JPH11118629A - Magnetostrictive strain sensor - Google Patents

Magnetostrictive strain sensor

Info

Publication number
JPH11118629A
JPH11118629A JP29356497A JP29356497A JPH11118629A JP H11118629 A JPH11118629 A JP H11118629A JP 29356497 A JP29356497 A JP 29356497A JP 29356497 A JP29356497 A JP 29356497A JP H11118629 A JPH11118629 A JP H11118629A
Authority
JP
Japan
Prior art keywords
magnetic film
strain sensor
change
magnetic
film
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.)
Abandoned
Application number
JP29356497A
Other languages
Japanese (ja)
Inventor
Mitsuaki Ikeda
満昭 池田
Koji Kamimura
浩司 上村
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.)
Yaskawa Electric Corp
Original Assignee
Yaskawa Electric Corp
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 Yaskawa Electric Corp filed Critical Yaskawa Electric Corp
Priority to JP29356497A priority Critical patent/JPH11118629A/en
Publication of JPH11118629A publication Critical patent/JPH11118629A/en
Abandoned legal-status Critical Current

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Abstract

(57)【要約】 【課題】 使用環境の温度変化が大きいとセンサ特性が
経時変化を起こさないようにする。 【解決手段】軸1の所定位置外周表面に逆磁歪効果を有
する磁性膜2を形成し、磁性膜2に近接させて励磁コイ
ル3および検出コイル4とを配置し、軸1に伝わる歪み
により軸表面に発生する歪を磁性膜2の透磁率変化に対
応して変わるコイルのインピーダンス変化を測定して歪
を検出する磁歪式歪センサにおいて、磁性膜2の真応力
が+3kgf/mm2 〜−3kgf/mm2 の値に調整
されている磁性膜2を使用するようにした。したがっ
て、経時変化を生じない逆磁歪効果を有する磁性膜を得
ることができる。
(57) [Summary] [PROBLEMS] To prevent a sensor characteristic from changing with time when a temperature change of a use environment is large. A magnetic film having an inverse magnetostriction effect is formed on an outer peripheral surface of a predetermined position of a shaft, and an exciting coil and a detection coil are arranged close to the magnetic film. In a magnetostrictive strain sensor that detects a distortion by measuring a change in impedance of a coil that changes a strain generated on the surface in accordance with a change in the magnetic permeability of the magnetic film 2, the true stress of the magnetic film 2 is +3 kgf / mm 2 to −3 kgf. The magnetic film 2 adjusted to a value of / mm 2 was used. Therefore, it is possible to obtain a magnetic film having the reverse magnetostriction effect that does not change with time.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は磁性体の逆磁歪効果
を利用した磁歪式歪センサ、例えば、モータのトルク、
液体の圧力や電線の張力を測定するための磁歪式歪セン
サに関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetostrictive strain sensor utilizing a reverse magnetostriction effect of a magnetic material, for example, a motor torque,
The present invention relates to a magnetostrictive strain sensor for measuring pressure of a liquid or tension of an electric wire.

【0002】[0002]

【従来の技術】回転駆動系を有するロボットやマニプレ
ータおよび工作機械などの制御に非接触小型トルクセン
サが要求されている。このようなトルクセンサとしては
本発明の構成の図1と同じように構成している。回転軸
1としてはマルエージング鋼やステンレス鋼などが使用
される。回転軸1がSUS304ステンレス鋼のように
非磁性材料の場合はその表面に磁性膜2(Ni−Feパ
ーマロイ膜)などがスパッタ法などで形成される。マル
エージング鋼の場合も高感度センサを構成する場合はそ
の表面にパーマロイ膜などが形成されて使用される。回
転軸1にトルクが印加されると回転軸1の表面に形成さ
れている磁性膜2に歪が加わり磁気特性が変化する。こ
の磁気特性の変化を回転軸1の周囲に巻いている励磁コ
イル3によりインピーダンス変化として検出コイル4で
検出し、トルクに換算する。前記軸1に形成する磁性膜
2については種々の磁性材料があげられるが、保持力が
低くて、膜の強度が大きく磁歪定数の大きい組成からな
るパーマロイが望ましい。具体的には50%〜75%N
i−Feパーマロイもしくは85%〜95%パーマロイ
である。また、その製造法としては組成や膜厚の再現性
が良いスパッタ法が好ましい。送電線や電車線の張力を
測定する試みが進められている。例えば、送電線に雪が
つもり、その重さが増すと電線が荷重に耐えきらなくな
り、断線にいたる。従って、電線の張力を監視して、事
故を未然に防ぐ試みが進められている。張力センサの構
成例を図2に示す。非磁性ステンレスよりなる軸1の外
周にNi−Fe合金膜5が形成されている。張力変化に
基づく合成膜5の変化を励磁コイル3によるインピーダ
ンス変化を検出コイル4で磁気特性の変化としてとら
え、張力に換算する。
2. Description of the Related Art Non-contact small torque sensors are required for controlling robots, manipulators, and machine tools having a rotary drive system. Such a torque sensor has the same configuration as that of FIG. 1 of the configuration of the present invention. As the rotating shaft 1, maraging steel, stainless steel, or the like is used. When the rotating shaft 1 is made of a non-magnetic material such as SUS304 stainless steel, a magnetic film 2 (Ni-Fe permalloy film) or the like is formed on its surface by a sputtering method or the like. When a maraging steel is used to form a high-sensitivity sensor, a permalloy film or the like is formed on the surface thereof before use. When a torque is applied to the rotating shaft 1, strain is applied to the magnetic film 2 formed on the surface of the rotating shaft 1, and the magnetic characteristics change. The change in the magnetic characteristics is detected by the detection coil 4 as an impedance change by the exciting coil 3 wound around the rotating shaft 1 and converted into torque. Various magnetic materials can be used for the magnetic film 2 formed on the shaft 1. Permalloy having a composition having a low coercive force, a large film strength and a large magnetostriction constant is desirable. Specifically, 50% to 75% N
i-Fe permalloy or 85% to 95% permalloy. Further, as the manufacturing method, a sputtering method having good reproducibility of the composition and the film thickness is preferable. Attempts are being made to measure the tension of transmission lines and train lines. For example, when a power transmission line is supposed to be snowy and the weight increases, the power line cannot withstand the load, leading to disconnection. Therefore, attempts have been made to monitor the tension of the electric wires to prevent an accident. FIG. 2 shows a configuration example of the tension sensor. A Ni-Fe alloy film 5 is formed on the outer periphery of a shaft 1 made of non-magnetic stainless steel. The change in the synthetic film 5 based on the change in the tension is regarded as a change in the magnetic characteristics by the detection coil 4 by the impedance change due to the exciting coil 3 and is converted into a tension.

【0003】[0003]

【発明が解決しようとする課題】ところが、スパッタ法
により作製したパーマロイ膜を歪センサとして使用した
場合、使用環境の温度変化が大きいとセンサ特性が経時
変化を起こすことが分かった。歪センサを温度変化が激
しい環境で使用すると、磁性膜2と軸1との熱膨張係数
差により磁性膜2に歪がかかる。磁性膜2に真応力が残
留していると磁性膜2にかかる応力によりこの真応力が
変化する。真応力とはスパッタ法などの真空技術を利用
した膜形成法で作製した磁性膜2に特に現れるもので、
スパッタ膜形成時に膜内に取り込まれるガス、磁性膜2
の結晶のわずかな乱れなどに起因する。従って、長期的
にみた場合、繰り返し熱応力などの外部要因により微妙
に変化を起こすものである。この真応力を小さくすれば
歪センサの経時変化は小さくなる。そこで、本発明は、
経時変化を生じない逆磁歪効果を有する磁性膜からなる
歪センサを得ることを目的するものである。
However, it has been found that when a permalloy film produced by a sputtering method is used as a strain sensor, if the temperature of the operating environment changes greatly, the sensor characteristics change over time. When the strain sensor is used in an environment where the temperature changes drastically, the magnetic film 2 is distorted due to a difference in thermal expansion coefficient between the magnetic film 2 and the shaft 1. If the true stress remains in the magnetic film 2, the true stress changes due to the stress applied to the magnetic film 2. True stress is particularly apparent in the magnetic film 2 produced by a film forming method using a vacuum technique such as a sputtering method.
Gas taken in the film when forming a sputtered film, magnetic film 2
Due to slight disturbance of the crystal of the crystal. Therefore, over a long period of time, a slight change is caused by external factors such as repeated thermal stress. If this true stress is reduced, the change over time of the strain sensor is reduced. Therefore, the present invention
It is an object of the present invention to obtain a strain sensor made of a magnetic film having a reverse magnetostriction effect that does not change with time.

【0004】[0004]

【課題を解決するための手段】上記問題点を解決するた
め、本発明は、軸の所定位置外周表面に逆磁歪効果を有
する磁性膜を形成し、前記磁性膜に近接させて励磁コイ
ルおよび検出コイルを配置し、前記軸に伝わる歪みによ
り軸表面に発生する歪を前記磁性膜の透磁率変化に対応
して変わる前記コイルのインピーダンス変化を測定して
歪を検出する磁歪式歪センサにおいて、前記磁性膜の真
応力が+3kgf/mm2 〜−3kgf/mm2 の値に
調整されている磁性膜を使用している。
SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, the present invention forms a magnetic film having an inverse magnetostrictive effect on an outer peripheral surface of a predetermined position of a shaft, and brings an exciting coil and a detection coil close to the magnetic film. A magnetostrictive strain sensor for arranging a coil and measuring a change in impedance of the coil, which changes a strain generated on a shaft surface by a strain transmitted to the shaft in accordance with a change in magnetic permeability of the magnetic film, and detects the strain, A magnetic film whose true stress is adjusted to a value of +3 kgf / mm 2 to −3 kgf / mm 2 is used.

【0005】[0005]

【発明の実施の形態】以下、本発明の実施例を図に基づ
いて説明する。図1は磁歪式トルクセンサの構成図であ
る。図2は磁歪式張力センサの構成図である。図におい
て、1は直径30mmのシャフトで、材料はTiもしく
はSUS304ステンレスシャフトからなる軸を洗浄し
た後、スパッタ法でその表面に厚さ5μmの55%Ni
−Fe膜をTiシャフト上に、90%Ni−Fe膜をS
US304シャフト上に被覆した。膜形成時の軸の温度
は400°Cとした。一方、Ti合金シャフトと同じ熱
膨張係数を有するソーダライムガラス(5×10mm、
厚さ1mm)、SUS304シャフトと同じ熱膨張係数
を有するSUS304薄板(5×10mm、厚さ1m
m)上も同じ厚さの磁性膜2あるいは合成膜5を形成し
た。この試料を500°Cで種々の時間条件で熱処理し
たのち、曲がり測定法(例えば小林、細川:薄膜技術入
門、p149、総合電子出版社)で膜に残っている真応
力を測定した。次に、この曲がり測定法を参考にして両
材質のシャフト試料に付いて、種々の真応力が残る条件
で熱処理を行った試料を作製した。引き続き、この試料
を−15〜+50°Cのヒートサイクルを加えたヒート
サイクル回数50回後の張力と出力の関係を測定し出力
変化率を調べた。特性測定は試料の磁性膜2あるいは合
成膜5の周辺に200ターンの励磁コイル3と400タ
ーンの検出コイル4を配置し行った。下表の結果で分か
るように真応力が小さいと経時変化が少ないことが分か
る。真応力が+3kgf/mm2 〜−3kgf/mm2
の値の範囲を越えると、経時変化が大きくなることが分
かった。実施例では真応力除去に熱処理を使用したが、
超音波の印加により除去する方法やスパッタ時に同時熱
処理する方法などがある。また、実施例では磁性膜2あ
るいは合成膜5としてパーマロイだけしか取り上げなか
ったが、他の磁性膜2あるいは合成膜5でも真応力が起
因しているので同じ結果になることは明らかである。さ
らに、出力の検出は磁気ヘッドで検出してもよい。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 is a configuration diagram of a magnetostrictive torque sensor. FIG. 2 is a configuration diagram of the magnetostrictive tension sensor. In the figure, reference numeral 1 denotes a shaft having a diameter of 30 mm. The shaft is made of Ti or SUS304 stainless steel.
-Fe film on Ti shaft, 90% Ni-Fe film on S shaft
Coated on US304 shaft. The axis temperature during film formation was 400 ° C. On the other hand, soda-lime glass (5 × 10 mm,
SUS304 thin plate (5 mm thick, 1 m thick) having the same coefficient of thermal expansion as SUS304 shaft
m) The magnetic film 2 or the synthetic film 5 having the same thickness was formed on the upper surface. After heat-treating this sample at 500 ° C. for various time conditions, the true stress remaining in the film was measured by a bending measurement method (for example, Kobayashi and Hosokawa: Introduction to Thin Film Technology, p149, Sogo Denshi Publishing Co., Ltd.). Next, with reference to this bending measurement method, a sample was prepared by performing a heat treatment on the shaft samples of both materials under the condition that various true stresses remain. Subsequently, the relationship between the tension and the output was measured 50 times after the sample was subjected to a heat cycle of −15 to + 50 ° C. and the output change rate was examined. The characteristics were measured by placing a 200-turn excitation coil 3 and a 400-turn detection coil 4 around the magnetic film 2 or the synthetic film 5 of the sample. As can be seen from the results in the following table, when the true stress is small, the change with time is small. True stress is +3 kgf / mm 2 to -3 kgf / mm 2
It has been found that when the value exceeds the range, the change with time increases. In the example, the heat treatment was used for removing the true stress.
There are a method of removing by applying ultrasonic waves and a method of performing simultaneous heat treatment during sputtering. Although only Permalloy is taken up as the magnetic film 2 or the composite film 5 in the embodiment, it is apparent that the same result is obtained in other magnetic films 2 or the composite film 5 because the true stress is caused. Further, the output may be detected by a magnetic head.

【0006】[0006]

【表1】 [Table 1]

【0007】[0007]

【発明の効果】以上述べたように本発明による磁歪式歪
センサは長時間使用しても経時変化を生じないので、信
頼性の高い歪センサを構成できる。トルク、張力等の測
定が必要な機器の高度化に寄与できる。
As described above, since the magnetostrictive strain sensor according to the present invention does not change with time even when used for a long time, a highly reliable strain sensor can be constructed. This can contribute to the advancement of equipment that requires measurement of torque, tension, and the like.

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

【図1】 本発明の磁歪式トルクセンサの構成図であ
る。
FIG. 1 is a configuration diagram of a magnetostrictive torque sensor of the present invention.

【図2】 本発明の磁歪式張力センサの構成図である。FIG. 2 is a configuration diagram of a magnetostrictive tension sensor of the present invention.

【符号の説明】[Explanation of symbols]

1 軸、 2 磁性膜、 3 励磁コイル、 4 検出
コイル、5 合成膜
1 axis, 2 magnetic film, 3 excitation coil, 4 detection coil, 5 synthetic film

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 軸の外周表面に逆磁歪効果を有する磁性
膜を形成し、前記磁性膜に近接させて励磁コイルおよび
検出コイルを配置し、前記軸に生じる歪みにより軸表面
に発生する歪を前記磁性膜の透磁率変化に対応して変わ
る前記コイルのインピーダンス変化を測定して歪を検出
する磁歪式歪センサにおいて、 前記磁性膜の真応力が+3kgf/mm2 〜−3kgf
/mm2 の値に調整されていることを特徴とする磁歪式
歪センサ。
A magnetic film having an inverse magnetostriction effect is formed on an outer peripheral surface of a shaft, and an exciting coil and a detection coil are arranged close to the magnetic film. In a magnetostrictive strain sensor for detecting distortion by measuring an impedance change of the coil corresponding to a change in magnetic permeability of the magnetic film, a true stress of the magnetic film is +3 kgf / mm 2 to −3 kgf.
The magnetostrictive strain sensor is adjusted to a value of / mm 2 .
【請求項2】 前記軸がSUS304ステンレスである
ことを特徴とする請求項1記載の磁歪式歪センサ。
2. The magnetostrictive strain sensor according to claim 1, wherein said shaft is made of SUS304 stainless steel.
【請求項3】 前記磁性膜がパーマロイであることを特
徴とする請求項1または2記載の磁歪式歪センサ。
3. The magnetostrictive strain sensor according to claim 1, wherein said magnetic film is made of permalloy.
【請求項4】 前記インピーダンス変化の検出を磁気ヘ
ッドで行うようにしたことを特徴とする請求項1乃至3
記載の磁歪式歪センサ。
4. The apparatus according to claim 1, wherein the detection of the impedance change is performed by a magnetic head.
A magnetostrictive strain sensor according to claim 1.
【請求項5】 前記インピーダンス変化の検出を前記磁
性膜の外周に同心円に配置した励磁コイルおよび検出コ
イルで行うようにしたことを特徴とする請求項1乃至4
記載の磁歪式歪センサ。
5. The apparatus according to claim 1, wherein the detection of the impedance change is performed by an excitation coil and a detection coil arranged concentrically around the outer periphery of the magnetic film.
A magnetostrictive strain sensor according to claim 1.
JP29356497A 1997-10-09 1997-10-09 Magnetostrictive strain sensor Abandoned JPH11118629A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29356497A JPH11118629A (en) 1997-10-09 1997-10-09 Magnetostrictive strain sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29356497A JPH11118629A (en) 1997-10-09 1997-10-09 Magnetostrictive strain sensor

Publications (1)

Publication Number Publication Date
JPH11118629A true JPH11118629A (en) 1999-04-30

Family

ID=17796388

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29356497A Abandoned JPH11118629A (en) 1997-10-09 1997-10-09 Magnetostrictive strain sensor

Country Status (1)

Country Link
JP (1) JPH11118629A (en)

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