JPH087068B2 - Sound piece type vibration gyro - Google Patents

Sound piece type vibration gyro

Info

Publication number
JPH087068B2
JPH087068B2 JP3196685A JP3196685A JPH087068B2 JP H087068 B2 JPH087068 B2 JP H087068B2 JP 3196685 A JP3196685 A JP 3196685A JP 3196685 A JP3196685 A JP 3196685A JP H087068 B2 JPH087068 B2 JP H087068B2
Authority
JP
Japan
Prior art keywords
sound piece
piezoelectric ceramic
piece type
type vibration
vibration gyro
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.)
Expired - Fee Related
Application number
JP3196685A
Other languages
Japanese (ja)
Other versions
JPS61191918A (en
Inventor
正 近野
博章 山田
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP3196685A priority Critical patent/JPH087068B2/en
Publication of JPS61191918A publication Critical patent/JPS61191918A/en
Publication of JPH087068B2 publication Critical patent/JPH087068B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は回転速度を検出するための音片型振動ジヤイ
ロに関する。
Description: TECHNICAL FIELD The present invention relates to a sound piece type vibration gyro for detecting a rotation speed.

〔従来の技術〕[Conventional technology]

従来の音片型振動ジヤイロを第3図(a),(b)お
よび(c)に例示する。本図において、断面が正方形の
音片1の一つの側面の中央に駆動用の圧電セラミック2
および前記側面と直角をなす隣の側面の中央に抽出用の
圧電セラミック3が接着されている。本音片型振動ジヤ
イロにおいて駆動用の圧電セラミック2に信号を加える
と、音片は第3図(b)のような振動モードでX軸方向
の屈曲振動をするが、抽出用の圧電セラミックが、駆動
用の圧電セラミックの接着面と直角に側面中央部に接着
されているので、抽出用圧電セラミック内に発生する電
荷は正負同量となり打消し合う。したがって抽出用の圧
電セラミックには週力が発生しない。しかし、本音片型
振動ジヤイロを第3図(a)に示したようにZ軸で回転
させると、コリオリの力によるY軸方向の力が発生し、
第3図(c)に示したようなY軸方向の横振動も発生す
る。したがって、抽出用圧電セラミックに出力を生じ
る。コリオリの力Fcは次式で表わされる。
A conventional sound piece type vibration gyro is illustrated in FIGS. 3 (a), (b) and (c). In this figure, a piezoelectric ceramic 2 for driving is placed at the center of one side surface of a sound piece 1 having a square cross section.
The piezoelectric ceramic 3 for extraction is adhered to the center of the adjacent side surface that is perpendicular to the side surface. When a signal is applied to the driving piezoelectric ceramic 2 in the sound piece type vibration gyro, the sound piece makes bending vibration in the X-axis direction in the vibration mode as shown in FIG. 3B, but the extraction piezoelectric ceramic Since the driving piezoelectric ceramic is bonded to the central portion of the side surface at a right angle to the bonding surface, the charges generated in the extracting piezoelectric ceramic have the same positive and negative amounts and cancel each other out. Therefore, no week force is generated in the piezoelectric ceramic for extraction. However, when the real piece vibration gyro is rotated about the Z axis as shown in FIG. 3 (a), a force in the Y axis direction due to the Coriolis force is generated,
Lateral vibration in the Y-axis direction as shown in FIG. 3 (c) is also generated. Therefore, an output is produced in the extracting piezoelectric ceramic. The Coriolis force Fc is expressed by the following equation.

Fc=−2mΩ この式で:mは等価質量,Ωは回転の角速度,はY軸
方向の速度である。
Fc = −2mΩ In this formula: m is the equivalent mass, Ω is the angular velocity of rotation, and is the velocity in the Y-axis direction.

以上のように、抽出用圧電セラミックに発生する出力
によりZ軸に対する回転の角速度を検出することができ
る。
As described above, the angular velocity of rotation with respect to the Z axis can be detected by the output generated in the extracting piezoelectric ceramic.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

上述した従来の音片型振動ジヤイロは、駆動用および
抽出用の圧電セラミックが音片の各々の面の中央に正確
に接着することにより、駆動用の圧電セラミックでは、
X方向の振動を駆動せず、また抽出用の圧電セラミック
ではY方向の振動を抽出しない構成となっている。した
がって、圧電セラミックの接着位置が正確に面の中央で
なく多少でもずれた場合には、駆動用の圧電セラミック
によりX方向の振動も駆動される。また、同様に、抽出
用圧電セラミックでもY方向の振動も抽出する。そのた
め音片型振動ジヤイロが回転しない場合にも出力が発生
し、回転成分のみを正確に検出できなくなるという欠点
がある。さらに、駆動用圧電セラミックと抽出用圧電セ
ラミックの距離が近いため、双方の圧電セラミック間で
容量を持ち直接圧電セラミック間で信号が漏れて、無回
転時にも出力を発生し易いという欠点もある。
In the conventional sound piece type vibration gyroscope described above, the driving and extracting piezoelectric ceramics are accurately adhered to the centers of the respective surfaces of the sound piece, so that in the driving piezoelectric ceramics,
The vibration in the X direction is not driven, and the piezoelectric ceramic for extraction does not extract the vibration in the Y direction. Therefore, when the bonding position of the piezoelectric ceramic is not exactly in the center of the surface but is slightly displaced, vibration in the X direction is also driven by the driving piezoelectric ceramic. Similarly, the piezoelectric ceramic for extraction also extracts vibration in the Y direction. Therefore, there is a drawback that an output is generated even when the sound piece type vibration gyro does not rotate, and only the rotation component cannot be accurately detected. Further, since the driving piezoelectric ceramic and the extracting piezoelectric ceramic are close to each other, there is a drawback that a capacitance exists between both piezoelectric ceramics and a signal leaks directly between the piezoelectric ceramics, so that an output is easily generated even when there is no rotation.

〔問題点を解決するための手段〕[Means for solving problems]

本発明の目的は上述の欠点を除去した音片型振動ジヤ
イロを提供することにある。
An object of the present invention is to provide a sound piece type vibration gyro which eliminates the above-mentioned drawbacks.

本発明の音片型振動ジヤイロは、正方形の一つの角に
面取りを施した断面をもつ音片と、その音片の面取りに
隣接した1つの側面に接着した一枚の圧電セラミック
と、前記側面に隣接する2つの側面にそれぞれ一枚づつ
接着された一対の圧電セラミックとを有している。
The sound piece type vibrating gyroscope of the present invention comprises a sound piece having a cross section in which one corner of a square is chamfered, one piezoelectric ceramic bonded to one side surface adjacent to the chamfer of the sound piece, and the side surface. And a pair of piezoelectric ceramics, one of which is adhered to each of the two side surfaces adjacent to each other.

〔実施例〕〔Example〕

次に、本発明について図面を参照して説明する。 Next, the present invention will be described with reference to the drawings.

第1図(a),(b)および(c)に本発明の実施例
の斜視図,正面時および右側面図である。本図におい
て、面取り部4を持つ音片1の面取り部に接した一側面
には駆動用圧電セラミック2が接着されている。また、
駆動用圧電セラミックが接着されている面に隣接する2
つの側面にはそれぞれ1枚づつ抽出用圧電セラミック3,
3′が接着されている。そしてこれらの抽出用圧電セラ
ミックはそれぞれの接着面上で駆動側の圧電セラミック
の接着面とは反対側の面と接する角に沿って配置されて
いる。第1図(c)で+−は圧電セラミックの分極方向
を示すための表側の極性の表示である。本音片型振動ジ
ャイロで、駆動用圧電セラミックに信号を入力すると、
第1図(c)に示すように、駆動用圧電セラミック2の
近傍に面取り部4があるので、X方向およびY方向に縮
退した振動モードの2つの振動が励起される。双方の振
動により抽出用圧電セラミック3および3′には極性が
逆で、同量の電荷が発生するため、電荷は相殺される。
したがって無回転時には出力は発生しない。そして、回
転があった場合には、次式のコリオリの力Fxy(X成
分),Fxy(Y成分)が発生する。
1 (a), (b) and (c) are a perspective view, a front view and a right side view of an embodiment of the present invention. In the figure, a driving piezoelectric ceramic 2 is bonded to one side surface of the sound piece 1 having a chamfered portion 4 in contact with the chamfered portion. Also,
Adjacent to the surface where the driving piezoelectric ceramic is bonded 2
One piezoelectric ceramic for extraction on each side 3,
3'is glued. These extraction piezoelectric ceramics are arranged on the respective bonding surfaces along the corners that contact the surface on the opposite side of the bonding surface of the driving-side piezoelectric ceramics. In FIG. 1 (c), +-is a display of the polarity on the front side to indicate the polarization direction of the piezoelectric ceramic. With this sound piece type vibration gyro, when a signal is input to the driving piezoelectric ceramic,
As shown in FIG. 1C, since the chamfered portion 4 is provided in the vicinity of the driving piezoelectric ceramic 2, two vibrations in a vibration mode degenerated in the X direction and the Y direction are excited. Both vibrations have opposite polarities in the extracting piezoelectric ceramics 3 and 3 ', and the same amount of electric charge is generated, so that the electric charges are canceled.
Therefore, no output is generated when there is no rotation. When there is rotation, Coriolis forces Fxy (X component) and Fxy (Y component) of the following equations are generated.

Fxy=2m2Ω Fxy=−2m1Ω ここでm1,m2は等価質量,Ωは回転の角速度,およ
びはそれぞれX軸およびY軸方向の速度である。これ
らのX方向及びY方向に発生するFxy(X成分)、Fxy
(Y成分)は、等価質量m1、m2が異なるため、違った値
となる。従って、抽出用圧電セラミック3および3′に
発生する電荷の量も異なってくるため、出力を発生す
る。本音片型振動子の等価回路を第2図に示す。本回路
ではZ1=Z2なので無回転はFxy=0,Fxy=0となり出力は
0となる。回転時にはFxy≠0,Fxy≠0となり出力を発生
する。
Fxy = 2m 2 Ω Fxy = −2m 1 Ω where m 1 and m 2 are equivalent masses, Ω is the angular velocity of rotation, and is the velocity in the X-axis and Y-axis directions, respectively. Fxy (X component) generated in these X direction and Y direction, Fxy
The (Y component) has different values because the equivalent masses m 1 and m 2 are different. Therefore, the amount of electric charge generated in the extracting piezoelectric ceramics 3 and 3'is also different, so that an output is generated. An equivalent circuit of the present sound piece type vibrator is shown in FIG. Since Z 1 = Z 2 in this circuit, non-rotation results in Fxy = 0, Fxy = 0 and output is 0. At the time of rotation, Fxy ≠ 0 and Fxy ≠ 0, and an output is generated.

本発明の音片型振動ジヤイロでは抽出側の圧電セラミ
ックが音片の角に沿って配置されるので、圧電セラミッ
クの位置決めが容易で位置ずれを起こしにくいという特
長を有している。また、駆動側と抽出側の圧電セラミッ
ク間の距離を大きくとれるので、双方の圧電セラミック
間の静電的な結合も小さいといる利点もある。
In the sound piece type vibration gyroscope of the present invention, since the piezoelectric ceramics on the extraction side are arranged along the corners of the sound piece, the piezoelectric ceramics can be easily positioned and are not easily displaced. Further, since the distance between the piezoelectric ceramics on the drive side and the extraction side can be made large, there is an advantage that the electrostatic coupling between both piezoelectric ceramics is also small.

〔発明の効果〕〔The invention's effect〕

以上説明したように、本発明には、抽出側の圧電セラ
ミックを2枚に分けることにより、接着位置ずれを起し
にくく、入出力間の結合を小さくできる効果がある。
As described above, according to the present invention, by dividing the piezoelectric ceramic on the extraction side into two pieces, the displacement of the bonding position is unlikely to occur, and the coupling between the input and the output can be reduced.

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

第1図(a),(b)および(c)はそれぞれ本発明の
音片型振動ジヤイロの斜視図,正面図および右側面図、
第2図は本発明の音片型振動ジヤイロの等価回路図、第
3図(a)は従来の音片型振動ジヤイロの斜視図、第3
図(b)および(c)ぱ振動モードを説明するための図
である。 図において、1……音片、2……駆動側圧電セラミッ
ク、3,3′……抽出側圧電セラミック、4……面取り
部。
1 (a), (b) and (c) are respectively a perspective view, a front view and a right side view of a sound piece type vibration gyro according to the present invention,
FIG. 2 is an equivalent circuit diagram of the sound piece type vibration gyro of the present invention, and FIG. 3 (a) is a perspective view of a conventional sound piece type vibration gyro.
It is a figure for explaining the figure (b) and (c) vibration mode. In the figure, 1 ... sound piece, 2 ... drive side piezoelectric ceramic, 3,3 '... extraction side piezoelectric ceramic, 4 ... chamfered portion.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】一つの角が面取りされた正方形の断面を持
つ音片と、該音片の側面に接着された3枚の圧電セラミ
ックとから構成される音片型振動ジヤイロにおいて、前
記圧電セラミックの一枚は前記面取りと接した側面に配
置され、同一形状の残りの2枚は前記一側面と隣接する
2つの側面上にそれぞれ前記一側面と接しない角部に沿
って配置されたことを特徴とする音片型振動ジヤイロ。
1. A sound piece type vibrating gyroscope comprising a sound piece having a square cross section with one corner chamfered and three piezoelectric ceramics bonded to the side surfaces of the sound piece. One of the sheets is arranged on the side surface in contact with the chamfer, and the remaining two sheets of the same shape are arranged on two side surfaces adjacent to the one side surface along the corners not in contact with the one side surface, respectively. Characteristic type vibration gyro.
JP3196685A 1985-02-20 1985-02-20 Sound piece type vibration gyro Expired - Fee Related JPH087068B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3196685A JPH087068B2 (en) 1985-02-20 1985-02-20 Sound piece type vibration gyro

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3196685A JPH087068B2 (en) 1985-02-20 1985-02-20 Sound piece type vibration gyro

Publications (2)

Publication Number Publication Date
JPS61191918A JPS61191918A (en) 1986-08-26
JPH087068B2 true JPH087068B2 (en) 1996-01-29

Family

ID=12345693

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3196685A Expired - Fee Related JPH087068B2 (en) 1985-02-20 1985-02-20 Sound piece type vibration gyro

Country Status (1)

Country Link
JP (1) JPH087068B2 (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5874674A (en) * 1988-08-12 1999-02-23 Murata Manufacturing Co., Ltd. Vibrator including piezoelectric electrodes or detectors arranged to be non-parallel and non-perpendicular to coriolis force direction and vibratory gyroscope using the same
JPH0354414A (en) * 1989-07-24 1991-03-08 Yazaki Corp Angular velocity sensor
JPH0760095B2 (en) * 1992-11-13 1995-06-28 株式会社村田製作所 Vibrating gyro
JPH0760094B2 (en) * 1992-11-13 1995-06-28 株式会社村田製作所 Vibrating gyro
JPH0762617B2 (en) * 1993-03-08 1995-07-05 株式会社村田製作所 Vibrating gyro
JPH0762616B2 (en) * 1993-03-08 1995-07-05 株式会社村田製作所 Vibrating gyro

Also Published As

Publication number Publication date
JPS61191918A (en) 1986-08-26

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