JPS5844321A - Vibration type force detector - Google Patents
Vibration type force detectorInfo
- Publication number
- JPS5844321A JPS5844321A JP14187881A JP14187881A JPS5844321A JP S5844321 A JPS5844321 A JP S5844321A JP 14187881 A JP14187881 A JP 14187881A JP 14187881 A JP14187881 A JP 14187881A JP S5844321 A JPS5844321 A JP S5844321A
- Authority
- JP
- Japan
- Prior art keywords
- vibrators
- force
- vibrator
- bellows
- difference
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L9/00—Measuring steady of quasi-steady pressure of fluid or fluent solid material by electric or magnetic pressure-sensitive elements; Transmitting or indicating the displacement of mechanical pressure-sensitive elements, used to measure the steady or quasi-steady pressure of a fluid or fluent solid material, by electric or magnetic means
- G01L9/0001—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means
- G01L9/0008—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Fluid Pressure (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は、与えられるカにょって共振周波数が変化する
ことを利用した弾性振動体を使用する振動式力検出器に
関するtのである・
弾性振動体を使用するとの種の装置祉、出力信号が周波
数信号で得られるとと、検出感度が高いこと勢の特長が
ある反面、弾性振動体とこれを支持する部材との線膨張
の差が力となって表われたり、振動体自身の温度係数が
問題と愈る可能性がある等、温度の影響を受けやすい欠
点を有しているO
本発明は、温度の影響を受けず、検出精度の高い振動式
力検出器を実現しようとするものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a vibrating force detector using an elastic vibrating body that utilizes the fact that the resonance frequency changes depending on applied force. When the output signal is obtained as a frequency signal, the detection sensitivity is high, but on the other hand, the difference in linear expansion between the elastic vibrating body and the member supporting it may be expressed as a force. , the temperature coefficient of the vibrating body itself may be a problem, and the vibration body itself has the disadvantage of being easily affected by temperature. It is an attempt to realize a vessel.
本発明に係る装置は、同一材料であって、一端が共通の
部材に結合する2以上の振動子で構成され、2以上の振
動子の各他端に、互いに差動的に検出すべき力を与える
とともに、2以上の振動子の各振動数に関連した周波数
信号の差を測定゛して力の大きさを知るようにした点に
特徴があ゛る。The device according to the present invention is composed of two or more vibrators made of the same material and whose one end is coupled to a common member, and a force to be detected differentially from each other is applied to each other end of the two or more vibrators. The unique feature is that the magnitude of the force can be determined by measuring the difference in frequency signals related to each frequency of two or more vibrators.
第1図は本発明の一実施例を示す構成図で、ここでは、
圧力計を構成した場合を例示する。FIG. 1 is a configuration diagram showing one embodiment of the present invention, and here,
A case where a pressure gauge is configured will be illustrated.
図において、1は断面り字形状の基台、2は基台1に取
付仕られたベローズ、3はベローズシの作動端20に一
端が結合し、他端が基台1に固定された可撓性基板で、
この基板は、片持ち梁を構成している。4は本発明で特
徴としている振動式の力検出手段であって、可撓性基板
3上に、例えば低融点ガラスで接着されている。In the figure, 1 is a base with a cross-sectional shape, 2 is a bellows attached to the base 1, and 3 is a flexible body whose one end is connected to the operating end 20 of the bellows and the other end is fixed to the base 1. sexual substrate,
This substrate constitutes a cantilever beam. Reference numeral 4 denotes a vibrating force detection means, which is a feature of the present invention, and is bonded onto the flexible substrate 3 using, for example, low-melting glass.
第2図は、振動式力検出手段4を拡大して示す構成図で
ある。仁の力検出手段4は、一端が共通部材40にそれ
ぞれ結合している5本の同一形状、同一材料の振動子4
1.42.43で構成されておシ、各振動子41.42
.43の他端が可撓性基板3に各振動子が等間隔で配列
するように接着されている。FIG. 2 is an enlarged configuration diagram showing the vibratory force detection means 4. As shown in FIG. The force detecting means 4 includes five vibrators 4 of the same shape and made of the same material, each of which has one end connected to a common member 40.
1.42.43, each vibrator 41.42
.. The other end of the vibrator 43 is bonded to the flexible substrate 3 so that the vibrators are arranged at equal intervals.
各振動子41.42.43には、図示してないが、それ
ぞれ振動子を振動させるための励振手段と、振動子の振
動数を検出するための振動検出手段とが設けられている
。これらの励振手段、振動検出手段としては、振動子の
材料が金属材料の場合には、例えげPZTを取付けたも
の、あるいは電磁力を利用したもの等が使用可能であ:
る。また振動子の材できる利点がある。Although not shown, each of the vibrators 41, 42, and 43 is provided with excitation means for vibrating the vibrator and vibration detection means for detecting the frequency of the vibrator. As these excitation means and vibration detection means, when the material of the vibrator is a metal material, for example, one attached with PZT or one using electromagnetic force can be used:
Ru. It also has the advantage of being used as a material for vibrators.
なお、とこでは、各振動子41〜43は、中央部に透孔
4!5が設けられ、デーワルビーム状のものとなってい
るが、との透孔45をカ<シ、シングルビーム状のもの
としてもよい。In this case, each of the vibrators 41 to 43 has a through hole 4!5 in the center, and is shaped like a dewal beam. You can also use it as
第1図に戻り、5,6は、いずれも発振増幅器で、一方
の発振増幅器5は、振動子41を含んで発振ループを形
成しておシ、また、他方の発振増幅器6は、中央の振動
子42を含んでもうひとつの発振ループを形成している
。7は、各発振増幅器5,6からの周波数信号f□、f
2の差を演算する演算回路である。Returning to FIG. 1, 5 and 6 are both oscillation amplifiers; one oscillation amplifier 5 forms an oscillation loop including the oscillator 41, and the other oscillation amplifier 6 is located in the center. Another oscillation loop including the vibrator 42 is formed. 7 is the frequency signal f□, f from each oscillation amplifier 5, 6
This is an arithmetic circuit that calculates the difference between two.
このように構成した装置の動作を次に説明する。The operation of the device configured in this way will be described next.
いま、ベローズ2に被測定圧力Pが印加され、ベローズ
2が伸長すると、可撓性基板Sは、第2図実線に誇張し
て示すように撓み、これによって、3本の振動子41〜
43には互いに差動的な外力が加わる◇すなわち、中□
央の振動子42には引張力Fが与えられ、また両端の振
動子41.43には、それされ圧縮力F/2が与えられ
る。Now, when the measured pressure P is applied to the bellows 2 and the bellows 2 expands, the flexible substrate S is bent as shown in an exaggerated solid line in FIG.
A differential external force is applied to 43 ◇ that is, inside □
A tensile force F is applied to the central vibrator 42, and a deflecting compressive force F/2 is applied to the vibrators 41 and 43 at both ends.
このような状態において、両端の振動子41.43の共
振周波数f工、中央の振動子42の共振周波数f2は、
それぞれ(1)式および(2)式で示すことができる。In this state, the resonant frequency f of the vibrators 41 and 43 at both ends and the resonant frequency f2 of the central vibrator 42 are as follows.
They can be expressed by equations (1) and (2), respectively.
ま
ただし、 fol:力rが0のときの振動子41.43
の共振周波数
f02 ”力Fが00ときの振動子42の共振周波数。Also, fol: oscillator when force r is 0 41.43
Resonant frequency f02 ``The resonant frequency of the vibrator 42 when the force F is 00.
ただし、この例で杜 振動子41〜43は同一材料、同一 形状であってf01キf。2 となる。However, in this example, Vibrators 41 to 43 are made of the same material and the same The shape is f01ki f. It becomes 2.
A:振動子41.43の力係数
B=振動子42の力係数
また、f工とf2の差Δfは、(1)式、(2)式から
(3)式の通りとなる。A: Force coefficient of the vibrator 41.43 B=force coefficient of the vibrator 42 Also, the difference Δf between f and f2 is as shown in equations (1) and (2) to (3).
Δf″f2−f1
(5)式において、f2+f□を一定に維持するものと
すれば、Δfは与えられる力Fに対応したものとと1k
F)、tを測定することによって、力F1すなわち、被
測定圧力Pを知ることができる。′第1図において、演
算回路7は、f□、f2を入力し、その差を演算するこ
とによって、被測定圧カPKII連した信号Δfl出力
する。Δf″f2−f1 In equation (5), if f2+f□ is kept constant, Δf corresponds to the applied force F and 1k
By measuring F) and t, the force F1, that is, the pressure to be measured P can be determined. ' In FIG. 1, the arithmetic circuit 7 inputs f□ and f2, calculates the difference between them, and outputs a signal Δfl that is connected to the measured pressure PKII.
このように構成した装置によれば、各振動子41〜43
が同一材料、同一形状で一体に構成されていることから
、各振動子の温度変化による共振周波数の変化は、各振
動子に同じように影響することとなるが、これは、演算
回路7における演算によって相殺されて、出力信号には
何んら影響しないものとなる。According to the device configured in this way, each of the vibrators 41 to 43
Since the oscillators are made of the same material and the same shape, changes in the resonant frequency due to temperature changes in each oscillator will affect each oscillator in the same way. It is canceled out by the calculation and has no effect on the output signal.
第5図及び第4図は、本発明の他の実施例を示す構成断
面図である。第5図の実施例では、ケース6内に5本の
振動子で構成゛される振動式力検出手段4を収容し、振
動子41.43の一端をケース8の底部80にそれぞれ
取付け、中央の振動子42の一端をベローズ2の作動端
2oに取付けたものである。FIGS. 5 and 4 are sectional views showing other embodiments of the present invention. In the embodiment shown in FIG. 5, a vibrating force detection means 4 composed of five vibrators is housed in a case 6, one end of the vibrators 41 and 43 is attached to the bottom 80 of the case 8, and the center One end of the vibrator 42 is attached to the operating end 2o of the bellows 2.
また、ベローズ2は、その作動端2oがケース8内に向
かって伸び縮みするようにケース8の底部に取付けられ
ている。このベローズ2は、ベローズに与えられる圧力
Pと、ケース2内の圧力(含む真!2りとの差圧に応じ
て伸び縮みし、力検出手段4は、この差圧を検出する。Further, the bellows 2 is attached to the bottom of the case 8 so that its operating end 2o expands and contracts toward the inside of the case 8. The bellows 2 expands and contracts in accordance with the differential pressure between the pressure P applied to the bellows and the pressure inside the case 2 (including the stem 2), and the force detection means 4 detects this differential pressure.
第4図の実施例は、第5図の実施例を変形し九ものであ
って、ベローズに代えて、ここにダイヤフラム21を設
置し、このダイヤプラムの変位を振動子42の一端に与
えるように構成したものである。The embodiment shown in FIG. 4 is a modification of the embodiment shown in FIG. It is composed of
たお、上記の各実施例では、いずれも圧力針に適用した
場合であるが、各種の物理量に応じた力を検出するため
の装置に適用することができる。Although each of the above embodiments is applied to a pressure needle, the present invention can also be applied to a device for detecting force corresponding to various physical quantities.
また、上記では、5@の同一形状の振動子で構成される
亀のを用いたが2個の振動子でもよく、また、各振動子
の形状は必ずしも同一形状でなくともよい。形状を異に
構成した場合の共振周波数の相違郷は、演算回路によっ
て補正が可能だからである。In addition, in the above description, a tortoise configuration consisting of five vibrators having the same shape is used, but two vibrators may be used, and the shape of each vibrator does not necessarily have to be the same. This is because the difference in resonance frequency when the shapes are configured differently can be corrected by the arithmetic circuit.
以上説明したように、本発明に、よれば、振動式のもつ
各特長を何ら阻害することなく、温度の影響を受けない
振動式検出器が実現できる。As explained above, according to the present invention, it is possible to realize a vibrating type detector that is not affected by temperature without impairing the various features of the vibrating type.
、第1図は本発明の一実施例を示す構成図、第2図は第
1図装置に使用されている力検出手段の一例を示す構成
図、第5図及び第4図は本発明の他の実施例を示す構成
断面図である。
4・・・振動式力検出手段、41〜43・・・振動子、
40・・・共通部材、5.6・・・発振増幅器、7・・
・演算回路。
第1図
行
111浣1力+P)
篇2図
篇3図, FIG. 1 is a block diagram showing an embodiment of the present invention, FIG. 2 is a block diagram showing an example of the force detection means used in the device shown in FIG. 1, and FIGS. FIG. 7 is a cross-sectional view showing another embodiment. 4... Vibratory force detection means, 41 to 43... Vibrator,
40... Common member, 5.6... Oscillation amplifier, 7...
・Arithmetic circuit. Figure 1 line 111 Kasuri 1 power + P) Volume 2 Figure 3
Claims (2)
結合する2以上の振動子で構成され、前記2以上の振動
子の各他端に互いに差動的に検出すべき力を与えるとと
もに、前記2IIの振動子の6振動数に関連し九周波数
信号の差を測定して前記力の大きさを知るようにした振
動式力検出器み(1) Consisting of two or more vibrators made of the same material and each having one end coupled to a common member, applying a force to be detected differentially to each other end of the two or more vibrators, and A vibrating force detector that measures the difference between nine frequency signals related to the six frequencies of the 2II vibrator to determine the magnitude of the force.
に電極板を形成させることによって振動子の励振手段、
振動検出手段を構成するようにした特許請求の範囲第1
項記載の振動式力検出器。(2) By using crystal as the material of the vibrator and forming an electrode plate on it, an excitation means for the vibrator;
Claim 1 constituting vibration detection means
Vibratory force detector as described in section.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14187881A JPS5844321A (en) | 1981-09-09 | 1981-09-09 | Vibration type force detector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14187881A JPS5844321A (en) | 1981-09-09 | 1981-09-09 | Vibration type force detector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5844321A true JPS5844321A (en) | 1983-03-15 |
Family
ID=15302258
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP14187881A Pending JPS5844321A (en) | 1981-09-09 | 1981-09-09 | Vibration type force detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5844321A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4947694A (en) * | 1988-03-16 | 1990-08-14 | W & T Avery Limited | Vibrating force sensor |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6110197U (en) * | 1984-06-22 | 1986-01-21 | 敏雄 工藤 | Extendable drying rack |
-
1981
- 1981-09-09 JP JP14187881A patent/JPS5844321A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6110197U (en) * | 1984-06-22 | 1986-01-21 | 敏雄 工藤 | Extendable drying rack |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4947694A (en) * | 1988-03-16 | 1990-08-14 | W & T Avery Limited | Vibrating force sensor |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US4306456A (en) | Elastic wave accelerometer | |
US4479385A (en) | Double resonator cantilever accelerometer | |
US4901586A (en) | Electrostatically driven dual vibrating beam force transducer | |
US4594898A (en) | Force sensors | |
US3238789A (en) | Vibrating bar transducer | |
US5117148A (en) | Vibrator | |
JPH05288774A (en) | Acceleration sensor | |
JPH02189433A (en) | Vibration type power-frequency converter | |
JPS60105917A (en) | Resonance conversion system, resonance-force conversion system and method of determining force or other parameter and temperature | |
JPS59126261A (en) | Accelerometer with needle resonator power transducer | |
JPH0599676A (en) | Gyroscope | |
JPS60239638A (en) | Resonator temperature transducer and resonator temperature measuring device | |
JPH0384467A (en) | Accelerometer sensor with curved vibration beam | |
JPH08105912A (en) | Acceleration sensor | |
US4531073A (en) | Piezoelectric crystal resonator with reduced impedance and sensitivity to change in humidity | |
JP3072354B2 (en) | Transducer accelerometer | |
JPH04363670A (en) | Vibrator type accelerometer | |
JPS5844321A (en) | Vibration type force detector | |
JPS60186725A (en) | Pressure sensor | |
KR100210707B1 (en) | Vibration gyroscope | |
JP3049305B2 (en) | Resonator accelerometer | |
JPH0331207B2 (en) | ||
JPS596369B2 (en) | force conversion mechanism | |
JPS596370B2 (en) | force conversion mechanism | |
JPS6333145Y2 (en) |