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JPH02135907A - Vertical crystal resonator - Google Patents

Vertical crystal resonator

Info

Publication number
JPH02135907A
JPH02135907A JP29054188A JP29054188A JPH02135907A JP H02135907 A JPH02135907 A JP H02135907A JP 29054188 A JP29054188 A JP 29054188A JP 29054188 A JP29054188 A JP 29054188A JP H02135907 A JPH02135907 A JP H02135907A
Authority
JP
Japan
Prior art keywords
oscillation
crystal resonator
vibrating
vertical crystal
flection
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
JP29054188A
Other languages
Japanese (ja)
Other versions
JPH0831765B2 (en
Inventor
Hirofumi Kawashima
宏文 川島
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.)
Seiko Electronic Components Ltd
Original Assignee
Seiko Electronic Components 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 Seiko Electronic Components Ltd filed Critical Seiko Electronic Components Ltd
Priority to JP63290541A priority Critical patent/JPH0831765B2/en
Publication of JPH02135907A publication Critical patent/JPH02135907A/en
Publication of JPH0831765B2 publication Critical patent/JPH0831765B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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

Abstract

PURPOSE:To suppress oscillation leakage by enclosing an oscillation part with a flection part connected to the oscillation part, connecting the flection part to a frame via both ends of a hole, and extending it to a mount part. CONSTITUTION:A resonator 1 is formed integrally from the oscillation part 2 to the flection part 5 via a bridge part 4 by an etching method, and the hole 7 to obtain sufficient oscillation in the flection part 5 is provided. Furthermore, both end parts of the hole 7 are connected to the frame 6, and are extended to the mount part 8. Simultaneously, the flection part 5 is constituted so as to enclose the oscillation part 2. Thereby, the oscillation of the oscillation part 2 in the direction of the bridge part 4 is converted to an inflection mode, and a vertical crystal resonator preventing the oscillation leakage from occurring completely can be obtained even when it is fixed on the mount part 8.

Description

【発明の詳細な説明】 [産業上の利用分野1 本発明は、共振周波数が約IMHz前後の中周波数帯域
をカバーする縦水晶振動子に関する。特に、その振動子
形状に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field 1] The present invention relates to a vertical crystal resonator whose resonance frequency covers a medium frequency band around IMHz. In particular, it concerns the shape of the vibrator.

[発明の撮要] 本発明は、振動モレが非常に少なく、R,の小さい、小
型縦水晶振動子を提供することにある。
[Summary of the Invention] An object of the present invention is to provide a compact vertical crystal resonator with very little vibration leakage and a small R.

水晶は物理的、および化学的に大変に安定した物質であ
り、従って、これから形成される。いわゆる水晶振動子
は損失抵抗の小さい、高いQ値を持った振動子を得るこ
とができる。しかしながらこのように優れた特性が得ら
れるのは、振動モレの小さい振動子形状の設計がなされ
て初めて得られるのである。本発明では振動部と支持部
がエツチング法によって一体に形成された噌水晶振動子
の支持部の形状を工夫、故善することにより、振動部の
エネルギーを振動部内部に閉じ込めることができる。そ
の結果、損失抵抗R,の小さい、且つ、Q値の高い縦水
晶振動子を得ることができる。
Quartz is a physically and chemically very stable substance and therefore forms from this. A so-called crystal resonator can have a low loss resistance and a high Q value. However, such excellent characteristics can only be obtained by designing a vibrator shape with small vibration leakage. In the present invention, the energy of the vibrating part can be confined within the vibrating part by devising and improving the shape of the supporting part of the quartz crystal resonator in which the vibrating part and the supporting part are integrally formed by etching. As a result, a vertical crystal resonator with a small loss resistance R and a high Q value can be obtained.

[従来の技術1 振動部と支持部をエツチング法によって一体に形成され
た従来の縦水晶振動子は支持部のフレームの幅が一様、
且つ、同一方向に形成され、その端部でマウントされる
ため、振動部のエネルギーがマウント部まで伝わり、振
動モレの原因となっていた。そのために、損失抵抗R1
の小さい権水品振動子を得ることができなかった。
[Prior art 1] In a conventional vertical crystal resonator in which the vibrating part and the supporting part are integrally formed by etching, the width of the frame of the supporting part is uniform;
Moreover, since they are formed in the same direction and mounted at their ends, the energy of the vibrating part is transmitted to the mount part, causing vibration leakage. Therefore, the loss resistance R1
I couldn't get a small water quality vibrator.

[発明が解決しようとする課題] このために、増幅器の増中度を高める等して対応してき
たが消費電流が多くなる等の欠点があり、ひどい時には
、機器に配置したときに、振動モレが大きく、発振停止
するという大きな問題が生じていた。そこで、本発明は
、この振動モレの非常に小さい縦水晶振動子を提案する
ものである。即ち、振動モレの非常に小さい形状を提供
するものである。
[Problems to be Solved by the Invention] To address this issue, attempts have been made to increase the power boost of the amplifier, but this has drawbacks such as increased current consumption, and in severe cases, when placed in equipment, vibration leakage may occur. was large, causing a major problem in which oscillation stopped. Therefore, the present invention proposes a vertical crystal resonator with extremely small vibration leakage. That is, it provides a shape with very little vibration leakage.

[課題を解決するための手段] 第1図は本発明の縦水晶振動子の一実施例で、第2図は
第1図の縦水晶振動子の原理を説明するための簡略化し
た平面図である。第2図において、振動子lは振動部2
と支持部3がら成り、支持部3は両端固定という境界条
件で固定されていると考えることができる。又、振動部
2は長さLL、幅W1、厚みTで表わし、支持部3は長
さ1−21幅W2で表わすと、今、振動子lの振動部2
は矢印Aで示したように、伸びの変位をすると、支持部
3の屈曲部は、当然矢印Bで示すごとく内側に曲げのモ
ードを発生する。ここでは屈曲モードを起こす部分を屈
曲部5で示す6逆に、振動部2が縮めば、支持部3の屈
曲部5は外側に曲げのモードを発生する。即ち5本発明
では、振動部2の幅方向の変位を支持部3の屈曲モード
に変換することによって、その振動の自由度を抑圧しな
いようにしている。そして、実際には、振動を抑圧しな
い寸法がある。この形状寸法は振動部2のひずみエネル
ギーによって決まる。すなわち。
[Means for Solving the Problems] Fig. 1 shows an embodiment of the vertical crystal resonator of the present invention, and Fig. 2 is a simplified plan view for explaining the principle of the vertical crystal resonator of Fig. 1. It is. In Fig. 2, the vibrator l is the vibrating part 2.
It can be considered that the support part 3 is fixed under the boundary condition that both ends are fixed. Also, if the vibrating part 2 is expressed by length LL, width W1, and thickness T, and the support part 3 is expressed by length 1-21 and width W2, now the vibrating part 2 of the vibrator l
When the supporting portion 3 undergoes an elongation displacement as shown by arrow A, the bent portion of the support portion 3 naturally generates a bending mode inward as shown by arrow B. Here, the part that causes the bending mode is shown as a bending part 5 6 Conversely, when the vibrating part 2 contracts, the bending part 5 of the support part 3 generates a bending mode outward. That is, in the present invention, by converting the displacement of the vibrating part 2 in the width direction into the bending mode of the support part 3, the degree of freedom of vibration is not suppressed. In reality, there are dimensions that do not suppress vibrations. The shape and dimensions are determined by the strain energy of the vibrating section 2. Namely.

振動部2のひずみエネルギーをtJ、、屈曲部のひずみ
エネルギーをU2とすると、U、、U2は次式で表わさ
れる。
When the strain energy of the vibrating section 2 is tJ, and the strain energy of the bending section is U2, U, U2 are expressed by the following equation.

但し、応力T2.ひずみS2.ヤング率E、断面2次モ
ーメント■、変位V1体fiV + 、 V2座標Xを
示す。又、縦水晶振動子の振動を抑圧しない関係は式(
1)、(2)より、次の関係が成り立つ。
However, stress T2. Strain S2. The Young's modulus E, the second moment of area (■), the displacement V1 body fiV + , and the V2 coordinate X are shown. Also, the relationship that does not suppress the vibration of the vertical crystal oscillator is expressed by the formula (
From 1) and (2), the following relationship holds true.

01>tJ2                 −(
3)これより、屈曲部5の寸法L2.W2が決定される
0例えば、本発明の周波g91 LI Hzのときの振
動部の寸法は長さり、=2.6mm、W80LLm、T
=160umのとき、支持部の屈曲部の寸法比W、’/
L2は0.16以下であれば良い。このように寸法を決
めることにより、損失抵抗の小さい、且つ、高いQ値を
持つ縦水晶振動子を得ることができる6次に、振動モレ
について述べる。2第2図の簡略化した図から分かるよ
うに、振動部2の振動エネルギーは支持部3ヘブリッジ
部4を介して伝達する。従って、支持部3でのエネルギ
ー損失を小さくすれば良い訳で、支持部3のモードは屈
曲モードに変換されるから、両端固定部の質量が実質的
に無限に大きければ、支持部3の屈曲部5のエネルギー
はマウント部8までモレないことになる。換言するなら
ば、本発明は、振動部2から伝わる支持部3の屈曲モー
ドに変換する形状、即ち、幅W2と長さ1..2の比W
、/L2を選択することにより、振動部の振動を自由に
し、且つ、屈曲モードする部分と接続する両端固定の境
界条件を持つ支持部の質量を無限に大きくすることによ
って1本発明の目的を達成するものである。
01>tJ2 −(
3) From this, the dimension L2 of the bent portion 5. For example, when the frequency of the present invention is g91 LI Hz, the dimensions of the vibrating part are length = 2.6 mm, W80LLm, T
= 160 um, the dimension ratio of the bent part of the support part W,'/
L2 may be 0.16 or less. By determining the dimensions in this way, a vertical crystal resonator with low loss resistance and a high Q value can be obtained.6 Next, vibration leakage will be described. 2 As can be seen from the simplified diagram in FIG. 2, the vibration energy of the vibrating part 2 is transmitted to the support part 3 via the bridge part 4. Therefore, it is only necessary to reduce the energy loss in the support part 3, and since the mode of the support part 3 is converted to a bending mode, if the masses of the fixed parts at both ends are substantially infinitely large, the bending of the support part 3 The energy in the portion 5 will not leak up to the mount portion 8. In other words, the present invention has a shape that converts the bending mode of the support part 3 transmitted from the vibrating part 2, that is, the width W2 and the length 1. .. 2 ratio W
, /L2, the object of the present invention can be achieved by freeing the vibration of the vibrating part and infinitely increasing the mass of the supporting part which has a boundary condition of fixed both ends connected to the bending mode part. It is something to be achieved.

[作用] このように、本発明は振動部と支持部から構成される、
エツチング法によって形成される縦水晶振動子の支持部
の形状寸法を改善することにより、損失抵抗の小さい、
且つ、高いQlaを有する縦水晶振動子を得ることがで
きる。同時に、支持部の振動モードを解析することによ
り、振動モレの小さい縦水晶振動子が得られる。
[Function] As described above, the present invention is composed of a vibrating section and a supporting section.
By improving the shape and dimensions of the support part of the vertical crystal resonator formed by the etching method, the loss resistance is reduced.
Moreover, a vertical crystal resonator having a high Qla can be obtained. At the same time, by analyzing the vibration mode of the support part, a vertical quartz crystal resonator with small vibration leakage can be obtained.

[実施例1 次に、本発明にて得られた結果を具体的に述べる。第1
図は本発明の縦水晶振動子の一実施例の平面図で、振動
子lは振動部2と支持部3からブノッジ部4を介して構
成されていて、エツチング法によって一体に形成されて
いる。尚、支持部3は屈曲部5、穴7.フレーム6とマ
ウント部8から成っている。振動部2は外部からの電界
駆動(図示されてない)にて、長平方向に伸縮運動をす
るが、それと同時に、その垂直方向、即ち、ブリッジ部
4の方向にも同様の振動をする。この時に、まず、振動
部2の長平方向の振動を自由に励振するには、ブリッジ
部4の方向の振動を十分に自由にすることが大切で、そ
のために、本発明では支持部3の屈曲部5が十分に自由
に振動できるように、穴7が設けられている。又、屈曲
部5の長さしと幅W(図示されてない)の比によって1
例えば、周波数が約IM)lzの場合、辺比W/Lが0
.16以下であれば、長手方向の振動の抑圧を十分に小
さくすることができる。次に、振動モレについては、振
動子lは振動部2からブリッジ部4を介して屈曲部5へ
と一体にエツチング法によって形成され、屈曲部5の振
動を十分に自由にさせるために、穴7が設けられている
。更に、穴7の両端部はフレーム6に接続され、マウン
ト部8まて延びている。同時に、屈曲部5は振動部2を
囲むように構成されている。それ故、振動部2のブリッ
ジ部4の方向の振動は屈曲モードに変換され、且つ、穴
7の両端部を介してフレム6に接続、マウント部まで延
びているので、マウント部8で固定しても、全く振動モ
レのない縦水晶振動子が得られる。
[Example 1] Next, the results obtained with the present invention will be specifically described. 1st
The figure is a plan view of an embodiment of the vertical quartz crystal resonator of the present invention, in which the resonator l is constructed from a vibrating section 2 and a support section 3 via a notch section 4, and is integrally formed by an etching method. . Note that the support portion 3 has a bent portion 5, a hole 7. It consists of a frame 6 and a mount part 8. The vibrating part 2 is driven by an external electric field (not shown) to expand and contract in the longitudinal direction, but at the same time, it also vibrates in the vertical direction, that is, in the direction of the bridge part 4. At this time, first of all, in order to freely excite vibrations in the longitudinal direction of the vibrating part 2, it is important to make the vibrations in the direction of the bridge part 4 sufficiently free. Holes 7 are provided so that part 5 can vibrate sufficiently freely. Also, depending on the ratio of the length of the bent portion 5 to the width W (not shown), 1
For example, if the frequency is approximately IM)lz, the side ratio W/L is 0.
.. If it is 16 or less, the suppression of vibration in the longitudinal direction can be made sufficiently small. Next, regarding vibration leakage, the vibrator l is integrally formed from the vibrating part 2 to the bending part 5 via the bridge part 4 by an etching method, and in order to make the vibration of the bending part 5 sufficiently free, holes are formed. 7 is provided. Further, both ends of the hole 7 are connected to the frame 6 and extend to a mount section 8. At the same time, the bending section 5 is configured to surround the vibrating section 2. Therefore, the vibration of the vibrating part 2 in the direction of the bridge part 4 is converted into a bending mode, and is connected to the frame 6 through both ends of the hole 7 and extends to the mount part, so it can be fixed by the mount part 8. However, a vertical crystal resonator with no vibration leakage can be obtained.

〔発明の効果1 以上述べたように1本発明は振動部と支持部をエツチン
グ法によって一体に形成する縦水晶振動子に於いて、新
形状の縦水晶振動子を提案することにより1次の著しい
効果を有する。
[Effects of the Invention 1 As stated above, the present invention achieves the first order by proposing a vertical crystal resonator with a new shape in a vertical crystal resonator in which the vibrating part and the support part are integrally formed by an etching method. It has a remarkable effect.

■支持部の形状寸法を改善することにより、振動を自由
にさせることができるので、 tmm低抵抗小さくなる
■By improving the shape and dimensions of the support part, vibration can be made free, resulting in low tmm resistance.

■屈曲部とフレームの間に穴を設けているので、振動部
の振動を自由にさせることができると同時に、屈曲部の
エネルギーはフレームに伝わらないので、振動モレがな
くなり、マウント部で固定しても、R1の小さい振動子
が得られる。
■Since there is a hole between the bending part and the frame, the vibrating part can vibrate freely, and at the same time, the energy of the bending part is not transmitted to the frame, eliminating vibration leakage and fixing it with the mount part. However, a resonator with a small R1 can be obtained.

■片側でマウントするので、製造が容易、且つ小型化で
きる。
■Since it is mounted on one side, it is easy to manufacture and can be made smaller.

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

第1図は本発明の縦水晶振動子形状寸法の一実施例を示
す平面図である。 第2図は本発明の縦水晶振動子の原理を説明するだめの
簡略化した平面図である。 1 ・ ・ ・ 2 ・ ・ ・ 3 ・ ・ ・ 4 ・ ・ ・ 5 ・ ・ ・ 6 ・ ・ 7 ・ ・ ・ 8 ・ ・ ・ 11、 L2 W、W2 Ll ・ ・ W   ・ ・ 振動子 振動部 支持部 ブリッジ部 屈曲部 フレーム 穴 マウント部 屈曲部の長さ 屈曲部の幅 振動部の長さ 振動部の幅 本発明の一天兄例とホ(平面図 弔1 図
FIG. 1 is a plan view showing an embodiment of the shape and dimensions of a vertical crystal resonator of the present invention. FIG. 2 is a simplified plan view for explaining the principle of the vertical crystal resonator of the present invention. 1 ・ ・ ・ 2 ・ ・ ・ 3 ・ ・ 4 ・ ・ ・ 5 ・ ・ 6 ・ ・ 7 ・ ・ ・ 8 ・ ・ 11, L2 W, W2 Ll ・ ・ W ・ ・ Vibrator vibrating part support part bridge Bent part Frame hole Mount part Length of bent part Width of bent part Length of vibrating part Width of vibrating part

Claims (1)

【特許請求の範囲】[Claims]  振動部と支持部をエッチング法によって、一体に形成
された縦水晶振動子に於いて、振動部と接続する屈曲部
は前記振動部を囲み、更に、穴の両端を介してフレーム
に接続されるとともに、マウント部まで延びていること
を特徴とする縦水晶振動子。
In a vertical crystal resonator in which the vibrating part and the supporting part are integrally formed by etching, the bent part connected to the vibrating part surrounds the vibrating part and is further connected to the frame through both ends of the hole. Also, a vertical crystal resonator characterized by extending to the mount part.
JP63290541A 1988-11-17 1988-11-17 Vertical crystal unit Expired - Lifetime JPH0831765B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63290541A JPH0831765B2 (en) 1988-11-17 1988-11-17 Vertical crystal unit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63290541A JPH0831765B2 (en) 1988-11-17 1988-11-17 Vertical crystal unit

Publications (2)

Publication Number Publication Date
JPH02135907A true JPH02135907A (en) 1990-05-24
JPH0831765B2 JPH0831765B2 (en) 1996-03-27

Family

ID=17757360

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63290541A Expired - Lifetime JPH0831765B2 (en) 1988-11-17 1988-11-17 Vertical crystal unit

Country Status (1)

Country Link
JP (1) JPH0831765B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5218260A (en) * 1991-07-10 1993-06-08 Seiko Electronic Components Ltd. Longitudinal quartz crystal resonator
JP2016513406A (en) * 2013-02-14 2016-05-12 オネラ(オフィス・ナショナル・ドゥエチュード・エ・ドゥ・ルシェルチェ・アエロスパシャル)Onera (Office National D’Etudes Et De Recherches Aerospatiales) Planar structure of mechanical resonator separated by bending vibration and extension / compression vibration

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5552621A (en) * 1978-10-11 1980-04-17 Matsushima Kogyo Co Ltd Vertical vibration-type piezo-vibrator
JPS5917627U (en) * 1982-07-23 1984-02-02 キンセキ株式会社 piezoelectric vibrator
JPS5937722A (en) * 1982-08-26 1984-03-01 Matsushima Kogyo Co Ltd Longitudinal oscillation type piezoelectric oscillator
JPS6210518U (en) * 1985-07-04 1987-01-22

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5552621A (en) * 1978-10-11 1980-04-17 Matsushima Kogyo Co Ltd Vertical vibration-type piezo-vibrator
JPS5917627U (en) * 1982-07-23 1984-02-02 キンセキ株式会社 piezoelectric vibrator
JPS5937722A (en) * 1982-08-26 1984-03-01 Matsushima Kogyo Co Ltd Longitudinal oscillation type piezoelectric oscillator
JPS6210518U (en) * 1985-07-04 1987-01-22

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5218260A (en) * 1991-07-10 1993-06-08 Seiko Electronic Components Ltd. Longitudinal quartz crystal resonator
JP2016513406A (en) * 2013-02-14 2016-05-12 オネラ(オフィス・ナショナル・ドゥエチュード・エ・ドゥ・ルシェルチェ・アエロスパシャル)Onera (Office National D’Etudes Et De Recherches Aerospatiales) Planar structure of mechanical resonator separated by bending vibration and extension / compression vibration

Also Published As

Publication number Publication date
JPH0831765B2 (en) 1996-03-27

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