JPH1038913A - Piezoelectric oscillator - Google Patents
Piezoelectric oscillatorInfo
- Publication number
- JPH1038913A JPH1038913A JP8215322A JP21532296A JPH1038913A JP H1038913 A JPH1038913 A JP H1038913A JP 8215322 A JP8215322 A JP 8215322A JP 21532296 A JP21532296 A JP 21532296A JP H1038913 A JPH1038913 A JP H1038913A
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric vibrator
- piezoelectric
- electrode
- capacitance
- change
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P15/00—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration
- G01P15/02—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses
- G01P15/08—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values
- G01P2015/0805—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration
- G01P2015/0822—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration for defining out-of-plane movement of the mass
- G01P2015/084—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values being provided with a particular type of spring-mass-system for defining the displacement of a seismic mass due to an external acceleration for defining out-of-plane movement of the mass the mass being suspended at more than one of its sides, e.g. membrane-type suspension, so as to permit multi-axis movement of the mass
Landscapes
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Abstract
(57)【要約】
【目的】静電容量式の加速度検出器において、より高精
度で小型化、低価格化した加速度検出器の製造を目的と
する。
【構成】圧電素板の片面中心部に錘を具備し、圧電素板
の平面を切り放さずに4分割しその各々の両面に電極を
構成して成る圧電振動子と、この圧電振動子の電極と対
向する各々の面に構成された電極との容量とにより構成
される圧電振動子を用いて、圧電振動子の電極とその電
極に対向する電極間との容量の変化分を周波数に換算し
て加速度を検知することで、圧電振動子にかかるXY平
面に平行な任意の加速度の大きさと方向を検知すること
により目的を達成した。
(57) [Abstract] [Purpose] The object of the present invention is to manufacture a more accurate, smaller, and less expensive acceleration detector of a capacitance type. A piezoelectric vibrator comprising a weight at the center of one side of a piezoelectric element, dividing the surface of the piezoelectric element into four parts without cutting off the plane, and forming electrodes on both sides thereof; Using a piezoelectric vibrator composed of the capacitance of an electrode formed on each surface facing the electrode, the change in capacitance between the electrode of the piezoelectric vibrator and the electrode facing the electrode is converted into a frequency The object is achieved by detecting the acceleration and detecting the magnitude and direction of an arbitrary acceleration parallel to the XY plane applied to the piezoelectric vibrator.
Description
【0001】[0001]
【産業上の利用分野】圧電発振素子を応用した加速度検
出器に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an acceleration detector using a piezoelectric oscillation element.
【0002】[0002]
【従来の技術】従来の技術では、図7の静電容量式の加
速度検出器の断面図に示すような構造で分かるように、
対面する2面間の電極10の隙間でのギャップの変化量
で発生する静電容量の変化を直読して物体に加わった水
平方向の任意の2方向の加速度(X軸、Y軸)を検出し
ている。2. Description of the Related Art In the prior art, as can be seen from a structure shown in a sectional view of a capacitance type acceleration detector of FIG.
Capacitance change generated by the change amount of the gap in the gap between the electrodes 10 between the two facing surfaces is directly read to detect any two horizontal accelerations (X axis, Y axis) applied to the object. doing.
【0003】[0003]
【発明が解決しようとする課題】しかし、極小の隙間に
おけるギャップの変化量で発生する静電容量の変化量を
検出するのでは、そこに得られる容量の変化量を定量的
に測定するのが難しく、正確な容量変化を検知するのは
難しい。従って、容量の変化で得られた加速度の検知量
の信頼性も薄い。更に容量の直読方式では、検出器全体
が温度により膨張したり、収縮することによって加速度
の検出部である極小の隙間におけるギャップが変化する
のを補償することが困難で、正確な加速度を検出しにく
い。However, when detecting the change in the capacitance caused by the change in the gap in the minimum gap, it is necessary to quantitatively measure the change in the capacitance obtained therefrom. Difficult and difficult to detect accurate capacitance change. Therefore, the reliability of the detected amount of acceleration obtained by the change in capacitance is low. Further, in the direct reading method of the capacitance, it is difficult to compensate for a change in a gap in a very small gap, which is an acceleration detecting unit, due to expansion and contraction of the entire detector due to temperature, and accurate detection of acceleration is performed. Hateful.
【0004】[0004]
【課題を解決するための手段】昨今の電子装置、セット
部品は高信頼性、高精度化、更に小型軽量化、低価格化
の傾向にある。従って、これらに使用される電子部品に
も同様なことが要求されている。また最近では機械分野
と電子・電気分野が統合した、いわゆるメカトロニクス
への応用が日常生活に不可欠とも言える自家用車の分野
にも積極的に導入され、TRC、ABSやエアバッグシ
ステムなど電気的にセンシングされた情報をコンピュー
タが判断し、その結果アクチュエータである機械システ
ムが働き、安全性を確保する方法の一手段として利用さ
れている。そしてTRCやエアバッグシステムを作動さ
せるセンサーとして圧力センサーが利用されており、通
常走行中の加速度(G)から衝突時に加わる加速度
(G)(せいぜい0.2〜5.0Gの範囲)を正確に計
測し判断するシステムが作られてきている。In recent years, electronic devices and set parts have tended to have high reliability, high accuracy, small size, light weight, and low cost. Therefore, the same is required for the electronic components used for these components. Recently, the application of so-called mechatronics, which integrates the mechanical and electronic / electrical fields, has been actively introduced into the field of private cars, which can be said to be indispensable for everyday life. Electrical sensing such as TRC, ABS and airbag systems The computer judges the information thus obtained, and as a result, the mechanical system, which is the actuator, operates, and is used as one means of ensuring safety. A pressure sensor is used as a sensor for activating the TRC or the airbag system, and can accurately measure an acceleration (G) applied during a collision from an acceleration (G) during a normal running (a range of 0.2 to 5.0 G at most). Measurement and judgment systems have been created.
【0005】本発明では、従来ある静電容量式の加速度
検知器に圧電振動子を用い、容量変化を周波数変化に置
き換えることにより、現象変化(加速度の検出部である
極小の隙間におけるギャップ)を増幅して検出すること
ができるため、高安定、高精度、高信頼性のものが提供
できる。その主な原理としては、図5に示すように圧電
振動子とそれに直列に接続した容量(負荷容量)の変化
により周波数が変化する特性、すなわち負荷容量特性を
利用することであり、発振器として構成した場合も同様
な傾向の特性が得られる。負荷容量特性は圧電振動子に
直列に接続された容量の変化で、共振周波数は非直線的
に変化するのが特徴である。In the present invention, a piezoelectric vibrator is used as a conventional capacitance type acceleration detector, and a capacitance change is replaced with a frequency change to thereby reduce a phenomenon change (a gap in a very small gap which is an acceleration detecting portion). Since it can be amplified and detected, a highly stable, highly accurate and highly reliable product can be provided. The main principle is to use a characteristic in which the frequency changes due to a change in the piezoelectric vibrator and the capacitance (load capacitance) connected in series with the piezoelectric vibrator, that is, a load capacitance characteristic as shown in FIG. In this case, similar characteristics can be obtained. The load capacitance characteristic is characterized by a change in the capacitance connected in series to the piezoelectric vibrator, and the resonance frequency varies nonlinearly.
【0006】従来の加速度検出器は、加速度変化による
容量変化を直接計測する方法がとられているが、本発明
では圧電振動子を構成する電極の少なくとも一方の電極
と、微少間隔を保って配置された対向電極により形成さ
れる容量(これは圧電振動子に直列に接続されることに
なり負荷容量として使用される)とが発振回路に接続さ
れたものが複数個、同一基板上に対角線状に配置されて
おり、圧電振動子素子が加速度変化の大きさと方向に応
じて変形する。A conventional acceleration detector employs a method of directly measuring a change in capacitance due to a change in acceleration. However, in the present invention, at least one of the electrodes constituting the piezoelectric vibrator is arranged with a small interval. And a capacitor (which is connected in series to the piezoelectric vibrator and used as a load capacitor) formed by the opposing electrodes and a plurality of diagonal lines connected to the oscillation circuit on the same substrate. The piezoelectric vibrator element is deformed according to the magnitude and direction of the change in acceleration.
【0007】その結果、複数個の容量値がそれぞれ変動
し加速度変化量と方向に応じて個々の発振周波数変化が
計測され、これを演算回路で処理することにより加速度
の大きさと方向を発振周波数で検出するものである。な
お、図5からも分かるように容量変化と周波数変化の関
係は、直線的でないので、分解能を良くする場合は、C
Lを小さく設定し、比較的ラフにしたい場合はCLを大
きく(あるいは外付けでCLを付加)するなどの感度調
整も可能となる。As a result, a plurality of capacitance values fluctuate, and individual oscillation frequency changes are measured in accordance with the acceleration change amount and direction, and are processed by an arithmetic circuit to determine the magnitude and direction of the acceleration by the oscillation frequency. It is to detect. As can be seen from FIG. 5, the relationship between the capacitance change and the frequency change is not linear.
If L is set to be small and relatively rough, sensitivity adjustment such as increasing CL (or adding CL externally) becomes possible.
【0008】一方圧電振動子の加工にはエッチング技術
を用いることにより小型化、軽量化が行えることや、一
度の製造工程で複数の圧電振動子の加工が同時に行える
ためコストの低減ができる。また加速度検出器としての
安定度は、従来の静電容量式に比べ元来温度特性が安定
している圧電振動子を用いることに加え、圧電発振器に
培われた温度補償回路を用いることで温度管理も容易に
制御できることから、周囲温度変化にも対応し動作温度
全域にわたり安定した周波数が得られることで安定した
加速度の検出も実現できる。On the other hand, the size and weight of the piezoelectric vibrator can be reduced by using an etching technique for processing the piezoelectric vibrator, and the cost can be reduced because a plurality of piezoelectric vibrators can be processed simultaneously in a single manufacturing process. In addition, the stability of the acceleration detector can be measured by using a temperature compensation circuit cultivated in a piezoelectric oscillator, in addition to using a piezoelectric vibrator whose temperature characteristics are originally stable compared to the conventional capacitance type. Since the management can be easily controlled, a stable frequency can be obtained over the entire operating temperature range in response to changes in the ambient temperature, so that stable acceleration can be detected.
【0009】[0009]
【実施例】以下、添付図面に従ってこの発明の実施例を
説明する。なお、各図において同一の符号は同様の対象
を示すものとする。図1に本発明の圧電発振素子の斜視
図を示す。一例としてエッチング加工により製造された
圧電振動子1を用い、圧電振動子1の同一平面の一部を
抜き加工でスリット部9を形成して4つに分割した構造
で、同一圧電振動子1の平面を両側から挟み込む格好
(図3)で例えばガラス材質から成る容器5と容器6と
で被う形状をした圧電発振素子が構成される。圧電振動
子1と容器5、容器6との接合(挟み込み)には、圧電
振動子1端から出る4カ所の脚7とで行われる。Embodiments of the present invention will be described below with reference to the accompanying drawings. In each drawing, the same reference numeral indicates the same object. FIG. 1 shows a perspective view of the piezoelectric oscillation element of the present invention. As an example, a piezoelectric vibrator 1 manufactured by etching is used, a slit portion 9 is formed by punching a part of the same plane of the piezoelectric vibrator 1 and divided into four parts. A piezoelectric oscillator having a shape sandwiching a flat surface from both sides (FIG. 3) is formed by, for example, a container 5 and a container 6 made of a glass material. The joining (sandwiching) of the piezoelectric vibrator 1 to the container 5 and the container 6 is performed by four legs 7 protruding from the end of the piezoelectric vibrator 1.
【0010】圧電振動子1端から出る4カ所の脚7は、
圧電振動子1の片面の中心部に具備する錘8により圧電
振動子1が自由に撓めるような構造となっている。図1
に示す圧電発振動子1における4カ所の脚7は、圧電振
動子1よりオーバハングした形状となっているが、圧電
振動子1の中心部分に脚7を配置するなど構造の制約は
なく、容器に用いる材質についてもガラス材質以外のセ
ラミックなどでも構わない。また後述するX方向、Y方
向については、図1中にその方向を記載する。なお、錘
8は容器6とはいかなる状態においても接触することは
ない。The four legs 7 protruding from one end of the piezoelectric vibrator 1
The piezoelectric vibrator 1 has a structure in which the piezoelectric vibrator 1 is freely bent by a weight 8 provided at the center of one surface of the piezoelectric vibrator 1. FIG.
Although the four legs 7 of the piezoelectric vibrator 1 shown in FIG. 4 are overhanged from the piezoelectric vibrator 1, there is no structural restriction such as disposing the legs 7 at the center of the piezoelectric vibrator 1, and the container The material to be used may be ceramic other than glass. The X direction and the Y direction described later are described in FIG. The weight 8 does not come into contact with the container 6 in any state.
【0011】図2に示す圧電振動子1の平面図のよう
に、本発明で用いる圧電振動子1は1枚の圧電素板を4
分割し、その各々分割した部分の両面に電極2が有り、
圧電振動子1の背面中心部分に錘8が構成され、同一圧
電素板内にスリット部9による分割で4つの圧電振動子
1が独立して形成されている。As shown in the plan view of the piezoelectric vibrator 1 shown in FIG. 2, the piezoelectric vibrator 1 used in the present invention comprises one piezoelectric element plate.
There are electrodes 2 on both sides of each divided part,
A weight 8 is formed in the center of the back surface of the piezoelectric vibrator 1, and four piezoelectric vibrators 1 are independently formed in the same piezoelectric element plate by division by a slit portion 9.
【0012】この4つの圧電振動子1をそれぞれ1A、
1B、1C、1Dとして説明する。図中には電極2、対
向電極3からの引き回し(電極)は省略している。な
お、圧電振動子1の厚みは30μm、電極2と対向電極
3間の間隔は3〜5μm、電極2と対向電極3の厚みは
それぞれ1500オングストローム程度である。Each of the four piezoelectric vibrators 1 is 1A,
1B, 1C, and 1D. The drawing (electrode) from the electrode 2 and the counter electrode 3 is omitted in the figure. The thickness of the piezoelectric vibrator 1 is 30 μm, the distance between the electrode 2 and the counter electrode 3 is 3 to 5 μm, and the thickness of the electrode 2 and the counter electrode 3 is about 1500 Å.
【0013】圧電振動子1(1A、1B、1C、1D)
に被せる容器5には、圧電振動子1に対向する配置で対
向電極3が配置されている。仮に圧電振動子1の電極2
を圧電振動子1A、圧電振動子1B、圧電振動子1C、
圧電振動子1Dに対応してそれぞれ電極2A、2B、2
C、2Dとした場合、圧電振動子1を容器5で被ったと
きの対向電極3は、それぞれ3A、3B、3C、3Dと
なる。The piezoelectric vibrator 1 (1A, 1B, 1C, 1D)
The counter electrode 3 is disposed in the container 5 covering the piezoelectric vibrator 1 so as to face the piezoelectric vibrator 1. The electrode 2 of the piezoelectric vibrator 1
To the piezoelectric vibrator 1A, the piezoelectric vibrator 1B, the piezoelectric vibrator 1C,
The electrodes 2A, 2B, and 2 correspond to the piezoelectric vibrator 1D, respectively.
In the case of C and 2D, the counter electrodes 3 when the piezoelectric vibrator 1 is covered with the container 5 are 3A, 3B, 3C and 3D, respectively.
【0014】圧電振動子1の電極2や対向電極3からの
電極引き回しは図示していないが、この圧電振動子1の
電極2と容器5の対向電極3との間に発生する容量を、
図6に示す本発明の圧電発振素子を用いて加速度を検出
する回路例により回路を構成したときに、圧電振動子1
の電極2と容器5の対向電極3との容量の変化量からそ
れぞれの周波数が変化し、これらを演算回路で周波数値
を比較することにより、XY平面に平行な任意の加速度
の大きさと方向を検知するものである。Although the wiring of the electrodes from the electrode 2 and the counter electrode 3 of the piezoelectric vibrator 1 is not shown, the capacitance generated between the electrode 2 of the piezoelectric vibrator 1 and the counter electrode 3 of the container 5 is represented by
When a circuit is configured by a circuit example for detecting acceleration using the piezoelectric oscillation element of the present invention shown in FIG.
The respective frequencies change from the amount of change in the capacitance between the electrode 2 and the counter electrode 3 of the container 5, and by comparing the frequency values with an arithmetic circuit, the magnitude and direction of an arbitrary acceleration parallel to the XY plane can be determined. It is to detect.
【0015】図5の負荷容量特性図に示すように、圧電
振動子1に直列に接続された容量の変化で発振周波数が
変化する特性を応用するもので、発振周波数は圧電振動
子1に直列に容量が接続されている場合、容量が増える
と周波数が下がり、しかも直線的でない特性を持ってい
る。As shown in the load capacitance characteristic diagram of FIG. 5, a characteristic in which the oscillation frequency is changed by the change of the capacitance connected in series to the piezoelectric vibrator 1 is applied. When a capacitor is connected to the power supply, the frequency decreases as the capacity increases, and the characteristic is not linear.
【0016】図4に示す、本発明の圧電振動子1を用い
て加速度を検出する様子を示す概念図で説明する。図4
のように紙面の左から右へ加速度が発生すると、圧電振
動子1は錘8の持つ慣性により「く」の字形になる。そ
のため、容量CA、CB、CC、CDが変化するが、C
A、CCは同じ方向へ変化し、CB、CDは逆方向に変
化することにより、CA、CCの容量変化による発振周
波数差は零となりCB、CDの容量変化による発振周波
数のみがΔFとして検出される。FIG. 4 is a conceptual diagram showing how acceleration is detected using the piezoelectric vibrator 1 of the present invention. FIG.
When the acceleration is generated from left to right on the paper as shown in FIG. 3, the piezoelectric vibrator 1 has the shape of a “C” due to the inertia of the weight 8. Therefore, although the capacitances CA, CB, CC, and CD change, C
Since A and CC change in the same direction, and CB and CD change in the opposite direction, the oscillation frequency difference due to the change in the capacitance of CA and CC becomes zero, and only the oscillation frequency due to the change in the capacitance of CB and CD is detected as ΔF. You.
【0017】同様に、紙面に垂直に加速度が発生する
と、やはり容量CA、CB、CC、CDが変化するが、
DB、CDは同じ方向に変化し、CA、CCは逆方向に
変化するので、CB、CD変化による発振周波数は零と
なりCA、CCの容量の変化による発振周波数差のみが
ΔFとして検出される。このようにX方向、Y方向のこ
れらの発振周波数差を更に演算回路で処理することによ
り、XY平面に平行な任意の方向の加速度の方向と大き
さを検出することが可能となる。Similarly, when an acceleration occurs perpendicular to the plane of the paper, the capacitances CA, CB, CC, and CD also change.
Since DB and CD change in the same direction, and CA and CC change in the opposite direction, the oscillation frequency due to the change in CB and CD becomes zero, and only the difference in the oscillation frequency due to the change in the capacitance of CA and CC is detected as ΔF. As described above, by further processing the difference between the oscillation frequencies in the X direction and the Y direction by the arithmetic circuit, it is possible to detect the direction and magnitude of the acceleration in any direction parallel to the XY plane.
【0018】なお、本実施例には圧電振動子1の電極2
と対向する対向電極3は、容器5に構成した内容で記述
してあるが、容器6に対向電極3を構成しても、容器
5、容器6の両方に対向電極3を構成しても構わない。In this embodiment, the electrodes 2 of the piezoelectric vibrator 1 are used.
Although the counter electrode 3 opposing to the above is described in the configuration of the container 5, the counter electrode 3 may be configured in the container 6, or the counter electrode 3 may be configured in both the container 5 and the container 6. Absent.
【0019】[0019]
【発明の効果】本発明による圧電発振素子を加速度検出
器として応用することにより小型、高精度で、かつ安価
に加速度を検出することができる。また、圧電振動子の
周波数変化量を加速度の変化分として検出することで、
動作環境温度の変化に対しては、圧電振動子の温度補償
回路を採用することで高性能な検出も得られる。以上の
ように、小型で安価、高品質の加速度検出器が提供でき
ることにより、手軽に精度の良い加速度検出が行えるよ
うになった。By applying the piezoelectric oscillation element according to the present invention as an acceleration detector, it is possible to detect acceleration at a small size, with high accuracy and at low cost. Also, by detecting the amount of frequency change of the piezoelectric vibrator as the change in acceleration,
For a change in the operating environment temperature, high-performance detection can be obtained by employing a temperature compensation circuit of the piezoelectric vibrator. As described above, by providing a small, inexpensive, and high-quality acceleration detector, acceleration can be easily and accurately detected.
【図1】本発明の圧電発振素子の全体を示す斜視図であ
る。FIG. 1 is a perspective view showing an entire piezoelectric oscillation element of the present invention.
【図2】本発明の圧電発振素子の圧電振動子の平面図で
ある。FIG. 2 is a plan view of a piezoelectric vibrator of the piezoelectric oscillation element according to the present invention.
【図3】本発明の圧電発振素子構造を示す側面図であ
る。FIG. 3 is a side view showing the structure of the piezoelectric oscillation element of the present invention.
【図4】本発明の圧電発振素子を用いて加速度を検出す
る様子を示す概念図である。FIG. 4 is a conceptual diagram showing how acceleration is detected using the piezoelectric oscillation element of the present invention.
【図5】一般的な容量の変化伴う周波数変化を示す負荷
容量特性図である。FIG. 5 is a load capacitance characteristic diagram showing a frequency change with a general capacitance change.
【図6】本発明の圧電発振素子で加速度を検出する回路
例である。FIG. 6 is an example of a circuit for detecting acceleration by the piezoelectric oscillation element of the present invention.
【図7】従来の静電容量式の加速度検出器の断面図であ
る。FIG. 7 is a cross-sectional view of a conventional capacitance type acceleration detector.
1 圧電振動子 2 電極 3 対向電極 4 圧電発振素子 8 錘 DESCRIPTION OF SYMBOLS 1 Piezoelectric vibrator 2 electrode 3 Counter electrode 4 Piezoelectric oscillator 8 Weight
Claims (2)
る面に設けた対向電極間とで容量を持たせる構造を有す
る圧電発振素子において、 該圧電振動子の電極と、該圧電振動子の電極に対向する
少なくとも一面に設けられた対向電極との間に発生する
容量変化で周波数変化を検出することを特徴とする圧電
発振素子。1. A piezoelectric oscillation element having a structure in which a capacitance is provided between an electrode of a piezoelectric vibrator and an opposing electrode provided on a surface facing the electrode, wherein the electrode of the piezoelectric vibrator and the piezoelectric vibrator are provided. A frequency change is detected by a change in capacitance generated between the electrode and a counter electrode provided on at least one surface facing the electrode.
振動子と、該圧電振動子の電極と対向する面に設けた対
向電極間とで容量を持たせる構造を有する圧電発振素子
において、 該圧電素板の片面の中心部に該圧電素板と一体の錘を具
備し、該圧電素板の平面を4分割した両面に電極を有す
る圧電振動子と、該圧電振動子の電極と対向する少なく
とも一面の各々の対向面に構成された対向電極との容量
変化による周波数変化量で、加速度を検知することを特
徴とする圧電発振素子。2. A piezoelectric oscillation element having a structure in which a capacitance is provided between a piezoelectric vibrator having electrodes on both surfaces of the same piezoelectric element plate and a counter electrode provided on a surface of the piezoelectric vibrator facing the electrode, A piezoelectric vibrator having a weight integral with the piezoelectric plate at the center of one surface of the piezoelectric plate, and having electrodes on both surfaces obtained by dividing the plane of the piezoelectric plate into four parts, and opposing the electrodes of the piezoelectric vibrator. A piezoelectric oscillation element for detecting acceleration by an amount of frequency change due to a change in capacitance with respect to at least one opposing electrode formed on each of the opposing surfaces.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21532296A JP3433015B2 (en) | 1996-07-26 | 1996-07-26 | Piezoelectric oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21532296A JP3433015B2 (en) | 1996-07-26 | 1996-07-26 | Piezoelectric oscillator |
Publications (2)
Publication Number | Publication Date |
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JPH1038913A true JPH1038913A (en) | 1998-02-13 |
JP3433015B2 JP3433015B2 (en) | 2003-08-04 |
Family
ID=16670394
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JP21532296A Expired - Fee Related JP3433015B2 (en) | 1996-07-26 | 1996-07-26 | Piezoelectric oscillator |
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JP (1) | JP3433015B2 (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004514894A (en) * | 2000-12-02 | 2004-05-20 | エーアーデーエス・ドイッチュラント・ゲーエムベーハー | Micro inertial sensor |
EP1596208A1 (en) * | 2004-05-14 | 2005-11-16 | Fujitsu Limited | Capacitance difference detecting circuit and mems sensor |
JP2012255669A (en) * | 2011-06-07 | 2012-12-27 | Nippon Dempa Kogyo Co Ltd | Acceleration measuring apparatus |
JP2013029489A (en) * | 2011-01-17 | 2013-02-07 | Nippon Dempa Kogyo Co Ltd | External force detection method and external force detection device |
JP2013033020A (en) * | 2011-01-17 | 2013-02-14 | Nippon Dempa Kogyo Co Ltd | External force detector and external force detection sensor |
JP2014052263A (en) * | 2012-09-06 | 2014-03-20 | Nippon Dempa Kogyo Co Ltd | External force detection device and external force detection sensor |
-
1996
- 1996-07-26 JP JP21532296A patent/JP3433015B2/en not_active Expired - Fee Related
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004514894A (en) * | 2000-12-02 | 2004-05-20 | エーアーデーエス・ドイッチュラント・ゲーエムベーハー | Micro inertial sensor |
EP1596208A1 (en) * | 2004-05-14 | 2005-11-16 | Fujitsu Limited | Capacitance difference detecting circuit and mems sensor |
US7119550B2 (en) | 2004-05-14 | 2006-10-10 | Fujitsu Limited | Capacitance difference detecting circuit and MEMS sensor |
EP1857826A3 (en) * | 2004-05-14 | 2007-12-26 | Fujitsu Ltd. | Capacitance difference detecting circuit and mems sensor |
JP2013029489A (en) * | 2011-01-17 | 2013-02-07 | Nippon Dempa Kogyo Co Ltd | External force detection method and external force detection device |
JP2013033020A (en) * | 2011-01-17 | 2013-02-14 | Nippon Dempa Kogyo Co Ltd | External force detector and external force detection sensor |
JP2012255669A (en) * | 2011-06-07 | 2012-12-27 | Nippon Dempa Kogyo Co Ltd | Acceleration measuring apparatus |
JP2014052263A (en) * | 2012-09-06 | 2014-03-20 | Nippon Dempa Kogyo Co Ltd | External force detection device and external force detection sensor |
Also Published As
Publication number | Publication date |
---|---|
JP3433015B2 (en) | 2003-08-04 |
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