ基準磁極とは逆極性のバックグラウンド磁極からなる環 状のZ相着磁帯と、異なる極性の磁極を交互に配してなる環状のAB相着磁帯と 、前記Z相着磁帯およびAB相着磁帯の中間に設けられた環状磁性体と、前記Z 相着磁帯に対向して配設された回転基準検知用Z相センサと、前記AB相着磁帯 に対向して配設された回転角検知用AB相センサとを具備すると共に、前記各着 磁帯は回転角被検知物体の回転方向に沿って配設された点に特徴がある。 In order to solve the above problems, the present invention provides one reference magnetic pole and this reference magnetic pole. A ring consisting of a background magnetic pole connected to both ends of the pole and of opposite polarity to the reference magnetic pole. A Z-phase magnetized belt with a shape, and an annular AB-phase magnetized belt with magnetic poles of different polarities arranged alternately. , an annular magnetic body provided between the Z phase magnetized zone and the AB phase magnetic zone; a Z-phase sensor for rotation reference detection disposed opposite to the complementary magnetic belt; and the AB complementary magnetic belt. and an AB phase sensor for rotational angle detection disposed opposite to each other. The magnetic belt is characterized in that it is arranged along the rotation direction of the object whose rotation angle is to be detected.
【0013】[0013]
Z相センサの出力波形は、これを両磁界方式で整形した場合でも回転子の1回 転につきオフからオンへの変化点は1か所、つまり基準磁極とバックグラウンド 磁極との境界の一方でしか現れないので、この変化点に基づいて回転角検知の基 準点を容易に認識できる。また、AB着磁帯とZ相着磁帯との間に設けられた環 状磁性体によってZ相着磁帯の磁力がAB相着磁帯で形成される磁界に影響を及 ぼすのを防止できる。 Even when the output waveform of the Z-phase sensor is shaped using both magnetic field methods, the output waveform of the Z-phase sensor is There is only one change point from off to on per cycle, namely the reference magnetic pole and the background. Since it only appears on one side of the boundary with the magnetic pole, the rotation angle detection is based on this change point. Quasi-points can be easily recognized. In addition, a ring provided between the AB magnetized zone and the Z phase magnetized zone The magnetic force of the Z-phase magnetized zone influences the magnetic field formed by the AB-phase magnetic zone due to the shaped magnetic body. It can prevent spills.
【0014】[0014]
以下に図面を参照して、本考案を詳細に説明する。図1は本考案の一実施例を 示す磁電変換式回転角検知装置の斜視図およびその要部拡大図であり、図5と同 符号は同一または同等部分を示す。 同図において、回転子1に装着された着磁リング2の円周方向には、AB相着 磁帯3と、Z相着磁帯7とが設けられている。AB相着磁帯3は、多数のN極お よびS極が交互に配置されて環状を形成した着磁帯である。一方、Z相着磁帯7 は、基準磁極となるS極と、この基準磁極に連続し、バックグラウンド磁極とな るN極とで環状を形成した着磁帯である。 The present invention will be described in detail below with reference to the drawings. Figure 1 shows an example of the present invention. 5 is a perspective view and an enlarged view of the main parts of the magneto-electric conversion type rotation angle detection device shown in FIG. Codes indicate the same or equivalent parts. In the same figure, in the circumferential direction of the magnetized ring 2 attached to the rotor 1, there are A magnetic belt 3 and a Z-phase magnetic belt 7 are provided. The AB phase polarized magnetic belt 3 has many N poles and This is a magnetized belt in which the and S poles are arranged alternately to form an annular shape. On the other hand, Z-phase magnetic belt 7 is the S pole, which is the reference magnetic pole, and the S pole, which is continuous with this reference magnetic pole and is the background magnetic pole. This is a magnetized belt that forms an annular shape with the N pole.
【0015】 本実施例において、Z相着磁帯7の基準磁極であるS極の大きさつまりZ相着 磁帯の環状方向(長さ方向)寸法lは、前記AB相着磁帯3の1つの磁極の大き さとほぼ同一にしているが、これは任意に設定できる。要は、Z相着磁帯7の回 転子1の回転方向に沿った環状領域、つまり回転子1の円周領域の一部分をN極 またはS極の基準磁極で着磁し、それとは逆極性の磁極でこの基準磁極の両側に 繋がるバックグラウンド磁極が形成されていればよい。 AB相着磁帯3とZ相着磁帯7との間には、Z相着磁帯7に隣接して中間着磁 帯8が形成されている。この中間着磁帯8は前記基準磁極と同じ極性すなわちS 極に着磁される。[0015] In this embodiment, the size of the S pole, which is the reference magnetic pole of the Z-phase magnetized belt 7, that is, the Z-phase polarization The annular direction (longitudinal direction) dimension l of the magnetic belt is the size of one magnetic pole of the AB compatible magnetic belt 3. It is set almost the same as , but this can be set arbitrarily. In short, the rotation of the Z-phase magnetic belt 7 The annular region along the rotation direction of the trochanter 1, that is, a part of the circumferential region of the rotor 1 is set as the N pole. Alternatively, magnetize with the S-pole reference magnetic pole, and use magnetic poles of opposite polarity on both sides of this reference magnetic pole. It is sufficient that connected background magnetic poles are formed. Between the AB phase magnetized zone 3 and the Z phase magnetic zone 7, there is an intermediate magnetized zone adjacent to the Z phase magnetic zone 7. A band 8 is formed. This intermediate magnetized belt 8 has the same polarity as the reference magnetic pole, that is, S It is magnetized to the pole.
【0016】 次に、上記の着磁が施されたAB相着磁帯3およびZ相着磁帯7の磁界の作用 によってAB相センサ5およびZ相センサ6から出力される信号の波形を示す。 図2はZ相センサ6から出力される信号波形を示す図であり、図3はAB相セン サ5から出力される信号波形を示す図である。 図2および図3において、“1回転”と示した分が、回転子1の1回転によっ てAB相センサ5およびZ相センサ6から出力される信号である。このように、 信号がオフからオンへ変化するのは回転子1の1回転中に1回のみである。[0016] Next, the effect of the magnetic field of the AB-phase magnetized belt 3 and the Z-phase magnetized belt 7 that have been magnetized as described above will be explained. 3 shows the waveforms of the signals output from the AB phase sensor 5 and the Z phase sensor 6. 2 is a diagram showing the signal waveform output from the Z-phase sensor 6, and FIG. 3 is a diagram showing the signal waveform output from the Z-phase sensor 6. 5 is a diagram showing a signal waveform output from the sensor 5. FIG. In Figs. 2 and 3, the amount indicated as “one rotation” is due to one rotation of rotor 1. This is a signal output from the AB phase sensor 5 and the Z phase sensor 6. in this way, The signal changes from off to on only once during one revolution of the rotor 1.
【0017】 なお、図3において鎖線で示した波形SWdは、前記中間着磁帯8を設けなか った場合のAB相センサ5の出力波形である。図示のように、中間着磁帯8を設 けない場合は、バックグラウンド磁極であるN極の影響を受け、AB相センサ5 に作用するAB相着磁帯3のN極の磁束数が減少し、逆にS極の磁束数が増加す るため波形の中点がS極側にずれるのである。このように、バックグラウンド磁 極はAB相センサの出力に与える影響を排除するために設けられる。[0017] Note that the waveform SWd shown by the chain line in FIG. This is the output waveform of the AB phase sensor 5 when As shown in the figure, an intermediate magnetized zone 8 is provided. If the AB phase sensor 5 The number of magnetic fluxes at the N pole of the AB complementary magnetic belt 3 that acts on the magnetic field decreases, and conversely, the number of magnetic fluxes at the S pole increases. As a result, the midpoint of the waveform shifts toward the south pole. In this way, the background magnetic The poles are provided to eliminate any influence on the output of the AB phase sensor.
【0018】 以上説明した実施例では、各着磁帯を回転子1の円周に装着した着磁リング2 の上に形成したが、回転子1または回転角の被検知物体に直接着磁するようにし てもよい。また、着磁位置は回転子1や着磁リング2の円周に限らず、被検知物 体の形状や大きさに応じ、回転子1や被検知物体の他の面に設けても良い。すな わち、被検知物体である回転体の回転方向に着磁帯が沿って形成されていればよ い。[0018] In the embodiment described above, the magnetized ring 2 has each magnetized band attached to the circumference of the rotor 1. The magnet is formed on the rotor 1 or the object to be detected at the rotation angle is directly magnetized. It's okay. In addition, the magnetized position is not limited to the circumference of the rotor 1 or the magnetized ring 2, but also Depending on the shape and size of the body, it may be provided on other surfaces of the rotor 1 or the object to be detected. sand In other words, it is better if the magnetized band is formed along the rotation direction of the rotating body that is the object to be detected. stomach.
【0019】 図4は、被検知物体の端面にAB相着磁帯3およびZ相着磁帯7ならびに中間 着磁帯8を形成した例である。同図において、被検知物体9は矢印11の方向に 回転する物体であり、その端面10に、直径の異なる環状の着磁帯3,7,8が それぞれ形成されている。[0019] FIG. 4 shows an AB phase magnetic zone 3, a Z phase magnetic zone 7, and an intermediate magnetic zone on the end face of the object to be detected. This is an example in which a magnetized band 8 is formed. In the figure, the detected object 9 is in the direction of the arrow 11. It is a rotating object, and its end face 10 has annular magnetized bands 3, 7, and 8 with different diameters. each formed.
【0020】 なお、中間着磁帯8は積極的に着磁させる代わりに、鉄などの磁性体で環状の シールド領域を形成することによっても本実施例と同様の効果が得られる。[0020] Note that instead of being actively magnetized, the intermediate magnetized zone 8 is made of a ring-shaped magnetic material such as iron. The same effects as in this embodiment can also be obtained by forming a shield region.
【0021】[0021]
以上の説明から明らかなように、本考案によれば、両磁界方式によってZ相セ ンサの出力を整形した場合でも、センサの出力が単純化されているので回転の基 準点を容易に認識できる。したがって、両磁界方式を使用できるようになり、着 磁帯の磁界をセンサに有効に作用させることができる。その結果、Z相センサの 検知能力が上がり、取付け公差を緩和できる。 As is clear from the above explanation, according to the present invention, Z-phase separation is achieved using both magnetic field methods. Even if the output of the sensor is shaped, the basis of rotation is Quasi-points can be easily recognized. Therefore, both magnetic field methods can be used and The magnetic field of the magnetic belt can be effectively applied to the sensor. As a result, the Z phase sensor Detection ability is increased and installation tolerances can be relaxed.
【図1】本考案の実施例を示す回転角検知装置の斜視図
である。FIG. 1 is a perspective view of a rotation angle detection device showing an embodiment of the present invention.
【図2】Z相センサの出力波形を示す図である。FIG. 2 is a diagram showing an output waveform of a Z-phase sensor.
【図3】AB相センサの出力波形を示す図である。FIG. 3 is a diagram showing an output waveform of an AB phase sensor.
【図4】第2実施例を示す回転角検知装置の斜視図であ
る。FIG. 4 is a perspective view of a rotation angle detection device showing a second embodiment.
【図5】従来技術を示す回転角検知装置の斜視図であ
る。FIG. 5 is a perspective view of a rotation angle detection device showing a prior art.
【図6】従来技術のZ相センサの出力波形を示す図であ
る。FIG. 6 is a diagram showing an output waveform of a conventional Z-phase sensor.
1…回転子、 2…着磁リング、 3…AB相着磁帯、
4,7…Z相着磁帯、8…中間着磁帯、 9…被検知
物体1... Rotor, 2... Magnetized ring, 3... AB complementary magnetized belt,
4, 7...Z phase magnetized belt, 8...Intermediate magnetized belt, 9...Detected object
───────────────────────────────────────────────────── フロントページの続き (72)考案者 古海 洋 埼玉県和光市中央一丁目4番1号 株式会 社本田技術研究所内 ──────────────────────────────────────────────── ─── Continuation of front page (72) Creator Hiroshi Furukai 1-4-1 Chuo, Wako City, Saitama Prefecture Co., Ltd. Inside Honda Technical Research Institute
Claims (3)
置された着磁帯を有し、この着磁帯の磁気作用によって
磁電変換素子から出力される電気信号に基づいて回転体
の回転角を検知する磁電変換式回転角検知装置におい
て、1個の基準磁極およびこの基準磁極の両端に繋が
り、かつ基準磁極と逆極性のバックグラウンド磁極から
なる環状のZ相着磁帯と、異なる極性の磁極を交互に配
してなる環状のAB相着磁帯と、前記Z相着磁帯および
AB相着磁帯の中間に設けられた環状磁性体と、前記Z
相着磁帯に対向して配設された回転基準検知用Z相セン
サと、前記AB相着磁帯に対向して配設された回転角検
知用AB相センサとを具備すると共に、前記各着磁帯は
回転角被検知物体の回転方向に沿って配設されたことを
特徴とする磁電変換式回転角検知装置。Claim 1: The object to be detected has a magnetized band in which magnetic poles are arranged alternately, and the rotating body is rotated based on an electric signal output from a magnetoelectric transducer due to the magnetic action of the magnetized band. In a magneto-electric conversion type rotation angle detection device that detects an angle, an annular Z-phase magnetized band consisting of a reference magnetic pole and a background magnetic pole connected to both ends of the reference magnetic pole and having a polarity opposite to that of the reference magnetic pole, and an annular AB phase magnetized zone formed by alternately arranging magnetic poles; an annular magnetic body provided between the Z phase magnetized zone and the AB phase magnetized zone;
A Z-phase sensor for rotation reference detection disposed facing the mutually magnetized belt, and an AB phase sensor for rotational angle detection disposed facing the AB phase magnetized belt, and each of the above-mentioned A magneto-electric conversion type rotation angle detection device characterized in that the magnetized belt is arranged along the rotation direction of an object whose rotation angle is to be detected.
長さ方向寸法が、前記AB相着磁帯の各磁極の同方向寸
法以下であることを特徴とする請求項1記載の磁電変換
式回転角検知装置。2. The reference magnetic pole of the Z-phase magnetized zone has a longitudinal dimension of the magnetized zone that is equal to or smaller than the dimension in the same direction of each magnetic pole of the AB-phase magnetized zone. The magneto-electric conversion type rotation angle detection device described above.
性の着磁帯であることを特徴とする請求項1記載の磁電
変換式回転角検知装置。3. The magnetoelectric conversion type rotation angle detection device according to claim 1, wherein the annular magnetic body is a magnetized band having the same polarity as the reference electrode.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2091491U JP2523654Y2 (en) | 1991-03-11 | 1991-03-11 | Magnetoelectric conversion rotation angle detector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2091491U JP2523654Y2 (en) | 1991-03-11 | 1991-03-11 | Magnetoelectric conversion rotation angle detector |
Publications (2)
Publication Number | Publication Date |
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JPH04110917U true JPH04110917U (en) | 1992-09-25 |
JP2523654Y2 JP2523654Y2 (en) | 1997-01-29 |
Family
ID=31906875
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JP2091491U Expired - Fee Related JP2523654Y2 (en) | 1991-03-11 | 1991-03-11 | Magnetoelectric conversion rotation angle detector |
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JP (1) | JP2523654Y2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2009216590A (en) * | 2008-03-11 | 2009-09-24 | Makome Kenkyusho:Kk | Absolute value type magnetic scale device |
-
1991
- 1991-03-11 JP JP2091491U patent/JP2523654Y2/en not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2009216590A (en) * | 2008-03-11 | 2009-09-24 | Makome Kenkyusho:Kk | Absolute value type magnetic scale device |
Also Published As
Publication number | Publication date |
---|---|
JP2523654Y2 (en) | 1997-01-29 |
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