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JPH0245845B2 - - Google Patents
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JPH0245845B2 - - Google Patents

Info

Publication number
JPH0245845B2
JPH0245845B2 JP57177433A JP17743382A JPH0245845B2 JP H0245845 B2 JPH0245845 B2 JP H0245845B2 JP 57177433 A JP57177433 A JP 57177433A JP 17743382 A JP17743382 A JP 17743382A JP H0245845 B2 JPH0245845 B2 JP H0245845B2
Authority
JP
Japan
Prior art keywords
electrodes
extraction
oscillation frequency
piezoelectric element
electrode
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 - Lifetime
Application number
JP57177433A
Other languages
Japanese (ja)
Other versions
JPS5967709A (en
Inventor
Mitsuyuki Sugita
Hirofumi Yanagi
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.)
Seikosha KK
Original Assignee
Seikosha KK
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 Seikosha KK filed Critical Seikosha KK
Priority to JP17743382A priority Critical patent/JPS5967709A/en
Publication of JPS5967709A publication Critical patent/JPS5967709A/en
Publication of JPH0245845B2 publication Critical patent/JPH0245845B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
    • H03H9/02Details
    • H03H9/125Driving means, e.g. electrodes, coils
    • H03H9/13Driving means, e.g. electrodes, coils for networks consisting of piezoelectric or electrostrictive materials
    • H03H9/132Driving means, e.g. electrodes, coils for networks consisting of piezoelectric or electrostrictive materials characterized by a particular shape

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、水晶振動子などの圧電振動子に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a piezoelectric resonator such as a crystal resonator.

[従来の技術とその問題点] 従来、厚みすべり振動を行う水晶振動子は両主
面の中央部に駆動電極が設けてある。この水晶振
動子の発振周波数の調整は、駆動電極上に真空蒸
着により銀などを付加したり、レーザ光線により
駆動電極中央部の電極膜を除去(トリミング)し
たりする方法が採用されていた。
[Prior art and its problems] Conventionally, a crystal resonator that performs thickness-shear vibration has drive electrodes provided at the center of both principal surfaces. The oscillation frequency of this crystal resonator has been adjusted by adding silver or the like to the drive electrode by vacuum deposition, or by removing (trimming) the electrode film at the center of the drive electrode using a laser beam.

しかしながら付加質量効果による調整は、調整
時の雰囲気を真空としなければならないから作業
性が極めて悪い問題を有している。
However, adjustment using the added mass effect has a problem in that workability is extremely poor because the atmosphere during adjustment must be kept in a vacuum.

またレーザ光線によるトリミング調整による
と、発振に最も敏感な水晶片の中央部に熱衝撃が
加わるために、熱衝撃による経時変化が避けられ
ない問題を有している。
In addition, trimming adjustment using a laser beam has the problem that thermal shock is applied to the center of the crystal piece, which is most sensitive to oscillation, so that changes over time due to thermal shock are unavoidable.

また、従来において、駆動電極を二つに分割し
たものも知られてはいる(例えば、特公昭51−
49386号公報、特開昭57−13806号公報、特開昭54
−157463号公報等)が、これら公知のものは、い
ずれも分割電極からの引出し電極は別々に保持部
材に接続してあり、引出し電極の途中を切断する
ことによつて発振周波数を調整するものではな
い。
Furthermore, in the past, it has been known that the drive electrode is divided into two parts (for example,
Publication No. 49386, Japanese Unexamined Patent Publication No. 1983-13806, Japanese Unexamined Patent Publication No. 1987-13806
-157463, etc.), but in all of these known devices, the extraction electrodes from the split electrodes are connected to a holding member separately, and the oscillation frequency is adjusted by cutting the extraction electrodes in the middle. isn't it.

[発明の目的] 本発明は、発振周波数の調整を簡便に行なえて
しかも圧電素子の中央部に熱衝撃を与えず長期間
安定した発振精度を維持できる圧電振動子を提供
することを目的とするものである。
[Object of the Invention] An object of the present invention is to provide a piezoelectric vibrator that can easily adjust the oscillation frequency and maintain stable oscillation accuracy for a long period of time without applying thermal shock to the center of the piezoelectric element. It is something.

[目的を達成するための手段] 上記目的を達成するために、本発明による圧電
振動子は、圧電素子の両主面の中央部に互いに対
向する関係で形成してある1対の駆動電極の少な
くとも一方が、複数の少電極に分割してあり、小
電極のそれぞれからは、圧電素子の外周部に延伸
する引出し電極が互いに分離した状態で1箇所に
集められて形成してある。引出し電極のそれぞれ
は、機械的かつ電気的に圧電素子の外周部で同一
保持部材に接続してあり、引出し電極のいずれか
を途中で切断することによつて、発振周波数が調
整可能である。
[Means for Achieving the Object] In order to achieve the above object, the piezoelectric vibrator according to the present invention has a pair of driving electrodes formed at the center of both main surfaces of the piezoelectric element so as to face each other. At least one of the electrodes is divided into a plurality of small electrodes, and from each of the small electrodes, lead electrodes extending to the outer periphery of the piezoelectric element are separated from each other and collected at one location. Each of the extraction electrodes is mechanically and electrically connected to the same holding member at the outer periphery of the piezoelectric element, and the oscillation frequency can be adjusted by cutting any of the extraction electrodes in the middle.

[実施例] 以下、本発明の詳細を、添付図面に示す好適な
実施例にそつて説明する。
[Embodiments] Hereinafter, the present invention will be described in detail with reference to preferred embodiments shown in the accompanying drawings.

第1〜2図において、は圧電振動子である厚
みすべり振動を行う水晶振動子であり、圧電素子
である水晶片2の両主面2a,2bには、それぞ
れ駆動電極3,4が真空蒸着などの手法により形
成してある。
In FIGS. 1 and 2, reference numeral 1 denotes a piezoelectric vibrator that performs thickness-shear vibration, and drive electrodes 3 and 4 are provided on both main surfaces 2a and 2b of a crystal piece 2 that is a piezoelectric element, respectively, in a vacuum state. It is formed by a method such as vapor deposition.

一方、主面2aに形成された駆動電極3は、横
方向のスリツトにより複数の少電極3A,3B…
3Iに分割されている。これらの少電極3A,3
B…3Iには、それぞれ電気的に接続できるよう
に水晶片2の外周端まで導かれた引出し電極3
a,3b…3iが形成してある。
On the other hand, the drive electrode 3 formed on the main surface 2a has a plurality of small electrodes 3A, 3B, . . . formed by horizontal slits.
It is divided into 3I. These small electrodes 3A, 3
B...3I has lead electrodes 3 each led to the outer peripheral edge of the crystal piece 2 so as to be electrically connected.
a, 3b...3i are formed.

水晶片2の他方の主面2bに形成された駆動電
極4は、単一の円形電極であり、この駆動電極4
からは引出し電極4aが外周端まで延出して形成
してある。
The drive electrode 4 formed on the other main surface 2b of the crystal blank 2 is a single circular electrode.
From there, a lead electrode 4a is formed extending to the outer peripheral end.

引出し電極3a,3b…3iおよび引出し電極
4aは、それぞれ反対方向に引き出されており、
水晶片2はこれらの引出し電極の部分で保持部材
(保持バネ)5,6に図示しない導電性接着剤を
介して機械的かつ電気的に接続保持されている。
The extraction electrodes 3a, 3b...3i and the extraction electrode 4a are each extracted in opposite directions,
The crystal piece 2 is mechanically and electrically connected and held to holding members (holding springs) 5 and 6 via a conductive adhesive (not shown) at these extraction electrode portions.

厚みすべり振動を行う水晶振動子の発振周波
数は、一般に、 で与えられる。上式において、tは水晶片の厚
さ、C66は弾性定数、ρは密度である。
Generally, the oscillation frequency of the crystal resonator 1 that performs thickness-shear vibration is as follows: is given by In the above formula, t is the thickness of the crystal piece, C 66 is the elastic constant, and ρ is the density.

いま水晶片の厚さtを0.42mm=0.42×10-3mと
すると、水晶片の密度ρ=2.34×103Kg/m3であ
り、引出し電極3a,3b…3iが全部接続され
た電界一定の場合の弾性定数は、CE 66=29.326×
109N/m2に近い値をとり、これらを上式に代入
すると、fs1=3.943MHzとなる。
Now, if the thickness t of the crystal piece is 0.42 mm = 0.42 × 10 -3 m, the density of the crystal piece is ρ = 2.34 × 10 3 Kg/m 3 , and the electric field where all the extraction electrodes 3a, 3b...3i are connected is The elastic constant for a constant case is C E 66 = 29.326×
By taking values close to 10 9 N/m 2 and substituting these into the above equation, fs 1 =3.943MHz.

また、引出し電極3a,3b…3iが全部切断
された電気変位一定の場合の弾性定数は、CD 66
28.967×109N/m2に近い値をとり、これを上式
に代入すると、fs2=3.968MHzとなる。
In addition, the elastic constant when the electrical displacement is constant when all the extraction electrodes 3a, 3b...3i are cut is C D 66 =
Taking a value close to 28.967×10 9 N/m 2 and substituting this into the above equation yields fs 2 =3.968MHz.

すなわち、水晶振動子は、3.968MHzから
3.943MHzまでの間で第3図示のように発振周波
数の調整が可能である。
In other words, crystal oscillator 1 starts from 3.968MHz.
The oscillation frequency can be adjusted up to 3.943MHz as shown in the third diagram.

第4図は、水晶振動子1の発振周波数を調整す
るため引出し電極3a,3iを切断した状態で示
す。
FIG. 4 shows a state in which the extraction electrodes 3a and 3i are cut in order to adjust the oscillation frequency of the crystal resonator 1.

この場合は、第1図示の引出し電極が全部接続
された場合より発振周波数は高くなる。引出し電
極を1本切断した場合の発振周波数の変化率は、
予め実験的に測定しておく。そして、引出し電極
を適当に切断することにより、目標の発振周波数
に近づけることができる。
In this case, the oscillation frequency will be higher than when all the extraction electrodes shown in the first figure are connected. The rate of change in oscillation frequency when one extraction electrode is cut is:
Measure it experimentally in advance. Then, by appropriately cutting the extraction electrode, the oscillation frequency can be brought close to the target oscillation frequency.

引出し電極をレーザ光線により切断する場合、
切断は空気中で行うことができる。またレーザ光
線による熱衝撃は、水晶片2の外周部に受けるた
め振動変位の大きい中心部に影響はなく、長期間
に亘つて安定して発振精度を維持することができ
る。
When cutting the extraction electrode with a laser beam,
Cutting can be done in air. Furthermore, since the thermal shock caused by the laser beam is applied to the outer periphery of the crystal piece 2, the center part, where vibrational displacement is large, is not affected, and oscillation accuracy can be stably maintained over a long period of time.

第5図は、本発明の他の実施例を示すものであ
る。
FIG. 5 shows another embodiment of the invention.

水晶振動子11は、厚みすべり振動を行う水晶
片12と、この水晶片の両主面に形成した駆動電
極13,14とから構成され、一方の駆動電極1
3は水晶片12の中央部に同心的に分割して設け
た小電極13A,13B…13Eにより構成され
ている。これらの小電極13A,13B,13E
からは、外周までそれぞれ引出し電極13a,1
3b…13eが延出して形成されている。他方の
駆動電極14は単一の円形電極であり、他方の外
周まで引出し電極14aが延出形成してある。
The crystal resonator 11 is composed of a crystal piece 12 that performs thickness-shear vibration, and drive electrodes 13 and 14 formed on both main surfaces of this crystal piece.
3 is constituted by small electrodes 13A, 13B, . These small electrodes 13A, 13B, 13E
From there, the extraction electrodes 13a and 1 are extended to the outer periphery, respectively.
3b...13e are formed to extend. The other drive electrode 14 is a single circular electrode, and an extraction electrode 14a is formed extending to the outer periphery of the other drive electrode 14.

この水晶振動子11も、引出し電極13A,1
3B…13Eを中途で切断することにより発振周
波数の調整を行うが、切断は引出し電極13e,
13d,13c,13bの順序で行う。このよう
に切断すると、残つた小電極群が円形状となるた
め他面の円形状の駆動電極とのマツチングがよ
く、効率よい励振を行うことができる。
This crystal resonator 11 also has extraction electrodes 13A, 1
The oscillation frequency is adjusted by cutting 3B...13E in the middle, but the cutting is done at the extraction electrodes 13e,
Perform steps 13d, 13c, and 13b in this order. By cutting in this manner, the remaining small electrode group becomes circular, so it matches well with the circular drive electrode on the other side, and efficient excitation can be performed.

なお圧電振動子として厚みすべり水晶振動子の
例を示したが、他の振動モード、他の圧電素子を
用いることも可能である。また両方の駆動電極を
ともに複数の小電極に分割することも可能であ
る。
Although a thickness-shear crystal vibrator is shown as an example of the piezoelectric vibrator, it is also possible to use other vibration modes and other piezoelectric elements. It is also possible to divide both drive electrodes into a plurality of small electrodes.

[発明の効果] 本発明の圧電振動子によれば、発振周波数の調
整が圧電素子の外周部に位置する引出し電極の途
中をレーザ光線などにて切断することにより達成
でき、その結果、圧電素子の中央部に熱衝撃を与
えないので発振精度の安定した圧電振動子を提供
することができる。
[Effects of the Invention] According to the piezoelectric vibrator of the present invention, the oscillation frequency can be adjusted by cutting the extraction electrode located on the outer periphery of the piezoelectric element in the middle using a laser beam or the like, and as a result, the piezoelectric element Since no thermal shock is applied to the central part of the piezoelectric vibrator, it is possible to provide a piezoelectric vibrator with stable oscillation accuracy.

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

第1図は本発明による圧電振動子の一実施例の
正面図、第2図はその背面図、第3図は発振周波
数の変化を示す特性図、第4図は発振周波数を調
整した後の状態の正面図、第5図は他の実施例の
正面図である。 2,12……圧電素子(水晶片)、3,4,1
3,14……駆動電極、3A〜3E,13A〜1
3E……小電極、3a〜3e,13a〜13e…
…小電極の引出し電極、4a,4b……円形電極
の引出し電極、5,6……保持部材。
Fig. 1 is a front view of an embodiment of a piezoelectric vibrator according to the present invention, Fig. 2 is a rear view thereof, Fig. 3 is a characteristic diagram showing changes in the oscillation frequency, and Fig. 4 is a diagram after adjusting the oscillation frequency. FIG. 5 is a front view of another embodiment. 2, 12...Piezoelectric element (crystal piece), 3, 4, 1
3, 14... Drive electrode, 3A-3E, 13A-1
3E...Small electrodes, 3a to 3e, 13a to 13e...
...extraction electrodes of small electrodes, 4a, 4b...extraction electrodes of circular electrodes, 5, 6...holding members.

Claims (1)

【特許請求の範囲】 1 圧電素子の両主面の中央部に互いに対向する
関係で形成してある1対の駆動電極の少なくとも
一方が、複数の少電極に分割してあり、 上記小電極のそれぞれからは、上記圧電素子の
外周部に延伸する引出し電極が互いに分離した状
態で1箇所に集められて形成してあり、 上記引出し電極のそれぞれは、機械的かつ電気
的に上記圧電素子の外周部で同一保持部材に接続
してあり、 上記引出し電極のいずれかを途中で切断するこ
とによつて、発振周波数が調整可能である ことを特徴とする圧電振動子。
[Scope of Claims] 1. At least one of a pair of drive electrodes formed in a mutually opposing relationship at the center of both main surfaces of a piezoelectric element is divided into a plurality of small electrodes; From each of them, extraction electrodes extending to the outer periphery of the piezoelectric element are formed separated from each other and collected in one place, and each of the extraction electrodes is mechanically and electrically extended to the outer periphery of the piezoelectric element. A piezoelectric vibrator, characterized in that the piezoelectric vibrator is connected to the same holding member at both ends thereof, and the oscillation frequency can be adjusted by cutting one of the lead-out electrodes midway.
JP17743382A 1982-10-08 1982-10-08 Piezoelectric oscillator Granted JPS5967709A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17743382A JPS5967709A (en) 1982-10-08 1982-10-08 Piezoelectric oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17743382A JPS5967709A (en) 1982-10-08 1982-10-08 Piezoelectric oscillator

Publications (2)

Publication Number Publication Date
JPS5967709A JPS5967709A (en) 1984-04-17
JPH0245845B2 true JPH0245845B2 (en) 1990-10-12

Family

ID=16030852

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17743382A Granted JPS5967709A (en) 1982-10-08 1982-10-08 Piezoelectric oscillator

Country Status (1)

Country Link
JP (1) JPS5967709A (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6118628U (en) * 1984-07-04 1986-02-03 株式会社村田製作所 piezoelectric vibrating parts
JP2549491Y2 (en) * 1991-02-25 1997-09-30 トヨタ自動車株式会社 Internal combustion engine piston cooling device
JP4513150B2 (en) * 2000-01-07 2010-07-28 エプソントヨコム株式会社 High frequency piezoelectric vibrator
CN104541148B (en) * 2012-08-10 2018-06-05 富士通株式会社 Qcm sensor and its manufacturing method

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5149386A (en) * 1974-10-28 1976-04-28 Hitachi Ltd SHUCHUKAN SHISEIGYOHOHO
JPS53147494A (en) * 1977-05-27 1978-12-22 Kinsekisha Lab Ltd Piezooelectric resonator and method of regulating frequency of same
JPS54157493A (en) * 1978-06-01 1979-12-12 Seikosha Kk Piezooelectric vibrator
JPS5713806A (en) * 1980-06-27 1982-01-23 Hitachi Ltd Piezoelectric oscillator

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Publication number Publication date
JPS5967709A (en) 1984-04-17

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