JP3022671B2 - Displacement sensor - Google Patents
Displacement sensorInfo
- Publication number
- JP3022671B2 JP3022671B2 JP3347497A JP34749791A JP3022671B2 JP 3022671 B2 JP3022671 B2 JP 3022671B2 JP 3347497 A JP3347497 A JP 3347497A JP 34749791 A JP34749791 A JP 34749791A JP 3022671 B2 JP3022671 B2 JP 3022671B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode members
- displacement
- electrode
- measured
- pair
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P15/00—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration
- G01P15/02—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses
- G01P15/08—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values
- G01P2015/0805—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration
- G01P2015/0822—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration for defining out-of-plane movement of the mass
- G01P2015/0825—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration for defining out-of-plane movement of the mass for one single degree of freedom of movement of the mass
- G01P2015/0828—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration for defining out-of-plane movement of the mass for one single degree of freedom of movement of the mass the mass being of the paddle type being suspended at one of its longitudinal ends
Landscapes
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、例えば物体の傾斜角、
加速度、位置等の変位の検出に用いられる静電容量式の
変位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, for example, an inclination angle of an object,
The present invention relates to a capacitance type displacement sensor used for detecting displacement such as acceleration and position.
【0002】[0002]
【従来の技術】従来、傾斜角用の変位計には、接触式と
非接触式のものが知られている。2. Description of the Related Art Conventionally, a contact type and a non-contact type are known as displacement meters for inclination angles.
【0003】接触式は、図8で示すように振子60の先
端に取付けたブラシ61を、一定電圧を印加した抵抗体
62に摺接させる構造となっており、このブラシ61に
よって分圧された電圧を検出出力として取出すことによ
り傾斜角を検出するものである。The contact type has a structure in which a brush 61 attached to the tip of a pendulum 60 is slidably contacted with a resistor 62 to which a constant voltage is applied as shown in FIG. The inclination angle is detected by extracting the voltage as a detection output.
【0004】一方、非接触式は、図9で示すように振子
70の先端に取付けた磁石71を磁気抵抗素子72,7
3に沿わせて非接触で揺動させ、磁気抵抗素子72,7
3の抵抗値変化から差動的に傾斜角を検出するものであ
る。On the other hand, in a non-contact type, as shown in FIG.
3 and are oscillated in a non-contact manner along the magnetoresistive elements 72 and 7.
The inclination angle is differentially detected from the change in the resistance value of No. 3.
【0005】[0005]
【発明が解決しようとする課題】上記接触式変位計にお
いては、ヒステリシスの発生が不可避であり、また抵抗
体やこの抵抗体に摺接するブラシが長年の使用により摩
耗してしまうため、変位量の検出精度や耐久性に問題が
あった。In the above-mentioned contact type displacement meter, the occurrence of hysteresis is inevitable, and the resistor and the brush which is in sliding contact with the resistor are worn due to long-term use. There were problems in detection accuracy and durability.
【0006】又、非接触式変位計においては、かかる問
題は発生しないが、磁石の経年変化による磁気特性の劣
化が生じ易く、検出精度や耐久性に問題があり、また磁
気抵抗素子が半導体であるため温度特性が悪く、広い温
度範囲における使用には何らかの温度補償を考慮しなけ
ればならなかった。In the non-contact type displacement meter, such a problem does not occur, but the magnetic characteristics are easily deteriorated due to aging of the magnet, and there are problems in detection accuracy and durability. Therefore, the temperature characteristics are poor, and some temperature compensation must be considered for use in a wide temperature range.
【0007】本発明は、このような問題点に鑑み、ヒス
テリシスが発生せず長年の使用及び比較的広い温度範囲
の環境下で使用しても変位量の検出精度の悪化がなく、
耐久性の高い変位センサを提供することをその目的とし
ている。[0007] In view of the above problems, the present invention does not cause hysteresis and does not deteriorate the displacement detection accuracy even when used for a long time and in an environment in a relatively wide temperature range.
It is an object of the present invention to provide a highly durable displacement sensor.
【0008】[0008]
【課題を解決するための手段】上記目的を達成すべく本
発明は、互いに対向して配置された一対の電極部材と、
一対の電極部材間に設けられた一定容量の付加容量手段
と、一対の電極部材の一方に交流電圧を印加する信号源
とを備え、一対の電極部材は、これらの間の距離および
対向面積の少なくとも一方が測定すべき変位に応じて非
線形に変化するよう、一端側が傾斜可能に保持されると
共に測定対象物に取り付けられ、変位の検出結果が一対
の電極部材の他方の電位として出力されることを特徴と
する。In order to achieve the above object, the present invention comprises a pair of electrode members arranged opposite to each other,
An additional capacitance means having a constant capacitance provided between the pair of electrode members, and a signal source for applying an AC voltage to one of the pair of electrode members, wherein the pair of electrode members have a distance between them and a facing area. One end side is tiltably held and attached to the object to be measured so that at least one of them changes nonlinearly according to the displacement to be measured, and the detection result of the displacement is output as the other potential of the pair of electrode members. It is characterized by.
【0009】ここで、一対の電極部材の各々の一端部が
測定すべき傾斜角の変位方向に可動な第1のヒンジによ
り測定対象物と結合され、一対の電極部材の各々の他端
部間に雰囲気に比べて高誘電率の材料を介在させること
で付加容量手段が構成され、付加容量手段の構成部分が
変位方向に可動な第2のヒンジにより一対の電極部材の
中間部分と結合されていることが好ましい。Here, one end of each of the pair of electrode members is connected to the object to be measured by a first hinge movable in the direction of displacement of the inclination angle to be measured, and between the other end of each of the pair of electrode members. The additional capacitance means is constituted by interposing a material having a higher dielectric constant than the atmosphere, and the constituent part of the additional capacitance means is connected to the intermediate part of the pair of electrode members by the second hinge movable in the displacement direction. Is preferred.
【0010】また、本発明は、互いに対向して配置され
た第1および第2の電極部材と、第1および第2の電極
部材間にこれらと対向するように配置された第3の電極
部材と、第1および第3の電極部材間と第2および第3
の電極部材間に設けられた一定容量の付加容量手段と、
第1および第2の電極部材間に交流電圧を印加する信号
源とを備え、第1、第2および第3の電極部材は、第1
および第3の電極部材間と第2および第3の電極部材間
の距離および対向面積の少なくとも一方が測定すべき変
位に応じて非線形に変化するよう、一端側が傾斜可能に
保持されると共に測定対象物に取り付けられ、変位の検
出結果が第3の電極部材の電位として出力されることを
特徴とする。The present invention is also directed to a first and a second electrode member disposed opposite each other, and a third electrode member disposed between the first and second electrode members so as to face the first and second electrode members. And between the first and third electrode members and between the second and third electrode members.
An additional capacitance means having a constant capacitance provided between the electrode members of
A signal source for applying an AC voltage between the first and second electrode members, wherein the first, second, and third electrode members have a first
One end is held so as to be tiltable so that at least one of the distance between the third electrode member and the distance between the second and third electrode members and the opposing area changes non-linearly in accordance with the displacement to be measured. It is attached to an object, and a detection result of the displacement is output as a potential of the third electrode member.
【0011】この場合、第1、第2および第3の電極部
材の各々における互いに同じ側の一端部が測定すべき傾
斜角の変位方向に可動な第1のヒンジにより測定対象物
と結合され、第1および第2の電極部材と第3の前記第
1のヒンジ結合位置が変位方向で異なっていることが好
ましい。一方で、第1、第2および第3の電極部材の各
々の他端部間に雰囲気に比べて高誘電率の材料を介在さ
せることで付加容量手段が構成され、付加容量手段の構
成部分が変位方向に可動な第2のヒンジにより第1、第
2および第3の電極部材の中間部分と結合されているこ
とも好ましい。In this case, one end of each of the first, second and third electrode members on the same side is connected to the object to be measured by a first hinge movable in a direction of displacement of the inclination angle to be measured, It is preferable that the first and second electrode members and the third first hinge connection position are different in the displacement direction. On the other hand, the additional capacitance means is configured by interposing a material having a higher dielectric constant than the atmosphere between the other end portions of the first, second, and third electrode members, and the constituent parts of the additional capacitance means It is also preferable that the first, second and third electrode members are connected to an intermediate portion by a second hinge movable in the displacement direction.
【0012】[0012]
【作用】測定すべき変位により、例えば平行配置した電
極部材が互に平行状態を保ったまま傾動し、これに伴っ
て電極部材間の距離、対向面積が変化する。その結果、
電極部材間の静電容量が変化するので、ある電極部材に
交流電圧を印加しておけば、他の電極部材の電位により
変位量が検出される。すなわち、静電容量式のセンサを
3枚の電極部材で構成し、中間の電極部材のヒンジをそ
の両側の電極部材のヒンジに対し変位方向と直交方向に
位置をずらして設けておけば、変位に伴うこれら電極部
材の傾動により、中間の電極部材に対する一側の電極部
材の対面距離と他側の電極部材の対面距離とは、一方が
減少すると他方が増加することになる。According to the displacement to be measured, for example, the electrode members arranged in parallel tilt while keeping the parallel state, and the distance between the electrode members and the facing area change accordingly. as a result,
Since the capacitance between the electrode members changes, if an AC voltage is applied to a certain electrode member, the amount of displacement is detected by the potential of another electrode member. In other words, if the capacitance type sensor is composed of three electrode members, and the hinge of the intermediate electrode member is displaced in the direction orthogonal to the displacement direction with respect to the hinges of the electrode members on both sides, the displacement is increased. Due to the tilting of these electrode members, the facing distance of the electrode member on one side with respect to the intermediate electrode member and the facing distance of the electrode member on the other side decrease and increase the other.
【0013】このことは、中間の電極部材と一側の電極
部材との間の静電容量と中間の電極部材と他側の電極部
材との間の静電容量とが増減することと等価になり、両
側の電極部材を交流電源に接続し、中間の電極部材から
検出出力を取出すことで、これらの変化を差動的に検出
でき、温度補償された正確な検出出力を得ることができ
る。この場合、静電容量の変化は測定すべき変位に対し
て非線形(例えば正弦波状)であるので、付加容量を配
設することにより、線形な出力電圧を検出できる。This is equivalent to an increase or decrease in the capacitance between the intermediate electrode member and the one-side electrode member and the capacitance between the intermediate electrode member and the other-side electrode member. In other words, by connecting the electrode members on both sides to an AC power source and taking out the detection output from the intermediate electrode member, these changes can be detected differentially, and an accurate temperature-compensated detection output can be obtained. In this case, since the change in the capacitance is non-linear (for example, sinusoidal) with respect to the displacement to be measured, a linear output voltage can be detected by providing the additional capacitance.
【0014】[0014]
【実施例】図1を参照して、本発明の第1の実施例に係
る変位計について説明する。導電性の材質からなる2枚
の電極板1,1を互いに平行に配設して静電容量部材2
が構成されている。両電極板1,1の両端部は、それぞ
れ絶縁板6を挾んだ状態で接着剤等により積層固着され
ている。そして、静電容量部材2の一端を固定部3と
し、他端を可動部4として、固定部3に対し可動部4が
平行に移動できるように各電極板1の両端部にそれぞれ
ヒンジ5,5を設けている。各ヒンジ5は固定部3の下
面、及び可動部4の上面にそれぞれ接するように設けら
れており、これにより、両電極1,1にいわゆる平行リ
ンク機構が構成されている。また、固定部3の上面に電
極板1,1に連なる電極端子7,7が設けられており、
一方が電源端子、他方が出力端子となっている。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A displacement meter according to a first embodiment of the present invention will be described with reference to FIG. Two electrode plates 1 and 1 made of a conductive material are disposed in parallel with each other to form a capacitance member 2.
Is configured. Both ends of the two electrode plates 1 and 1 are laminated and fixed with an adhesive or the like with the insulating plate 6 interposed therebetween. One end of the capacitance member 2 is a fixed part 3, and the other end is a movable part 4, and hinges 5 are provided at both ends of each electrode plate 1 so that the movable part 4 can move parallel to the fixed part 3. 5 are provided. Each hinge 5 is provided so as to be in contact with the lower surface of the fixed portion 3 and the upper surface of the movable portion 4, thereby forming a so-called parallel link mechanism between the electrodes 1 and 1. Further, electrode terminals 7, 7 connected to the electrode plates 1, 1 are provided on the upper surface of the fixing portion 3,
One is a power terminal and the other is an output terminal.
【0015】以上の構成において、両端部のヒンジ5,
5間における両電極板1,1の間隔及び有効対向面積を
L1 及びS1 とし、また、ヒンジ5,5の外側すなわち
静電容量部材2の固定部3及び可動部4における電極板
間隔及び有効対向面積をL0 及びS0 とすると、静電容
量部材2の静電容量Cは、 C=ε0 (S1 /L1 +εS ・S0 /L0 ) で表わされる。ここで、ε0 は真空の誘電率、εS は絶
縁板6の比誘電率である。ここで、固定部3に対して可
動部4が変位して電極板1,1が角度ψだけ傾動する
と、変位後の電極板間隔L1 は、L0 cosψとなり、
静電容量は変位角度ψに対応し上式に従って変化する。In the above configuration, the hinges 5 at both ends are provided.
5, the distance between the two electrode plates 1 and 1 and the effective facing area are defined as L 1 and S 1. Assuming that the effective facing area is L 0 and S 0 , the capacitance C of the capacitance member 2 is represented by C = ε 0 (S 1 / L 1 + ε S · S 0 / L 0 ). Here, ε 0 is a dielectric constant in a vacuum, and ε S is a relative dielectric constant of the insulating plate 6. Here, when the movable portion 4 is displaced with respect to the fixed portion 3 and the electrode plates 1 and 1 are tilted by the angle ψ, the electrode plate interval L 1 after the displacement becomes L 0 cosψ,
The capacitance changes according to the above equation according to the displacement angle ψ.
【0016】したがって、可動部4がピン(図示せず)
等を介して被測定物の変位に応じて変位するようにして
おけば、静電容量Cの変化により被測定物の変位を測定
できる。また、可動部4に錘9を取付けることにより、
固定部3の重力方向に対する傾斜角も測定できることと
なる。また、比誘電率εs の絶縁板6が介在することに
より形成された付加的な浮遊容量C0 =ε0 ・εs ・S
0 /L0 は、出力電圧の非線形性を改善し、線形な出力
をもたらすように作用する。このような作用は、特に後
述の第2実施例において顕著である。Therefore, the movable portion 4 is provided with a pin (not shown).
If the object is displaced in accordance with the displacement of the object to be measured, the displacement of the object can be measured by a change in the capacitance C. Also, by attaching the weight 9 to the movable part 4,
The inclination angle of the fixed part 3 with respect to the direction of gravity can also be measured. Further, an additional stray capacitance C 0 = ε 0 · ε s · S formed by the interposition of the insulating plate 6 having a relative permittivity ε s.
0 / L 0 serves to improve the non-linearity of the output voltage and provide a linear output. Such an effect is particularly remarkable in a second embodiment described later.
【0017】以下、図2及び図3を参照して本発明を第
2実施例である傾斜角計に適用した場合を説明する。Hereinafter, a case where the present invention is applied to an inclinometer according to a second embodiment will be described with reference to FIGS.
【0018】この実施例では、3枚の電極板1a,1
b,1cが相互に平行に配設され、これら電極1a,1
b,1cの両端を上記実施例と同様にそれぞれ絶縁板6
を挾んだ状態で接着剤等により積層固着して、実質的に
2つのコンデンサから成る静電容量部材2が構成されて
いる。この静電容量部材2は、その上端を固定部3と
し、下端を可動部4として構成されており、図2に示す
如く、固定部3に静電容量部材2を被測定物に垂設する
ためのブラケット8が取付けられ、一方で可動部4に錘
9が取付けられている。In this embodiment, three electrode plates 1a, 1
b, 1c are arranged in parallel with each other, and these electrodes 1a, 1c
b, 1c at both ends in the same manner as in the above embodiment.
Are sandwiched and laminated by an adhesive or the like, thereby forming a capacitance member 2 substantially composed of two capacitors. This capacitance member 2 is configured such that its upper end is a fixed part 3 and its lower end is a movable part 4, and as shown in FIG. Bracket 8 is attached, while a weight 9 is attached to the movable part 4.
【0019】また、これら電極板1a,1b,1cによ
り、可動部4を固定部3に対して平行移動させる平行リ
ンク機構が構成されるように各電極板の両端部にはヒン
ジ5が設けられている。この場合、中間の電極板1bの
ヒンジ5の位置は、左右両側の電極板1a,1cのヒン
ジ5の位置に対し、上下方向に所定量hだけずらして設
けられている。これにより、傾動に伴う一方の電極板1
a,1b間の距離と他方の電極板1b,1c間の距離と
は、一方が増加すれば他方が減少し、一方が減少すれば
他方が増加することになる(図3参照)。Hinges 5 are provided at both ends of each of the electrode plates 1a, 1b and 1c so that a parallel link mechanism for moving the movable portion 4 in parallel with the fixed portion 3 is constituted by these electrode plates 1a, 1b and 1c. ing. In this case, the position of the hinge 5 of the intermediate electrode plate 1b is shifted vertically by a predetermined amount h from the position of the hinge 5 of the left and right electrode plates 1a, 1c. Thereby, one electrode plate 1 accompanying the tilting
The distance between a and 1b and the distance between the other electrode plates 1b and 1c are such that if one increases, the other decreases, and if one decreases, the other increases (see FIG. 3).
【0020】各ヒンジ5は、電極板1a,1b,1cに
一体成形した弾性的で屈曲可能な折曲げ部で構成されて
いる。この折曲げ部は、図2に示す長孔や、図3に示す
薄肉部のように部材の一部を加工して屈曲可能に形成す
るようにしても良いし、或いは断面Ω状等の可撓部で構
成しても良い。Each hinge 5 is constituted by an elastic and bendable bent portion integrally formed with the electrode plates 1a, 1b, 1c. The bent portion may be formed by processing a part of the member like a long hole shown in FIG. 2 or a thin portion shown in FIG. You may comprise a bending part.
【0021】一方、固定部3に各電極板1a,1b,1
cに連なる電極端子7a,7b,7cを設け、図4に示
すように左右両側の電極板1a,1cを交流電源10に
接続し、中間の電極板1bからの交流出力を増幅器11
とで増幅し、整流器12を介して直流レベルの検出出力
を取出すようにしている。On the other hand, each electrode plate 1a, 1b, 1
c, electrode terminals 7a, 7b, 7c are provided, and the left and right electrode plates 1a, 1c are connected to an AC power source 10 as shown in FIG.
And a DC level detection output is taken out via the rectifier 12.
【0022】以上の構成において、被測定物が傾いて電
極板1a,1b,1cが錘9の働きにより、例えば図3
に仮想線で示す如く右方に角度ψだけ傾動すると、中間
の電極板1bのヒンジ5の位置の変位量hに起因して、
中間の電極板1bと左側の電極板1aとの距離L1 は、 L1 =(L0 −h・tanψ)cosψ となり、一方、中間の電極板1bと右側の電極板1cと
の距離L2 は、 L2 =(L0 +h・tanψ)cosψ となる。このように、h・tanψが中間の電極板1b
に対する左側電極板1aの距離L1 と右側電極板1cの
距離L2 とで正負逆になるため、電極板1bと電極板1
aとの間の静電容量と、電極板1bと電極板1cとの間
の静電容量とが差動的に変化し、温度変化や誘電率変化
に対する影響が相殺されて、傾斜角に応じた正確な検出
出力が得られるようになる。In the above configuration, the object to be measured is inclined and the electrode plates 1a, 1b, 1c are operated by the weight 9 so that, for example, FIG.
Is tilted rightward by an angle ψ as shown by the imaginary line, due to the displacement amount h of the position of the hinge 5 of the intermediate electrode plate 1b,
Distance L 1 between the intermediate electrode plate 1b and the left electrode plate 1a is, L 1 = (L 0 -h · tanψ) cosψ . On the other hand, the distance between the intermediate electrode plate 1b and the right side of the electrode plate 1c L 2 Is L 2 = (L 0 + h · tan {) cos}. Thus, h · tan ・ is an intermediate electrode plate 1b
To become a sign reversed between the distance L 2 of the distance L 1 and the right electrode plate 1c of the left electrode plate 1a with respect to the electrode plate 1b and the electrode plate 1
a and the capacitance between the electrode plate 1b and the electrode plate 1c change differentially, and the influence on the temperature change and the change in the dielectric constant is canceled out. Thus, an accurate detection output can be obtained.
【0023】ところで、上記の如くヒンジ5を弾性的に
屈曲可能な折曲げ部で構成すると、ヒンジ5に働く弾性
力により、被測定物の傾斜角θと電極板1a,1b,1
cの傾斜角ψは一致しなくなるが、ヒンジ5のばね定数
をK、両端部のヒンジ間距離をLV 、錘9の重量をMと
して、ψとθとの間には、 ψ=sin-1(M/K・LV ・sinθ) の関係式が成立し、ψに応じた検出出力からθを求める
ことができる。When the hinge 5 is constituted by a bent portion which can be elastically bent as described above, the inclination angle θ of the object to be measured and the electrode plates 1a, 1b, 1
Although the inclination angle の of c does not coincide, the spring constant of the hinge 5 is K, the distance between the hinges at both ends is L V , and the weight of the weight 9 is M, and between ψ and θ, ψ = sin − 1 relation is satisfied for (M / K · L V · sinθ), can be obtained θ from the detection output corresponding to [psi.
【0024】図5は、3枚の電極板1a,1b,1cの
傾動角ψに対する検出出力の変化特性を示し、各電極板
間の静電容量にヒンジ5の外端側、すなわち固定部3や
可動部4の絶縁板6によって得られる絶縁静電容量(浮
遊容量)が付加されない場合には、A線の如く非線形の
変化特性となるが、両端部のヒンジ5間における各電極
板間の静電容量に所定の浮遊容量を付加することで、B
線のようなほぼ線形の変化特性となる。FIG. 5 shows a change characteristic of the detection output with respect to the tilt angle の of the three electrode plates 1a, 1b, 1c. When the insulating capacitance (floating capacitance) obtained by the insulating plate 6 of the movable part 4 is not added, the characteristic changes nonlinearly like the A line, but between the electrode plates between the hinges 5 at both ends. By adding a predetermined stray capacitance to the capacitance, B
It has a substantially linear change characteristic like a line.
【0025】図6、図7は変化特性の実測値を示してい
る。いずれも、浮遊容量としての付加容量を除く零点時
容量は42.5pFである。そして、ヒンジにおけるバ
ネ係数は、図6の例では0.6、図7の例では0.8と
し、±65degの傾斜角センサとして求めた。6 and 7 show measured values of the change characteristics. In each case, the capacitance at zero point excluding the additional capacitance as the stray capacitance is 42.5 pF. The spring coefficient of the hinge was 0.6 in the example of FIG. 6 and 0.8 in the example of FIG. 7, and was obtained as a tilt angle sensor of ± 65 deg.
【0026】図6(a)は出力;{C1 /(C1 +
C2 )}の角度(deg)依存性を示し、同図(b)は
その直線性[%FS]を示す。図において、曲線Aは付
加浮遊容量が50pFのとき、曲線Bは付加浮遊容量が
無いとき、曲線E、Fはそれぞれ付加浮遊容量が90p
F、110pFのときである。浮遊容量を付加すること
で、非線形な変化を線形に近づけ得ることが理解でき
る。FIG. 6A shows an output; ΔC 1 / (C 1 +
C 2 )} shows the angle (deg) dependency, and FIG. 2B shows the linearity [% FS]. In the figure, the curve A is when the additional stray capacitance is 50 pF, the curve B is when there is no additional stray capacitance, and the curves E and F are respectively when the additional stray capacitance is 90 pF.
F, 110 pF. It can be understood that by adding the stray capacitance, the nonlinear change can be made closer to linear.
【0027】図7(a)、(b)についても同様であ
り、曲線Aはポリイミドフィルム(εS =3.5)を用
いることにより付加浮遊容量が50pFのとき、曲線B
はテフロンフィルム(εS =2.2)を用いることによ
り浮遊容量が30pF付加されたときを示す。また、曲
線Cは浮遊容量が15pFと仮定した場合であり、曲線
Dは付加浮遊容量が無い場合である。この場合にも、検
出特性を線形にできることがわかる。The same applies to FIGS. 7 (a) and 7 (b). Curve A is obtained by using a polyimide film (ε S = 3.5), and when the additional floating capacitance is 50 pF, the curve B
Shows a case where a stray capacitance of 30 pF is added by using a Teflon film (ε S = 2.2). Curve C shows the case where the stray capacitance is 15 pF, and curve D shows the case where there is no additional stray capacitance. Also in this case, it can be seen that the detection characteristic can be made linear.
【0028】又、ヒンジ5に弾性力を作用させることに
より、電極板を加速度によって可動部に働く力に応じた
角度に傾動させられるようになり、本発明の変位計を加
速度センサとして用いることもできる。また、可動部を
固定部とは相対移動する物体に取り付けることにより、
直線的な位置変位のセンサとして用いることもできる。Further, by applying an elastic force to the hinge 5, the electrode plate can be tilted at an angle corresponding to the force acting on the movable portion by acceleration, and the displacement meter of the present invention can be used as an acceleration sensor. it can. Also, by attaching the movable part to the object that moves relatively to the fixed part,
It can also be used as a linear displacement sensor.
【0029】[0029]
【発明の効果】以上の説明で明らかなように、本発明に
よれば、測定すべき変位により、平行配置した電極部材
が互に平行状態を保ったまま傾動し、これに伴って電極
部材間の静電容量が変化するので、ある電極部材に交流
電圧を印加しておけば、他の電極部材の電位により変位
量が検出される。また、静電容量部材を3枚の電極部材
で構成し、中間の電極部材のヒンジをその両側の電極部
材のヒンジに対し変位と直交方向に位置をずらして設け
ておけば、変位に伴うこれら電極部材の傾動により、中
間の電極部材と一側の電極部材との間の静電容量と中間
の電極部材と他側の電極部材との間の静電容量とが増減
することとなり、両側の電極部材を交流電源に接続し、
中間の電極部材から検出出力を取出すことで、これらの
変化を差動的に検出でき、温度補償された正確な検出出
力を得ることができる。この場合、静電容量の変化は測
定すべき変位に対して非線形(例えば正弦波状)である
ので、付加容量を配設することにより、線形な出力電圧
を検出できる。As is apparent from the above description, according to the present invention, due to the displacement to be measured, the electrode members arranged in parallel tilt while maintaining the parallel state with each other. Since the capacitance of the electrode member changes, if an AC voltage is applied to a certain electrode member, the displacement amount is detected based on the potential of another electrode member. Further, if the capacitance member is constituted by three electrode members, and the hinges of the intermediate electrode members are provided so as to be displaced in the direction orthogonal to the displacement with respect to the hinges of the electrode members on both sides thereof, it is possible to reduce the displacement due to the displacement. Due to the tilting of the electrode members, the capacitance between the intermediate electrode member and the electrode member on one side and the capacitance between the intermediate electrode member and the electrode member on the other side increase or decrease. Connect the electrode members to an AC power supply,
By extracting the detection output from the intermediate electrode member, these changes can be detected differentially, and an accurate temperature-compensated detection output can be obtained. In this case, since the change in the capacitance is non-linear (for example, sinusoidal) with respect to the displacement to be measured, a linear output voltage can be detected by providing the additional capacitance.
【0030】また、電極部材間の距離、対向面積の変化
に起因した静電容量の変化により変位を検出するため、
接触式と違いヒステリンスの発生がなく磨耗による耐久
性及び検出精度の悪化はなく、更に従来の非接触式変位
計のように磁石及び磁気抵抗素子等の半導体を使用して
ないため経時変化による検出精度の悪化はなく、広い温
度範囲においても使用できる効果がある。Further, in order to detect a displacement based on a change in capacitance due to a change in the distance between the electrode members and a facing area,
Unlike contact type, there is no occurrence of hysteresis, there is no deterioration of durability and detection accuracy due to abrasion, and since it does not use semiconductors such as magnets and magnetoresistive elements unlike conventional non-contact type displacement gauges, detection by aging changes There is no deterioration in accuracy and there is an effect that it can be used in a wide temperature range.
【図1】本発明の第1実施例に係る変位計の側面図であ
る。FIG. 1 is a side view of a displacement meter according to a first embodiment of the present invention.
【図2】本発明の第2実施例に係る変位計の斜視図であ
る。FIG. 2 is a perspective view of a displacement meter according to a second embodiment of the present invention.
【図3】図2の実施例でヒンジを変えた場合の裁断側面
図である。FIG. 3 is a cut-away side view when the hinge is changed in the embodiment of FIG. 2;
【図4】図2、図3の実施例に適用される検出回路を示
す回路図である。FIG. 4 is a circuit diagram showing a detection circuit applied to the embodiment of FIGS. 2 and 3;
【図5】検出出力の変化特性図である。FIG. 5 is a change characteristic diagram of a detection output.
【図6】検出出力の角度依存性を示す実測図である。FIG. 6 is an actual measurement diagram showing the angle dependence of a detection output.
【図7】検出出力の直線性を示す実測図である。FIG. 7 is an actual measurement diagram showing linearity of a detection output.
【図8】従来の接触式変位計を示す構造図である。FIG. 8 is a structural view showing a conventional contact displacement meter.
【図9】従来の非接触式変位計を示す構造図である。FIG. 9 is a structural diagram showing a conventional non-contact displacement meter.
1…電極板、2…静電容量部材、3…固定部、4…可動
部、5…ヒンジ、9…錘DESCRIPTION OF SYMBOLS 1 ... Electrode plate, 2 ... Capacitance member, 3 ... Fixed part, 4 ... Movable part, 5 ... Hinge, 9 ... Weight
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平2−145901(JP,A) 特開 平1−165920(JP,A) 実開 平3−122319(JP,U) 実開 昭62−193536(JP,U) (58)調査した分野(Int.Cl.7,DB名) G01B 7/00 - 7/34 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-2-145901 (JP, A) JP-A-1-165920 (JP, A) JP-A 3-122319 (JP, U) JP-A 62-145 193536 (JP, U) (58) Field surveyed (Int. Cl. 7 , DB name) G01B 7/ 00-7/34
Claims (5)
材と、 前記一対の電極部材間に設けられた一定容量の付加容量
手段と、 前記一対の電極部材の一方に交流電圧を印加する信号源
とを備え、 前記一対の電極部材は、これらの間の距離および対向面
積の少なくとも一方が測定すべき変位に応じて非線形に
変化するよう、一端側が傾斜可能に保持されると共に測
定対象物に取り付けられ、 前記変位の検出結果が前記一対の電極部材の他方の電位
として出力されることを特徴とする変位センサ。1. A pair of electrode members arranged to face each other, an additional capacitance means having a constant capacity provided between the pair of electrode members, and a signal for applying an AC voltage to one of the pair of electrode members. A pair of electrode members, at least one of a distance between them and an opposing area is non-linearly changed in accordance with a displacement to be measured, and one end side is held to be tiltable and attached to a measurement target. A displacement sensor, wherein the detection result of the displacement is output as the other potential of the pair of electrode members.
定すべき傾斜角の変位方向に可動な第1のヒンジにより
前記測定対象物と結合され、前記一対の電極部材の各々
の他端部間に雰囲気に比べて高誘電率の材料を介在させ
ることで前記付加容量手段が構成され、前記付加容量手
段の構成部分が前記変位方向に可動な第2のヒンジによ
り前記一対の電極部材の中間部分と結合されている請求
項1記載の変位センサ。2. One end of each of the pair of electrode members is coupled to the object to be measured by a first hinge movable in a displacement direction of a tilt angle to be measured, and the other end of each of the pair of electrode members is provided. The additional capacitance means is constituted by interposing a material having a higher dielectric constant than the atmosphere between the portions, and the constituent part of the additional capacitance means is formed by a second hinge movable in the displacement direction. 2. The displacement sensor according to claim 1, wherein the displacement sensor is connected to an intermediate part.
2の電極部材と、 前記第1および第2の電極部材間にこれらと対向するよ
うに配置された第3の電極部材と、 前記第1および第3の電極部材間と前記第2および第3
の電極部材間に設けられた一定容量の付加容量手段と、 前記第1および第2の電極部材間に交流電圧を印加する
信号源とを備え、 前記第1、第2および第3の電極部材は、前記第1およ
び第3の電極部材間と前記第2および第3の電極部材間
の距離および対向面積の少なくとも一方が測定すべき変
位に応じて非線形に変化するよう、一端側が傾斜可能に
保持されると共に測定対象物に取り付けられ、 前記変位の検出結果が前記第3の電極部材の電位として
出力されることを特徴とする変位センサ。A first and a second electrode member disposed opposite to each other; a third electrode member disposed between the first and second electrode members so as to face the first and second electrode members; Between the first and third electrode members and the second and third electrode members;
And a signal source for applying an AC voltage between the first and second electrode members, wherein the first, second and third electrode members are provided. One end can be tilted so that at least one of the distance and the facing area between the first and third electrode members and between the second and third electrode members changes non-linearly according to the displacement to be measured. A displacement sensor that is held and attached to an object to be measured, and the detection result of the displacement is output as a potential of the third electrode member.
各々の一端部が測定すべき傾斜角の変位方向に可動な第
1のヒンジにより前記測定対象物と結合され、前記第1
および第2の電極部材と前記第3の前記第1のヒンジ結
合位置が前記変位方向で異なっている請求項3記載の変
位センサ。4. One end of each of the first, second, and third electrode members is coupled to the object by a first hinge movable in a displacement direction of a tilt angle to be measured, and
4. The displacement sensor according to claim 3, wherein the second electrode member and the third first hinge coupling position are different in the displacement direction. 5.
各々の他端部間に雰囲気に比べて高誘電率の材料を介在
させることで前記付加容量手段が構成され、前記付加容
量手段の構成部分が前記変位方向に可動な第2のヒンジ
により前記第1、第2および第3の電極部材の中間部分
と結合されている請求項4記載の変位センサ。5. The additional capacitance means is constituted by interposing a material having a higher dielectric constant than the atmosphere between the other end of each of the first, second and third electrode members. 5. The displacement sensor according to claim 4, wherein a component part of the means is connected to an intermediate portion between the first, second and third electrode members by a second hinge movable in the displacement direction.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3347497A JP3022671B2 (en) | 1991-12-27 | 1991-12-27 | Displacement sensor |
| US07/974,160 US5323118A (en) | 1991-11-12 | 1992-11-10 | Hinged displacement sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3347497A JP3022671B2 (en) | 1991-12-27 | 1991-12-27 | Displacement sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH05180612A JPH05180612A (en) | 1993-07-23 |
| JP3022671B2 true JP3022671B2 (en) | 2000-03-21 |
Family
ID=18390627
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3347497A Expired - Lifetime JP3022671B2 (en) | 1991-11-12 | 1991-12-27 | Displacement sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3022671B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5081692B2 (en) * | 2008-03-31 | 2012-11-28 | アルプス電気株式会社 | Physical quantity sensor |
| CN110986755B (en) * | 2019-12-16 | 2020-12-29 | 珠海格力电器股份有限公司 | Electrical appliance tilt detection structure, method, device, storage medium and electrical appliance |
-
1991
- 1991-12-27 JP JP3347497A patent/JP3022671B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH05180612A (en) | 1993-07-23 |
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