JPH0476422B2 - - Google Patents
Info
- Publication number
- JPH0476422B2 JPH0476422B2 JP8287085A JP8287085A JPH0476422B2 JP H0476422 B2 JPH0476422 B2 JP H0476422B2 JP 8287085 A JP8287085 A JP 8287085A JP 8287085 A JP8287085 A JP 8287085A JP H0476422 B2 JPH0476422 B2 JP H0476422B2
- Authority
- JP
- Japan
- Prior art keywords
- inductance
- alloy plate
- magnetic
- signal
- pressure
- 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
Links
- 238000001514 detection method Methods 0.000 claims description 15
- 229910001004 magnetic alloy Inorganic materials 0.000 claims description 11
- 230000010355 oscillation Effects 0.000 claims description 5
- 239000000696 magnetic material Substances 0.000 claims description 2
- 230000005347 demagnetization Effects 0.000 description 12
- 229910000808 amorphous metal alloy Inorganic materials 0.000 description 11
- 230000008859 change Effects 0.000 description 11
- 238000005259 measurement Methods 0.000 description 11
- 238000010586 diagram Methods 0.000 description 10
- 230000035699 permeability Effects 0.000 description 10
- 230000000694 effects Effects 0.000 description 8
- 230000007423 decrease Effects 0.000 description 7
- 230000005415 magnetization Effects 0.000 description 5
- 238000000034 method Methods 0.000 description 4
- 230000008569 process Effects 0.000 description 4
- 230000035945 sensitivity Effects 0.000 description 4
- 238000006243 chemical reaction Methods 0.000 description 2
- 230000005381 magnetic domain Effects 0.000 description 2
- 230000004308 accommodation Effects 0.000 description 1
- 230000009471 action Effects 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 244000145845 chattering Species 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 230000001965 increasing effect Effects 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 230000001603 reducing effect Effects 0.000 description 1
- 230000000087 stabilizing effect Effects 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING 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
- G01D5/00—Mechanical 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
- G01D5/12—Mechanical 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
- G01D5/243—Mechanical 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 the phase or frequency of AC
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Fluid Pressure (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、非晶質合金板を用いた力学量−イン
ダクタンス変換型のセンサ検出方法に関する。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a mechanical quantity-inductance conversion type sensor detection method using an amorphous alloy plate.
従来の技術
従来の検出方法を圧力センサを用いて説明す
る。第4図は非晶質磁性合金板を用いた圧力セン
サの断面図である。1は磁歪を有する非晶質合金
板、2は軟磁性フエライトからなるコア、3はコ
ア2の中に設けられたコイルで、コイル3に電流
を流すと非晶質合金板1とコア2で磁気回路Hを
構成する。全体はケース4に納められている。圧
力は導入部5と透孔6からなる圧力伝達手段7に
より非晶質合金板1の他面の一部に加えられる。
圧力の印加に伴い非晶質合金板1に歪が発生する
と磁歪効果により非晶質合金板1の磁性が変化
し、発振電源8とインダクタンス測定回路9から
なる検出部10によりその変化が検出され、圧力
がインダクタンスで検出される。Prior Art A conventional detection method will be explained using a pressure sensor. FIG. 4 is a sectional view of a pressure sensor using an amorphous magnetic alloy plate. 1 is an amorphous alloy plate with magnetostriction, 2 is a core made of soft magnetic ferrite, and 3 is a coil installed in the core 2. When a current is applied to the coil 3, the amorphous alloy plate 1 and core 2 A magnetic circuit H is configured. The whole thing is housed in Case 4. Pressure is applied to a part of the other surface of the amorphous alloy plate 1 by a pressure transmitting means 7 consisting of an introduction part 5 and a through hole 6.
When strain occurs in the amorphous alloy plate 1 due to the application of pressure, the magnetism of the amorphous alloy plate 1 changes due to the magnetostrictive effect, and the change is detected by the detection unit 10 consisting of the oscillation power supply 8 and the inductance measurement circuit 9. , pressure is sensed by inductance.
従来は、第5図に示す単一周波数の交流信号を
用いて検出していたが、その圧力−インダクタン
スの変化が小さく再現性も悪く、圧力に対してヒ
ステリシスが発生し、非晶質磁性合金板1のデイ
スアコモデーシヨン(以下D.Aと略す)により安
定性も悪い。 Conventionally, detection was performed using a single frequency alternating current signal as shown in Figure 5, but the change in pressure-inductance was small and the reproducibility was poor, hysteresis occurred with respect to pressure, and amorphous magnetic alloy Stability is also poor due to the day accommodation (hereinafter abbreviated as DA) on board 1.
第6図はこの第5図のような単一周波数の交流
信号を用いた第3図の圧力センサの圧力−インダ
クタンスの関係を示す図である。矢印は測定の順
序を示している。また、第7図は圧力一定の場合
のインダクタンスの経時変化の様子を示してい
る。 FIG. 6 is a diagram showing the pressure-inductance relationship of the pressure sensor of FIG. 3 using a single frequency alternating current signal as shown in FIG. Arrows indicate the order of measurements. Moreover, FIG. 7 shows how the inductance changes over time when the pressure is constant.
この変化は非晶質合金板1のDA及び消磁の不
充分さがインダクタンスの再現性を悪くしている
事を示している。そこでセンサ検出方法として消
磁を繰り返せば特性の改善が得られる。第8図は
通常の低周波での消磁波形を示しており、充分大
きな振幅より零振幅まで連続的に減少するもので
あり、測定のためには高周波、一定振幅の測定信
号に切り換える必要がある。しかしこの切換えに
はチヤタリングのない事が肝要であるがその実現
のためには検出部が高価格になつてしまう欠点が
あつた。 This change indicates that insufficient DA and demagnetization of the amorphous alloy plate 1 deteriorate the reproducibility of the inductance. Therefore, if demagnetization is repeated as a sensor detection method, the characteristics can be improved. Figure 8 shows a normal low-frequency demagnetization waveform, which continuously decreases from a sufficiently large amplitude to zero amplitude, and for measurement it is necessary to switch to a high-frequency, constant-amplitude measurement signal. . However, although it is essential for this switching to be free of chattering, there is a drawback in that the detection section becomes expensive in order to achieve this.
発明が解決しようとする問題点
非晶質合金板を用いたセンサのインダクタンス
を単一周波数の交流信号を用いて検出した場合、
その値はDAにより安定性が悪く、また再現性も
悪い。さらに単一周波数の交流信号だけでは非晶
質合金板の透磁率や応力に対し大きな変化を示さ
ず、コイルのインダクタンス変化が小さい。Problems to be Solved by the Invention When the inductance of a sensor using an amorphous alloy plate is detected using an AC signal of a single frequency,
The value has poor stability due to DA and poor reproducibility. Furthermore, an alternating current signal of a single frequency does not show a large change in the magnetic permeability or stress of the amorphous alloy plate, and the change in the inductance of the coil is small.
一方繰り返し消磁においても消磁電流と測定電
流との切換えを特性に影響を及ぼさないように行
なうことが難しかつた。 On the other hand, even in repeated demagnetization, it is difficult to switch between the demagnetizing current and the measurement current without affecting the characteristics.
問題点を解決するための手段
上記問題解決のために、本発明は、コイルのイ
ンダクタンス検出あたり、発振電源からの信号を
時間的に低周波から高周波まで連続的に変化さ
せ、低周波印加後に高周波が印加された時のイン
ダクタンスにより圧力を検出する。Means for Solving the Problems In order to solve the above problems, the present invention continuously changes the signal from the oscillation power supply temporally from low frequency to high frequency when detecting the inductance of the coil, and after applying the low frequency, the high frequency Pressure is detected by inductance when applied.
さらに、感度を向上させるため直流信号を重畳
した交流信号を用いる。 Furthermore, in order to improve sensitivity, an AC signal on which a DC signal is superimposed is used.
作 用
一定電圧を有する低周波から高周波まで変化す
る交流信号は、インダクタンスが一定の場合その
インピーダンスが周波数に比例して大きくなるた
め、電流の大きさが低周波時の大振幅から高周波
時の小振幅へと変化するように働く。すなわちこ
の交流信号は消磁作用を持つている。そのためこ
の交流信号を繰り返し用いる事により消磁直後の
安定したインダクタンスを検出する事が可能とな
る。Action For AC signals that have a constant voltage and vary from low frequency to high frequency, if the inductance is constant, the impedance increases in proportion to the frequency, so the magnitude of the current changes from large amplitude at low frequency to small amplitude at high frequency. It works to change the amplitude. In other words, this AC signal has a demagnetizing effect. Therefore, by repeatedly using this AC signal, it is possible to detect stable inductance immediately after demagnetization.
その理由は、消磁を行うと、非晶質合金板の磁
区構造がリセツトされる。すなわち磁区構造は初
期状態になる。そのためコイルのインダクタンス
は再現性が良くなり、ヒステリシスは少なくな
る。また消磁は、磁壁を大きく動かしてからリセ
ツトするので、消磁後は磁壁の環境が新しくな
り、DAが始まる最初の部分になるので短時間に
測定を行えば、DAそのものの影響から逃れるこ
とができる。そこでセンサ検出方法として消磁を
繰り返せば特性の改善が得られる。 The reason is that when demagnetization is performed, the magnetic domain structure of the amorphous alloy plate is reset. In other words, the magnetic domain structure is in its initial state. Therefore, the coil inductance has better repeatability and less hysteresis. Furthermore, since demagnetization moves the domain wall significantly and then resets it, the environment of the domain wall becomes new after demagnetization, and this is the first part where DA begins, so if the measurement is carried out in a short period of time, it is possible to escape from the influence of DA itself. . Therefore, if demagnetization is repeated as a sensor detection method, the characteristics can be improved.
消磁効果のみでもインダクタンスの安定性には
有効であるが、さらに直流信号を重畳すると、す
なわち直流磁界を重畳すると、非晶質磁性合金板
を用いたセンサの応力や歪に対する感度が大きく
なる。この様な効果が得られるのは次のような理
由によると考えられる。 Although the demagnetization effect alone is effective for stabilizing the inductance, when a DC signal is further superimposed, that is, when a DC magnetic field is superimposed, the sensitivity of a sensor using an amorphous magnetic alloy plate to stress and strain increases. The reason why such an effect is obtained is considered to be due to the following reasons.
歪が非晶質磁性合金板内に発生すると、その歪
が生じた部分で透磁率が減少する。その結果磁気
回路内では磁束が連続であるため、歪を生じた部
分で直流及び交流磁界が他の部分より大きくな
る。直流磁界が大きくなると、非晶質磁性合金板
の透磁率は通常の軟磁性体同様減少するので、始
めの歪だけによる透磁率の減少以上に透磁率の減
少が大きくなる。この変化は交流磁界に対する透
磁率の直流磁界依存性が大きいB−Hループの肩
に相当する部分で効果が大きい。このB−Hルー
プの肩に相当するように直流磁界を設定すれば磁
気抵抗は数倍に増大する。この部分がセンサ出力
が増大する直流磁界領域に相当すると考えられ
る。この直流磁界による透磁率減少効果、磁気抵
抗増大効果が大きいため、交流磁界成分振幅がや
や大きくなつても影響がほとんど無い。 When strain occurs within an amorphous magnetic alloy plate, magnetic permeability decreases in the portion where the strain occurs. As a result, since the magnetic flux is continuous within the magnetic circuit, the DC and AC magnetic fields are larger in the distorted part than in other parts. As the DC magnetic field increases, the magnetic permeability of the amorphous magnetic alloy plate decreases like a normal soft magnetic material, so the decrease in magnetic permeability becomes greater than the decrease in magnetic permeability due to initial strain alone. This change has a large effect in the portion corresponding to the shoulder of the B-H loop, where the dependence of magnetic permeability on the AC magnetic field on the DC magnetic field is large. If the DC magnetic field is set to correspond to the shoulder of this B-H loop, the magnetic resistance will increase several times. This portion is considered to correspond to the DC magnetic field region where the sensor output increases. Since the magnetic permeability reducing effect and magnetic resistance increasing effect due to this DC magnetic field are large, there is almost no effect even if the AC magnetic field component amplitude becomes slightly large.
一方磁気回路中歪を生じない部分では磁界が減
少し透磁率は大きくなり、磁気抵抗は減少する。
しかしこの部分の磁気抵抗は、歪の生じた部分の
磁気抵抗と直列に接続されるため、全体の磁気抵
抗変化は、歪を受けた部分の大きな磁気抵抗変化
が主なものとなる。よつてセンサの感度が直流磁
界印加により大きくなると考えられる。 On the other hand, in parts of the magnetic circuit where no distortion occurs, the magnetic field decreases, magnetic permeability increases, and magnetic resistance decreases.
However, since the magnetic resistance of this portion is connected in series with the magnetic resistance of the strained portion, the overall magnetic resistance change is mainly due to the large magnetic resistance change of the strained portion. Therefore, it is thought that the sensitivity of the sensor increases with the application of a DC magnetic field.
また直流磁界を重畳された交流磁界で測定を行
うと、回転磁化過程を用いた測定になる。磁壁移
動磁化過程では、磁壁が磁性体内の温度により変
化しやすいエネルギー障壁を越えて行くため温度
の影響をうけやすいが、回転磁化過程での透磁率
は温度による影響はすくない。これは磁化の回転
による磁化過程のため、透磁率が磁気モーメント
の温度特性だけで決まるからである。このような
理由から直流磁界を重畳された交流磁界で測定を
行うと、温度特性のよいセンサが構成できる。 Furthermore, when measurement is performed using an alternating current magnetic field superimposed with a direct current magnetic field, the measurement uses a rotational magnetization process. In the domain wall displacement magnetization process, the domain wall crosses an energy barrier that easily changes depending on the temperature inside the magnetic body, so it is easily affected by temperature, but in the rotational magnetization process, magnetic permeability is not affected by temperature much. This is because the magnetic permeability is determined only by the temperature characteristics of the magnetic moment due to the magnetization process due to rotation of magnetization. For these reasons, a sensor with good temperature characteristics can be constructed by performing measurements with an alternating current magnetic field superimposed on a direct current magnetic field.
実施例
第1図に本実施例における発振電源からの信号
を示す。Embodiment FIG. 1 shows signals from an oscillation power supply in this embodiment.
aは電圧波形を、bはコイルに発生する磁界波
形を示す。すなわち、信号を時間的に低周波から
高周波まで連続的に変化させ、低周波印加後に高
周波を印加した時にインダクタンスを測定して圧
力を検出する。 a indicates a voltage waveform, and b indicates a magnetic field waveform generated in the coil. That is, the signal is temporally changed continuously from a low frequency to a high frequency, and when a high frequency is applied after the low frequency is applied, the inductance is measured and the pressure is detected.
コイルのインダクタンスをLとすると、そのイ
ンピーダンスZは周波数を用いて
Z=2π・L ……(1)
で求められる。そこで電流に比例するコイルに発
生する磁界Hは
H∝i∝V/2π・L
(ここでVは電圧振幅)
で表わされる。そのためaの如き一定電圧の低周
波から高周波に連続的に変化する信号を用いれば
b図に示すように消磁波形が実現できる。 If the inductance of the coil is L, its impedance Z can be found using the frequency as follows: Z=2π・L (1). Therefore, the magnetic field H generated in the coil, which is proportional to the current, is expressed as H∝i∝V/2π·L (where V is the voltage amplitude). Therefore, by using a signal such as a that changes continuously from a low frequency to a high frequency with a constant voltage, a demagnetizing waveform as shown in figure b can be realized.
すなわち第1図の信号を印加することにより再
現性のよいDAの影響の少ないセンサが得られ
る。 That is, by applying the signal shown in FIG. 1, a sensor with good reproducibility and less influence of DA can be obtained.
第2図は、第4図の圧力センサに直流磁界を重
畳した場合のインダクタンスが、直流磁界Hdcの
大きさによりどのように変化するかを0気圧、30
気圧において示したものである。測定温度は50
℃、周波数は20KHzである。これから交流磁界の
みで測定するよりも、直流磁界を重畳した場合に
もり出力が増大する事が判る。 Figure 2 shows how the inductance when a DC magnetic field is superimposed on the pressure sensor shown in Figure 4 changes depending on the magnitude of the DC magnetic field Hdc at 0 atmospheres and 30
It is shown in atmospheric pressure. The measurement temperature is 50
℃, the frequency is 20KHz. It can be seen from this that the output increases when a DC magnetic field is superimposed, rather than when measuring only with an AC magnetic field.
第3図aは、第1図aの信号より直流電圧を重
畳した他の実施例の信号を示している。同図bは
aの信号を用いた場合第4図の圧力センサの圧力
とインダクタンスの関係を示している。直流磁界
を印加している事と消磁の繰り返しにより、再現
性、感度、安定性において従来例に対し著しく改
善が行なわれた事が判る。 FIG. 3a shows a signal of another embodiment in which a DC voltage is superimposed on the signal of FIG. 1a. FIG. 4b shows the relationship between the pressure and inductance of the pressure sensor of FIG. 4 when the signal of a is used. It can be seen that by applying a DC magnetic field and repeating demagnetization, the reproducibility, sensitivity, and stability were significantly improved over the conventional example.
発明の効果
以上述べたように本発明による検出方法を用い
れば、非晶質磁性合金板の磁歪を用いた力学量−
インダクタンス変換型のセンサにおいて、出力の
再現性、安定性のよい、経時変化が少なく、出力
の大きいものが得られ、その効果は極めて大き
い。Effects of the Invention As described above, if the detection method according to the present invention is used, the mechanical quantity using magnetostriction of an amorphous magnetic alloy plate -
In the inductance conversion type sensor, a sensor with good output reproducibility and stability, little change over time, and a large output can be obtained, and its effects are extremely large.
第1図aは本発明の一実施例の検出方法の信号
波形を示す図、第1図bは同じく磁界波形を示す
図、第2図は0気圧、30気圧印加した時の圧力セ
ンサのインダクタンスの直流磁界依存性を示す
図、第3図aは他の実施例の信号波形を示す図、
第3図bはそれを用いた圧力とインダクタンスの
関係を示す図、第4図は非晶質合金板を用いた圧
力センサの断面図、第5図は従来の信号波形を示
す図、第6図は従来の検出方法による圧力とイン
ダクタンスの関係を示す図、第7図は従来の検出
方法におけるインダクタンスの経時変化を示す
図、第8図は従来の消磁波形を示す図である。
1……非晶質磁性合金板、2……コア、3……
コイル、7……圧力伝達手段、8……発振電源、
9……インダクタンス測定回路、10……検出
部。
Figure 1a is a diagram showing the signal waveform of the detection method according to an embodiment of the present invention, Figure 1b is a diagram showing the magnetic field waveform, and Figure 2 is the inductance of the pressure sensor when 0 atm and 30 atm are applied. FIG. 3a is a diagram showing the signal waveform of another embodiment,
Fig. 3b is a diagram showing the relationship between pressure and inductance using the same, Fig. 4 is a cross-sectional view of a pressure sensor using an amorphous alloy plate, Fig. 5 is a diagram showing a conventional signal waveform, and Fig. 6 is a diagram showing the relationship between pressure and inductance. FIG. 7 is a diagram showing the relationship between pressure and inductance according to the conventional detection method, FIG. 7 is a diagram showing the change in inductance over time according to the conventional detection method, and FIG. 8 is a diagram showing the conventional demagnetization waveform. 1...Amorphous magnetic alloy plate, 2...Core, 3...
Coil, 7...pressure transmission means, 8...oscillation power supply,
9...Inductance measurement circuit, 10...Detection section.
Claims (1)
性材からなるコアを設け、そのコア中にコイルを
設け、上記非晶質磁性合金板とコアで磁気回路を
構成し、上記非晶質磁性合金板の他面の一部に圧
力伝達手段を設け、上記コイルに発振電源とイン
ダクタンス測定回路からなる検出部を設け、上記
圧力電圧手段より非晶質磁性合金板の一部に発生
する歪をコイルのインダクタンスで検出するセン
サにおいて、発振電源からの信号を時間的に低周
波から高周波まで連続的に変化させ、低周波印加
後に高周波が印加された時のインダクタンスによ
り圧力を検出することを特徴とするセンサ検出方
法。 2 交流信号に直流信号が重畳されていることを
特徴とする特許請求の範囲第1項記載のセンサ検
出方法。[Claims] 1. A core made of a soft magnetic material is provided on one surface of an amorphous magnetic alloy plate having magnetostriction, a coil is provided in the core, and a magnetic circuit is configured by the amorphous magnetic alloy plate and the core. A pressure transmitting means is provided on a part of the other surface of the amorphous magnetic alloy plate, a detection section consisting of an oscillation power source and an inductance measuring circuit is provided on the coil, and the amorphous magnetic alloy plate is detected by the pressure voltage means. In a sensor that detects the strain that occurs in a part using the inductance of a coil, the signal from the oscillating power source is changed continuously from low frequency to high frequency over time, and when a high frequency is applied after a low frequency is applied, the inductance causes pressure to be applied. A sensor detection method characterized by detecting. 2. The sensor detection method according to claim 1, wherein a DC signal is superimposed on an AC signal.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60082870A JPS61240132A (en) | 1985-04-18 | 1985-04-18 | Sensor detection method |
| US06/853,717 US4812758A (en) | 1985-04-18 | 1986-04-18 | Method of operating an amorphous-magnetic-alloy sensor |
| EP86105368A EP0204928B1 (en) | 1985-04-18 | 1986-04-18 | Exciting of magnetic field for amorphous-alloy sensor |
| DE8686105368T DE3680387D1 (en) | 1985-04-18 | 1986-04-18 | MAGNETIC FIELD CONTROL FOR AMORPHOUS ALLOY SENSOR. |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60082870A JPS61240132A (en) | 1985-04-18 | 1985-04-18 | Sensor detection method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61240132A JPS61240132A (en) | 1986-10-25 |
| JPH0476422B2 true JPH0476422B2 (en) | 1992-12-03 |
Family
ID=13786335
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60082870A Granted JPS61240132A (en) | 1985-04-18 | 1985-04-18 | Sensor detection method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS61240132A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2001018514A1 (en) * | 1999-09-02 | 2001-03-15 | Sanyo Electric Co., Ltd. | Load cell and washing machine with load cell |
| US7913569B2 (en) | 2007-12-11 | 2011-03-29 | Israel Aerospace Industries Ltd. | Magnetostrictive type strain sensing means and methods |
| JP5642438B2 (en) * | 2010-07-02 | 2014-12-17 | 日置電機株式会社 | Capacitance measuring apparatus and capacitance measuring method |
| CN103454024B (en) * | 2013-05-24 | 2016-01-13 | 招商局重庆交通科研设计院有限公司 | Based on the concrete-bridge tendon tension measuring method of converse magnetostriction |
-
1985
- 1985-04-18 JP JP60082870A patent/JPS61240132A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61240132A (en) | 1986-10-25 |
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| EXPY | Cancellation because of completion of term |