JPS58113730A - Electronic clinical thermometer - Google Patents

Electronic clinical thermometer

Info

Publication number
JPS58113730A
JPS58113730A JP56210829A JP21082981A JPS58113730A JP S58113730 A JPS58113730 A JP S58113730A JP 56210829 A JP56210829 A JP 56210829A JP 21082981 A JP21082981 A JP 21082981A JP S58113730 A JPS58113730 A JP S58113730A
Authority
JP
Japan
Prior art keywords
signal
temperature
counting
crystal oscillator
counter
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
JP56210829A
Other languages
Japanese (ja)
Inventor
Seizo Yoshikawa
吉川 晴三
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 JP56210829A priority Critical patent/JPS58113730A/en
Publication of JPS58113730A publication Critical patent/JPS58113730A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01KMEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
    • G01K7/00Measuring temperature based on the use of electric or magnetic elements directly sensitive to heat ; Power supply therefor, e.g. using thermoelectric elements
    • G01K7/32Measuring temperature based on the use of electric or magnetic elements directly sensitive to heat ; Power supply therefor, e.g. using thermoelectric elements using change of resonant frequency of a crystal
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01KMEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
    • G01K13/00Thermometers specially adapted for specific purposes
    • G01K13/20Clinical contact thermometers for use with humans or animals

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Measuring Temperature Or Quantity Of Heat (AREA)

Abstract

PURPOSE:To measure the bodily temperature with high accuracy in a short thermometic time, by using a small-sized crystal oscillator as a temperature sonsor. CONSTITUTION:A detection pulse signal P1 is inputted to a counter 7 as a counting pulse and on one hand, a reference pulse sigal P2 is applied to the counter 7 as a gate signal and reset signal. Further, counting of the number of input pulses of the signal P1 at each rising point of the signal P2 is started and its counting action is continued during the time when a level of the signal P2 is high. And, the counting action is ended at each falling point of the signal P2 and the counter 7 is reset. After all, pulse number of the signal P1 generated at a high level period T of the signal P2 are counted repeatedly by the counter 7 and its counted data D are taken out as an output of a counting circuit 3.

Description

【発明の詳細な説明】 本発Fij4は電子体温計に関し、更に特定して述べる
と、I1度竜ン夕として小型の水晶振動子管用いt電子
体温計に@する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electronic thermometer, and more specifically, it is an electronic thermometer using a small crystal oscillator tube as an I1 degree thermometer.

従来から m度センサとしてサーミスタを用い★電子体
温針が広く用いられているが、1−1スタを用いた電子
体温計の場合には。
Conventionally, a thermistor has been used as the m degree sensor, and electronic body temperature needles have been widely used, but in the case of electronic thermometers that use a 1-1 star.

(&1 サーミスタ素子の特性の製造上のバラツキが大
舞〈、素子の互換性tもtせf(い。
(&1) There are large manufacturing variations in the characteristics of the thermistor elements, and the compatibility of the elements is also poor.

(b)  t−ミスタ素子の抵抗値とIl膨とのl11
411が直線でないtめ信脅処珍が警備となる。
(b) l11 between the resistance value of the t-mister element and the Il expansion
If 411 is not a straight line, it will be used as security.

(c)アナログ処m回路管必智とするため、電源、電圧
、アンプ等のド11フトの影響にLh s+定静誤差生
じやすい。
(c) Since the analog processing circuit is essential, Lhs + static errors are likely to occur due to the influence of drifts such as power supply, voltage, amplifier, etc.

勢の欠点を有している。It has some disadvantages.

これらの欠点管解消する★め、従来においても。These shortcomings can be resolved in the conventional system as well.

水晶振動子を温度セン賃とし*11度針が用いられてい
るが、セン賃としての水晶振動子の熱容量が大舞いので
検温時間が比験的長い上#r、l1ff化に対する8波
数変仕が小さく、Va定精度が低いという欠点を有して
いる。1*、従来の水晶式sit針でに、水晶lfl動
子の尭蜘同波数が高い大め1発振回路における消費電諸
が大き(、電池動作による携帯性に優れ★体温針管構成
することが困難であつ★。
A crystal oscillator is used as a temperature sensor and an 11 degree needle is used, but since the heat capacity of the crystal oscillator is large, the temperature measurement time is relatively long. It has the disadvantage that the value of Va is small and the accuracy of determining Va is low. 1*.In the conventional crystal SIT needle, the power consumption in the large 1 oscillation circuit with high frequency of the crystal lfl oscillator is large (and it has excellent portability due to battery operation. It's difficult and hot★.

本発明の目的材、従って、!1かい検温時間でょ鈴高精
度に体温の測定を行なうことができ、携帯I!Iff優
れt電子体温計f梯供することVrIhる。
The object material of the present invention, therefore! It is possible to measure body temperature with high accuracy within 1 month of temperature measurement time, and it is a portable I! If you are looking for an excellent electronic thermometer, you can use it.

本発明の電子体魯計Fj、フォトIIングラフメ技#を
用いて作つ*sui:*数e)大亀い音叉型温度センサ
水晶振動子と、この温度センサ水晶69子の振V崗期を
測定する周期沖1定回路と1周期測定回#ff′1?叶
るm1定結果から被検温体の温度管演算する演11回路
と、演算回路からの演算結果に従って温度f表示する表
示餘とを備えた点に特徴がめる。
The electronic body temperature sensor Fj of the present invention is made using the photo II graphing technology #Sui: *Number e) Okame tuning fork type temperature sensor crystal oscillator and the vibration period of this temperature sensor crystal 69 element is measured. 1 constant circuit and 1 period measurement #ff'1? It is characterized by the fact that it is equipped with an operation circuit which calculates the temperature of the temperature body to be tested from the m1 constant result obtained, and a display unit which displays the temperature f according to the calculation result from the calculation circuit.

趣下、−示の実線−により本発IP1管詳細f説明する
Below, the details of the IP1 tube of the present invention will be explained using the solid line shown below.

w111ハ本発明rする電子体温計の一実施例のブロッ
ク図管示し、この電子体温計1に、被検温体(図示せず
)の検温センナとして、音叉型温1センサ水晶IIs千
2を備えている。この水晶振動子2に、後で詳しく述べ
るように、小型で、熱容量が小さく、単位温度賞化轟り
の振動周期の質4Ffd大−くなるように構成されてお
り、この振動周期を計数する★めの計数回路5#1ri
lII綬これている・ 計数回路5に、水晶振動子2と接続されて発振回路f#
Ilする検出信置発生回路4と、基本水晶発振回路5と
を備え、検出信員発生回−4からに水晶振動子2の振l
#I18期に従う周期の繰返しパルス信号が検出パルス
信書P1として出カメねる。
W111C shows a block diagram of an embodiment of the electronic thermometer according to the present invention, and the electronic thermometer 1 is equipped with a tuning fork type temperature sensor 1 sensor crystal IIs 2 as a temperature measuring sensor for a body to be tested (not shown). . As will be described in detail later, this crystal oscillator 2 is small, has a small heat capacity, and is configured so that the vibration period of the unit temperature is 4Ffd large, and this vibration period is counted. ★Me counting circuit 5#1ri
This is the case. The counting circuit 5 is connected to the crystal oscillator 2 and the oscillation circuit f#
It is equipped with a detection signal generation circuit 4 that generates a signal and a basic crystal oscillation circuit 5, and the vibration of the crystal oscillator 2 starts from the detection signal generation circuit 4.
A repetitive pulse signal having a period according to the #I18 period is output as the detection pulse letter P1.

一方、基本水晶発振回路5に、湿度特性の良好な水晶振
動子6f含んで成りs1m囲温度の質化に拘らず、実質
的に所定の一定繰返し一期のパルス信号でめる基本パル
ス信号Paが出力される。
On the other hand, the basic crystal oscillator circuit 5 includes a crystal oscillator 6f with good humidity characteristics, and the basic pulse signal Pa is substantially generated by a predetermined constant repetition of one period of pulse signals regardless of the quality of the ambient temperature. is output.

第2図(al 、 (b)から判る1うf、基皐パルス
信憐ア■の繰返し一期は、検出パルス信書Fsの繰返し
周期よりも長く設定されている。
As can be seen from FIGS. 2(al) and (b), the repetition period of 1f and 2 is set longer than the repetition period of the detection pulse message Fs.

第1′fAr戻ると、検出パルス信号11に、力ゆン夕
7に計数パルスとして入力されており、一方。
Returning to the 1st fAr, the detection pulse signal 11 is input as a counting pulse to the force generator 7, and on the other hand.

基本パルス信号P―は、カウンタ7にゲート信号兼リセ
ット信号として印加されており、基準パルス信号PsO
各立上)時点で検出パルス信号P1の入力パルス数の計
数管−始し、基準パAX信号F、のレベルが高レベルの
期間中その計数−作を継続せしめる。そして、基本パル
ス信号シーの会立下り時点において計数1・作が終了し
、カウンタ7がリセットされる。即ち、基醜パルス信!
psの高レベル期間テにおいて発生する検出パルス信i
i F 、 f)パルス数が力bン夕7Fおいて繰返し
計#!iメれ、その計数データDが計数回路Sの出力と
して暖めされる。従って、計数データDに、検出パルス
信号Psの周波数、即ち、繰返し周期ff1lする情W
t有しているととfなる。
The basic pulse signal P- is applied to the counter 7 as a gate signal and a reset signal, and the reference pulse signal PsO
The counter starts counting the number of input pulses of the detection pulse signal P1 at each rising point, and continues counting while the level of the reference signal F is at a high level. Then, at the falling edge of the basic pulse signal C, counting 1 is completed and the counter 7 is reset. In other words, the fundamental pulse belief!
The detection pulse signal i generated during the high level period of ps
i F, f) When the number of pulses is equal to 7F, the repetition counter #! Then, the counting data D is heated as the output of the counting circuit S. Therefore, the count data D includes information W that is the frequency of the detection pulse signal Ps, that is, the repetition period ff1l.
If it has t, it becomes f.

バイナリデータとして峨出ph大計数データD汀、演算
回路8f入力ζねる。演算回路8に、予め判っている水
晶振動子2の温度とその時の検出パルス信14 F *
の@波数との間の関係に基づいて。
The output ph large count data D is input as binary data to the arithmetic circuit 8f. The arithmetic circuit 8 receives the pre-known temperature of the crystal oscillator 2 and the detection pulse signal 14 F *
Based on the relationship between @wavenumber and

計数データD管、ii度管示す温度データKKt換する
。従って、演算@@Bとしてt−j、911えは上述の
温度と一波数との間の+snが書−込まれているT4o
Mt用いて構成することがで参る。
The counting data D tube and the temperature data KKt shown in the ii degree tube are exchanged. Therefore, as the calculation @@B, t-j, 911 is T4o where +sn between the above-mentioned temperature and one wave number is written.
It can be configured using Mt.

−縦データ!に1表示回路9f入力され、そOwkkの
温度がディジタル形式にて表示される。
-Vertical data! 1 display circuit 9f is inputted to 1 display circuit 9f, and the temperature of that Owkk is displayed in digital form.

w4s図1h本発明による電子体温計の重書な構匝豐件
である音叉嬰温度セン賃水晶振動子2のユニットの構造
を示す断面−が示されている。水晶振か子2は、ステム
21とキャップ22とt有し・キャップ22内ffFi
音叉型屈曲水晶1!e子ニレメン)2Mが、半田付文に
接着剤fLって支持II−V線24.25ff固着され
て成っている。キャップ22ij、洋白(65910u
−10%Ni −残Zn)から成り、熱伝導性?向上さ
せる斤め。
Fig. 1h shows a cross section showing the structure of a unit of a tuning fork temperature sensor and a crystal oscillator 2, which is an important structure of the electronic thermometer according to the present invention. The crystal pendulum 2 has a stem 21, a cap 22, and a ffFi inside the cap 22.
Tuning fork type bent crystal 1! 2M is fixed to the soldering pattern with adhesive fL and support II-V wires 24.25ff. Cap 22ij, nickel silver (65910u
-10%Ni -Remaining Zn) and has thermal conductivity? Improve your loaf.

その表面trta金メツ中層26が形成されている。A trta gold metal intermediate layer 26 is formed on the surface thereof.

従って、被検温体の温度は、この金メッキ層!6を介し
て鳥好f水晶振動子エレメント25ff伝達される。こ
のキャップ22の直l!は約t5■が。
Therefore, the temperature of the warm body to be tested is this gold plating layer! 6 to the Toriyoshi f crystal oscillator element 25ff. This cap is straight from 22! is about t5■.

長ざは約6−に形成されており、fiめて軽量で参るか
ら、熱容量も著しく小ざ〈、被検温体の温度に金メツ中
層26f介してずばや(水晶振動子エレメント2Sf伝
達され、熱応答tirx極めて優れている。
The length is approximately 6 mm, and since it is light in weight, the heat capacity is also extremely small. , thermal response TIRX is extremely excellent.

この水晶振動子エレメント25に、第4図に詳#lff
示す1うに、11叉型の平板状部材に形成されており、
その主平面fFj励振電極27.28が配普メれると共
に、その反射−の平面にも励振璽会が配W−;Xれてい
る。そして、これらの励振電極に交番電昇を印加すると
とVrlわ、第5図に示すようf水晶振動子エレメント
25が屈曲モート9で励振源ねる。
For this crystal oscillator element 25, details #lff are shown in FIG.
As shown in 1, it is formed into an 11-pronged flat plate member,
The excitation electrodes 27 and 28 are disposed on the main plane fFj, and an excitation ring is also disposed on the reflection plane. When an alternating current voltage is applied to these excitation electrodes, the f-crystal resonator element 25 becomes an excitation source at the bending moat 9, as shown in FIG.

#61!!i!l#/rに、水晶振か子エレメント2S
の切出し状物が示ざわている。既f述べkようff、こ
の水晶振動子ニレメン) 25jJ、その振動周期が大
食なI!度%性ケ廟することが必要とされるため。
#61! ! i! l#/r, crystal pendulum element 2S
A cutout-like object is visible. As I have already said, this crystal oscillator is 25jJ, and its vibration period is voracious! Because it is necessary to have a degree of sexual intercourse.

その切出し方向及び角lILを樵々変えて最も温度特性
が大★くなる切出し状物が選ばれている。この−Ifに
、水晶振か子エレメント2■ハ z截−を!114+を
回虻軸として所定の角11″0(反時計方向管圧方向と
する)回(させて切出している。
The cut-out direction and angle lIL are changed depending on the woodcutter, and the cut-out material with the greatest temperature characteristics is selected. In this -If, crystal pendulum element 2■Ha zcut-! It is cut out at a predetermined angle of 11''0 (counterclockwise direction of pipe pressure) with 114+ as the turning axis.

蒙7ryUvに、θの値と1℃当りの8波数費化寒αと
の一優がグラフにて示ブれている。このグラフから刊る
工うv、eが大壷くなるf従ってαは大負(なわ、α−
−20(ppM/T、)となるカット角θに約25°で
ある。更Vrθが増大するとaもl!f増大し、50°
から60”(D闇テa rj最大と′fkh、その時の
αに約−80〔アPM/’C)  と非常f天真な値と
なる。
At 7ryUv, the graph shows the difference between the value of θ and the 8-wave number cost per 1°C. From this graph, we can calculate that v, e becomes a large pot, and therefore α is very negative (α−
-20 (ppM/T,), the cut angle θ is approximately 25°. Furthermore, as Vrθ increases, a also increases! f increases, 50°
60'' (maximum D darkness and fkh, α at that time is approximately -80 [a PM/'C), which is a very naive value.

更にカット角が大壷(丹ると、αけ小型(なり。Furthermore, the cut angle is large (tan) and α small (α).

θが約90°付近ではαij棲小となる。#が史f大食
くなると、αは再び大きくηわ、θ−120゜でαは極
大となり、以vk、θが大−(なるに従って一αの絶対
値は小ざくなり、σ−165°付近でα謬−20CPP
M/”C)  となる、ところで0体温計のセンサの加
電用途fおいてに、αの[H。
When θ is around 90°, αij is small. When # becomes history f gluttony, α increases again to η, and α reaches its maximum at θ-120°, and after that, as vk and θ become larger, the absolute value of α becomes smaller and becomes σ-165°. α-20CPP nearby
By the way, in the application f of the sensor of a zero thermometer, [H of α].

通常、少なくとも絶対値で−20(prM/’C)の変
化IIが必要であるから、θの値とじては、25゜乃至
165@の岬囲管使用すれば工いことVrなゐ。
Normally, a change II of at least -20 (prM/'C) in absolute value is required, so if a cape envelope tube with a value of θ of 25° to 165@ is used, no modification is necessary.

次f、第111(a)乃至第81H(a)會参照して、
第6図及び第71!!lで開明しt如くして切出した水
晶ウェハーから、第4図f示す水晶振動子エレメント2
5を、フォム11ングラフイ技術Vrより作る場合の工
程?説明する。
See Sections 111(a) to 81H(a),
Figures 6 and 71! ! A crystal resonator element 2 shown in FIG.
What is the process for making 5 using Foam 11 graphing technology Vr? explain.

まず、厚ざ100μ書程度の、肉面t##、面に研岸し
た水晶ウェハー511−用層し、この115mgタロ^
52お工び金55の1lljの薄膜金蒸着する(第8図
(a)) 、次IIr両面fフォトレジストを温布シ、
振か子形状のパターンの入ったフォトマスクを用いて、
マスク・丁ライナで投影II資する。クロムお工び金の
エツチングfIiを用いてエツチングすると、露’fぎ
わ大パターンを持つ金Jli 211111が仕上がる
(第8図(b)) 、この後、水晶管溶かすフッ酸系の
エツチング溌f浸凛すると、金栖2層膜(52,55)
が保瞼膜となり、水晶ウエーノ・は所望のシ状Vr払け
る(第8図(c))−この後、電極パターンも1wt様
のプロセスf工り形成しく第8図(A)> 、所望の水
晶振動子エレメントが出来上る。
First, a polished crystal wafer 511-layer with a thickness of about 100 μm was layered on the flesh side t##, and this 115 mg taro was used.
52 Deposit a 1llj thin film of gold on the fabrication plate 55 (Fig. 8(a)), then apply IIr double-sided photoresist with a hot cloth
Using a photomask with a pendulum-shaped pattern,
Projection II is carried out using a mask and liner. Etching with chrome metal etching fIi produces gold Jli 211111 with a large dew pattern (Fig. 8(b)).After this, a hydrofluoric acid etching bath is applied to dissolve the quartz tube. When it comes to Rin, Kanasu two-layer film (52, 55)
becomes the eyelid membrane, and the crystal wafer is removed in the desired shape (Fig. 8 (c)) - After this, the electrode pattern is also formed by the 1wt-like process (Fig. 8 (A)), as desired. A crystal oscillator element is completed.

この方法で作ると、*か子は数μmo精度で加工で壷、
しかも1枚のウエーノ・から百数十本の振動子が一時に
で亀るtめ1%件の揃ったものがで舞−る、この緒果、
棲めて小型であわ、温度変化に対する振か周期の塞化率
の大きい、特性の揃つr水晶振−子分大量vm造するこ
とができる。
When made using this method, *the pot can be processed with an accuracy of several microns,
What's more, more than 100 oscillators are produced from one Ueno disk at a time, and 1% of them are all dancing.
It is possible to manufacture a large quantity of r-quartz crystal pendulums with uniform characteristics such as being compact and easy to live in, and having a high blockage rate of the shaking cycle with respect to temperature changes.

この工うな構11iyJ’r!ると、温度センサである
水晶振動子がフォト+1ンクラフイ技術#r工り小#I
Kヤ防で龜るので、センサの熱容量が小ざ〈、従来のセ
ンー%7f比べて、過渡応答特性が著しく優れ。
This construction is 11iyJ'r! Then, the crystal oscillator, which is a temperature sensor, uses photo+1 technology.
Due to the heat resistance of the sensor, the heat capacity of the sensor is small, and the transient response characteristics are significantly superior compared to the conventional sensor.

従って検温所1時間の極めて蝮かい体温計を実現するこ
とができる。更f、音叉型水晶振動子?利甲することに
より、その発振8波数會低く設定することfにで*、従
って回路の消費電カケ着しく小型くすることがwW!で
あるから、電池動作が可能なのに勿論のこと、電池が小
型のもので済み、携帯性に優れた小型の体温計を構成す
ることかで−る。また、フォトリングラツメ技術VrL
り水晶振動子を製造するので、%性の揃ったセンサを得
ることかで一1七ンサの互換性に優れた電子式体温針管
提供することがwrtittlにる。
Therefore, it is possible to realize an extremely reliable thermometer that can be used for one hour at a temperature measuring station. Furthermore, a tuning fork type crystal oscillator? By increasing the number of waves, the oscillation frequency can be set lower*, and therefore the power consumption of the circuit can be reduced and the size can be reduced lol! Therefore, it is possible to construct a compact thermometer that can be operated with a battery, but requires only a small battery and is highly portable. In addition, photo ring latsume technology VrL
Since we manufacture crystal oscillators, we are able to provide electronic body temperature needles with excellent compatibility with 117 sensors by obtaining sensors with uniform % performance.

本発Q14ff工れげ、上述の如く、短かい検温時間で
済み、IIl定精度が憂い上ff、携帯性及びセンサの
互換OK優れ大電子式体温計を提供することかで負る。
As mentioned above, the Q14ff design of the present invention is to provide a large electronic thermometer that requires only a short temperature measurement time, has poor accuracy, and is excellent in portability and sensor compatibility.

表 図面の簡単taav4 第1図は本発明の電子式体温計の一実wA−のブロック
図、縞2図(&1及び第2図(b)に第1図中の各信号
の波形図、第S図灯第1図中に示゛すa1度センサ水晶
振動子の拡大断面−,第4図に第5関f示す水晶振動子
エレメントの拡大斜視図、館5図に幀4図のムーム紳断
面図、t1g6図に水晶振か子エレメントの切出し角r
rt#Il明するための説明図。
Table Simple drawings taav4 Figure 1 is a block diagram of an electronic thermometer wA- of the present invention, stripe diagram 2 (&1 and Figure 2 (b) are waveform diagrams of each signal in Figure 1, Figure 1 shows an enlarged cross-section of the a1 degree sensor crystal oscillator, Figure 4 shows an enlarged perspective view of the crystal oscillator element shown in Figure 5, and Figure 5 shows an enlarged cross-section of the crystal oscillator element shown in Figure 4. The cutting angle r of the crystal pendulum element is shown in Figure t1g6.
An explanatory diagram for explaining rt#Il.

艙7−は水a振動子エレメントの切出し角1σと蜘波数
変什率との間の関係を示す特性曲線図、嬉8図(a)乃
至第8図((1)flフォトリングラフィ技1[’rよ
る水晶振か子エレメントの製造工程を示す工程−である
Room 7- is a characteristic curve diagram showing the relationship between the cut-out angle 1σ of the water a oscillator element and the spider wave number variation rate, Figures 8 (a) to 8 ((1) fl photolithography technique 1 [This is a process showing the manufacturing process of a crystal pendulum element by 'r.

1・・・電子体温計 2・・・音51pm度センサ水晶振動子6・・・計数回
路 4・・・検出信褐発生回路 5・・・Iks水晶発振回路 6・・・水晶振動子 7・・・カウンタ 8・・・演算回路 9・・・表示回路 2s・・・音叉型屈曲水晶振動子エレメントPa・・・
検出パルスp3 D・・・計数データ K・・・温変データ 9土 出願人 株式会社 嬉二精工舎 第1図 悌2図(a) ′J1210(b) し     丁         T        
 T悌3図 算5S 第6(2)
1...Electronic thermometer 2...Sound 51pm degree sensor Crystal oscillator 6...Counting circuit 4...Detection signal brown generation circuit 5...Iks crystal oscillation circuit 6...Crystal oscillator 7...・Counter 8...Arithmetic circuit 9...Display circuit 2s...Tuning fork type bent crystal resonator element Pa...
Detection pulse p3 D...Counting data K...Temperature change data 9 Applicant: Keiji Seikosha Co., Ltd. Figure 1 Figure 2 (a) 'J1210 (b) Shi Ding T
T 悌 3 Illustrations 5S 6th (2)

Claims (1)

【特許請求の範囲】[Claims] 1、 フォトリングラフィ技術管用いて作っt温fil
ビに対する振動局期費化率の大きい音叉型温度量ンサ水
晶振動子と、該IIFセン賃水晶振書1子C)振#l1
ilaを#赦する周期測定回路とh該周期−5?回路f
よる渕?結果を温度に換算する演算回路と、WA演算回
路からの演算結果に従って11411flI!示する表
示器とt備えたこと1*徴とする電子体温計。
1. Temperature film made using photolithography technology tube
A tuning fork type temperature sensor crystal oscillator with a large vibration station rate for B, and the IIF sensor crystal oscillator 1 child C) oscillation #l1
A period measuring circuit that # forgives ila and h the period -5? circuit f
Yorubuchi? 11411flI! according to the calculation results from the calculation circuit that converts the result into temperature and the WA calculation circuit! An electronic thermometer that is equipped with a display that indicates 1*.
JP56210829A 1981-12-26 1981-12-26 Electronic clinical thermometer Pending JPS58113730A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56210829A JPS58113730A (en) 1981-12-26 1981-12-26 Electronic clinical thermometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56210829A JPS58113730A (en) 1981-12-26 1981-12-26 Electronic clinical thermometer

Publications (1)

Publication Number Publication Date
JPS58113730A true JPS58113730A (en) 1983-07-06

Family

ID=16595799

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56210829A Pending JPS58113730A (en) 1981-12-26 1981-12-26 Electronic clinical thermometer

Country Status (1)

Country Link
JP (1) JPS58113730A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60131433A (en) * 1983-12-20 1985-07-13 Yokogawa Hokushin Electric Corp Temperature sensor
JPH01210834A (en) * 1988-02-18 1989-08-24 Seiko Electronic Components Ltd Crystal thermal conductivity type vacuum gauge

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60131433A (en) * 1983-12-20 1985-07-13 Yokogawa Hokushin Electric Corp Temperature sensor
JPH0544612B2 (en) * 1983-12-20 1993-07-06 Yokogawa Electric Corp
JPH01210834A (en) * 1988-02-18 1989-08-24 Seiko Electronic Components Ltd Crystal thermal conductivity type vacuum gauge

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