JPH06174476A - Rotation angular velocity sensor - Google Patents

Rotation angular velocity sensor

Info

Publication number
JPH06174476A
JPH06174476A JP4350995A JP35099592A JPH06174476A JP H06174476 A JPH06174476 A JP H06174476A JP 4350995 A JP4350995 A JP 4350995A JP 35099592 A JP35099592 A JP 35099592A JP H06174476 A JPH06174476 A JP H06174476A
Authority
JP
Japan
Prior art keywords
angular velocity
velocity sensor
rotation
rotational angular
pair
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
Application number
JP4350995A
Other languages
Japanese (ja)
Inventor
Shinichi Kuromoto
晋一 黒本
Kazuyoshi Sukai
和義 須貝
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.)
Faurecia Clarion Electronics Co Ltd
Original Assignee
Clarion 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 Clarion Co Ltd filed Critical Clarion Co Ltd
Priority to JP4350995A priority Critical patent/JPH06174476A/en
Publication of JPH06174476A publication Critical patent/JPH06174476A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To provide a small-sized rotation angular velocity sensor with high precision at a low cost. CONSTITUTION:A piezoelectric thin film 12 and a dielectric thin film 13 are formed on a silicon substrate 11 in multiple layers, and electrodes 14, 15 for propagating Lamb waves are formed on the piezoelectric thin film 12 to constitute an oscillating circuit. The silicon at the propagation portion of the Lamb waves is etched from the back face to form a thin plate having the wavelength lower than that of the Lamb waves. When rotation is applied to a rotation angular velocity sensor (a semiconductor element formed on the substrate 11) centering on the Z-axis, the propagation speed of the Lamb waves is changed in response to the rotating direction and the angular velocity OMEGA by the effect of the Coriolis force. The change of the oscillation frequency proportional to the angular velocity OMEGA is outputted as the electric signal (a). This output is detected by a counter 17, the frequency difference is obtained by an arithmetic device 18, and the rotation angular velocity of the rotation angular velocity sensor is calculated from the obtained frequency difference.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は回転角速度センサ(圧電
振動ジャイロ)に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a rotational angular velocity sensor (piezoelectric vibrating gyro).

【0002】[0002]

【従来の技術】従来の回転角速度センサ(圧電振動ジャ
イロ)は音叉型または音片型の振動子に圧電磁器を接着
した構造をしており、励振用圧電磁器と接着層を介して
振動子に与えた振動を、接着層と検出用圧電磁器を介し
て電圧に変換し、検出信号を得る構成をなしている。こ
の動作の基本原理は、振動子の回転角速度に比例したコ
リオリ力により振動子の変位が変調されることを利用
し、検出信号からコリオリ力による変調成分を抽出して
角速度を求める。
2. Description of the Related Art A conventional rotary angular velocity sensor (piezoelectric vibrating gyro) has a structure in which a piezoelectric ceramic is bonded to a tuning fork type or a tuning piece type vibrator, and the piezoelectric vibrator for excitation is bonded to the vibrator via an adhesive layer. The applied vibration is converted into a voltage via the adhesive layer and the piezoelectric ceramic for detection to obtain a detection signal. The basic principle of this operation is that the displacement of the oscillator is modulated by the Coriolis force proportional to the rotational angular velocity of the oscillator, and the modulation component due to the Coriolis force is extracted from the detection signal to obtain the angular velocity.

【0003】図4は現在実用化されている正三角形音片
型振動子を用いた回転角速度センサの構成及びその周辺
装置の例を示す斜視図及びブロック図である。図4
(A)に示すように、圧電振動ジャイロ40は恒弾性金
属材料で作成された正三角形音片型振動子41の3辺に
励振用及び検出用圧電磁器42を接着剤で張り合わせた
構造をなしている。
FIG. 4 is a perspective view and a block diagram showing a configuration of a rotational angular velocity sensor using an equilateral triangular sound piece type vibrator which is currently in practical use and an example of a peripheral device thereof. Figure 4
As shown in (A), the piezoelectric vibrating gyro 40 has a structure in which an exciting and detecting piezoelectric ceramic 42 is attached to three sides of an equilateral triangular sound piece type oscillator 41 made of a constant elastic metal material with an adhesive. ing.

【0004】回路構成としては図4(B)に示すように
正三角形音片型ジャイロ40の左右2辺の圧電磁器42
−42を駆動用として用い、残る1辺の圧電磁器42を
帰還用として発振回路43、位相補正回路45と共に自
励振による発振回路を構成する。また、左右2辺の圧電
磁器42−42は検出用として兼用し、差動回路44の
差動出力を同期検波回路46及び直流増幅器47で処理
することによりコリオリ信号を抽出する。
As a circuit configuration, as shown in FIG. 4B, the piezoelectric ceramics 42 on the left and right sides of the equilateral triangular sound piece type gyro 40.
The -42 is used for driving, and the remaining one side of the piezoelectric ceramic 42 is used for feedback together with the oscillation circuit 43 and the phase correction circuit 45 to form an oscillation circuit by self-excitation. The left and right piezoelectric ceramics 42-42 are also used for detection, and the differential output of the differential circuit 44 is processed by the synchronous detection circuit 46 and the DC amplifier 47 to extract the Coriolis signal.

【0005】[0005]

【発明が解決しようとする課題】しかしながら、従来の
音片型振動子に圧電磁器を接着した構造の回転角速度セ
ンサは、圧電磁器を振動子に接着剤で張り合わせる工程
を必要とするため、位置ずれが生じやすい等、機械工作
上精度に問題があり、このためセンサの性能の再現性が
悪く、また、歩留りの等生産性の向上やコストダウンや
小型化も困難であるという問題点があった。
However, the conventional rotary angular velocity sensor having a structure in which the piezoelectric ceramic is bonded to the sound piece type vibrator requires a step of adhering the piezoelectric ceramic to the vibrator with an adhesive. There is a problem in mechanical precision such as misalignment.Therefore, the reproducibility of sensor performance is poor, and it is difficult to improve productivity such as yield, reduce cost, and reduce size. It was

【0006】本発明は、上記問題点を解消するためにな
されたものであり、精度の良い、小型、低コストの回転
角速度センサを提供することを目的とする。
The present invention has been made to solve the above problems, and an object of the present invention is to provide a highly accurate, small-sized, low-cost rotation angular velocity sensor.

【0007】弾性波(SAW,Lamb波)が伝搬する煤
質が回転運動(回転ベクトルは波の進行方向と基盤の深
さ方向に垂直)をすると、コリオリ力が働き、波の伝搬
速度が変化する。この伝搬速度の変化から回転角速度を
検出するのが、SAW、Lamb波を用いた振動ジャイロ
の動作原理である。従来はコリオリ力により振動子の変
位が変調され、これにより回転角速度が検出されたが本
発明では伝搬速度が変調される。
When the soot that propagates the elastic waves (SAW, Lamb waves) makes a rotational motion (the rotation vector is perpendicular to the traveling direction of the wave and the depth direction of the substrate), Coriolis force works and the propagation velocity of the wave changes. To do. Detecting the rotational angular velocity from the change in the propagation velocity is the operating principle of the vibration gyro using SAW and Lamb waves. Conventionally, the displacement of the oscillator is modulated by the Coriolis force, and the rotational angular velocity is detected by this, but in the present invention, the propagation velocity is modulated.

【0008】ナビゲーション等への応用を考えた場合、
ジャイロは比較的小さな回転角速度を検出するセンサと
見做すことができる。そのため弾性波を用いた振動ジャ
イロは本質的に低周波動作が要求されると考えられる。
SAWを用いた場合、低周波化により素子サイズが大き
くなる可能性が懸念される。弾性波として反対称モード
のLamb波に着目すると、図5に示すようにプレートの
厚みを極めて薄くすることで波の伝搬速度を小さくでき
るという性質があり、低周波動作する上で大きな利点を
有している。
Considering the application to navigation, etc.,
The gyro can be regarded as a sensor that detects a relatively small rotational angular velocity. Therefore, it is considered that the low-frequency operation is essentially required for the vibration gyro using elastic waves.
When SAW is used, there is a concern that the element size may increase due to the low frequency. Focusing on antisymmetric Lamb waves as elastic waves, as shown in FIG. 5, there is a property that the propagation speed of the waves can be reduced by making the plate extremely thin, which is a great advantage in operating at low frequencies. is doing.

【0009】[0009]

【課題を解決するための手段】そこで、前記の目的を達
成するために第1の発明による回転角速度センサは、所
定の基盤上に設けられた誘電体膜層及び圧電膜層によっ
て形成される半導体素子と、圧電膜層に形成された、所
定のモードの弾性波を伝搬させるための一対の電極と、
半導体素子の回転に伴う所定モードの弾性波の変化を検
出する検出装置と、検出装置により検出された周波数の
変化から半導体素子の回転角速度を算出する演算装置
と、を有することを特徴とする。
In order to achieve the above-mentioned object, the rotational angular velocity sensor according to the first invention is a semiconductor formed by a dielectric film layer and a piezoelectric film layer provided on a predetermined substrate. An element and a pair of electrodes formed on the piezoelectric film layer for propagating an elastic wave of a predetermined mode,
It is characterized by including a detection device that detects a change in elastic wave in a predetermined mode due to rotation of the semiconductor element, and an arithmetic device that calculates a rotational angular velocity of the semiconductor element from a change in frequency detected by the detection device.

【0010】第2の発明は上記第1の発明による回転角
速度センサにおいて、所定モードの弾性波がLamb波で
あることを特徴とする。
A second invention is characterized in that, in the rotational angular velocity sensor according to the first invention, the elastic wave in a predetermined mode is a Lamb wave.

【0011】また、第3の発明による回転角速度センサ
は、所定の基盤上に設けられた誘電体膜層及び圧電膜層
によって形成される一対の半導体素子と、それぞれの半
導体素子上の圧電膜層に形成された、所定のモードの弾
性波をそれぞれ逆方向に伝搬させるための一対の電極
と、一対の半導体素子の回転に伴う各半導体素子におけ
る所定モードの弾性波の周波数を検出する検出装置と、
それぞれ検出された周波数の差を求めることにより、一
対の半導体素子の回転角速度を算出する演算装置と、を
有することを特徴とする。
The rotational angular velocity sensor according to the third aspect of the invention is a pair of semiconductor elements formed by a dielectric film layer and a piezoelectric film layer provided on a predetermined substrate, and a piezoelectric film layer on each semiconductor element. A pair of electrodes for propagating elastic waves of a predetermined mode in opposite directions, respectively, and a detection device for detecting the frequency of the elastic wave of a predetermined mode in each semiconductor element accompanying the rotation of the pair of semiconductor elements; ,
And an arithmetic unit for calculating the rotational angular velocities of the pair of semiconductor elements by obtaining the difference between the respective detected frequencies.

【0012】第4の発明は上記第2の発明による回転角
速度センサにおいて、所定モードの弾性波がLamb波で
あることを特徴とする。
A fourth invention is characterized in that, in the rotational angular velocity sensor according to the second invention, the elastic wave of a predetermined mode is a Lamb wave.

【0013】[0013]

【作用】上記構成により第1の発明による回転角速度セ
ンサは、圧電膜層に形成された一対の電極により所定の
モードの弾性波を伝搬させ、検出装置により半導体素子
の回転に伴う所定モードの弾性波の変化を検出し、演算
装置で検出装置により検出された周波数差から半導体素
子の回転角速度を算出する。
With the above structure, the rotational angular velocity sensor according to the first aspect of the invention propagates the elastic wave of a predetermined mode by the pair of electrodes formed on the piezoelectric film layer, and the detection device elastically moves in a predetermined mode as the semiconductor element rotates. The change in the wave is detected, and the rotational angular velocity of the semiconductor element is calculated from the frequency difference detected by the detection device by the arithmetic device.

【0014】また、第3の発明による回転角速度センサ
は、それぞれの半導体素子上の圧電膜層に形成された一
対の電極により、所定のモードの弾性波をそれぞれ逆方
向に伝搬させ、検出装置により一対の半導体素子の回転
に伴う各半導体素子における所定モードの弾性波の周波
数を検出し、演算装置によりそれぞれ検出された周波数
の差を求めることにより、一対の半導体素子の回転角速
度を算出する。
In the rotational angular velocity sensor according to the third aspect of the invention, a pair of electrodes formed on the piezoelectric film layer on each semiconductor element causes elastic waves of a predetermined mode to propagate in opposite directions, and a detection device is used. The rotational angular velocity of the pair of semiconductor elements is calculated by detecting the frequency of the elastic wave in a predetermined mode in each semiconductor element due to the rotation of the pair of semiconductor elements and obtaining the difference between the frequencies detected by the arithmetic unit.

【0015】[0015]

【実施例】【Example】

〈実施例1〉図1は本発明に基づく回転角速度センサの
一実施例の構造を示す。図1(A)において、シリコン
(Si)基盤11上に圧電体薄膜12と共に誘電体薄膜
13を多層に形成し、圧電体薄膜12上にLamb波を伝
搬させるための電極14,15を形成し、増幅器16と
共に発振回路10を構成する。ここで、圧電体薄膜1
2、誘電体薄膜13の組合せとしてはZnO(酸化亜
鉛)/SiN(窒素珪素)等が考えられるが、これ以外
の薄膜の組合せも可能である。薄膜の組合せによる性能
向上の可能性がある。
<Embodiment 1> FIG. 1 shows the structure of an embodiment of a rotational angular velocity sensor according to the present invention. In FIG. 1A, a dielectric thin film 13 is formed in multiple layers together with a piezoelectric thin film 12 on a silicon (Si) substrate 11, and electrodes 14 and 15 for propagating Lamb waves are formed on the piezoelectric thin film 12. , The amplifier 16 and the oscillation circuit 10 are configured. Here, the piezoelectric thin film 1
2. ZnO (zinc oxide) / SiN (silicon nitride) or the like can be considered as the combination of the dielectric thin film 13, but other thin film combinations are also possible. There is a possibility of improving performance by combining thin films.

【0016】Lamb波の伝搬部分のシリコンを裏面から
エッチングし、Lamb波の波長以下の薄いプレートとす
る。これはLamb波の伝搬モードとして音速の遅い反対
称モードを用いるためである。z軸を中心として回転角
速度センサ(基盤11上に形成された半導体素子)に回
転が加わるとコリオリ力の影響でLamb波の伝搬速度が
回転方向及び角速度に応じて変化する。これが角速度Ω
に比例した発振周波数の変化が電気信号aとして出力す
る。この出力をカウンタ17で検出し、演算装置18で
周波数差を求め、得られた周波数差から回転角速度セン
サの回転角速度を算出する。出力aは発振周波数fの変
化分として検出される。回転角速度センサが回転してい
ない時の周波数をf0、回転時の周波数f0からのずれ
を△fとすると図1(B)に示すようになる。
Silicon in the Lamb wave propagation portion is etched from the back surface to form a thin plate having a Lamb wave wavelength or less. This is because an antisymmetric mode having a slow sound velocity is used as a propagation mode of Lamb waves. When the rotation angular velocity sensor (semiconductor element formed on the substrate 11) is rotated about the z-axis, the propagation velocity of the Lamb wave changes according to the rotation direction and the angular velocity due to the influence of the Coriolis force. This is the angular velocity Ω
A change in the oscillation frequency proportional to is output as an electric signal a. This output is detected by the counter 17, the frequency difference is obtained by the arithmetic unit 18, and the rotational angular velocity of the rotational angular velocity sensor is calculated from the obtained frequency difference. The output a is detected as a change in the oscillation frequency f. If the frequency when the rotation angular velocity sensor is not rotating is f0, and the deviation from the frequency f0 when rotating is Δf, the result is as shown in FIG. 1 (B).

【0017】〈実施例2〉図2は本発明に基づく回転角
速度センサの他の実施例の構造を示し、図3は発振周波
数の特性図である。図2(A)において、図1(A)に
示した発振回路と同様の構造を有する同一特性の一対の
発振回路21,22を互いにLamb波の向きが逆になる
ように配置し、z軸を中心として正の向きの回転が加わ
ると、コリオリ力の影響でxの正の向きに伝搬するLam
b波の伝搬速度は大きくなる。逆にxの負の向きに伝搬
するLamb波の伝搬速度は小さくなる。
<Embodiment 2> FIG. 2 shows the structure of another embodiment of the rotational angular velocity sensor according to the present invention, and FIG. 3 is a characteristic diagram of the oscillation frequency. In FIG. 2A, a pair of oscillation circuits 21 and 22 having the same characteristics as the oscillation circuit shown in FIG. 1A and having the same characteristics are arranged so that the Lamb waves have opposite directions, and the z-axis Lamb propagates in the positive direction of x under the influence of the Coriolis force when a rotation in the positive direction about
The propagation velocity of b-wave becomes large. On the contrary, the propagation speed of the Lamb wave propagating in the negative direction of x becomes small.

【0018】回転角速度Ωは周波数f1の出力23と周
波数f2の出力24の周波数差として検出することがで
きる。図2(B)に示すように発振回路21,22から
の出力バルス23,24をそれぞれカウンタ31,32
で検出し、演算回路33で周波数差を得て回転角速度セ
ンサの回転角速度を算出する。2つの出力の周波数差を
使うことにより、温度変化等による周波数のドリフトの
影響をキャンセルし、センサ性能の向上が期待できる。
The rotational angular velocity Ω can be detected as a frequency difference between the output 23 of the frequency f1 and the output 24 of the frequency f2. As shown in FIG. 2B, the output pulses 23 and 24 from the oscillation circuits 21 and 22 are counted by the counters 31 and 32, respectively.
Then, the arithmetic circuit 33 obtains the frequency difference to calculate the rotational angular velocity of the rotational angular velocity sensor. By using the frequency difference between the two outputs, it is possible to cancel the influence of frequency drift due to temperature changes and the like, and improve the sensor performance.

【0019】[0019]

【発明の効果】以上説明したように本発明の回転角速度
センサによれば、シリコン基盤上に圧電体薄膜と誘電体
薄膜を多層に形成した構造を用いることで、Lamb波を
利用した回転角速度センサの実現が可能となる。これに
より、半導体プロセス技術を用いて製造できる、小型、
低コストの回転角速度センサを実現し得る。更に、周辺
回路を同一基盤上に集積化した高性能センサを実現し得
る。
As described above, according to the rotational angular velocity sensor of the present invention, the rotational angular velocity sensor utilizing the Lamb wave is used by using the structure in which the piezoelectric thin film and the dielectric thin film are formed in multiple layers on the silicon substrate. Can be realized. This makes it possible to manufacture using semiconductor process technology,
A low-cost rotation angular velocity sensor can be realized. Furthermore, it is possible to realize a high-performance sensor in which peripheral circuits are integrated on the same substrate.

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

【図1】本発明に基づく回転角速度センサの一実施例の
構造を示す図である。
FIG. 1 is a diagram showing a structure of an embodiment of a rotational angular velocity sensor according to the present invention.

【図2】本発明に基づく回転角速度センサの他の実施例
の構造を示す図である。
FIG. 2 is a diagram showing the structure of another embodiment of the rotational angular velocity sensor according to the present invention.

【図3】発振周波数の特性図である。FIG. 3 is a characteristic diagram of an oscillation frequency.

【図4】従来の回転角速度センサの例である。FIG. 4 is an example of a conventional rotation angular velocity sensor.

【図5】Lamb波の分散関係である。FIG. 5 is a dispersion relation of Lamb waves.

【符号の説明】[Explanation of symbols]

10,21,22 発振回路(半導体素子) 12 圧電体薄膜(圧電体薄膜層) 13 誘電体薄膜(誘電体薄膜層) 14,15 電極 17,31,32 カウンタ(検出装置) 18,33 演算装置 10, 21 and 22 Oscillation circuit (semiconductor element) 12 Piezoelectric thin film (piezoelectric thin film layer) 13 Dielectric thin film (dielectric thin film layer) 14, 15 Electrode 17, 31, 32 Counter (detecting device) 18, 33 Arithmetic device

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 所定の基盤上に設けられた誘電体膜層及
び圧電膜層によって形成される半導体素子と、前記圧電
膜層に形成された、所定のモードの弾性波を伝搬させる
ための一対の電極と、前記半導体素子の回転に伴う前記
所定モードの弾性波の変化を検出する検出装置と、前記
検出装置により検出された周波数の変化から前記半導体
素子の回転角速度を算出する演算装置と、を有すること
を特徴とする回転角速度センサ。
1. A semiconductor element formed of a dielectric film layer and a piezoelectric film layer provided on a predetermined substrate, and a pair formed on the piezoelectric film layer for propagating elastic waves of a predetermined mode. An electrode, a detection device that detects a change in the elastic wave in the predetermined mode due to the rotation of the semiconductor element, and an arithmetic device that calculates the rotational angular velocity of the semiconductor element from the change in the frequency detected by the detection device, A rotational angular velocity sensor having:
【請求項2】 請求項1記載の回転角速度センサにおい
て、所定モードの弾性波がLamb波であることを特徴と
する回転角速度センサ。
2. The rotational angular velocity sensor according to claim 1, wherein the elastic wave in the predetermined mode is a Lamb wave.
【請求項3】 所定の基盤上に設けられた誘電体膜層及
び圧電膜層によって形成される一対の半導体素子と、前
記それぞれの半導体素子上の圧電膜層に形成された、所
定のモードの弾性波をそれぞれ逆方向に伝搬させるため
の一対の電極と、前記一対の半導体素子の回転に伴う各
半導体素子における前記所定モードの弾性波の周波数を
検出する検出装置と、それぞれ検出された周波数の差を
求めることにより、前記一対の半導体素子の回転角速度
を算出する演算装置と、を有することを特徴とする回転
角速度センサ。
3. A pair of semiconductor elements formed by a dielectric film layer and a piezoelectric film layer provided on a predetermined base, and a pair of semiconductor elements of a predetermined mode formed on the piezoelectric film layer on each of the semiconductor elements. A pair of electrodes for propagating the elastic waves in opposite directions, a detection device for detecting the frequency of the elastic wave in the predetermined mode in each semiconductor element accompanying the rotation of the pair of semiconductor elements, and the detected frequency A rotation angular velocity sensor, comprising: an arithmetic unit that calculates a rotation angular velocity of the pair of semiconductor elements by obtaining a difference.
【請求項4】 請求項3記載の回転角速度センサにおい
て、所定モードの弾性波がLamb波であることを特徴と
する回転角速度センサ。
4. The rotational angular velocity sensor according to claim 3, wherein the elastic wave in the predetermined mode is a Lamb wave.
JP4350995A 1992-12-04 1992-12-04 Rotation angular velocity sensor Pending JPH06174476A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4350995A JPH06174476A (en) 1992-12-04 1992-12-04 Rotation angular velocity sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4350995A JPH06174476A (en) 1992-12-04 1992-12-04 Rotation angular velocity sensor

Publications (1)

Publication Number Publication Date
JPH06174476A true JPH06174476A (en) 1994-06-24

Family

ID=18414326

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4350995A Pending JPH06174476A (en) 1992-12-04 1992-12-04 Rotation angular velocity sensor

Country Status (1)

Country Link
JP (1) JPH06174476A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004010081A1 (en) * 2002-07-23 2004-01-29 National Institute Of Advanced Industrial Science And Technology Method and device for accurately detecting attitude of movable body
JP2008026275A (en) * 2006-07-25 2008-02-07 Denso Corp Surface acoustic wave angular velocity sensor
US8256289B2 (en) 2006-07-25 2012-09-04 Denso Corporation Angular rate sensor

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004010081A1 (en) * 2002-07-23 2004-01-29 National Institute Of Advanced Industrial Science And Technology Method and device for accurately detecting attitude of movable body
JP2008026275A (en) * 2006-07-25 2008-02-07 Denso Corp Surface acoustic wave angular velocity sensor
US8256289B2 (en) 2006-07-25 2012-09-04 Denso Corporation Angular rate sensor

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