JPS61215932A - Piezoelectric vibrator - Google Patents

Piezoelectric vibrator

Info

Publication number
JPS61215932A
JPS61215932A JP5796685A JP5796685A JPS61215932A JP S61215932 A JPS61215932 A JP S61215932A JP 5796685 A JP5796685 A JP 5796685A JP 5796685 A JP5796685 A JP 5796685A JP S61215932 A JPS61215932 A JP S61215932A
Authority
JP
Japan
Prior art keywords
electrodes
vacuum
piezoelectric vibrator
vibrator
make
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.)
Pending
Application number
JP5796685A
Other languages
Japanese (ja)
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 JP5796685A priority Critical patent/JPS61215932A/en
Publication of JPS61215932A publication Critical patent/JPS61215932A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L9/00Measuring steady of quasi-steady pressure of fluid or fluent solid material by electric or magnetic pressure-sensitive elements; Transmitting or indicating the displacement of mechanical pressure-sensitive elements, used to measure the steady or quasi-steady pressure of a fluid or fluent solid material, by electric or magnetic means
    • G01L9/0001Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means
    • G01L9/0008Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations
    • G01L9/0022Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations of a piezoelectric element

Abstract

PURPOSE:To make small the equivalent serial resistance, to make high the sensitivity, to make wide a vacuum degree measuring scope, to make small-sized and to make light by arranging the exciting electrode at both edge parts and the central part of the vibrator. CONSTITUTION:For a piezoelectric vibrator 1, the supporting pat 3 is fixed by adhesives 4, etc., on a supporting base 2 composed of a ceramics material, etc. The exciting electrode is arranged on the four surfaces of respective arms, the number of electrodes is three pieces each on respective surfaces and arranged so that the adjoining electrode can be the different electrode. Namely, at one side arm, electrodes 5, 6, 7, 8, 9 and 10 and electrodes, which respectively go to be the same electrodes to these facing surfaces, are arranged, for example, electrodes 6, 8, and 10 and electrodes 5, 7 and 9 are connected so that respective electrodes can be the same electrodes. Electrodes 11, 12, 13, 14, 15, 16, etc., of other arm are in the same manner, and the polarity is made opposite. Thus, by making easy the both edge fixing bending mode the third higher harmonic vibration is made easy, thereby the equivalent serial resistance can be made smaller.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は真空度を測定するために真空センサーとして使
用する真空センサー圧電振動子に関する。特に、両端固
定の屈曲モードの圧電揚動子の電極配置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a vacuum sensor piezoelectric vibrator used as a vacuum sensor to measure the degree of vacuum. In particular, it relates to the electrode arrangement of a bending mode piezoelectric lifter with both ends fixed.

〔発明の概要〕[Summary of the invention]

この発明は両端固定タイプの圧電振動子を真空度測定の
真空センサーとして使用する場合、真空度測定範囲を広
くできる振動子の最適電極配置を提供するものである。
The present invention provides an optimal electrode arrangement of the vibrator that can widen the range of vacuum measurement when a piezoelectric vibrator with both ends fixed is used as a vacuum sensor for measuring the degree of vacuum.

〔従来の技術〕[Conventional technology]

真空計は古くから色々な分野の装置に使用さnてきた。 Vacuum gauges have been used in equipment in various fields since ancient times.

その中で、特に、ピラニー真空計が多用さnてi!た。Among them, the Pirani vacuum gauge is especially frequently used! Ta.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかしながら、最近は装置の小型化、軽量化に伴ない、
真空計の小型化、軽5°化も同様に要求さnている。前
記したビラニー真空計はサイズが大きく、貫いため最近
の!%I2に充分に応えらnないのが実情である。又、
従来の真空センサーを使用した真空計ではぶ子炉などの
高碍場が発生する装置内での真空度測定はできなかった
。そこで、本発明は前記の欠点を改善する真空計用の新
センサーを提案するものであり、轡に、両端固定タイプ
の振動子t−2つ接続した圧電振動子を効率よく励振す
る電極配置、構造を提供するものである。換言するなら
ば、等価直列抵抗R,の小さい、小型で、衝撃に強く、
信頼性に優r′した真空センサー圧電振動子を提供する
ものである。
However, recently, as devices have become smaller and lighter,
There is also a similar demand for vacuum gauges to be smaller and lighter. The Villany vacuum gauge mentioned above is large in size and penetrates, so it is a recent model! The reality is that %I2 cannot be fully met. or,
Conventional vacuum gauges that use vacuum sensors cannot measure the degree of vacuum in equipment that generates high-voltage fields, such as thruster furnaces. Therefore, the present invention proposes a new sensor for vacuum gauges that improves the above-mentioned drawbacks, and includes an electrode arrangement that efficiently excites piezoelectric vibrators in which two fixed-end type vibrators are connected to the back; It provides structure. In other words, it is compact, has a low equivalent series resistance R, and is strong against impact.
The present invention provides a vacuum sensor piezoelectric vibrator with excellent reliability.

〔問題点t−解決するための手段〕[Problem t-Means for solving]

槙3図は本発明の両端固定屈曲モード3次高調波振動で
の真空度と圧電振動子の等価厘列抵抗R1との関係を示
し、横軸に真空度(Toデデ〕を縦軸にR,(KΩ]を
とっている。例えば、圧電材料として水晶の場合、実験
によると真空度の劣化に伴って1!、は上昇tgける。
Figure 3 shows the relationship between the degree of vacuum and the equivalent row resistance R1 of the piezoelectric vibrator in the third-order harmonic vibration in the bending mode with both ends fixed according to the present invention. , (KΩ).For example, in the case of crystal as the piezoelectric material, experiments show that 1!, increases with the deterioration of the degree of vacuum.

そして、真空度0、ITorr〜ITorデと変化する
とそnに伴ってR,の上昇をまねく、即ち、本発明はR
ヨの真空度依存性に注目し、この関係から真空度を正確
に測定するものである。
When the degree of vacuum changes from 0 to 1 Torr, R increases accordingly.
By focusing on the vacuum degree dependence of y, the degree of vacuum can be accurately measured from this relationship.

実際には、振動子のR,が変化することは圧電振動子に
Nnる電流が変化する事と等価であり、実際の真空計と
してはKnる電流を真空度に変換して表示する。又、本
発明の振動子は衝撃に対して強くするために、片持ちタ
イプと異なって両端固定タイプを採用している。さらに
具体的に説明すると圧電振動子はセラミックス等の材料
でできている支持台座の上にセットさn、そして圧電振
動子の両端部に設けらnた支持部で接着剤等によって支
持固定さnる。そn故、本発明の圧電振動子は外乱、荷
に、特長を有する。次に、真空度と等個直列抵抗R,と
の関係を示す。圧電振動子の真空度に対する感度Sは高
真空時(10″″”l’or’r以上]の等個直列抵抗
R1、大気圧でのそn ’ft: R。
In reality, a change in R of the vibrator is equivalent to a change in the current Nn flowing through the piezoelectric vibrator, and in an actual vacuum gauge, the current Kn is converted into the degree of vacuum and displayed. Further, in order to make the vibrator of the present invention strong against shock, a fixed-end type is used, unlike a cantilever type. To explain more specifically, the piezoelectric vibrator is set on a support pedestal made of a material such as ceramics, and is supported and fixed with an adhesive or the like using support parts provided at both ends of the piezoelectric vibrator. Ru. Therefore, the piezoelectric vibrator of the present invention has features with respect to disturbances and loads. Next, the relationship between the degree of vacuum and the equal series resistance R is shown. The sensitivity S to the degree of vacuum of the piezoelectric vibrator is equal series resistance R1 at high vacuum (more than 10"""l'or'r), and n'ft: R at atmospheric pressure.

とすると次式で表さnる。Then, n is expressed by the following formula.

但し、ΔR=R1−R,である。However, ΔR=R1−R.

式■より明らかなように、感度Bt−高めるには圧電振
動子のR1を小さく、且つ、1ΔR1を大きくすnばよ
い。ここで、1ΔR1は振動子の形状、寸法によって決
まり、棒の幅W、長さLとすると、@Wに反比例し、長
、さLに比例する。従って、IΔR1t−大きくするに
は細い棒でしかも長いほど1ΔR1は大きくなる。しか
し、この靭長いnを基本波の屈曲モード振動をするよう
に圧電振動子上に励振電標を配置するとR,が大きくな
り、実質的感度日があまり大きくならない。そこで、本
発明は前記した細長い棒に屈曲モードの第8次高調波振
動を容易に引き起こす励振電極vi−配置することによ
り、同一寸法でもさらにRlt−小さくできるので感度
gを著しく大きくできるのである。第2図(a) 、 
Cb)は本発明の両端固定棒の振動子とその振動子が第
8次高調波振動したときの各位置での変位を示す。ここ
で、振動子の長さ一1幅W、厚みtである。第2−図の
)より明らかなように、変位が零となる箇所は4ケ所存
在する。ffOち、両端部とその端部から0.859L
の位置である。又、変位が零となる4箇所は歪が最も多
く発生する場所であるから、この4ケ所のいずnかに歪
が発生するように電極を配置すnばよい。この結果、屈
曲モードの第3次高調波振動での等価亘列抵抗R*’を
小さくでき、同一寸法の振動子でも感度日を高くするこ
とができる。
As is clear from equation (2), in order to increase the sensitivity Bt-, it is sufficient to reduce R1 of the piezoelectric vibrator and increase 1ΔR1. Here, 1ΔR1 is determined by the shape and dimensions of the vibrator, and if the width W and length L of the bar are inversely proportional to @W and proportional to the length L. Therefore, in order to increase IΔR1t, the thinner the rod is and the longer it is, the larger 1ΔR1 becomes. However, if an excitation electric mark is arranged on the piezoelectric vibrator so that this long n vibrates in the bending mode of the fundamental wave, R becomes large, and the actual sensitivity does not become very large. Therefore, in the present invention, by arranging the excitation electrode vi- which easily causes the eighth harmonic vibration in the bending mode on the elongated rod described above, Rlt- can be further reduced even with the same dimensions, so that the sensitivity g can be significantly increased. Figure 2(a),
Cb) shows the transducer of the rod fixed at both ends of the present invention and the displacement at each position when the transducer vibrates at the eighth harmonic. Here, the length of the vibrator is 1, the width is W, and the thickness is t. As is clear from Figure 2), there are four locations where the displacement is zero. ffOchi, both ends and 0.859L from that end
This is the position of Furthermore, since the four locations where the displacement is zero are the locations where the most strain occurs, the electrodes may be arranged so that the strain occurs at any one of these four locations. As a result, the equivalent series resistance R*' in the third harmonic vibration of the bending mode can be reduced, and the sensitivity can be increased even with a vibrator of the same size.

〔作用〕[Effect]

このように、本発明は圧1!振動子の拶動モード次数を
充分に考慮に入n、更に具体的に述べると屈曲モードの
第3次高調波振動の変位分布とその時に発生する歪分布
より、最適となる励振電極を圧電振動子上に設けること
により、第3次高調波振動を容易に引き起こし、lk小
さくすることができる。この結果、真空度に対する感度
を高めることができる。
In this way, the present invention has a pressure of 1! Taking into account the vibration mode order of the vibrator, and more specifically, from the displacement distribution of the third harmonic vibration of the bending mode and the strain distribution generated at that time, the optimum excitation electrode is selected for piezoelectric vibration. By providing it on the child, third harmonic vibration can be easily caused and lk can be reduced. As a result, sensitivity to the degree of vacuum can be increased.

〔実施例〕〔Example〕

以下に本発明の実施例を図面にもとづいて説明する。第
1図6)、の)は本発明の両端固定数屈曲モード圧電振
動子の実施例で、第1図(ハ)は圧電振動子固定の正面
図、第1図の)は第1図b)の側面図である。圧電振動
子1はセラミックス材料等で作らnている支持台座2の
上にセットさns接層剤4等によって、振動子の支持部
8の端部で支持固定さnている。そして、励振電極は6
腕の4面に配置さnていて、電極数は各面に8個づつ配
置さn、隣り合う電極は異極になるように配置さnてい
る。即ち、一方の腕には電極5,6,7,8,9.10
が、さらに、記号では示していないが俳面電槍5 、8
 、9にも対向面に各々と同極となる電極が配置さnて
いる。そして、斜線で示し几電極6.8.IQは同極に
、又、点で示し九電極5,7゜9は同極になるように接
続さnている(図示さnていない】。そして、2端子構
造を成している。
Embodiments of the present invention will be described below based on the drawings. Figures 1 (6) and 1) are examples of the bending mode piezoelectric vibrator with a fixed number at both ends of the present invention, Figure 1 (c) is a front view of the fixed piezoelectric vibrator, and Figure 1) is Figure 1 b. ) is a side view. A piezoelectric vibrator 1 is set on a support pedestal 2 made of a ceramic material or the like, and is supported and fixed at the end of a support portion 8 of the vibrator with a layer adhesive 4 or the like. And the excitation electrode is 6
They are arranged on four sides of the arm, with eight electrodes on each side, and adjacent electrodes are arranged so that they have different polarities. That is, one arm has electrodes 5, 6, 7, 8, 9.10
However, in addition, although not shown in symbols, there are haimen den spears 5 and 8.
, 9 are also provided with electrodes having the same polarity on their opposing surfaces. The diagonally shaded electrodes 6.8. IQ is connected to have the same polarity, and the nine electrodes 5, 7 and 9 (shown by dots) are connected to have the same polarity (not shown), forming a two-terminal structure.

全くrifI様に、他方の椀にも同梯の電極が配置さn
ているが、極性は反対になるように配置さnている。従
って、電極5 、7 、9 、11 、13 、15は
同極に、そして、電@6 、8.10,12,14.1
6は同極になるように設けらnている。こnにより、両
端固定屈曲モード第8次高調波多動を容易にすることが
できs”st小さくすることができる。
Just like rifI, the same ladder electrode is placed on the other bowl.
However, they are arranged so that the polarity is opposite. Therefore, electrodes 5, 7, 9, 11, 13, 15 are of the same polarity, and electrodes 6, 8.10, 12, 14.1
6 are provided so that they have the same polarity. This makes it possible to easily prevent the eighth harmonic hyperactivity in the bending mode with both ends fixed, and to reduce s''st.

〔発明の効果〕〔Effect of the invention〕

以上述べたように、本発明は真空度に対する感度Sを憂
めるには圧電振動子の等価直列抵抗R1金小さくすnば
よい。そして、本発明はlΔR1を大きくする細長い棒
に第8次高調波振動を容易に引き起こす励振電極の配置
によりR皿を小さくし、その結果、感度Bt−高くでき
真空度測定範囲を広くできるという効果を有する。さら
に、圧電振動子を真空センサーとしているから大変に小
型化、軽量化が可能であること、又、圧電振動子は支持
台座にマウントさnているから衝撃に強い等の効果t−
Nする。同時に、圧電振動子は高磁場に対しても強いの
で原子炉等の高研場発生装置内でも真空度測定ができる
効果音も有する。
As described above, in the present invention, in order to reduce the sensitivity S to the degree of vacuum, it is sufficient to reduce the equivalent series resistance R1 of the piezoelectric vibrator. In addition, the present invention has the effect of reducing the size of the R plate by arranging an excitation electrode that easily causes 8th harmonic vibration on a long and thin rod that increases lΔR1.As a result, the sensitivity Bt can be increased and the vacuum degree measurement range can be widened. has. Furthermore, since the piezoelectric vibrator is used as a vacuum sensor, it can be made extremely compact and lightweight, and since the piezoelectric vibrator is mounted on a support base, it has effects such as being resistant to shocks.
Do N. At the same time, since piezoelectric vibrators are strong against high magnetic fields, they also have sound effects that can be used to measure the degree of vacuum even in high field generating devices such as nuclear reactors.

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

第1図(φは本発明の圧電撮動子固定の正面図、第1図
の)は第1図れ)の側面図。 WJz図は本発明を説明する几めの両端固定圧電振動子
−と変位(b)t−示す図、 第8図は本発明の圧電振動子の真空度と等価直列抵抗と
の関係を示す因である。 1、、圧電撮動子 20.支持台座 80.支持部 46.接溜剤 5、〜160.電極 以上
FIG. 1 (φ is a front view of fixing the piezoelectric sensor of the present invention, and FIG. 1 is a side view of FIG. 1). The WJz diagram is a diagram showing the piezoelectric vibrator fixed at both ends and the displacement (b) t to explain the present invention, and Figure 8 is a diagram showing the relationship between the degree of vacuum and the equivalent series resistance of the piezoelectric vibrator of the present invention. It is. 1. Piezoelectric camera 20. Support pedestal 80. Support part 46. Coating agent 5, ~160. More than electrode

Claims (1)

【特許請求の範囲】[Claims] 屈曲モードで振動する両端固定の振動子を2つ接続した
圧電振動子に於いて、前記振動子の両端部と中央部に励
振電極を配置したことを特徴とする圧電振動子。
1. A piezoelectric vibrator comprising two connected vibrators fixed at both ends that vibrate in a bending mode, characterized in that excitation electrodes are arranged at both ends and the center of the vibrators.
JP5796685A 1985-03-22 1985-03-22 Piezoelectric vibrator Pending JPS61215932A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5796685A JPS61215932A (en) 1985-03-22 1985-03-22 Piezoelectric vibrator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5796685A JPS61215932A (en) 1985-03-22 1985-03-22 Piezoelectric vibrator

Publications (1)

Publication Number Publication Date
JPS61215932A true JPS61215932A (en) 1986-09-25

Family

ID=13070752

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5796685A Pending JPS61215932A (en) 1985-03-22 1985-03-22 Piezoelectric vibrator

Country Status (1)

Country Link
JP (1) JPS61215932A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04131032U (en) * 1991-05-27 1992-12-01 日本航空電子工業株式会社 Torsional vibration twin tuning fork type vibrator
JP2011217348A (en) * 2010-03-17 2011-10-27 Seiko Epson Corp Vibrator element, sensor element, sensor, and electronic apparatus

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04131032U (en) * 1991-05-27 1992-12-01 日本航空電子工業株式会社 Torsional vibration twin tuning fork type vibrator
JP2011217348A (en) * 2010-03-17 2011-10-27 Seiko Epson Corp Vibrator element, sensor element, sensor, and electronic apparatus

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