JPS594263Y2 - Temperature difference measuring device - Google Patents

Temperature difference measuring device

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Publication number
JPS594263Y2
JPS594263Y2 JP8515278U JP8515278U JPS594263Y2 JP S594263 Y2 JPS594263 Y2 JP S594263Y2 JP 8515278 U JP8515278 U JP 8515278U JP 8515278 U JP8515278 U JP 8515278U JP S594263 Y2 JPS594263 Y2 JP S594263Y2
Authority
JP
Japan
Prior art keywords
operational amplifier
resistance
resistor
input terminal
inverting input
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
JP8515278U
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Japanese (ja)
Other versions
JPS553724U (en
Inventor
増生 花若
Original Assignee
横河電機株式会社
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 横河電機株式会社 filed Critical 横河電機株式会社
Priority to JP8515278U priority Critical patent/JPS594263Y2/en
Publication of JPS553724U publication Critical patent/JPS553724U/ja
Application granted granted Critical
Publication of JPS594263Y2 publication Critical patent/JPS594263Y2/en
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は、測温抵抗体を用いて2個所の温度の差を測定
する装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for measuring the difference in temperature between two locations using a resistance temperature detector.

従来の測温抵抗体を用いた温度差測定装置では、測温抵
抗体に測定現場の検出端から信号の処理を行う変換器ま
での導線の抵抗が加わす、シかも温度差を検出する2つ
の測定現場までの距離の違いにより、導線抵抗が2個の
測温抵抗体で異るため、その影響を受は誤差を生ずる欠
点がある。
In conventional temperature difference measuring devices using resistance temperature detectors, the resistance of the conductor from the detection end at the measurement site to the converter that processes the signal is added to the resistance temperature detector, and the temperature difference is detected by the resistance of the resistance thermometer. Due to the difference in distance to the two measurement sites, the resistance of the conductor wires differs between the two resistance temperature sensors, which has the disadvantage of causing errors.

本考案は、上述の如き導線抵抗の影響を有効に1除去し
、2個所の温度差を簡単な構成で正確に測定できる装置
を提供するものである。
The present invention provides a device that can effectively eliminate the influence of the conductor resistance as described above and accurately measure the temperature difference between two locations with a simple configuration.

第1図は本考案装置の一実施例を示す接続図である。FIG. 1 is a connection diagram showing one embodiment of the device of the present invention.

図において、Rtlは第1の測定個所に配置された3線
式の測温抵抗体、Rt2は第2の測定個所に配置された
3線式の測温抵抗体、11□、 l 12. l 13
は各々Rt1の導線、120,12□、123は各々R
t2の導線、al、bl、CIは各々Rt1(7)導線
端子、a2.b2.C2は各々Rt2の導線端子である
In the figure, Rtl is a three-wire resistance temperature detector placed at the first measurement location, Rt2 is a three-wire resistance temperature detector located at the second measurement location, 11□, l 12. l 13
are the conductors of Rt1, and 120, 12□, 123 are the conductors of Rt1, respectively.
The conductors of t2, al, bl, and CI are the Rt1 (7) conductor terminals, a2. b2. C2 are respective conductor terminals of Rt2.

導線端子a1は電流源■に、C1はa2に、C2は基準
点にそれぞれ接続され、R41トRt2ニ電流iカa1
→11□→R1,→113→c1→a2→12□→R1
2→l 23→C2の経路で流れるように構成されてい
る。
The conductor terminal a1 is connected to the current source ■, C1 is connected to a2, and C2 is connected to the reference point.
→11□→R1,→113→c1→a2→12□→R1
It is configured to flow along the path 2→l 23→C2.

OPl、O20は各々演算増幅器である。OPl and O20 are each operational amplifiers.

OPlはその反転入力端子←)に導線端子a1が演算抵
抗R1を介して接続されるとともに、O20の出力端が
演算抵抗R2を介して接続され、非反転入力端子(ト)
に導線端子b1が接続されている。
The conductor terminal a1 is connected to the inverting input terminal (←) of OPl via the arithmetic resistor R1, and the output terminal of O20 is connected via the arithmetic resistor R2, and the non-inverting input terminal (T)
A conductor terminal b1 is connected to the terminal b1.

またO20の入出力端子間には演算抵抗R3が接続され
ている。
Further, a calculation resistor R3 is connected between the input and output terminals of O20.

O20はその非反転入力端子(1)に導線端子b2が接
続され、反転入力端子(−)にO20の出力を分圧する
演算抵抗R4,R5の分圧点が接続されている。
O20 has a non-inverting input terminal (1) connected to a conductor terminal b2, and an inverting input terminal (-) connected to a voltage dividing point of operational resistors R4 and R5 that divide the output of O20.

このように構威した本考案装置において、電流源■から
の電流iは演算抵抗R1が信号源のRtl。
In the device of the present invention constructed in this way, the current i from the current source ① is Rtl whose signal source is the calculation resistor R1.

Rt、2.l□1.l□3. l 21. l 23の
抵抗に比して充分に大きく選ばれているので、抵抗R1
側への分流はほとんどなく、またOPl、O20の入力
インピーダンスも充分に大きいので、OPl、O20の
非反転入力端子(1)側への分流もほとんどない。
Rt, 2. l□1. l□3. l 21. The resistor R1 is selected to be sufficiently large compared to the resistor R123.
There is almost no shunt to the side, and since the input impedances of OPl and O20 are sufficiently large, there is almost no shunt of current to the non-inverting input terminal (1) side of OPl and O20.

またRtlの導線11、。112、 l 13の各抵抗
はほとんど等しくこれをrlとし、Rt2の導線120
. l 22. l 23の各抵抗もほとんど等しくこ
れをr2とすると、導線の端子a1. bl、 clに
それぞれ生ずる電圧El、R2,R3は各々次式で与え
られる。
Also, the conductor 11 of Rtl. The resistances of 112 and l 13 are almost equal, and this is rl, and the conductor 120 of Rt2 is
.. l 22. The resistances of terminals a1 and 23 of the conductive wire are also almost equal, and if this is designated as r2, The voltages El, R2, and R3 generated at bl and cl, respectively, are given by the following equations.

Ell(2rl + 2r2 + RJ + R
t2) (す
R2= 1(rl + 2rz + RthI+ Rt
2) (2)R3= t (r2+
Rt2) (3)
そして、演算増幅* OPtの出力電圧Eo#i、で与
えられ、 fた演算増幅器oP2の出力E4も で与えられるので、 (す。
Ell(2rl + 2r2 + RJ + R
t2) (R2= 1(rl + 2rz + RthI+ Rt
2) (2) R3= t (r2+
Rt2) (3)
Then, the output voltage Eo#i of the operational amplifier *OPt is given by, and the output E4 of the operational amplifier oP2 is also given by f, so (

(乃。(No.

(5)。(5).

(4)。(4).

(5)式から出 力電圧Eotj となる、ここで、 2R1・R2・R3(η 3R4冒R5(句 を満足するように、演算抵抗R1〜R5の値をぺけ、出
力電圧Eoti、 Eo富2(RJ −Rt2)i
(ガとなり、導線抵抗r1.r2の影響を有効に除去
でき、測温抵抗体R11,R42の抵抗値の差のみに対
応した出力電圧Eoが得られる。
From equation (5), the output voltage Eotj is obtained, where: 2R1, R2, R3(η 3R4, R5 RJ-Rt2)i
(The influence of the conductor resistances r1 and r2 can be effectively removed, and an output voltage Eo corresponding only to the difference in resistance value between the resistance temperature sensors R11 and R42 can be obtained.

したがって、測定抵抗体Rt1.Rt2が銅測温抵抗体
の場合には、抵抗値が温度に対してリニアであるので、
電流iが一定であれば゛、出力電圧Eoは、 れば、出力電圧Eo#i、 Eo = K (T I −72)
(2)ただし、Kけ定数 となり、2個所の温度差を導線抵抗の影響を受けること
なく正確に測定することができる。
Therefore, the measuring resistor Rt1. If Rt2 is a copper resistance temperature sensor, the resistance value is linear with respect to temperature, so
If the current i is constant, the output voltage Eo is, If the output voltage Eo#i, Eo = K (T I -72)
(2) However, K is a constant, and the temperature difference between two places can be accurately measured without being affected by the resistance of the conductor.

第2図は本考案装置の他の実施例で、Rtl、Rt2と
して白金測温抵抗体を用いる場合の接続図である。
FIG. 2 is a connection diagram showing another embodiment of the device according to the present invention, in which platinum resistance temperature detectors are used as Rtl and Rt2.

周知のように白金測温抵抗体は抵抗値と温度の関係が非
直線性を有し、通常は T″:k (Rt+αRt2)
(1:0ただし、klαは定数 で近似されており、温度によって同じ温度差に対する2
つの測温体の抵抗値の差が異なる。
As is well known, platinum resistance thermometers have a nonlinear relationship between resistance value and temperature, and usually T″:k (Rt+αRt2)
(1:0 However, klα is approximated by a constant, and depending on the temperature, the
The difference in the resistance values of the two thermometers is different.

本実施例ではこのような非直線性を補正し、温度差を正
確に測定できるようにしたものである。
In this embodiment, such nonlinearity is corrected so that temperature differences can be measured accurately.

第2図の実施例において、第1図の実施例と異るところ
は、電流源■を演算増幅器OP3.OP4を主体に構威
し、出力電流iをRtl、Rt2の値に応じて変化させ
るようにした点である。
The embodiment shown in FIG. 2 differs from the embodiment shown in FIG. The main feature is that OP4 is used as the main component, and the output current i is changed according to the values of Rtl and Rt2.

すなわち、O20はその反転入力端子(−)に基準電圧
Esが演算抵抗R6を介して加えられるとともに、演算
抵抗R7を介してO20の出力E4が加えられており、
非反転入力端子(1)には導線端子C1の電圧E5が加
えられている。
That is, the reference voltage Es is applied to the inverting input terminal (-) of O20 via a calculation resistor R6, and the output E4 of O20 is applied via a calculation resistor R7.
The voltage E5 of the conductor terminal C1 is applied to the non-inverting input terminal (1).

またO20の出力E6が演算抵抗R8を介して反転入力
端子(−)に帰還されている。
Further, the output E6 of O20 is fed back to the inverting input terminal (-) via the operational resistor R8.

よって、O20の出力E6は次式で与えられる。Therefore, the output E6 of O20 is given by the following equation.

なお、導線端子C2の電圧E5は次式で与えられる。Note that the voltage E5 of the conductor terminal C2 is given by the following equation.

R5= <zrz + atz) i
(’1また、O12はその反転入力端子(
ヨにO20の出力E6が演算抵抗R9を介して加えられ
、非反転入力端子(→に導線端子b2の電圧E2が加え
られている。
R5= <zrz + atz) i
('1 Also, O12 is its inverting input terminal (
The output E6 of O20 is applied to Y via the operational resistor R9, and the voltage E2 of the conductor terminal b2 is applied to the non-inverting input terminal (→).

またO12の出力E7が演算抵抗R1oを介して反転入
力端子(−)に帰還されているので、出力E7はとなる
Also, since the output E7 of O12 is fed back to the inverting input terminal (-) via the operational resistor R1o, the output E7 becomes.

この出力E7が抵抗Rfで次式に示す如く電流iに変換
されて測温抵抗体R41,Rt2に供給される。
This output E7 is converted into a current i by a resistor Rf as shown in the following equation, and is supplied to the temperature measuring resistors R41 and Rt2.

したがって、各式から電流源■の出力電流iは次式で与
えられる。
Therefore, from each equation, the output current i of current source (2) is given by the following equation.

ここで゛、 R6= R7= 2RB R9・Rlov) を満足するように、演算抵抗R6〜R1oの値を選定す
れば、出力電流iは、 となり、導線抵抗r□、r2には無関係で、かつR11
゜R42の値に応じて変化するようになる。
If the values of the operational resistors R6 to R1o are selected so as to satisfy ゛, R6=R7=2RB R9・Rlov), the output current i becomes R11
It changes according to the value of °R42.

よって、O40の出力電圧Eoは、 となる。Therefore, the output voltage Eo of O40 is becomes.

そして白金測温抵抗体の場合には、が成立するので、(
19)式は(21)式の如く展開できる。
And in the case of a platinum resistance thermometer, holds true, so (
Equation 19) can be expanded as shown in Equation (21).

(11)式と(21)式とから出力電圧Eoは、となり
、白金測温抵抗体の非直線性が補正され、温度差に正確
に比例した出力電圧が得られる。
From equations (11) and (21), the output voltage Eo is as follows, the nonlinearity of the platinum resistance temperature sensor is corrected, and an output voltage that is accurately proportional to the temperature difference is obtained.

以上説明したように本考案によれば、2個所の温度差を
導線抵抗の影響を受けることなく正確に測定できる温度
差測定装置が簡単な構成で得られる。
As explained above, according to the present invention, a temperature difference measuring device that can accurately measure the temperature difference between two locations without being affected by the resistance of the conductor wire can be obtained with a simple configuration.

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

第1図は本考案装置の一実施例を示す接続図、第2図は
本考案装置の他の実施例を示す接続図である。 Rtl、R42・・・・・・測温抵抗体、OP1〜OP
4・・・・・・演算増幅器、R1〜RIO・・・・・・
演算抵抗、Rf・・・・・・抵抗、■・・・・・・電流
源、■・・・・・・電圧源。
FIG. 1 is a connection diagram showing one embodiment of the device of the present invention, and FIG. 2 is a connection diagram showing another embodiment of the device of the present invention. Rtl, R42...Resistance temperature sensor, OP1~OP
4...Operation amplifier, R1~RIO...
Arithmetic resistance, Rf...Resistance, ■...Current source, ■...Voltage source.

Claims (4)

【実用新案登録請求の範囲】[Scope of utility model registration request] (1)第1の測定個所に配置された3線式の測温抵抗体
と、第2の測定個所に配置された3線式の測温抵抗体と
、両測温抵抗体と各測温抵抗体の両端の導線を電流源に
直列に接続する手段と、第1の測温抵抗体の残りの導線
が非反転入力端子に接続されており、かつ第1の測温抵
抗体の電流源側の導線が演算抵抗を介して反転入力端子
に接続されている第1の演算増幅器と、第2の測温抵抗
体の残りの導線が非反転入力端子に接続されている第2
の演算増幅器と、第2の演算増幅器の出力を分圧してそ
の反転入力端子に帰環するための演算抵抗と、第2の演
算増幅器の出力を第1の演算増幅器の反転入力端子に加
えるための演算抵抗と、第の演算増幅器の出力をその反
転入力端子に帰還するための演算抵抗を有し、前記各演
算抵抗の値を選定することによって第1、第2の測温抵
抗体の導線の抵抗の影響を受けないようにしたことを特
徴とする温度差測定装置。
(1) A 3-wire resistance temperature detector placed at the first measurement location, a 3-wire resistance temperature detector placed at the second measurement location, both resistance bulbs, and each temperature measurement means for connecting the conductors at both ends of the resistor in series to a current source, the remaining conductors of the first resistance temperature detector being connected to the non-inverting input terminal, and a current source for the first resistance temperature detector; A first operational amplifier whose side conductor is connected to the inverting input terminal via the operational resistor, and a second operational amplifier whose remaining conductor of the second resistance temperature detector is connected to the non-inverting input terminal.
an operational amplifier, an operational resistor for voltage-dividing the output of the second operational amplifier and returning it to its inverting input terminal, and an operational resistor for applying the output of the second operational amplifier to the inverting input terminal of the first operational amplifier. and an operational resistor for feeding back the output of the first operational amplifier to its inverting input terminal. A temperature difference measuring device characterized in that it is not affected by resistance.
(2)電流源として定電流源を用いたことを特徴とする
実用新案登録請求の範囲第1項記載の温度差測定装置。
(2) The temperature difference measuring device according to claim 1, characterized in that a constant current source is used as the current source.
(3)第1、第2の測温抵抗体の抵抗値に応じて出力電
流が変化する電流源を用いたことを特徴とする実用新案
登録請求の範囲第1項記載の温度差測定装置。
(3) The temperature difference measuring device according to claim 1, which is a registered utility model, characterized in that it uses a current source whose output current changes depending on the resistance values of the first and second resistance temperature sensors.
(4)入出力端子間に演算抵抗を有し、反転入力端子に
基準電圧が演算抵抗を介して加えられ、かつ第2の演算
増幅器の出力が演算抵抗を介して加えられており、また
非反転入力端子には第1、第2の測温抵抗体の接続点の
電位が与えられている第3の演算増幅器と、入出力端子
間に演算抵抗を有し、反転入力端子に第3の演算増幅器
の出力が演算抵抗を介して加えられ、非反転入力端子に
第1の測温抵抗体の一端の電位が与えられている第4の
演算増幅器と、第4の演算増幅器の出力電圧を電流に変
換して第1、第2の測温抵抗体に供給するための抵抗と
で構成された電流源を用いたことを特徴とする実用新案
登録請求の範囲第1項記載の温度差測定装置。
(4) A calculation resistor is provided between the input and output terminals, the reference voltage is applied to the inverting input terminal via the calculation resistance, and the output of the second operational amplifier is applied via the calculation resistance, and the A third operational amplifier having an inverting input terminal supplied with the potential at the connection point of the first and second resistance temperature detectors, and a third operational amplifier having an operational resistor between the input and output terminals, a fourth operational amplifier to which the output of the operational amplifier is applied via the operational resistor and the potential of one end of the first resistance temperature detector is applied to the non-inverting input terminal; and the output voltage of the fourth operational amplifier. Temperature difference measurement according to claim 1 of the utility model registration claim, characterized in that a current source configured with a resistor for converting into current and supplying the current to the first and second resistance temperature sensors is used. Device.
JP8515278U 1978-06-21 1978-06-21 Temperature difference measuring device Expired JPS594263Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8515278U JPS594263Y2 (en) 1978-06-21 1978-06-21 Temperature difference measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8515278U JPS594263Y2 (en) 1978-06-21 1978-06-21 Temperature difference measuring device

Publications (2)

Publication Number Publication Date
JPS553724U JPS553724U (en) 1980-01-11
JPS594263Y2 true JPS594263Y2 (en) 1984-02-07

Family

ID=29008510

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8515278U Expired JPS594263Y2 (en) 1978-06-21 1978-06-21 Temperature difference measuring device

Country Status (1)

Country Link
JP (1) JPS594263Y2 (en)

Also Published As

Publication number Publication date
JPS553724U (en) 1980-01-11

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