JPS61212737A - Power detector - Google Patents
Power detectorInfo
- Publication number
- JPS61212737A JPS61212737A JP5364385A JP5364385A JPS61212737A JP S61212737 A JPS61212737 A JP S61212737A JP 5364385 A JP5364385 A JP 5364385A JP 5364385 A JP5364385 A JP 5364385A JP S61212737 A JPS61212737 A JP S61212737A
- Authority
- JP
- Japan
- Prior art keywords
- force detection
- density
- crystal resonator
- frequency
- resonance frequency
- 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
Links
- 238000001514 detection method Methods 0.000 claims abstract description 35
- 239000013078 crystal Substances 0.000 claims abstract description 23
- 230000005284 excitation Effects 0.000 claims description 13
- 238000012937 correction Methods 0.000 claims description 4
- 239000003990 capacitor Substances 0.000 abstract description 2
- 238000010276 construction Methods 0.000 abstract 2
- 238000010586 diagram Methods 0.000 description 5
- 230000035945 sensitivity Effects 0.000 description 3
- 238000003384 imaging method Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L1/00—Measuring force or stress, in general
- G01L1/16—Measuring force or stress, in general using properties of piezoelectric devices
- G01L1/162—Measuring force or stress, in general using properties of piezoelectric devices using piezoelectric resonators
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Abstract
Description
【発明の詳細な説明】
〈発明の利用分野〉
本発明は、測定すべき力に対応した周波数信号を出力す
る力検出装置に関し、密度補正をはかった力検出装置に
関する。DETAILED DESCRIPTION OF THE INVENTION Field of Application of the Invention The present invention relates to a force detection device that outputs a frequency signal corresponding to a force to be measured, and more particularly to a force detection device that performs density correction.
〈従来の技術〉
第4図は、従来公知のこの種の装置の一例を示す構成説
明図で、特開昭56−79221号公報に記載されてい
る。この装置は、測定圧力(力)を受けるダイアフラム
1と、一端が筐体2の内甲に、他端がダイアフラム1に
固着された平板状力検出振動子3と、この平板状力検出
振動子3の固有振動数を検出する信号処理手段4とで構
成されている。この様な構成の装置によれば圧力感度が
高く、又圧力に対応した信号をコンピュータとの整合性
のよいディジタル信号で得ることができる。<Prior Art> FIG. 4 is a configuration explanatory diagram showing an example of a conventionally known device of this type, which is described in Japanese Patent Laid-Open No. 56-79221. This device includes a diaphragm 1 that receives measurement pressure (force), a flat force detection vibrator 3 whose one end is fixed to the inner shell of a housing 2 and the other end to the diaphragm 1, and this flat force detection vibrator. The signal processing means 4 detects the natural frequency of 3. An apparatus having such a configuration has high pressure sensitivity and can obtain a signal corresponding to pressure as a digital signal that is highly compatible with a computer.
〈発明が解決しようとする問題点〉
ところでこのような力検出装置においては力検出振動子
の感度が高いので共振周波数が周囲気体の密度による影
響を受け、零点が変動するという問題がある。<Problems to be Solved by the Invention> However, in such a force detection device, since the sensitivity of the force detection vibrator is high, there is a problem that the resonance frequency is affected by the density of the surrounding gas, and the zero point fluctuates.
く問題点を解決するための手段〉
本発明は上記問題点に鑑みて成されたもので、周囲気体
の密度変化に伴う共振周波数の影響を補正した力検出装
置を提供することを目的とし、その構成状の特徴は、変
換すべき入力が軸方向に加えられる力検出振動子と、こ
の力検出振動子を固有振動数で共振させる第1の励振手
段J5よび前記力検出振動子の撮動を検出する信号処理
手段と、水晶振動子と、この水晶振動子を励振させる第
2の励振手段とを有し、前記水晶振動子の共振周波数を
前記信号処理手段に入力し、密度補正を行うようにした
ものである。Means for Solving the Problems> The present invention has been made in view of the above problems, and an object of the present invention is to provide a force detection device that corrects the influence of the resonance frequency due to changes in the density of surrounding gas. Its configuration is characterized by a force detection vibrator to which the input to be converted is applied in the axial direction, a first excitation means J5 that causes this force detection vibrator to resonate at its natural frequency, and an imaging device for the force detection vibrator. , a crystal resonator, and a second excitation means for exciting the crystal resonator, the resonant frequency of the crystal resonator is input to the signal processing means, and density correction is performed. This is how it was done.
ぐ作用〉
測定すべき力が加えられ、そのツノに対応した共振周波
数で振動している力検出装置は、この装置が配置された
周囲気体の密度により影響を受(プで共振周波数が変動
する。一方水晶振動子の共振周波数も変動するが、この
水晶振動子からの出力を力検出装置の信号処理回路に入
力し、密度変化に伴う共振周波数の変動を補正する
・ぐ実施例〉
第1図は本発明による力検出装置の一実施例を示すブロ
ック図である。When a force to be measured is applied to the force detection device, which vibrates at a resonant frequency corresponding to the horn, the force detection device is affected by the density of the surrounding gas in which the device is placed (the resonant frequency changes due to On the other hand, the resonant frequency of the crystal oscillator also fluctuates, but the output from this crystal oscillator is input to the signal processing circuit of the force detection device to correct the fluctuation of the resonant frequency due to the density change. Example 1 The figure is a block diagram showing one embodiment of a force detection device according to the present invention.
図において、17は第1の励振手段である。1Ω−は力
検出撮動子であり、2枚の゛ビーム状板11a、11b
が対称に平行して設けられ、結合部12により口字状に
形成され、フレクシャ13を介して支持部14に連結さ
れている。15a、15bは結合部の側面にそれぞれ取
付けられた圧電素子で、例えば15aは励振素子、15
bは振動の検出素子であり、それぞれの素子は外部に設
けられた増幅器16に接続されて第1の励振手段17が
構成されている。2oは第1の励振手段17からの出力
を処理する信号処理部である。21は第2の励振手段で
、水晶振動子22およびインバータ23.抵抗24.コ
ンデンサ25により構成され、この第2の励振手段21
からの出力は信号処理部20に入力される。なお、水晶
振動子22はフォトグラフィの技術により製作された司
法精度。In the figure, 17 is the first excitation means. 1Ω- is a force detection sensor, which consists of two beam-shaped plates 11a and 11b.
are provided symmetrically and in parallel, are formed into a mouth shape by the connecting portion 12, and are connected to the support portion 14 via a flexure 13. 15a and 15b are piezoelectric elements attached to the side surfaces of the joint, for example, 15a is an excitation element;
b is a vibration detection element, and each element is connected to an externally provided amplifier 16 to constitute a first excitation means 17. 2o is a signal processing section that processes the output from the first excitation means 17. 21 is a second excitation means, which includes a crystal resonator 22 and an inverter 23 . Resistance 24. This second excitation means 21 is constituted by a capacitor 25.
The output from is input to the signal processing section 20. The crystal oscillator 22 is manufactured with judicial precision using photography technology.
密度感度の揃った例えば時計用水晶音叉振動子が望まし
い。この様な水晶発振回路21はインバータ1個と水晶
m動子が1個あればよいので極めて安価である。For example, a crystal tuning fork vibrator for watches with uniform density sensitivity is desirable. Such a crystal oscillation circuit 21 is extremely inexpensive because it only requires one inverter and one crystal m-driver.
上記の構成による力検出振動子10の周囲気体密度を含
めた共振周波数は次式により求めることができる。The resonance frequency including the surrounding gas density of the force detection vibrator 10 having the above configuration can be determined by the following equation.
f m p = f m o / r丁]−1丁
・ (1)ここでfmo : 力検出撮動子の真空中
での共振周波数
A : 定数
又、水晶振動子の周囲気体密度を含めた共振周波数は次
式により求めることができる。f m p = f m o / r c] - 1 c)
(1) Here, fmo: Resonant frequency of the force detection sensor in vacuum A: Constant Also, the resonant frequency including the surrounding gas density of the crystal resonator can be determined by the following equation.
f Q D 7 f Q o / FrT■7− (2
>ここでfqo: 水晶振動子の真空中での共振周波
数
B : 定数
第2図は上記計算式および実験値により求めた密度に対
する共振周波数の変化率を示すものである。図によれば
、力検出振動子10の変化率は密度が2 m Q /
c m 3のときおよそ0.32%に対し、水晶振動子
22の変化率はおよそ0.03%であることがわかる。f Q D 7 f Q o / FrT■7- (2
>Here, fqo: Resonant frequency of the crystal resonator in vacuum B: Constant Figure 2 shows the rate of change of the resonant frequency with respect to the density determined by the above calculation formula and experimental values. According to the figure, the rate of change of the force detection vibrator 10 is such that the density is 2 m Q /
It can be seen that the rate of change of the crystal resonator 22 is approximately 0.03%, compared to approximately 0.32% when cm 3 .
(σ−1,2〜2.4mg/ c m ’は1気圧〜2
気圧に相当する)上記(2)式からその時点での密度は
次式により求めることが出来る。(σ-1,2~2.4mg/cm' is 1 atm~2
From the above equation (2) (corresponding to atmospheric pressure), the density at that point can be determined by the following equation.
ρ−1/B ((fQo /fqρM−1))・・・〈
3)
(3)式により求めたその時点での密度から次式により
補正ずべき力検出撮動子の周波数を求めることが出来る
。ρ-1/B ((fQo /fqρM-1))...<
3) The frequency of the power detection sensor to be corrected can be determined from the density at that point determined by the formula (3) using the following formula.
Δfm−fmo/r丁TW下’f m o ・” (4
)第3図は第1図に示す信号処理部20において、上記
各式に示す演算を行って力検出撮動子二工の密度に対す
る周波数変化率を補正した結果を、横軸を密度、縦軸を
周波数変化率として示すものである。図によれば密度変
化に対する周波数変化率が0.001%以下となり、水
晶振動子による補正を行うことにより、力検出撮動子の
みの場合に比較し周波数変化率が2桁以上改善されたこ
とがわかる。Δfm-fmo/r-TW bottom'f m o ・” (4
) Figure 3 shows the results of correcting the rate of frequency change with respect to the density of the second force detection sensor by performing the calculations shown in the above formulas in the signal processing unit 20 shown in Figure 1, with the horizontal axis representing the density and the vertical axis representing the density. The axis is shown as the frequency change rate. According to the figure, the rate of frequency change with respect to density change is less than 0.001%, and by making corrections using the crystal oscillator, the rate of frequency change is improved by more than two orders of magnitude compared to the case of only a force-detecting camera element. I understand.
〈発明の効果〉
以上実施例とともに具体的に説明したように本発明によ
れば、力検出振動子の密度変化に伴う共振周波数の変動
を水晶振動子の共振周波数により補正したので、精度の
良い力検出装置を簡単な構成で安価に実現することが出
来る。<Effects of the Invention> As specifically explained above in conjunction with the embodiments, according to the present invention, fluctuations in the resonant frequency due to changes in the density of the force detection resonator are corrected by the resonant frequency of the crystal resonator. A force detection device can be realized at low cost with a simple configuration.
第1図は本発明に係る力検出装置の一実施例を示すブロ
ック図、第2図は計算式および実験値により求めた密度
に対する力検出振動子と水晶振動子の共振周波数の変化
率を示す図、第3図は力検出振動子の密度に対する周波
数変化率を補正した結果を示す図、第4図は従来例を示
す構成説明図である。
10・・・力検出振動子、15a・・・励振素子、15
b・・・検出素子、17・・・第1の励振手段、20・
・・信号処理部、21・・・第2の励振手段、22・・
・水晶振動子。
第3図
第4図
第2図
f[mg/d]Fig. 1 is a block diagram showing an embodiment of the force detection device according to the present invention, and Fig. 2 shows the rate of change in the resonant frequency of the force detection oscillator and the crystal oscillator with respect to the density determined by calculation formulas and experimental values. FIG. 3 is a diagram showing the result of correcting the frequency change rate with respect to the density of the force detection vibrator, and FIG. 4 is a configuration explanatory diagram showing a conventional example. 10...force detection vibrator, 15a...excitation element, 15
b...detection element, 17...first excitation means, 20.
...Signal processing unit, 21...Second excitation means, 22...
·Crystal oscillator. Figure 3 Figure 4 Figure 2 f [mg/d]
Claims (1)
の力検出振動子を固有振動数で共振させる第1の励振手
段と、前記力検出振動子の振動を検出する信号処理手段
と、水晶振動子と、この水晶振動子を励振させる第2の
励振手段とを有し、前記水晶振動子の共振周波数を前記
信号処理手段に入力し、密度補正を行うようにしたこと
を特徴とする力検出装置。a force detection oscillator to which a force to be converted is applied in the axial direction; a first excitation means for resonating the force detection oscillator at a natural frequency; and a signal processing means for detecting vibrations of the force detection oscillator; It has a crystal resonator and a second excitation means for exciting the crystal resonator, and the resonant frequency of the crystal resonator is input to the signal processing means to perform density correction. Force detection device.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5364385A JPS61212737A (en) | 1985-03-18 | 1985-03-18 | Power detector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5364385A JPS61212737A (en) | 1985-03-18 | 1985-03-18 | Power detector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61212737A true JPS61212737A (en) | 1986-09-20 |
Family
ID=12948574
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5364385A Pending JPS61212737A (en) | 1985-03-18 | 1985-03-18 | Power detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61212737A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013015366A (en) * | 2011-07-01 | 2013-01-24 | Kobe Steel Ltd | Total tension measuring apparatus for band-shaped body |
JP2013024717A (en) * | 2011-07-21 | 2013-02-04 | Kobe Steel Ltd | Tension distribution measuring apparatus of belt-like body |
JP2014178330A (en) * | 2014-05-28 | 2014-09-25 | Kobe Steel Ltd | Total tension measuring apparatus of belt-like body |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59153130A (en) * | 1983-02-22 | 1984-09-01 | Yokogawa Hokushin Electric Corp | Vibration type transducer |
-
1985
- 1985-03-18 JP JP5364385A patent/JPS61212737A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59153130A (en) * | 1983-02-22 | 1984-09-01 | Yokogawa Hokushin Electric Corp | Vibration type transducer |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013015366A (en) * | 2011-07-01 | 2013-01-24 | Kobe Steel Ltd | Total tension measuring apparatus for band-shaped body |
JP2013024717A (en) * | 2011-07-21 | 2013-02-04 | Kobe Steel Ltd | Tension distribution measuring apparatus of belt-like body |
JP2014178330A (en) * | 2014-05-28 | 2014-09-25 | Kobe Steel Ltd | Total tension measuring apparatus of belt-like body |
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