JPS63171026A - Magnetic encoder - Google Patents
Magnetic encoderInfo
- Publication number
- JPS63171026A JPS63171026A JP232787A JP232787A JPS63171026A JP S63171026 A JPS63171026 A JP S63171026A JP 232787 A JP232787 A JP 232787A JP 232787 A JP232787 A JP 232787A JP S63171026 A JPS63171026 A JP S63171026A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- detector
- magnetic field
- disk
- generating means
- 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
Links
- 230000005291 magnetic effect Effects 0.000 title claims abstract description 105
- 238000001514 detection method Methods 0.000 claims description 8
- 239000000463 material Substances 0.000 claims description 4
- 229910000889 permalloy Inorganic materials 0.000 claims description 2
- 230000005389 magnetism Effects 0.000 abstract description 5
- 239000002184 metal Substances 0.000 abstract description 3
- 238000006073 displacement reaction Methods 0.000 abstract 2
- 238000010586 diagram Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 238000005516 engineering process Methods 0.000 description 3
- 239000000696 magnetic material Substances 0.000 description 3
- 238000007796 conventional method Methods 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000005355 Hall effect Effects 0.000 description 1
- 238000005553 drilling Methods 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 230000005294 ferromagnetic effect Effects 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000000779 smoke Substances 0.000 description 1
- 230000000087 stabilizing effect Effects 0.000 description 1
Landscapes
- Analogue/Digital Conversion (AREA)
Abstract
Description
【発明の詳細な説明】
〔]既要〕
磁気パルス列に磁気検出手段を組み合わせてなる磁気エ
ンコーダにおいて、
該磁気パルス列が磁気発生手段と、磁気遮蔽材料の板に
スリット列を穿設してなる磁気遮蔽手段とで構成したこ
とにより、
高分解能の磁気エンコーダを実現したものである。[Detailed Description of the Invention] [Already Required] A magnetic encoder comprising a magnetic pulse train combined with a magnetic detection means, wherein the magnetic pulse train is a magnetic encoder formed by combining a magnetic generating means and a magnetic shielding material plate with a slit row. By configuring it with shielding means, a high-resolution magnetic encoder was realized.
本発明は印字ヘッドの位置検出や回転体の回転角度を検
出する等に利用する磁気エンコーダ、特に高分解能の磁
気エンコーダを提供する新規構成に関する。The present invention relates to a magnetic encoder used for detecting the position of a print head or the rotation angle of a rotating body, and particularly to a novel configuration for providing a high-resolution magnetic encoder.
第4図は従来の磁気エンコーダの主要構成例を示す斜視
図であり、回転角度を検出するための磁気エンコーダ1
1は、同極面同士が接するように多数個の磁気パターン
12をリング状に配設した回転体13と、回転体13の
上方に配設した磁気検出器14を具えてなる。FIG. 4 is a perspective view showing an example of the main configuration of a conventional magnetic encoder.
1 includes a rotating body 13 in which a large number of magnetic patterns 12 are arranged in a ring shape so that the same polar surfaces are in contact with each other, and a magnetic detector 14 disposed above the rotating body 13.
かかる磁気エンコーダ11において、回転体13を例え
ばモータの回転軸に装着し、該モータを駆動させると回
転体13が回転し、適宜な手段で固着した磁気検出器1
4は、磁気パターン12の境界の通過数を検出回路で計
数し、その該測定値から回転軸の回転角度を検出できる
。In such a magnetic encoder 11, the rotating body 13 is attached to the rotating shaft of a motor, for example, and when the motor is driven, the rotating body 13 rotates, and the magnetic detector 1 fixed by an appropriate means is rotated.
4, the number of times the boundary of the magnetic pattern 12 has passed is counted by a detection circuit, and the rotation angle of the rotating shaft can be detected from the measured value.
磁気パルス列または磁気検出器の移動からその移動量を
検知する磁気エンコーダは、煙霧等に妨げられず移動物
体の位置や回転角度を検知可能である。しかし、従来の
ものは非磁性体上に磁性体を塗布し、該磁性体に磁気パ
ターンを着磁するという製造上の煩わしさがあると共に
、幅Wが数no++程度の該磁気パターンの長さしは、
製造技術的に40μm程度が限度であり、分解能をさら
に向上させ高精度化したい要望は、磁気パターンの長さ
Lを小さくできないことが障害となって、実現しないと
いう問題点があった。A magnetic encoder that detects the amount of movement of a magnetic pulse train or a magnetic detector can detect the position and rotation angle of a moving object without being hindered by smoke or the like. However, in the conventional method, a magnetic material is coated on a non-magnetic material and a magnetic pattern is magnetized on the magnetic material, which is a manufacturing hassle. Shiha,
The production technology has a limit of about 40 .mu.m, and the desire to further improve the resolution and achieve higher precision has been hindered by the inability to reduce the length L of the magnetic pattern, which has been a problem.
第1図は本発明の基本構成例を示す斜視図(イ)と、そ
の出力特性の模式図(+7)である。FIG. 1 is a perspective view (A) showing an example of the basic configuration of the present invention, and a schematic diagram (+7) of its output characteristics.
第1図(イ)において、磁界発生手段1と磁気ヰ★出手
段2の対向間に帯状の磁気遮蔽手段く磁気遮蔽板)3を
配設し、磁界発生手段1と磁気遮蔽手段3の対向関係を
維持しながら磁界発生手段1と磁気検出手段2または、
整列する複数のスリット4をピッチpで穿設してなる磁
気遮蔽手段3の少なくとも一方が、スリット4の整列方
向(矢印A方向)に移動可能に構成してなる。In FIG. 1(A), a strip-shaped magnetic shielding means (magnetic shielding plate) 3 is arranged between the magnetic field generating means 1 and the magnetic shielding means 2, and the magnetic field generating means 1 and the magnetic shielding means 3 are opposed to each other. The magnetic field generating means 1 and the magnetic detecting means 2 while maintaining the relationship, or
At least one of the magnetic shielding means 3, which is formed by forming a plurality of aligned slits 4 at a pitch p, is configured to be movable in the direction in which the slits 4 are aligned (in the direction of arrow A).
かかる磁気エンコーダにおいて、磁界発生手段1が発生
する上向き磁界5の一部5b (図示せず)は磁気遮蔽
手段3に吸収され、他の一部5aはスリット4を通過し
磁気検出手段2に入力する。In such a magnetic encoder, a part 5b (not shown) of the upward magnetic field 5 generated by the magnetic field generating means 1 is absorbed by the magnetic shielding means 3, and the other part 5a passes through the slit 4 and is input to the magnetic detecting means 2. do.
すると、磁気検出手段2は第1図(ロ)に示すように、
スリット4のピッチpに対応するピークを生しる出力が
得られる。Then, the magnetic detection means 2, as shown in FIG. 1 (b),
An output that produces a peak corresponding to the pitch p of the slits 4 is obtained.
第1図においてスリット4の幅すは、エツチング技術を
利用する等によって5μm程度に形成することが可能で
あり、幅すが5μmのスリット4をピッチlOμmで形
成した磁気エンコーダの分解能は、回転ドラム上に着磁
された磁気パターンを利用した従来の磁気エンコーダの
4倍になる。In Fig. 1, the width of the slit 4 can be formed to about 5 μm by using etching technology, etc., and the resolution of a magnetic encoder in which the slit 4 with a width of 5 μm is formed at a pitch of 10 μm is the same as that of a rotating drum. This is four times as large as a conventional magnetic encoder that uses a magnetic pattern magnetized on top.
以下に、図面を用いて本発明の実施例による磁気エンコ
ーダを説明する。EMBODIMENT OF THE INVENTION Below, the magnetic encoder by the Example of this invention is demonstrated using drawing.
第2図は本発明の一実施例による回転磁気エンコーダの
側面図(イ)とその回転円板の平面図(0)、第3図は
磁気検出測定系の回路図である。FIG. 2 is a side view (A) of a rotary magnetic encoder according to an embodiment of the present invention and a plan view (0) of its rotating disk, and FIG. 3 is a circuit diagram of a magnetic detection measurement system.
第2図において、回転軸21の回転角度を検出する磁気
エンコーダ24は、例えばパーマロイの如く磁気を遮蔽
する材料を使用し多数のスリット25を同一円周上に一
定の角度ピンチで形成した円板(磁気遮蔽手段)26と
、磁界発生手段1に相当する永久磁石27および、磁気
抵抗素子を収容し磁気検出手段2に相当する磁気検出器
28を具え、永久磁石27と磁気検出器28は円板26
のスリット25形成部を挟んで対向するように、適宜の
手段で固着される。In FIG. 2, a magnetic encoder 24 that detects the rotation angle of the rotating shaft 21 is a disc made of a material that shields magnetism, such as permalloy, and in which a large number of slits 25 are formed on the same circumference with a fixed angle pinch. (Magnetic shielding means) 26, a permanent magnet 27 corresponding to the magnetic field generating means 1, and a magnetic detector 28 containing a magnetic resistance element and corresponding to the magnetic detecting means 2, the permanent magnet 27 and the magnetic detector 28 being circular. Board 26
are fixed by appropriate means so as to face each other across the slit 25 forming portion.
なお図中において、22は回転軸21と一体に形成した
フランジ、23は円板26をフランジ22の前面に固着
させるための締め付は金具である。In the figure, 22 is a flange formed integrally with the rotating shaft 21, and 23 is a metal fitting for fixing the disk 26 to the front surface of the flange 22.
このように構成した磁気エンコーダ24において、永久
磁石27が発生する磁界29の一部29b(図示せず)
は円板26に遮蔽され、他の一部29aはスリット25
を通過し磁気検出器28に入射する。そこで、回転軸2
1を回転させると、通過磁界B′のパルス列を検出した
磁気検出器28は、スリット25の穿設ピッチでピーク
の生じる出力を送出するようになる。In the magnetic encoder 24 configured in this way, a portion 29b (not shown) of the magnetic field 29 generated by the permanent magnet 27
is shielded by the disk 26, and the other part 29a is shielded by the slit 25
and enters the magnetic detector 28. Therefore, the rotating shaft 2
1, the magnetic detector 28 detects the pulse train of the passing magnetic field B' and outputs an output that has a peak at the pitch of the slits 25.
第3図において、31は強磁性体の磁気抵抗効果を利用
した磁気検出器280等価回路、32は定電流源、33
は不平衡電圧の調整増幅回路、34は差動増幅回路であ
る。定電流源32の入力端子35に印加する電圧Vをか
えることで磁気検出器2日に印加する電流Iが゛変化可
能であり、磁気検出器28が有するブリッジ抵抗のアン
バランスにより外部磁界と関係なく生じる不平衡電圧は
、可変抵抗Rによって調整することができる。そして、
磁気検出器28の出力は差動増幅回路34を通って、例
えば約100倍に増幅され、出力端子36に接続したデ
ジタルマルチメータやX−Yレコーダ等にて、測定およ
び記録されるようになる。In FIG. 3, 31 is an equivalent circuit of a magnetic detector 280 that utilizes the magnetoresistive effect of a ferromagnetic material, 32 is a constant current source, and 33
34 is an unbalanced voltage adjustment amplifier circuit, and 34 is a differential amplifier circuit. By changing the voltage V applied to the input terminal 35 of the constant current source 32, the current I applied to the magnetic detector 2 can be changed. The unbalanced voltage that arises can be adjusted by a variable resistor R. and,
The output of the magnetic detector 28 passes through a differential amplifier circuit 34 and is amplified, for example, about 100 times, and is measured and recorded by a digital multimeter, an X-Y recorder, etc. connected to an output terminal 36. .
なお、前記実施例において、磁界発生手段1に永久磁石
27を使用し、磁気検出手段2に強磁性金属の磁気抵抗
を利用した磁気検出器28を使用している。これらは、
永久磁石27が電力を使用しないこと、磁気検出器28
が温度変化に対し安定であり微小磁界の検知能力に優れ
るためであるが、本発明はかかる永久磁石27および磁
気検出器28に限定されず、例えば磁界発生手段1に電
磁石を使用し、磁気検出手段2に半導体の磁気抵抗を利
用したものやホール効果を利用したものおよび、磁気ヘ
ッドが使用できることを付記する。In the embodiment described above, a permanent magnet 27 is used as the magnetic field generating means 1, and a magnetic detector 28 using magnetic resistance of ferromagnetic metal is used as the magnetic detecting means 2. these are,
Permanent magnet 27 does not use electric power, magnetic detector 28
This is because it is stable against temperature changes and has excellent ability to detect minute magnetic fields, but the present invention is not limited to such permanent magnets 27 and magnetic detectors 28. For example, an electromagnet may be used as the magnetic field generating means 1 to detect magnetic fields. It should be noted that means 2 can use a method using semiconductor magnetoresistance, a method using the Hall effect, or a magnetic head.
以上説明したように本発明によれば、磁気パルス列のピ
ンチを従来より微細に形成可能であり、分解能を従来の
4倍程度に高めることができた。As explained above, according to the present invention, the pinch of the magnetic pulse train can be formed finer than before, and the resolution can be increased to about four times that of the conventional method.
と共に、磁気遮蔽手段は厚さ0.05〜0 、5mm程
度の薄板を使用して軽量化し、磁気遮蔽手段を移動させ
たときその慣性力が低減し、測定値を安定化された効果
がある。In addition, the magnetic shielding means is lightweight by using a thin plate with a thickness of about 0.05 to 0.5 mm, which reduces the inertial force when the magnetic shielding means is moved, and has the effect of stabilizing the measured values. .
第1図は本発明の基本構成例を示す斜視図とその出力特
性図、
第2図は本発明の一実施例による回転磁気エンコーダの
側面図とその回転円板の平面図、第3図は磁気検出測定
系の回路図、
第4図は従来の磁気エンコーダを示す斜視図、である。
1は磁界発生手段、
2は磁気検出手段、
3は磁気遮蔽手段、
4.25はスリット、
24は磁気エンコーダ、
26は円板(磁気遮蔽手段)、
27は永久磁石(磁界発生手段)、
28は磁気検出器(磁気検出手段)、
pはスリット穿設ピッチ、
を示す。
1ユ穎
一;り
訟気遼脹−P股■移栃方匈
(c7)
$1図FIG. 1 is a perspective view showing an example of the basic configuration of the present invention and its output characteristic diagram. FIG. 2 is a side view of a rotary magnetic encoder according to an embodiment of the present invention and a plan view of its rotating disk. FIG. FIG. 4 is a circuit diagram of a magnetic detection measurement system. FIG. 4 is a perspective view showing a conventional magnetic encoder. 1 is a magnetic field generating means, 2 is a magnetic detecting means, 3 is a magnetic shielding means, 4.25 is a slit, 24 is a magnetic encoder, 26 is a disk (magnetic shielding means), 27 is a permanent magnet (magnetic field generating means), 28 is a magnetic detector (magnetic detection means), and p is a slit drilling pitch. 1 Yu Ying 1; ri suit Qi Liaoyu-P crotch ■ transfer Tochi Fang Huong (c7) $1 figure
Claims (4)
生手段(1)に対向する磁気検出手段(2)と、該磁界
発生手段(1)と該磁気検出手段(2)との対向間に配
設し磁気遮蔽材料の板に適宜の間隔(p)で多数のスリ
ット(4)を整列せしめ穿設した磁気遮蔽手段(3)と
を具え、該磁界発生手段(1)と該磁気検出手段(2)
または、該磁気遮蔽手段(3)の少なくとも一方が該ス
リット(4)の整列方向に移動するように構成したこと
を特徴とする磁気エンコーダ。(1) A magnetic field generating means (1), a magnetic detecting means (2) facing the magnetic field generating means (1) separated by an appropriate amount, and a magnetic field generating means (1) and the magnetic detecting means (2). The magnetic field generating means (1) and the magnetic shielding means (3) are arranged between opposing sides and have a large number of slits (4) arranged and bored in a plate of magnetic shielding material at appropriate intervals (p). Magnetic detection means (2)
Alternatively, a magnetic encoder characterized in that at least one of the magnetic shielding means (3) is configured to move in the direction in which the slits (4) are aligned.
特徴とする前記特許請求の範囲第1項記載の磁気エンコ
ーダ。(2) The magnetic encoder according to claim 1, wherein the magnetic field generating means (1) is a permanent magnet.
とを特徴とする前記特許請求の範囲第1項記載の磁気エ
ンコーダ。(3) The magnetic encoder according to claim 1, wherein the magnetic detection means (2) is a magnetoresistive element.
とする前記特許請求の範囲第1項記載の磁気エンコーダ
。(4) The magnetic encoder according to claim 1, wherein the magnetic shielding material is permalloy.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP232787A JPS63171026A (en) | 1987-01-08 | 1987-01-08 | Magnetic encoder |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP232787A JPS63171026A (en) | 1987-01-08 | 1987-01-08 | Magnetic encoder |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63171026A true JPS63171026A (en) | 1988-07-14 |
Family
ID=11526218
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP232787A Pending JPS63171026A (en) | 1987-01-08 | 1987-01-08 | Magnetic encoder |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63171026A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102019112423A1 (en) * | 2019-05-13 | 2020-11-19 | RUAG Space Germany GmbH | ENCODER |
-
1987
- 1987-01-08 JP JP232787A patent/JPS63171026A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102019112423A1 (en) * | 2019-05-13 | 2020-11-19 | RUAG Space Germany GmbH | ENCODER |
DE102019112423B4 (en) | 2019-05-13 | 2022-07-28 | Beyond Gravity Germany GmbH | ENCODERS |
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