JPS6338578Y2 - - Google Patents

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Publication number
JPS6338578Y2
JPS6338578Y2 JP11392880U JP11392880U JPS6338578Y2 JP S6338578 Y2 JPS6338578 Y2 JP S6338578Y2 JP 11392880 U JP11392880 U JP 11392880U JP 11392880 U JP11392880 U JP 11392880U JP S6338578 Y2 JPS6338578 Y2 JP S6338578Y2
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JP
Japan
Prior art keywords
electrodes
substrate
width
electrode
piezoelectric vibrating
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
Application number
JP11392880U
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Japanese (ja)
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JPS5736018U (en
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.)
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Publication date
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Priority to JP11392880U priority Critical patent/JPS6338578Y2/ja
Publication of JPS5736018U publication Critical patent/JPS5736018U/ja
Application granted granted Critical
Publication of JPS6338578Y2 publication Critical patent/JPS6338578Y2/ja
Expired legal-status Critical Current

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  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Description

【考案の詳細な説明】 <産業上の利用分野> この考案は、各種電子回路に組み込んで使用す
る圧電振動部品に関するものである。
[Detailed description of the invention] <Industrial application field> This invention relates to a piezoelectric vibrating component that is used by being incorporated into various electronic circuits.

<従来の技術> 第1図Aは従来の圧電振動部品を示すもので、
1は矢印の方向に分極された圧電基板であつて、
この基板1の片面に、分極方向に二分割された励
振電極12を対向させて設け、この各電極12に
引き出し用導電路4、リード線取付け電極5をそ
れぞれ設けたものである。このような周知の圧電
振動部品は基板1の振動方向に向かつて第1図B
に示すような定在波が考えられ、基本振動r1
奇数倍高調波が表れる。
<Prior art> Figure 1A shows a conventional piezoelectric vibrating component.
1 is a piezoelectric substrate polarized in the direction of the arrow,
Excitation electrodes 12 divided into two parts in the polarization direction are provided on one side of the substrate 1 to face each other, and each electrode 12 is provided with a lead-out conductive path 4 and a lead wire attachment electrode 5, respectively. Such a known piezoelectric vibrating component is oriented in the direction of vibration of the substrate 1 as shown in FIG.
A standing wave as shown in is considered, and odd-numbered harmonics of the fundamental vibration r 1 appear.

<考案が解決しようとする課題> 上記のような従来の圧電振動部品は、その振動
の周波数応答が第2図に示すように、振動の基本
波r1の奇数倍高調波が表れるために発振周波数
のジヤンプあるいは他の信号をピツクアツプして
しまう等の問題があつた。
<Problems to be solved by the invention> Conventional piezoelectric vibrating components such as those described above oscillate because the frequency response of the vibration is an odd harmonic of the fundamental wave r1 of vibration, as shown in Figure 2. There were problems such as frequency jumps or picking up other signals.

<課題を解決するための手段> この考案は、上記のような従来の圧電部品の問
題を解決するためになされたもので、幅方向に分
極された圧電基板の片面に、圧電基板の幅方向に
間隙をおいて複数の励振電極を形成して幅方向振
動モードを生じさせる圧電振動部品において、基
板の幅方向寸法をW、使用する奇数倍高調波次数
をnとした時、励振電極の数をn+1とし、基板
の幅方向の最外側にそれぞれ位置する二つの電極
の幅寸法を実質的にW/2n、それ以外の電極の幅を 実質的にW/nとして、使用する奇数倍高調波振動 定在波において互いに同相状態になるよう電極相
互を接続して終局的に2端子構成とするものであ
る。
<Means for solving the problem> This invention was made to solve the problems of conventional piezoelectric components as described above. In a piezoelectric vibrating component that produces a widthwise vibration mode by forming multiple excitation electrodes with gaps between them, the number of excitation electrodes is determined by the widthwise dimension of the substrate being W, and the odd harmonic order used being n. is n+1, the width dimension of the two outermost electrodes in the width direction of the substrate is substantially W/2n, and the width of the other electrodes is substantially W/n, and the odd harmonics to be used are The electrodes are connected to each other so that they are in phase with each other in the vibration standing wave, resulting in a two-terminal configuration.

<実施例> 第3図A、第4図Aはこの考案の圧電振動部品
を示すものである。
<Example> FIG. 3A and FIG. 4A show the piezoelectric vibrating component of this invention.

第3図において基板1は第1図Aに示す従来例
と同様に矢印方向に分極された圧電セラミツクか
らなるもので、この基板1の片側に一対の外側励
振電極2と、この各外側励振電極2にそれぞれ対
向する一対の内側励振電極3がそれぞれ設けられ
て、4分割電極となり、この各電極2,3にそれ
ぞれ引き出し用導電路4を設け、基板1の端部に
幅方向に設けたリード線取付電極5,5は対向す
る電極2,3から交互に反対方向に設けた引き出
し用導電路4,4に接続したものである。
In FIG. 3, a substrate 1 is made of piezoelectric ceramic polarized in the direction of the arrow, similar to the conventional example shown in FIG. A pair of inner excitation electrodes 3 facing each other are provided on each of the electrodes 2 and 3 to form a quarter electrode, and each electrode 2 and 3 is provided with a lead-out conductive path 4, and a lead provided in the width direction at the end of the substrate 1. The wire attachment electrodes 5, 5 are connected to lead-out conductive paths 4, 4 alternately provided in opposite directions from the opposing electrodes 2, 3.

この基板1の幅(分極方向の長さ)をW、基本
波の高調波次数をn、n次高調波の波長をλnと
したとき 分極の分割数を n+1 外側電極2の幅を 1/2nW=1/4λn 内側電極3の幅を 1/nW=1/2λn とすれば、第3図の実施例の場合、 電極分割数 n+1は 3+1=4 外側電極2の幅1/2nWは 1/2×3W=1/6W 内側電極3の幅1/nWは 1/3W となり、定在波は第3図Bのようになつて、 外側の電極2の幅W/6は1/4λ3 内側の電極3の幅W/3は1/2λ3 に相当する。これを基本波で励振したとき電極表
面に誘起される電荷分布は第5図Aのようにな
り、3次高調波で励振したときは同図Bのように
なる。4分割した電極では基本波励振の場合は第
6図Aの電荷分布となつて正負電荷が相殺され、
励振できなくなるが、3次高調波で励振すると同
図Bのように正負電荷が電極交互に分布するの
で、第7図に示すように同相電極を順次接続し、
実質的に2端子構成とすることによつて第8図に
示すように3次高調波r3の奇数倍の高調波だけ
となる。
When the width of this substrate 1 (length in the polarization direction) is W, the harmonic order of the fundamental wave is n, and the wavelength of the n-th harmonic is λn, the number of polarization divisions is n+1, and the width of the outer electrode 2 is 1/2nW. = 1/4λn If the width of the inner electrode 3 is 1/nW = 1/2λn, in the case of the embodiment shown in Fig. 3, the number of electrode divisions n+1 is 3+1=4 and the width 1/2nW of the outer electrode 2 is 1/2. ×3W=1/6W The width 1/nW of the inner electrode 3 becomes 1/3W, and the standing wave becomes as shown in Figure 3B, and the width W/6 of the outer electrode 2 becomes 1/4λ. The width W/3 of the electrode 3 corresponds to 1/2λ 3 . When this is excited with a fundamental wave, the charge distribution induced on the electrode surface is as shown in FIG. 5A, and when excited with a third harmonic, it is as shown in FIG. 5B. In the case of fundamental wave excitation, the electrode divided into four parts becomes the charge distribution shown in Figure 6A, and the positive and negative charges cancel each other out.
However, when exciting with the third harmonic, positive and negative charges are distributed alternately between the electrodes as shown in Figure B, so connect the in-phase electrodes in sequence as shown in Figure 7.
By essentially having a two-terminal configuration, only harmonics that are odd multiples of the third harmonic r3 are produced as shown in FIG.

第4図は5次高調波を利用する場合の電極構造
の実施例である。
FIG. 4 shows an example of the electrode structure when using the fifth harmonic.

この第4図Aにおいて基板1は第1図Aに示す
従来例と同様に矢印方向に分極された圧電セラミ
ツクからなるもので、この基板1の片側に一対の
外側励振電極2と、この各外側励振電極2にそれ
ぞれ対向する各一対の内側励振電極3がそれぞれ
設けられて6分割電極となり、各電極2,3には
それぞれ引き出し用導電路4を設け、基板1の端
部に設けた幅方向のリード線取付け電極5,5は
対向する各電極2,3から交互に反対方向に設け
た引き出し用導電路4,4に接続されている。
In this FIG. 4A, the substrate 1 is made of piezoelectric ceramic polarized in the direction of the arrow as in the conventional example shown in FIG. Each pair of inner excitation electrodes 3 facing the excitation electrode 2 is provided to form a six-divided electrode, and each electrode 2 and 3 is provided with a lead-out conductive path 4, which is provided at the end of the substrate 1 in the width direction. The lead wire attachment electrodes 5, 5 are connected to lead-out conductive paths 4, 4 provided alternately in opposite directions from the opposing electrodes 2, 3.

この場合の定在波は第4図Bのようになり、こ
の場合の定在波は同図Bのようになり、 電極の分割数n+1は5+1=6 外側電極2の幅1/2nWは 1/2×5W=1/10W=1/4λ5 内側電極3の幅1/nWは 1/5W=1/2λ5 となり、5次高調波の周波数r5の奇数倍の高調
波だけとなる。
The standing wave in this case is as shown in Figure 4B, and the standing wave in this case is as shown in Figure 4B.The number of electrode divisions n+1 is 5+1=6.The width 1/2nW of the outer electrode 2 is 1. /2×5W=1/10W=1/4λ 5 The width 1/nW of the inner electrode 3 becomes 1/5W=1/2λ 5 , and only harmonics are odd multiples of the fifth harmonic frequency r 5 .

尚、上記の実施例は共振子にこの考案を実施し
たものについて述べたが、圧電振動を利用する発
振子、濾波器、トラツプ素子等の電極にも利用し
得ることは勿論である。
In the above embodiment, the present invention was applied to a resonator, but it goes without saying that it can also be used for electrodes of oscillators, filters, trap elements, etc. that utilize piezoelectric vibration.

<効果> この考案の圧電振動部品は上記の構造であり、
以下に列記する効果がある。
<Effect> The piezoelectric vibrating component of this invention has the above structure,
It has the effects listed below.

基板の幅方向の寸法をW、使用する奇数倍高調
波次数をnとしたとき、励振電極の数をn+1と
し、基板の幅方向の最外側にそれぞれ位置する二
つの電極の幅寸法を実質的にW/2n、それ以外の電 極の幅を実質的にW/nとして、使用する奇数倍高 調波振動定在波において互いに同相状態となるよ
うに電極相互を接続して終局的に2端子構成とし
たものであるから発振周波数のジヤンプあるいは
他信号をピツクアツプする原因とな基本波および
奇数波高調波の相当数が抑制される。
When the dimension in the width direction of the substrate is W, and the odd harmonic order used is n, the number of excitation electrodes is n+1, and the width dimension of the two electrodes located at the outermost side in the width direction of the substrate is substantially The width of the other electrodes is set to W/2n, and the width of the other electrodes is substantially W/n, and the electrodes are connected to each other so that they are in phase with each other in the odd harmonic vibration standing waves used, resulting in a two-terminal configuration. Therefore, a considerable number of the fundamental wave and odd-number harmonics that cause jumps in the oscillation frequency or pickup of other signals are suppressed.

従つて、従来の単純2分割電極を有する圧電振
動部品のような欠点は減少し、振動特性に対する
信頼度、安定性は著しく向上する。また、共振周
波数rと反共周波数aとの山谷比も大きくなり、
機械的結合度Qmが大きくなるので、共振子等に
も好ましい結果が得られる。
Therefore, the drawbacks of the conventional piezoelectric vibrating component having a simple two-part electrode are reduced, and the reliability and stability of the vibration characteristics are significantly improved. In addition, the peak-to-valley ratio between the resonant frequency r and the anti-resonant frequency a increases,
Since the degree of mechanical coupling Qm increases, favorable results can also be obtained for resonators and the like.

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

第1図Aは従来の圧電振動部品の一例を示す斜
視図、同図Bは同上の定在波の説明図、第2図は
第1図の圧電振動部品の振動特性曲線、第3図、
第4図はこの考案の圧電振動部品の各例を示すも
ので、各図のAは正面図、Bはそれぞれの定在波
の説明図、第5図、第6図、第7図は3次高調波
を利用する第3図の圧電振動部品の電極の説明
図、第8図は3次高調波を利用した共振子周波数
特性曲線を示すものである。 1……圧電基板、2……外側電極、3……内側
電極。
FIG. 1A is a perspective view showing an example of a conventional piezoelectric vibrating component, FIG. 1B is an explanatory diagram of the standing wave of the same as above, FIG.
Fig. 4 shows each example of the piezoelectric vibrating component of this invention. In each figure, A is a front view, B is an explanatory diagram of each standing wave, and Figs. 5, 6, and 7 are 3 FIG. 3 is an explanatory diagram of electrodes of a piezoelectric vibrating component that utilizes third-order harmonics, and FIG. 8 shows a resonator frequency characteristic curve that utilizes third-order harmonics. 1...Piezoelectric substrate, 2...Outer electrode, 3...Inner electrode.

Claims (1)

【実用新案登録請求の範囲】 幅方向に分極された圧電基板の片面に、圧電基
板の幅方向に間隙をおいて複数の励振電極を形成
して幅方向振動モードを生じさせる圧電振動部品
において、基板の幅方向寸法をW、使用する奇数
倍高調波次数をnとした時、励振電極の数をn+
1とし、基板の幅方向の最外側にそれぞれ位置す
る二つの電極の幅寸法を実質的にW/2n、それ以外 の電極の幅を実質的にW/nとして、使用する奇数 倍高調波振動定在波において互いに同相状態にな
るよう電極相互を接続して終局的に2端子構成と
する圧電振動部品。
[Claims for Utility Model Registration] A piezoelectric vibrating component that generates a widthwise vibration mode by forming a plurality of excitation electrodes with gaps in the widthwise direction of the piezoelectric substrate on one side of a piezoelectric substrate polarized in the widthwise direction, When the width direction dimension of the substrate is W, and the odd harmonic order used is n, the number of excitation electrodes is n+
1, the width dimensions of the two electrodes located at the outermost sides in the width direction of the substrate are substantially W/2n, and the widths of the other electrodes are substantially W/n, and the odd harmonic vibration to be used is A piezoelectric vibrating component whose electrodes are connected to each other so that they are in phase with each other in a standing wave, resulting in a two-terminal configuration.
JP11392880U 1980-08-11 1980-08-11 Expired JPS6338578Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11392880U JPS6338578Y2 (en) 1980-08-11 1980-08-11

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11392880U JPS6338578Y2 (en) 1980-08-11 1980-08-11

Publications (2)

Publication Number Publication Date
JPS5736018U JPS5736018U (en) 1982-02-25
JPS6338578Y2 true JPS6338578Y2 (en) 1988-10-12

Family

ID=29474928

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11392880U Expired JPS6338578Y2 (en) 1980-08-11 1980-08-11

Country Status (1)

Country Link
JP (1) JPS6338578Y2 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58172220U (en) * 1982-05-12 1983-11-17 キンセキ株式会社 piezoelectric vibrator
JPS59195830U (en) * 1983-06-13 1984-12-26 東光株式会社 piezoelectric vibrator
JPH0622309B2 (en) * 1984-10-11 1994-03-23 日本電波工業株式会社 Piezoelectric vibrator for etching monitor
JP2854581B2 (en) * 1988-06-27 1999-02-03 富士通株式会社 Piezoelectric vibrating element and its frequency adjustment method

Also Published As

Publication number Publication date
JPS5736018U (en) 1982-02-25

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