JPH035899Y2 - - Google Patents
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- Publication number
- JPH035899Y2 JPH035899Y2 JP9821182U JP9821182U JPH035899Y2 JP H035899 Y2 JPH035899 Y2 JP H035899Y2 JP 9821182 U JP9821182 U JP 9821182U JP 9821182 U JP9821182 U JP 9821182U JP H035899 Y2 JPH035899 Y2 JP H035899Y2
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- JP
- Japan
- Prior art keywords
- resistor
- detection device
- capacitance
- change
- voltage
- 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.)
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- Measurement Of Resistance Or Impedance (AREA)
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
Description
【考案の詳細な説明】
本考案は溶液(例えば食塩水)の濃度変化を検
知する装置に関し、特にその溶液のインピーダン
ス変化に基づいて濃度変化を検知する装置に関す
るものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for detecting a change in concentration of a solution (eg, saline solution), and more particularly to a device for detecting a change in concentration based on a change in impedance of the solution.
第1図は従来の溶液の濃度変化検知回路を示し
ており、図中、1は矩形波発振器、2及び3は電
極、4は円筒形の容器、5は溶液、6は抵抗器、
7は増幅・検波装置、そして8は出力計である。 FIG. 1 shows a conventional solution concentration change detection circuit, in which 1 is a square wave oscillator, 2 and 3 are electrodes, 4 is a cylindrical container, 5 is a solution, 6 is a resistor,
7 is an amplification/detection device, and 8 is an output meter.
第2図は増幅・検波装置7の入力側における等
価回路を示しており、C1及びR1は、それぞれ電
極2−3間の静電容量及び抵抗値を示し、R2は
抵抗器6の抵抗値を示す。 FIG. 2 shows an equivalent circuit on the input side of the amplification/detection device 7, where C 1 and R 1 represent the capacitance and resistance value between the electrodes 2 and 3, respectively, and R 2 represents the resistance value of the resistor 6. Indicates resistance value.
第3図は第1図の従来装置に関する波形を示す
図で、第3図aは矩形波発振器1のパルス電圧波
形で、このパルスが図示の通り両極性(交流)を
有しているのは溶液が電気分解を起こして片方の
電極に特定の物質が集まるのを防ぐためである。
第3図bは抵抗器6の両端電圧、すなわち増幅・
検波装置7の入力電圧、の波形を示している。図
示の通り、電極間容量C1の影響で抵抗器6の両
端電圧波形は前縁部分が後縁部分に比べて少し大
きくなつている。すなわち、容量C1が充電され
て行くに従つて抵抗器6の両端電圧は、抵抗値
R1とR2とで決まる電流値(1/R1+R2×E(入力電
圧))に抵抗値R2を乗じた電圧値(E×R2/R1+R2)
に向かつて低下し、発振器1からの矩形波の周期
に従つて後縁部分で図示の如く反転する。第3図
cは、第3図bよりも濃度が高い場合の抵抗器6
の両端電圧波形を示しており、濃度が高くなつた
ことは第2図の等価回路においては静電容量C1
が大きくなり、抵抗値R1が減少した場合に相当
する。第3図cの場合も静電容量C1の影響で前
縁部分が後縁部分に比べて大きくなるが、静電容
量C1が大きくなり、抵抗値R1が小さくなる結果、
抵抗器6の両端電圧(E×R2/R1+R2)は図示の如
く第3図bの場合より高く立ち上がり且つ、充電
波形は第3図bの場合より緩やかになる。 FIG. 3 is a diagram showing waveforms related to the conventional device shown in FIG. 1, and FIG. This is to prevent specific substances from collecting on one electrode due to electrolysis of the solution.
Figure 3b shows the voltage across the resistor 6, that is, the amplification voltage.
The waveform of the input voltage of the detection device 7 is shown. As shown in the figure, due to the influence of the interelectrode capacitance C 1 , the voltage waveform across the resistor 6 is slightly larger at the leading edge than at the trailing edge. In other words, as the capacitor C1 is charged, the voltage across the resistor 6 changes to the resistance value.
The current value (1/R 1 + R 2 × E (input voltage)) determined by R 1 and R 2 decreases toward the voltage value (E × R 2 /R 1 + R 2 ) multiplied by the resistance value R 2 . , is inverted at the trailing edge as shown in the figure according to the period of the rectangular wave from the oscillator 1. Figure 3c shows the resistor 6 when the concentration is higher than that in Figure 3b.
In the equivalent circuit of Figure 2, the increase in concentration means that the capacitance C 1
This corresponds to a case where the resistance value R 1 decreases as the resistance value R 1 increases. In the case of Fig. 3c, the leading edge becomes larger than the trailing edge due to the effect of capacitance C1 , but as a result of the capacitance C1 becoming larger and the resistance value R1 becoming smaller,
As shown, the voltage across the resistor 6 (ExR 2 /R 1 +R 2 ) rises higher than in the case of FIG. 3b, and the charging waveform becomes gentler than in the case of FIG. 3b.
一方、増幅・検波装置7は入力波形を増幅し半
波整流をするのであるが入力電圧のピーク値に比
例した電圧を出力し出力計8を振らせるものであ
る。従つて濃度が変化した場合の抵抗器6の両端
電圧の変化は、平均値同士の変化よりもピーク値
同士の変化の方が小さくなつて居れば、濃度変化
が出力計8に与える変化も小さくなり、これを大
きくするためには増幅・検波装置7に所要部品を
付加せねばならず高価になるという欠点があつ
た。 On the other hand, the amplification/detection device 7 amplifies the input waveform and performs half-wave rectification, and outputs a voltage proportional to the peak value of the input voltage, causing the output meter 8 to swing. Therefore, if the change in the voltage across the resistor 6 when the concentration changes is smaller between peak values than the change between average values, then the change in concentration will have a smaller effect on the output meter 8. However, in order to increase this size, necessary parts must be added to the amplification/detection device 7, which has the drawback of increasing the cost.
従つて、本考案の目的は、実質的に高価にする
ことなく濃度変化すなわちインピーダンス変化の
検知感度を向上させた溶液の濃度変化検知装置を
提供することである。 SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a solution concentration change detection device that improves the detection sensitivity of concentration changes, that is, impedance changes, without increasing the cost substantially.
この目的を達成するため、本考案は、溶液中に
隔離配置された電極対と、該電極対に抵抗器を介
して直列接続された矩形波発振器と、前記抵抗器
の両端電圧を増幅・検波するため同抵抗器に接続
され、同抵抗器からの入力電圧のピーク値に比例
した電圧を出力する増幅・検波装置と、該増幅・
検波装置に接続された出力計とを備えた溶液の濃
度変化検知装置において、前記抵抗器と並列に所
定容量のコンデンサを接続すると共に、前記所定
容量C2、前記電極間の静電容量をC1、前記電極
間の抵抗値をR1、前記抵抗器の抵抗値をR2とす
る時、前記所定容量C2がC1R1≧C2R2の関係にあ
ることを特徴とするものである。 In order to achieve this objective, the present invention includes a pair of electrodes arranged in isolation in a solution, a rectangular wave oscillator connected in series to the pair of electrodes via a resistor, and amplifying and detecting the voltage across the resistor. an amplification/detection device connected to the resistor to output a voltage proportional to the peak value of the input voltage from the resistor;
In a solution concentration change detection device equipped with an output meter connected to a detection device, a capacitor of a predetermined capacitance is connected in parallel with the resistor, and the predetermined capacitance C 2 and the capacitance between the electrodes are C 1. Where the resistance value between the electrodes is R 1 and the resistance value of the resistor is R 2 , the predetermined capacitance C 2 has a relationship of C 1 R 1 ≧C 2 R 2 . It is.
以下、本考案を、本考案の好ましい実施例に沿
つて説明する。 Hereinafter, the present invention will be explained along with preferred embodiments of the present invention.
第4図は本考案に係る溶液の濃度変化検知装置
の好ましい実施例を示す回路図で、第1図の従来
装置と異なる点は、抵抗器6にコンデンサ9が並
列接続されていることだけである。 FIG. 4 is a circuit diagram showing a preferred embodiment of the solution concentration change detection device according to the present invention. The only difference from the conventional device shown in FIG. 1 is that a capacitor 9 is connected in parallel to a resistor 6. be.
第5図は第4図の検知装置の等価回路図で、静
電容量C2のコンデンサ9を追加したことにより、
第3図aに示す矩形波入力電圧の前縁部分におい
て矩形波に含まれる高調波成分の位相に変化が生
じ、第6図a及びbに示すように抵抗器6の両端
電圧は振動部分を含んでいる。これらの振動部分
は、電極間抵抗値R1が小さくなるとその振幅が
小さくなつて行き、電極間容量C1が大きくなる
と振幅が大きくなるので、互いに打ち消し合う傾
向を有し、濃度変化による振動部の振幅の大きさ
の変化はほとんど無視できる。 Figure 5 is an equivalent circuit diagram of the detection device shown in Figure 4, and by adding a capacitor 9 with a capacitance of C2 ,
At the leading edge of the rectangular wave input voltage shown in FIG. 3a, a change occurs in the phase of the harmonic component included in the rectangular wave, and as shown in FIGS. Contains. The amplitude of these vibration parts decreases as the interelectrode resistance value R 1 decreases, and the amplitude increases as the interelectrode capacitance C 1 increases, so they tend to cancel each other out, and the vibration parts due to concentration changes decrease. The change in the amplitude of is almost negligible.
一方、矩形波の前縁部分から矩形波の後縁部分
に至る充電波形の傾斜は、コンデンサ9を追加し
たことによつて水平に近づき、第6図aからbへ
の濃度変化に基づく傾斜の変化が少なくなる。 On the other hand, the slope of the charging waveform from the leading edge of the rectangular wave to the trailing edge of the rectangular wave approaches the horizontal due to the addition of the capacitor 9, and the slope due to the concentration change from a to b in FIG. There will be less change.
この結果、濃度変化による増幅・検波装置7の
出力変化は、ピーク値変化に比例する変化であつ
ても、コンデンサC1の充電終期(パルスの後縁)
の電圧の変化と略比例し、平均値にも比例するこ
ととなり従来のものよりも出力計8に与える変化
を大きくすることができる。 As a result, even if the change in the output of the amplification/detection device 7 due to the change in concentration is proportional to the change in peak value, the change in the output of the amplification/detection device 7 due to the change in concentration will occur at the end of charging of the capacitor C1 (the trailing edge of the pulse).
It is approximately proportional to the change in the voltage of , and is also proportional to the average value, so that the change given to the output meter 8 can be made larger than in the conventional case.
尚、コンデンサ9の静電容量C2の大きさは、
測定しようとする溶液の濃度範囲(一定の濃度を
基準として予め測定しておく)と電極構造によつ
て決まるC1,R1に対してC1R1≧C2R2なる関係を
満足するように選ぶ。若しC1R1<C2R2となれば
第7図に示す通り矩形波の立ち上がりが遅れ、三
角波に近い波形となり濃度変化検知という目的を
達成出来ない。 Furthermore, the size of the capacitance C 2 of the capacitor 9 is:
Satisfy the relationship C 1 R 1 ≧ C 2 R 2 for C 1 and R 1 , which are determined by the concentration range of the solution to be measured (measured in advance based on a certain concentration) and the electrode structure. Choose as you like. If C 1 R 1 <C 2 R 2 , as shown in FIG. 7, the rise of the rectangular wave will be delayed and the waveform will be close to a triangular wave, making it impossible to achieve the purpose of detecting concentration changes.
また、増幅・検波装置7の入力端子から増幅・
検波装置7を見たインピーダンスすなわち入力イ
ンピーダンスには容量分(Ca)も含されるが、
これは溶液の濃度検知に使用される増幅・検波装
置においては極めて小さく0.5%〜5%程度の範
囲の濃度で使用する食塩水の濃度変化検知を、例
えば直径7cm、高さ7cmの円筒容器4で行なう場
合、種々の電極構造が考えられるが、電極間容量
C1は0.1μF〜0.5μF、電極間抵抗R1は数10Ω〜数
KΩ程度であり、コンデンサ9の静電容量C2を追
加せずに、R2CaをC1R1に近づけることは困難で
ある。単に抵抗値R2を大きくするだけでは抵抗
器6の両端電圧(E×R2/R1+R2)の変化が小さく
なり所期の目的が達成できない。電極間容量C1
及び抵抗値R1が上記の数値を上回るものであつ
ても、適当な静電容量C2のコンデンサ9を付加
することにより増幅・検波装置7への入力波形の
傾斜を少なくし、出力の変化を改善できる。 In addition, the input terminal of the amplification/detection device 7
The impedance when looking at the detection device 7, that is, the input impedance, includes the capacitance (Ca),
This is an extremely small amplification/detection device used to detect the concentration of a solution, and it can detect changes in the concentration of saline solution used at concentrations in the range of about 0.5% to 5%. Various electrode structures are possible, but the interelectrode capacitance
C 1 is 0.1 μF to 0.5 μF, interelectrode resistance R 1 is several tens of Ω to several
It is approximately KΩ, and it is difficult to bring R 2 Ca close to C 1 R 1 without adding the capacitance C 2 of the capacitor 9. If the resistance value R 2 is simply increased, the change in the voltage across the resistor 6 (E×R 2 /R 1 +R 2 ) becomes small, and the intended purpose cannot be achieved. Interelectrode capacitance C 1
Even if the resistance value R1 exceeds the above value, by adding a capacitor 9 with an appropriate capacitance C2 , the slope of the input waveform to the amplification/detection device 7 can be reduced and the change in output can be reduced. can be improved.
以上述べたように、本考案によれば、溶液の濃
度変化に対する電圧変化を従来の装置より大きく
できるので、増幅機構が簡単になるという効果が
得られる。 As described above, according to the present invention, the change in voltage with respect to the change in concentration of the solution can be made larger than that in the conventional device, so that the effect of simplifying the amplification mechanism can be obtained.
第1図は従来の溶液の濃度変化検知装置を示す
回路図、第2図は第1図の装置の一部を等価回路
で示した図、第3図a〜cは第1図の装置に関し
て得られる波形図、第4図は本考案に係る溶液の
濃度変化検知装置を示す回路図、第5図は第4図
のの装置の一部を等価回路で示した図、第6図a
及びbは第4図の装置に関して得られる波形図、
そして第7図は矩形波の立上りが遅れた場合に波
形図である。
1……矩形波発振器、2,3……電極、4……
容器、5……溶液、6……抵抗器、7……増幅・
検波装置、8……出力計、9……コンデンサ。
尚、図中、同一符号は同一又は相当部分を示す。
Fig. 1 is a circuit diagram showing a conventional solution concentration change detection device, Fig. 2 is an equivalent circuit diagram of a part of the device shown in Fig. 1, and Figs. 3 a to c are related to the device shown in Fig. 1. The obtained waveform diagram, Fig. 4 is a circuit diagram showing the solution concentration change detection device according to the present invention, Fig. 5 is a diagram showing an equivalent circuit of a part of the device in Fig. 4, and Fig. 6 a.
and b is a waveform diagram obtained for the apparatus of FIG. 4,
FIG. 7 is a waveform diagram when the rise of the rectangular wave is delayed. 1... Square wave oscillator, 2, 3... Electrode, 4...
Container, 5...solution, 6...resistor, 7...amplification/
Detection device, 8... Output meter, 9... Capacitor.
In addition, in the figures, the same reference numerals indicate the same or corresponding parts.
Claims (1)
抵抗器を介して直列接続された矩形波発振器と、
前記抵抗器の両端電圧を増幅・検波するため同抵
抗器に接続され、同抵抗器からの入力電圧のピー
ク値に比例した電圧を出力する増幅・検波装置
と、該増幅・検波装置に接続された出力計とを備
えた溶液の濃度変化検知装置において、 前記抵抗器と並列に所定容量のコンデンサを接
続すると共に、前記所定容量をC2、前記電極間
の静電容量をC1、前記電極間の抵抗値をR1、前
記抵抗器の抵抗値をR2とする時、前記所定容量
C2がC1R1≧C2R2の関係にあることを特徴とする
溶液の濃度変化検知装置。[Claims for Utility Model Registration] A pair of electrodes arranged in isolation in a solution, a rectangular wave oscillator connected in series to the pair of electrodes via a resistor,
an amplification/detection device connected to the resistor for amplifying and detecting the voltage across the resistor and outputting a voltage proportional to the peak value of the input voltage from the resistor; In the solution concentration change detection device equipped with an output meter, a capacitor of a predetermined capacity is connected in parallel with the resistor, the predetermined capacitance is C 2 , the capacitance between the electrodes is C 1 , and the capacitance between the electrodes is C 2 . When the resistance value between the resistors is R1 and the resistance value of the resistor is R2 , the predetermined capacitance
A solution concentration change detection device characterized in that C 2 satisfies the relationship C 1 R 1 ≧C 2 R 2 .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9821182U JPS594461U (en) | 1982-07-01 | 1982-07-01 | Solution concentration change detection device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9821182U JPS594461U (en) | 1982-07-01 | 1982-07-01 | Solution concentration change detection device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS594461U JPS594461U (en) | 1984-01-12 |
| JPH035899Y2 true JPH035899Y2 (en) | 1991-02-14 |
Family
ID=30233278
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9821182U Granted JPS594461U (en) | 1982-07-01 | 1982-07-01 | Solution concentration change detection device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS594461U (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5448178A (en) * | 1993-11-05 | 1995-09-05 | Nalco Chemical Company | Transient technique to determine solution resistance for simple and accurate corrosion rate measurements |
-
1982
- 1982-07-01 JP JP9821182U patent/JPS594461U/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS594461U (en) | 1984-01-12 |
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