JPH0127070Y2 - - Google Patents

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Publication number
JPH0127070Y2
JPH0127070Y2 JP17856583U JP17856583U JPH0127070Y2 JP H0127070 Y2 JPH0127070 Y2 JP H0127070Y2 JP 17856583 U JP17856583 U JP 17856583U JP 17856583 U JP17856583 U JP 17856583U JP H0127070 Y2 JPH0127070 Y2 JP H0127070Y2
Authority
JP
Japan
Prior art keywords
resistor
temperature sensor
temperature
operational amplifier
input terminal
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.)
Expired
Application number
JP17856583U
Other languages
Japanese (ja)
Other versions
JPS6086934U (en
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 filed Critical
Priority to JP17856583U priority Critical patent/JPS6086934U/en
Publication of JPS6086934U publication Critical patent/JPS6086934U/en
Application granted granted Critical
Publication of JPH0127070Y2 publication Critical patent/JPH0127070Y2/ja
Granted legal-status Critical Current

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  • Measuring Temperature Or Quantity Of Heat (AREA)
  • Measurement Of Resistance Or Impedance (AREA)

Description

【考案の詳細な説明】 (a) 考案の技術分野 本考案はニツケル又は白金等を用いた抵抗体温
度センサーを使用し、該抵抗体温度センサーと温
度測定器間の線路抵抗値を無視出来るようにした
温度計測回路に係り、使用部品を少なくし測定精
度を容易に上げることが出来る温度計測回路に関
する。
[Detailed description of the invention] (a) Technical field of the invention This invention uses a resistor temperature sensor made of nickel or platinum, etc., so that the line resistance between the resistor temperature sensor and the temperature measuring device can be ignored. The present invention relates to a temperature measurement circuit that can reduce the number of parts used and easily improve measurement accuracy.

(b) 従来技術と問題点 第1図は従来例の温度計測回路のブロツク図で
ある。
(b) Prior art and problems Figure 1 is a block diagram of a conventional temperature measuring circuit.

図中1はニツケル又は白金等を用いた抵抗体温
度センサー、2は変換回路、10は温度測定器、
Ra,Rbは抵抗、rは線路抵抗、Eは電圧Eの電
源、Vは電圧計を示す。
In the figure, 1 is a resistor temperature sensor using nickel or platinum, 2 is a conversion circuit, 10 is a temperature measuring device,
Ra and Rb are resistances, r is line resistance, E is a power source of voltage E, and V is a voltmeter.

ニツケル又は白金等を用い温度変化が抵抗値変
化に対応する抵抗温度センサー1を用い温度を計
測する温度計測回路では、抵抗体温度センサー1
と温度測定器10間の線路抵抗rを無視する為
に、第1図に示す如く抵抗体温度センサー1と温
度測定器10間を3線にて結び、ブリツジ回路を
用い、抵抗体温度センサー1の抵抗値Rx(例えば
温度0℃の時の抵抗値である基準抵抗値Rと温度
変化により変化する抵抗ΔRとの和)を、電圧計
Vの電圧値及びこの電圧値を抵抗体温度センサー
1の抵抗値Rxに変換する変換回路2により求め
温度を計測する方法は良く知られている。
In a temperature measurement circuit that measures temperature using a resistance temperature sensor 1 made of nickel, platinum, etc., and whose temperature change corresponds to a resistance value change, a resistance temperature sensor 1 is used.
In order to ignore the line resistance r between the resistor temperature sensor 1 and the temperature measuring device 10, three wires are used to connect the resistor temperature sensor 1 and the temperature measuring device 10 as shown in FIG. The resistance value R A method of measuring temperature by using a conversion circuit 2 that converts it into a resistance value R x of 1 is well known.

しかしこの場合測定した電圧値より抵抗体温度
センサ1の抵抗値Rxを求める式は複雑であり、
従つて変換回路2の構成も複雑で使用する部品点
数も多く部品個々の誤差が加わり測定精度向上が
困難な欠点がある。
However, in this case, the formula for calculating the resistance value R x of the resistor temperature sensor 1 from the measured voltage value is complicated,
Therefore, the configuration of the conversion circuit 2 is complicated and the number of parts used is large, and errors of individual parts are added, making it difficult to improve measurement accuracy.

(c) 考案の目的 本考案の目的は上記の欠点に鑑み、出力電圧値
と抵抗体温度センサーの抵抗値との変換回路を不
要にして、使用部品を少なく出来測定精度を容易
に向上出来る温度計測回路の提供にある。
(c) Purpose of the invention In view of the above drawbacks, the purpose of the invention is to eliminate the need for a conversion circuit between the output voltage value and the resistance value of the resistor temperature sensor, reduce the number of parts used, and easily improve temperature measurement accuracy. The aim is to provide measurement circuits.

(d) 考案の構成 本考案は上記の目的を達成するために、抵抗体
温度センサーの一方の端子を、負入力端子と出力
端子間を第1の抵抗で接続した第1の演算増巾器
の正入力端子に接続し、該抵抗温度センサーの他
方の端子を出力電圧の1/4の電圧を負入力端子に
入力する第2の演算増巾器の正入力端子に接続す
ると共に該抵抗体温度センサーの基準抵抗値に等
しい値の抵抗を介してアースに接続し、又該第1
の演算増巾器の正入力端子とアース間には定電流
を流すようにし、又該第2の演算増巾器の出力端
子と該第1の演算増巾器の負入力端子を該第1の
抵抗の値と等しい値の抵抗を介して接続し、該抵
抗体温度センサーの温度変化により変化する抵抗
値を該第1の演算増巾器の出力電圧に比例するよ
うにしたことを特徴とする。
(d) Structure of the invention In order to achieve the above object, the invention provides a first operational amplifier in which one terminal of a resistor temperature sensor is connected between a negative input terminal and an output terminal through a first resistor. and the other terminal of the resistance temperature sensor is connected to the positive input terminal of a second operational amplifier which inputs a voltage of 1/4 of the output voltage to the negative input terminal of the resistor. Connected to ground through a resistor with a value equal to the reference resistance value of the temperature sensor, and
A constant current is caused to flow between the positive input terminal of the second operational amplifier and the ground, and the output terminal of the second operational amplifier is connected to the negative input terminal of the first operational amplifier. The resistor temperature sensor is connected through a resistor having a value equal to the value of the resistor, so that the resistance value that changes due to a temperature change of the resistor temperature sensor is proportional to the output voltage of the first operational amplifier. do.

(e) 考案の実施例 以下本考案の一実施例につき図に従つて説明す
る。
(e) Embodiment of the invention An embodiment of the invention will be described below with reference to the drawings.

第2図は本考案の実施例の温度計測回路のブロ
ツク図である。
FIG. 2 is a block diagram of a temperature measuring circuit according to an embodiment of the present invention.

図中第1図と同一機能のものは同一記号で示
し、3〜7は抵抗で3,4,6の抵抗値はR1
5の抵抗値は3R1,7の抵抗値は抵抗体温度セ
ンサーの例えば温度0℃における抵抗値である基
準抵抗値Rと同じである。8,9は演算増巾器、
10′は温度測定器、11は定電流回路で、電流
Iを流し又抵抗体温度センサー1の抵抗値Rx
基準抵抗値Rと温度変化により変化する抵抗ΔR
との和である。
In the figure, the same functions as in Figure 1 are indicated by the same symbols, 3 to 7 are resistors, and the resistance values 3, 4, and 6 are R 1 ,
The resistance value of No. 5 is 3R 1 , and the resistance value of No. 7 is the same as the reference resistance value R, which is the resistance value of the resistor temperature sensor at a temperature of 0° C., for example. 8 and 9 are operational amplifiers,
10' is a temperature measuring device, 11 is a constant current circuit through which a current I is passed, and the resistance value R x of the resistor temperature sensor 1 is a resistance ΔR that changes with the reference resistance value R and temperature changes.
It is the sum of

定電流回路11より電流Iを流すと、演算増巾
器8,9の入力インピーダンスは高いので、電流
Iは抵抗r→抵抗体温度センサー1→抵抗r→7
(抵抗値R)を経てアースに流れる。この場合イ
点の電圧をV1、ロ点の電圧をV2とすれば、抵抗
体温度センサー1の温度により変化する抵抗値
ΔRは次式(1)の如くなる。
When a current I is passed from the constant current circuit 11, the input impedance of the operational amplifiers 8 and 9 is high, so the current I flows from the resistor r → resistor temperature sensor 1 → resistor r → 7
(resistance value R) and flows to ground. In this case, if the voltage at point A is V 1 and the voltage at point B is V 2 , then the resistance value ΔR that changes depending on the temperature of the resistor temperature sensor 1 is expressed by the following equation (1).

ΔR=V1−2V2/I ……(1) 又ハ点の電圧は4V2となり二点の電圧はV1とな
る。従つて演算増巾器9の出力電圧V0は次式の
如くなる。
ΔR=V 1 −2V 2 /I (1) Also, the voltage at point C becomes 4V 2 and the voltage at two points becomes V 1 . Therefore, the output voltage V 0 of the operational amplifier 9 is as shown in the following equation.

V0=2(V1−2V2) ……(2) よつて、温度変化する抵抗値ΔRは次式(3)で表
はされる。
V 0 =2(V 1 -2V 2 )...(2) Therefore, the resistance value ΔR that changes with temperature is expressed by the following equation (3).

ΔR=2V0/I ……(3) (3)式を見れば判る如く、温度により変化する抵
抗値ΔRは出力電圧V0に比例した値として求めら
れ、温度は出力電圧V0で、変換回路を用いるこ
となく求めることが出来る。従つて温度計側回路
は第2図に示すものでよく、第1図に示す従来の
温度計測回路に比し使用部品を少なく出来測定精
度を容易に向上出来る。
ΔR=2V 0 /I...(3) As you can see from equation (3), the resistance value ΔR, which changes with temperature, is found as a value proportional to the output voltage V 0 , and the temperature is the output voltage V 0 , and the conversion It can be obtained without using a circuit. Therefore, the thermometer side circuit may be the one shown in FIG. 2, and compared to the conventional temperature measurement circuit shown in FIG. 1, fewer parts can be used and measurement accuracy can be easily improved.

(f) 考案の効果 以上詳細に説明せる如く本考案によれば、抵抗
体温度センサーの温度により変化する抵抗値を出
力電圧に比例して求めることが出来るので、温度
計測回路の使用部品を少なく出来測定精度を容易
に向上出来る効果がある。
(f) Effect of the invention As explained in detail above, according to the invention, the resistance value that changes depending on the temperature of the resistor temperature sensor can be determined in proportion to the output voltage, so the number of parts used in the temperature measurement circuit can be reduced. This has the effect of easily improving performance measurement accuracy.

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

第1図は従来例の温度計測回路のブロツク図、
第2図は本発明の実施例の温度計測回路のブロツ
ク図である。 図中1は抵抗体温度センサー、2は変換回路、
3〜7,Ra,Rbは抵抗、rは線路抵抗、Eは電
源、Vは電圧計、8,9は演算増巾器、10,1
0′は温度測定器、11は定電流回路を示す。
Figure 1 is a block diagram of a conventional temperature measurement circuit.
FIG. 2 is a block diagram of a temperature measuring circuit according to an embodiment of the present invention. In the figure, 1 is a resistor temperature sensor, 2 is a conversion circuit,
3 to 7, Ra and Rb are resistances, r is line resistance, E is power supply, V is voltmeter, 8 and 9 are operational amplifiers, 10, 1
0' indicates a temperature measuring device, and 11 indicates a constant current circuit.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 抵抗体温度センサーの一方の端子を、負入力端
子と出力端子間を第1の抵抗で接続した第1の演
算増巾器の正入力端子に接続し、該抵抗温度セン
サーの他方の端子を出力電圧の1/4の電圧を負入
力端子に入力する第2の演算増巾器の正入力端子
に接続すると共に該抵抗体温度センサーの基準抵
抗値に等しい値の抵抗を介してアースに接続し、
又該第1の演算増巾器の正入力端子とアース間に
は定電流を流すようにし、又該第2の演算増巾器
の出力端子と該第1の演算増巾器の負入力端子を
該第1の抵抗の値と等しい値の抵抗を介して接続
したことを特徴とする温度計測回路。
One terminal of the resistor temperature sensor is connected to the positive input terminal of a first operational amplifier having a first resistor connected between the negative input terminal and the output terminal, and the other terminal of the resistor temperature sensor is output. Connect it to the positive input terminal of a second operational amplifier that inputs 1/4 of the voltage to the negative input terminal, and connect it to ground via a resistor with a value equal to the reference resistance value of the resistor temperature sensor. ,
Further, a constant current is caused to flow between the positive input terminal of the first operational amplifier and the ground, and a constant current is caused to flow between the output terminal of the second operational amplifier and the negative input terminal of the first operational amplifier. A temperature measurement circuit characterized in that the temperature measurement circuit is connected through a resistor having a value equal to the value of the first resistor.
JP17856583U 1983-11-18 1983-11-18 temperature measurement circuit Granted JPS6086934U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17856583U JPS6086934U (en) 1983-11-18 1983-11-18 temperature measurement circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17856583U JPS6086934U (en) 1983-11-18 1983-11-18 temperature measurement circuit

Publications (2)

Publication Number Publication Date
JPS6086934U JPS6086934U (en) 1985-06-14
JPH0127070Y2 true JPH0127070Y2 (en) 1989-08-14

Family

ID=30387649

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17856583U Granted JPS6086934U (en) 1983-11-18 1983-11-18 temperature measurement circuit

Country Status (1)

Country Link
JP (1) JPS6086934U (en)

Also Published As

Publication number Publication date
JPS6086934U (en) 1985-06-14

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