JPS59218022A - Long side piezoelectric vibrator - Google Patents

Long side piezoelectric vibrator

Info

Publication number
JPS59218022A
JPS59218022A JP9152783A JP9152783A JPS59218022A JP S59218022 A JPS59218022 A JP S59218022A JP 9152783 A JP9152783 A JP 9152783A JP 9152783 A JP9152783 A JP 9152783A JP S59218022 A JPS59218022 A JP S59218022A
Authority
JP
Japan
Prior art keywords
length
vibrating plate
electrodes
vibration
diaphragm
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
Application number
JP9152783A
Other languages
Japanese (ja)
Other versions
JPH0239885B2 (en
Inventor
Arata Doi
新 土井
Eiji Ise
伊勢 英二
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.)
Kyocera Crystal Device Corp
Original Assignee
Kyocera Crystal Device 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 Kyocera Crystal Device Corp filed Critical Kyocera Crystal Device Corp
Priority to JP9152783A priority Critical patent/JPH0239885B2/en
Publication of JPS59218022A publication Critical patent/JPS59218022A/en
Publication of JPH0239885B2 publication Critical patent/JPH0239885B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/15Constructional features of resonators consisting of piezoelectric or electrostrictive material
    • H03H9/17Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/02Details
    • H03H9/05Holders; Supports
    • H03H9/0595Holders; Supports the holder support and resonator being formed in one body

Abstract

PURPOSE:To reduce the effect of harmonics by setting the length of an electrode adhered to a side face part in the long side direction supported perpendicularly of a piezoelectric vibrating plate to 78.0-79.5% of the vibrating plate so as to increase (series resonance resistance to ternary harmonics/series resonance resistance to fundamental wave. CONSTITUTION:The vibrating plate 11 is fixed to a frame-formed support part 13 via a connecting part 12 led vertically from both side faces (X planes). Electrodes 14a, 14b for exciting lengthwise vibration are adhered nearly symmetrically around the connecting part 12 and lead electrodes 15a, 15b are adhered from a leg part 13a of the support part 13 to a base 13b. L-d subtracting a width (d) from the total length L of the vibrating plate 11 is taken as the length of the vibrating plate as a part participating to the vibration and similarly (l-d) subtracting the width (d) from the total length (l) of the electrodes 14a, 14b is used as the length of the electrodes, then it is considered that the optimum electrode length for vibrating the fundamental wave is within nearly 66.7-80% or 83% of the length of the vibrating plate.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は長辺圧電振動子、特にその励振電極構造に関す
るものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a long-side piezoelectric vibrator, and particularly to its excitation electrode structure.

〔従来技術〕[Prior art]

長辺圧電振動子において、その基本波振動を利用しよう
とする場合、基本波振動以外に、スプリアスとして基本
波振動のおよそ3倍、5倍の周波数を有する3次、5次
等の高調波の振動があり、基本波振動を安定に行なわせ
るためにはこれらを極力抑制しなければならないが、特
に影響の太きい3次の振動を抑えるために、基本波に対
する直列共振抵抗(CI、 )の値と3次の高調波に対
する直列共振抵抗(CI3)の値との比c■3/cII
をなるべく大きくすることが必要である。
When trying to utilize the fundamental vibration of a long-side piezoelectric vibrator, in addition to the fundamental vibration, there are spurious harmonics such as the 3rd and 5th harmonics, which have frequencies approximately 3 to 5 times the fundamental vibration. There are vibrations, and these must be suppressed as much as possible in order to stabilize the fundamental wave vibration, but in order to suppress the third-order vibration, which has a particularly strong influence, the series resonant resistance (CI, ) to the fundamental wave must be suppressed. The ratio between the value and the value of the series resonant resistance (CI3) for the third harmonic: c3/cII
It is necessary to make it as large as possible.

〔発明の目的および構成〕[Object and structure of the invention]

本発明はこのような事情に鑑みてなされたもので、その
目的はC1,/CI、を大きくした基本波励振用の長辺
圧電振動子を提供することにある。
The present invention has been made in view of these circumstances, and its purpose is to provide a long-side piezoelectric vibrator for fundamental wave excitation in which C1, /CI is increased.

このような目的を達成するために、本発明は、圧電振動
板の垂直支持した長辺方向側面部に付着させる電極の長
さを、振動板の長さの78.0〜79.5係に設定した
ものである。以下、実施例を用いて本発明の詳細な説明
する。
In order to achieve such an object, the present invention sets the length of the electrode attached to the vertically supported side surface of the piezoelectric diaphragm to be 78.0 to 79.5 times the length of the diaphragm. This is the setting. Hereinafter, the present invention will be explained in detail using Examples.

〔実施例〕〔Example〕

第1図は本発明の一実施例を示す斜視図である。 FIG. 1 is a perspective view showing an embodiment of the present invention.

本実施例は、ZQK乎直な水晶素板(2板)から、その
長辺方向がY軸、短辺方向がX軸に苓れぞれ平行となる
ような四辺形状に形成した振動板を用いた例で、振動板
11は、その両側面(X面)において、当該側面から垂
直に引出された連結部12を介して、フォトリングラフ
ィによシ一体形成された周囲を取シ囲む枠状の支持部1
3に画定されている。上記側面には、その中央部から引
出された上記連結部12を中心として、はぼ対称に長辺
振動励振用の電極14g、14L+を伺着し、さらに支
持部13の脚部138から基部13bにかけて、引出し
電極15a、15bが利着しである。なお、同様の引出
し電極は裏面にも設けである。ここで、連結部120幅
dの部分に関しては、振動板11の振動に対してデッド
部となっているため、実質的に振動に関与する部分とし
て、振動板11の全長りから上記幅dを差し引いた[、
−dを振動板の長さとし、同じく電極14a、14bの
全長りから上記幅dを差1〜引いたt−dを電極の長さ
と称することとする。
In this example, a diaphragm is formed from ZQK straight crystal plates (two plates) into a quadrilateral shape with the long side direction parallel to the Y axis and the short side direction parallel to the X axis. In the example used, the diaphragm 11 has a frame that surrounds the periphery integrally formed by photolithography on both sides (X plane) of the diaphragm 11 via connecting parts 12 drawn out perpendicularly from the sides. shaped support part 1
3. On the side surface, electrodes 14g and 14L+ for long-side vibration excitation are attached symmetrically around the connecting portion 12 pulled out from the center thereof, and further extend from the leg portion 138 of the support portion 13 to the base portion 13b. The extraction electrodes 15a and 15b are in contact with each other. Note that similar extraction electrodes are also provided on the back surface. Here, regarding the portion of the width d of the connecting portion 120, since it is a dead portion with respect to the vibration of the diaphragm 11, the width d is subtracted from the entire length of the diaphragm 11 as a portion that is substantially involved in vibration. deducted[,
-d is the length of the diaphragm, and t-d, which is obtained by subtracting the width d from the total length of the electrodes 14a and 14b, is called the length of the electrode.

一般に励振用の電極は、その面積が広いほど圧電板の電
気的等価定数における並列容量C6が大きくなり、CI
の低下に寄与すると考えられるが、本発明におけるよう
に基本波励振用として用いる場合には、先に述べたよう
に高調波、特に3次の高調波の励振を抑えるような電極
構造を用いる必要がある。
Generally, the larger the area of the excitation electrode, the larger the parallel capacitance C6 in the electrical equivalent constant of the piezoelectric plate, and the CI
However, when used for fundamental wave excitation as in the present invention, it is necessary to use an electrode structure that suppresses the excitation of harmonics, especially third harmonics, as described above. There is.

ここで、純粋に理論的に考えた場合、基本波、3次、5
次の振動時における振動板の歪の状態は第2図(a)(
基本波)、同図(b)(3次)および同図(C)(5次
)のようになシ、3次の振動を最小にするためには振動
板の長さAに対してB#0.667Aの電極長、5次の
振動を最小にするためにはC=0.8OAの電極長が望
ましいと考えられる。
Here, if we consider purely theoretically, the fundamental wave, 3rd order, 5th order
The state of distortion of the diaphragm during the next vibration is shown in Figure 2 (a) (
(fundamental wave), the same figure (b) (3rd order) and the same figure (C) (5th order), in order to minimize the 3rd order vibration, B It is considered that an electrode length of #0.667A and an electrode length of C=0.8OA are desirable in order to minimize the fifth-order vibration.

しかし、実際に第3図に示すような振動子について、X
線トポグラフにより振動板11の歪の状態を観察してみ
ると、第2図に示したような理想的な振動モードとはな
らず、はぼ第4図に示したような振動モードを示すこと
が確認された(ただし符号(■e)は明らかではない)
。ここで使用した振動子は、第1図の振動子が振動板1
1の全周を取シ囲むような枠状の支持部13を有するの
に対し、音叉形の支持部16を備えているが、振動板1
1の振動モード自体にはほとんど差がないと考えられる
。この観察の結果ではDキ0.83Aの電極長にすると
良好なことがわかる。なお、第3図において引出し電極
15.は支持部16の脚部16aから基部16bにかけ
て裏面側に付着しである。
However, in reality, for a vibrator as shown in Figure 3,
When we observe the state of distortion in the diaphragm 11 using a line topography, we find that it does not show the ideal vibration mode as shown in FIG. 2, but instead shows a vibration mode as shown in FIG. 4. was confirmed (however, the sign (■e) is not clear)
. The vibrator used here is the vibrator shown in Figure 1 on the diaphragm 1.
The diaphragm 1 has a frame-shaped support part 13 that surrounds the entire circumference of the diaphragm 1, while a tuning fork-shaped support part 16 is provided.
It is considered that there is almost no difference in the vibration mode of No. 1 itself. The results of this observation indicate that an electrode length of 0.83A is good. In addition, in FIG. 3, the extraction electrode 15. is attached to the back side of the support portion 16 from the leg portion 16a to the base portion 16b.

以上の結果から、基本波励振用に最適の電極長は振動板
の長さのほぼ66.7%から80チないし83チの範囲
内にあると考えられる。
From the above results, it is considered that the optimum electrode length for fundamental wave excitation is within the range of approximately 66.7% of the length of the diaphragm to 80 to 83 inches.

次に、第1図に示した振動子について、振動板11の全
長りを2.8朋、幅Wを0.08朋、厚みtを約0、2
 mmとして電極15a+15bの全長tを変えながら
CI3/C1,の(” )/(t、−d)依存性を調べ
てみると、第5図に示すような実験結果が得られた。
Next, regarding the vibrator shown in FIG. 1, the total length of the diaphragm 11 is 2.8 mm, the width W is 0.08 mm, and the thickness t is approximately 0.2 mm.
When the dependence of CI3/C1 on ('')/(t, -d) was investigated while changing the total length t of the electrodes 15a+15b in mm, the experimental results shown in FIG. 5 were obtained.

この場合基本波の周波数はIMHzで、上記cr3/C
1,の値はほぼ100以上あればよいから、結局、励振
電極の長さは振動板の長さの78.0〜79.5%に設
定すればよいことがわかる。CI3/C1,の値は、上
記電極長の割合が83チを越える領域でも100以上と
なる傾向が見られるが、78〜79.5係の範囲ではC
I3/C1,がきわめて急峻な上昇を示してピーク値も
高いのに対してその上昇傾向はなだらかであり、また実
験結果にもばらつきが太きかった。これに対し、78.
0〜79.5%ではばらつきも少なく、この範囲に設定
することではt丁確実に良好な基本波励振が得られる。
In this case, the frequency of the fundamental wave is IMHz, and the above cr3/C
Since the value of 1 only needs to be approximately 100 or more, it can be seen that the length of the excitation electrode may be set to 78.0 to 79.5% of the length of the diaphragm. The value of CI3/C1 tends to be 100 or more even in the region where the electrode length ratio exceeds 83 cm, but in the range of 78 to 79.5 cm, the value of CI3/C1,
While I3/C1 showed a very steep rise and had a high peak value, its rising tendency was gentle, and the experimental results also varied widely. On the other hand, 78.
In the range of 0 to 79.5%, there is little variation, and by setting it within this range, excellent fundamental wave excitation can be obtained reliably.

なお、周波数が変わればCI3/CI、  の絶対値そ
のものは変化するが、(1−d )/(L−d)依存性
は第5図に示したと同様の傾向を示し、78.0〜79
.5%で良好な結果が得られる。
Note that if the frequency changes, the absolute value of CI3/CI changes, but the (1-d)/(L-d) dependence shows the same tendency as shown in Figure 5, and is 78.0 to 79.
.. Good results are obtained with 5%.

また、第1図に示しだ水晶振動子に限らず第3図に示し
たような振動子、その細長辺方向両側面に長辺振動励振
用の対向電極を付し、当該側面で垂直に支持してなる長
辺圧電振動子一般に適用して同様の効果が得られる。
In addition to the crystal oscillator shown in Fig. 1, the oscillator shown in Fig. 3 can also be used with counter electrodes for long-side vibration excitation on both sides in the direction of its narrow sides, and supported vertically on the sides. Similar effects can be obtained by applying the present invention to general long-side piezoelectric vibrators.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明によれは、励振電極長を振
動板の長さの78.0〜79.5%にしたことによシ、
CI s / CI Hを太きくし、高調波の影響を少
なくして良好な基本波励振用の長辺圧電振動子を得るこ
とができる。
As explained above, according to the present invention, by setting the length of the excitation electrode to 78.0 to 79.5% of the length of the diaphragm,
By increasing CI s / CI H and reducing the influence of harmonics, it is possible to obtain a long-side piezoelectric vibrator for good fundamental wave excitation.

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

第1図は本発明の一実施例を示す振動子の斜視図、第2
図(−) 、 (b) 、 (C)は基本波、3次、5
次の理論的な振動モードを示す図、第3図はX線トポグ
ラフによる撮動モードの観察に用いた振動子を示“ す
斜視図、第4図はその観察結果を示す図、第5図は第1
図の振動子についてCI3/CIIの(z−d)/(し
−d)依存性を示すグラフである。 11・・・會振動板、12・・・・連結部、13.16
−−−−支持部、14a、14b −譬−・励振用の電
極。 特許出願人  キンセキ株式会社 代 理 人  山 川 政、樹(ほか1名)41図 第3図 第5ト遣 (f−d)/(L−d) (′/。)
FIG. 1 is a perspective view of a vibrator showing one embodiment of the present invention, and FIG.
Figures (-), (b), and (C) are fundamental waves, 3rd order, 5
Figure 3 is a perspective view showing the vibrator used for observation in the imaging mode using X-ray topography; Figure 4 is a diagram showing the observation results; Figure 5 shows the following theoretical vibration modes. is the first
It is a graph which shows (z-d)/(shi-d) dependence of CI3/CII about the oscillator of a figure. 11... Meeting diaphragm, 12... Connection part, 13.16
----Support part, 14a, 14b - Excitation electrode. Patent applicant Kinseki Co., Ltd. Agent Masa Yamakawa, Itsuki (and one other person) 41 Figure 3 Figure 5 (f-d)/(L-d) ('/.)

Claims (1)

【特許請求の範囲】[Claims] 圧電振動板の長辺方向両側面に長辺振動励振用の電極を
付着し、尚該側面においてt丘ぼ垂直に支持してなる長
辺圧電振動子において、上記電極の長さを、振動板の長
さの78.0〜79.5%としたことを0徴とする長辺
圧電振動子。
In a long-side piezoelectric vibrator in which electrodes for long-side vibration excitation are attached to both sides in the long side direction of a piezoelectric diaphragm and the t-hills are supported perpendicularly on the sides, the length of the electrodes is determined by the length of the diaphragm. A long side piezoelectric vibrator whose zero characteristic is 78.0 to 79.5% of the length.
JP9152783A 1983-05-26 1983-05-26 NAGAHENATSU DENSHINDOSHI Expired - Lifetime JPH0239885B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9152783A JPH0239885B2 (en) 1983-05-26 1983-05-26 NAGAHENATSU DENSHINDOSHI

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9152783A JPH0239885B2 (en) 1983-05-26 1983-05-26 NAGAHENATSU DENSHINDOSHI

Publications (2)

Publication Number Publication Date
JPS59218022A true JPS59218022A (en) 1984-12-08
JPH0239885B2 JPH0239885B2 (en) 1990-09-07

Family

ID=14028899

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9152783A Expired - Lifetime JPH0239885B2 (en) 1983-05-26 1983-05-26 NAGAHENATSU DENSHINDOSHI

Country Status (1)

Country Link
JP (1) JPH0239885B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0343000A2 (en) * 1988-05-20 1989-11-23 Seiko Electronic Components Ltd. Length-extensional piezo-electric resonator
EP0365268A2 (en) * 1988-10-17 1990-04-25 Seiko Electronic Components Ltd. Length longitudinal resonator
US5001383A (en) * 1988-09-09 1991-03-19 Seiko Electronic Components Ltd. Longitudinal quartz crystal resonator

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0343000A2 (en) * 1988-05-20 1989-11-23 Seiko Electronic Components Ltd. Length-extensional piezo-electric resonator
US5001383A (en) * 1988-09-09 1991-03-19 Seiko Electronic Components Ltd. Longitudinal quartz crystal resonator
EP0365268A2 (en) * 1988-10-17 1990-04-25 Seiko Electronic Components Ltd. Length longitudinal resonator

Also Published As

Publication number Publication date
JPH0239885B2 (en) 1990-09-07

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