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JPH0217068B2 - - Google Patents
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JPH0217068B2 - - Google Patents

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Publication number
JPH0217068B2
JPH0217068B2 JP58151914A JP15191483A JPH0217068B2 JP H0217068 B2 JPH0217068 B2 JP H0217068B2 JP 58151914 A JP58151914 A JP 58151914A JP 15191483 A JP15191483 A JP 15191483A JP H0217068 B2 JPH0217068 B2 JP H0217068B2
Authority
JP
Japan
Prior art keywords
resistor
temperature
cold junction
circuit
thermocouple
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 - Lifetime
Application number
JP58151914A
Other languages
Japanese (ja)
Other versions
JPS6042626A (en
Inventor
Tadashi Hashimoto
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP15191483A priority Critical patent/JPS6042626A/en
Publication of JPS6042626A publication Critical patent/JPS6042626A/en
Publication of JPH0217068B2 publication Critical patent/JPH0217068B2/ja
Granted 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
    • G01K7/02Measuring temperature based on the use of electric or magnetic elements directly sensitive to heat ; Power supply therefor, e.g. using thermoelectric elements using thermoelectric elements, e.g. thermocouples
    • G01K7/10Arrangements for compensating for auxiliary variables, e.g. length of lead
    • G01K7/12Arrangements with respect to the cold junction, e.g. preventing influence of temperature of surrounding air
    • G01K7/13Circuits for cold-junction compensation

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Temperature Or Quantity Of Heat (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔発明の技術分野〕 この発明は熱電対利用温度測定装置の冷接点補
償回路、即ち、熱電対の冷接点の温度に対応する
熱起電力に相当する信号を発生する冷接点補償回
路に関するものである。 熱電対の熱起電力は測温接点と冷接点との温度
差によつて生じる。つまり、熱電対の起電力を温
度に換算した場合には、測温接点と冷接点との間
の温度差が出て来る。処で、通常は、温度測定を
する場合には、測温接点と冷接点との温度差のみ
を検出だけでは足らず、測温接点の実際の温度を
検出する必要がある場合が殆んどであり、従つ
て、このように測温接点の実際の温度を測定する
ためには、冷接点の温度、即ち周囲温度に対応す
る熱起電力に相当する信号を求め、この信号と上
記温度差による起電力に加算し、この加算した信
号量から測温接点の実際の温度、つまり被測温部
の実際の温度を求める必要がある。即ち、被測温
部の実際の温度を測定するためには、上記のよう
な冷接点の温度に対応する熱起電力に相当する信
号を発生する所謂冷接点補償回路が必要なのであ
つて、この発明はこのような冷接点補償回路に関
するものである。 〔従来技術〕 従来のこの種冷接点補償回路を第1図により説
明する。第1図において、1及び2は何れも抵抗
値がR1の第1及び第2の抵抗、3は温度係数を
α、温度をtとした場合の抵抗値がR0(1+α・
t)で表わされる測温抵抗で、熱電対の冷接点部
(図示せず)の温度を検出するものである。4は
抵抗値がR0の第3の抵抗、5は演算増幅器で、
反転入力端子5aと非反転入力端子5bとを有し
ている。6は電圧値がErの基準電圧電源で、直流
電源である。7は直流の出力電圧EOAを出力する
出力端子、8は上記第1〜第3の抵抗1,2,4
と測温抵抗3と演算増幅器5とにより構成された
ブリツジ回路で上記基準電圧源6から基準電圧Er
が供給されている。8a,8bはこのブリツジ回
路8の電圧比較端子部である。 次に、この第1図の回路の動作を説明する。 測温抵抗3はその温度が0℃の時には抵抗値が
R0となるので、ブリツジ回路8は平衡状態とな
る。従つて、その電圧比較端子部8a,8b間の
電位差は0であり、出力端子7の出力電圧も0で
ある。次に、測温抵抗3はその温度が0℃から上
昇あるいは下降すると、抵抗値が変化する。即ち
ブリツジ回路8の一枝路の抵抗値が変化する。従
つて、ブリツジ回路8は不平衡状態となつて、測
温抵抗3の抵抗値の変化に比例して電圧比較端子
8a,8b間に電位差が生じ、この電位差に応じ
て演算増幅器5から電圧信号EOAが出力される。
この出力電圧EOAは次のように表わされる。即ち、 EOA=Er・R0/R1+R0・α・t ……(1) =A・t(但し、A=Er・R0/R1+R0・α) ……(2) となり、この(2)式で表わされるように、温度に対
して直線的に変化する。 次いで、この第1図の回路における冷接点補償
誤差について言及する。下記の第1にはJ(IC)
熱電対の規準熱起電力を、JISC1602により示し、
表2には、表1の熱電対の規準熱起電力に相当す
る電圧値を、第1図の回路のA=0.0517として出
力する値を示す。こゝで、第1図の回路の場合に
おいて、J(IC)の熱電対につき、例えば−10゜〜
100℃に亘る広い温度範囲で冷接点の補償誤差を
求めてみると、冷接点の補償誤差は100℃で最大
−0.098mVの誤差を生じており、これを温度換
算すると約1.8℃の誤差を生じることになる。つ
まり、この第1図の回路は冷接点補償を極く一般
的な23℃±20degのような狭い温度範囲で行なう
場合には補償誤差は小さいが、例えば、車載用温
度計等にその温度センサとして熱電対を使用する
場合には、車の広範な利用形態から、冷接点部が
広い温度範囲に亘つて周囲温度の影響を受けるの
で、補償誤差が増大し、高精度な温度測定をする
ことができないという欠点があつた。
[Technical Field of the Invention] The present invention relates to a cold junction compensation circuit for a temperature measuring device using a thermocouple, that is, a cold junction compensation circuit that generates a signal corresponding to a thermoelectromotive force corresponding to the temperature of a cold junction of a thermocouple. be. The thermoelectromotive force of a thermocouple is generated by the temperature difference between the hot junction and the cold junction. That is, when the electromotive force of the thermocouple is converted into temperature, the temperature difference between the temperature measuring junction and the cold junction appears. However, when measuring temperature, it is usually not enough to detect only the temperature difference between the temperature-measuring junction and the cold junction; in most cases, it is necessary to detect the actual temperature of the temperature-measuring junction. Therefore, in order to measure the actual temperature of the temperature measuring junction in this way, a signal corresponding to the thermoelectromotive force corresponding to the temperature of the cold junction, that is, the ambient temperature, is obtained, and this signal and the signal corresponding to the above temperature difference are calculated. It is necessary to add it to the electromotive force and find the actual temperature of the temperature measuring contact, that is, the actual temperature of the temperature measured part, from this added signal amount. That is, in order to measure the actual temperature of the temperature-measured part, a so-called cold junction compensation circuit is required, which generates a signal corresponding to the thermoelectromotive force corresponding to the temperature of the cold junction as described above. The invention relates to such a cold junction compensation circuit. [Prior Art] A conventional cold junction compensation circuit of this type will be explained with reference to FIG. In FIG. 1, 1 and 2 are the first and second resistors whose resistance value is R 1 , and 3 is the resistance value where α is the temperature coefficient and t is the temperature.
t) is used to detect the temperature of a cold junction (not shown) of a thermocouple. 4 is a third resistor with a resistance value of R 0 , 5 is an operational amplifier,
It has an inverting input terminal 5a and a non-inverting input terminal 5b. 6 is a reference voltage power supply with a voltage value of E r , which is a DC power supply. 7 is an output terminal that outputs the DC output voltage EOA , and 8 is the first to third resistor 1, 2, 4.
A bridge circuit composed of a temperature measuring resistor 3 and an operational amplifier 5 generates a reference voltage E r from the reference voltage source 6.
is supplied. Reference numerals 8a and 8b are voltage comparison terminals of this bridge circuit 8. Next, the operation of the circuit shown in FIG. 1 will be explained. When the temperature of resistance thermometer 3 is 0℃, the resistance value is
Since R0 , the bridge circuit 8 is in an equilibrium state. Therefore, the potential difference between the voltage comparison terminal portions 8a and 8b is 0, and the output voltage of the output terminal 7 is also 0. Next, when the temperature of the temperature measuring resistor 3 rises or falls from 0° C., the resistance value changes. That is, the resistance value of one branch of the bridge circuit 8 changes. Therefore, the bridge circuit 8 is in an unbalanced state, and a potential difference occurs between the voltage comparison terminals 8a and 8b in proportion to the change in the resistance value of the temperature measuring resistor 3, and a voltage signal is output from the operational amplifier 5 in accordance with this potential difference. E OA is output.
This output voltage E OA is expressed as follows. That is, E OA =E r・R 0 /R 1 +R 0・α・t ……(1) =A・t (However, A=E r・R 0 /R 1 +R 0・α) ……(2 ), and as expressed by equation (2), it changes linearly with temperature. Next, the cold junction compensation error in the circuit shown in FIG. 1 will be discussed. The first one below is J (IC)
The standard thermoelectromotive force of thermocouples is shown by JISC1602,
Table 2 shows the voltage value corresponding to the standard thermoelectromotive force of the thermocouple in Table 1, which is output as A=0.0517 in the circuit of FIG. Here, in the case of the circuit shown in Figure 1, for example, -10° to
When calculating the compensation error of the cold junction over a wide temperature range of 100℃, the compensation error of the cold junction causes a maximum error of -0.098mV at 100℃, and when converted to temperature, this is an error of approximately 1.8℃. will occur. In other words, the circuit shown in Figure 1 has a small compensation error when performing cold junction compensation in a narrow temperature range such as the extremely common 23℃±20deg, but When using a thermocouple as a thermocouple, due to the wide range of vehicles used, the cold junction is affected by the ambient temperature over a wide temperature range, which increases compensation errors and makes it difficult to measure temperature with high precision. The drawback was that it was not possible.

【表】【table】

〔発明の概要〕[Summary of the invention]

この発明は、上記のような従来の回路の欠点を
解消し、周囲温度の影響による検出誤差を抑制す
ることを目的としてなされたもので、熱電対の熱
起電力が温度に対して双曲線的に変化することに
着眼し、ブリツジ回路の出力を補償抵抗を介して
ブリツジ回路にフイードバツクするフイードバツ
ク回路を設けることにより、熱電対の冷接点の温
度に対応する熱起電力に近似した信号を発生して
冷接点補償を行なう熱電対利用温度測定装置の冷
接点補償回路を提供するものである。 〔発明の実施例〕 第2図はこの発明の一実施例を示す接続図で、
同図において、符号1,2,3,4,5,5a,
5b,6,7,8,8a,8bは第1図に示す従
来の回路と同様に、1及び2は何れも抵抗値が
R1の第1及び第2の抵抗、3は温度係数をα、
温度をtとした場合の抵抗値がR0(1+α・t)
で表わされる測温抵抗で、熱電対の冷接点部(図
示せず)の温度を検出するものである。4は抵抗
値がR0の第3の抵抗、5は演算増幅器で、反転
入力端子5aと非反転入力端子5bとを有してい
る。6は電圧値がErの基準電圧電源で、直流電源
である。7は直流の出力電圧EOBを出力する出力
端子、8は上記第1〜第3の抵抗1,2,4と測
温抵抗3と演算増幅器5とにより構成されたブリ
ツジ回路で、上記基準電圧源6から基準電圧Er
供給されている。8a,8bはこのブリツジ回路
8の電圧比較端子部、9は抵抗値が(n−1)
R2の補償抵抗、10は抵抗値がR2の補償抵抗、
11は上記両補償抵抗9,10の接続点即ち分圧
点、12は加算回路で、反転増幅の機能も有して
いる。13は上記演算増幅器5の出力EOBをブリ
ツジ回路8にフイードバツクするフイードバツク
回路で、上記補償抵抗9,10及び加算回路12
で構成されている。上記ブリツジ回路8の出力電
圧EOBは、補償抵抗9,10により分圧され、更
にこの分圧されたブリツジ回路8の出力電圧EOB
の一部即ち、分圧点11の電圧と基準電圧源6の
電圧Erとを加算回路12が加算すると共に極性を
反転して出力し、この加算回路12の出力が、上
記ブリツジ回路8への供給電圧となるように構成
されている。 次に第2図の動作を説明する。この第2図の回
路において、ブリツジ回路8の一枝路にある測温
抵抗3の抵抗値はその温度が0℃のときR0とな
り、ブリツジ回路8は平衡状態となり、電圧比較
端子部8a,8b間の電位差は0であり、従つて
出力端子7の出力電圧も0〔V〕となつているが、
測温抵抗3はその温度が上昇あるいは下降するこ
とにより抵抗値が、上昇あるいは下降し、ブリツ
ジ回路8が不平衡状態となる。こゝで、上記平衡
状態となれば、上記測温抵抗3の抵抗値の変化に
応じて出力端子7に出力電圧EOBが発生するので
あるが、この出力EOBの一部がブリツジ回路8の
基準電圧源6の電圧Erに加算回路12により加算
されると、等価的に基準電圧源6の電圧は、温度
変化に比例して高められることとなり、ブリツジ
回路8の出力EOBは、温度に対して双曲線カーブ
となるように変化する。 こゝで第2図の出力EOBを求めてみると、 EOB=Er・R0/R1+R0・α・t/1−R0・α/n(R1
+R0)・t……(3) =B・t/1−C・t ……(4) (但し、B=Er・R0/R1+R0・α、C= R0・α/n(R1+R0)) となる。(4)式で示すように、ブリツジ回路8の出
力EOBは双曲線カーブで表わされ、(4)式において、
BとCとを適当な値に選択すれば、熱電対(図示
せず)の熱起電力の温度特性と近似することがで
きる。 上記J(IC)熱電対の場合について、例えば上
記(4)式におけるBとCとを、 B=5.0756×10-2、C=3.6526×10-4 となるように設定し、上記第2図の実施例の場合
の出力EOBを求めてみると、下記の表3のように
表わされる。この場合の最大誤差は−10℃におい
て−0.005〔mV〕となつており、これを温度に換
算すると約0.1℃となり、第1図に示す従来の回
路の最大誤差即ち1.8℃と比較すると、約18倍も
の改善がみられる。
This invention was made with the aim of eliminating the above-mentioned drawbacks of conventional circuits and suppressing detection errors caused by the influence of ambient temperature. By focusing on the change in temperature and providing a feedback circuit that feeds back the output of the bridge circuit to the bridge circuit via a compensation resistor, we can generate a signal that approximates the thermoelectromotive force corresponding to the temperature of the cold junction of the thermocouple. The present invention provides a cold junction compensation circuit for a thermocouple-based temperature measurement device that performs cold junction compensation. [Embodiment of the invention] Figure 2 is a connection diagram showing an embodiment of the invention.
In the figure, symbols 1, 2, 3, 4, 5, 5a,
5b, 6, 7, 8, 8a, and 8b are similar to the conventional circuit shown in Fig. 1, and 1 and 2 have resistance values.
The first and second resistance of R 1 , 3 is the temperature coefficient α,
The resistance value when temperature is t is R 0 (1+α・t)
This is a temperature measuring resistor expressed as , which detects the temperature of a cold junction part (not shown) of a thermocouple. 4 is a third resistor having a resistance value R 0 , and 5 is an operational amplifier, which has an inverting input terminal 5 a and a non-inverting input terminal 5 b. 6 is a reference voltage power supply with a voltage value of E r , which is a DC power supply. 7 is an output terminal for outputting the DC output voltage E OB ; 8 is a bridge circuit composed of the first to third resistors 1, 2, 4, a temperature measuring resistor 3, and an operational amplifier 5; A reference voltage E r is supplied from a source 6 . 8a and 8b are voltage comparison terminals of this bridge circuit 8, and 9 is a resistance value (n-1).
Compensation resistor with R 2 , 10 is compensation resistor with resistance value R 2 ,
Reference numeral 11 denotes a connection point between the compensation resistors 9 and 10, that is, a voltage dividing point. Reference numeral 12 denotes an adder circuit, which also has an inverting amplification function. 13 is a feedback circuit that feeds back the output EOB of the operational amplifier 5 to the bridge circuit 8;
It consists of The output voltage E OB of the bridge circuit 8 is divided by compensation resistors 9 and 10, and the output voltage E OB of the bridge circuit 8 is further divided by the compensation resistors 9 and 10.
That is, the voltage at the voltage dividing point 11 and the voltage E r of the reference voltage source 6 are added together by an adder circuit 12 and outputted with the polarity inverted, and the output of this adder circuit 12 is sent to the bridge circuit 8. The supply voltage is Next, the operation shown in FIG. 2 will be explained. In the circuit shown in FIG. 2, the resistance value of the temperature measuring resistor 3 in one branch of the bridge circuit 8 becomes R 0 when its temperature is 0°C, the bridge circuit 8 is in an equilibrium state, and the voltage comparison terminals 8a, 8b The potential difference between them is 0, and therefore the output voltage at the output terminal 7 is also 0 [V].
As the temperature of the temperature measuring resistor 3 increases or decreases, the resistance value increases or decreases, and the bridge circuit 8 becomes unbalanced. Now, when the above-mentioned equilibrium state is reached, an output voltage E OB is generated at the output terminal 7 according to the change in the resistance value of the temperature-detecting resistor 3, and a part of this output E OB is connected to the bridge circuit 8. When added to the voltage E r of the reference voltage source 6 by the addition circuit 12, the voltage of the reference voltage source 6 is equivalently increased in proportion to the temperature change, and the output E OB of the bridge circuit 8 is: It changes in a hyperbolic curve with respect to temperature. Now, when we calculate the output E OB in Figure 2, E OB = E r・R 0 /R 1 +R 0・α・t/1−R 0・α/n(R 1
+R 0 )・t……(3) =B・t/1−C・t……(4) (However, B=E r・R 0 /R 1 +R 0・α, C= R 0・α/ n(R 1 +R 0 )). As shown in equation (4), the output E OB of the bridge circuit 8 is expressed by a hyperbolic curve, and in equation (4),
By selecting appropriate values for B and C, it is possible to approximate the temperature characteristics of the thermoelectromotive force of a thermocouple (not shown). In the case of the above J (IC) thermocouple, for example, set B and C in the above equation (4) so that B = 5.0756 × 10 -2 and C = 3.6526 × 10 -4 , and as shown in Fig. 2 above. When the output E OB in the case of the embodiment is determined, it is expressed as shown in Table 3 below. The maximum error in this case is -0.005 [mV] at -10°C, which is approximately 0.1°C when converted to temperature, which is approximately 1.8°C when compared with the maximum error of the conventional circuit shown in Figure 1. This is an 18 times improvement.

〔発明の効果〕〔Effect of the invention〕

この発明は上述のように、一枝路に測温抵抗を
有したブリツジ回路と、このブリツジ回路に基準
電圧を与える基準電圧源とを有した熱電対利用温
度測定装置の冷接点補償回路において、上記ブリ
ツジ回路の出力を補償抵抗を介して上記ブリツジ
回路にフイードバツクするフイードバツク回路を
設けたので、従来の冷接点補償回路に比べて、補
償誤差を十分小さくでき、また広い温度範囲に亘
つて冷接点補償ができる効果がある。
As described above, the present invention provides a cold junction compensation circuit for a thermocouple-based temperature measuring device, which has a bridge circuit having a temperature measuring resistor in one branch, and a reference voltage source that supplies a reference voltage to the bridge circuit. Since a feedback circuit is provided that feeds back the output of the bridge circuit to the bridge circuit through the compensation resistor, the compensation error can be sufficiently reduced compared to the conventional cold junction compensation circuit, and the cold junction compensation can be performed over a wide temperature range. It has the effect of

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

第1図は従来の熱電対利用温度測定装置の冷接
点補償回路を示す接続図、第2図はこの発明によ
る熱電対利用温度測定装置の冷接点補償回路の一
実施例を示す接続図、第3図はこの発明の他の実
施例を示す接続図である。 図において、1は第1の抵抗、2は第2の抵
抗、3は測温抵抗、4は第3の抵抗、5は演算増
幅器、5aは反転入力端子、5bは非反転入力端
子、6は基準電圧源、7は出力端子、8はブリツ
ジ回路、8a,8bは電圧比較端子である。な
お、各図中同一符号は同一または相当部分を示
す。
FIG. 1 is a connection diagram showing a cold junction compensation circuit of a conventional temperature measurement device using a thermocouple, and FIG. 2 is a connection diagram showing an embodiment of the cold junction compensation circuit of a temperature measurement device using a thermocouple according to the present invention. FIG. 3 is a connection diagram showing another embodiment of the present invention. In the figure, 1 is the first resistor, 2 is the second resistor, 3 is the temperature measuring resistor, 4 is the third resistor, 5 is the operational amplifier, 5a is the inverting input terminal, 5b is the non-inverting input terminal, and 6 is the non-inverting input terminal. Reference voltage source, 7 is an output terminal, 8 is a bridge circuit, and 8a, 8b are voltage comparison terminals. Note that the same reference numerals in each figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】 1 抵抗値が同一でR1の第1、第2の抵抗と、
抵抗値がR0の第3の抵抗と、抵抗値がR0(1+
αt)(αは温度係数、tは温度)の熱電対冷接点
温度検出用の測温抵抗と、演算増幅器とでブリツ
ジ回路を構成し、このブリツジ回路に基準電圧を
与える基準電圧源の一端に上記第1の抵抗と第2
の抵抗の接続点を、上記演算増幅器の反転入力端
子に上記第1の抵抗と測温抵抗の接続点を、この
演算増幅器の非反転入力端子に上記第2の抵抗と
第3の抵抗の接続点を、上記基準電圧源の他端に
上記第2の抵抗の他端を、上記演算増幅器の出力
端子に上記第3の抵抗の他端をそれぞれ接続し、
この演算増幅器の出力端子から熱電対の冷接点温
度に対応する電圧信号を取出すようにした熱電対
利用温度測定装置の冷接点補償回路において、上
記演算増幅器の出力電圧を補償抵抗を介して上記
演算増幅器の入力側にフイードバツクするフイー
ドバツク回路を設けたことを特徴とする熱電対利
用温度測定装置の冷接点補償回路。 2 フイードバツク回路は基準電圧と演算増幅器
の分圧出力電圧とを加算する加算回路を有し、上
記演算増幅器は上記加算回路の出力と熱電対の冷
接点の温度に比例する電圧との積に相当する電圧
を出力するものであることを特徴とする特許請求
の範囲第1項に記載の熱電対利用温度測定装置の
冷接点補償回路。 3 フイードバツク回路は演算増幅器の出力端子
と非反転入力端子との間に補償抵抗を有したもの
であることを特徴とする特許請求の範囲第1項に
記載の熱電対利用温度測定装置の冷接点補償回
路。
[Claims] 1. First and second resistors having the same resistance value and R 1 ;
A third resistor with a resistance value R 0 and a third resistor with a resistance value R 0 (1+
αt) (α is the temperature coefficient, t is the temperature) A temperature measuring resistor for detecting the thermocouple cold junction temperature and an operational amplifier constitute a bridge circuit, and one end of the reference voltage source that provides a reference voltage to this bridge circuit The first resistor and the second resistor
A connection point between the first resistor and the temperature measuring resistor is connected to the inverting input terminal of the operational amplifier, and a connection point between the second resistor and the third resistor is connected to the non-inverting input terminal of the operational amplifier. a point, the other end of the second resistor is connected to the other end of the reference voltage source, and the other end of the third resistor is connected to the output terminal of the operational amplifier,
In the cold junction compensation circuit of the thermocouple-using temperature measuring device, which extracts a voltage signal corresponding to the cold junction temperature of the thermocouple from the output terminal of the operational amplifier, the output voltage of the operational amplifier is calculated by the above-mentioned calculation via the compensation resistor. A cold junction compensation circuit for a thermocouple-based temperature measuring device, characterized in that a feedback circuit for providing feedback is provided on the input side of an amplifier. 2. The feedback circuit has an addition circuit that adds the reference voltage and the divided output voltage of the operational amplifier, and the operational amplifier has a voltage corresponding to the product of the output of the addition circuit and the voltage proportional to the temperature of the cold junction of the thermocouple. 2. A cold junction compensation circuit for a thermocouple-based temperature measurement device according to claim 1, wherein the cold junction compensation circuit outputs a voltage that 3. The cold junction of the thermocouple temperature measuring device according to claim 1, wherein the feedback circuit has a compensation resistor between the output terminal of the operational amplifier and the non-inverting input terminal. Compensation circuit.
JP15191483A 1983-08-19 1983-08-19 Cold junction compensating circuit of temperature measuring device utilizing thermocouple Granted JPS6042626A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15191483A JPS6042626A (en) 1983-08-19 1983-08-19 Cold junction compensating circuit of temperature measuring device utilizing thermocouple

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15191483A JPS6042626A (en) 1983-08-19 1983-08-19 Cold junction compensating circuit of temperature measuring device utilizing thermocouple

Publications (2)

Publication Number Publication Date
JPS6042626A JPS6042626A (en) 1985-03-06
JPH0217068B2 true JPH0217068B2 (en) 1990-04-19

Family

ID=15528952

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15191483A Granted JPS6042626A (en) 1983-08-19 1983-08-19 Cold junction compensating circuit of temperature measuring device utilizing thermocouple

Country Status (1)

Country Link
JP (1) JPS6042626A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5171935B2 (en) 2008-03-07 2013-03-27 山洋電気株式会社 Optical encoder device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS601429Y2 (en) * 1977-11-18 1985-01-16 横河電機株式会社 Reference temperature conversion type temperature compensation circuit
JPS5720484A (en) * 1980-07-11 1982-02-02 Yamatake Honeywell Co Ltd Cold junction compensating circuit for thermocouple

Also Published As

Publication number Publication date
JPS6042626A (en) 1985-03-06

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