JPH083421B2 - Inclination detector - Google Patents
Inclination detectorInfo
- Publication number
- JPH083421B2 JPH083421B2 JP61272879A JP27287986A JPH083421B2 JP H083421 B2 JPH083421 B2 JP H083421B2 JP 61272879 A JP61272879 A JP 61272879A JP 27287986 A JP27287986 A JP 27287986A JP H083421 B2 JPH083421 B2 JP H083421B2
- Authority
- JP
- Japan
- Prior art keywords
- core
- housing
- coil
- guide groove
- tilt angle
- 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 - Fee Related
Links
- 238000006073 displacement reaction Methods 0.000 claims description 16
- 238000001514 detection method Methods 0.000 claims description 12
- 239000011553 magnetic fluid Substances 0.000 claims description 11
- 238000010586 diagram Methods 0.000 description 5
- 230000005484 gravity Effects 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 239000000725 suspension Substances 0.000 description 3
- 238000006243 chemical reaction Methods 0.000 description 2
- 238000010276 construction Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01C—MEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
- G01C9/00—Measuring inclination, e.g. by clinometers, by levels
- G01C9/02—Details
- G01C9/06—Electric or photoelectric indication or reading means
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は、水平または重力の方向に対する被測定物、
特に揺動体の変化する傾斜角を電気的に検出する傾斜角
検出器に関する。DETAILED DESCRIPTION OF THE INVENTION (Industrial field of application) The present invention relates to an object to be measured in a horizontal or gravity direction,
In particular, the present invention relates to a tilt angle detector that electrically detects a changing tilt angle of an oscillator.
(従来技術) 従来、振子が重力の作用によって常に鉛直方向を指向
することを利用して、振子の支持部の傾きを検出する傾
斜角検出器が実用化されている。これは、振子の位置が
支持部の傾きに応じて相対的に変化するので、基準時の
振子の位置に対する傾斜時の位置の変化を直接的又は間
接的に電気的に検出することによって傾斜角を求めよう
とするものである(実開昭57−94813号、実開昭58−177
811号)。このような従来の振子構造の検出器では、振
子の吊り線部の加工、組立等には非常に微妙な熟練を要
し高度な精密技術を必要とする。その結果高価なものと
なっている。また、温度変化や衝撃等に起因する吊り線
部の変形による基準時の位置の変動等も大きく、傾斜角
検出において誤差を持つことが免れ得なかった。(Prior Art) Conventionally, an inclination angle detector that detects the inclination of the support portion of the pendulum has been put into practical use by utilizing that the pendulum always directs in the vertical direction by the action of gravity. This is because the position of the pendulum relatively changes according to the tilt of the support portion, and therefore the tilt angle is detected by directly or indirectly electrically detecting the change in the tilt position with respect to the reference pendulum position. (Actual No. 57-94813, No. 58-177).
No. 811). Such a conventional pendulum structure detector requires a very delicate skill in processing and assembling the suspension wire portion of the pendulum and requires a high precision technique. As a result, it is expensive. In addition, the fluctuation of the position at the time of reference due to the deformation of the suspension wire portion due to the temperature change, the impact, etc. is large, and it is unavoidable that there is an error in the inclination angle detection.
(発明が解決しようとする問題点) 本発明は、上記のような従来の傾斜角検出器にみられ
る高度な加工、組立技術を必要とせず、温度変化や衝撃
等に対する傾斜角検出誤差をなくすためになされたもの
で、従来の吊り線構造の傾斜角検出器とは全く構造を異
にした安価で精度の高い傾斜角検出器を提供することを
目的としている。(Problems to be Solved by the Invention) The present invention eliminates the inclination angle detection error with respect to temperature change, impact, etc., without requiring the advanced processing and assembly techniques found in the conventional inclination angle detectors described above. The purpose of the present invention is to provide an inexpensive and highly accurate inclination angle detector having a completely different structure from the inclination angle detector of the conventional suspension wire structure.
(問題点を解決するための手段) 本発明の傾斜角検出器は、1実施例を示す第1図にお
いて、筐体1内に磁性流体3を介して磁石よりなるコア
2を支持する。筐体1のコア支持面にコア2をガイドす
る凹状に湾曲した案内溝内6を形成し、筐体1のまわり
にコイル4を巻回する。そして、コイル4にコイルのイ
ンダクタンスの変化を検出する検出回路5Aを接続する。(Means for Solving Problems) In the inclination angle detector of the present invention, in FIG. 1 showing an embodiment, a core 2 made of a magnet is supported in a housing 1 via a magnetic fluid 3. A concave guide groove 6 for guiding the core 2 is formed on the core supporting surface of the housing 1, and the coil 4 is wound around the housing 1. Then, the coil 4 is connected to a detection circuit 5A that detects a change in the inductance of the coil.
(作用) 磁性流体3はコア2の磁極の周囲に集合するため、コ
ア2は筐体1の案内溝面6より浮上し、筐体1が傾斜す
ると重力により湾曲した溝面6の最も低い位置へ自由に
移動する。第3図に示すように、筐体1が水平からθ傾
くと、コア2と磁性流体3は最も低い位置へ移動して基
準位置10から変位し、この変位11に相当する出力がコイ
ル4より得られる。この変位11をdとし、湾曲した案内
溝面6の曲率半径をRとすると、d=θRが成り立ち、
一方コイル4のインダクタンスLは変位dに対して直線
的に変化するので、コイル4のインダクタンスLの変化
量を検出回路5Aによって検出することにより、筐体1の
傾斜角θを検出することができる。(Operation) Since the magnetic fluid 3 gathers around the magnetic poles of the core 2, the core 2 floats above the guide groove surface 6 of the housing 1, and when the housing 1 tilts, the lowest position of the groove surface 6 curved by gravity. Move freely to. As shown in FIG. 3, when the housing 1 tilts from the horizontal by θ, the core 2 and the magnetic fluid 3 move to the lowest position and are displaced from the reference position 10, and the output corresponding to this displacement 11 is output from the coil 4. can get. If this displacement 11 is d and the radius of curvature of the curved guide groove surface 6 is R, then d = θR holds,
On the other hand, since the inductance L of the coil 4 changes linearly with respect to the displacement d, the inclination angle θ of the housing 1 can be detected by detecting the change amount of the inductance L of the coil 4 by the detection circuit 5A. .
(実施例) 第1図は本発明の1実施例による傾斜角検出器の構成
を示すもので、この傾斜角検出器は、例えば棒状の磁石
よりなるコア2と、コア2の磁極周囲に吸引保持されコ
ア2を浮上させてこれが自由に移動できるようにするた
めの磁性流体3と、コア2と磁性流体3を収容する高抵
抗体又は絶縁体でかつ非磁性の材質からなる容器(筐
体)1と、容器1のまわりに配置されコア2の基準位置
10(第3図)からの変位11(第3図)を検出するための
同一の巻数、大きさの相互に間隔を置いて配置された2
個のコイル4と、コイル4に接続され各コイル4の端子
電圧を測定して容器1の傾斜角に相当する電気信号を出
力する検出回路5Aとを備えている。そして、第1図の実
施例においては、2個のコイル4は交流の定電流源Sに
直列に接続されている。(Embodiment) FIG. 1 shows the structure of an inclination angle detector according to an embodiment of the present invention. This inclination angle detector is composed of, for example, a core 2 made of a bar-shaped magnet and a magnetic pole around the core 2. A magnetic fluid 3 for holding and floating the core 2 so that it can move freely, and a container (housing) made of a non-magnetic material that is a high resistance or an insulator for housing the core 2 and the magnetic fluid 3. ) 1 and the reference position of the core 2 arranged around the container 1
2 spaced apart from each other with the same number of turns and size to detect displacement 11 (Fig. 3) from 10 (Fig. 3)
Each coil 4 and a detection circuit 5A connected to the coil 4 for measuring the terminal voltage of each coil 4 and outputting an electric signal corresponding to the inclination angle of the container 1 are provided. Further, in the embodiment shown in FIG. 1, the two coils 4 are connected in series to an alternating constant current source S.
ところで、容器(筐体)1の外形は例えば円筒形状
で、その内部のコア2の載置面には半円形状断面(第2
図(a))の案内溝6が筐体長手方向に形成されてお
り、この案内溝6は第1図に示すように鉛直方向上方に
凹となるように湾曲形状(曲率半径R)となっている。
容器1に形成する溝6は第2図(b)に示すようにV字
型断面としてもよく、その他磁性流体3の摺動ガイドと
して機能できる形状のものであれば、円、V字型以外
に、例えば台形型、楕円型等のいかなる断面形状のもの
でもよい。By the way, the outer shape of the container (housing) 1 is, for example, a cylindrical shape, and the mounting surface of the core 2 inside thereof has a semicircular cross section (second
A guide groove 6 of FIG. (A) is formed in the longitudinal direction of the housing, and the guide groove 6 has a curved shape (curvature radius R) so as to be concave upward in the vertical direction as shown in FIG. ing.
The groove 6 formed in the container 1 may have a V-shaped cross section as shown in FIG. 2 (b), and if it has a shape that can function as a sliding guide for the magnetic fluid 3, other than a circle or a V-shape. In addition, any cross-sectional shape such as a trapezoidal shape or an elliptical shape may be used.
このように配置すると、磁性流体3はコア2の磁極の
周囲に集合するため、コア2は容器1の溝面より浮上
し、容器1が傾斜すると重力により最も低い位置へ自由
に移動することができる。そして、コア2が2つのコイ
ル4の中央に位置する場合を基準位置10(第3図)と
し、容器1が第3図に示すように水平方向から角度θ傾
くと、コア2と磁性流体3は最も低い位置へ滑って基準
位置10から変位11だけ移動する。この変位11をdとし、
湾曲溝面6の曲率半径をRとすると、d=θRの関係が
成り立つので、変位11は傾斜角θに比例する。ところ
で、コア2の変位11をdで表わした時、各コイル4のイ
ンダクタンスLは第8図に示したように直線的に変化す
る(L∝d)。第8図の実線は一方のコイル4のインダ
クタンスの変化を示し、点線は他方のコイルのインダク
タンスの変化を示す。インダクタンスはコアがコイルの
中に入る時に上昇し、逆にコイルから出る時に減少する
関係にある。したがって、各コイル4の端子間電圧には
変位11に相当する電圧変化が生じるので、この2つの端
子間電圧の差を求めると第4図のような特性となり、そ
の値より傾斜角θを求めることができる。With this arrangement, since the magnetic fluid 3 gathers around the magnetic poles of the core 2, the core 2 floats above the groove surface of the container 1 and can freely move to the lowest position by gravity when the container 1 tilts. it can. Then, when the core 2 is located at the center of the two coils 4 as the reference position 10 (FIG. 3), when the container 1 is tilted by an angle θ from the horizontal direction as shown in FIG. 3, the core 2 and the magnetic fluid 3 Slides to the lowest position and moves from the reference position 10 by a displacement 11. This displacement 11 is d,
When the radius of curvature of the curved groove surface 6 is R, the relationship of d = θR is established, and the displacement 11 is proportional to the tilt angle θ. By the way, when the displacement 11 of the core 2 is represented by d, the inductance L of each coil 4 changes linearly as shown in FIG. 8 (L∝d). The solid line in FIG. 8 shows the change in the inductance of one coil 4, and the dotted line shows the change in the inductance of the other coil. Inductance increases when the core enters the coil and conversely decreases when it exits the coil. Therefore, a voltage change corresponding to the displacement 11 occurs in the voltage between the terminals of each coil 4, so that the difference between these two terminals has the characteristic shown in FIG. be able to.
第5図は本発明の他の実施例の構成を示すもので、各
コイル4は交流定電圧源Sに並列に接続されており、各
コイル4に流れる電流が電流電圧変換回路5Bを介して検
出回路5Aで検出されるようになっている。容器1の傾斜
に伴ない各コイル4に変位11に相当する電流変化が起こ
り、この2つの電流の差も第4図のような傾斜角に対し
て比例する特性となるので、その値より傾斜角θを求め
ることができる。FIG. 5 shows the configuration of another embodiment of the present invention, in which each coil 4 is connected in parallel to the AC constant voltage source S, and the current flowing through each coil 4 passes through the current-voltage conversion circuit 5B. It is designed to be detected by the detection circuit 5A. Along with the inclination of the container 1, a current change corresponding to the displacement 11 occurs in each coil 4, and the difference between these two currents also has a characteristic proportional to the inclination angle as shown in FIG. The angle θ can be obtained.
第6図は本発明の別の実施例の構成を示すもので、こ
の場合コイル4は差動トランスを構成するように容器1
のまわりに巻きつけられている。コイル4aは一次コイル
で、交流定電流源Sにより励磁され、コイル4bは二次コ
イルで、コア2の変位11に相当する電圧を出力する。二
次コイル4bの各出力電圧の差は第4図のような特性とな
るので、同様にして傾斜角θを求めることができる。FIG. 6 shows the construction of another embodiment of the present invention, in which case the coil 4 constitutes the container 1 so as to constitute a differential transformer.
Wrapped around. The coil 4a is a primary coil, which is excited by the AC constant current source S, and the coil 4b is a secondary coil, which outputs a voltage corresponding to the displacement 11 of the core 2. Since the difference between the output voltages of the secondary coil 4b has the characteristic shown in FIG. 4, the inclination angle θ can be obtained in the same manner.
第7図は本発明のもう1つの実施例における容器(筺
体)1の断面図であり、検出回路系としては上記実施例
のいずれのものでも用いることができる。この場合、容
器1の内面は、半径Rの円弧を容器1の円筒軸を中心に
回転させてできるたる型の曲面又はその一部となってお
り、この内面が案内溝面6として作用する。この実施例
の特徴は、容器1がその円筒軸を中心に回転しても、こ
の軸の水平面に対する傾斜角θの検出精度に何らの影響
も与えないということである。FIG. 7 is a sectional view of a container (housing) 1 according to another embodiment of the present invention, and any of the above-mentioned embodiments can be used as a detection circuit system. In this case, the inner surface of the container 1 is a barrel-shaped curved surface formed by rotating an arc of radius R about the cylindrical axis of the container 1 or a part thereof, and this inner surface acts as the guide groove surface 6. The feature of this embodiment is that even if the container 1 rotates about its cylindrical axis, it does not affect the detection accuracy of the inclination angle θ of this axis with respect to the horizontal plane.
以上、いくつかの実施例を示したが、その他多くの変
形が可能であることは明らかであろう。Although several embodiments have been shown above, it will be apparent that many other modifications are possible.
(発明の効果) 以上の様に、この発明による傾斜角検出器は、磁石よ
りなるコアと磁性流体とを湾曲内面を有する筐体に収容
するという簡単な構造によって傾斜によるコアの変位を
生じさせ、筐体のまわりのコイルでこの変位を電気量に
変換するため、高度の加工、組立技術を必要とせずに安
価で精度の高い傾斜角検出器を提供することができる。
また、傾斜に対する感度は曲率半径Rを変えることで自
由に設定することができる利点もある。この傾斜角検出
器によって被測定物の傾斜を高精度で検出でき、検出し
た電気信号によってその物体又はそれが関与する他の物
体の傾斜角調整駆動部にフイードバック制御をかけるこ
とができるので、この検出器は自動制御や遠隔制御など
に安価な素子として利用できる。そして、この傾斜角検
出器は、従来のものに比して、温度変化や衝撃等に対す
る傾斜角検出誤差が極めて小さいものである。(Effects of the Invention) As described above, the inclination angle detector according to the present invention causes the displacement of the core due to the inclination with a simple structure in which the core made of the magnet and the magnetic fluid are housed in the housing having the curved inner surface. Since this displacement is converted into an electric quantity by the coil around the housing, it is possible to provide an inexpensive and highly accurate inclination angle detector without requiring advanced processing and assembly techniques.
There is also an advantage that the sensitivity to inclination can be freely set by changing the radius of curvature R. This tilt angle detector can detect the tilt of the object to be measured with high accuracy, and feedback control can be applied to the tilt angle adjustment drive unit of the object or other objects related to the detected electric signal. The detector can be used as an inexpensive element for automatic control or remote control. The inclination angle detector has an extremely small inclination angle detection error with respect to temperature change, impact, etc., as compared with the conventional one.
第1図は本発明の1実施例による傾斜角検出器を示す構
成図、第2図(a)、(b)は第1図の線II−IIに沿っ
ての容器のみの断面図、第3図は傾斜時のコアの状態を
示す説明図、第4図は検出回路の傾斜角対出力特性図、
第5図は他の実施例の構成図、第6図は別の実施例の構
成図、第7図はもう1つの実施例の筐体の断面図、第8
図はコイルのコア変位対インダクタンス変化特性図であ
る。 1:容器(筐体)、2:磁石よりなるコア、3:磁性流体、4:
コイル、4a:差動トランスの一次コイル、4b:差動トラン
スの二次コイル、5A:検出回路、5B:電流電圧変換回路、
6:案内溝、10:基準位置、11:変位、S:電源FIG. 1 is a block diagram showing a tilt angle detector according to an embodiment of the present invention, and FIGS. 2 (a) and 2 (b) are sectional views of only the container along line II-II in FIG. 3 is an explanatory view showing the state of the core at the time of tilt, FIG. 4 is a tilt angle vs. output characteristic diagram of the detection circuit,
FIG. 5 is a block diagram of another embodiment, FIG. 6 is a block diagram of another embodiment, FIG. 7 is a sectional view of a housing of another embodiment, and FIG.
The figure is a core displacement vs. inductance change characteristic diagram of the coil. 1: container (case), 2: core consisting of magnet, 3: magnetic fluid, 4:
Coil, 4a: primary coil of differential transformer, 4b: secondary coil of differential transformer, 5A: detection circuit, 5B: current-voltage conversion circuit,
6: Guide groove, 10: Reference position, 11: Displacement, S: Power supply
Claims (3)
変位する磁石よりなるコアと、このコアを取り巻くよう
に前記筐体に巻回されたコイルと、このコイルに接続さ
れコアの変位に応じたコイルのインダクタンスの変化量
を検出して前記筐体の傾斜角を検出する検出回路とを備
えた傾斜角検出器であって、前記コアと前記筐体のコア
支持面との間に磁性流体を介在させるとともに、このコ
ア支持面にコア摺動用ガイドとして凹状に湾曲した案内
溝面を形成してなることを特徴とする傾斜角検出器1. A core made of a magnet housed in a housing and displaced according to the inclination of the housing, a coil wound around the housing so as to surround the core, and a core connected to the coil. A tilt angle detector comprising a detection circuit for detecting the amount of change in the inductance of the coil according to the displacement to detect the tilt angle of the housing, the tilt angle detector being provided between the core and a core supporting surface of the housing. Inclination angle detector characterized in that a magnetic fluid is interposed in the core and a guide groove surface curved in a concave shape is formed on the core support surface as a core sliding guide.
円型のいずれかとなるように構成したことを特徴とする
特許請求範囲第1項記載の傾斜角検出器2. The tilt angle detector according to claim 1, wherein the guide groove surface has a V-shaped, trapezoidal, or elliptical cross-sectional shape.
る型の曲面またはその一部から凹状に湾曲した案内溝面
を形成したことを特徴とする特許請求範囲第1項記載の
傾斜角検出器3. A guide groove surface curved in a concave shape is formed from a curved surface of a barrel formed by rotating an arc around a shaft of a housing or a part thereof, and a guide groove surface is formed. Inclination detector
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61272879A JPH083421B2 (en) | 1986-11-18 | 1986-11-18 | Inclination detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61272879A JPH083421B2 (en) | 1986-11-18 | 1986-11-18 | Inclination detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63128221A JPS63128221A (en) | 1988-05-31 |
| JPH083421B2 true JPH083421B2 (en) | 1996-01-17 |
Family
ID=17520034
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61272879A Expired - Fee Related JPH083421B2 (en) | 1986-11-18 | 1986-11-18 | Inclination detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH083421B2 (en) |
Families Citing this family (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3833062A1 (en) * | 1988-09-29 | 1990-04-05 | Schmidt Paul | INCLINATION ANGLE SENSOR |
| JP3180398B2 (en) * | 1991-12-27 | 2001-06-25 | 株式会社デンソー | Catalyst deterioration detection device for internal combustion engine |
| JP3496307B2 (en) * | 1994-02-18 | 2004-02-09 | 株式会社デンソー | Catalyst deterioration detection method and air-fuel ratio sensor |
| JP3063517B2 (en) * | 1994-03-14 | 2000-07-12 | 日産自動車株式会社 | Exhaust gas purification device for internal combustion engine |
| US5452520A (en) * | 1994-03-14 | 1995-09-26 | Ferrofluidics Corporation | Ferrofluid inclinometer |
| US7222433B2 (en) * | 2002-01-23 | 2007-05-29 | Autonnic Research, Inc. | Electromagnetic inclinometer |
| JP4265497B2 (en) | 2004-07-05 | 2009-05-20 | トヨタ自動車株式会社 | Exhaust purification device control method |
| DE102006061198B4 (en) * | 2006-05-31 | 2019-07-18 | Asm Automation Sensorik Messtechnik Gmbh | tilt sensor |
| CN103149384B (en) * | 2013-02-07 | 2016-02-10 | 北京交通大学 | A kind of magnetic liquid acceleration sensor |
| CN112880641A (en) * | 2021-03-26 | 2021-06-01 | 重庆科技学院 | Inductance type inclinometer and angle measuring method thereof |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS488293U (en) * | 1971-06-11 | 1973-01-30 | ||
| JPS5835726B2 (en) * | 1980-09-19 | 1983-08-04 | 日本染色機械株式会社 | filtration device |
-
1986
- 1986-11-18 JP JP61272879A patent/JPH083421B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63128221A (en) | 1988-05-31 |
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