JPS5985106A - Linearizing circuit - Google Patents

Linearizing circuit

Info

Publication number
JPS5985106A
JPS5985106A JP18309383A JP18309383A JPS5985106A JP S5985106 A JPS5985106 A JP S5985106A JP 18309383 A JP18309383 A JP 18309383A JP 18309383 A JP18309383 A JP 18309383A JP S5985106 A JPS5985106 A JP S5985106A
Authority
JP
Japan
Prior art keywords
circuit
input
operational amplifier
output
resistor
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.)
Granted
Application number
JP18309383A
Other languages
Japanese (ja)
Other versions
JPS6350644B2 (en
Inventor
Junichi Kondo
純一 近藤
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.)
NIPPON RANKO KK
Original Assignee
NIPPON RANKO KK
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 NIPPON RANKO KK filed Critical NIPPON RANKO KK
Priority to JP18309383A priority Critical patent/JPS5985106A/en
Publication of JPS5985106A publication Critical patent/JPS5985106A/en
Publication of JPS6350644B2 publication Critical patent/JPS6350644B2/ja
Granted legal-status Critical Current

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  • Indication And Recording Devices For Special Purposes And Tariff Metering Devices (AREA)
  • Amplifiers (AREA)

Abstract

PURPOSE:To compensate the measuring temperature versus converting voltage characteristic of an input signal by providing a nonlinearity compensating circuit using a Zener diode to an input circuit of an operational amplifier. CONSTITUTION:The measured output of a temperature measuring circuit 1 is amplified at an amplifier circuit 9 and inputted to a linearizing circuit 10. Said linearizing circuit 10 has an operational amplifier 25, a series circuit comprising resistors 28, 29 and a Zener diode 30 is connected to the 1st input and a circuit comprising resistors 26, 27 and a Zener diode 31 connected between a connecting point of the resistors and ground is connected to the 2nd input. An input signal is impressed to a connecting point between the resistors 28 and 26. Thus, the measuring temperature versus converting voltage characteristic of the input signal is compensated and linearized by the circuit comprising the Zener diode and the resistors, and a compensated output is obtained between terminals 23 and 32.

Description

【発明の詳細な説明】 技術分野 本発明は例えば抵抗体の温度による抵抗値の変化によっ
て得られる出力信号を温度変化に対し直線的に変化する
ように補償する直線化回路に関する。
TECHNICAL FIELD The present invention relates to a linearization circuit that compensates for an output signal obtained by a change in resistance value due to temperature, for example, of a resistor so that it changes linearly with respect to temperature change.

従来技術 従来、温度変化による抵抗値の変化を重圧に変換する回
路としては、測温抵抗素子全抵抗ブリッジの一辺に接続
し、測温抵抗素子の或基準値において他要素を調整して
平衡をとり、その後は測温抵抗素子の抵抗値の変化によ
るブリッジの不平衡のため発生する電圧を計器でm・i
r、み取るような回路が用いられていた。この回路にお
いては、測温抵抗素子は一般に部属測定回路本体と1ζ
1すれていることが多く、その場合にはり一ド腺の影響
のために測定が不正確になり、それを避けようとしてリ
ード線の断面積の太きbものを用いても、測定誤差を所
定値以下にすることができないという問題点があった。
Conventional technology Conventionally, as a circuit for converting changes in resistance value due to temperature changes into heavy pressure, a resistance temperature detector is connected to one side of a total resistance bridge, and other elements are adjusted at a certain reference value of the resistance temperature detector to maintain balance. After that, the voltage generated due to the unbalance of the bridge due to the change in the resistance value of the resistance temperature sensor is measured with a meter.
r, a similar circuit was used. In this circuit, the temperature measuring resistance element is generally connected to the main body of the measuring circuit.
1. In this case, the measurement will be inaccurate due to the influence of the lead wire, and even if you use a lead wire with a thicker cross-sectional area to avoid this, the measurement error will still be avoided. There was a problem in that it was not possible to lower the value below a predetermined value.

この問題点を解決するため2つの演算増幅器回路を用い
、そのうちの1つの演算増幅器回路の帰還抵抗に測温抵
抗素子を接続t2、他方の/1437ハ’zll〜゛1
1器回路の帰還抵抗として基準潟18″における1ll
11温4I(抗素子の抵抗値を有する抵抗全接続し7、
両噌幅器回路の差を求める回路が本発明者によって発明
さf 1. !−+fj示さlj−た(こ)、′膜OK
;54−102795号参照)。
To solve this problem, two operational amplifier circuits are used, and a temperature measuring resistance element is connected to the feedback resistance of one of the operational amplifier circuits t2, and the other /1437 h'zll~゛1
1ll as a feedback resistor for a single circuit at a reference angle of 18''
11 temperature 4I (all resistors with the resistance value of the resistance element are connected 7,
The inventor invented a circuit for determining the difference between the two width scale circuits.f1. ! -+fj showed lj-ta(ko), 'membrane OK
; see No. 54-102795).

この11・回路乞1t1 ? 、6とリード線の影゛;
卑は減少させることができるが、市販の測温抵抗素子に
おりては、yilA Jgとその抵抗値とは非直線的関
係Vこあり、最大の所で例えば数・Ω−セントの差があ
り、測定温度ス・1変換電圧!?、¥性に直線的関係が
外来さり、る1μ合には適応できないという別の問題点
が発生した。
This 11 circuit beggar 1t1? , 6 and the shadow of the lead wire;
However, in commercially available RTDs, there is a non-linear relationship between yilA Jg and its resistance value, and there is a difference of, for example, several Ω-cents at the maximum point. , measurement temperature and 1 conversion voltage! ? , another problem arose in that the linear relationship was foreign to the value and could not be applied to the 1μ case.

発「シ」の目的 本発明の目的(/i、前述の問題点にかんがみ、増幅回
路の入力回路に抵抗およびツェナーダイオードによる回
路網を設け、入力信号の非直線性を補償するという構想
に基づき、測温抵抗素子の温度対抵抗値の特性に起因す
る測定温度対変換電圧特性を補償してiIV線的関係と
し、1M線的な測定温度対変換爾1川lIk性が要求さ
れる用途に適合できるようにすることにある。
Purpose of the invention (/i) In view of the above-mentioned problems, the present invention is based on the concept of providing a circuit network of resistors and Zener diodes in the input circuit of an amplifier circuit to compensate for the nonlinearity of the input signal. , the measured temperature vs. converted voltage characteristic caused by the temperature vs. resistance value characteristic of the resistance thermometer element is compensated for an iIV linear relationship, and is suitable for applications that require a 1M linear measured temperature vs. converted voltage characteristic. The goal is to be able to adapt.

発明の構成 本発明に卦いては、演算増幅器の第1入力回路に抵抗2
よびツェナーダイオードのin列回路を接続し、第2入
力回路に直列接続された抵抗を設け、該抵抗の直列接続
点と払:、 tlb点との間に別のツェナーダイオード
を接続し、該第、1入力回路に接続された直列回路の積
演算増幅?1:と反対■111の−(儒と、該第2入力
回路に1投けられ、ンλ曲列j:[′i、杭回路のi<
F<演算増幅器と反対(l11の一昨とを41、続し入
カイへ号を加えるように1−1該人力信号供給点と該演
算増幅器)二の出力端子の間から出力を取出すようにし
たi71′線化回路が提供さハ、る。
Structure of the Invention According to the present invention, a resistor 2 is connected to the first input circuit of the operational amplifier.
and an in-line circuit of Zener diodes, a resistor connected in series to the second input circuit is provided, another Zener diode is connected between the series connection point of the resistor and the point TLB, and the second input circuit is , product amplification of series circuits connected to one input circuit? 1: Opposite ■ 111 - (Confucian, 1 is thrown into the second input circuit, nλ curve sequence j: ['i, i< of the pile circuit
F< Opposite of operational amplifier (111 and 41, and add a number to input Kai, 1-1 the human power signal supply point and the operational amplifier) Take the output from between the output terminals of 2 An i71' wiring circuit is provided.

実施例 本発明の一実施例としての「α線化回路を用いた・需度
測定装尚゛の[1()If路図が第] 12jに示され
る。本装置は温度測足回路1.増幅回路9.オアーよび
直線化回路10を具備する。
Embodiment A demand measuring device using an α-ray converting circuit as an embodiment of the present invention is shown in [1() If route diagram] 12j.This device has a temperature measuring circuit 1. Amplification circuit 9. Includes OR and linearization circuit 10.

温度3+il 5:j雪(4)路1について一児[yj
する。ン則J績抵抗人子13は第1演10Xl曽幅器1
1の反1転入力からリード線18を月1いてその−☆1
1.1へ」入細二さ)1、泪11ρ訃↓FC+11素子
13の他端(づ、リード糺用6ふ・よび17の一端1が
接続さ力2、リード線1i−1ぞの他端か記1演;ζ1
、増幅器11の出力へJ&続さJI、で丸・す、4I、
1の定71ij圧jul昌11C源6aは第2演算増1
ij、器11)す、夕)の各削号′I増描器の76、源
と[7て用いら)9るほか、中性点が接地さカフ、箱4
圧を分割して第1演算増幅器回路7の人ノルihj子4
0へ供給する。入力端子40と第1演算増幅器11の反
転入力の間には適当な抵抗領置・有する抵抗器12が挿
入さハ、る。第1演算増幅器11の非反転入力は接地さ
れる。第1演算増幅器11の出力端子と第2前算増1賜
器19の出力端子は互に接続さハ、てふ・す、前述のリ
ード線1Gはその他端が基I曽電圧設定およびリード線
影響打消用第2演ず〕:増幅器回路8の帰還用抵抗器1
5の一端へ接続きノ11、シ′九2の定電圧il流電源
6bは第2の演算増幅器】9の電1源を供給するほか、
電圧全労′、!;Uして第2の、メ算増幅器19の反転
入力へ通ずる人力j’1m子41へ印加さり1、入力端
子4】より適当な抵抗2:÷14を介して第2演算増幅
器19の反転入力へ接続され、該反転入力Uニオブこト
1(抗器15の他端へ接続き)1、ている。第2の定電
圧直流、電源6bの中性点は物足の一位に固定されて訃
らず、第2演慢増幅器j9の非反転入力端子に接続され
、この中性点と接地点の間の電圧は第1演tリー増幅器
回路7、および基ifQ′駈圧設定圧設定リード糺!影
響打消用第2演算増幅器回路8の系統L・(:おける出
力となる。
Temperature 3 + il 5: j Snow (4) Ichiko about road 1 [yj
do. N rule J performance resistance person 13 is the first performance 10Xl width instrument 1
Connect the lead wire 18 from the inverted input of 1 to -☆1.
1.1) 1, 11 ρ ↓ FC + 11 The other end of the element 13 (Du, one end 1 of the lead wire 6 and 17 is connected. Force 2, the other end of the lead wire 1i-1) Hatakaki 1 performance; ζ1
, J& continued to the output of amplifier 11, JI, demaru・su, 4I,
1 constant 71ij pressure jul change 11C source 6a is second calculation increase 1
ij, vessel 11), evening), each erasure number 'I intensifier's 76, source and [7 used) 9, as well as the neutral point being grounded, cuff, box 4
Divide the pressure into the first operational amplifier circuit 7
Supply to 0. A resistor 12 having an appropriate resistance is inserted between the input terminal 40 and the inverting input of the first operational amplifier 11. The non-inverting input of the first operational amplifier 11 is grounded. The output terminal of the first operational amplifier 11 and the output terminal of the second preamplifier 19 are connected to each other. Second part for canceling the influence]: Feedback resistor 1 of amplifier circuit 8
A constant voltage current power source 6b connected to one end of the second operational amplifier 11 and 92 supplies a power source for the second operational amplifier 9.
Voltage Zenrō′,! ; U is applied to the input terminal 41 which leads to the inverting input of the second operational amplifier 19 through a suitable resistor 2:÷14; The inverting input U niobium oxide 1 (connected to the other end of the resistor 15) is connected to the input. The neutral point of the second constant voltage DC power source 6b is fixed at the first position and is connected to the non-inverting input terminal of the second performance amplifier j9, and the neutral point and the ground point are connected to the non-inverting input terminal of the second performance amplifier j9. The voltage between the first lead amplifier circuit 7 and the base if Q' is the lead pressure setting lead! This is the output of the system L·(: of the second operational amplifier circuit 8 for canceling the influence.

次にその佃1作を説明する。;lj ] rt’j、算
増幅器回路7に卦いてはその増幅、四G (、寸、ここ
にR1,:測温抵抗素子13の抵抗++1+、R12゜
抵抗器120(1(抗値である。従って入力9″11.
1子40に常に一定の1f1流′t!シ圧か印加さ]1
.てふ・れは第1演1*i+iQ l照器11の出力1
171.Gに比例した、すなわち1N12を一定とずノ
1. iJ R、3に比1・・1]シた出力をイ!Iる
ことができる。
Next, I will explain Tsukuda's first work. ;lj ] rt'j, the amplification of the arithmetic amplifier circuit 7, 4G .Therefore, input 9″11.
1 child 40 always has a constant 1f1 style't! Pressure applied]1
.. Tefu・Reha 1st performance 1*i+iQ l illuminator 11 output 1
171. Proportional to G, that is, 1N12 is constant. iJ R, 3 to 1...1] output! I can.

第2.偵窟増′M器19(・Cついても同様に抵抗器1
5に比例し7プと増liv、′1度が告らft、入力端
子・11に入力端一1″4()と回じ′トシ、用が印加
さノ11、抵抗x:112および】4の抵抗(的かII
+1−であり、測?1.+’+ ’J’:抗宋二■′の
ある基準温度(たとえば0℃に五ぶとJ:lS ’Gが
よい)にふ・ける抵抗値に舌しくJ」(抗器15孕、浸
定するならば、該)、l−j’lfi 1・嘉;仄VC
上−いて1山〕で”山、’A−,”5jlQri君、の
出力(d: ji1ルベルとなる。ここにおいて円演算
増幅器の出力の差をこる。Lう出力回路を直列接続すれ
ば1、該ノー、準温fg−にふ・いては出力はイ丁消し
て0とカリ、基1■篇度より7品度が変化し44]]温
抵抗素子の抵抗値が変化した1171合、 (差のW、力)−k X (Rt  Rr )  −−
−(2)となり所望の関係が得られる。ここにkは比例
定数、Rtばt℃に」?ける測温抵抗素子の抵抗値、R
rは該基準ンvツメVcおける611J温抵抗素子の抵
抗値である。
Second. Reconnaissance increase 'M device 19 (Similarly for C, resistor 1
Proportional to 5, 7p and increase liv, '1 degree is given, ft is applied to input terminal 11, input terminal 1''4 () and turn 'toshi, 11, resistor x: 112 and ] 4 resistance (target II
+1- and measurement? 1. +'+ 'J': Anti-Song 2 ■' Please note the resistance value at a certain standard temperature (for example, 0℃ and 5 J:lS'G is good). If specified, then), l-j'lfi 1・嘉;仄VC
The output of Qri (d: ji1 level) is 1 level.If the output circuits are connected in series, the output is 1. , when the quasi-temperature fg- is reached, the output is turned off and becomes 0, and the resistance value of the temperature resistance element changes 1171 times, with 7 quality changes from the basic 1. (Difference W, force) -k X (Rt Rr) --
-(2), and the desired relationship is obtained. Here, k is a constant of proportionality, and Rt is t°C. The resistance value of the resistance temperature measuring element, R
r is the resistance value of the 611J temperature resistance element at the reference point Vc.

一般に測温抵抗素子は温度測定回路の本体と離れた場所
に設置l″1′する場合が多く、そのIJ −1’線の
抵抗値か測温抵抗素子の抵抗値に加算さね、誤差の原因
となる。本回路においては、第1演算増幅器11の帰還
回路用の抵抗である測温抵抗素子にはり−)°線17お
よび18が加算さ力、第2演絢−増幅器1つの帰還回路
用の抵抗器15にu:リード線16と17か加算さiす
るようになっているから、リード線16,17.18が
同一」Jで接値であればその影響は同じであり、両演算
増幅器の出力の差をとることによってリード線の抵抗値
により俊1カ電:圧に生ずる誤差をij消すことができ
る。
Generally, the resistance temperature detector is often installed at a location far away from the main body of the temperature measurement circuit, and the resistance value of the IJ -1' wire is not added to the resistance value of the resistance temperature detector, resulting in an error. In this circuit, the force of the wires 17 and 18 is added to the temperature measuring resistance element which is the resistance for the feedback circuit of the first operational amplifier 11, and the feedback circuit of the second operational amplifier 11 is Since the lead wires 16 and 17 are added to the resistor 15 for the purpose, the effect is the same if the lead wires 16, 17, and 18 are the same and have the same value. By taking the difference in the outputs of the operational amplifiers, it is possible to eliminate errors that occur in the voltage due to the resistance values of the lead wires.

増幅回路9について説明−(る。1jjl述の温度測定
回路lの出力は添1子4:3と接地点の間に′r10上
とし。
Explanation of the amplifier circuit 9-(1jjl) The output of the temperature measuring circuit 1 described above is placed above 'r10 between the support 4:3 and the ground point.

て出力さ)1、端子43の出力は増幅回路9の入力端子
へ供給訟れる。入力端予力・ら(J適当な抵抗21を介
して演算増幅’di 200反転入力へ接続され、帰還
用抵抗22は所嘗増幅器2oの反転入力と出力の間に挿
入官力1、抵抗21 i;−、J:び22ケ1lIij
’、1幅回路9において後述する所望の増幅度がイuら
)1゜るように決定される。
The output of the terminal 43 is supplied to the input terminal of the amplifier circuit 9. The input terminal is connected to the inverting input of the operational amplifier 200 through a suitable resistor 21, and the feedback resistor 22 is inserted between the inverting input and the output of the amplifier 2o. i;-, J:bi22ke1lIij
', the desired amplification degree, which will be described later, in the 1-width circuit 9 is determined to be 1 degree.

直線化回路1 (1(tCついで6,7明する。増幅回
路9の出力は11′1線化回路1 (]のW−線化回路
網へ接続される。iμ線化回路網C1ぞの入力端がら抵
イ冗1:: 28、ツェナーダイオード:30 % U
’−i>j−、k 29を介して演)゛ン増幅?×25
の反転入力へ接続呑ね、ツェナーダイオードの方向は抵
抗器28の11+11に陰=極、抵抗器29のII+1
1 K、陽(返が接紬−さ)する。lI′l純fヒ回路
網の残部は入力端から抵抗器26 :lL−よび27ケ
ブ1−シて削p−増幅詣25の非反転入力へ12、経、
さ′i11、抵4ノ)器2fi:I’i−よび′)7の
jど^、tシ点と接地間にツェナーダ・fオード;(1
か挿入される。ツェナーダイオード、′]1の方向(7
J、その陽A版が接池倶:1に接A泳官)7、る。演算
増幅器25の反転入力と出力の間には帰還用抵抗′(3
が接h′シされる。
Linearizing circuit 1 (1(tC), then 6 and 7. The output of the amplifier circuit 9 is connected to the W-line converting circuit network 11'1 line converting circuit 1 (). Input terminal resistance redundancy 1: 28, Zener diode: 30% U
'-i>j-, k amplification through 29? ×25
Connect to the inverting input of the zener diode.
1 K, Yang (returning to Tsumugi-sa). The remainder of the network is connected from the input end to the non-inverting input of the amplification circuit 25 through resistors 26:1L- and 27,
(1
or inserted. Zener diode, ']1 direction (7
J, the positive A version is connected to the pond: 1) 7. Ru. A feedback resistor' (3) is connected between the inverting input and the output of the operational amplifier 25.
is connected h'.

前述の回路のjif+作を・第2ないし第5図の特性図
全容1jjしつつ説、明」−る。僧11w3回路9は第
]演算116幅器回路7、とノ、を帖%I、圧設定およ
びリー16線影響打消用Vf′X’ 2演算増幅器回路
の差の出力全適当に増幅する。6()]定する1晶度囲
囲(’ro−T、)に対応する変換Δノ″l−だil’
、出値のij、ij、囲(Vo〜V11 )が、if、
を線化回路網の入力に」・・因で、直線化回路網に使用
するツェナーダイオード”30 、31のノエノーー電
圧の約2倍であることが要求されるので、その条件を満
足するよう抵抗器22により利イ↓J全調整する。出力
嬬イ43件たけ出力端子23においては、完全な正比例
するif、’+tlQ! ?1′1 <やや上に凸な温
度(r)?を宙、圧出力M75B4! r)ILル(第
2 L”’、:破Md )。もち輪画と間では絶対値は
演算増幅器20の回路の1曽、1県用゛/どけ異なる。
The operation of the above-mentioned circuit will be explained with reference to the complete characteristic diagrams shown in FIGS. 2 to 5. The 11w3 circuit 9 appropriately amplifies the output of the difference between the 116th operational amplifier circuit 7 and the 2nd operational amplifier circuit 7, %I, pressure setting, and Vf'X' for canceling the influence of the 16th line. 6()] The transformation Δノ″l-dil′ corresponding to the crystallinity range ('ro-T,) defined
, the output value ij, ij, and the range (Vo to V11) are if,
For the input of the linearization network, it is required that the voltage be approximately twice the voltage of the Zener diodes 30 and 31 used in the linearization network, so the resistor must be set to meet that condition. The output terminal 23 has a total of 43 outputs, and the output terminal 23 has a perfectly directly proportional if,'+tlQ!?1'1 <Slightly upwardly convex temperature (r)? Pressure force M75B4! r) IL le (2nd L"',: Break Md). The absolute value differs between the mochi ring and the circuit of the operational amplifier 20 by one degree and one degree.

このグラフのl1ft線が1h線とならないのは測温抵
抗表子の1’!’X、 IL”f対抵抗類の同右の特性
に依存しでいる。泊fl’):I化1!」: II’、
X41本・こ便用さハ2るツェナーダイオード3 (1
、:l ]のツェナーtIL圧は、該回路網の入力に′
3.−いて、i′11.7.1租副定イQ) 1jjl
 (’I’ o 〜E’ I )Vl対応する電圧’j
’i>t!tl (vo−Vll )の(・ユは半分で
あることを必要とする。1ず第1の分枝については、入
力の印Jlil霜、圧V、がv、、72以下の場合導i
76、すずvl、/2L−J、上にかいては(印加電圧
−v、、/2)の電圧イ直を】用!関させ(第4[ン1
44)i寅算J胃11県器250反転入力に印加される
。第2の分1支にお−ては入力の[)」加重、用がvi
+/’21反−トの場合は、その寸ま導通し”1+/2
全超える与1合は”11/2の一定値をとる( Ff>
 4しI45)。第1の分枝の出力を(損性を変えて、
第2の分枝の11′カと)J自−すると折(Ydi!状
の出力′市川が11子ら)′)−る(ごf’! 、51
シ昌16)。演絆増幅藩25の帰還jJ(抗33m1病
当に魂ぶCとにより折線を変換することができるので(
2→シ5図46−47)結局円弧状の’l(j、 lf
f−を・41することかできる(第31ン])。ここに
」斤ノ腺が円弧状に変っf(−J’!i1山シ、L、こ
のグをンフは3:jjjj 、倫r]白−でなぐ、′ス
何蒲iの11〆j−c;もっ−こノエす−ゴノイτ−1
゛の電、+ F:、 グー盲i1.I′/114曲紳が
即用的な文士り’I’¥ 4;−Cを示さなし−まため
である。この円弧状の出゛力市川(第゛3図)を演拌噌
)1参20の出力f8’、 I上(鉋72しl破線から
差引ぐことによって、すなわち実施例(第1し1)C′
こぶ・いて出力を端子23と32の間から引出すことに
より、正比例直線に相当する変換特性をイ(Iることか
できる( 2J’ 2図実線)。
The reason why the l1ft line in this graph is not the 1h line is 1' of the resistance temperature measurement table! 'X, IL' depends on the same characteristics of the resistance class. Night fl'): I conversion 1!': II',
X41 pcs. 2 Zener diodes 3 (1
, :l ] at the input of the network.
3. -i'11.7.1 Tax sub-determination iQ) 1jjl
('I' o ~ E' I ) Vl corresponding voltage 'j
'i>t! tl (vo-Vll) is required to be half.1.For the first branch, if the input mark Jlil frost, the pressure V, is less than or equal to v, 72, then the guide i
76, Tin vl, /2L-J, above is the voltage I of (applied voltage -v,, /2)] for! Related (4th [n1)
44) It is applied to the inversion input of the i-calculation J stomach 11 prefecture device 250. In the second branch, the input [)” weight is used as vi
In the case of +/'21 counter-t, conduction to that extent is "1+/2
The total exceeds 1 and takes a constant value of 11/2 (Ff>
4 I45). The output of the first branch (with different loss characteristics,
11' of the second branch) J - Then fold (Ydi!-shaped output 'Ichikawa is 11 children)') - (go f'!, 51
Shisho 16). The return of the Enkin Amplification Domain 25 jJ (anti-33m1 illness ni soul bu C and the broken line can be converted (
2→C5 Figures 46-47) Eventually, the arc-shaped 'l(j, lf
It is possible to change f- to 41 (31st n]). Here, the gland changes into an arc f (-J'! c; More Konoesu Gonoi τ-1
゛den, +F:, goo blindness i1. I' / 114 Song Gentleman is a handy literary writer 'I' ¥ 4;-C is not shown-Matame. By subtracting this arc-shaped output power Ichikawa (Figure 3) from the output f8', I (plane 72) from the dashed line, that is, Example (1st 1) C'
By drawing out the output from between terminals 23 and 32, a conversion characteristic corresponding to a directly proportional straight line can be obtained (2J' solid line in Figure 2).

発明の効果 本発明によれば、7’1jll温抵抗未子の温度対抵抗
値の特性に起因する61す定温度対変換電圧特性を補償
]−7て直線的関係とU7、直線的な測定温度対変換電
圧1.1を性が要求さノ1.る用途に適合させることが
できる。
Effects of the Invention According to the present invention, it is possible to compensate for the constant temperature vs. converted voltage characteristics caused by the temperature vs. resistance characteristics of the temperature resistance. Temperature versus conversion voltage 1.1 is required. It can be adapted to various applications.

4 図面のfrti単な説、明 第1図に1、本発明の−pyIi+i例と12での11
1線化回路全川−た温j、L +1lll ’jjl装
蓚の回路図、第2図、第3図。
4 A simple explanation of the drawings, 1 in Figure 1, 1 in -pyIi + i example of the invention and 11 in 12
Circuit diagrams of the one-wire circuit, Figures 2 and 3.

第4図、訃よび第51メ]は第1(シ1に示す装置の動
作を説明する特性図である。
Figures 4 and 51 are characteristic diagrams illustrating the operation of the device shown in Figure 1.

1・・・温度測定回路、6a−第1の定電圧部m1電源
、6b・・・第2の定電圧1α流喧源、7・・・第1演
算増幅器回路、8・・・基部1.t E[設定釦よびリ
ード純影響打消用第2演算増幅器回路、9・・・増1[
・畠回路、1()・・・直線化回路、11・aP、 ]
演算増幅器、12・・・抵抗器、】3・・・1ill温
抵抗素子、14.15・・抵抗2()、16,17.1
8・・・リード線、19・・・第2演算増幅器、20・
・・演算増幅器、21.22・抵抗器、23・・・増幅
回路出力端子、24・・接地端子、25・・・演算増幅
器、2F+ 、27.28.29・・抵抗器、30 、
31・・・ツェナーダイオード、32・・・直線化回路
H1力)′/!1.1子、33・・・抵抗器1.4 (
1、41・・入力端子、42・・・第2の定■、正直流
電源の中性点、43・・・出ツルjIA子。
DESCRIPTION OF SYMBOLS 1...Temperature measurement circuit, 6a-1st constant voltage part m1 power supply, 6b...2nd constant voltage 1α flow source, 7...1st operational amplifier circuit, 8...Base 1. t E[Setting button and second operational amplifier circuit for canceling read net effect, 9...Additional 1[
・Hata circuit, 1()... linearization circuit, 11・aP, ]
Operational amplifier, 12...Resistor, ]3...1ill temperature resistance element, 14.15...Resistor 2(), 16, 17.1
8... Lead wire, 19... Second operational amplifier, 20...
...Operation amplifier, 21.22.Resistor, 23..Amplification circuit output terminal, 24..Ground terminal, 25..Operation amplifier, 2F+, 27.28.29..Resistor, 30.
31... Zener diode, 32... Linearization circuit H1 power)'/! 1.1 child, 33...resistor 1.4 (
1, 41...Input terminal, 42...Second constant ■, neutral point of direct current power supply, 43...Output terminal JIA terminal.

特許出願人 日本ランコ株式会行 牛FlF出願代、1里人 弁理」−宵 木    朗 弁理士  西  舘  和  之 弁理士  山  [1昭 之 第2V ゝ′1 第3図 ■ 第4図 ^1Vλ 第50patent applicant Nippon Lanco Co., Ltd. Cattle FlF application fee, 1 ri person ``Patent Attorney'' - Akira Yoiki Patent attorney Kazuyuki Nishi Patent attorney Yama [1 Akira] 2nd V ゝ′1 Figure 3 ■ Figure 4 ^1Vλ 50th

Claims (1)

【特許請求の範囲】[Claims] 演算増幅器の第1入力回路に抵抗およびツェナーダイオ
ードの直列回路を接続し、第2入力回路に直列接続され
た抵抗を設け、該抵抗の直列接続点と接地点との間に別
のツェナーダイオードを接続し、該第1入力回路に接続
された直列回路の該演算増幅器と反対側の一1d4と、
該第2入力回路に設けられた直列抵抗回路の該演算増幅
器と反対側の一端と全接続し入力信号を加えるようにし
、該入力信号供給点と該演は増%、i器の出力端子の間
から出力を取出すようにした直線化回路。
A series circuit of a resistor and a Zener diode is connected to the first input circuit of the operational amplifier, a resistor connected in series is provided to the second input circuit, and another Zener diode is connected between the series connection point of the resistor and the ground point. and one 1d4 on the opposite side of the operational amplifier of the series circuit connected to the first input circuit;
The series resistance circuit provided in the second input circuit is fully connected to one end on the opposite side from the operational amplifier, and an input signal is applied. A linearization circuit that extracts output from between.
JP18309383A 1983-10-03 1983-10-03 Linearizing circuit Granted JPS5985106A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18309383A JPS5985106A (en) 1983-10-03 1983-10-03 Linearizing circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18309383A JPS5985106A (en) 1983-10-03 1983-10-03 Linearizing circuit

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP10279579A Division JPS5932730B2 (en) 1979-08-14 1979-08-14 temperature measurement circuit

Publications (2)

Publication Number Publication Date
JPS5985106A true JPS5985106A (en) 1984-05-17
JPS6350644B2 JPS6350644B2 (en) 1988-10-11

Family

ID=16129636

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18309383A Granted JPS5985106A (en) 1983-10-03 1983-10-03 Linearizing circuit

Country Status (1)

Country Link
JP (1) JPS5985106A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104748877A (en) * 2015-04-08 2015-07-01 深圳市航盛电子股份有限公司 Linear signal collection circuit and system of temperature sensor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104748877A (en) * 2015-04-08 2015-07-01 深圳市航盛电子股份有限公司 Linear signal collection circuit and system of temperature sensor

Also Published As

Publication number Publication date
JPS6350644B2 (en) 1988-10-11

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