JPS6190030A - Piezoelectric oscillator pressure sensor device - Google Patents

Piezoelectric oscillator pressure sensor device

Info

Publication number
JPS6190030A
JPS6190030A JP21304084A JP21304084A JPS6190030A JP S6190030 A JPS6190030 A JP S6190030A JP 21304084 A JP21304084 A JP 21304084A JP 21304084 A JP21304084 A JP 21304084A JP S6190030 A JPS6190030 A JP S6190030A
Authority
JP
Japan
Prior art keywords
pressure
diaphragm
oscillation
frequency
pressure sensor
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.)
Granted
Application number
JP21304084A
Other languages
Japanese (ja)
Other versions
JPH0435018B2 (en
Inventor
Haruyoshi Oota
太田 治良
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.)
Nihon Dempa Kogyo Co Ltd
Original Assignee
Nihon Dempa Kogyo Co Ltd
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 Nihon Dempa Kogyo Co Ltd filed Critical Nihon Dempa Kogyo Co Ltd
Priority to JP21304084A priority Critical patent/JPS6190030A/en
Publication of JPS6190030A publication Critical patent/JPS6190030A/en
Publication of JPH0435018B2 publication Critical patent/JPH0435018B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L9/00Measuring 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
    • G01L9/0041Transmitting or indicating the displacement of flexible diaphragms
    • G01L9/0072Transmitting or indicating the displacement of flexible diaphragms using variations in capacitance
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L9/00Measuring 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
    • G01L9/0001Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means
    • G01L9/0008Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations
    • G01L9/0022Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations of a piezoelectric element

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Fluid Pressure (AREA)

Abstract

PURPOSE:To detect pressure which has a wide temperature range and a wide pressure range by providing counter electrodes and three couples of piezoelectric oscillators in an airtight container, connecting an oscillation circuit externally through an electric circuit formed of the counter electrodes and one of the piezoelectric oscillators, and deciding on the frequency of the oscillator. CONSTITUTION:The diaphragm 2 is provided on the top surface of the airtight container 1. The counter electrodes 2a are provided on the reverse surface of the diaphragm 2. The piezoelectric oscillators 3 are provided opposite the electrodes 2a, and oscillation parts 3a, 3b, and 3c are fitted thereto. Then, a pressure difference applied to the diaphragm 2 is converted electrically by the counter electrodes 2a and oscillation part 3a and connected to the external oscillation circuit 7. Then, the electric signal is led to the frequency decision circuit 6 including the oscillation parts 3b and 3c through a buffer 5 to detect variation in frequency and detect the pressure. Then, the plural oscillation parts are provided, so an error caused by variation of temperature charac teristics of a piezoelectric body is eliminated and the pressure is detected with high precision.

Description

【発明の詳細な説明】 1mとの利用分野) 本発明は、圧セ振動子圧カセンサ装ごに係り、特に、圧
電振動子の周波数の安定性を利用し、かつ、広範な温度
域と圧力域をもつ圧力をlC7流で検出可能な圧電振動
子圧力センサ装置に関する。
[Detailed Description of the Invention] [Field of Application with 1m] The present invention relates to a pressure sensor device using a piezoelectric vibrator, and in particular, utilizes the stability of the frequency of a piezoelectric vibrator, and has a wide range of temperature and pressure. The present invention relates to a piezoelectric vibrator pressure sensor device capable of detecting a pressure within a range of 1C7 using an 1C7 flow.

(従来技術とその問題点) i7s9図および:jSlO図は従来の圧力センサの一
例を説明する説明図である0図中、20は円筒状の容器
であり、そのvq端部には薄いセラミックダイアプラム
21を設ける。該ダイアプラム21の裏側には’電極b
1.b2を形成させ、その電極b1 、b2には内部対
向電極aを設けるようにする、そこで、ダイアフラム外
部の圧力が変化するとダイアフラムが変化し、′;電極
bl、b2と内部対向電極aとの間隔が変化することに
なるので、この変化を静電容41. cの変化として検
出し、圧力センサとして用いるようにしている。しかし
、この種の圧力センサは1!極す、、b2と内部対向I
t極aの設定が面倒であると共に圧力域を広くとるため
の調整を行なうことが困難であった。
(Prior art and its problems) Figures i7s9 and :jS1O are explanatory diagrams for explaining an example of a conventional pressure sensor. A plum 21 is provided. On the back side of the diaphragm 21 is an electrode b.
1. b2, and the electrodes b1 and b2 are provided with an internally opposing electrode a, so that when the pressure outside the diaphragm changes, the diaphragm changes, and the distance between the electrodes bl, b2 and the internally opposing electrode a increases. will change, so this change can be expressed as capacitance 41. It is detected as a change in c and used as a pressure sensor. However, this type of pressure sensor is 1! Extreme, b2 and internal facing I
Setting the t-pole a is troublesome, and it is also difficult to make adjustments to widen the pressure range.

一方、圧電振動子は励振電力の印加によりその固有周波
数(電気共振周波数ともいう)で強く共振を生じるので
安定な一定周波数を得る手段としてd Lff機などに
広く用いられてきており この圧、シ撮勤tを用いた圧
カセノサをりすることが強く望まれていた。
On the other hand, piezoelectric vibrators generate strong resonance at their natural frequency (also called electrical resonance frequency) when excitation power is applied, so they have been widely used in dLff machines as a means of obtaining a stable constant frequency. There was a strong desire to learn how to measure pressure using a camera.

(発明の目的) 本発明は、X囲気に影響されず、圧電振動子の4&I動
の安定性を利用し、かつ、広範な温度域と圧力域をもつ
圧力を直流で検出可能なコンパクトな圧TL振動子圧カ
センサ装置を提供することを目的とする。
(Objective of the Invention) The present invention is a compact pressure sensor that is not affected by the An object of the present invention is to provide a TL vibrator pressure sensor device.

(発明のIN要) 本発明は、気密容器内に同一平板状の圧題体とに形成さ
れる厚み振動をする三対の同一′Wl極対(振動部)を
所定距離隔てて配設し、中央に位置する電極対(rA動
B)の−表面に平行に対応してダイアフラムが圧力差に
よって生ずる変位を伝える対向心棒を設け、この対向電
極とこの中央の電極対の前記対向電極と反対側の電極間
に外部より発振をJa続するための発振回路を接続する
と共に該発振回路からバッファを介して中央のt極対以
外の2つの1極対(振動部)が含まれる周波数判別回路
を接続して、周波数の変化をf1流出力として検出する
ようにする。
(IN Essentials of the Invention) The present invention is characterized in that three pairs of identical 'Wl pole pairs (vibrating parts) that vibrate through thickness and are formed on the same flat plate-shaped pressure plate are arranged at a predetermined distance apart in an airtight container. , a counter mandrel is provided parallel to the surface of the centrally located electrode pair (rA and B), the diaphragm transmitting the displacement caused by the pressure difference, and this counter electrode and the opposite electrode of the central electrode pair A frequency discrimination circuit in which an oscillation circuit for externally connecting oscillation is connected between the side electrodes, and two one-pole pairs (vibrating portions) other than the central t-pole pair are connected from the oscillation circuit via a buffer. is connected to detect the change in frequency as the f1 output.

(χ施例) 以下、未発明の一実施例を図面を参照しながら詳細に説
明する。
(X Example) Hereinafter, an uninvented example will be described in detail with reference to the drawings.

第1図は圧電振妨子圧カセンサ装置の内部を破断して示
した傾斜図、第2図は圧電振動子圧カセ/す回路図であ
る0図中、1は気密容器、2はダイアフラム、2aはダ
イアプラムの裏面に取付けられた対向′@極、3は圧i
t振動子片、3&〜3cは圧電振動部、4は圧電振動子
片保持具、5は定眉圧バッファ、6は周波数判別回路、
7は発振回路である。
Fig. 1 is a cutaway view of the inside of the piezoelectric vibrator pressure sensor device, and Fig. 2 is a circuit diagram of the piezoelectric vibrator pressure sensor device. 2a is the opposing '@ pole attached to the back side of the diaphragm, 3 is the pressure i
t vibrator piece, 3&~3c a piezoelectric vibrating part, 4 a piezoelectric vibrator piece holder, 5 a constant eyebrow pressure buffer, 6 a frequency discrimination circuit,
7 is an oscillation circuit.

次に、この圧電振動子圧カセンサ装2の動作について説
明する。まず1片面にダイアフラム2を有する気密容器
l内に、同−平板状圧?ttM動子3の上に形成した厚
み振動をする三対の同一1電極対(振動部)を互いに音
饗結合しないとみなせる所定距離(圧電体中の波長の1
0倍以上)に離して大々配設する。これらの振動部のう
ち中央の振動部3bの一表面に平行に対応してダイアフ
ラム2が圧力差によって生ずる変位を伝える対向電極2
aを設ける。この対向電極2aとこの中央の振動部3b
のうち灼応電極2aと反対側の電極間で形成した電気回
路に外部より発振を持続するための発振回路7を持続す
る。
Next, the operation of this piezoelectric vibrator pressure sensor device 2 will be explained. First, the same flat plate-like pressure ? Three pairs of identical electrodes (vibrating parts) formed on the ttM actuator 3 that vibrate through the thickness are separated by a predetermined distance (1 of the wavelength in the piezoelectric material) at which it can be considered that they are not acoustically coupled to each other.
0 times or more). Among these vibrating parts, the diaphragm 2 has a counter electrode 2 corresponding to one surface of the central vibrating part 3b that transmits the displacement caused by the pressure difference.
Provide a. This counter electrode 2a and this central vibrating part 3b
An oscillation circuit 7 for sustaining oscillation from the outside is connected to an electric circuit formed between the cauterizing electrode 2a and the electrode on the opposite side.

一方、この発振回路7から発振に影1を及ぼさないため
のバッファ5を介して三対の電極対(振動部)3m、3
b、3cのうち、中央の振動部3bを除く2つの振動部
3m、3cが含まれる周波数判別回路6に43周波数の
変化を直流出力として検出する。尚、W4波数判別回路
6におけるコンデ/すC5は整合トランスTの同調コン
デンサ、コンデ/すc、、C2はほぼ振動部2a、2c
の静電容’k c oと等しくする。抵抗Rは検出出力
負荷抵抗である。
On the other hand, from this oscillation circuit 7, three pairs of electrodes (vibration part) 3m, 3
A change in 43 frequencies is detected as a DC output to a frequency discrimination circuit 6 which includes two vibrating parts 3m and 3c, excluding the central vibrating part 3b, among the vibrating parts b and 3c. In addition, in the W4 wave number discrimination circuit 6, the capacitor C5 is a tuning capacitor of the matching transformer T, and the capacitors C2 and C2 are approximately the vibrating portions 2a and 2c.
be equal to the capacitance 'k c o. Resistor R is a detection output load resistance.

L6の動作を更に詳細に説明する。The operation of L6 will be explained in more detail.

ダイアフラム2Fの圧力が変化すると気密容器l内の気
圧との圧力差が変化するので、その圧力差の変化に応じ
てダイアフラム2は変位する。するとそのダイアフラム
2に取付けられている対向電極2m#3′11位する。
When the pressure of the diaphragm 2F changes, the pressure difference between it and the atmospheric pressure inside the airtight container l changes, so the diaphragm 2 is displaced in accordance with the change in the pressure difference. Then, the counter electrode 2m#3'11 attached to the diaphragm 2 is placed.

一方、圧電振動子片3は保持具4によって保持されてお
り、圧力の変動には左右されない、つまり、圧力の変動
によっても圧電振動子片3上に形成された振動部3bは
変位しない。
On the other hand, the piezoelectric vibrator piece 3 is held by the holder 4 and is not affected by pressure fluctuations. In other words, the vibrating part 3b formed on the piezoelectric vibrator piece 3 is not displaced even by pressure fluctuations.

従って、気密容!!lの外部の気圧変化によって、に4
向電極2&と圧1を振動子片3との振動部3bとの間H
tが変化することになる。
Therefore, airtight! ! Due to changes in the external pressure of l, to 4
H
t will change.

このように構成されたものは第2図に示される外部発振
回路7に接続し発振させるようにする。
The device configured in this manner is connected to an external oscillation circuit 7 shown in FIG. 2 to cause oscillation.

つまり、振動部3bに対向#l極2&と振動部3bとの
間で形成される静電容積C1を直列に接続し、この両端
に発振回路7を接続する。
That is, the capacitance C1 formed between the opposing #l pole 2& and the vibrating part 3b is connected in series to the vibrating part 3b, and the oscillation circuit 7 is connected to both ends of the capacitance C1.

そして、振動部3bの助振回路中にそれと直列にこの負
荷容量とよばれる静電容量CLを挿入すると、この^)
電容礒の大きさに従って固有周波数fは直列共振周波数
f0かも次のように変化するる電極間静電6碩、c1は
同じ〈等価直列静電容71テアリ、rltA)’it容
11比(r−Co /C+ ) とよばれる圧電体の電
気機械結合係数と、圧電振動子の構造によって決まる定
数である。
Then, when a capacitance CL called a load capacitance is inserted in series with the vibration auxiliary circuit of the vibrating part 3b, this ^)
Depending on the magnitude of the capacitance, the natural frequency f and the series resonant frequency f0 change as follows.The interelectrode electrostatic capacitance 6, c1 is the same. It is a constant determined by the electromechanical coupling coefficient of the piezoelectric material called Co /C+ ) and the structure of the piezoelectric vibrator.

また、この真向容量CLは第3図から明らかなように、
ダイアフラム2に取付けられた対向電極2&と振動aB
3 brI!It7)間PIA* t トt6ト。
Also, as is clear from FIG. 3, this direct capacitance CL is
Opposite electrode 2 and vibration aB attached to diaphragm 2
3brI! It7) PIA*ttt6t.

CL−に/(tXs)       −=(2)となる
CL-/(tXs) -=(2).

ここで、には静電容IIk算出定数、Sは対向電極2a
と振動部3bのなす有効静電容量面積を表わすものとす
る。
Here, is the capacitance IIk calculated constant, and S is the counter electrode 2a.
and represents the effective capacitance area formed by the vibrating portion 3b.

そこで、第2図から明らかなように、当該圧力センサの
外部に発振回路7を接続し1発振させると、該圧力セン
サ容器内の不活性気体圧力とダイアフラムの外圧との間
に圧力差を生ずるとその圧力差と、ダイアプラムの弾性
反撥力にほぼ比例した省だけダイアフラム2が可動し、
間隙t(第3図8 ’!’、 )が変化する。するとこ
の間隙tの変化により、−tJ記式(2)に従って静1
容睦CLが変化する。
Therefore, as is clear from FIG. 2, when the oscillation circuit 7 is connected to the outside of the pressure sensor and oscillates once, a pressure difference is created between the inert gas pressure inside the pressure sensor container and the external pressure of the diaphragm. The diaphragm 2 moves by an amount approximately proportional to the pressure difference between and the elastic repulsive force of the diaphragm.
The gap t (Fig. 3, 8'!', ) changes. Then, due to this change in the gap t, the static 1
Yong Mutsu CL changes.

そして、該振動部3b、つまり、中央の電極対はダイア
フラム2の変位Δtによって周fm散fの変化tΔfと
して現われ次式で表現できる。
The vibrating portion 3b, that is, the center electrode pair, appears as a change tΔf in the circumferential fm dispersion f due to the displacement Δt of the diaphragm 2, which can be expressed by the following equation.

ムf m −に’fe’ACL 、’:’l ΔCL−−Ct”K″11t   、°、
Δ+−−に’cte”fs”Δtよって、ダイアフラム
2の変位に比例した14波数の変化として検出すること
ができる。
'fe'ACL, ':'l ΔCL--Ct"K"11t, °,
It can be detected as a change in 14 wave numbers proportional to the displacement of the diaphragm 2 by adding 'cte"fs"Δt to Δ+−−.

ここで検出された信号は第2図から明らかなようにバッ
ファ5を介してヤーマントランスTに導 ・〈、このト
ランスからの出力、つまり、前記周波数変化量Δfを、
同一圧電振動子片3上に形成した同一構造の他の振動部
2m、2cで形成した周波数判別回路6を介して直流電
圧Vとして検出するように構成する。また、第5図から
明らかなように振動部2m、2cの周波数を振動部2b
を中心にほぼ等間隔に周波数を設定するが、この位置に
より1周波数判別回路のS特性を選択で!a感度を自由
に設定できる。ただし、ここで、変位Δt=Oのとき、
Δf−0となるように予め調整するようにする。
As is clear from FIG. 2, the signal detected here is guided to the Yarman transformer T via the buffer 5.
The configuration is such that it is detected as a DC voltage V via a frequency discrimination circuit 6 formed by other vibrating parts 2m and 2c of the same structure formed on the same piezoelectric vibrator piece 3. Moreover, as is clear from FIG. 5, the frequencies of the vibrating parts 2m and 2c are changed to
The frequencies are set at approximately equal intervals around the center, but depending on this position, the S characteristic of the frequency discrimination circuit can be selected! a Sensitivity can be set freely. However, here, when the displacement Δt=O,
Adjustment is made in advance so that Δf-0.

次に、この圧−、を振動子圧力センサ装置の圧力のi’
T ′n4iIll!!のm整手段の具体的構成につい
て説明する。
Next, this pressure - is the pressure i' of the vibrator pressure sensor device.
T'n4iIll! ! The specific configuration of the m adjustment means will be explained.

:!S5図乃至:iSa図は当該圧力センサのy4!!
手段の一実施例の説明図である0図中、6はy4繁用つ
まみネジ、7はコイルスプリング、8はm!i!ボルト
であり、その他は前記した実施例におけるものと同一の
ものであるので説明を省略する。
:! S5 diagram to iSa diagram are y4! of the pressure sensor. !
In Figure 0, which is an explanatory diagram of one embodiment of the means, 6 is a Y4 commonly used thumbscrew, 7 is a coil spring, and 8 is m! i! This is a bolt, and the other parts are the same as those in the embodiment described above, so a description thereof will be omitted.

次に この調整手段の動作について説明する。Next, the operation of this adjusting means will be explained.

i常は、第5図に示されるように調整ポルト8をダイヤ
フラムに1ざかる方向にセットするためコイルスプリン
グ7で調整ボルト8に設けられた回転止め溝に沿ってっ
まみ6を一杯に回転し固定させて置く、このときは圧電
振動子3の表面に設けられた゛?極3&はダイアフラム
対向電極2aから敲れている0次に圧力のbf測範囲を
調整するために圧電振動子3をっまみ6を回して調整ボ
ルト8を第8図の状態から押し上げて間隙tを小さくす
る。このように圧itN動子3とダイアフラム対向電極
2&の間隙tを変化させると静電容量CLを変化させる
ことがで3.従って、圧力の可amit囲を調整するこ
とができる。尚、気密容Mlと調整ボルト8との間は気
布性を保つため1例えば。
Normally, as shown in Fig. 5, in order to set the adjustment port 8 in the direction that rotates toward the diaphragm, use the coil spring 7 to fully rotate the knob 6 along the anti-rotation groove provided in the adjustment bolt 8. The piezoelectric vibrator 3 is fixed. In order to adjust the bf measurement range of the 0-order pressure which is drawn from the diaphragm counter electrode 2a, the pole 3 & is adjusted by turning the knob 6 of the piezoelectric vibrator 3 and pushing up the adjustment bolt 8 from the state shown in Fig. 8 to set the gap t. Make smaller. 3. By changing the gap t between the pressure itN mover 3 and the diaphragm counter electrode 2 in this way, the capacitance CL can be changed. Therefore, the possible pressure range can be adjusted. In addition, in order to maintain air-tightness between the airtight volume Ml and the adjustment bolt 8, for example, 1.

第8図に示すようにジャバラ7&をスプリング7の、周
りに設けるようにする。また、ダイアフラム対向電極2
&と圧Ml振動子3のなす角度0を予め適りに選ぶこと
により、圧力測定域を広範囲に扛り自由に設定で3る。
As shown in FIG. 8, a bellows 7& is provided around the spring 7. In addition, the diaphragm counter electrode 2
By appropriately selecting the angle 0 formed by & and the pressure Ml oscillator 3 in advance, the pressure measurement range can be freely set over a wide range.

ここでは片面ダイアプラムの場合を示したが圧it振動
子保持を空器の側面或いはもう一方のダイアプラム面2
で固定して行なえばダイアプラムとなし得ることはいう
までもない。
Although the case of a single-sided diaphragm is shown here, the pressure IT vibrator can be held on the side of the empty vessel or on the other diaphragm surface 2.
Needless to say, if it is fixed in place, it can be made into a diaphragm.

また1本発明を一実施例によって説明したが、本発明は
この実施例に限定されるものではなく。
Furthermore, although the present invention has been described by way of one embodiment, the present invention is not limited to this embodiment.

未発明の↑旨に従い、種々の変形が町ず屯であり。According to the uninvented ↑ point, various variations are available.

これらを木発す1の範囲から排除するものではない(9
1明の効果) 転RIllによれば、気密容器内に圧′N、揚動f B
を組み込み圧力センサ装置を得るようにしたので、n:
 z振動子が雰囲気条件に左右されることなく安定に動
作し、かつ再現性が良好である。また、同一の圧電振動
子片りに三つの振動部2a 、 2b 。
This does not exclude these from the scope of 1 (9
According to RIll, there is a pressure 'N in the airtight container and a lifting force f B
In order to obtain a pressure sensor device, n:
The z oscillator operates stably regardless of atmospheric conditions and has good reproducibility. Moreover, three vibrating parts 2a and 2b are provided on the same piezoelectric vibrator piece.

2cを同一構造で配設するようにしたので、6振動部の
条件は同一となり、特に、圧電体の温度特性の変化に基
づく誤差を生ずることがないコンパクトな、かつ信頼性
の高い圧力センサ装置を得ることができる。更に1発振
回路出力の一部を用いて容器内圧と被測定圧の差圧変位
に比例した一魔出力電圧をネ^確に、しかもfillに
得ることができる。
2c are arranged with the same structure, the conditions of the 6 vibrating parts are the same, and in particular, a compact and highly reliable pressure sensor device that does not cause errors due to changes in the temperature characteristics of the piezoelectric body. can be obtained. Furthermore, by using a part of the output of one oscillation circuit, it is possible to accurately and fillly obtain an output voltage proportional to the differential pressure displacement between the internal pressure of the container and the pressure to be measured.

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

第1図は本発明に係る圧電振動子圧力センサ装置の内部
を破断した斜視図、OS2図は本発明に係る圧力センサ
装置の回路図、第3図は第1図における一部拡大図、第
4図は周波数の変化を説明する説明図、第5図乃至第8
図は圧力の軒側範囲のA整f役を説明するJ’JI図、
第9因は従来の圧力セ/すの斜視図、第10図は第9図
の断面図である。 l・・・気烹容器、2・・・ダイアフラム、2a・・・
対向電極、3・・・圧電振動子片、3m、3b、3c・
・・振i11部、4・・・圧tIi動子の保持具、5・
・・バッファ。 6・・・周波数判別回路、7・・・発振回路、8・・・
調整用つまみ、9・・・調整用位履決め装置、1G・・
・調整ロット。 特許出願人 日本゛−電波工業株式会社代  理  人
  弁理士  辻       實図 第10図
FIG. 1 is a perspective view of the inside of the piezoelectric vibrator pressure sensor device according to the present invention, FIG. 2 is a circuit diagram of the pressure sensor device according to the present invention, and FIG. Figure 4 is an explanatory diagram explaining changes in frequency, Figures 5 to 8
The figure is a J'JI diagram that explains the A adjustment function in the eaves side range of pressure.
The ninth factor is a perspective view of a conventional pressure cell, and FIG. 10 is a sectional view of FIG. 9. l...Air heating container, 2...Diaphragm, 2a...
Counter electrode, 3... Piezoelectric vibrator piece, 3m, 3b, 3c.
... Shaking i11 part, 4... Pressure tIi mover holder, 5.
··buffer. 6... Frequency discrimination circuit, 7... Oscillation circuit, 8...
Adjustment knob, 9...Adjustment positioning device, 1G...
・Adjustment lot. Patent applicant: Japan Denpa Kogyo Co., Ltd. Representative: Patent attorney Minoru Tsuji Figure 10

Claims (1)

【特許請求の範囲】[Claims] 気密容器内に同一平板状の圧電体上に形成される厚み振
動をする三対の同一電極対を所定距離隔てて配設し、中
央に位置する電極対の一表面に平行に対応してダイアフ
ラムが圧力差によって生ずる変位を伝える対向電極を設
け、この対向電極とこの中央の電極対の前記対向電極と
反対側の電極間に外部より発振を持続するための発振回
路を接続すると共に該発振回路からバッファを介して中
央の電極対以外の2つの電極対が含まれる周波数判別回
路を接続して、周波数の変化を直流出力として検出する
ようにしたことを特徴とする圧電振動子圧力センサ装置
In an airtight container, three pairs of identical electrodes that vibrate in thickness and are formed on the same flat piezoelectric material are arranged at a predetermined distance apart, and a diaphragm is placed parallel to one surface of the central pair of electrodes. An oscillation circuit for sustaining oscillation is connected from the outside between the opposing electrode and the electrode on the opposite side of the opposing electrode of the central pair of electrodes, and the oscillating circuit A piezoelectric vibrator pressure sensor device characterized in that a frequency discrimination circuit including two electrode pairs other than the center electrode pair is connected through a buffer to detect a change in frequency as a DC output.
JP21304084A 1984-10-11 1984-10-11 Piezoelectric oscillator pressure sensor device Granted JPS6190030A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21304084A JPS6190030A (en) 1984-10-11 1984-10-11 Piezoelectric oscillator pressure sensor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21304084A JPS6190030A (en) 1984-10-11 1984-10-11 Piezoelectric oscillator pressure sensor device

Publications (2)

Publication Number Publication Date
JPS6190030A true JPS6190030A (en) 1986-05-08
JPH0435018B2 JPH0435018B2 (en) 1992-06-09

Family

ID=16632518

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21304084A Granted JPS6190030A (en) 1984-10-11 1984-10-11 Piezoelectric oscillator pressure sensor device

Country Status (1)

Country Link
JP (1) JPS6190030A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62173656A (en) * 1986-01-28 1987-07-30 Mitsui Petrochem Ind Ltd Information recording substrate and its production
EP0273649A2 (en) * 1986-12-29 1988-07-06 Halliburton Company Temperature-compensated transducer

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62173656A (en) * 1986-01-28 1987-07-30 Mitsui Petrochem Ind Ltd Information recording substrate and its production
EP0273649A2 (en) * 1986-12-29 1988-07-06 Halliburton Company Temperature-compensated transducer

Also Published As

Publication number Publication date
JPH0435018B2 (en) 1992-06-09

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