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JPS6018943B2 - conductivity meter - Google Patents
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JPS6018943B2 - conductivity meter - Google Patents

conductivity meter

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Publication number
JPS6018943B2
JPS6018943B2 JP4671875A JP4671875A JPS6018943B2 JP S6018943 B2 JPS6018943 B2 JP S6018943B2 JP 4671875 A JP4671875 A JP 4671875A JP 4671875 A JP4671875 A JP 4671875A JP S6018943 B2 JPS6018943 B2 JP S6018943B2
Authority
JP
Japan
Prior art keywords
conductivity
signal
temperature
measured
operational amplifier
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
JP4671875A
Other languages
Japanese (ja)
Other versions
JPS51121393A (en
Inventor
正紀 本間
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.)
Ohkura Electric Co Ltd
Original Assignee
Ohkura Electric Co Ltd
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 Ohkura Electric Co Ltd filed Critical Ohkura Electric Co Ltd
Priority to JP4671875A priority Critical patent/JPS6018943B2/en
Publication of JPS51121393A publication Critical patent/JPS51121393A/en
Publication of JPS6018943B2 publication Critical patent/JPS6018943B2/en
Expired legal-status Critical Current

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  • Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)

Description

【発明の詳細な説明】 この発明は、不純物を含む水溶液の導軍率を測定する導
電率計に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a conductivity meter for measuring the conductivity of an aqueous solution containing impurities.

なお、この明細書では、「導電率」はその逆数て;ある
抵抗率を指す場合にも使用する。一般に、被測定水溶液
の導電率Gは、次式のように純粋の水の電離にもとづく
導電率G.と、それに含まれる不純物(主として塩類)
の電離による導電率G2との和により表わされる。
In this specification, "conductivity" is also used to refer to a certain resistivity as its reciprocal. In general, the conductivity G of an aqueous solution to be measured is calculated based on the ionization of pure water as shown in the following equation. and the impurities it contains (mainly salts)
It is expressed by the sum of the conductivity G2 due to ionization.

G=G,十G2 …・・・・・
・‘1)被測定水溶液の導電率Gは温度によって変化し
、第2図に示すような温度特性を示す。
G=G, 10G2...
・'1) The conductivity G of the aqueous solution to be measured changes depending on the temperature, and exhibits temperature characteristics as shown in FIG.

従って、一般に25つ0を示す換算温度tmにおける被
測定水溶液の導電率をGm、水の電離にもとづく導電率
をG,m、不純物の電離による導電率をG2mとすると
、{1}式はつぎのように書き換えることができる。G
m=G,m十G2m ・・・・・・
・・・■被測定水溶液の導電率Gは、第2図に示すよう
に、温度によって異なった値を示す特性を有するので、
換算温度(一般には25qoを示す)における導篭率G
mに換算して表わされる。
Therefore, if the conductivity of the aqueous solution to be measured at the converted temperature tm, which generally indicates 25 zero, is Gm, the conductivity based on the ionization of water is G,m, and the conductivity due to the ionization of impurities is G2m, the formula {1} is as follows. It can be rewritten as G
m=G, m×G2m ・・・・・・
...■The conductivity G of the aqueous solution to be measured has the characteristic of showing different values depending on the temperature, as shown in Figure 2.
Conduction rate G at converted temperature (generally indicates 25qo)
It is expressed in terms of m.

この換算の際、導電率Gの温度変化分を補正する必要が
あるが、この変化分は非線形のものなので、精度よく補
正することは困難である。ところで、被測定水溶液が有
するある温度t(≠tm)における導電率G2と換算温
度tmにおける導電率G2mとの比を示す係数をaとす
ると、a=憲 .・・.・・.・側となるので
、導電率○2mは G2m=G2手 …‐‐‐…‘41となる。
At the time of this conversion, it is necessary to correct the temperature change in the conductivity G, but since this change is nonlinear, it is difficult to accurately correct it. By the way, if a is a coefficient indicating the ratio of the electrical conductivity G2 at a certain temperature t (≠tm) of the aqueous solution to be measured to the electrical conductivity G2m at the converted temperature tm, then a=conductivity.・・・.・・・. - side, so the conductivity ○2m becomes G2m = G2 hand ...---...'41.

式【1}、‘2)及び【4}から、換算温曳昼mにおけ
る被測定水溶液の導電率GmはGm=言(G−GI)+
GIm ‐……‐‐【51により表わされる。
From formulas [1}, '2) and [4}, the electrical conductivity Gm of the aqueous solution to be measured at the converted temperature daytime m is Gm=G(G-GI)+
Represented by GIm -...--[51.

水の電離にもとづく導電率G,mは予め知ることができ
るので、不純物の導軽率を示す‘5}式の右辺第1項が
その第2項より十分に大きいときは導電率GmはGm=
妻(G−GI) ‐……‐‐‘61と表わすこと
ができる。
Since the electrical conductivity G, m based on the ionization of water can be known in advance, when the first term on the right side of equation '5, which indicates the conductivity of impurities, is sufficiently larger than the second term, the electrical conductivity Gm is Gm=
Wife (G-GI) -...--'61.

更に、被測定水溶液の導電率Gに対して水の電離にもと
づく導電率○,mが無視し得る程度に小さい場合には、
(6}式の導電率Gmは近似的に、Gm=;G
…‐…‐‐‘7’で表わすことができる。
Furthermore, if the conductivity ○, m based on the ionization of water is small enough to be ignored with respect to the conductivity G of the aqueous solution to be measured,
(6) The electrical conductivity Gm in equation (6) is approximately as follows: Gm=;G
...----It can be expressed as '7'.

この発明は、以上述べた点に注目してなされたもので、
イオン化する不純物を含む被測定水溶液が有する任意の
温度及び予め設定された換算温度における導電率間の比
からなる係数の逆数と、被測定水溶液とを掛けることに
よって温度変化率の小さな測定導電率信号を導出すると
共に、この測定導電率信号を上記係数の逆数を掛けた水
の導電率信号及び上記換算温度におよび水の導亀率の少
なくとも一方を用いて補正することによって検出された
上記測定導電率信号を広い温度範囲にわたって精度よく
補正することができる導電率計を提供することを目的と
する。
This invention was made with attention to the points mentioned above.
A measured conductivity signal with a small temperature change rate is obtained by multiplying the measured aqueous solution by the reciprocal of a coefficient consisting of the ratio between the conductivity at an arbitrary temperature and a preset converted temperature of the measured aqueous solution containing ionizable impurities. and correcting the measured conductivity signal using the water conductivity signal multiplied by the reciprocal of the coefficient and at least one of the converted temperature and the conductivity of the water. An object of the present invention is to provide a conductivity meter that can accurately correct a conductivity signal over a wide temperature range.

以下、この発明の一実施例について詳細に説明する。Hereinafter, one embodiment of the present invention will be described in detail.

第1図はこの発明の一実施例として示す導電率計の回路
図であり、【5’式に基づいて構成されている。検出セ
ルDは導電率を測定すべき被測定水溶液中に浸潰された
一対の電極を有し、一方の電極が交流電源1に接続され
、他方の電極が演算増幅器2の第1入力に接続される。
検出セルDは、一対の電極の構造によって定まる定数K
を有する。
FIG. 1 is a circuit diagram of a conductivity meter shown as an embodiment of the present invention, and is constructed based on formula 5'. The detection cell D has a pair of electrodes immersed in the aqueous solution to be measured whose conductivity is to be measured, one electrode is connected to the AC power supply 1 and the other electrode is connected to the first input of the operational amplifier 2. be done.
The detection cell D has a constant K determined by the structure of the pair of electrodes.
has.

いま、rdを被測定水溶液中の検出セルDの抵抗値、G
を被測定水溶液の導電率とすると、定数KはK工rd×
G ………【81により表わ
される。演算増幅器2は第1演算回路として機能するも
ので、第1入力を後述する感温抵抗体4にも接続し、第
2入力を接地しており、ゲイン亭を有する。
Now, rd is the resistance value of the detection cell D in the aqueous solution to be measured, G
When is the conductivity of the aqueous solution to be measured, the constant K is K rd ×
G......[Represented by 81. The operational amplifier 2 functions as a first operational circuit, has a first input connected to a temperature-sensitive resistor 4 to be described later, a second input grounded, and has a gain terminal.

ただし、Gは被測定水溶液の導電率、aは{3ー式で示
すように不純物によるイオンを含む被測定水溶液のある
温度tにおける導電率○2と換算温駒雌ける蛾数mの比
巻‘こ等しし・係数である。演算増幅器2の出力は同期
整流回路3に入力される。
However, G is the electrical conductivity of the aqueous solution to be measured, and a is the ratio of the electrical conductivity ○2 at a certain temperature t of the aqueous solution to be measured containing ions due to impurities to the number m of moths that can be converted into warm-up moths, as shown in equation 3. 'This is the coefficient. The output of the operational amplifier 2 is input to a synchronous rectifier circuit 3.

同期整流回路3は公知のものでよく、例えば第3図に示
すような構成を有する。第3図において、電界効果トラ
ンジスタQ,はスイッチとして機能するもので、演算増
幅器2の出力端にドレィンを接続し、ソースを抵抗R4
を介して同期整流回路3の出力端に接続し、ゲートを信
号源S,に接続している。
The synchronous rectifier circuit 3 may be of a known type, and has a configuration as shown in FIG. 3, for example. In FIG. 3, the field effect transistor Q, functions as a switch, and its drain is connected to the output terminal of the operational amplifier 2, and its source is connected to the resistor R4.
It is connected to the output end of the synchronous rectifier circuit 3 via the synchronous rectifier circuit 3, and its gate is connected to the signal source S.

信号源S,は交流電源1の交流電圧を半波整流し、即ち
交流電圧の正期間の波形を得、更にこの波形を矩形波に
波形変換した1800おきのパルスを発生し、このパル
スを電界効果トランジスタQ,のゲートに印加し、これ
をオン又はオフにする。電界効果トランジスタQ2はド
レィンを演算増幅器2の第1入力に接続し、ソースを電
界効果トランジスタQ.のソースに接続し、ゲートを信
号源S2に接続している。信号源S2は信号源S,と同
一構成を有するが、信号源S,と逆極性のパルスを出力
する。電界効果トランジスタQ2のドレィンとソースと
の間には感温抵抗体4が接続されている。感温抵抗体4
は、例えば固定抵抗とサーミスタとを直列又は並列に接
続し、ある温tにおけるその抵抗値r4と、換算温度t
mとにおけるその抵抗値r靴との比:羊が係数aに等し
くなるょ化選択される。
The signal source S performs half-wave rectification of the AC voltage of the AC power source 1, that is, obtains a waveform of the positive period of the AC voltage, and further converts this waveform into a rectangular wave to generate pulses every 1800, and converts these pulses into an electric field. is applied to the gate of the effect transistor Q, turning it on or off. The field effect transistor Q2 has a drain connected to the first input of the operational amplifier 2, and a source connected to the field effect transistor Q. The gate is connected to the source of the signal source S2, and the gate is connected to the signal source S2. The signal source S2 has the same configuration as the signal source S, but outputs pulses of opposite polarity to the signal source S. A temperature sensitive resistor 4 is connected between the drain and source of the field effect transistor Q2. Temperature sensitive resistor 4
For example, a fixed resistor and a thermistor are connected in series or parallel, and the resistance value r4 at a certain temperature t and the converted temperature t
The ratio of its resistance value r to m: the sheep is selected to be equal to the coefficient a.

即ち、a=羊 .・・.・・.・側 従って、演算増幅器2、同期整流回路3及び感温抵抗体
4からなる演算回路の出力電圧壬3は、交流電源1の電
圧をes、検出セルDの抵抗値をrd、感溢抵抗体4の
抵抗値をr4とすると、e3=−き‐r4
‐‐‐‐‐‐‐‐‐{10により表わされる。
That is, a=sheep.・・・.・・・. Therefore, the output voltage 3 of the arithmetic circuit consisting of the operational amplifier 2, the synchronous rectifier circuit 3, and the temperature-sensitive resistor 4 is expressed as follows: the voltage of the AC power supply 1 is es, the resistance value of the detection cell D is rd, and the overflow-sensitive resistor If the resistance value of 4 is r4, then e3=-ki-r4
----------{10.

従って、(IQ式は、(8}、【9}式を用いると、e
3=−eS‐長‐き−r御 ………(11)(9}式
におけるes、K、r4mの値はそれぞれ測定レンジ、
検出セルD及び感温抵抗体4に固有の値をとり得るので
、(11)式はe3で−きG …仙…(12) となる。
Therefore, (IQ formula is e
3=-eS-long-ki-r control......(11) The values of es, K, and r4m in equation (9) are the measurement range,
Since the detection cell D and the temperature-sensitive resistor 4 can take values specific to the detection cell D and the temperature-sensitive resistor 4, the equation (11) can be expressed as e3.

(12)式はe3を測定すれば、換算温屋耳mにおける
導電率G2mが求められることを示す。なお、m、【2
}、{3’式を用いると、(12)式はe3戊−貴G=
−妻(G.十G2)=−(G2m+葦号こ.)……(1
3) ○2m》G,のときは e3は−G2m …,.,…(14
)となる。
Equation (12) shows that by measuring e3, the electrical conductivity G2m at the converted warm-up m is found. Note that m, [2
}, {Using the 3' formula, the formula (12) becomes e3戊-KiG=
− Wife (G. 10G2) = − (G2m + Ashigoko.)……(1
3) When ○2m》G, e3 is -G2m...,. ,…(14
).

第1図の説明に戻る。Returning to the explanation of FIG.

同期整流回路3の出力は抵抗R3を介して演算増幅器5
の第1入力に供給される。一方、直流電流e,は感温抵
抗体8を介して演算増幅器9の第1入力に接続され、そ
の第2入力は接地されている。
The output of the synchronous rectifier circuit 3 is connected to the operational amplifier 5 via a resistor R3.
is supplied to the first input of. On the other hand, the direct current e is connected to a first input of an operational amplifier 9 via a temperature-sensitive resistor 8, and its second input is grounded.

また、演算増幅器9の出力機は、抵抗R,を介してその
第1入力に接続され、かつ抵抗R2及びスイッチS,を
介して演算増幅器10の第1入力に接続される。ここで
、感温抵抗体8は感温抵抗素子、例えばサーミスタ及び
固定抵抗器を直列又は並列接続して構成され、その抵抗
値r8はaG,m .........(
15)r8=rtm・−a「を満足するように選択され
る。
The output of the operational amplifier 9 is also connected to its first input via a resistor R, and to the first input of an operational amplifier 10 via a resistor R2 and a switch S. Here, the temperature-sensitive resistor 8 is constructed by connecting temperature-sensitive resistive elements such as a thermistor and a fixed resistor in series or in parallel, and its resistance value r8 is aG, m. .. .. .. .. .. .. .. .. (
15) Selected to satisfy r8=rtm・-a.

ただし、rtmは換算温度tmにおけるサーミスタの抵
抗値である。
However, rtm is the resistance value of the thermistor at the converted temperature tm.

演算増幅器10は、第1入力をスイッチS,及び抵抗R
2を介して演算増幅器9の出力三端に接続され、かつス
イッチS2及び抵抗R3を介して直流電源e2に接続し
、第2入力を接地し、出力機を抵抗R7を介して第1入
力及び抵抗R6を介して演算増幅器5の第1入力に接続
されている。
The operational amplifier 10 has a first input connected to a switch S and a resistor R.
2 to the three output terminals of the operational amplifier 9, and is connected to the DC power supply e2 via the switch S2 and resistor R3, the second input is grounded, and the output device is connected to the first input and the output terminal via the resistor R7. It is connected to the first input of the operational amplifier 5 via a resistor R6.

ここで、直流電源e,「感温抵抗体8、抵抗R,及び演
算増幅器9から構成される第1信号発生回路は、演算増
幅器9の出力をe3とすると、(15)式より、e3=
‐e.・黒=‐a誌だ.・…・・(16)(16)式に
おけるR,、r伽、e,は既知の定数であるから(16
)式はe3は−事 ・・‐・‐‐‐・・(1
7)となる。
Here, the first signal generation circuit composed of a DC power supply e, a temperature-sensitive resistor 8, a resistor R, and an operational amplifier 9 has the following equation: If the output of the operational amplifier 9 is e3, then from equation (15), e3=
-e.・Black = -a magazine. ...(16) Since R, , r, and e in equation (16) are known constants, (16
) formula is e3 is - thing ・・・-・---・(1
7).

即ち演算増幅器9はスイッチS,が閉成されてし、ると
歌−鼻こより示される出力e6を抵抗R2及びスイッチ
S,を介して演算増幅器101こ入力する。また、直流
電源e2は第2信号発生回路として機能し、スイッチS
2が閉成されているときはG,mにより示される信号を
抵抗R3及びスイッチS2を介して演算増幅器10に入
力する。
That is, when the switch S of the operational amplifier 9 is closed, the output e6 shown from the nose is inputted to the operational amplifier 101 via the resistor R2 and the switch S. Further, the DC power supply e2 functions as a second signal generation circuit, and the switch S
2 is closed, a signal indicated by G, m is input to the operational amplifier 10 via the resistor R3 and the switch S2.

従って、演算増幅器1川まスイッチS,(又はS2)及
び抵抗R2(又はR3)を介して信号を入力し、反転増
幅するので、事(又‘ま−G・m)はり示される信号地
力する。演算増幅器5は第1入力を抵抗R5,R8及び
R9の一端に接続し、第2入力を接地し、出力端を抵抗
R9の他端に接続し、かつ指示メータ6を介して出力端
子7に接続している。
Therefore, the signal is input through the operational amplifier 1, switch S, (or S2) and resistor R2 (or R3), and is inverted and amplified. . The operational amplifier 5 has a first input connected to one end of the resistors R5, R8 and R9, a second input connected to ground, an output end connected to the other end of the resistor R9, and an output terminal 7 via the indicator meter 6. Connected.

出力端子7は抵抗R.oを介して接地される。測定にお
いて、例えばスイッチS,およびS2の両者をオンに設
定したときは、演算増幅器5の出力は{5)式を満足す
る演算が実行される。
Output terminal 7 is connected to resistor R. grounded via o. In the measurement, for example, when both switches S and S2 are set to ON, the output of the operational amplifier 5 is calculated to satisfy the equation {5).

また、被測定水溶液における不純物の導電率が大きいと
きはスイッチS,のみをオンにすることができるので、
このときは、演算増幅器5の出力は(6}式を満足する
ものとなる。更に、水の導電率G,mも無視できるとき
はスイッチS,およびS2をオフにすることができ、こ
のときは、演算増幅器5の出力は‘7ー式を満足する演
算が実行される。このように演算増幅器5は、第2演算
回路として被測定水溶液の導電率Gを関数とし、−きG
により示される信財抵抗R5を介し、また号、G.m又
‘ま(事−G.m)、事刈o‘こ小武れる信号を抵抗虫
8を介して入力し、反転した両者の和、即ち{動、‘6
ー又は【7ー式により示される演算をしてGmにより示
される信号を指示メータ6を介して出力端子7に供給す
る。
In addition, when the conductivity of impurities in the aqueous solution to be measured is high, only switch S can be turned on.
At this time, the output of the operational amplifier 5 satisfies equation (6).Furthermore, when the conductivity G and m of water can also be ignored, the switches S and S2 can be turned off; The output of the operational amplifier 5 is calculated to satisfy the formula '7-.In this way, the operational amplifier 5 functions as a function of the conductivity G of the aqueous solution to be measured as a second calculation circuit, and the output of the operational amplifier 5 is calculated as follows.
Through the credit resistance R5 indicated by G. Input the mata'ma (koto-G.m), kokotogari o'ko small signal through the resistor insect 8, and invert the sum of both, that is, {movement, '6
- or [7-] and supplies the signal indicated by Gm to the output terminal 7 via the indicator meter 6.

出力端子7の信号は、補正された被測定水溶液の導電率
を示す信号である。なお、感温抵抗体4及び8を礎成す
るサーミスタは、一般に定数Bにより評価され、次式の
ような関係式により示されることが知られている。
The signal at the output terminal 7 is a signal indicating the corrected conductivity of the aqueous solution to be measured. Note that it is known that the thermistors that form the basis of the temperature-sensitive resistors 4 and 8 are generally evaluated by a constant B, and are expressed by the following relational expression.

R=RoeXPB(壬−≠) ‐‐…‐‐‐‐(18
)ただし、Bは温度TKにおけるサーミスタの抵抗値、
R。は温度Toにおけるサーミスタの抵抗値である。従
って、定数Bはとなり、通常300血〜400皿程度の
値をとる。
R=RoeXPB(壬-≠) ‐‐…‐‐‐‐(18
) However, B is the resistance value of the thermistor at temperature TK,
R. is the resistance value of the thermistor at temperature To. Therefore, the constant B is, and usually takes a value of about 300 to 400 blood dishes.

以上のように、この発明によれば、温度変化に対して導
電率の信号の変化が小さくなるように測定信号に対して
係数を掛けて補正を行なうようにしたので、被測定水溶
液が温度変化の大きなものであっても広い温度範囲にわ
たって導電率の測定精度を高く保つことができ、またこ
のような係数を得るための感溢抵抗体は製造が容易なも
のであり、そのコストも低いので、経済的な装置とする
ことができる。
As described above, according to the present invention, since the measurement signal is multiplied by a coefficient and corrected so that the change in the conductivity signal becomes small with respect to temperature change, the aqueous solution to be measured is Even if the coefficient is large, it is possible to maintain high conductivity measurement accuracy over a wide temperature range, and the sensitive resistor used to obtain such a coefficient is easy to manufacture and its cost is low. , it can be an economical device.

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

第1図はこの発明の一実施例による導電率計の回路図、
第2図は被測定液の導電率の温度特性を示す特性図、第
3図は第1図に示す同期整流回路の回路図である。 1・・・・・・交流電源、2,5,9,10・・・・・
・演算増幅器、3・・・…同期整流回路、4,8・・…
・感温抵抗体、6……指示メータ、D……検出セル、e
,,e2’es・・・・・・直流電源。 第1図 第2図 第3図
FIG. 1 is a circuit diagram of a conductivity meter according to an embodiment of the present invention.
FIG. 2 is a characteristic diagram showing the temperature characteristics of the conductivity of the liquid to be measured, and FIG. 3 is a circuit diagram of the synchronous rectifier circuit shown in FIG. 1. 1... AC power supply, 2, 5, 9, 10...
・Operation amplifier, 3...Synchronous rectifier circuit, 4, 8...
・Temperature-sensitive resistor, 6... Indication meter, D... Detection cell, e
,,e2'es...DC power supply. Figure 1 Figure 2 Figure 3

Claims (1)

【特許請求の範囲】[Claims] 1 導電率Gmを測定対象とした水溶液中に浸漬されて
上記導電率を測定するための電圧が印加される一対の電
極を有し、上記電極を介する上記電圧を検出信号Gとし
た検出器Dと、予め設定される換算温度tm及びこの換
算温度と異なる任意の温度tにおける上記被測定対象の
導電率間の比により定められる係数1/aを上記検出信
号Gに対して掛算する第1演算回路2,3,4と、純粋
な水の基準導電率G_1に上記係数を掛けた値(G_1
)/aをもつ第1補正信号を発生する第1信号発生回路
8,9,R_1と、上記換算温度における上記測定対象
中の水の導電率G_1mに対応した第2補正信号を発生
する第2信号発生回路e_2と、上記第1及び第2信号
発生回路から出力される上記第1及び第2補正信号の少
なくとも一方を選択するスイツチ回路S_1,S_2と
、上記第1演算回路の出力信号と上記スイツチ回路の出
力信号とを加算する第2演算回路R_5,R_8,R_
9,5とを備え、上記第2演算回路の出力信号を上記測
定対象の導電率を示す測定信号とした導電率計。
1 Detector D having a pair of electrodes to which a voltage is applied for measuring the conductivity by being immersed in an aqueous solution whose conductivity Gm is to be measured, and using the voltage passed through the electrodes as a detection signal G. and a first calculation in which the detection signal G is multiplied by a coefficient 1/a determined by the ratio between the conductivity of the object to be measured at a preset converted temperature tm and an arbitrary temperature t different from this converted temperature. Circuits 2, 3, 4 and the value obtained by multiplying the standard conductivity G_1 of pure water by the above coefficient (G_1
)/a, and a second signal generating circuit that generates a second correction signal corresponding to the conductivity G_1m of water in the measurement object at the converted temperature. A signal generation circuit e_2, a switch circuit S_1, S_2 that selects at least one of the first and second correction signals outputted from the first and second signal generation circuits, and an output signal of the first arithmetic circuit and the above. Second arithmetic circuit R_5, R_8, R_ which adds the output signal of the switch circuit
9 and 5, wherein the output signal of the second arithmetic circuit is used as a measurement signal indicating the conductivity of the object to be measured.
JP4671875A 1975-04-17 1975-04-17 conductivity meter Expired JPS6018943B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4671875A JPS6018943B2 (en) 1975-04-17 1975-04-17 conductivity meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4671875A JPS6018943B2 (en) 1975-04-17 1975-04-17 conductivity meter

Publications (2)

Publication Number Publication Date
JPS51121393A JPS51121393A (en) 1976-10-23
JPS6018943B2 true JPS6018943B2 (en) 1985-05-13

Family

ID=12755112

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4671875A Expired JPS6018943B2 (en) 1975-04-17 1975-04-17 conductivity meter

Country Status (1)

Country Link
JP (1) JPS6018943B2 (en)

Also Published As

Publication number Publication date
JPS51121393A (en) 1976-10-23

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