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JPS6212860B2 - - Google Patents
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JPS6212860B2 - - Google Patents

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Publication number
JPS6212860B2
JPS6212860B2 JP14111779A JP14111779A JPS6212860B2 JP S6212860 B2 JPS6212860 B2 JP S6212860B2 JP 14111779 A JP14111779 A JP 14111779A JP 14111779 A JP14111779 A JP 14111779A JP S6212860 B2 JPS6212860 B2 JP S6212860B2
Authority
JP
Japan
Prior art keywords
circuit
voltage
output
oscillation
isolation transformer
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
JP14111779A
Other languages
Japanese (ja)
Other versions
JPS5664663A (en
Inventor
Shoichi Nishikawa
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.)
DKK TOA Corp
Original Assignee
DKK 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 DKK Corp filed Critical DKK Corp
Priority to JP14111779A priority Critical patent/JPS5664663A/en
Publication of JPS5664663A publication Critical patent/JPS5664663A/en
Publication of JPS6212860B2 publication Critical patent/JPS6212860B2/ja
Granted legal-status Critical Current

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  • Arrangements For Transmission Of Measured Signals (AREA)
  • Measurement Of Resistance Or Impedance (AREA)
  • Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)

Description

【発明の詳細な説明】 本発明は、溶液導電率の測定装置に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an apparatus for measuring solution conductivity.

溶液導電率の検出器を現場(送信側)に設置
し、この検出器の検出信号を遠隔地点に設けた受
信側の指示又は記録計に伝送する場合、従来は送
信側及び受信側間を四線式伝送線路を以て接続
し、その中の二線によつて送信側回路の作動電力
を受信側から供給し、他の二線によつて送信側の
検出信号を受信側に伝送するように構成したもの
が最も普通に用いられているが、線路構成が複雑
となるを免れ得ない。
When a solution conductivity detector is installed on-site (transmitting side) and the detection signal of this detector is transmitted to an indicator or recorder on the receiving side installed at a remote location, conventionally, the distance between the transmitting side and the receiving side is four-way. Connected by a wire transmission line, two wires of which supply the operating power of the transmitting circuit from the receiving side, and the other two wires transmit the detection signal from the transmitting side to the receiving side. is the most commonly used, but the line configuration is unavoidably complicated.

このため送信側及び受信側間を二線式伝送線路
を以て接続し、作動電力の供給と検出信号の伝送
に兼用することにより線路構成を簡潔ならしめた
ものが提案実施されているが、送信側回路の入出
力間が直流的に絶縁されていないため、送信側及
び受信側の各回路を独立に接地することが不可能
で、したがつて各回路を安定に作動せしめること
が困難である。
For this reason, a proposal has been made to simplify the line configuration by connecting the transmitting side and the receiving side with a two-wire transmission line, which is used for both supplying operating power and transmitting detection signals. Since there is no DC insulation between the input and output of the circuit, it is impossible to ground each circuit on the transmitting side and the receiving side independently, and therefore it is difficult to operate each circuit stably.

本発明は、送信側及び受信側間を二線式伝送線
路を以て接続し、作動電力の供給と検出信号の伝
送に兼用することにより線路構成を簡潔ならしめ
ると共に送信側回路の入出力間を直流的に絶縁す
ることにより送信側及び受信側の各回路を各別に
接地して作動を安定ならしめ得る溶液導電率測定
装置を実現することを目的とする。
The present invention connects the transmitting side and the receiving side with a two-wire transmission line, which is used for both supplying operating power and transmitting detection signals, simplifying the line configuration, and connecting the input and output of the transmitting side circuit with a two-wire transmission line. The purpose of the present invention is to realize a solution conductivity measuring device that can stabilize operation by separately grounding each circuit on the transmitting side and the receiving side by insulating the circuits.

図は、本発明の一実施例を示す図で、Q1は矩
形波発振回路を形成する演算増幅器、Q2は電界
効果トランジスタ、Z1はツエナダイオード、C
1は直流阻止用コンデンサ、Q3はインピーダン
ス変換用演算増幅器、CEは導電率測定用セル
で、セル内に被測定液の導電率測定用電極を設け
てある。Q4は交流増幅用演算増幅器、T1は絶
縁トランス、Q5は例えば理想化ダイオード回路
のような整流回路を形成する演算増幅器、R1及
びC2はフイルタFを形成する抵抗及びコンデン
サ、Q6は温度補償回路を形成する演算増幅器
で、その帰還回路に挿入される温度補償素子(例
えばサーミスタ)RTは導電率測定用セルCE内に
取付けてある。Q7はトランジスタQ8及びQ9
と共に電圧・電流変換回路を形成する演算増幅
器、Z2はツエナダイオード、Q10は起動用電
界効果トランジスタ、RSはスパン調整用可変抵
抗、RZは零調整用可変抵抗、RFは帰還抵抗、
RCは演算抵抗、R2及びR3は分圧抵抗、Q1
1は加算回路を形成する演算増幅器、Q12及び
Q13は発振回路を形成するインバータ、Q14
はバツフア用インバータ、T2は絶縁トランス、
D1,D2及びD3は整流素子、C3ないしC5
は平滑コンデンサ、+E1及び+E2は正側作動
電圧供給端子、−E1及び−E2は負側作動電圧
供給端子、Lは二線式伝送線路、ESは直流電
源、RDは受信装置で、指示又は記録計より成
る。尚、演算増幅器Q1,Q3ないしQ7及びQ
11は、例えば消費電力の小なるマイクロパワー
演算増幅器を以つて形成し、インバータQ12な
いしQ14は、例えばCMOSインバータを以つて
形成する。
The figure shows an embodiment of the present invention, in which Q1 is an operational amplifier forming a rectangular wave oscillation circuit, Q2 is a field effect transistor, Z1 is a Zener diode, and C
1 is a DC blocking capacitor, Q3 is an operational amplifier for impedance conversion, and CE is a cell for measuring conductivity, in which an electrode for measuring the conductivity of the liquid to be measured is provided. Q4 is an operational amplifier for AC amplification, T1 is an isolation transformer, Q5 is an operational amplifier forming a rectifier circuit such as an idealized diode circuit, R1 and C2 are resistors and capacitors forming filter F, and Q6 is a temperature compensation circuit. A temperature compensation element (for example, a thermistor) RT inserted into the feedback circuit of the operational amplifier formed is installed in the conductivity measurement cell CE. Q7 is transistor Q8 and Q9
Z2 is a Zener diode, Q10 is a starting field effect transistor, RS is a variable resistor for span adjustment, RZ is a variable resistor for zero adjustment, RF is a feedback resistor,
RC is a calculation resistor, R2 and R3 are voltage dividing resistors, Q1
1 is an operational amplifier forming an adder circuit, Q12 and Q13 are inverters forming an oscillation circuit, Q14
is a buffer inverter, T2 is an isolation transformer,
D1, D2 and D3 are rectifying elements, C3 to C5
is a smoothing capacitor, +E1 and +E2 are positive operating voltage supply terminals, -E1 and -E2 are negative operating voltage supply terminals, L is a two-wire transmission line, ES is a DC power supply, and RD is a receiving device for indicating or recording. Consists of total. In addition, operational amplifiers Q1, Q3 to Q7 and Q
11 is formed using, for example, a micropower operational amplifier with low power consumption, and inverters Q12 to Q14 are formed using, for example, CMOS inverters.

受信側の直流電源ESを線路Lを介して送信側
回路に接続すると、ツエナダイオードZ2の一端
に接続された端子+E2から定電圧化された正側
作動電圧が取出され、絶縁トランスT2の一次巻
線電流が整流素子D1で整流されて得られる負側
作動電圧が端子−E2から取出される。この作動
電圧によりインバータQ12及びQ13より成る
発振回路が作動し、その発振出力がバツフア用イ
ンバータQ14を介して絶縁トランスT2の一次
巻線に加えられ、二次側出力が整流素子D2及び
D3並に平滑コンデンサC4及びC5により整流
平滑され、端子+E1及び−E1から正負の作動
電圧として取出される。この作動電圧によつて演
算増幅器Q1から成る発振回路が発振し、その矩
形波発振出力が電界効果トランジスタQ2のゲー
トに加えられ、ツエナダイオードZ1の一定電圧
をQ2によつて断続せしめる。したがつて電界効
果トランジスタQ2のドレーン及びソースから演
算増幅器Q1の発振出力の周期に等しく振幅の安
定な半波の矩形波信号が取出され、直流阻止用コ
ンデンサC1及びインピーダンス変換用演算増幅
器Q3を介して導電率測定用セルCEの電極に加
えられる。演算増幅器Q4の交流出力はセルCE
に内装された電極間に介在する被測定液の導電率
に比例したものとなり、絶縁トランスT1を介し
て演算増幅器Q5から成る整流回路に加えられて
整流され、フイルタFを介して演算増幅器Q6か
ら成る温度補償回路に加えられ、被測定液の温度
変化に基づく導電率の変化分が補償された後、ス
パン調整用可変抵抗RS、演算増幅器Q7及びト
ランジスタQ8を介してトランジスタQ9のベー
スに加えられる。したがつてトランジスタQ9の
コレクタ電流、即ち伝送線路Lに流れる電流が演
算増幅器Q7の出力電圧に応じて変化し、受信装
置RDの指示又は記録計に被測定液の導電率が指
示又は記録される。
When the receiving side DC power supply ES is connected to the transmitting side circuit via the line L, the regulated positive working voltage is taken out from the terminal +E2 connected to one end of the Zener diode Z2, and the primary winding of the isolation transformer T2 A negative side operating voltage obtained by rectifying the line current with the rectifying element D1 is taken out from the terminal -E2. This operating voltage activates an oscillation circuit consisting of inverters Q12 and Q13, and its oscillation output is applied to the primary winding of isolation transformer T2 via buffer inverter Q14, and the secondary output is applied to rectifiers D2 and D3 as well as It is rectified and smoothed by smoothing capacitors C4 and C5, and taken out as positive and negative operating voltages from terminals +E1 and -E1. This operating voltage causes an oscillation circuit consisting of operational amplifier Q1 to oscillate, and its rectangular wave oscillation output is applied to the gate of field effect transistor Q2, causing the constant voltage of Zener diode Z1 to be interrupted by Q2. Therefore, a stable half-wave rectangular wave signal with an amplitude equal to the period of the oscillation output of the operational amplifier Q1 is extracted from the drain and source of the field effect transistor Q2, and is passed through the DC blocking capacitor C1 and the impedance conversion operational amplifier Q3. is added to the electrode of the conductivity measurement cell CE. The AC output of operational amplifier Q4 is connected to cell CE.
The conductivity of the liquid to be measured is proportional to the conductivity of the liquid to be measured interposed between the electrodes installed in the , and is rectified by being applied to a rectifier circuit consisting of an operational amplifier Q5 via an isolation transformer T1. After compensating for changes in conductivity due to temperature changes in the liquid to be measured, it is applied to the base of transistor Q9 via variable resistor RS for span adjustment, operational amplifier Q7, and transistor Q8. . Therefore, the collector current of the transistor Q9, that is, the current flowing through the transmission line L, changes depending on the output voltage of the operational amplifier Q7, and the conductivity of the liquid to be measured is indicated or recorded by the receiving device RD or by the recorder. .

そしてスパン調整用可変抵抗RS及び零調整用
可変抵抗RZを調整することにより被測定液の導
電率の変化に対応する線路Lの電流の変化を例え
ば4mAから20mAの範囲に制限することが出来
る。
By adjusting the span adjustment variable resistor RS and the zero adjustment variable resistor RZ, it is possible to limit the change in the current of the line L corresponding to the change in the conductivity of the liquid to be measured to a range of, for example, 4 mA to 20 mA.

尚、トランジスタQ9のコレクタ回路に挿入し
た帰還抵抗RFにおける電圧降下が演算抵抗RCを
介して演算増幅器Q7の非反転入力端子に負帰還
せしめられ、電圧・電流変換動作が極めて安定に
行われる。
Note that the voltage drop across the feedback resistor RF inserted in the collector circuit of the transistor Q9 is negatively fed back to the non-inverting input terminal of the operational amplifier Q7 via the operational resistor RC, so that the voltage/current conversion operation is performed extremely stably.

又、端子+E1及び−E1の作動電圧は測定用
セルCE内における被測定液の抵抗値に比例して
変動し、例えば被測定液の抵抗値が低い場合には
端子+E1及び−E1の電圧も下ろうとするが、
この場合にはトランジスタQ9のコレクタ電流が
増加して帰還抵抗RFにおける電圧降下が大とな
り、この電圧降下が分圧抵抗R2及びR3の分電
圧、即ち端子+E2の電圧の分電圧と演算増幅器
Q11で加算されてインバータQ12及びQ13
より成る発振回路の作動電圧として供給され、端
子+E1及び−E1の電圧を高めるように作動す
るので、被測定液の抵抗値の高低に関係なく常に
正確な測定が可能となる。
In addition, the operating voltages of terminals +E1 and -E1 vary in proportion to the resistance value of the liquid to be measured in the measurement cell CE. For example, when the resistance value of the liquid to be measured is low, the voltages of terminals +E1 and -E1 also change. I try to go down, but
In this case, the collector current of the transistor Q9 increases and the voltage drop across the feedback resistor RF becomes large, and this voltage drop is divided between the voltage divided by the voltage dividing resistors R2 and R3, that is, the voltage divided by the voltage at the terminal +E2, and the operational amplifier Q11. Added to inverters Q12 and Q13
Since the voltage is supplied as the operating voltage of the oscillation circuit consisting of the oscillator circuit and operates to increase the voltages of the terminals +E1 and -E1, accurate measurement is always possible regardless of the resistance value of the liquid to be measured.

尚、本発明装置における入出力関係を数式を以
て示すと次式の通りである。
The input/output relationship in the device of the present invention is expressed numerically as follows.

Io=1/RF(K・E1/CRC/RSRT・K+E2
/RZ) 但し、 Io:線路Lの電流 RF:帰還抵抗RFの抵抗値 K :定数 E :演算増幅器Q3の出力電圧 C :測定用セルCEのセル定数 RC:演算抵抗RCの抵抗値 RS:スパン調整用可変抵抗RSの抵抗値 RT:温度補償素子RTの抵抗値 K :被測定液の導電率 E2:端子+E2の作動電圧 RZ:零調整用可変抵抗RZの抵抗値 以上の説明から明らかなように、本発明は、二
線式伝送線路を作動電力の供給と検出信号の伝送
に兼用することにより線路構成を簡潔ならしめる
と共に送信側の入出力間を絶縁トランスによつて
直流的に絶縁することにより送信側及び受信側回
路を各別に接地して作動を安定ならしめることが
出来、更にインバータQ12及びQ13から成る
発振回路の発振出力電圧を被測定液の抵抗値の高
低に応じて変化せしめることにより被測定液の抵
抗値(即ち導電率)測定回路の作動電圧を一定に
保持して常に正確な測定を行い得るように構成し
たもので、その効果甚だ大である。
Io=1/RF(K・E1/CRC/RSRT・K+E2
/RZ) However, Io: Current in line L RF: Resistance value of feedback resistor RF K: Constant E: Output voltage of operational amplifier Q3 C: Cell constant of measurement cell CE RC: Resistance value of operational resistor RC RS: Span Resistance value of variable resistor RS for adjustment RT: Resistance value of temperature compensation element RT K: Conductivity of liquid to be measured E2: Operating voltage of terminal + E2 RZ: Resistance value of variable resistor RZ for zero adjustment As is clear from the above explanation In addition, the present invention simplifies the line configuration by using a two-wire transmission line for both supplying operating power and transmitting detection signals, and also provides direct current isolation between input and output on the transmitting side using an isolation transformer. This makes it possible to stabilize the operation by separately grounding the transmitter and receiver circuits, and also to change the oscillation output voltage of the oscillation circuit consisting of inverters Q12 and Q13 according to the resistance value of the liquid to be measured. Therefore, the operating voltage of the resistance value (i.e., conductivity) measurement circuit of the liquid to be measured is held constant to ensure accurate measurement at all times, which is extremely effective.

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

図は、本発明の一実施例を示す図で、Q1,Q
3ないしQ7及びQ11:演算増幅器、Q2及び
Q10:電界効果トランジスタ、Z1及びZ2:
ツエナダイオード、C1ないしC5:コンデン
サ、CE:導電率測定用セル、T1及びT2:絶
縁トランス、R1ないしR3:抵抗、RT:温度
補償素子、Q8及Q9:トランジスタ、RS及び
RZ:可変抵抗、RF:帰還抵抗、RC:演算抵
抗、Q12ないしQ14:インバータ、D1ない
しD3:整流素子、+E1,−E1,+E2及び−
E2:作動電圧供給端子、L:伝送線路、ES:
直流電源、RD:受信装置である。
The figure shows one embodiment of the present invention, and Q1, Q
3 to Q7 and Q11: operational amplifier, Q2 and Q10: field effect transistor, Z1 and Z2:
Zener diode, C1 to C5: capacitor, CE: conductivity measurement cell, T1 and T2: isolation transformer, R1 to R3: resistor, RT: temperature compensation element, Q8 and Q9: transistor, RS and
RZ: variable resistor, RF: feedback resistor, RC: operational resistor, Q12 to Q14: inverter, D1 to D3: rectifier, +E1, -E1, +E2 and -
E2: Operating voltage supply terminal, L: Transmission line, ES:
DC power supply, RD: Receiving device.

Claims (1)

【特許請求の範囲】[Claims] 1 溶液導電率測定用セルに内装された導電率測
定電極に出力を加える第1の発振回路と、前記導
電率測定電極間に介在する被測定液の導電率に対
応する出力を送出する交流増幅器と、第1の絶縁
トランスを介して前記交流増幅器出力の導入され
る整流回路と、温度補償回路を介して前記整流回
路出力の導入される電圧・電流変換回路と、この
電圧・電流変換回路の出力側に指示又は記録計よ
り成る受信装置及び直流電源を直列に接続する二
線式伝送線路と、第2の発振回路と、前記電圧・
電流変換回路の出力側に挿入されたツエナダイオ
ードの両端電圧を前記整流回路、温度補償回路、
電圧・電流変換回路及び第2の発振回路の正側作
動電圧として供給する回路と、前記電圧・電流変
換回路の出力側に挿入された抵抗における電圧降
下に応じて前記第2の発振回路の作動電圧を制御
する回路と、前記第2の発振回路出力の加えられ
る第2の絶縁トランスと、この第2の絶縁トラン
スの一次巻線電流を整流して前記整流回路、温度
補償回路、電圧・電流変換回路及び第2の発振回
路の負側作動電圧として供給する回路と、前記第
2の絶縁トランスの二次側出力を正負の極性毎に
整流して前記第1の発振回路及び交流増幅器の正
負の作動電圧として供給する回路とより成ること
を特徴とする溶液導電率測定装置。
1. A first oscillation circuit that applies an output to a conductivity measurement electrode installed in a solution conductivity measurement cell, and an AC amplifier that sends out an output corresponding to the conductivity of the liquid to be measured interposed between the conductivity measurement electrodes. a rectifier circuit into which the output of the AC amplifier is introduced via a first isolation transformer; a voltage/current conversion circuit into which the output of the rectification circuit is introduced via a temperature compensation circuit; a two-wire transmission line connecting in series a receiving device consisting of an indicator or recorder and a DC power supply on the output side; a second oscillation circuit;
The voltage across the Zener diode inserted on the output side of the current conversion circuit is converted into the rectifier circuit, the temperature compensation circuit,
A circuit that supplies a positive operating voltage to a voltage/current conversion circuit and a second oscillation circuit, and operation of the second oscillation circuit in response to a voltage drop across a resistor inserted on the output side of the voltage/current conversion circuit. a circuit for controlling voltage; a second isolation transformer to which the output of the second oscillation circuit is applied; and a circuit for rectifying the primary winding current of the second isolation transformer to connect the rectifier circuit, temperature compensation circuit, voltage/current A circuit that supplies the negative side operating voltage of the conversion circuit and the second oscillation circuit, and a circuit that rectifies the secondary side output of the second isolation transformer for each positive and negative polarity to supply the positive and negative operating voltage of the first oscillation circuit and the AC amplifier. A solution conductivity measurement device characterized by comprising a circuit for supplying an operating voltage.
JP14111779A 1979-10-31 1979-10-31 Solution electric conductivity measuring system Granted JPS5664663A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14111779A JPS5664663A (en) 1979-10-31 1979-10-31 Solution electric conductivity measuring system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14111779A JPS5664663A (en) 1979-10-31 1979-10-31 Solution electric conductivity measuring system

Publications (2)

Publication Number Publication Date
JPS5664663A JPS5664663A (en) 1981-06-01
JPS6212860B2 true JPS6212860B2 (en) 1987-03-20

Family

ID=15284546

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14111779A Granted JPS5664663A (en) 1979-10-31 1979-10-31 Solution electric conductivity measuring system

Country Status (1)

Country Link
JP (1) JPS5664663A (en)

Also Published As

Publication number Publication date
JPS5664663A (en) 1981-06-01

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