JPS626164B2 - - Google Patents

Info

Publication number
JPS626164B2
JPS626164B2 JP56106373A JP10637381A JPS626164B2 JP S626164 B2 JPS626164 B2 JP S626164B2 JP 56106373 A JP56106373 A JP 56106373A JP 10637381 A JP10637381 A JP 10637381A JP S626164 B2 JPS626164 B2 JP S626164B2
Authority
JP
Japan
Prior art keywords
electrode plates
amplifier
plate
electrode
displacement meter
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
Application number
JP56106373A
Other languages
Japanese (ja)
Other versions
JPS587503A (en
Inventor
Yukio Nakamori
Toshimi Washitani
Shinichi Kamimura
Hiroshi Soga
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 JP56106373A priority Critical patent/JPS587503A/en
Publication of JPS587503A publication Critical patent/JPS587503A/en
Publication of JPS626164B2 publication Critical patent/JPS626164B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B7/00Measuring arrangements characterised by the use of electric or magnetic techniques
    • G01B7/02Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness
    • G01B7/023Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness for measuring distance between sensor and object

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)

Description

【発明の詳細な説明】 本発明は、静電容量式変位計に関するものであ
り、先に提案した変位計の改良を図るものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a capacitive displacement meter, and is intended to improve the previously proposed displacement meter.

静電容量式変位計の基本的な測定原理を第1図
に示す。電極板の面積をs、電極板間隔をd、誘
電率をεとすれば、静電容量CはC=(ε・
s)/dとなる。この基本原理を利用した静電容
量式変位計としては公開特許公報昭54−41764、
昭53−107354、昭52−110655があるが、次に述べ
る欠点を有する。(1)測定距離が小さい。せいぜい
最大10mm位である。(2)検出器から増幅器等までの
配線距離が最大5m位である。(3)配線と大地間の
浮遊容量の影響を受ける。(4)被測定物体が高温の
場合には測定できない。
Figure 1 shows the basic measurement principle of a capacitive displacement meter. If the area of the electrode plate is s, the electrode plate spacing is d, and the dielectric constant is ε, then the capacitance C is C=(ε・
s)/d. As a capacitive displacement meter using this basic principle, published patent publication No. 54-41764,
There are 107354 (1983) and 110655 (1982), but they have the following drawbacks. (1) Measurement distance is small. At most, it is about 10mm. (2) The maximum wiring distance from the detector to the amplifier, etc. is approximately 5 m. (3) Affected by stray capacitance between wiring and ground. (4) Measurement cannot be performed if the object to be measured is at high temperature.

これらの欠点を解決する第2図に示す如き静電
容量式変位計を本発明者は先に提案した。本発明
はこの方式の改良に係るものである。第2図に示
す如く、静電容量式変位計は検出器5、高周波発
振器10、チヤージ増幅器11、フイルター1
2、検波増幅器13、リニアライザー14から構
成されている。検出器5は、2板の電極板1,2
とシールドケース3、および電極板間のシールド
板4から構成され、被測定物体20に対して電極
板1,2は対向して配置されている。
The present inventor previously proposed a capacitive displacement meter as shown in FIG. 2 which solves these drawbacks. The present invention relates to an improvement of this method. As shown in FIG. 2, the capacitive displacement meter includes a detector 5, a high frequency oscillator 10, a charge amplifier 11, and a filter 1.
2, a detection amplifier 13, and a linearizer 14. The detector 5 has two electrode plates 1 and 2.
It is composed of a shield case 3, a shield plate 4 between electrode plates, and the electrode plates 1 and 2 are arranged to face the object to be measured 20.

検出器5の電極板1はチヤージ増幅器11に接
続され、電極板2は高周波発振器10に接続され
ている。シールドケース3,4は接地されてい
る。高周波発振器10から供給される一定周波数
の正弦波、三角波、またはパルス高周波電流は、
電極板2より電極板1に供給される。高周波電流
の大きさは、検出器5と被測定物体間の距離lに
ほぼ比例する。勿論、電極板の面積にも比例する
ことは云うまでもない。この高周波電流の大きさ
は電荷量としてチヤージ増幅器11で検出され、
増幅される。増幅された信号はフイルター12に
て雑音を除去し、検波増幅器13にて増幅、整流
して直流に変換する。更にリニアライザー14に
て測定距離lに対して比例した出力電圧/電流を
得ている。この静電容量式変位計において測定距
離や測定感度の調整において電極板1,2とシー
ルドケース3,4との間隔Δlが重要であること
を先に提案した。
The electrode plate 1 of the detector 5 is connected to a charge amplifier 11, and the electrode plate 2 is connected to a high frequency oscillator 10. Shield cases 3 and 4 are grounded. The constant frequency sine wave, triangular wave, or pulsed high frequency current supplied from the high frequency oscillator 10 is
It is supplied from electrode plate 2 to electrode plate 1 . The magnitude of the high frequency current is approximately proportional to the distance l between the detector 5 and the object to be measured. Of course, it goes without saying that it is also proportional to the area of the electrode plate. The magnitude of this high frequency current is detected as the amount of charge by the charge amplifier 11,
amplified. A filter 12 removes noise from the amplified signal, and a detection amplifier 13 amplifies and rectifies the signal to convert it into direct current. Furthermore, the linearizer 14 obtains an output voltage/current proportional to the measurement distance l. It was previously proposed that the distance Δl between the electrode plates 1, 2 and the shield cases 3, 4 is important in adjusting the measurement distance and measurement sensitivity in this capacitive displacement meter.

本発明は検出器5の改良に関するものである。
第3図に電極板間のシールド板4を取り除いた場
合の検出器5の構造を示す。第6図にシールド板
4の有無における距離特性を示す。第6図の曲線
aはシールド板4が有るときの特性(第2図の検
出器)、第6図の曲線bはシールド板4無しの特
性を示すものである。なお距離特性は検波増幅器
13の出力である。シールド板4の有無により測
定距離と感度を変更できる。第4図はシールド板
4を第2図のシールド板より長さDだけ短かくし
た検出器5の構造を示す。
The present invention relates to an improvement of the detector 5.
FIG. 3 shows the structure of the detector 5 when the shield plate 4 between the electrode plates is removed. FIG. 6 shows the distance characteristics with and without the shield plate 4. Curve a in FIG. 6 shows the characteristics with the shield plate 4 (detector in FIG. 2), and curve b in FIG. 6 shows the characteristics without the shield plate 4. Note that the distance characteristic is the output of the detection amplifier 13. The measurement distance and sensitivity can be changed depending on the presence or absence of the shield plate 4. FIG. 4 shows the structure of a detector 5 in which the shield plate 4 is made shorter by a length D than the shield plate shown in FIG.

第4図の検出器の距離特性は、第6図の曲線c
の特性となる。第5図はシールド板4を三角形状
に取り除いた場合の検出器5の構造を示すもので
あるが、この形状においても距離特性と感度を改
善することが出来る。
The distance characteristic of the detector in Fig. 4 is the curve c in Fig. 6.
It is a characteristic of FIG. 5 shows the structure of the detector 5 when the shield plate 4 is removed in a triangular shape, and even with this shape, the distance characteristics and sensitivity can be improved.

即ち電極板1,2の面積Sと電極板の厚みLを
一定とすれば、シールドケース3内の電極板1,
2間に生じる静電容量をシールド板4にて制御す
ることにより距離特性と感度を改善することが出
来る。距離特性と感度の決定において電極板1,
2の面積Sが支配的であることは云うまでもな
い。また電極板1,2の厚みLによつても距離特
性と感度の改良も多少有効である。
That is, if the area S of the electrode plates 1 and 2 and the thickness L of the electrode plates are constant, the electrode plates 1 and 2 in the shield case 3
By controlling the capacitance generated between the two using the shield plate 4, distance characteristics and sensitivity can be improved. In determining distance characteristics and sensitivity, electrode plate 1,
It goes without saying that the area S of 2 is dominant. Furthermore, it is also somewhat effective to improve the distance characteristics and sensitivity by changing the thickness L of the electrode plates 1 and 2.

上に述べたように、対象の変位を測定するとき
の距離特性と感度の最適領域を決定するときの操
作パラメータとして電極板間をシールドしている
金属板の面積を採ることができる。電極板間のシ
ールド板の面積を変化させる手段の1つとして、
離散的にこれを行なう場合は第5図に示す手段が
ある。
As described above, the area of the metal plate shielding between the electrode plates can be taken as an operating parameter when determining the optimal range of distance characteristics and sensitivity when measuring the displacement of an object. As one means of changing the area of the shield plate between the electrode plates,
When this is done discretely, there is a means shown in FIG.

前記シールド板の面積を変化させるに際しこれ
を連続的に行なおうとする場合は、例えばシール
ド板を昇降自在に構成して第4図aに示すDの値
を連続的に変化させる。シールド板の昇降手段と
しては公知のねじ機構、流体圧機構が利用でき
る。
If the area of the shield plate is to be changed continuously, the value of D shown in FIG. 4a is continuously changed by, for example, making the shield plate movable up and down. A known screw mechanism or fluid pressure mechanism can be used as a means for raising and lowering the shield plate.

感度の改良において、第2図に示す如く、電極
板2に高周波発振器10から供給する高周波電
流/電圧は正弦波よりもパルスの方が、感度がよ
い。
In improving the sensitivity, as shown in FIG. 2, the sensitivity is better when the high frequency current/voltage supplied from the high frequency oscillator 10 to the electrode plate 2 is a pulse rather than a sine wave.

そしてそのときの波形は、矩形波の方が感度を
高める上ですぐれている。
As for the waveform at that time, a rectangular wave is better in increasing sensitivity.

以上、述べた如く、本発明はシールド板4の形
状により、距離特性や感度を改善することが出来
る。また高周波パルス発振信号において感度の向
上が出来る。
As described above, the present invention can improve distance characteristics and sensitivity by changing the shape of the shield plate 4. Furthermore, sensitivity can be improved in high frequency pulse oscillation signals.

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

第1図は静電容量式変位計の基本原理を示す等
価回路図であり、第2図は先に提案した静電容量
式変位計の構成を示すブロツク図であり、第3、
第4、第5図は本発明の検出器を示す図でaは断
面図、bは底面図、第5図のcは側面図であり、
第6図は距離特性を示す図表である。 1:電極板、2:電極板、3:シールドケー
ス、4:シールド板、5:検出器、10:高周波
発振器、11:チヤージ増幅器、12:フイルタ
ー、13:検波増幅器、14:リニアライザー、
15:アース、20:被測定物体。
Figure 1 is an equivalent circuit diagram showing the basic principle of a capacitance type displacement meter, Figure 2 is a block diagram showing the configuration of the capacitance type displacement meter proposed earlier, and Figure 3.
4 and 5 are diagrams showing the detector of the present invention, in which a is a cross-sectional view, b is a bottom view, and c in FIG. 5 is a side view,
FIG. 6 is a chart showing distance characteristics. 1: Electrode plate, 2: Electrode plate, 3: Shield case, 4: Shield plate, 5: Detector, 10: High frequency oscillator, 11: Charge amplifier, 12: Filter, 13: Detection amplifier, 14: Linearizer,
15: Earth, 20: Object to be measured.

Claims (1)

【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
を設け、該シールドケースを導線によつて接地し
さらに、前記電極板の一方に交流電流を供給する
交流発振器と、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ヤージ増幅器と電圧増幅
器とから構成される増幅器と、該増幅器からの出
力を線型化する変換器とを設けた静電容量式変位
計において、前記一対の電極板間に設けたシール
ド板の面積を、変位を測定しようとする距離範囲
と所要検出感度に応じて離散的に或は連続的に変
更せしめる如く構成してなる容量式変位計。
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. An AC oscillator, an amplifier consisting of a charge amplifier and a voltage amplifier that convert the capacitance between the other electrode plate and the object to be measured into voltage, and a converter that linearizes the output from the amplifier. In the capacitive displacement meter, the area of the shield plate provided between the pair of electrode plates is configured to be changed discretely or continuously depending on the distance range in which displacement is to be measured and the required detection sensitivity. Capacitive displacement meter.
JP56106373A 1981-07-08 1981-07-08 Capacity type displacement gage Granted JPS587503A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56106373A JPS587503A (en) 1981-07-08 1981-07-08 Capacity type displacement gage

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56106373A JPS587503A (en) 1981-07-08 1981-07-08 Capacity type displacement gage

Publications (2)

Publication Number Publication Date
JPS587503A JPS587503A (en) 1983-01-17
JPS626164B2 true JPS626164B2 (en) 1987-02-09

Family

ID=14431912

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56106373A Granted JPS587503A (en) 1981-07-08 1981-07-08 Capacity type displacement gage

Country Status (1)

Country Link
JP (1) JPS587503A (en)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63115706U (en) * 1987-01-23 1988-07-26
JPS6444425U (en) * 1987-09-10 1989-03-16
JP2748863B2 (en) * 1994-07-05 1998-05-13 日本電気株式会社 IC package evaluation system
JP2000028309A (en) * 1996-09-06 2000-01-28 Yashima Engineering Kk Capacitance sensor
US6476620B2 (en) 1996-09-06 2002-11-05 Ks Techno Co., Ltd. Electrostatic capacity sensor
JP2001035327A (en) * 1999-07-22 2001-02-09 Sumitomo Metal Ind Ltd Capacitance type proximity sensor
US6388452B1 (en) * 2000-04-20 2002-05-14 Hewlett-Packard Company Device for sensing media thickness using capacitance measurements
CN101029883B (en) 2001-09-04 2010-06-16 株式会社阿尔宝 Capacitive coupling type sensor device

Also Published As

Publication number Publication date
JPS587503A (en) 1983-01-17

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