JPS58155302A - Electrostatic capacity type displacement gage - Google Patents

Electrostatic capacity type displacement gage

Info

Publication number
JPS58155302A
JPS58155302A JP57039149A JP3914982A JPS58155302A JP S58155302 A JPS58155302 A JP S58155302A JP 57039149 A JP57039149 A JP 57039149A JP 3914982 A JP3914982 A JP 3914982A JP S58155302 A JPS58155302 A JP S58155302A
Authority
JP
Japan
Prior art keywords
amplifier
voltage
electrode
capacitance
measured
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.)
Pending
Application number
JP57039149A
Other languages
Japanese (ja)
Inventor
Yukio Nakamori
中森 幸雄
Shinichi Kamimura
真一 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.)
Nippon Steel Corp
Original Assignee
Nippon Steel 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 Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP57039149A priority Critical patent/JPS58155302A/en
Publication of JPS58155302A publication Critical patent/JPS58155302A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To measure the vibration and displacement of a body highly sensitively and a highly accurately, by constituting the system so that an input voltage to a detecting end becomes large. CONSTITUTION:The AC voltage outputted from an AC oscillator 8 is amplified by a booster circuit 9 and supplied to one of electrode plates P of the detecting end. The AD signal outputted from an amplifier 2 is converted into a DC by a full wave linear detector circuit 4. The effect of a temperature drift is eliminated by a temperature compensating circuit 5. The DC signal outputted from the detector circuit 4 is smoothed by an amplfier 6, and the electric signal corresponding to a distance (d) between the electrode P and an object to be measured is outputted. The voltage, which is approximately equal to the output voltage from the amplifier 6, is outputted from a reference voltage generator 10. The output voltage from the amplifier 6 and the output voltage from the reference voltage generator 10 are compared in a differential amplifier 7 and amplified. The infinitesimal change in the distance (d) between the electrode plate P and the object to be measured is amplified by the differential amplifier 7, and the output voltage proportional to the amount of change is obtained.

Description

【発明の詳細な説明】 この発明は、測定対象の振動や変位を2つの電極間の静
電容量変化によって測定する静電容量式変位計に関する
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a capacitive displacement meter that measures vibration or displacement of an object to be measured by a change in capacitance between two electrodes.

従来、非接触で物体の微小変位を測定する手段として渦
電流式、光学式(レーザ)、静電容量式等がある。渦電
流方式は、測定原理から、対象が導電性物体に限られ、
測定距離も実用的には100■以下である。光学式(レ
ーザ)は、測長に対しては自由度があ夛精度も高いが、
高価であ夛しか本凹凸面に対しては測定が困難である。
Conventionally, there are eddy current type, optical type (laser), capacitance type, etc. as means for measuring minute displacements of objects without contact. Due to the measurement principle, the eddy current method is limited to conductive objects;
The measurement distance is also practically 100 square meters or less. The optical method (laser) has a high degree of freedom and high precision for length measurement, but
It is expensive and difficult to measure on irregular surfaces.

静電容量変化と距離変化との対応関係を利用して測定対
象と検出端間の距離を測定し、物体の振動や変位を測定
する手段に容量式変位針がある。第1図に(a)、(b
)その原理を示す。
A capacitive displacement needle is a means for measuring the vibration or displacement of an object by measuring the distance between the object to be measured and the detection end using the correspondence between changes in capacitance and changes in distance. Figure 1 shows (a) and (b).
) to show its principle.

第1図(&)に示す計測システムにおいては、2枚の電
極板を間隔を置いて配置し、これらの電極板間の間隔と
静電容量の関係を利用するものである。
In the measurement system shown in FIG. 1(&), two electrode plates are arranged with a gap between them, and the relationship between the gap between these electrode plates and the capacitance is utilized.

2枚の電極板間の間隔をd1電極板の表面積をS1電極
板間における誘電率をεとすると、電極板間の静電容量
Cは、 で与えられる。従って、Cの変化からdを知ることがで
きる。
When the distance between the two electrode plates is d1, the surface area of the electrode plate is S1, and the dielectric constant between the electrode plates is ε, the capacitance C between the electrode plates is given by: Therefore, d can be known from the change in C.

第1図(b)に示すのは、2つの固定電極板Pt*Pm
を対向して配設しておき、この固定電極板Pl*Ptと
1つの極板Mで2つの静電容量OH# Cgを形作りて
いる。固定電極板Px、Pm間の中央位置に極板−が存
在するときの極板Mと電極板PIe hそれぞれとの間
隔をdとすると、極板Mが電極板P1或いはPaの面に
垂直な方向にXだけ変位すると、2つの静電容量CI、
C雪は、 で与えられ、C1とCmの差によって極板Mの変位量X
を知ることができる。このような原理を応用した容量式
変位針として特開昭52−110655号、特開昭54
−152562号、%開F1854−41764号、た
技術がある。
FIG. 1(b) shows two fixed electrode plates Pt*Pm
These fixed electrode plates Pl*Pt and one electrode plate M form two capacitances OH# Cg. If the distance between the electrode plate M and the electrode plate PIe h is d when the electrode plate - exists at the center position between the fixed electrode plates Px and Pm, then the electrode plate M is perpendicular to the plane of the electrode plate P1 or Pa. When displaced by X in the direction, two capacitances CI,
C snow is given by
can be known. As a capacitive displacement needle applying such a principle, Japanese Patent Application Laid-open Nos. 110655/1982 and 1983
There are techniques such as No.-152562 and No. F1854-41764.

しかしながら、これら先行技術は、静電容量式変位針に
おける問題点である。(1)各電極と大地との間の浮遊
容量の問題、(乃各電極と、測定器までの配線の長さに
対応する大地との間の浮遊容量の影響と、配線における
分布容量の問題、及び(3)測定対象に対する浮遊容量
の有無の問題を解決したものではなくたとえば、何れか
一方の電極が大地接地している場合には、電圧変換器の
バランスが崩れ測定不可能になる。
However, these prior art techniques have problems with capacitive displacement needles. (1) The problem of stray capacitance between each electrode and the ground (The effect of stray capacitance between each electrode and the ground corresponding to the length of the wiring to the measuring device, and the problem of distributed capacitance in the wiring) , and (3) does not solve the problem of the presence or absence of stray capacitance to the measurement target. For example, if either electrode is grounded, the voltage converter will be unbalanced and measurement will be impossible.

発明者等は、上に述べた、先行技術における問題点を解
決した静電容量式変位計を、既に特願昭56−6659
7号にて提案した。この技術は、測定対象に対向して一
対の電極板を設け、各々の電極板を、大地接地されたシ
ールドケースでWI繞し電極板の1つに交流発振器から
交流を供給し、他方の電極板と測定対象間の靜電容iを
電圧に変換するチャージ増幅器と電圧を増幅する増幅器
に出力し、これを線屋化する変換器からなる回路に出方
して信号どして取り出すシステムである。
The inventors have already proposed a capacitive displacement meter that solved the problems in the prior art described above in patent application No. 56-6659.
This was proposed in issue 7. This technology involves installing a pair of electrode plates facing the measurement target, surrounding each electrode plate with a grounded shield case, supplying alternating current from an AC oscillator to one of the electrode plates, and supplying alternating current to the other electrode plate. It is a system that outputs the static capacitance i between the board and the object to be measured to a voltage to a charge amplifier and an amplifier to amplify the voltage, and then outputs it to a circuit consisting of a converter that converts it into a line and outputs it as a signal. .

本発明者等は、この静電容量式変位計測システムはさら
に改良を加え、高感度、高精度で物体の変位、振動等を
計測できるシステムを発明したものである。その特徴と
する処は、測定対象に対向して一対の電極板を設けると
ともに、各々の電極板を囲繞するシールドケースを設は
該シールドケースを導線によって接地しさらに、前記電
極板の一方に交流電流を供給する交流発振器をブースタ
回路を介して設け、他方の電極板と測定対象間の静電容
量を電圧に変換するチャージ増幅器と電圧増幅器とから
構成される増幅器とを設けてなる点にある。以下に、こ
の発明の詳細な説明する。
The present inventors further improved this capacitive displacement measurement system and invented a system that can measure the displacement, vibration, etc. of an object with high sensitivity and precision. Its features include a pair of electrode plates facing the object to be measured, a shield case surrounding each electrode plate, the shield case being grounded by a conductor, and an alternating current connected to one of the electrode plates. An AC oscillator that supplies current is provided via a booster circuit, and an amplifier consisting of a charge amplifier and a voltage amplifier that converts the capacitance between the other electrode plate and the object to be measured into voltage is provided. . The present invention will be explained in detail below.

発明者等が、特願昭56−66597号にて提案した計
測システムにおいて、チャージ増幅器1の人。
In the measurement system proposed by the inventors in Japanese Patent Application No. 56-66597, charge amplifier 1 is used.

出力の関係は、 し! で示される。ここに1 V・;第2図における、a点の出力電圧Vi;第2図に
おける、b点の入力電圧、Cf;チャージ増幅器1内の
帰還容量、Cx;測定の対象とする静電容量、つまシミ
極板と測定対象との間隔の大きさに対応する静電容量。
The relationship between the outputs is as follows! It is indicated by. Here, 1 V: output voltage at point a in FIG. 2; input voltage at point b in FIG. 2; Cf: feedback capacitance in charge amplifier 1; Cx: capacitance to be measured; Capacitance that corresponds to the distance between the tab stain electrode plate and the object to be measured.

チャージ増幅器からの出力電圧りの大きさは、電極板と
測定対象間における静電容量Cxの大きさ、入力電圧V
tの大きさおよびチャージ増幅器における帰還容量Cf
によって定まる。従って、静電容量を利用した、物体の
振動、変位の計測システムにめって、回路的にチャージ
増幅器の出力を大きくするためには、入力電圧Viを大
きくすること、ならびにチャージ増幅器における帰還容
量Cfを小さくすることが有効である。
The magnitude of the output voltage from the charge amplifier is determined by the magnitude of the capacitance Cx between the electrode plate and the object to be measured, and the input voltage V.
The size of t and the feedback capacitance Cf in the charge amplifier
Determined by Therefore, in order to increase the output of the charge amplifier in terms of the circuit for a measurement system of vibration and displacement of an object using capacitance, it is necessary to increase the input voltage Vi and to increase the feedback capacitance in the charge amplifier. It is effective to reduce Cf.

そこで、本発明においては検出端への入力電圧V1を大
きくするようシステムを構成した。第2図にこの発明に
なる物体の振動、変位計測システムを示す。第2図にお
いて、1繻才、ヤージ増幅器、であp1電極板P、!:
測定対象間における静電容量Cxを電圧に変換する。2
#i増幅器であり、チヤージ増幅器1からの出力電圧を
増幅する。3は、フィルタであシ、検出器11に印加さ
れた周波数を選択的に取シ出し、計測システムにおける
S/Nを向上させる。4は、余波直線検波回路であり、
フィルタ3から出力される交流を直流に変換する。
Therefore, in the present invention, the system is configured to increase the input voltage V1 to the detection terminal. FIG. 2 shows a system for measuring vibration and displacement of an object according to the present invention. In Fig. 2, the p1 electrode plate P,! :
The capacitance Cx between the objects to be measured is converted into voltage. 2
#i amplifier, which amplifies the output voltage from charge amplifier 1. 3 uses a filter to selectively extract the frequency applied to the detector 11 to improve the S/N in the measurement system. 4 is an aftereffect linear detection circuit,
The alternating current output from the filter 3 is converted into direct current.

全波直線検波回路4は温度補償回路5を内蔵しておシ、
全波直線検波回路4中の検波用ダイオードに生起する温
度ドリフトを消去すべく機能し、計測システムの測定′
!l!度低下全低下する。測定精度が±a1閣の場合、
4IK温度ドリフトの影響はないが、測定精度が±5s
rm@変の水準になると温度ドリフトの影響が顕在化し
てくる。温度ドリフトの影響を生起せしめない手段とし
て回路全体をオープン回路に収める方法もあるけれども
、この発明においては、安価で、しかも回路定数の決定
が簡単なサーミス漣と抵抗を使った回路によって温度ド
リフトの影響を消去するようにした。
The full-wave linear detection circuit 4 has a built-in temperature compensation circuit 5.
It functions to eliminate the temperature drift that occurs in the detection diode in the full-wave linear detection circuit 4, and the measurement system's measurement
! l! The degree decreases completely. If the measurement accuracy is ±a1,
There is no effect of 4IK temperature drift, but the measurement accuracy is ±5s.
At the level of rm@change, the influence of temperature drift becomes apparent. Although there is a method of keeping the entire circuit in an open circuit as a means to prevent the effects of temperature drift from occurring, in this invention, temperature drift can be avoided by using a circuit using a thermistor resistor and a resistor, which are inexpensive and whose circuit constants are easy to determine. The effect was removed.

また6は、増幅器であ〕、全線直線検波回路4からの出
力信号の平滑化と、測定距離に比例した電気信号を出力
する。7社、差動増幅器であシ、増幅器6からの出力電
圧と、基準電圧発生器10からの出力電圧を比較して、
増幅する。これによって、測定対象と検出端(電極P)
の間の微小な距離変化の検出も可能になる。8は、交流
発振器、9はブースタ回路であって、交流発振器8から
の出力電圧を増幅(外圧)して、検出器11における電
極板(P)の一方に供給する。11Fi、検出器であっ
て、電極板(P)および電極板(P)の各々を囲繞する
、大地接地されたシールドケース(S)とからなってい
る。第2図においてdは、電極板(P)と測定対象間の
距離である。
Further, 6 is an amplifier which smoothes the output signal from the full-line linear detection circuit 4 and outputs an electric signal proportional to the measurement distance. 7 companies used differential amplifiers, compared the output voltage from the amplifier 6 and the output voltage from the reference voltage generator 10,
Amplify. This allows the measurement target and the detection end (electrode P) to
It is also possible to detect minute changes in distance between the two. 8 is an AC oscillator, and 9 is a booster circuit, which amplifies (external pressure) the output voltage from the AC oscillator 8 and supplies it to one of the electrode plates (P) in the detector 11. 11Fi, the detector is composed of an electrode plate (P) and a grounded shield case (S) surrounding each of the electrode plates (P). In FIG. 2, d is the distance between the electrode plate (P) and the object to be measured.

次に、上に述べた如く構成し友、この発明になる静電容
量式変位針の作用を説明する。交流発振器8から出力さ
れる交流電流はブースタ回路9によってその電圧を増幅
され検出端11の電極板(P)の一方に供給される。他
方の電停板(P)と測定対象間の距離dK対応する静電
容量Cxはチャージ増幅器1で電圧に変換され、次いで
増幅器2で増幅される。一対の電極[(P)はシールド
ケースC8>でそれぞれ囲繞されているから各電極と大
地との間の浮遊容量の影響は消去される。さらにチャー
ジ増幅器で静電容量Cxは電圧に変換され信号として取
扱われるから各電極と信号として取出すまでの配線の長
さに対応する大地との間の浮遊容量の影響も消去される
。前記各事項により測定対象に対する浮遊容量の有無の
問題もなくなる。増幅器2から出力される交流信号は、
全波直線検波回路4によって直流に変換されるとともに
、温度補償回路5によって温度ドリフトの影響も消去さ
れる。
Next, the operation of the capacitive displacement needle according to the present invention constructed as described above will be explained. The voltage of the alternating current output from the alternating current oscillator 8 is amplified by the booster circuit 9 and then supplied to one of the electrode plates (P) of the detection end 11 . The capacitance Cx corresponding to the distance dK between the other stop plate (P) and the object to be measured is converted into a voltage by the charge amplifier 1, and then amplified by the amplifier 2. Since the pair of electrodes [(P) are each surrounded by a shield case C8>, the influence of stray capacitance between each electrode and the ground is eliminated. Furthermore, since the capacitance Cx is converted into a voltage by the charge amplifier and treated as a signal, the influence of stray capacitance between each electrode and the ground corresponding to the length of the wiring until it is taken out as a signal is also eliminated. The above-mentioned items eliminate the problem of the presence or absence of stray capacitance to the measurement target. The AC signal output from amplifier 2 is
The full-wave linear detection circuit 4 converts the current into direct current, and the temperature compensation circuit 5 eliminates the influence of temperature drift.

全波直線検波回路4から出力される直流信号は、増幅器
6によって平滑され、電極(P)と測定対象間の距11
i1 (d)に対応し九電気信号を出力する。基準電圧
発生器10からは増幅器6からの出力電圧にはt1i′
等しい電圧が出力され差動増幅器7によって、増幅器6
からの出力電圧と基準電圧発生器10からの出力電圧が
比較され増幅される。
The DC signal output from the full-wave linear detection circuit 4 is smoothed by an amplifier 6, and the distance 11 between the electrode (P) and the measurement object is
It outputs nine electric signals corresponding to i1 (d). From the reference voltage generator 10, the output voltage from the amplifier 6 is t1i'.
Equal voltages are outputted by the differential amplifier 7, and the amplifier 6
The output voltage from the reference voltage generator 10 is compared and amplified.

今、電極板(P)と掬定対象間の距離dが微小変化すれ
ば、増幅器6の出力電圧41微小変化する。
Now, if the distance d between the electrode plate (P) and the scooped object changes slightly, the output voltage 41 of the amplifier 6 changes slightly.

この微小変化分は、差動増幅器7で増幅され、変化量に
比例し九出力電圧が得られる。このようにすることによ
って、dのμmオーダの微小変化が検出できる。この発
明による計測システAKよれば一般的なコンデンサの容
量も高精度で測定でき、0.019Fの測定が可能であ
る。
This minute change is amplified by the differential amplifier 7, and nine output voltages are obtained in proportion to the amount of change. By doing so, minute changes in d on the order of μm can be detected. According to the measurement system AK according to the present invention, the capacitance of a general capacitor can be measured with high precision, and measurement of 0.019F is possible.

この発明は、以上述べたように構成しかつ作用せしめる
ようにしたから、物体の振動、変位を高感度、高精度下
に測定することができる。
Since the present invention is configured and operated as described above, it is possible to measure the vibration and displacement of an object with high sensitivity and high accuracy.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は容量式変位針の原理説明図、第2図はこの発明
になる静電容量式変位計の回路図である。 1:チャージ増幅器、2:増幅器、5:フィルター、4
:全波直線検波回路、5:i1度補償回路、6:増幅器
、7:差動増幅器、8:交流発振器、9:ブースタ回路
、10:DC基準電圧発生器、11:検出器。 出願人 新日本製鐵株式会社
FIG. 1 is an explanatory diagram of the principle of a capacitive displacement needle, and FIG. 2 is a circuit diagram of a capacitive displacement meter according to the present invention. 1: Charge amplifier, 2: Amplifier, 5: Filter, 4
: full wave linear detection circuit, 5: i1 degree compensation circuit, 6: amplifier, 7: differential amplifier, 8: AC oscillator, 9: booster circuit, 10: DC reference voltage generator, 11: detector. Applicant Nippon Steel Corporation

Claims (2)

【特許請求の範囲】[Claims] (1)測定対象に対向して一対の電極板を設けるととも
に、各々の電極板を囲繞するシールドケースを設は該シ
ールドケースを導線によって接地しさらに、前記電極板
の一方に交流電流を供給する交流発振器をブースタ回路
を介して設け、他方の4M板と測定対象間の静電容量を
電圧に変換するチャージ増幅器と電圧増幅器とから構成
される増幅器とを設けてなる静電容量変位針。
(1) A pair of electrode plates is provided facing the measurement target, a shield case is provided surrounding each electrode plate, the shield case is grounded by a conductor, and an alternating current is supplied to one of the electrode plates. A capacitance displacement needle provided with an AC oscillator via a booster circuit, and an amplifier composed of a charge amplifier and a voltage amplifier that convert the capacitance between the other 4M board and the object to be measured into voltage.
(2)測定対象に対向して一対の電極板を設けるととも
に各々の電極板を囲繞するシールドケースを設は該シー
ルドケースを導線によって接地しさらに、前記電極板の
一方に交流電流を供給する交流発振器をブースタ回路を
介して設け、また他方の電極板と測定対象間の静電容量
を電圧に変換するチャージ増幅器と電圧増幅器とからな
る増幅器を設けさらに温度補償回路を含む全波直線検波
回路を設けてなる静電容量式変位計。
(2) A pair of electrode plates is provided facing the measurement target, and a shield case surrounding each electrode plate is provided.The shield case is grounded by a conductor, and an alternating current is supplied to one of the electrode plates. An oscillator is provided via a booster circuit, and an amplifier consisting of a charge amplifier and a voltage amplifier that converts the capacitance between the other electrode plate and the object to be measured into voltage is provided, and a full-wave linear detection circuit including a temperature compensation circuit is provided. A capacitive displacement meter is provided.
JP57039149A 1982-03-12 1982-03-12 Electrostatic capacity type displacement gage Pending JPS58155302A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57039149A JPS58155302A (en) 1982-03-12 1982-03-12 Electrostatic capacity type displacement gage

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57039149A JPS58155302A (en) 1982-03-12 1982-03-12 Electrostatic capacity type displacement gage

Publications (1)

Publication Number Publication Date
JPS58155302A true JPS58155302A (en) 1983-09-16

Family

ID=12545046

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57039149A Pending JPS58155302A (en) 1982-03-12 1982-03-12 Electrostatic capacity type displacement gage

Country Status (1)

Country Link
JP (1) JPS58155302A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007127615A (en) * 2005-10-05 2007-05-24 Yosoji Tanji Capacitance level sensor
KR101083070B1 (en) 2010-02-11 2011-11-16 (주)케이엠비앤센서 Control apparatus for improving non-linear characteristic of an electric capacity displacement sensor
CN111693111A (en) * 2020-05-27 2020-09-22 佛山市川东磁电股份有限公司 Compensation method and compensation circuit of non-contact sensor

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4826169A (en) * 1971-08-09 1973-04-05

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4826169A (en) * 1971-08-09 1973-04-05

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007127615A (en) * 2005-10-05 2007-05-24 Yosoji Tanji Capacitance level sensor
KR101083070B1 (en) 2010-02-11 2011-11-16 (주)케이엠비앤센서 Control apparatus for improving non-linear characteristic of an electric capacity displacement sensor
CN111693111A (en) * 2020-05-27 2020-09-22 佛山市川东磁电股份有限公司 Compensation method and compensation circuit of non-contact sensor

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