JPH0574003B2 - - Google Patents
Info
- Publication number
- JPH0574003B2 JPH0574003B2 JP62255894A JP25589487A JPH0574003B2 JP H0574003 B2 JPH0574003 B2 JP H0574003B2 JP 62255894 A JP62255894 A JP 62255894A JP 25589487 A JP25589487 A JP 25589487A JP H0574003 B2 JPH0574003 B2 JP H0574003B2
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- coil
- coils
- shield
- metal
- 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
Links
Landscapes
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Transmission And Conversion Of Sensor Element Output (AREA)
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は変位演算素子に関し、特に磁性体部材
に直列接続して配設した2つの導体コイルと空間
的に重なり合う2つの金属導体シールドと磁性体
部材(導体コイル)との間の2つの微小変位の
和、差および積を検出する変位演算素子に関す
る。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a displacement calculation element, and in particular, to a displacement calculation element, in which two conductor coils are connected in series to a magnetic member, two metal conductor shields spatially overlap each other, and a magnetic The present invention relates to a displacement calculation element that detects the sum, difference, and product of two minute displacements with respect to a body member (conductor coil).
数値制御工作機器等では、物体の変位を精度良
く検出することは極めて重要な技術である。物体
の変位を検出する技術としては、従来次の諸技術
が広くしられている。即ち、ポテンシヨメータを
介して変位量を電気抵抗値に変換する方法、歪み
ゲージを用いる方法、ホール効果又は磁気抵抗効
果を用いるマグネスケールを利用する方法、光エ
ンコーダを用いる方法、レーザー光の反射とその
位相ずれを利用する光干渉法、超音波反射とその
位相ずれを利用する超音波干渉法等である。
In numerically controlled machine tools, etc., it is an extremely important technology to accurately detect the displacement of an object. Conventionally, the following techniques are widely known as techniques for detecting the displacement of an object. That is, a method of converting the amount of displacement into an electrical resistance value via a potentiometer, a method of using a strain gauge, a method of using a Magnescale using the Hall effect or magnetoresistive effect, a method of using an optical encoder, and a method of reflecting laser light. These include optical interferometry, which uses ultrasonic reflection and its phase shift, and ultrasonic interferometry, which utilizes ultrasonic reflection and its phase shift.
ポテンシヨメータで変位を検出するためには、
電気抵抗体と位置検出用電極を接触させ、たがい
に摺動させる必要がある。この方法では、電極の
接触摺動が不可欠となる。 To detect displacement with a potentiometer,
It is necessary to bring the electric resistor and the position detection electrode into contact and to slide them against each other. In this method, contact sliding of the electrodes is essential.
歪みゲージは、電気抵抗線の長さが変化したと
きの電気抵抗値の変化によつて歪み量を検出する
ものである。従つて、物体の変位を検出するには
その物体と基準位置とをこの歪みゲージで繋ぐ必
要がある。 A strain gauge detects the amount of strain based on a change in electrical resistance value when the length of an electrical resistance wire changes. Therefore, in order to detect the displacement of an object, it is necessary to connect the object and the reference position using this strain gauge.
マグネスケールは、直線状の高保磁力磁性体を
その長さ方向に規則正しく正逆に磁化したもので
ある。このマグネスケールの近傍にホール効果或
は磁気抵抗効果を用いた磁界センサを設ける。磁
界センサをマグネスケールに沿つて移動させ、磁
界センサが検知する磁界変動数を用いて磁界セン
サの移動量即ち変位を計算する。 Magnescale is a linear high-coercivity magnetic material that is regularly magnetized in the normal and reverse directions along its length. A magnetic field sensor using the Hall effect or magnetoresistive effect is provided near this magnetescale. The magnetic field sensor is moved along the magnet scale, and the amount of movement, that is, the displacement of the magnetic field sensor is calculated using the number of changes in the magnetic field detected by the magnetic field sensor.
光エンコーダによる変位検出も、マグネスケー
ルと同様に複雑な光学パタンを持つスケールと、
光強度変化から変位を計算する。 Displacement detection using an optical encoder also uses a scale with a complex optical pattern similar to Magnescale.
Calculate displacement from changes in light intensity.
光干渉法や超音波干渉法を用いる変位測定で
は、光源や音波源から発する光や超音波を物体に
照射し、物体から反射してくる光や超音波の位相
を検出して、物体の移動に伴う位相の変化を検出
して、変位を算出する。 Displacement measurement using optical interferometry or ultrasonic interferometry involves irradiating an object with light or ultrasonic waves emitted from a light source or sound wave source, detecting the phase of the light or ultrasonic waves reflected from the object, and measuring the movement of the object. The displacement is calculated by detecting the change in phase associated with the change in phase.
又、二つの変位量を用いて、その和、差、積な
どを計算する場合には、これらの変位測定手段で
変位を算出した後、改めて計算手段或は演算回路
を用いて計算する必要があつた。 In addition, when calculating the sum, difference, product, etc. using two displacement amounts, it is necessary to calculate the displacement using these displacement measurement means and then calculate it again using a calculation means or an arithmetic circuit. It was hot.
上述した従来の変位検出技術はそれぞれ次のよ
うな欠点がある。
The conventional displacement detection techniques described above each have the following drawbacks.
すなわち、ポテンシヨメータで変位を検出する
技術では位相検出用電極の接触摺動が不可欠であ
るため摩耗に基づく耐久性や信頼性の問題があ
る。 That is, in the technology of detecting displacement using a potentiometer, since contact and sliding of the phase detection electrode is essential, there are problems with durability and reliability due to wear.
歪みゲージで変位を検出する技術は、繰返し使
用による電気抵抗線の塑性変形をもたらし、信頼
性に欠け、さらに圧縮方向の変位の測定が困難で
あるという欠点がある。 The technique of detecting displacement with a strain gauge has the disadvantage that repeated use causes plastic deformation of the electrical resistance wire, lacks reliability, and furthermore makes it difficult to measure displacement in the compression direction.
マグネスケールにより変位を検出する技術は、
複雑な構成を必要とするばかりでなく高価な計算
手段を要するという欠点がある。 The technology to detect displacement using Magnescale is
It has the disadvantage that it not only requires a complicated structure but also requires expensive calculation means.
光エンコーダにより変位を検出する技術は、マ
グネスケールと同様に複雑な光学パターンを有す
るスケールと光強度変化から変位を計算する複雑
な回路を必要とするという欠点がある。 The technique of detecting displacement using an optical encoder has the disadvantage that, like the Magnescale, it requires a scale with a complicated optical pattern and a complicated circuit for calculating displacement from changes in light intensity.
光干渉法や超音波干渉法により変位を検出する
技術は、高価な光源や音源を必要とするほか、高
精度の位相検出器ならびに検出した位相変化から
変位を計算する高性能の計算手段が必要とろると
いう欠点がある。 Technologies that detect displacement using optical interferometry or ultrasonic interferometry require expensive light and sound sources, as well as high-precision phase detectors and high-performance calculation means to calculate displacement from detected phase changes. There is a drawback that it is melty.
さらに、2つの変位量を用いて和、差、積など
を計測する場合には、上述した各変位測定手段で
変位を算出したのち、あらためて計算することが
必要であるという欠点がある。 Furthermore, when measuring the sum, difference, product, etc. using two displacement amounts, there is a drawback that it is necessary to calculate the displacement again after calculating the displacement with each of the above-mentioned displacement measuring means.
本発明の目的は上述した欠点を除去し、簡素か
つ安価な構成で信頼度の高い変位量の差、和及び
積の演算ができる測定容易な変位演算素子を提供
することにある。 SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks and to provide a displacement calculation element that is easy to measure and can calculate the difference, sum, and product of displacement amounts with a simple and inexpensive configuration and with high reliability.
本発明の変位演算素子は、棒状軟磁性体の互い
に相離れた3箇所にそれぞれ第1及び第2ならび
に第3の導体コイルを前記第2と第3の導体コイ
ル間に前記第1の導体コイルが介在するように設
けたうえ前記第1の導体コイルには交番電流を印
加し前記第2の導体コイルと第3の導体コイルは
磁気的には逆方向でかつ電気的には直列に接続さ
れるとともに前記第2及び第3の導体コイル近傍
の周囲にはそれぞれ第1及び第2の金属導体シー
ルドを設けて前記導体コイルと金属導体シールド
との重なり長さがそれぞれ独立に可変としうる構
造、もしくは棒状軟磁性体の互いに相離れた3箇
所にそれぞれ第1及び第2ならびに第3の導体コ
イルを前記第2と第3の導体コイル間に前記第1
の導体コイルが介在するように設けたうえ前記第
1の導体コイルには交番電流を印加前記第2の導
体コイルと第3の導体コイルは磁気的には同方向
でかつ電気的には直列に接続されるとともに前記
第2及び第3の導体コイル近傍の周囲にはそれぞ
れ第1及び第2の金属導体シールドを設けて前記
導体コイルと金属導体シールドとの重なり長さが
それぞれ独立に可変としうる構造、もしくは棒状
軟磁性体の互いに相離れた2箇所にそれぞれ第1
及び第2の導体コイルを設けるとともに前記第1
及び第2の導体コイルのいずれか一方には交番電
流を印加し前記第1及び第2のコイルの近傍の周
囲にはそれぞれ金属導体シールドを配したうえ前
記コイルと導体シールドとの重なり長さがそれぞ
れ独立に可変としうる構造を備えて構成される。
In the displacement calculation element of the present invention, first, second, and third conductor coils are respectively arranged at three locations apart from each other on a rod-shaped soft magnetic body, and the first conductor coil is disposed between the second and third conductor coils. is provided so that an alternating current is applied to the first conductor coil, and the second conductor coil and the third conductor coil are connected magnetically in opposite directions and electrically in series. and a structure in which first and second metal conductor shields are provided around the second and third conductor coils, respectively, so that the overlapping length of the conductor coil and the metal conductor shield can be independently varied, Alternatively, the first, second, and third conductor coils are respectively placed at three locations apart from each other on the rod-shaped soft magnetic material, and the first, second, and third conductor coils are disposed between the second and third conductor coils.
A conductor coil is provided so that an alternating current is applied to the first conductor coil, and the second conductor coil and the third conductor coil are magnetically in the same direction and electrically in series. First and second metal conductor shields are provided around the second and third conductor coils, respectively, so that the overlapping length of the conductor coil and the metal conductor shield can be independently varied. The structure or the rod-shaped soft magnetic material has two first parts located apart from each other.
and a second conductor coil, and the first conductor coil.
An alternating current is applied to either one of the first and second conductor coils, a metal conductor shield is arranged around the first and second coils, and the overlapping length of the coil and the conductor shield is Each of them is constructed with a structure that can be independently varied.
本発明は、以下の原理に基づいて作用する。す
なわち、棒状の軟磁性体の一部に励磁コイルを付
して交番電流を印加する。棒状の軟磁性体の励磁
コイルとは相離れた一端に磁束検出コイルを設け
ると、この検出コイルには電磁誘導により励磁電
流の周波数と振幅に比例する電圧が生じる。この
磁束検出コイルを空間的に囲むように電気伝導度
の高い材料でシールドを設ける。棒状の軟磁性体
の一端から発生する磁界が導体シールド内に渦電
流を生じさせ、この渦電流が磁性体に逆磁界を生
じる。従つて、シールドされた磁性体部には実質
的に磁束が存在し無くなる。換言すれば、シール
ドと磁束検出コイルの重なり領域には実質的に磁
束がなく、重なりの大きさに比例して磁束検出コ
イルに生じる誘導電圧は減少する。しかして、こ
の重なりの大きさは、変位に対応する。導体シー
ルドと磁束検出コイルとは接触している必要はな
く、この原理を用いることにより非接触変位セン
サが実現される。更に、シールドを磁性体の両端
部に設けることにより二つの変位量の演算が可能
となる。
The invention operates on the following principles. That is, an excitation coil is attached to a part of the rod-shaped soft magnetic material and an alternating current is applied thereto. When a magnetic flux detection coil is provided at one end of a bar-shaped soft magnetic material separated from the excitation coil, a voltage proportional to the frequency and amplitude of the excitation current is generated in the detection coil due to electromagnetic induction. A shield made of a material with high electrical conductivity is provided so as to spatially surround this magnetic flux detection coil. A magnetic field generated from one end of the rod-shaped soft magnetic material generates an eddy current in the conductive shield, and this eddy current creates a reverse magnetic field in the magnetic material. Therefore, substantially no magnetic flux exists in the shielded magnetic material portion. In other words, there is substantially no magnetic flux in the overlapping region of the shield and the magnetic flux detection coil, and the induced voltage generated in the magnetic flux detection coil decreases in proportion to the magnitude of the overlap. The magnitude of this overlap thus corresponds to the displacement. The conductor shield and the magnetic flux detection coil do not need to be in contact with each other, and by using this principle, a non-contact displacement sensor can be realized. Furthermore, by providing shields at both ends of the magnetic body, calculation of two displacement amounts becomes possible.
次に図面を参照して本発明を説明する。 Next, the present invention will be explained with reference to the drawings.
第1図Aは本発明の変位演算素子の第1の実施
例の構成図、第1図Bは第1図Aの実施例の検出
コイルの出力特性図である。第1図Aに示す第1
の実施例は、棒状軟磁性体としての軟磁性体パタ
ン1と、軟磁性体パタン1の両端近傍に電気的に
は直列接続、磁気的には巻線方向を互いに逆とし
て逆特性を有するように配設した一対の検出コイ
ル3及び5と、検出コイル3と5との間に介在さ
せて配設し交番電流源20により交番電流を印加
して軟磁性体パタン1を磁化する励磁コイル2
と、検出コイル3及び5と空間的に非接触状態で
重なり合うように同心的に配置した一対の導体シ
ールドパタン4及び5を備える。導体シールドパ
タン4と検出コイル3との重なり長さをx1、導体
シールドパタン6と検出コイル5との重なり長さ
をx2とすると、検出コイル3,5単独での出力は
それぞれ重なり長さx1とx2に比例し極性は互い
に逆である。両コイルの合成出力は、第1図Bに
示すように(x1−x2)に比例する。即ち、本実施
例は、なんら特別な演算回路を用いなくとも二つ
の変位量の差を容易に求める演算素子を提供する
ものである。 FIG. 1A is a block diagram of a first embodiment of the displacement calculation element of the present invention, and FIG. 1B is an output characteristic diagram of the detection coil of the embodiment of FIG. 1A. The first shown in Figure 1A
In the embodiment, a soft magnetic material pattern 1 as a rod-shaped soft magnetic material is electrically connected in series near both ends of the soft magnetic material pattern 1, and magnetically the winding directions are reversed to have opposite characteristics. a pair of detection coils 3 and 5 arranged at
and a pair of conductor shield patterns 4 and 5 arranged concentrically so as to spatially overlap with the detection coils 3 and 5 in a non-contact state. If the overlapping length between the conductor shield pattern 4 and the detection coil 3 is x 1 and the overlapping length between the conductor shield pattern 6 and the detection coil 5 is x 2 , then the output of the detection coils 3 and 5 alone is the overlap length. They are proportional to x1 and x2, and their polarities are opposite to each other. The combined output of both coils is proportional to (x 1 -x 2 ) as shown in FIG. 1B. That is, this embodiment provides an arithmetic element that can easily determine the difference between two displacement amounts without using any special arithmetic circuit.
第2図Aは本発明の変位演算素子の第2の実施
例の構成図である。第2図Aに示すように、軟磁
性体パタン1、励磁コイル2、検出コイル3,
5、交番電流源20及び導体シールドパタン4,
6は、第1図Aの場合とほぼ同じである。異なる
点は、検出コイルの巻線方向が第1図Aの場合と
逆となり同一方向に巻いてある点である。導体シ
ールドパタン4と検出コイル3との重なり長さを
x1、導体シールドパタン6と検出コイル5との重
なり長さをx2とすると、検出コイル3,5単独で
の出力は第1図Aの実施例からも容易に解るよう
にそれぞれ−x1及び−x2に比例する。従つて、両
コイルの合成出力は、第2図Bに示すように(x1
+x2)に比例する。即ち、本実施例は、なんら特
別な演算回路を用いなくとも二つの変位量の和を
容易に求める演算素子を提供するものである。 FIG. 2A is a block diagram of a second embodiment of the displacement calculation element of the present invention. As shown in FIG. 2A, a soft magnetic material pattern 1, an excitation coil 2, a detection coil 3,
5, alternating current source 20 and conductor shield pattern 4,
6 is almost the same as in FIG. 1A. The difference is that the winding direction of the detection coil is opposite to that in FIG. 1A and is wound in the same direction. The overlapping length of conductor shield pattern 4 and detection coil 3 is
x 1 , and the overlapping length between the conductor shield pattern 6 and the detection coil 5 is x 2 , the output of the detection coils 3 and 5 alone is -x 1 , as can be easily seen from the embodiment shown in FIG. 1A. and −x is proportional to 2 . Therefore, the combined output of both coils is (x 1
+x 2 ). That is, this embodiment provides an arithmetic element that can easily calculate the sum of two displacement amounts without using any special arithmetic circuit.
第3図は本発明の変位演算素子の第3の実施例
の構成図である。第3図に示す変位演算素子は、
第1図と同じ軟磁性体パタン1と、第1の導体コ
イルとしての検出コイル3と、第2の導体コイル
としての励磁コイル2と、第1及び第2の導体シ
ールドパタン4及び6とを備え、なお交番電流源
20を併記して示す。導体シールド4と検出コイ
ル3との重なり長さをx1、導体シールドパタン6
と励磁コイル2との重なり長さをx2とすると、励
磁コイルから発生する磁束は、x2に比例して減少
する。このx2に比例した磁束を検出コイル3は検
出するが、この際x1に比例して検出出力は減少す
る。即ち、この検出出力は、結果としてx1・x2に
比例することになる。換言すれば、本実施例は、
なんら特別な演算回路を用いなくとも二つの変位
量の積を容易に求める演算素子を提供するもので
ある。 FIG. 3 is a configuration diagram of a third embodiment of the displacement calculation element of the present invention. The displacement calculation element shown in Fig. 3 is
The same soft magnetic material pattern 1 as in FIG. 1, a detection coil 3 as a first conductor coil, an excitation coil 2 as a second conductor coil, and first and second conductor shield patterns 4 and 6. In addition, an alternating current source 20 is also shown. The overlapping length of conductor shield 4 and detection coil 3 is x 1 , conductor shield pattern 6
When the overlapping length between the excitation coil 2 and the excitation coil 2 is x2, the magnetic flux generated from the excitation coil decreases in proportion to x2 . The detection coil 3 detects the magnetic flux proportional to x 2 , but at this time the detection output decreases in proportion to x 1 . That is, this detection output is proportional to x 1 x 2 as a result. In other words, in this example,
The present invention provides an arithmetic element that easily calculates the product of two displacement amounts without using any special arithmetic circuit.
なお、第3図に示す第3の実施例において、交
番電源を第2の検出コイルたる励磁コイル2に印
加しているが、これを検出コイル3に印加するも
のとしても同様に実施しうることは明らかであ
る。 Note that in the third embodiment shown in FIG. 3, the alternating power supply is applied to the excitation coil 2, which is the second detection coil, but it can also be applied to the detection coil 3 in the same way. is clear.
以上述べたように本発明によれば、棒状の磁性
部材の両端に検出コイルを配設し、かつこれら検
出コイルと空間的に重なり合う導体シールドを配
置したうえ専用の励磁コイルもしくはいずれかの
検出コイルを利用する励磁コイルで交流励磁する
ことにより、棒状の磁性部材に対する2つの検出
コイルの変位の和、差および積を特別な演算回路
を要することなく、高感度、高信頼性を確保して
容易に求めることができる効果がある。
As described above, according to the present invention, detection coils are arranged at both ends of a rod-shaped magnetic member, conductor shields are arranged that spatially overlap these detection coils, and a dedicated excitation coil or any detection coil is arranged. By using an excitation coil that uses AC excitation, it is possible to easily calculate the sum, difference, and product of the displacement of two detection coils with respect to a rod-shaped magnetic member, ensuring high sensitivity and high reliability without the need for a special calculation circuit. It has the desired effect.
第1図Aは本発明の第1の実施例の構成図、第
1図Bは第1図Aの検出コイルの出力特性図、第
2図Aは本発明の第2の実施例の構成図、第2図
Bは第2図Aの検出コイルの出力特性図、第3図
は本発明の第3の実施例の構成図である。
1……軟磁性体パタン、2……励磁コイル、
3,5……検出コイル、4,6……導体シールド
パタン、20……交番電流源。
Fig. 1A is a block diagram of the first embodiment of the present invention, Fig. 1B is an output characteristic diagram of the detection coil of Fig. 1A, and Fig. 2A is a block diagram of the second embodiment of the present invention. , FIG. 2B is an output characteristic diagram of the detection coil of FIG. 2A, and FIG. 3 is a configuration diagram of a third embodiment of the present invention. 1... Soft magnetic material pattern, 2... Excitation coil,
3, 5...detection coil, 4, 6...conductor shield pattern, 20...alternating current source.
Claims (1)
ぞれ第1及び第2ならびに第3の導体コイルを前
記第2と第3の導体コイル間に前記第1の導体コ
イルが介在するように設けたうえ前記第1の導体
コイルには交番電流を印加し前記第2の導体コイ
ルと第3の導体コイルは磁気的には逆方向でかつ
電気的には直列に接続されるとともに前記第2及
び第3の導体コイル近傍の周囲にはそれぞれ第1
及び第2の金属導体シールドを設け前記第2及び
第3の導体コイルと前記第1及び第2の金属導体
シールドとの空間的な重なり長さがそれぞれ独立
に可変としうる構造を有し、前記第1の金属導体
シールドと前記第2の導体コイルとの空間的な重
なり長さx1と前記第2の金属導体シールドと前
記第3の導体コイルとの空間的な重なり長さx2
との差(x1−x2)に対応する出力を前記棒状軟
磁性体に対する前記第1及び第2の金属導体シー
ルドの変位量差として前記第2の導体コイルと前
記第3の導体コイルの両端間に出力することを特
徴とする変位演算素子。 2 棒状軟磁性体の互いに相離れた3箇所にそれ
ぞれ第1及び第2ならびに第3の導体コイルを前
記第2と第3の導体コイル間に前記第1の導体コ
イルが介在するように設けたうえ前記第1の導体
コイルには交番電流を印加し前記第2の導体コイ
ルと第3の導体コイルは磁気的には同方向でかつ
電気的には直列に接続されるとともに前記第2及
び第3の導体コイル近傍の周囲にはそれぞれ第1
及び第2の金属導体シールドを設けて前記第2及
び第3の導体コイルと前記第1及び第2の金属導
体シールドとの空間的な重なり長さがそれぞれ独
立に可変としうる構造を有し、前記第1の金属導
体シールドと前記第2の導体コイルとの空間的な
重なり長さx1と前記第2の金属導体シールドと
前記第3の導体コイルとの空間的な重なり長さ
x2との和(x1+x2)に対応する出力を前記棒状
軟磁性体に対する前記第1及び第2の金属導体シ
ールドの変位量和として前記第2の導体コイルと
前記第3の導体コイルの両端間に出力することを
特徴とする変位演算素子。 3 棒状軟磁性体の互いに相離れた2箇所にそれ
ぞれ第1及び第2の導体コイルを設けるとともに
前記第1及び第2の導体コイルいずれか一方を励
磁コイルとして交番電流を印加し前記第1及び第
2のコイルの近傍の周囲にはそれぞれ第1及び第
2の金属導体シールドを配したうえ前記第1及び
第2の導体コイルと前記第1及び第2の導体シー
ルドとの空間的な重なり長さがそれぞれ独立に可
変としうる構造を有し、前記第1の金属導体シー
ルドと前記第1の導体コイルとの空間的な重なり
長さx1と前記第2の金属導体シールドと前記第
3の導体コイルとの空間的な重なり長さx2との
積(x1・x2)に対応する出力を前記棒状軟磁性
体に対する前記第1及び第2の金属導体シールド
の変位量積として前記第1及び第2の導体コイル
の励磁コイルとしない他方の導体コイルの両端間
に出力することを特徴とする変位演算素子。[Scope of Claims] 1. First, second, and third conductor coils are respectively placed at three locations apart from each other on a rod-shaped soft magnetic body, and the first conductor coil is disposed between the second and third conductor coils. An alternating current is applied to the first conductor coil, and the second conductor coil and the third conductor coil are magnetically connected in opposite directions and electrically connected in series. At the same time, there are first conductor coils around the second and third conductor coils, respectively.
and a second metal conductor shield having a structure in which spatial overlapping lengths of the second and third conductor coils and the first and second metal conductor shields can be independently varied, Spatial overlap length x1 between the first metal conductor shield and the second conductor coil and spatial overlap length x2 between the second metal conductor shield and the third conductor coil
The output corresponding to the difference (x1 - x2) between both ends of the second conductor coil and the third conductor coil is calculated as the difference in displacement of the first and second metal conductor shields with respect to the rod-shaped soft magnetic body. A displacement calculation element characterized by outputting. 2. First, second, and third conductor coils are provided at three mutually distant locations of the rod-shaped soft magnetic material such that the first conductor coil is interposed between the second and third conductor coils. Furthermore, an alternating current is applied to the first conductor coil, and the second and third conductor coils are connected magnetically in the same direction and electrically in series, and Each of the first conductor coils is placed around the third conductor coil.
and a structure in which a second metal conductor shield is provided so that the spatial overlapping lengths of the second and third conductor coils and the first and second metal conductor shields can be varied independently, a spatial overlap length x1 between the first metal conductor shield and the second conductor coil; and a spatial overlap length x1 between the second metal conductor shield and the third conductor coil.
The output corresponding to the sum (x1+x2) of A displacement calculation element characterized by output. 3. First and second conductor coils are provided at two mutually apart locations of the rod-shaped soft magnetic material, and an alternating current is applied using one of the first and second conductor coils as an excitation coil, so that the first and second conductor coils are First and second metal conductor shields are arranged around the vicinity of the second coil, respectively, and the spatial overlapping length between the first and second conductor coils and the first and second conductor shields is determined. a spatial overlap length x1 between the first metal conductor shield and the first conductor coil, and a spatial overlap length x1 between the second metal conductor shield and the third conductor coil; The output corresponding to the product (x1 x A displacement calculation element characterized in that an output is output between both ends of the excitation coil of the conductor coil and the other conductor coil.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP25589487A JPH0196511A (en) | 1987-10-08 | 1987-10-08 | Displacement detecting element and displacement arithmetic element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP25589487A JPH0196511A (en) | 1987-10-08 | 1987-10-08 | Displacement detecting element and displacement arithmetic element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0196511A JPH0196511A (en) | 1989-04-14 |
| JPH0574003B2 true JPH0574003B2 (en) | 1993-10-15 |
Family
ID=17285046
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP25589487A Granted JPH0196511A (en) | 1987-10-08 | 1987-10-08 | Displacement detecting element and displacement arithmetic element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0196511A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5789915A (en) * | 1989-02-17 | 1998-08-04 | Nartron Corporation | Magnetic field energy responsive position sensing apparatus and method |
| GB2435518B (en) * | 2006-02-28 | 2009-11-18 | Alexy Davison Karenowska | Position sensor |
| JP2009204348A (en) * | 2008-02-26 | 2009-09-10 | Panasonic Electric Works Co Ltd | Position sensor |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB2012431A (en) * | 1977-08-17 | 1979-07-25 | Hayter J E | Electromagnetic Position Transducer Uses Eddy Currents Induced in Conductive Member |
-
1987
- 1987-10-08 JP JP25589487A patent/JPH0196511A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0196511A (en) | 1989-04-14 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP3246727B2 (en) | Inductive electronic caliper | |
| CN110657826B (en) | Scale construction for inductive position encoders | |
| EP0390261B1 (en) | Device for measuring a relative displacement | |
| US4229696A (en) | Sensor for measuring magnetic field changes | |
| JPH0464007B2 (en) | ||
| JPH09508466A (en) | Micro coil device made by flattening technology to detect ferromagnetic material | |
| SE7501217L (en) | ||
| JPH0229961B2 (en) | ||
| JP4390347B2 (en) | Position detection device | |
| US3178696A (en) | Position transducers | |
| US20150061650A1 (en) | Method and arrangement and sensor for determing the postion of a component | |
| JPH0574003B2 (en) | ||
| JPS63271112A (en) | Position detecting device | |
| JPS6411969B2 (en) | ||
| EP0876580A1 (en) | A method and a device for inductive measurement of measures and positions of objects of electrically conductive material | |
| JP3097094B2 (en) | Non-contact displacement detector | |
| JPS61292014A (en) | position detector | |
| ATE415634T1 (en) | FERRARIS SENSOR | |
| JPS6134606B2 (en) | ||
| JPH0458881B2 (en) | ||
| RU2300737C1 (en) | Inductive optical transformer of electric cable eccentricity meter | |
| SU1516745A1 (en) | Galvanometric device for measuring displacements | |
| JPS61175504A (en) | Positioning sensor | |
| SU443247A1 (en) | Electric Inductive Motion Sensor | |
| JP4573417B2 (en) | Load sensor |