JPS5862918A - Tuning fork type bending crystal oscillator - Google Patents

Tuning fork type bending crystal oscillator

Info

Publication number
JPS5862918A
JPS5862918A JP16159181A JP16159181A JPS5862918A JP S5862918 A JPS5862918 A JP S5862918A JP 16159181 A JP16159181 A JP 16159181A JP 16159181 A JP16159181 A JP 16159181A JP S5862918 A JPS5862918 A JP S5862918A
Authority
JP
Japan
Prior art keywords
tuning fork
fork type
axis
crystal oscillator
bending crystal
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
JP16159181A
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 Instruments Inc
Original Assignee
Seiko Instruments Inc
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 Instruments Inc filed Critical Seiko Instruments Inc
Priority to JP16159181A priority Critical patent/JPS5862918A/en
Publication of JPS5862918A publication Critical patent/JPS5862918A/en
Pending 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
    • H03H9/21Crystal tuning forks
    • H03H9/215Crystal tuning forks consisting of quartz

Abstract

PURPOSE:To obtain a large frequency change against temperature, by selecting a cut-angle suitably. CONSTITUTION:A tuning fork bending crystal oscillator is formed with a Z plate. This tuning fork type bending crystal oscillator is turned by an angle phi, taking the X axis as a rotary axis and an angle of theta, taking a new axis Z' of the Z axis as a rotary angle. Denoting phi=-30-30 deg. and theta=25-165 deg., the tuning fork type bending crystal oscillator with a large frequency change, i.e. excellent sensitivity can be obtained. In using this oscillator as a temperature sensor for a clinical thermometer, with a short thermometry time and excellent resolution, i.e. excellent accuracy, the clinical thermometer can be obtained.

Description

【発明の詳細な説明】 本発明は体温計用音叉型屈自水晶振動子のカット角に関
する0本発明の目的はカット角を最適に選ぶ拳により塩
度に対する周波数変化の大きい。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a cut angle of a tuning fork type quartz crystal resonator for a thermometer.An object of the present invention is to optimally select a cut angle so that the frequency changes with respect to salinity are large.

即ち、感度の良い音叉型屈曲水晶!&iM子を提供する
@にめゐ。
In other words, a tuning fork-shaped bent crystal with good sensitivity! @Nimei provides &iM child.

通”常、体温計としては水銀ガラス体温針が多用されて
来た。この理由としてIfiまず第−KJIEiiでる
る、夏に、安価でるり、取り扱いが簡単でろる等が挙げ
られる。しかし、この水銀体温計にも欠一点がある。向
えは1体温の測定時間が長く、新生児や乳幼児への検温
が難しい、振下げが面倒、更に、壊れやすいという欠点
がめった。最近はこれらの欠点gr改善したサーミスタ
一体温計が出現しているが、偏度と抵抗の関係か直線で
ない、tfc。
Normally, mercury glass thermometer needles have been widely used as thermometers.The reasons for this are that they are easy to use, easy to use in summer, inexpensive, and easy to handle.However, this mercury Thermometers also have shortcomings.They take a long time to measure body temperature, are difficult to measure the temperature of newborns and infants, are troublesome to shake, and are easy to break.Recently, these shortcomings have been improved. Thermistor type thermometers have appeared, but the relationship between eccentricity and resistance is not a straight line, TFC.

サーミスターは製造による素子のバラツキがるり、素子
の互換性をも九せにくいことも欠点でめった。
Thermistors suffer from the disadvantages of large variations in the elements due to manufacturing and the difficulty in ensuring element compatibility.

更に1体温時間が水銀体温計より改善されて来ているが
約1分〜2分と長く満足できるようなものでなかった。
Furthermore, although the time required for one body temperature has been improved over that of a mercury thermometer, it is still unsatisfactory and takes about 1 to 2 minutes.

そこで、本発8Aは新しく1体温計の塩度センサーとし
て音叉型屈曲水晶振動子を提案するものであり、カット
角の選択によって体温計用としてg度の良い超少型の音
叉型屈曲水晶振動子ta!供する蔓ができる。それ故、
検量時間の頬い電子体11計管可?!にするものでるる
Therefore, the present invention 8A proposes a new tuning fork type bent crystal oscillator as a salinity sensor for a thermometer.By selecting the cut angle, an ultra-small tuning fork type bent crystal oscillator with a good g degree can be used for thermometers. ! A vine will form to serve. Therefore,
Is it possible to measure 11 electronic bodies during calibration time? ! There is something to do.

以下、8面に沿って本発tat−詳細に説明する。Hereinafter, the present invention will be explained in detail along the 8th plane.

体温計として1!釆される物性としては、(1)  熱
応答性を良くするために小型・軽量でるること。
1 as a thermometer! The physical properties to be considered are: (1) It must be small and lightweight to improve thermal response.

(2111度に対する周波数感度が良いこと。(Good frequency sensitivity to 2111 degrees.

が挙げられる。この2つの内、(1)については最近、
音叉型屈曲水晶振動子を使ってかなり小型の水晶ユニッ
トが開発され、腕時計の涼扱として多用されている。そ
れ故、これを体温計の湯度ヤンサーとして使用し穴場合
、熱応答性が良く体温を検出する時間を短くする事が出
来る。
can be mentioned. Of these two, regarding (1), recently,
A fairly small crystal unit was developed using a tuning fork-shaped bent crystal unit, and is often used as a cooling device for wristwatches. Therefore, when this is used as a hot water sensor for a thermometer, it has good thermal response and can shorten the time it takes to detect body temperature.

第1〜は本発明の音叉型屈曲振動子か子の電極配置の一
実施例の斜視卸で、音叉型水晶1には励振電接2,5が
配置されている。
1 to 1 are perspective views of an embodiment of the electrode arrangement of a tuning fork type bending vibrator according to the present invention, in which excitation electrical contacts 2 and 5 are arranged on a tuning fork type crystal 1.

第2図は第1図のA−A断面図を示し、音叉型水晶1の
表裏面と側面に励振電極を配置した例でめの、N、RN
圧管印加したときは矢印方向VcW介はかかる。交番璽
圧會印加することによって電界方向は逆転し、屈曲モー
ドで励振させる事ができる。
FIG. 2 shows a cross-sectional view taken along the line A-A in FIG.
When the pressure tube is applied, VcW is applied in the direction of the arrow. By applying an alternating force, the direction of the electric field is reversed, making it possible to excite it in the bending mode.

15図は本発明の音叉型屈曲水晶振動子の電極配置の池
の実施例の斜視図で、音叉型水晶40我裏面にのみ励振
電極5.6が配置された例である。
FIG. 15 is a perspective view of an embodiment of the electrode arrangement of the tuning fork type bent crystal resonator of the present invention, and is an example in which excitation electrodes 5.6 are arranged only on the back side of the tuning fork type crystal 40.

紀4図は第5図のB−B断面口でろる。第2■と同様へ
直fit圧によらて矢印方向KIIl界は動く、交番電
圧を印加する事によって電界方向は逆転し、屈曲モード
で励振さゼる事ができる。
Figure 4 is located at the B-B cross section in Figure 5. As in the second case, the KII field moves in the direction of the arrow due to the direct fit pressure.By applying an alternating voltage, the direction of the electric field is reversed, and it is possible to excite it in the bending mode.

第5図は本発明の水晶畿動子ユニットを示し、ステム1
2とキャンプ10から構成されている。
FIG. 5 shows a crystal oscillator unit of the present invention, with stem 1
It consists of Camp 2 and Camp 10.

ユニット内には旨叉型屈曲水晶伽動子7が支持リード線
8,9eこ半田あるいは接着剤によって固着されている
。又、キャラ710Vi洋白(65%(Iu−10%N
1−残Zn)でできているか熱電導性が不光分であるの
で更に表面には一部、ろるうは全面に熱電導性の良い材
料、例えば、佐メッキ11が施されている0体温Fi金
メッキ11管介して音叉型屈曲水晶振動子の共振周波数
で測定される。水晶ユニットの直径口は約1.5−m6
.長さT、+F!約61IIsと超小塵の水晶ユニット
であるから質量も小さく熱応答性は優れている。
Inside the unit, a fork-shaped bent crystal mover 7 is fixed to support lead wires 8, 9e by solder or adhesive. Also, Chara 710Vi nickel silver (65% (Iu-10%N)
1- Residual Zn) Since the thermoconductivity is non-luminous, a part of the surface is coated with a material with good thermoconductivity, such as Samekki 11, on the entire surface of the wax. It is measured at the resonant frequency of a tuning fork type bent crystal resonator through an 11-fi gold-plated tube. The diameter of the crystal unit is approximately 1.5-m6
.. Length T, +F! Since it is an ultra-fine crystal unit of about 61 IIs, its mass is small and its thermal response is excellent.

第6図は常温からJ4o℃に1度を変化さぜ喪ときの共
通周波数の安定する時間を示している。
FIG. 6 shows the time required for the common frequency to stabilize when the temperature changes by 1 degree from room temperature to J4o°C.

常温での共振周波1!!fo  から約40℃での共振
局tII数fIVcなり安定するには約15秒から20
秒と従来の素子と比較して熱応答性は′I[當に良い事
が分かる。
Resonance frequency 1 at room temperature! ! From fo to the resonance station tII number fIVc at about 40℃, it takes about 15 seconds to 20 seconds to stabilize.
It can be seen that the thermal response is quite good compared to the conventional element.

次に、(2)の温度に対する周波数W&度が良いことが
必要であり、通常は絶対値でzoppφ以上の周波数感
度管持つ音叉型屈曲振動子が必侵である。
Next, in (2), it is necessary that the frequency W and degree with respect to the temperature be good, and normally a tuning fork type bending vibrator having a frequency sensitivity tube with an absolute value of zoppφ or more is required.

第7因は本発明の音叉型屈曲水晶振動子で2板から形成
された例でるる。
The seventh factor is an example of the tuning fork type bent crystal resonator of the present invention formed from two plates.

第8図番1丸7図の音叉型屈曲水晶振動子をX軸を回転
軸として(反w8引方向を正とする)φg向回転、更に
、z軸の新軸ガ軸管回転軸として0度回転したときのφ
、θ度と周波数感度αとの関係で、0m−50,。0°
、30°のときのj[i的関係である。#雪0° のさ
き、φが大きくなるに従って、周波数感度は大きくなり
α−−2αppm/’Cとなるカット角φは約25°で
6号、更に、φが大きくなるとαFi増加し50[から
6orlFの間でαは最大となり、そのときのαけ約−
80/lと非常に大きい感度管示す、更に、カット角が
大きくなるとαは小さくなりφが約90艷付近でαは極
小となり、カット角がさらに大きくなるとふたたびαに
大きくなり約120度、でali’l極大となり、カッ
ト角ψが大きくなるに従つ“て、αの絶対値は小さくな
りαが−20/”C,!−なるカット角は約165度で
6る。 UIC%# −5II’、50° ト2’軸回
転をする事vζよってαは若干変化する。7このとき、
aの変化tC対し、φΩ変化によるαは0−0のときの
全く同層−こ変化する1本理論計3IKよるとσN−3
0°、  50.”  f)トf!ia −−20pp
I/ICトlkhカット角φけ約20°・と約16&o
 である、即ちφ富25(165’ で#■−50°〜
506であれd本発明のαを提供する事ができる。
Rotate the tuning fork type bent crystal resonator in Figure 8, No. 1, Circle 7 in the φg direction with the X axis as the rotation axis (with the anti-W8 pull direction as positive), and further rotate the z-axis with the new axis as the tube rotation axis. φ when rotated by degrees
, 0m-50, due to the relationship between θ degrees and frequency sensitivity α. 0°
, 30°, it is a j [i relationship. #Before snow 0°, the frequency sensitivity increases as φ increases, and the cut angle φ that becomes α-2αppm/'C is approximately 25°, which is 6. Further, as φ increases, αFi increases, and from 50[ α becomes maximum between 6orlF, and at that time α coefficient −
The sensitivity tube is very large at 80/l.Furthermore, as the cut angle increases, α decreases, and when φ is around 90 degrees, α reaches a minimum, and when the cut angle becomes even larger, α increases again to about 120 degrees. ali'l reaches a maximum, and as the cut angle ψ increases, the absolute value of α decreases, and α becomes −20/”C,! - The cut angle is approximately 165 degrees, which is 6. UIC%# -5II', 50° α changes slightly due to the 2'-axis rotation vζ. 7 At this time,
For the change tC in a, α due to the change in φΩ is exactly the same as when it is 0-0.According to the theoretical total 3IK, σN-3
0°, 50. ” f) トf!ia --20pp
I/IC cut angle φ approximately 20° and approximately 16°
That is, φ wealth 25 (165' and #■ -50° ~
506 can provide α of the present invention.

以上述べたφ、θとαの関係は理論値でるるか、本発明
のカット角u諺0°、φ−120’  での実験でけα
−−1007’cと大変に周波数感度の良い、音叉型屈
曲振動子動子を得る事がで、!た。・次1tch具体的
に例を挙けて説明すると1.計時用として共振周波数f
、  を52768Hzを使用し、湯度検出用として共
振周波数f、’410へ0OOH2を使用し、周波数−
感度αt′−1GO/′cとすると廁定時間・1秒で温
度分解能がa1℃と相当に良い体温計を提供できると同
時に、検温時間が測定時間を含めて士数秒と従来のサー
ミスターのに〜%と短縮できる。又、塩度分解能は周波
数感度と計時用共振周波数と湿度検出用共振周波数によ
って決められ、分解能は周波数感度が良い#1ど、共振
周波数が高いほどろがる。
Is the relationship between φ, θ, and α described above a theoretical value, or is it determined by an experiment using the cut angle u of the present invention of 0° and φ-120'?
--1007'c, a tuning fork type bending vibrator with very good frequency sensitivity can be obtained! Ta.・Next 1tchTo explain with specific examples, 1. Resonant frequency f for timekeeping
, using 52768Hz, using resonance frequency f, '410 to 0OOH2 for hot water temperature detection, and frequency -
If the sensitivity is αt'-1GO/'c, it is possible to provide a thermometer with a temperature resolution of a1℃ in a fixed time of 1 second, which is quite good, and at the same time, the temperature measurement time including the measurement time is several seconds, which is much faster than that of conventional thermistors. It can be shortened to ~%. Further, the salinity resolution is determined by the frequency sensitivity, the resonant frequency for timing, and the resonant frequency for humidity detection, and the resolution becomes worse as the resonant frequency becomes higher, such as #1, which has good frequency sensitivity.

以上、述べたように本発明は音叉型屈曲水晶撮動子のカ
ント角を最適に選ぶことによって周波数感度の良い音叉
型屈曲水晶撮動子を提供し、この振動子を体温計の塩度
センサーとして使用することによって、検温時間の短い
、分′lf4能の良い、即ち、精度の良い体温針管提供
する事ができ友。
As described above, the present invention provides a tuning fork type bent crystal sensor with good frequency sensitivity by optimally selecting the cant angle of the tuning fork type bent crystal sensor, and uses this vibrator as a salinity sensor for a thermometer. By using this, it is possible to provide a temperature needle tube that takes a short temperature measurement time and has good minute function, that is, has high accuracy.

これにより新生児、あるいは乳幼児の体温測定vC@ま
される事が71k(なった。
As a result, it is no longer necessary to measure the body temperature of newborns or infants by 71k.

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

第1Nは本発明の音叉型屈曲水晶振動子のt極配置の一
実施例の斜視−である。 w42図扛第1図のA−A断翻図を示す。 第5図は本発明の音叉型屈曲水晶振動子の電極配置の油
の実施例の斜視図でろる。 第4図は第5図のB−BIIFr面図である。 第5図は本発明の水晶振動子ユニットの断面図を示す。 舘6図は常温から約40℃に塩度を変化させたときの共
振層f1.IIXの安定する時間を示すグー)7でめる
。 m7図はヰ発明の音叉型屈曲水晶振動子で2板から杉成
され食倒の斜視図でおる。 m8図は第7囚の音叉型屈曲水晶振動子をX軸を回転軸
としてφ度、更に、Z軸の新軸d軸を回転軸としてU度
圓転したときのφ、#と周波数感1にαの関係を示すグ
ラフで理論値である。 X・・・電気軸   !・・・機械軸 2・・・元軸 以  上 出鵬人 株式会社 第二精工舎 代理人 弁理士 最 上   務 III 図 第6図 @2ae II4図 115図
1N is a perspective view of one embodiment of the t-pole arrangement of the tuning fork type bent crystal resonator of the present invention. Fig. w42 shows an AA cutaway of Fig. 1. FIG. 5 is a perspective view of an embodiment of the electrode arrangement of the tuning fork type bent quartz crystal resonator of the present invention. FIG. 4 is a B-BIIFr plane view of FIG. 5. FIG. 5 shows a sectional view of the crystal resonator unit of the present invention. Figure Tate 6 shows the resonance layer f1. when the salinity is changed from room temperature to about 40°C. 7 indicates the time for IIX to stabilize. Figure M7 is a perspective view of the tuning-fork type bent crystal resonator of I's invention, which is constructed from two plates. The m8 diagram shows the φ, #, and frequency sensitivity when the tuning fork type bent crystal resonator of the seventh prisoner is rotated by φ degrees with the X axis as the rotation axis, and further rotated by U degrees with the new axis of the Z axis, the d axis, as the rotation axis. This is a graph showing the relationship between α and the theoretical value. X...Electric axis! ...Machine axis 2...More than the original axis Mr. Daini Seikosha Co., Ltd. Agent Patent attorney Tsumugi Mogami III Fig. 6 @ 2ae Fig. II 4 Fig. 115

Claims (1)

【特許請求の範囲】[Claims] 音叉形状−KyEp成された水晶振動子で、前記音叉形
水晶振動子Fizw、txmt回転軸として25度から
165度回転し、更に、zの新軸l軸を回転軸として一
50度から30度回転した板より成形されている事t−
%徴とする音叉型屈曲水晶振動子。
The tuning fork-shaped crystal resonator has a KyEp shape, and the tuning fork crystal resonator Fizw, txmt rotates from 25 degrees to 165 degrees as the rotation axis, and further rotates from 150 degrees to 30 degrees using the new axis of z, the l axis, as the rotation axis. It is formed from a rotated plate.
Tuning fork type bent crystal resonator with % signature.
JP16159181A 1981-10-09 1981-10-09 Tuning fork type bending crystal oscillator Pending JPS5862918A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16159181A JPS5862918A (en) 1981-10-09 1981-10-09 Tuning fork type bending crystal oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16159181A JPS5862918A (en) 1981-10-09 1981-10-09 Tuning fork type bending crystal oscillator

Publications (1)

Publication Number Publication Date
JPS5862918A true JPS5862918A (en) 1983-04-14

Family

ID=15738040

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16159181A Pending JPS5862918A (en) 1981-10-09 1981-10-09 Tuning fork type bending crystal oscillator

Country Status (1)

Country Link
JP (1) JPS5862918A (en)

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