JPH10318705A - Position detecting apparatus - Google Patents
Position detecting apparatusInfo
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- JPH10318705A JPH10318705A JP13202897A JP13202897A JPH10318705A JP H10318705 A JPH10318705 A JP H10318705A JP 13202897 A JP13202897 A JP 13202897A JP 13202897 A JP13202897 A JP 13202897A JP H10318705 A JPH10318705 A JP H10318705A
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- 238000001514 detection method Methods 0.000 claims description 28
- 230000000694 effects Effects 0.000 claims description 4
- 238000000034 method Methods 0.000 abstract description 6
- 238000010586 diagram Methods 0.000 description 8
- 238000004519 manufacturing process Methods 0.000 description 3
- 238000006073 displacement reaction Methods 0.000 description 2
- 230000020169 heat generation Effects 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000010363 phase shift Effects 0.000 description 1
- 238000003908 quality control method Methods 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
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- Transmission And Conversion Of Sensor Element Output (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は例えば工作機械等の
位置検出に適用して好適な位置検出装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a position detecting device suitable for detecting a position of, for example, a machine tool.
【0002】[0002]
【従来の技術及び発明が解決しようとする課題】一般
に、図5に示す如くN極とS極とが繰返し同一ピッチλ
(λはN極とS極との間隔)で、目盛が磁気記録されて
いる磁気スケール1と、磁気抵抗効果素子(MR素子)
を使用した検出ヘッド2との相対位置を検出するように
した位置検出装置が提案されている。2. Description of the Related Art Generally, as shown in FIG. 5, an N pole and an S pole repeatedly have the same pitch λ.
(Λ is the distance between the N pole and the S pole), a magnetic scale 1 on which a scale is magnetically recorded, and a magnetoresistive element (MR element)
There has been proposed a position detecting device which detects a relative position with respect to the detecting head 2 using the method.
【0003】この従来のMR素子を使用した基本的な検
出ヘッド2の一例としては図6Aに示す如く、磁気スケ
ール1の目盛の記録方向にλ/2離れて配置された2個
のMR素子3a及び3bを直列接続し、このMR素子3
aの開放端4aより直流電圧VO を供給すると共にMR
素子3bの開放端4bを接地し、このMR素子3a及び
3bの接続中点より出力端子5aを導出する。As an example of a basic detection head 2 using this conventional MR element, as shown in FIG. 6A, two MR elements 3a arranged at a distance of λ / 2 in the recording direction of the scale of the magnetic scale 1 are used. And 3b are connected in series, and this MR element 3
DC voltage V O is supplied from the open end 4a of
The open end 4b of the element 3b is grounded, and the output terminal 5a is led out from the connection point between the MR elements 3a and 3b.
【0004】また、磁気スケール1の目盛の記録方向
に、λ/2離れて配置された2個のMR素子6a及び6
bを直列接続し、このMR素子6aの開放端7aより直
列電圧VO を供給すると共にMR素子6bの開放端を接
地し、このMR素子6a及び6bの接続中点より出力端
子5bを導出する。In addition, two MR elements 6a and 6a arranged at a distance of λ / 2 in the recording direction of the scale of the magnetic scale 1 are provided.
b are connected in series, the series voltage V O is supplied from the open end 7a of the MR element 6a, the open end of the MR element 6b is grounded, and the output terminal 5b is led out from the midpoint of connection between the MR elements 6a and 6b. .
【0005】この場合、隣接するMR素子3b及び6b
の間隔を磁気スケール1の目盛の記録方向にλ/4離し
て配置し、出力端子5a及び5bに90度(λ/4)位
相のずれた2相出力を得る如くする。In this case, adjacent MR elements 3b and 6b
Are arranged at a distance of λ / 4 in the recording direction of the scale of the magnetic scale 1 so that two-phase outputs having a phase shift of 90 degrees (λ / 4) are obtained at the output terminals 5a and 5b.
【0006】この磁気スケール1とMR素子3a,3
b,6a,6bより成る検出ヘッド2との相対変位によ
り、この出力端子5a及び5bに得られる出力信号は一
般に小さいため、各々図7Aに示す如き出力回路を使用
して90度位相の異なる2相の正弦波信号即ち、sin
及びcosの信号を得ている。The magnetic scale 1 and the MR elements 3a, 3
Since the output signals obtained at the output terminals 5a and 5b are generally small due to the relative displacement with respect to the detection head 2 consisting of b, 6a, and 6b, the output signals having 90 degrees different phases by using output circuits as shown in FIG. 7A. Phase sinusoidal signal, ie, sin
And cos signals.
【0007】この図7Aにつき説明するに出力端子5a
(又は5b)を抵抗器10を介して演算増幅回路11の
反転入力端子−に接続し、また直流電圧VO が供給され
る電源端子12を磁気抵抗効果素子3a,3b(6a,
6b)の抵抗値に対応して決る抵抗値の2個の抵抗器1
3及び14の直列回路を介して接地し、この抵抗器13
及び14の接続点を抵抗器15を介して、この演算増幅
回路11の非反転入力端子+に接続する。The output terminal 5a will be described with reference to FIG.
(Or 5b) is connected to the inverting input terminal of the operational amplifier circuit 11 via the resistor 10, and the power supply terminal 12 to which the DC voltage V O is supplied is connected to the magnetoresistive elements 3a, 3b (6a,
6b) Two resistors 1 having a resistance value determined according to the resistance value
3 and 14 are connected to ground, and this resistor 13
And 14 are connected via a resistor 15 to the non-inverting input terminal + of the operational amplifier circuit 11.
【0008】この演算増幅回路11の出力側より出力端
子16を導出すると共にこの演算増幅回路11の出力側
とこの反転入力端子−との間に抵抗器17を接続し、こ
の演算増幅回路11、抵抗器10,15,17で差動増
幅回路を構成する。An output terminal 16 is derived from the output side of the operational amplifier circuit 11, and a resistor 17 is connected between the output side of the operational amplifier circuit 11 and the inverting input terminal of the operational amplifier circuit 11. The resistors 10, 15, and 17 constitute a differential amplifier circuit.
【0009】また、この磁気抵抗効果素子3a,3b
(6a,6b)と抵抗器13,14とでブリッジ回路を
構成している。The magnetoresistive elements 3a, 3b
(6a, 6b) and the resistors 13, 14 constitute a bridge circuit.
【0010】また、従来のMR素子を使用した基本的な
検出ヘッド2の他の例としては図6Bに示す如く、磁気
スケール1の目盛の記録方向にλ/2離れて4個のMR
素子3a,3b,3d,3cを配置し、MR素子3a及
び3bを直列接続すると共にMR素子3c及び3dを直
列接続し、MR素子3a及び3cの夫々の開放端4a及
び4cに夫々直流電圧VO を供給すると共にMR素子3
b及び3dの夫々の開放端4b及び4dを夫々接地す
る。As another example of a basic detection head 2 using a conventional MR element, as shown in FIG. 6B, four MRs are separated by λ / 2 in the recording direction of the scale of the magnetic scale 1.
Elements 3a, 3b, 3d and 3c are arranged, MR elements 3a and 3b are connected in series, and MR elements 3c and 3d are connected in series. DC voltage V is applied to open ends 4a and 4c of MR elements 3a and 3c, respectively. Supply O and MR element 3
The open ends 4b and 4d of b and 3d are grounded, respectively.
【0011】MR素子3a及び3bの接続点より出力端
子5aを導出すると共にMR素子3c及び3dの接続点
より出力端子5cを導出する。この場合に出力端子5a
及び5cには互に位相が180度異なる出力信号が得ら
れる。An output terminal 5a is derived from a connection point between the MR elements 3a and 3b, and an output terminal 5c is derived from a connection point between the MR elements 3c and 3d. In this case, the output terminal 5a
5c have output signals 180 degrees out of phase with each other.
【0012】また、磁気スケール1の目盛の記録方向に
λ/2はなれて4個のMR素子6a,6b,6d,6c
を配置し、MR素子6a及び6bを直列接続すると共
に、MR素子6c及び6dを直列接続し、MR素子6a
及び6cの夫々の開放端7a及び7cに夫々直流電圧V
O を供給すると共にMR素子6b及び6dの夫々の開放
端7b及び7dを夫々接地する。The four MR elements 6a, 6b, 6d, 6c are separated by λ / 2 in the recording direction of the scale of the magnetic scale 1.
Are arranged, the MR elements 6a and 6b are connected in series, and the MR elements 6c and 6d are connected in series.
DC voltage V is applied to each of the open ends 7a and 7c.
O is supplied and the open ends 7b and 7d of the MR elements 6b and 6d are grounded, respectively.
【0013】MR素子6a及び6bの接続点より出力端
子5bを導出すると共にMR素子6c及び6dの接続点
より出力端子5dを導出する。この場合出力端子5b及
び5dには互に位相が180度異なる出力信号が得られ
る。An output terminal 5b is derived from a connection point between the MR elements 6a and 6b, and an output terminal 5d is derived from a connection point between the MR elements 6c and 6d. In this case, output signals whose phases are different from each other by 180 degrees are obtained at the output terminals 5b and 5d.
【0014】この場合、隣接するMR素子3c及び6a
の間隔を磁気スケール1の目盛の記録方向にλ/4離し
て配置し、出力端子5aと5b及び出力端子5cと5d
に夫々90度(λ/4)位相の異なる2相出力を得る如
くする。In this case, the adjacent MR elements 3c and 6a
Are arranged at a distance of λ / 4 in the recording direction of the scale of the magnetic scale 1, and the output terminals 5a and 5b and the output terminals 5c and 5d
To obtain two-phase outputs having different phases by 90 degrees (λ / 4).
【0015】この図6Bに示す如き検出ヘッド2を使用
したときは、出力回路として図7Bに示す如くものを使
用する。この図7Bにつき説明するに図7Aに対応する
部分には同一符号を付して示す。この出力端子5a(又
は5b)を抵抗器10を介して差動増幅回路を構成する
演算増幅回路11の反転入力端子−に接続し、また出力
端子5c(又は5d)を抵抗器15を介して、この演算
増幅回路11の非反転入力端子+に接続する。When the detecting head 2 as shown in FIG. 6B is used, an output circuit as shown in FIG. 7B is used. 7B, parts corresponding to those in FIG. 7A are denoted by the same reference numerals. The output terminal 5a (or 5b) is connected via a resistor 10 to the inverting input terminal-of an operational amplifier circuit 11 constituting a differential amplifier circuit, and the output terminal 5c (or 5d) is connected via a resistor 15. , Is connected to the non-inverting input terminal + of the operational amplifier circuit 11.
【0016】この場合この磁気抵抗効果素子3a,3
b,3c及び3d(6a,6b,6c及び6d)はブリ
ッジ回路を構成しており、また出力端子5a及び5c
(5b及び5d)には互に位相が180度異なる出力信
号が得られるので、この出力端子16には図7Aの出力
回路に比し2倍の大きさの出力信号が得られる。この場
合も、90度位相の異なる2相の正弦波信号即ちsi
n、cosの信号を得ることができる。In this case, the magnetoresistive elements 3a, 3
b, 3c and 3d (6a, 6b, 6c and 6d) constitute a bridge circuit, and output terminals 5a and 5c
At (5b and 5d), output signals whose phases are different from each other by 180 degrees are obtained. Therefore, an output signal having a magnitude twice as large as that of the output circuit of FIG. 7A is obtained at the output terminal 16. Also in this case, two-phase sine wave signals having phases different by 90 degrees, ie, si
Signals of n and cos can be obtained.
【0017】このsin及びcosの信号を処理するこ
とにより、 (1)相対移動方向の弁別 (2)記録ピッチの内挿(電気的に分割し分解能をアッ
プ) を行うことができる。By processing the sin and cos signals, it is possible to (1) discriminate the relative movement direction and (2) interpolate the recording pitch (electrically divide it to increase the resolution).
【0018】上述の如き位置検出装置の磁気スケール1
の磁気記録の目盛を精度良く検出するためには、下記の
条件が必要である。 (1)正確なピッチλで目盛が磁気記録されているこ
と。 (2)出力信号波形が歪みのない正弦波であること。 (3)sin、cosの出力電圧が検出範囲全域に亘り
同一であること。 (4)sin、cosの各出力信号は直流成分の変動が
ないこと。The magnetic scale 1 of the position detecting device as described above
In order to accurately detect the scale of magnetic recording described above, the following conditions are required. (1) The scale is magnetically recorded at an accurate pitch λ. (2) The output signal waveform is a sine wave without distortion. (3) The output voltages of sin and cos are the same over the entire detection range. (4) The output signals of sin and cos have no fluctuation of the DC component.
【0019】この「(1)正確なピッチλで目盛が磁気
記録されていること。」に対しては高精度に磁気記録す
ると共に検出ヘッド2を複数のMR素子で構成し、この
複数のMR素子を磁気スケール1の目盛に対して同一条
件位置に配置し、直列又は直・並列に接続することによ
り、たとえ磁気記録の目盛のピッチに誤差が生じても、
この複数のMR素子で検出することにより誤差が平均化
され、精度良く検出することができる。For "(1) The magnetic scale is recorded at an accurate pitch [lambda]", magnetic recording is performed with high precision and the detection head 2 is composed of a plurality of MR elements. By arranging the elements at the same condition position with respect to the scale of the magnetic scale 1 and connecting them in series or in series or in parallel, even if an error occurs in the pitch of the scale of magnetic recording,
The error is averaged by detecting with the plurality of MR elements, and the detection can be performed with high accuracy.
【0020】上述の点を考慮して、図6Aの検出ヘッド
2のMR素子3a,3b,6a及び6bを夫々4個のM
R素子3a−1,3a−2‥‥3a−4,3b−1‥‥
3b−4,6a−1‥‥6a−4及び6b−1‥‥6b
−4を直列に接続して構成した例を図8に示す。In consideration of the above points, the MR elements 3a, 3b, 6a and 6b of the detection head 2 shown in FIG.
R element 3a-1, 3a-2 {3a-4, 3b-1}
3b-4, 6a-1 @ 6a-4 and 6b-1 @ 6b
FIG. 8 shows an example in which -4 are connected in series.
【0021】この場合、図8の図6AのMR素子3a,
3b,6a及び6bを夫々構成する4個のMR素子3a
−1,3a−2,3a−3,3a−4、MR素子3b−
1,3b−2,3b−3.3b−4、MR素子6b−
4,6b−3,6b−2,6b−1、MR素子6a−
4,6a−3,6a−2,6a−1は夫々磁気スケール
1の目盛の記録方向に夫々λ離して配置する如くする。In this case, the MR elements 3a, 3a of FIG.
3b, 6a and four MR elements 3a respectively constituting 6b
-1, 3a-2, 3a-3, 3a-4, MR element 3b-
1, 3b-2, 3b-3.3b-4, MR element 6b-
4, 6b-3, 6b-2, 6b-1, MR element 6a-
The magnetic scales 4, 6a-3, 6a-2, 6a-1 are arranged at a distance of λ from each other in the recording direction of the scale of the magnetic scale 1.
【0022】このときは各グループのMR素子3a−1
‥‥3a−4,3b−1‥‥3b−4,6b−4‥‥6
b−1,6a−4‥‥6a−1は磁気スケール1の各位
置に対応する記録磁気により、同一の抵抗値変化を受
け、その結果、誤差が平均化され精度良く検出すること
ができる。At this time, the MR elements 3a-1 of each group
{3a-4,3b-1} 3b-4,6b-4} 6
b-1, 6a-4 ‥‥ 6a-1 receive the same change in resistance value by the recording magnetism corresponding to each position of the magnetic scale 1, and as a result, errors are averaged and can be accurately detected.
【0023】この図8において隣接するMR素子3a−
4と3b−1との間隔及びMR素子6b−1と6a−4
との間隔を夫々磁気スケール1の目盛の記録方向にλ/
2離す如くすると共に隣接するMR素子3b−4と6b
−4との間隔を磁気スケール1の目盛の記録方向にλ/
4離す如くする。In FIG. 8, adjacent MR elements 3a-
4 and 3b-1 and MR elements 6b-1 and 6a-4
In the recording direction of the scale of the magnetic scale 1 respectively.
2 away from each other and adjacent MR elements 3b-4 and 6b
-4 in the recording direction of the scale of the magnetic scale 1
4 away.
【0024】この図8においてはMR素子3a−1及び
6a−1の夫々の開放端4a及び7aに夫々直流電圧V
O を供給すると共にMR素子3b−4及び6b−4の夫
々の開放端4b及び7bを夫々接地し、MR素子3a−
4及び3b−1の接続点より出力端子5aを導出すると
共にMR素子6a−4及び6b−1の接続点より出力端
子5bを導出する。In FIG. 8, a DC voltage V is applied to the open ends 4a and 7a of the MR elements 3a-1 and 6a-1, respectively.
O , and the open ends 4b and 7b of the MR elements 3b-4 and 6b-4 are grounded, respectively.
The output terminal 5a is derived from the connection point of the MR elements 6a-4 and 6b-1, and the output terminal 5b is derived from the connection point of the MR elements 6a-4 and 6b-1.
【0025】この図8の検出ヘッド2の等価回路は図9
A及びBに示す如くである。FIG. 9 shows an equivalent circuit of the detection head 2 shown in FIG.
A and B.
【0026】この図6AのMR素子3aと3bとの中心
間間隔及びMR素子6aと6bとの中心間間隔は夫々λ
/2であり、またMR素子3a,3bのグループとMR
素子6a,6bのグループとの中心間間隔は3λ/4で
あったが、この図8例ではMR素子3a−1‥‥3a−
4のグループと3b−1‥‥3b−4のグループとの中
心間間隔及びMR素子6a−1‥‥6a−4のグループ
と6b−1‥‥6b−4のグループとの中心間間隔は夫
々(3+1/2)λであり、またMR素子3a−1‥‥
3a−4,3b−1‥‥3b−4のグループとMR素子
6a−1‥‥6a−4,6b−1‥‥6b−4のグルー
プとの中心間間隔は(6+3/4)λであり、この図8
例ではその間隔が増大している。即ち図8例ではMR素
子の増加に伴って、各中心間間隔も増大する。The center distance between the MR elements 3a and 3b and the center distance between the MR elements 6a and 6b in FIG.
/ 2, and the group of the MR elements 3a and 3b and the MR
The center-to-center spacing between the groups of the elements 6a and 6b was 3λ / 4, but in the example of FIG. 8, the MR elements 3a-1 ‥‥ 3a-
The center-to-center spacing between the group No. 4 and the group of 3b-1 @ 3b-4 and the center-to-center spacing between the group of MR elements 6a-1 @ 6a-4 and the group of 6b-1 @ 6b-4 respectively. (3 + 1/2) λ, and the MR element 3a-1 ‥‥
The center-to-center spacing between the group of 3a-4, 3b-1 @ 3b-4 and the group of MR elements 6a-1 @ 6a-4, 6b-1 @ 6b-4 is (6 + 3/4) λ. This FIG.
In the example, the interval is increasing. That is, in the example of FIG. 8, the center-to-center spacing increases as the number of MR elements increases.
【0027】ところで、このMR素子は抵抗体であり、
動作時、通電電流により発熱するので上述のMR素子3
a−1‥‥3a−4のグループと3b−1‥‥3b−4
のグループの中心間間隔及びMR素子6a−1‥‥6a
−4のグループと6b−1‥‥6b−4とのグループの
中心間間隔が離れると、発熱等による上述MR素子グル
ープ間の温度分布むらを生じ、この温度分布むらにより
抵抗値の増加に差が生じ、出力信号の直流成分が変動し
て上述条件(4)の「sin、cosの各出力信号は直
流成分の変動がないこと。」を満たさなくなる不都合が
ある。Incidentally, this MR element is a resistor,
During operation, heat is generated by the supplied current.
a-1 ‥‥ 3a-4 group and 3b-1 ‥‥ 3b-4
And the MR element 6a-1 ‥‥ 6a
When the center-to-center distance between the group of -4 group and the group of 6b-1 ‥‥ 6b-4 is large, unevenness in temperature distribution between the MR element groups due to heat generation or the like occurs. Occurs, and the DC component of the output signal fluctuates, so that the condition (4) that “the output signals of sin and cos do not fluctuate the DC component” cannot be satisfied.
【0028】またMR素子3a−1‥‥3a−4,3b
−1‥‥3b−4のグループとMR素子6a−1‥‥6
a−4,6b−1‥‥6b−4のグループとの中心間間
隔が増加すると磁気スケール1の検出位置が離れること
により、磁気記録むらにより、上述条件(3)のsi
n、cosの信号の出力電圧が同一であることをも満た
しにくくなる不都合がある。The MR elements 3a-1 @ 3a-4, 3b
-1 @ 3b-4 group and MR element 6a-1 @ 6
When the center-to-center spacing with the group of a-4, 6b-1 ‥‥ 6b-4 increases, the detection position of the magnetic scale 1 moves away.
There is a disadvantage that it is difficult to satisfy that the output voltages of the n and cos signals are the same.
【0029】また磁気記録の目盛を高精度に検出するM
R素子を使用した検出ヘッド2への要求事項として下記
項目がある。 (1)MR素子数を増加させる。 (2)MR素子3a−1‥‥3a−4のグループと3b
−1‥‥3b−4のグループとの中心間間隔及びMR素
子6a−1‥‥6a−4のグループと6b−1‥‥6b
−4のグループとの中心間間隔を夫々近付ける(最接近
理想値=λ/2)。 (3)MR素子3a−1‥‥3a−4,3b−1‥‥3
b−4のグループとMR素子6a−1‥‥6a−4,6
b−1‥‥6b−4のグループとの中心間間隔を近付け
る(最接近理想値=λ/4)。M for detecting the scale of magnetic recording with high accuracy
The following items are required for the detection head 2 using the R element. (1) Increase the number of MR elements. (2) MR element 3a-1 ‥‥ 3a-4 group and 3b
-1 ‥‥ 3b-4 center-to-center spacing and MR element 6a-1 ‥‥ 6a-4 group and 6b-1 ‥‥ 6b
The distance between centers with the group of −4 is made closer (ideal ideal value = λ / 2). (3) MR element 3a-1 @ 3a-4, 3b-1 @ 3
b-4 group and MR elements 6a-1 ‥‥ 6a-4,6
Close the center-to-center spacing with the group of b-1 ‥‥ 6b-4 (ideal closeness ideal value = λ / 4).
【0030】上述要求を満たす従来例として、特開平6
−11358号公報が提案されている。斯る従来例は8
個のMR素子を直、並列する如くして上述要求を満たし
ているが、sin出力信号を得るMR素子のパターン間
に、cos出力信号を得るMR素子のパターンをはめ込
んだような構成であり、当然ながらMR素子間の結線の
交差数が多い不都合がある。As a conventional example which satisfies the above-mentioned requirements, see
No. -11358 has been proposed. The conventional example is 8
The above requirement is satisfied by directly arranging the MR elements in parallel, but the configuration is such that the pattern of the MR element for obtaining the cos output signal is inserted between the patterns of the MR element for obtaining the sin output signal, Naturally, there is an inconvenience that the number of intersections of the connections between the MR elements is large.
【0031】即ち、このMR素子を基板上で結線の交差
を形成する方法としては、絶縁体を介して2相構造とす
る方法、スルーホールを設け背面で結線する方法、ラン
ドを設け結線する方法等が考えられるが何れにせよ構成
が複雑で高価となる不都合があり、また品質の管理に注
意を要する不都合があった。That is, as a method of forming a crossing of the connection of the MR element on the substrate, a method of forming a two-phase structure via an insulator, a method of forming a through hole and connecting the back side, and a method of forming a land and connecting the land In any case, there is a problem that the configuration is complicated and expensive, and there is a problem that care must be taken in quality control.
【0032】本発明は斯る点に鑑み、検出ヘッドを複数
のMR素子で構成しながら、この複数のMR素子間の結
線が交差することがないようにして製造を容易にすると
共に信頼性の高い位置検出装置を提供することを目的と
する。In view of the above, according to the present invention, while the detection head is composed of a plurality of MR elements, the connection between the plurality of MR elements is prevented from intersecting, thereby facilitating manufacture and improving reliability. It is an object to provide a high position detecting device.
【0033】[0033]
【課題を解決するための手段】本発明位置検出装置はN
極とS極とが繰返し同一ピッチλ(λはN極とS極との
間隔)で目盛が磁気記録されている磁気スケールと、磁
気抵抗効果素子を使用した検出ヘッドとの相対位置を検
出するようにした位置検出装置において、この検出ヘッ
ドは間隔を(n/2−1/4)λ(nは1,2,3‥‥
の自然数)離して、この磁気スケールの目盛の記録方向
に複数の磁気抵抗効果素子群より成る組みを2組配置
し、この複数の磁気抵抗効果素子群は夫々の間隔を(n
+2)λ(nは1,2,3‥‥の自然数)離してこの磁
気スケールの目盛の記録方向に配置し、この磁気抵抗効
果素子群はブリッジ回路の一の辺を構成する少なくとも
2つの磁気抵抗効果素子の直列回路とこのブリッジ回路
の他の辺を構成する少なくとも2つの磁気抵抗効果素子
の直列回路とから成るものである。According to the present invention, the position detecting device comprises an N
The relative position between the magnetic scale on which the scale is magnetically recorded at the same pitch λ (where λ is the interval between the N pole and the S pole) and the detection head using a magnetoresistive element is detected. In such a position detecting device, the distance between the detection heads is (n / 2−1 / 4) λ (n is 1, 2, 3).
Are separated from each other by two sets of a plurality of groups of a plurality of magnetoresistive elements in the recording direction of the scale of the magnetic scale.
+2) λ (n is a natural number of 1, 2, 3 °) spaced apart in the recording direction of the scale of the magnetic scale, and the magnetoresistive effect element group comprises at least two magnetic fields forming one side of a bridge circuit. The bridge circuit comprises a series circuit of a resistance effect element and a series circuit of at least two magnetoresistive elements forming the other side of the bridge circuit.
【0034】斯る本発明によればブリッジ回路の一の辺
を構成する複数のMR素子と他の辺を構成する複数のM
R素子との間隔を例えばλ/2とすることができると共
に90度位相の異なる2相の正弦波信号を得る複数のM
R素子の間隔を例えば(2+1/4)λとすることがで
き、信頼性の高い位置検出ができると共にこの複数のM
R素子間の結線を交差することがないようにでき、製造
を容易とすることができる。According to the present invention, a plurality of MR elements constituting one side of the bridge circuit and a plurality of M elements constituting the other side are provided.
A plurality of Ms that can set the interval with the R element to, for example, λ / 2 and obtain two-phase sine wave signals having a phase difference of 90 degrees.
The distance between the R elements can be set to, for example, (2 + /) λ, and highly reliable position detection can be performed.
The connection between the R elements can be prevented from crossing, and the manufacturing can be facilitated.
【0035】[0035]
【発明の実施の形態】以下、図1及び図2を参照して本
発明位置検出装置の実施の形態の例につき説明しよう。
本例の位置検出装置も図5に示す如くN極とS極とが繰
返し同一ピッチλ(λはN極とS極との間隔)で目盛が
磁気記録されている磁気スケール1と、磁界により抵抗
値が変化する磁気抵抗効果素子(MR素子)を使用した
検出ヘッド2との相対位置を検出するようにしたもので
あり、本例においては、この検出ヘッド2を図1に示す
如く構成する。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of a position detecting device according to the present invention will be described below with reference to FIGS.
As shown in FIG. 5, the position detecting device of this example also has a magnetic scale 1 on which scales are magnetically recorded at the same pitch [lambda] ([lambda] is an interval between the N pole and the S pole). The relative position with respect to the detection head 2 using a magnetoresistive element (MR element) whose resistance value changes is detected. In this example, the detection head 2 is configured as shown in FIG. .
【0036】この図1例は、磁気スケール1の目盛の記
録方向に配された複数例えば4つのMR素子群20,2
1,22,23より成る一の組とこの磁気スケール1の
目盛の記録方向に配された複数例えば4つのMR素子群
24,25,26,27より成る他の組との2組設け、
この2組の間隔をこの磁気スケール1の目盛の記録方向
に(n/2−1/4)λ(nは1,2,3‥‥の自然
数)本例ではn=1のλ/4とする如くする。FIG. 1 shows an example in which a plurality of, for example, four MR element groups 20, 2 arranged in the recording direction of the scale of the magnetic scale 1.
Two sets of one set consisting of 1, 2, 23 and another set consisting of a plurality of, for example, four MR element groups 24, 25, 26, 27 arranged in the recording direction of the scale of the magnetic scale 1;
In the recording direction of the scale of the magnetic scale 1, the distance between the two sets is (n / 2-1/4) λ (n is a natural number of 1, 2, 3). I will do it.
【0037】このMR素子群20,21‥‥27は夫々
磁気スケール1の目盛の記録方向に沿って配された4つ
のMR素子20a,20b,20c,20d,21a,
21b,21c,21d‥‥27a,27b,27c,
27dより構成し、夫々のMR素子群20,21‥‥2
7におけるMR素子20a,21a‥‥27aとMR素
子20b,21b‥‥27bとの間隔を磁気スケール1
の目盛の記録方向に夫々λ/2とし、MR素子20b,
21b‥‥27bとMR素子20c,21c‥‥27c
との間隔を磁気スケール1の目盛の記録方向に夫々λと
し、MR素子20c,21c‥‥27cとMR素子20
d,21d‥‥27dとの間隔を磁気スケール1の目盛
の記録方向に夫々λ/2とする。The MR element groups 20, 21 ‥‥ 27 are composed of four MR elements 20a, 20b, 20c, 20d, 21a, 21a arranged along the recording direction of the scale of the magnetic scale 1.
21b, 21c, 21d ‥‥ 27a, 27b, 27c,
27d, and the respective MR element groups 20, 21 ‥‥ 2
7, the distance between the MR elements 20a, 21a ‥‥ 27a and the MR elements 20b, 21b ‥‥ 27b is
Λ / 2 in the recording direction of the scale
21b ‥‥ 27b and MR elements 20c, 21c ‥‥ 27c
Are defined as λ in the recording direction of the scale of the magnetic scale 1, respectively, and the MR elements 20c, 21c ‥‥ 27c and the MR element 20c
The distance between d and 21d ‥‥ 27d is λ / 2 in the recording direction of the scale of the magnetic scale 1 respectively.
【0038】この場合夫々のMR素子20,21,‥‥
27におけるMR素子20a,201a‥‥27aとM
R素子20d,21d‥‥27dとは磁気スケール1の
目盛の記録方向に間隔2λ離れているので、磁気スケー
ル1の記録磁場により、同じ抵抗値変化を受け、また夫
々のMR素子群20,21‥‥27におけるMR素子2
0b,21b‥‥27bとMR素子20c,21c‥‥
27cとは磁気スケール1の目盛の記録方向に間隔λ離
れているので、磁気スケール1の記録磁場により、同じ
抵抗値変化を受ける。In this case, the respective MR elements 20, 21,.
27, the MR elements 20a, 201a ‥‥ 27a and M
Since the R elements 20d, 21d ‥‥ 27d are separated by 2λ in the recording direction of the scale of the magnetic scale 1, the same resistance value change is caused by the recording magnetic field of the magnetic scale 1, and the respective MR element groups 20, 21 # 27 MR element 2
0b, 21b {27b and MR elements 20c, 21c}
27c is separated from the magnetic scale 1 by an interval λ in the recording direction of the graduations, so that the recording magnetic field of the magnetic scale 1 receives the same resistance value change.
【0039】MR素子群20のMR素子20dとMR素
子群21のMR素子21aとの間隔、MR素子群21の
MR素子21dとMR素子群22のMR素子22aとの
間隔、MR素子群22のMR素子22dとMR素子群2
3のMR素子23aとの間隔、MR素子群24のMR素
子24dとMR素子群25のMR素子25aとの間隔、
MR素子群25のMR素子25dとMR素子群26のM
R素子26aとの間隔及びMR素子群26のMR素子2
6dとMR素子群27のMR素子27aとの間隔を磁気
スケール1の目盛の記録方向に夫々mλ(mは3以上の
整数)本例では3λとする。The distance between the MR element 20d of the MR element group 20 and the MR element 21a of the MR element group 21, the distance between the MR element 21d of the MR element group 21 and the MR element 22a of the MR element group 22, MR element 22d and MR element group 2
3, the distance between the MR element 24a of the MR element group 24 and the MR element 25a of the MR element group 25,
MR element 25d of MR element group 25 and M of MR element group 26
The distance from the R element 26a and the MR element 2 of the MR element group 26
The distance between 6d and the MR element 27a of the MR element group 27 is mλ (m is an integer of 3 or more) in the recording direction of the scale of the magnetic scale 1, and is 3λ in this example.
【0040】また本例においてはMR素子群20,21
‥‥27を図1に示す如く磁気スケール1の左から右方
向にMR素子群20,24,21,25,22,26,
23,27の順に配列し、MR素子群20のMR素子2
0dとMR素子群24のMR素子24aとの間隔、MR
素子群21のMR素子21dとMR素子群25のMR素
子25aとの間隔、MR素子群22のMR素子22dと
MR素子群26のMR素子26aとの間隔及びMR素子
群23のMR素子23dとMR素子群27のMR素子2
7aとの間隔を磁気スケール1の目盛の記録方向に夫々
(n/2−1/4)λ(nは1,2,3‥‥自然数)本
例ではλ/4とする。In this embodiment, the MR element groups 20, 21
# 27 is applied to the MR element groups 20, 24, 21, 25, 22, 26, from left to right of the magnetic scale 1 as shown in FIG.
Arranged in the order of 23 and 27, the MR element 2 of the MR element group 20
0d and the distance between MR element 24a of MR element group 24, MR
The distance between the MR element 21d of the element group 21 and the MR element 25a of the MR element group 25, the distance between the MR element 22d of the MR element group 22 and the MR element 26a of the MR element group 26, and the distance between the MR element 23d of the MR element group 23 MR element 2 of MR element group 27
The distance from the reference numeral 7a is (n / 2-1 /) λ (n is 1, 2, 3 ‥‥ natural number) in the recording direction of the scale of the magnetic scale 1, and is λ / 4 in this example.
【0041】従って本例ではMR素子群24のMR素子
24dとMR素子群21のMR素子21aとの間隔、M
R素子群25のMR素子25dとMR素子群22のMR
素子22aとの間隔及びMR素子群26のMR素子26
dとMR素子群23のMR素子23aとの間隔は磁気ス
ケール1の目盛の記録方向に夫々3λ/4となる。Accordingly, in this embodiment, the distance between the MR element 24d of the MR element group 24 and the MR element 21a of the MR element group 21, M
The MR element 25d of the R element group 25 and the MR of the MR element group 22
The distance from the element 22a and the MR element 26 of the MR element group 26
The distance between d and the MR element 23a of the MR element group 23 is 3λ / 4 in the recording direction of the scale of the magnetic scale 1 respectively.
【0042】本例においては、このMR素子20a,2
0d,21a,21d,22a,22d,23a,23
d,23c,23b,22c,22b,21c,21
b,20c及び20bをこの順に直列に接続し、MR素
子20aの開放端28aに直流電圧VO を供給すると共
にMR素子20bの開放端28bを接地し、MR素子2
3c及び23dの接続点より出力端子29aを導出す
る。In this embodiment, the MR elements 20a, 2
0d, 21a, 21d, 22a, 22d, 23a, 23
d, 23c, 23b, 22c, 22b, 21c, 21
b, 20c and 20b are connected in series in this order, a DC voltage V O is supplied to the open end 28a of the MR element 20a, and the open end 28b of the MR element 20b is grounded.
An output terminal 29a is derived from a connection point between 3c and 23d.
【0043】この場合、このMR素子20a,20b‥
‥23dの等価回路は図2Aに示す如くなり、MR素子
20a,20d,21a,21d,22a,22d,2
3a及び23dの直列回路が図7Aのブリッジ回路の一
の辺を構成し、MR素子23c,23b,22c,22
b,21c,21b,20c及び20bの直列回路が図
7Aのブリッジ回路の他の辺を構成する如くする。In this case, the MR elements 20a, 20b #
The equivalent circuit of # 23d is as shown in FIG. 2A, and the MR elements 20a, 20d, 21a, 21d, 22a, 22d, 2
The series circuit of 3a and 23d forms one side of the bridge circuit of FIG. 7A, and the MR elements 23c, 23b, 22c, 22
The series circuit of b, 21c, 21b, 20c and 20b constitutes another side of the bridge circuit of FIG. 7A.
【0044】また、このMR素子24a,24d,25
a,25d,26a,26d,27a,27d,27
c,27b,26c,26b,25c,25b,24c
及び24bをこの順に直列に接続し、MR素子24aの
開放端30aに直流電圧VO を供給すると共にMR素子
24bの開放端30bを接地し、MR素子27c及び2
7dの接続点より出力端子29bを導出する。The MR elements 24a, 24d, 25
a, 25d, 26a, 26d, 27a, 27d, 27
c, 27b, 26c, 26b, 25c, 25b, 24c
And 24b are connected in series in this order, a DC voltage V O is supplied to the open end 30a of the MR element 24a, and the open end 30b of the MR element 24b is grounded.
The output terminal 29b is derived from the connection point 7d.
【0045】この場合、このMR素子24a,24b‥
‥27dの等価回路は図2Bに示す如くなりMR素子2
4a,24d,25a,25d,26a,26d,27
a及び27dの直列回路が図7Aのブリッジ回路の一の
辺を構成し、MR素子27c,27b,26c,26
b,25c,25b,24c及び24bの直列回路が図
7Aのブリッジ回路の他の辺を構成する如くする。In this case, the MR elements 24a, 24b #
The equivalent circuit of # 27d is as shown in FIG.
4a, 24d, 25a, 25d, 26a, 26d, 27
7A constitute one side of the bridge circuit of FIG. 7A, and the MR elements 27c, 27b, 26c, 26
The series circuit of b, 25c, 25b, 24c and 24b constitutes another side of the bridge circuit of FIG. 7A.
【0046】この場合、MR素子20a,20b‥‥2
3d及びMR素子24a,24b‥‥27dの結線は交
差することなく行うようにすると共に開放端28a,2
8b,30a,30b及び出力端子29a,29bを一
方向(図1では下方)より引き出す如くする。In this case, the MR elements 20a, 20b # 2
The connection between the 3d and the MR elements 24a, 24b ‥‥ 27d should be made without crossing each other and the open ends 28a, 2
8b, 30a, 30b and output terminals 29a, 29b are drawn out from one direction (downward in FIG. 1).
【0047】このMR素子群20,21,22,23よ
り成る一方の組とMR素子群24,25,26,27よ
り成る他方の組との間隔を磁気スケール1の目盛の記録
方向にλ/4としているので出力端子29a及び29b
には90度(λ/4)位相の異なる2相の正弦波信号即
ちsin及びcosの信号が得られる。The distance between one set of the MR element groups 20, 21, 22, 23 and the other set of the MR element groups 24, 25, 26, 27 is set to λ / 4, the output terminals 29a and 29b
, Two-phase sine wave signals having different phases by 90 degrees (λ / 4), that is, signals of sin and cos are obtained.
【0048】本例においても、この磁気スケール1とM
R素子より成る検出ヘッド2との相対変位により、この
出力端子29a及び29bに得られる出力信号を図7A
に示す如き出力回路を使用して90度位相の異なる2相
の正弦波信号即ちsin及びcosの信号を得ている。Also in this example, the magnetic scales 1 and M
The output signals obtained at the output terminals 29a and 29b by the relative displacement with respect to the detection head 2 composed of the R element are shown in FIG.
Are used to obtain two-phase sine wave signals having a phase difference of 90 degrees, ie, sin and cos signals.
【0049】本例によればブリッジ回路の一の辺を構成
する8個のMR素子20a,20d,21a,21d,
22a,22d,23a,23d(又は24a,24
d,25a,25d,26a,26d,27a,27
d)と他の辺を構成する8個のMR素子23c,23
b,22c,22b,21c,21b,20c,20b
(又は27c,27b,26c,26b,25c,25
b,24c,24b)との間隔をλ/2とすることがで
きると共に90度位相の異なる2相の正弦波信号を得る
夫々16個のMR素子20a,20b‥‥23dの一の
組とMR素子24a,24b‥‥27dの他の組との間
隔を(2+1/4)λとすることができ信頼性の高い位
置検出ができる利益がある。According to this embodiment, the eight MR elements 20a, 20d, 21a, 21d,
22a, 22d, 23a, 23d (or 24a, 24
d, 25a, 25d, 26a, 26d, 27a, 27
d) and eight MR elements 23c and 23 forming other sides
b, 22c, 22b, 21c, 21b, 20c, 20b
(Or 27c, 27b, 26c, 26b, 25c, 25
b, 24c, 24b) can be set to λ / 2, and a set of 16 MR elements 20a, 20b ‥‥ 23d, each of which obtains a two-phase sine wave signal having a phase difference of 90 °, and an MR The interval between the elements 24a and 24b ‥‥ 27d and the other set can be set to (2 + /) λ, and there is an advantage that highly reliable position detection can be performed.
【0050】また本例によれば、32個のMR素子20
a,20b‥‥27d間の結線を交差することなく行う
ことができ、このMR素子と同一素材によりこのMR素
子と同時に結線も作製することができ、製造を容易とす
ることができる利益がある。According to the present embodiment, the 32 MR elements 20
The connection between a, 20b and 27d can be made without crossing, and the connection can be made simultaneously with this MR element using the same material as this MR element, which has the advantage of facilitating manufacture. .
【0051】図3及び図4は本発明の実施の形態の他の
例を示す。この図3及び図4につき説明するに図1及び
図2に対応する部分には同一符号を付して示す。この図
3例はMR素子20a,20b‥‥27dの配置は図1
例と同じとし、その結線を図1例とは異なるようにした
ものである。従ってここではMR素子20a,20b‥
‥27dの配置の説明は省略し、結線について説明す
る。FIGS. 3 and 4 show another embodiment of the present invention. 3 and 4, parts corresponding to those in FIGS. 1 and 2 are denoted by the same reference numerals. In the example of FIG. 3, the arrangement of the MR elements 20a, 20b ‥‥ 27d is shown in FIG.
The example is the same as the example, and the connection is different from the example in FIG. Therefore, here, the MR elements 20a, 20b
The description of the arrangement of # 27d is omitted, and the connection is described.
【0052】本例においては、このMR素子20a,2
0d,21a,21d,22a,22d,23a及び2
3dをこの順に直列に接続し、MR素子20a及び23
dの夫々の開放端28a及び28cに夫々直流電圧Vo
を供給すると共にMR素子21d及び22aの接続点よ
り出力端子29aを導出する。In this embodiment, the MR elements 20a, 20a
0d, 21a, 21d, 22a, 22d, 23a and 2
3d are connected in series in this order, and the MR elements 20a and 23
DC voltage V o at each of the open ends 28a and 28c of FIG.
And an output terminal 29a is derived from a connection point between the MR elements 21d and 22a.
【0053】またMR素子20b,20c,21b及び
21cをこの順の直列回路として出力端子29aに接続
すると共にMR素子23c,23b,22c及び22b
をこの順の直列回路として出力端子29aに接続し、こ
のMR素子20b及び23cの開放端28b及び28d
を夫々接地する。The MR elements 20b, 20c, 21b and 21c are connected to the output terminal 29a as a series circuit in this order, and the MR elements 23c, 23b, 22c and 22b are connected.
Are connected to the output terminal 29a as a series circuit in this order, and the open ends 28b and 28d of the MR elements 20b and 23c are connected.
Are grounded respectively.
【0054】この場合、MR素子20a,20b‥‥2
3dの等価回路は図4Aに示す如く、MR素子20a,
20d,21a及び21dの直列回路とMR素子23
d,23a,22d及び22aの直列回路との並列回路
が図7Aのブリッジ回路の一の辺を構成し、MR素子2
1c,21b,20c及び20bの直列回路とMR素子
22b,22c,23b及び23cの直列回路との並列
回路が図7Aのブリッジ回路の他の辺を構成する如くす
る。In this case, the MR elements 20a, 20b # 2
As shown in FIG. 4A, the equivalent circuit of 3d is the MR element 20a,
Series circuit of 20d, 21a and 21d and MR element 23
d, 23a, 22d and 22a constitute one side of the bridge circuit of FIG.
A parallel circuit of a series circuit of 1c, 21b, 20c and 20b and a series circuit of MR elements 22b, 22c, 23b and 23c constitutes another side of the bridge circuit of FIG. 7A.
【0055】またこのMR素子24a,24d,25
a,25d,26a,26d,27a及び27dをこの
順に直列に接続し、MR素子24a及び27dの夫々の
開放端30a及び30cに夫々直流電圧Vo を供給する
と共にMR素子25d及び26aの接続点より出力端子
29bを導出する。The MR elements 24a, 24d, 25
a, 25d, 26a, 26 d, to connect the 27a and 27d in this order in series, the connection point of the MR elements 25d and 26a supplies the respective DC voltage V o to the MR elements 24a and open ends 30a and 30c of each of 27d Then, the output terminal 29b is derived.
【0056】またMR素子24b,24c,25b及び
25cをこの順の直列回路として出力端子29bに接続
すると共にMR素子27c,27b,26c及び26b
をこの順の直列回路として出力端子29bに接続し、こ
のMR素子24b及び27cの開放端30b及び30d
を夫々接地する。The MR elements 24b, 24c, 25b and 25c are connected to the output terminal 29b as a series circuit in this order, and the MR elements 27c, 27b, 26c and 26b
Are connected to the output terminal 29b as a series circuit in this order, and the open ends 30b and 30d of the MR elements 24b and 27c are connected.
Are grounded respectively.
【0057】この場合、MR素子24a,24b‥‥2
7dの等価回路は図4Bに示す如く、MR素子24a,
24d,25a及び25dの直列回路とMR素子27
d,27a,26d及び26aの直列回路との並列回路
が図7Aのブリッジ回路の一の辺を構成し、MR素子2
5c,25b,24c及び24bの直列回路とMR素子
26b,26c,27b及び27cの直列回路との並列
回路が図7Aのブリッジ回路の他の辺を構成する如くす
る。In this case, the MR elements 24a, 24b # 2
As shown in FIG. 4B, the equivalent circuit of 7d is the MR element 24a,
Series circuit of 24d, 25a and 25d and MR element 27
d, 27a, 26d and a parallel circuit with the series circuit constitute one side of the bridge circuit of FIG.
A parallel circuit of a series circuit of 5c, 25b, 24c and 24b and a series circuit of MR elements 26b, 26c, 27b and 27c constitutes another side of the bridge circuit of FIG. 7A.
【0058】この場合MR素子20a,20b‥‥23
d及びMR素子24a,24b‥‥27dの結線は交差
することなく行うようにすると共に開放端28a,28
b,28c,28d,30a,30b,30c,30d
及び出力端子29a,29bを一方向(図3では下方)
より引き出す如くする。In this case, the MR elements 20a, 20b # 23
d and the MR elements 24a, 24b ‥‥ 27d are connected without crossing each other and open ends 28a, 28
b, 28c, 28d, 30a, 30b, 30c, 30d
And output terminals 29a, 29b in one direction (downward in FIG. 3)
So as to draw more out.
【0059】斯る図3例においても図1例と同様の作用
効果が得られることは容易に理解できよう。またこの図
3例ではMR素子を直列、並列接続しているので、MR
素子の総抵抗値を下げることができ省電力化が図れる利
益がある。It can be easily understood that the same effects as those of the example of FIG. 1 can be obtained in the example of FIG. In the example of FIG. 3, since the MR elements are connected in series and in parallel,
There is an advantage that the total resistance of the element can be reduced and power can be saved.
【0060】また図1又は図3に示す如き検出ヘッド2
を間隔を(n+1/2)λ(nは0,1,2,3‥‥の
整数)離して磁気スケール1の目盛の記録方向に2個配
置して、出力信号が互に逆位相(位相が180度異な
る)となる如くし、図7Bに示す出力回路を使用する如
くしても良い。Further, as shown in FIG. 1 or FIG.
Are arranged in the recording direction of the scale of the magnetic scale 1 at an interval of (n + /) λ (n is an integer of 0, 1, 2, 3}), and output signals are in opposite phases (phases). Are different by 180 degrees), and the output circuit shown in FIG. 7B may be used.
【0061】このときは、90度位相の異なる2相の信
号として安定且つ大きな出力信号を得ることができる利
益がある。At this time, there is an advantage that a stable and large output signal can be obtained as a two-phase signal having a phase difference of 90 degrees.
【0062】尚、上述図1図3の例においては開放端2
8a,28c,30a,30cに直流電圧VO を供給
し、開放端28b,28d,30b,30dを接地する
如く述べたが、開放端28a,28c,30a,30c
を接地し、開放端28b,28d,30b,30dに直
流電圧VO を供給するようにしても良い。このときの2
相の出力信号は位相差は270度となるが特性的には上
述と同一である。Incidentally, in the example of FIG. 1 and FIG.
Although it has been described that the DC voltage V O is supplied to 8a, 28c, 30a, and 30c and the open ends 28b, 28d, 30b, and 30d are grounded, the open ends 28a, 28c, 30a, and 30c
May be grounded to supply a DC voltage V O to the open ends 28b, 28d, 30b, 30d. 2 at this time
The phase output signal has a phase difference of 270 degrees, but is characteristically the same as described above.
【0063】また本発明は上述実施例に限ることなく、
本発明の要旨を逸脱することなく、その他種々の構成が
取り得ることは勿論である。The present invention is not limited to the above-described embodiment.
It goes without saying that various other configurations can be adopted without departing from the gist of the present invention.
【0064】[0064]
【発明の効果】本発明によればブリッジ回路の一の辺を
構成する複数のMR素子と他の辺を構成する複数のMR
素子との間隔を例えばλ/2とすることができると共に
90度位相の異なる2相の正弦波信号を得る複数のMR
素子の間隔を例えば(2+1/4)λとすることができ
信頼性の高い位置検出ができると共にこのMR素子間の
結線を交差することなく行うことができ、製造が容易と
なる利益がある。According to the present invention, a plurality of MR elements constituting one side of the bridge circuit and a plurality of MRs constituting the other side are provided.
A plurality of MRs that can set the interval with the element to, for example, λ / 2 and obtain two-phase sine-wave signals having a phase difference of 90 degrees
The distance between the elements can be set to, for example, (2 + λ) λ, the position can be detected with high reliability, and the connection between the MR elements can be performed without crossing.
【図1】本発明位置検出装置の例を示す構成図である。FIG. 1 is a configuration diagram showing an example of a position detection device of the present invention.
【図2】図1の検出ヘッドの等価回路を示す結線図であ
る。FIG. 2 is a connection diagram illustrating an equivalent circuit of the detection head of FIG. 1;
【図3】本発明位置検出装置の他の例を示す構成図であ
る。FIG. 3 is a configuration diagram showing another example of the position detection device of the present invention.
【図4】図3の検出ヘッドの等価回路を示す結線図であ
る。FIG. 4 is a connection diagram illustrating an equivalent circuit of the detection head of FIG. 3;
【図5】位置検出装置の例を示す斜視図である。FIG. 5 is a perspective view illustrating an example of a position detection device.
【図6】従来の位置検出装置の例を示す構成図である。FIG. 6 is a configuration diagram illustrating an example of a conventional position detection device.
【図7】出力回路の例を示す結線図である。FIG. 7 is a connection diagram illustrating an example of an output circuit.
【図8】従来の位置検出装置の例を示す構成図である。FIG. 8 is a configuration diagram illustrating an example of a conventional position detection device.
【図9】図8の検出ヘッドの等価回路を示す結線図であ
る。9 is a connection diagram illustrating an equivalent circuit of the detection head in FIG.
20,21,22,23,24,25,26,27 M
R素子群、20a,20b‥‥27d MR素子、28
a,28b,28c,28d,30a,30b,30
c,30d 開放端、29a,29b 出力端子20, 21, 22, 23, 24, 25, 26, 27 M
R element group, 20a, 20b ‥‥ 27d MR element, 28
a, 28b, 28c, 28d, 30a, 30b, 30
c, 30d open end, 29a, 29b output terminal
Claims (2)
はN極とS極との間隔)で目盛が磁気記録されている磁
気スケールと、磁気抵抗効果素子を使用した検出ヘッド
との相対位置を検出するようにした位置検出装置におい
て、 前記検出ヘッドは、間隔を(n/2−1/4)λ(nは
1,2,3‥‥の自然数)離して前記磁気スケールの目
盛の記録方向に複数の磁気抵抗効果素子群より成る組み
を2組配置し、この複数の磁気抵抗効果素子群は夫々の
間隔を(n+2)λ(nは1,2,3‥‥の自然数)離
して前記磁気スケールの目盛の記録方向に配置し、前記
磁気抵抗効果素子群はブリッジ回路の一の辺を構成する
少なくとも2つの磁気抵抗効果素子の直列回路と前記ブ
リッジ回路の他の辺を構成する少なくとも2つの磁気抵
抗効果素子の直列回路とから成ることを特徴とする位置
検出装置。1. An N-pole and an S-pole repeatedly having the same pitch λ (λ
A distance between a north pole and a south pole), and a position detecting device for detecting a relative position between a magnetic scale on which a scale is magnetically recorded and a detection head using a magnetoresistive element. Two sets each including a plurality of magnetoresistive element groups in the recording direction of the scale of the magnetic scale at an interval of (n / 2−1 / 4) λ (n is a natural number of 1, 2, 3 °). The plurality of magnetoresistive element groups are arranged in the recording direction of the scale of the magnetic scale at an interval of (n + 2) λ (n is a natural number of 1, 2, 3 °). The effect element group includes a series circuit of at least two magnetoresistive elements forming one side of the bridge circuit and a series circuit of at least two magnetoresistive elements forming the other side of the bridge circuit. Position detecting device.
1,2,3‥‥の整数)離して、前記磁気スケールの目
盛の記録方向に2個配置したことを特徴とする位置検出
装置。2. The position detecting device according to claim 1, wherein the distance between the detection heads is (n + /) λ (n is 0,
2. A position detecting device, wherein two magnetic scales are arranged in the recording direction of the scale of the magnetic scale at a distance from each other (an integer of 1, 2, 3).
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13202897A JPH10318705A (en) | 1997-05-22 | 1997-05-22 | Position detecting apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13202897A JPH10318705A (en) | 1997-05-22 | 1997-05-22 | Position detecting apparatus |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH10318705A true JPH10318705A (en) | 1998-12-04 |
Family
ID=15071818
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13202897A Pending JPH10318705A (en) | 1997-05-22 | 1997-05-22 | Position detecting apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH10318705A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN117197813A (en) * | 2023-08-21 | 2023-12-08 | 武汉博宇光电系统有限责任公司 | A deep learning-based analog instrument reading method |
-
1997
- 1997-05-22 JP JP13202897A patent/JPH10318705A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN117197813A (en) * | 2023-08-21 | 2023-12-08 | 武汉博宇光电系统有限责任公司 | A deep learning-based analog instrument reading method |
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