JPH0390832A - pressure measuring device - Google Patents
pressure measuring deviceInfo
- Publication number
- JPH0390832A JPH0390832A JP22879089A JP22879089A JPH0390832A JP H0390832 A JPH0390832 A JP H0390832A JP 22879089 A JP22879089 A JP 22879089A JP 22879089 A JP22879089 A JP 22879089A JP H0390832 A JPH0390832 A JP H0390832A
- Authority
- JP
- Japan
- Prior art keywords
- pressure
- liquid
- liquid column
- sensor chamber
- measuring device
- 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
Landscapes
- Measuring Fluid Pressure (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は、水晶振動子等の圧電振動子の共振周波数が周
囲の圧力と相関関係にあることを利用した圧力測定装置
に関する。DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a pressure measuring device that utilizes the fact that the resonance frequency of a piezoelectric vibrator such as a quartz crystal vibrator has a correlation with surrounding pressure.
〈従来の技術〉
圧電振動子の共振周波数が周囲の圧力に応じて直線的に
変化することが知られている(特開昭57136130
号公報)。しかし、周囲の気体または液体の種類が異な
ると比例定数が異なり、また、圧電振動子を直接外界へ
曝すことは塵埃等が付着して好ましくない。そのため、
例えば第3図に示すように、ベローズ、ダイヤフラム等
の弾性変形体で振動子を密閉構造として外部圧力を測定
していた。<Prior art> It is known that the resonance frequency of a piezoelectric vibrator changes linearly depending on the surrounding pressure (Japanese Patent Laid-Open No. 57136130).
Publication No.). However, the constant of proportionality differs depending on the type of surrounding gas or liquid, and it is not preferable to expose the piezoelectric vibrator directly to the outside world because dust and the like will adhere thereto. Therefore,
For example, as shown in FIG. 3, external pressure has been measured using a vibrator having a sealed structure using an elastically deformable body such as a bellows or a diaphragm.
〈発明が解決しようとする課題〉
このように、ベローズ、ダイヤフラム等を用いて密閉構
造とした従来例においては、ベローズあるいはダイヤフ
ラムの弾性定数が振動子周囲の内部圧力に大きく影響し
、また、温度変化によりベローズあるいはダイヤフラム
の容積が変化することも、内部圧力に影響を与えていた
。さらに、ベローズやダイヤフラムが金属製であってバ
ネ係数が大きいため、微小圧力変化を測定することか困
難であった。<Problems to be Solved by the Invention> As described above, in conventional examples of sealed structures using bellows, diaphragms, etc., the elastic constants of the bellows or diaphragm greatly affect the internal pressure around the vibrator, and the temperature Changes in the volume of the bellows or diaphragm also affected the internal pressure. Furthermore, since the bellows and diaphragm are made of metal and have a large spring coefficient, it has been difficult to measure minute pressure changes.
〈課題を解決するための手段〉
本発明の圧力測定装置は、振動子が設けられ所定のガス
が封入されたセンサ室と、上端が被測定圧力導入口とな
る第1の液柱と、その第1の液柱と底部のみで連通し上
端が上記センサ室に連通ずる第2の液柱と、その第1お
よび第2の液柱内に充填された不揮発性液体を有し、上
記振動子の共振周波数より上記被測定圧力導入口の圧力
を測定することを特徴としている。<Means for Solving the Problems> The pressure measuring device of the present invention comprises: a sensor chamber provided with a vibrator and filled with a predetermined gas; a first liquid column whose upper end serves as an inlet for introducing the pressure to be measured; a second liquid column that communicates with the first liquid column only at its bottom and whose upper end communicates with the sensor chamber; and a non-volatile liquid filled in the first and second liquid columns; It is characterized in that the pressure at the pressure to be measured inlet is measured from the resonance frequency of .
く作用〉
第1図の原理的実施例により説明する。測定すべき外圧
をPいセンサ室の内圧をP2、外圧側液柱の断面積をS
い内圧側液柱の断面積をS、、液面差をh、封止液体の
密度をρとすれば、センサ室の内圧P2は
P、=P、−ρS2h ・・・(1)測定すべき
外圧P1が増大ずれば液面差りが増大してセンサ室の内
容積Vが減少して内圧P2が増大する。反対に、圧力P
1が減少すればセンサ室の内容積Vが膨張し内圧P2が
減少する。Function> This will be explained using the principle embodiment shown in FIG. The external pressure to be measured is P, the internal pressure of the sensor chamber is P2, and the cross-sectional area of the liquid column on the external pressure side is S.
If the cross-sectional area of the liquid column on the internal pressure side is S, the liquid level difference is h, and the density of the sealing liquid is ρ, then the internal pressure P2 of the sensor chamber is P, = P, -ρS2h...(1) Measurement If the external pressure P1 increases, the liquid level difference increases, the internal volume V of the sensor chamber decreases, and the internal pressure P2 increases. On the contrary, pressure P
1 decreases, the internal volume V of the sensor chamber expands and the internal pressure P2 decreases.
センサ室のガス容積Vは、温度が一定のとき内圧P2に
逆比例する。また、封止液体の容積は変わらないから、
圧力変化による液面の変位をhh2とすれば
S Ih+ = S z h z ・・・(
2)内圧側の液柱の断面積S2および空間容積が大きい
ほど、測定レンジが拡がり、反対に82が小さいどきは
感度が高くなる。The gas volume V in the sensor chamber is inversely proportional to the internal pressure P2 when the temperature is constant. Also, since the volume of the sealing liquid does not change,
If the displacement of the liquid level due to pressure change is hh2, S Ih+ = S z h z ...(
2) The larger the cross-sectional area S2 and the space volume of the liquid column on the internal pressure side, the wider the measurement range; conversely, when 82 is small, the sensitivity becomes higher.
〈実施例〉
第1図に本発明の原理的実施例を示す。センサ室1内に
は屈曲振動を行う音叉形水晶振動子2が配設され、その
電極リード線3が室外に導出され、発振回路に接続され
ている。液槽4は、上端が測定すべき圧力導入口となる
第1の液柱41と、上端がセンサ室1に連通する第2の
液柱42と、両液柱を底で連通させる連通部43により
略U字形に構成され、不揮発性の封止液体5が適量充填
されてセンサ室1と外界を遮断している。封止液体5と
しては、水銀、シリコン油等の不揮発性のものが好まし
く、例えば水銀の液面にシリコン油等の他の液体層を設
けて用いることもできる。セン。<Example> FIG. 1 shows a principle example of the present invention. A tuning fork crystal resonator 2 that performs bending vibration is disposed within the sensor chamber 1, and its electrode lead wire 3 is led out to the outside and connected to an oscillation circuit. The liquid tank 4 includes a first liquid column 41 whose upper end serves as a pressure introduction port to be measured, a second liquid column 42 whose upper end communicates with the sensor chamber 1, and a communication section 43 which communicates both liquid columns at the bottom. The sensor chamber 1 is formed into a substantially U-shape and is filled with an appropriate amount of nonvolatile sealing liquid 5 to isolate the sensor chamber 1 from the outside world. The sealing liquid 5 is preferably a non-volatile liquid such as mercury or silicone oil. For example, another liquid layer such as silicone oil may be provided on the surface of the mercury. Sen.
す室1内には、不活性であって密度が大きい気体、例え
ば高圧トランス用絶縁ガスSF6が封入されている。The chamber 1 is filled with an inert, high-density gas such as an insulating gas SF6 for a high-voltage transformer.
第2図に本発明の好ましい実施例を示す、液槽4は底部
をのぞき二重円筒型に構成され、円筒44の上端がセン
サ室1に連通し、外筒45の上端が測定すべき圧力導入
口に開口している。FIG. 2 shows a preferred embodiment of the present invention. The liquid tank 4 has a double cylindrical shape except for the bottom, the upper end of the cylinder 44 communicates with the sensor chamber 1, and the upper end of the outer cylinder 45 connects to the pressure to be measured. It opens at the inlet.
〈発明の効果〉
本発明によれば、センサ室と測定圧導入口の間に不揮発
性の封止液体を介在させ、外圧P1と内圧P2とが封止
液体を介して均衡する構成としたので、弾性体のバネ定
数の影響が全くなく、従って、きわめて高感度であって
しかも測定レンジの広い圧力測定が可能となった。また
、液柱の断面積、液柱空間容積の選定により、測定レン
ジ等を任意に設計することができる。<Effects of the Invention> According to the present invention, a nonvolatile sealing liquid is interposed between the sensor chamber and the measurement pressure inlet, and the external pressure P1 and the internal pressure P2 are balanced through the sealing liquid. , there is no influence of the spring constant of the elastic body, making it possible to measure pressure with extremely high sensitivity and a wide measurement range. Further, by selecting the cross-sectional area of the liquid column and the volume of the liquid column space, the measurement range etc. can be arbitrarily designed.
第1図は本発明の原理的実施例を示す図、第2図は本発
明の好ましい実施例を示す図、第3図は従来例を示す図
である。
センサ室
音叉形水晶振動子
リード線
液槽
封止液体FIG. 1 is a diagram showing a principle embodiment of the present invention, FIG. 2 is a diagram showing a preferred embodiment of the present invention, and FIG. 3 is a diagram showing a conventional example. Sensor chamber Tuning fork crystal resonator lead wire Liquid tank Sealing liquid
Claims (2)
室と、上端が被測定圧力導入口となる第1の液柱と、そ
の第1の液柱と底部のみで連通し上端が上記センサ室に
連通する第2の液柱と、その第1および第2の液柱内に
充填された不揮発性液体を有し、上記振動子の共振周波
数より上記被測定圧力導入口の圧力を測定する圧力測定
装置。(1) A sensor chamber equipped with a vibrator and filled with a predetermined gas, a first liquid column whose upper end serves as an inlet for the pressure to be measured, and which communicates with the first liquid column only at its bottom, with its upper end above the It has a second liquid column communicating with the sensor chamber and a non-volatile liquid filled in the first and second liquid columns, and measures the pressure at the measured pressure inlet from the resonance frequency of the vibrator. pressure measuring device.
積よりも大きい、第1項記載の圧力測定装置。(2) The pressure measuring device according to item 1, wherein the cross-sectional area of the second liquid column is larger than the cross-sectional area of the first liquid column.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22879089A JPH0390832A (en) | 1989-09-04 | 1989-09-04 | pressure measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22879089A JPH0390832A (en) | 1989-09-04 | 1989-09-04 | pressure measuring device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0390832A true JPH0390832A (en) | 1991-04-16 |
Family
ID=16881894
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22879089A Pending JPH0390832A (en) | 1989-09-04 | 1989-09-04 | pressure measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0390832A (en) |
-
1989
- 1989-09-04 JP JP22879089A patent/JPH0390832A/en active Pending
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