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JPH0260964B2 - - Google Patents
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JPH0260964B2 - - Google Patents

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Publication number
JPH0260964B2
JPH0260964B2 JP56211454A JP21145481A JPH0260964B2 JP H0260964 B2 JPH0260964 B2 JP H0260964B2 JP 56211454 A JP56211454 A JP 56211454A JP 21145481 A JP21145481 A JP 21145481A JP H0260964 B2 JPH0260964 B2 JP H0260964B2
Authority
JP
Japan
Prior art keywords
detection
position signal
circuit
magnetic
signal
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 - Lifetime
Application number
JP56211454A
Other languages
Japanese (ja)
Other versions
JPS58111719A (en
Inventor
Akyoshi Narimatsu
Akira Himuro
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Sony Magnescale Inc
Original Assignee
Sony Magnescale Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Sony Magnescale Inc filed Critical Sony Magnescale Inc
Priority to JP21145481A priority Critical patent/JPS58111719A/en
Publication of JPS58111719A publication Critical patent/JPS58111719A/en
Publication of JPH0260964B2 publication Critical patent/JPH0260964B2/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
    • G01D5/244Mechanical 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
    • G01D5/245Mechanical 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 using a variable number of pulses in a train
    • G01D5/2451Incremental encoders

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)

Description

【発明の詳細な説明】 本発明は変位量検出器、特に発磁体と検出ヘツ
ドとの相対変位量を検出する装置において、固定
後においても位置信号を精度良く簡単に調整可能
ならしめるための改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention is an improvement in a displacement detector, particularly in a device that detects the relative displacement between a magnet and a detection head, so that the position signal can be easily adjusted with high accuracy even after fixation. Regarding.

第1図に示す如く発磁体1、検出ヘツド2及び
検出回路から成る変位量検出器は発磁体と検出ヘ
ツド2間の相対位置を高精度で検出可能なことか
ら、原点検出器、リミツトスイツチ或いは変位量
検出装置等として各方面で多用されている。
As shown in Fig. 1, the displacement detector consisting of the magnetizing body 1, the detection head 2, and the detection circuit can detect the relative position between the magnetizing body and the detection head 2 with high precision, so it can be used as an origin detector, a limit switch, or a displacement detector. It is widely used in various fields as a quantity detection device.

しかし、従来の変位量検出器は位置信号の調整
が不便であつて時間のかかる欠点があつた。即
ち、発磁体1と検出ヘツド2とを一度工作機械等
に取り付けてしまうと、当然のことながら両者間
の相対信号と、その検出出力としての位置信号と
の関係は固定してしまうから、この関係を少しず
らす等の調整をしたい場合には、発磁体1或いは
検出ヘツド2の位置を上記関係が得られる量だけ
ずらして固定しなければならず、このような機械
的微調整を精度良く行なうことはかなり難しく、
多大の時間と作業工数を要していた。
However, conventional displacement detectors have the disadvantage that adjusting the position signal is inconvenient and time consuming. That is, once the magnet generator 1 and the detection head 2 are attached to a machine tool, etc., the relationship between the relative signal between them and the position signal as the detection output is fixed. If it is desired to make an adjustment such as slightly shifting the relationship, it is necessary to shift and fix the position of the magnet 1 or the detection head 2 by an amount that obtains the above relationship, and such fine mechanical adjustments must be made with high precision. It is quite difficult,
This required a large amount of time and man-hours.

そこで、第2図に示す如く、検出回路3を構成
して電気的に位置信号の調整を行なう方式が提案
されている。同図において、D1,D2はダイオー
ド、OPは演算増幅器、VR1〜VR3は可変抵抗、
ACは交流バイアス電源、+E、−Eは直流バイア
ス電圧で、発磁体1と検出ヘツド2との相対位置
に応じて、第3図の実線に示すような位置信号
V0が得られる。このような検出回路3によれば、
いずれの可変抵抗VR1〜VR3を調整しても第3図
の点線で示す如く位置信号V0を調整できる。
Therefore, as shown in FIG. 2, a method has been proposed in which the detection circuit 3 is configured to electrically adjust the position signal. In the figure, D 1 and D 2 are diodes, OP is an operational amplifier, VR 1 to VR 3 are variable resistors,
AC is an AC bias power supply, +E and -E are DC bias voltages, and depending on the relative position between the magnet generator 1 and the detection head 2, a position signal is generated as shown by the solid line in Fig. 3.
V 0 is obtained. According to such a detection circuit 3,
By adjusting any of the variable resistors VR 1 to VR 3 , the position signal V 0 can be adjusted as shown by the dotted line in FIG.

しかし検出出力、即ち位置信号の最も安定する
レベルが第3図の実線で示す如くx=0でV0
0となるレベルルであるにもかかわらず、可変抵
抗の位置によつて点線の如く上下にシフトしてx
=0でV0=0とはならず、一定出力がでるので、
温度ドリフトを無視できなくなつてしまうため、
あまり大きな調整範囲をとりにくい欠点がある。
However, the most stable level of the detection output, that is, the position signal, is at x=0 and V 0 =
Although the level is 0, it shifts up and down as shown by the dotted line depending on the position of the variable resistor and becomes x
= 0, V 0 will not be 0, and a constant output will be produced, so
Because temperature drift can no longer be ignored,
The drawback is that it is difficult to have a very large adjustment range.

本発明はかかる従来技術の欠点を改良するため
になされたもので、発磁体に対して所定間隔ずれ
るように2個の検出ヘツドを配設し、夫々の検出
出力を検出回路に与えて、発磁体と各検出ヘツド
の相対位置に対応する位置信号を得、その各位置
信号を合成し、その合成比率を変えることにより
合成された位置信号の原点を前記間隔の範囲内で
任意に設定できるように構成して、検出器の固定
後でも、位置信号を精度良く簡単に調整できるよ
うにしたことを特徴とする。
The present invention has been made in order to improve the drawbacks of the prior art. Two detection heads are arranged at a predetermined interval with respect to the magnet, and the detection outputs of the two detection heads are provided to a detection circuit. By obtaining position signals corresponding to the relative positions of the magnetic body and each detection head, combining the position signals, and changing the combination ratio, the origin of the combined position signal can be arbitrarily set within the range of the above-mentioned intervals. The present invention is characterized in that the position signal can be easily adjusted with high precision even after the detector is fixed.

以下図面に示す実施例を参照して本発明を説明
すると、第4図において、例えば発磁体1,1′
に対し2個の検出ヘツド2,2′を配設し、発磁
体1,1′の間隔をLとすれば、検出ヘツド2,
2′はlだけずらしてL+lの間隔とする。各検
出ヘツドからの検出出力は前記したような検出回
路3,3′に与えられ、前述した如く発磁体と検
出ヘツドとの相対位置に対応した位置信号V1
V2を得、例えば抵抗R1,R2によりV1,V2を合成
する。
The present invention will be described below with reference to embodiments shown in the drawings. In FIG.
If two detection heads 2, 2' are arranged for the detection heads 2, 2', and the spacing between the magnetic generators 1, 1' is L, then the detection heads 2, 2'
2' is shifted by l to provide an interval of L+l. The detection output from each detection head is given to the detection circuits 3, 3' as described above, and as described above, position signals V 1 ,
V 2 is obtained, and V 1 and V 2 are combined using, for example, resistors R 1 and R 2 .

而して上記位置信号V1,V2は第5図のように、
夫々の原点が前記間隔のずれlだけ離れたものと
なる。これら信号の直線部分は相対変位xに対し
下記のように近似できる。
The above position signals V 1 and V 2 are as shown in FIG.
The respective origins are separated by the distance l. The linear portion of these signals can be approximated to the relative displacement x as follows.

V1=K0x (1) V2=K2(x−l) (2) 但し、K1,K2は検出ヘツド及び検出回路の利
得である。
V 1 =K 0 x (1) V 2 =K 2 (x-l) (2) where K 1 and K 2 are the gains of the detection head and detection circuit.

従つてV1とV2の合成された位置信号V0′は各検
出回路の出力抵抗が無視し得るので、第11図に
示す第4図の等価回路から明らかなように、次式
で表される。
Therefore, since the output resistance of each detection circuit can be ignored, the position signal V 0 ' which is the composite of V 1 and V 2 can be expressed by the following equation, as is clear from the equivalent circuit of FIG. 4 shown in FIG. be done.

V0′=V1R2/R1+R2−V2R2/R1+R2+V2 =V1R2/R1+R2+V2R1/R1+R2 (3) =K1R2+K2R2/R1+R2(x+1/1+K1R2/K2R1
)(4) (4)式から明らかなように、合成された位置信号
V0′はK1R2とK2R1との比、つまり合成比率を変
えることによりその原点(V0′=0)をx=0〜
lの範囲内の任意の位置に対応するように設定で
きる。
V 0 ′=V 1 R 2 /R 1 +R 2 −V 2 R 2 /R 1 +R 2 +V 2 =V 1 R 2 /R 1 +R 2 +V 2 R 1 /R 1 +R 2 (3) =K 1 R 2 +K 2 R 2 /R 1 +R 2 (x+1/1+K 1 R 2 /K 2 R 1 l
)(4) As is clear from equation (4), the synthesized position signal
By changing the ratio of K 1 R 2 and K 2 R 1 , that is, the composition ratio, V 0 ′ can change its origin (V 0 =0) from x=0 to
It can be set to correspond to any position within the range of l.

上記合成比率を変えるには例えば合成用抵抗
R1とR2との比を変えればよい。即ち、K1とK2
発磁体と検出ヘツド間のギヤツプを決めると一定
として良いから、(4)式よりV0′=0の原点はK=
K1/K2として x=1/1+KR2/R1l (5) であり、R2/R1を0〜∽まで変化させると、V0′の 原点は0〜lまで変化させることができる。
To change the above synthesis ratio, for example, use a synthesis resistor.
Just change the ratio of R 1 and R 2 . That is, since K 1 and K 2 can be assumed to be constant once the gap between the magnetizing body and the detection head is determined, from equation (4), the origin of V 0 '=0 is K=
As K 1 /K 2 , x=1/1+KR 2 /R 1 l (5), and when R 2 /R 1 is changed from 0 to ∽, the origin of V 0 ' can be changed from 0 to l. can.

第6図は上記の変化方法を実施するための一回
路例で、検出回路3,3′の出力にR2とR1の比を
変えるための可変抵抗Rが接続されており、また
検出ヘツド2,2′は単一の交流バイアス電源AC
に接続されている。
Figure 6 shows an example of a circuit for carrying out the above variation method, in which a variable resistor R for changing the ratio of R 2 and R 1 is connected to the outputs of the detection circuits 3 and 3', and a detection head 2, 2' is a single AC bias power supply AC
It is connected to the.

また上記の方法とは逆にR1/R2の比を一定にする と、V0′の原点はR=R2/R1として x=1/1+RR2/R1・l (6) とからなる、K1/K2を変えればよく、そのための回 路例を第7図に示す。同図において、OP1及び
OP2は演算増幅器で、夫々検出回路2,2′と合
成用抵抗R1,R2との間に接続され、その利得調
整用可変抵抗VR1,VR2を変えることによりK1/K2 を変えることができる。なお、以上の実施例で
は、2個の検出ヘツド2,2′に対応して2個の
発磁体1,1′を用いたが、第8図及び第9図に
示すように2個の検出ヘツドを一体化した構造と
することにより発磁体を1個に減少させることが
できる。同図において、4は保持部材で、検出ヘ
ツド2,2′を構成するコア5,5′及びコイル
6,6′を一体的に保持する構造となつており、
発磁体1に対し両検出ヘツドはlの間隔がずれる
ように配設される。
Also, contrary to the above method, if the ratio of R 1 /R 2 is kept constant, the origin of V 0 ' is given by R=R 2 /R 1 , and x=1/1+RR 2 /R 1・l (6) It is only necessary to change K 1 /K 2 , and an example of a circuit for this purpose is shown in FIG. In the same figure, OP 1 and
OP 2 is an operational amplifier, which is connected between the detection circuits 2 and 2' and the combining resistors R 1 and R 2 , respectively, and by changing the gain adjustment variable resistors VR 1 and VR 2 , K 1 /K 2 can be changed. In the above embodiment, two magnetic generating bodies 1 and 1' were used corresponding to two detection heads 2 and 2', but as shown in FIGS. By making the head into an integrated structure, the number of magnetizing bodies can be reduced to one. In the figure, reference numeral 4 denotes a holding member, which is structured to integrally hold cores 5, 5' and coils 6, 6' that constitute the detection heads 2, 2'.
Both detection heads are arranged so as to be spaced apart from each other by l with respect to the magnet generating body 1.

このように構成しても合成用可変抵抗Rによつ
て合成された位置信号V0′は前記実施例と同様に
合成比率R2/R1又はK1/K2を変えることによりV0′の原 点を0〜lの範囲内で任意に設定できる。特に本
実施例では検出ヘツドを一体構造としているの
で、発磁体と両ヘツド間のクリアランスを同じに
設定でき、しかも両ヘツドの特性はそろえ易く、
その交流バイアスを同一電源から供給し得る。従
つて両ヘツドの検出感度をほぼ同じにできるの
で、前記(4)式でK1≒K2=K、R1+R2=R0として V0′=K(x−R1/R2l) (7) となるから、特性の点かられば1個の検出ヘツド
となし得る。
Even with this configuration, the position signal V 0 ' synthesized by the variable resistor R for synthesis can be changed to V 0 ' by changing the synthesis ratio R 2 /R 1 or K 1 /K 2 as in the previous embodiment. The origin of can be set arbitrarily within the range of 0 to l. In particular, in this embodiment, since the detection head has an integral structure, the clearance between the magnet and both heads can be set to be the same, and the characteristics of both heads can be easily matched.
The AC bias can be supplied from the same power supply. Therefore, since the detection sensitivities of both heads can be made almost the same, in equation (4) above, K 1 ≒ K 2 = K, R 1 + R 2 = R 0 , and V 0 '=K (x-R 1 /R 2 l ) (7) Therefore, from the point of view of the characteristics, it can be treated as one detection head.

第10図は上記実施例における各点の出力特性
を示す実測図である。
FIG. 10 is an actual measurement diagram showing the output characteristics at each point in the above embodiment.

以上説明したように本発明によれば検出器と固
定した後でも、位置信号を精度良く微調整するこ
とができ実用に供してその効果著である。
As explained above, according to the present invention, the position signal can be finely adjusted with high accuracy even after being fixed to the detector, and the effect is remarkable when it is put to practical use.

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

第1図は本発明の対象とする変位量検出器の基
本的構成を示す略線図、第2図は該変位量検出器
における従来の検出回路の一例を示す回路図、第
3図はその出力特性図、第4図は本発明の一実施
例を示す概略図、第5図はその出力特性図、第6
図及び第7図は夫々該実施例における位置信号の
合成比率を変化する方法を示す回路図、第8図及
び第9図は本発明の他の実施例を示す図、第10
図はその出力特性実測図、第11図は第4図の等
価回路図である。 1,1′…発磁体、2,2′…検出ヘツド、3,
3′…検出回路、R…合成用可変抵抗。
Fig. 1 is a schematic diagram showing the basic configuration of a displacement detector to which the present invention is applied, Fig. 2 is a circuit diagram showing an example of a conventional detection circuit in the displacement detector, and Fig. 3 is a circuit diagram thereof. Output characteristic diagram, Figure 4 is a schematic diagram showing an embodiment of the present invention, Figure 5 is its output characteristic diagram, Figure 6 is a schematic diagram showing an embodiment of the present invention.
7 and 7 are circuit diagrams respectively showing a method of changing the combination ratio of position signals in this embodiment, FIGS. 8 and 9 are diagrams showing another embodiment of the present invention, and FIG.
The figure is an actual measurement diagram of its output characteristics, and FIG. 11 is an equivalent circuit diagram of FIG. 4. 1, 1'... Magnetizing body, 2, 2'... Detection head, 3,
3'...Detection circuit, R...Variable resistance for synthesis.

Claims (1)

【特許請求の範囲】 1 2つの発磁体と、これら発磁体の間隔に対し
所定長さだけずれた間隔を有するように配設さ
れ、夫々の発磁体に近づくに従つてその時期に感
応して電気信号を発生する2個の検出ヘツドと、
各検出ヘツドから出力される夫々の電気信号に応
答して上記各発磁体と各検出ヘツドとの相対位置
に対応した2つの位置信号を発生する検出回路
と、夫々の位置信号を合成比率可変回路を介して
合成して、合成された1つの位置信号を発生する
位置信号合成手段と、を備え、上記合成比率可変
回路によつて上記2つの位置信号の合成比率を調
節することにより上記合成された位置信号の原点
を上記所定長さの範囲内で設定可能としたことを
特徴とする変位量検出器。 2 1つの発磁体と、この発磁体の長さに対し所
定長さだけずれた間隔を有するように配設され、
夫々の発磁体に近づくに従つてその磁気に感応し
て電気信号を発生する2個の一体に保持された検
出ヘツドと、各検出ヘツドから出力される夫々の
電気信号に応答して上記各発磁体と各検出ヘツド
との相対位置に対応した2つの位置信号を発生す
る検出回路と、夫々の位置信号を合成比率可変回
路を介して合成して、合成された1つの位置信号
を発生する位置信号合成手段と、を備え、上記合
成比率可変回路によつて上記2つの位置信号の合
成比率を調節することにより上記合成された位置
信号の原点を上記所定長さの範囲内で設定可能と
したことを特徴とする変位量検出器。
[Scope of Claims] 1. Two magnet generating bodies, which are arranged so as to have an interval deviated by a predetermined length with respect to the interval between these magnetic bodies, and as they approach each magnetic body, the distance between the magnetic bodies changes depending on the timing. two detection heads that generate electrical signals;
A detection circuit that generates two position signals corresponding to the relative positions of each of the magnetic generators and each detection head in response to each electric signal output from each detection head, and a variable ratio circuit that synthesizes each position signal. position signal synthesis means for synthesizing the two position signals to generate one synthesized position signal, and adjusting the synthesis ratio of the two position signals by the synthesis ratio variable circuit to generate one synthesized position signal. A displacement detector characterized in that the origin of the position signal can be set within the range of the predetermined length. 2. One magnet generating body, arranged so as to have an interval deviated by a predetermined length with respect to the length of the magnet generating body,
Two integrally held detection heads generate electrical signals in response to the magnetism as they approach each magnetic generating body, and each of the above-mentioned generators responds to the respective electrical signals output from each detection head. A detection circuit that generates two position signals corresponding to the relative position of the magnetic body and each detection head, and a position that generates one synthesized position signal by synthesizing the respective position signals via a variable synthesis ratio circuit. A signal synthesizing means is provided, and the origin of the synthesized position signal can be set within the range of the predetermined length by adjusting the synthesis ratio of the two position signals by the variable synthesis ratio circuit. A displacement detector characterized by:
JP21145481A 1981-12-25 1981-12-25 Displacement quantity detector Granted JPS58111719A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21145481A JPS58111719A (en) 1981-12-25 1981-12-25 Displacement quantity detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21145481A JPS58111719A (en) 1981-12-25 1981-12-25 Displacement quantity detector

Publications (2)

Publication Number Publication Date
JPS58111719A JPS58111719A (en) 1983-07-02
JPH0260964B2 true JPH0260964B2 (en) 1990-12-18

Family

ID=16606205

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21145481A Granted JPS58111719A (en) 1981-12-25 1981-12-25 Displacement quantity detector

Country Status (1)

Country Link
JP (1) JPS58111719A (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6463824A (en) * 1987-09-02 1989-03-09 Fuji Photo Film Co Ltd Light and color measuring device for printing control
JPH0740173Y2 (en) * 1988-09-29 1995-09-13 多摩川精機株式会社 Angle detector
JPH02110566A (en) * 1988-10-20 1990-04-23 Fuji Photo Film Co Ltd Photometer and colorimeter for print control
US5514952A (en) * 1993-06-30 1996-05-07 Simmonds Precision Products Inc. Monitoring apparatus for rotating equipment dynamics for slow checking of alignment using plural angled elements
US5508609A (en) * 1993-06-30 1996-04-16 Simmonds Precision Product Inc. Monitoring apparatus for detecting axial position and axial alignment of a rotating shaft
US5456123A (en) * 1994-01-26 1995-10-10 Simmonds Precision Products, Inc. Static torque measurement for rotatable shaft

Also Published As

Publication number Publication date
JPS58111719A (en) 1983-07-02

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