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JPH0617895B2 - Coulometric analysis method - Google Patents
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JPH0617895B2 - Coulometric analysis method - Google Patents

Coulometric analysis method

Info

Publication number
JPH0617895B2
JPH0617895B2 JP58089519A JP8951983A JPH0617895B2 JP H0617895 B2 JPH0617895 B2 JP H0617895B2 JP 58089519 A JP58089519 A JP 58089519A JP 8951983 A JP8951983 A JP 8951983A JP H0617895 B2 JPH0617895 B2 JP H0617895B2
Authority
JP
Japan
Prior art keywords
electrode
working electrode
rotor
electrodes
analysis method
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 - Lifetime
Application number
JP58089519A
Other languages
Japanese (ja)
Other versions
JPS59214753A (en
Inventor
岳志 紀本
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.)
Kimoto Electric Co Ltd
Original Assignee
Kimoto 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 Kimoto Electric Co Ltd filed Critical Kimoto Electric Co Ltd
Priority to JP58089519A priority Critical patent/JPH0617895B2/en
Publication of JPS59214753A publication Critical patent/JPS59214753A/en
Publication of JPH0617895B2 publication Critical patent/JPH0617895B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N27/00Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
    • G01N27/26Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating electrochemical variables; by using electrolysis or electrophoresis
    • G01N27/416Systems
    • G01N27/48Systems using polarography, i.e. measuring changes in current under a slowly-varying voltage
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N27/00Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
    • G01N27/26Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating electrochemical variables; by using electrolysis or electrophoresis
    • G01N27/416Systems
    • G01N27/42Measuring deposition or liberation of materials from an electrolyte; Coulometry, i.e. measuring coulomb-equivalent of material in an electrolyte

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  • Chemical & Material Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Health & Medical Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Electrochemistry (AREA)
  • Molecular Biology (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Other Investigation Or Analysis Of Materials By Electrical Means (AREA)
  • Testing Resistance To Weather, Investigating Materials By Mechanical Methods (AREA)

Description

【発明の詳細な説明】 本発明は、電解セル内に設けられた複数の電極間に流れ
る電流を測定することによつて、電解セル内の検水中に
含まれる被測定イオンの濃度を定量するようにした電量
分析方法に関する。
The present invention quantifies the concentration of ions to be measured contained in test water in an electrolysis cell by measuring the current flowing between a plurality of electrodes provided in the electrolysis cell. The present invention relates to a coulometric analysis method.

このような電量分析方法は、アンペロメトリーまたはク
ーロメトリーと呼ばれ、電極反応が行なわれる電極表面
が、付着物や酸化被膜などによつて汚染されると、正確
な定量を行なうことができなくなる問題がある。
Such a coulometric analysis method is called amperometry or coulometry, and if the electrode surface on which the electrode reaction takes place is contaminated by deposits or oxide film, it becomes impossible to perform accurate quantification. There is.

このような問題を解決するための或る先行技術では、測
定操作が終了後電極表面を洗浄し、それによつて前記付
着物や酸化被膜を電極表面から除去するようにしている
が、作業が面倒であり、測定に要する時間を長く必要と
する。
In one prior art for solving such a problem, the electrode surface is cleaned after the measurement operation is completed, thereby removing the deposits and oxide film from the electrode surface, but the work is troublesome. Therefore, a long time is required for measurement.

本発明の目的は、上述のような作業を省略することがで
きるとともに正確な定量を行なうことができる電量分析
方法を提供することである。
An object of the present invention is to provide a coulometric analysis method capable of omitting the work described above and performing accurate quantification.

さらにこのような先行技術では、たとえばシアンイオン
濃度を測定するときには硫化物イオンによる悪影響を受
け、また臭素イオン濃度を測定するときには、ヨウ素イ
オンの悪影響を受け、正確な分析ができない。
Further, in such a prior art, for example, when measuring the cyan ion concentration, the sulfide ion is adversely affected, and when measuring the bromine ion concentration, the iodine ion is adversely affected, and an accurate analysis cannot be performed.

本発明の他の目的は、妨害成分によつて悪影響を受けな
いようにして、正確な電量分析を行なうことのできる電
量分析方法を提供することである。
Another object of the present invention is to provide a coulometric analysis method capable of performing accurate coulometric analysis without being adversely affected by interfering components.

本発明は、電解セル1内に設けられた一対の電極3,4
間に流れる電流を測定することによつて、電解セル1内
の検水中に含まれる被測定イオンの濃度を定量するよう
にした電量分析方法において、 前記電極3,4は円柱状の作用電極3と、作用電極3の
周囲に同軸に配置される円筒状の対極4とを有し、電極
3,4間の間隙には絶縁部材15が設けられ、電極3,
4における電極反応が行われる平面状の表面11には、
円柱状の永久磁石の全外周面および軸線方向の両端面を
耐摩耗性材料によつて被覆して形成される回転子13を
設け、回転子13をマグネチックスターラ14によつて
作用電極3の軸線まわりに摺動回転させ、 参照電極5と作用電極3との間に、前放電物質の限界電
流域に予め定められる直流成分V1と、時間経過ととも
に振幅V2が増大するパルスとパルス相互間のパルス休
止期間が交互に繰返される矩形波電圧とを印加すること
を特徴とする電量分析方法である。
The present invention relates to a pair of electrodes 3 and 4 provided in the electrolysis cell 1.
In the coulometric analysis method, in which the concentration of ions to be measured contained in the sample water in the electrolysis cell 1 is quantified by measuring the current flowing therethrough, the electrodes 3 and 4 are cylindrical working electrodes 3 And a cylindrical counter electrode 4 coaxially arranged around the working electrode 3, and an insulating member 15 is provided in the gap between the electrodes 3 and 4,
In the flat surface 11 on which the electrode reaction in 4 is performed,
A rotor 13 formed by covering the entire outer peripheral surface of the cylindrical permanent magnet and both end surfaces in the axial direction with a wear-resistant material is provided, and the rotor 13 is provided with a magnetic stirrer 14 to prevent the working electrode 3 from moving. Between the reference electrode 5 and the working electrode 3, the DC component V1 predetermined in the limiting current region of the pre-discharged substance and the pulse between which the amplitude V2 increases with the passage of time are slidably rotated around the axis line. It is a coulometric analysis method characterized in that a rectangular wave voltage in which pulse rest periods are alternately repeated is applied.

以下、図面によつて本発明の一実施例を説明する。第1
図は本発明に従つて構成される分析装置の一実施例の断
面図である。この分析装置は、たとえば検水中に含まれ
るシアンイオン濃度を測定するために用いられる。この
分析装置における電解セル1は、セル本体2と、作用電
極3と、対極4と、参照電極5とを含む。セル本体2
は、有底円筒状の底部6と、底部6の上方(第1図の上
方)に向けて先すぼまりに形成された逆錐形の部分7を
含む上部8とから構成される。底部6と上部8とは気密
的に一体化され、それによつてセル本体2内には電解室
9が形成される。このようにして構成されるセル本体2
は、たとえば塩化ビニル樹脂などの合成樹脂によつて形
成される。
An embodiment of the present invention will be described below with reference to the drawings. First
The figure is a cross-sectional view of an embodiment of an analytical device constructed in accordance with the present invention. This analyzer is used, for example, to measure the concentration of cyan ions contained in test water. The electrolysis cell 1 in this analyzer includes a cell body 2, a working electrode 3, a counter electrode 4, and a reference electrode 5. Cell body 2
Is composed of a bottomed cylindrical bottom portion 6 and an upper portion 8 including an inverted-pyramidal portion 7 which is formed in a tapered shape upward from the bottom portion 6 (upper side in FIG. 1). The bottom part 6 and the upper part 8 are hermetically integrated with each other, whereby an electrolytic chamber 9 is formed in the cell body 2. Cell body 2 configured in this way
Are formed of synthetic resin such as vinyl chloride resin.

作用電極3は、銀製であつて円柱状に形成される。対極
4はたとえばステンレス鋼製であつて円筒状に形成され
る。作用電極3は対極4に緩挿され、作用電極3および
対極4間の間隙ならびに対極4の外周には、たとえばア
ルミナか分散された合成樹脂などの電気絶縁性物質から
なる絶縁部材15が設けられる。こうして絶縁部材15
を介して一体化された作用電極3および対極4は、セル
本体2における底部6の底板10を気密的に貫通されて
セル本体2に固定される。電解室9に臨む作用電極3、
対極4および絶縁部材15における上端部の端面11は
面一に形成される。
The working electrode 3 is made of silver and is formed in a columnar shape. The counter electrode 4 is made of, for example, stainless steel and has a cylindrical shape. The working electrode 3 is loosely inserted into the counter electrode 4, and an insulating member 15 made of an electrically insulating substance such as alumina or a dispersed synthetic resin is provided in the gap between the working electrode 3 and the counter electrode 4 and the outer periphery of the counter electrode 4. . Thus, the insulating member 15
The working electrode 3 and the counter electrode 4 which are integrated via the airtightly penetrate the bottom plate 10 of the bottom portion 6 of the cell body 2 and are fixed to the cell body 2. Working electrode 3 facing the electrolysis chamber 9,
The end faces 11 at the upper ends of the counter electrode 4 and the insulating member 15 are formed flush with each other.

参照電極5は、先端12が電解室9に臨んでセル本体2
における上部8を気密的に貫通され、それによつて参照
電極5はセル本体2に固定される。参照電極5はたとえ
ば銀ー塩化銀電極が用いられる。
The reference electrode 5 has a tip 12 facing the electrolysis chamber 9 and a cell body 2
The upper part 8 is penetrated in an airtight manner, whereby the reference electrode 5 is fixed to the cell body 2. As the reference electrode 5, for example, a silver-silver chloride electrode is used.

第2図を併わせて参照して、端面11上には円柱状の回
転子13が乗載される。この回転子13は、円柱状の永
久磁石の全外周面および軸線方向の両端面を、炭化ケイ
素SiCなどの耐摩耗性材料によつて被覆して形成され
る。電解セル1における底部6の下方には、回転子13
に対応してマグネチツクスターラ14が配置される。こ
のマグネチツクスターラ14は、作用電極3の軸線まわ
りに等間隔に配置された複数の永久磁石または電磁石を
備え、これらの永久磁石または電磁石が前記軸線まわり
に回転駆動されることによつて、回転子13は前記軸線
まわりに回転可能である。回転子13の長さd1は、対
極4の外径d2よりも大きく選ばれる。
Referring to FIG. 2 together, a cylindrical rotor 13 is mounted on the end surface 11. The rotor 13 is formed by covering the entire outer peripheral surface of the cylindrical permanent magnet and both end surfaces in the axial direction with a wear resistant material such as silicon carbide SiC. Below the bottom portion 6 of the electrolysis cell 1, a rotor 13 is provided.
The magnetic stirrer 14 is arranged in correspondence with. This magnetic stirrer 14 is provided with a plurality of permanent magnets or electromagnets arranged at equal intervals around the axis of the working electrode 3, and these permanent magnets or electromagnets are driven to rotate around the axis to rotate. The child 13 is rotatable around the axis. The length d1 of the rotor 13 is selected to be larger than the outer diameter d2 of the counter electrode 4.

このようにして構成される分析装置において、検水はセ
ル本体2における底部6に形成された流路20を介して
電解室9内に導入される。電解室9内において、検水中
に含まれるシアンイオンCN-は作用電極3の端面11す
なわち電極表面において第1式に示すような電極反応を
行なう。
In the analyzer configured in this way, the test water is introduced into the electrolysis chamber 9 through the flow path 20 formed in the bottom portion 6 of the cell body 2. In the electrolytic chamber 9, the cyan ion CN contained in the test water causes an electrode reaction as shown in the first formula on the end surface 11 of the working electrode 3, that is, the electrode surface.

Ag+2CN→Ag(CN) +e…(1) 第1式に示される電極反応によつて放出された電子eに
基づく作用電極3と対極4との間に流れる電流は、作用
電極3、対極4および参照電極5に関連して設けられる
電流測定手段21によつて測定される。これによつて電
解室9内を流れる検水中に含まれるシアンイオンの濃度
が定量される。このようにシアンイオンの濃度が定量さ
れたあとの検水は、電解セル本体2における上部8の逆
円錐形の部分7に形成された流路22を介して電解室9
外に排出される。
Ag + 2CN → Ag (CN) 2 + e (1) The current flowing between the working electrode 3 and the counter electrode 4 based on the electron e emitted by the electrode reaction represented by the first formula is the working electrode 3, It is measured by a current measuring means 21 provided in association with the counter electrode 4 and the reference electrode 5. As a result, the concentration of cyan ions contained in the test water flowing in the electrolytic chamber 9 is quantified. The sample water after the concentration of cyan ions has been quantified in this way passes through the flow path 22 formed in the inverted conical portion 7 of the upper portion 8 of the electrolysis cell main body 2 to the electrolysis chamber 9
It is discharged outside.

上述のように検水中に含まれるシアンイオンの濃度の定
量の途中において、回転子13はマグネチックスターラ
によつて第2図示の矢符30で示すように作用電極3の
軸線まわりに回転される。そのため作用電極3および対
極4における端面11は、回転子13によつて摺擦され
ている。したがつて検水中に含まれる汚染物質が前記端
面11に付着しても回転子13の摺擦力によつて除去さ
れる。また作用電極3の端面11には、銀酸化物(Ag
O,Ag2O)などの被膜が形成されるおそれがあるが、こ
れらの被膜も前記汚染物質と同様に回転子13の摺擦力
によつて除去される。したがつて作用電極3および対極
4の端面11すなわち電極反応が行なわれる電極表面が
常に清浄に保たれ、各電極3,4間に流れる電流が正確
に測定され、検水中のシアンイオンの濃度が正確に定量
される。
As described above, the rotor 13 is rotated around the axis of the working electrode 3 by the magnetic stirrer during the quantification of the concentration of cyan ions contained in the test water, as indicated by the arrow 30 in the second illustration. . Therefore, the end faces 11 of the working electrode 3 and the counter electrode 4 are rubbed by the rotor 13. Therefore, even if contaminants contained in the test water adhere to the end surface 11, they are removed by the rubbing force of the rotor 13. Further, on the end surface 11 of the working electrode 3, silver oxide (Ag
O, Ag 2 O) and the like may be formed, but these films are also removed by the rubbing force of the rotor 13 like the contaminants. Therefore, the end surfaces 11 of the working electrode 3 and the counter electrode 4, that is, the electrode surfaces on which the electrode reaction takes place are always kept clean, the current flowing between the electrodes 3 and 4 is accurately measured, and the concentration of cyanide ions in the test water is Accurately quantified.

なお従来ではこのように電極間に流れる電流を測定する
ことによつて、電解セル内の検水中に含まれる被測定イ
オンの濃度を定量するようにした電量分析方法において
は、電解室9内を流れる検水が乱流になると、前記電流
が脈流となるので、このような回転子13を電解室9内
で回転させることは不可能であると考えられていた。し
かし本件発明者の実験によれば、回転子の回転数をたと
えば300rpmとしたときに、作用電極3と対極4との
間に流れる電流は、一定周期の交流電流となり、その交
流電流を平滑することにより、検水中に含まれる被測定
イオンすなわちシアンイオンの濃度に対応した前記電流
を得ることができた。
Incidentally, in the conventional coulometric analysis method in which the concentration of the ions to be measured contained in the test water in the electrolysis cell is quantified by measuring the current flowing between the electrodes as described above, the inside of the electrolysis chamber 9 is It has been considered impossible to rotate the rotor 13 in the electrolysis chamber 9 because the current becomes a pulsating flow when the flowing test water becomes a turbulent flow. However, according to the experiments by the inventor of the present invention, when the number of rotations of the rotor is set to, for example, 300 rpm, the current flowing between the working electrode 3 and the counter electrode 4 becomes an alternating current of a constant cycle, and the alternating current is smoothed. As a result, the current corresponding to the concentration of the ions to be measured contained in the test water, that is, the cyan ions, could be obtained.

本発明ではさらに、作用電極3と参照電極5との間に印
加する電圧を第3図に示されるように変化させる。この
印加電圧の波形は、直流成分V0が常に印加されてお
り、時間の経過とともに振幅がV1,V2,…と増大す
るパルスとパルス相互間のパルス休止期間とが交互に繰
返されるパルス波が重畳される。このような測定方法を
正常パルス法と呼ぶ。以上のような方法で電圧を作用電
極3と参照電極5との間に印加することによつて、両極
間に流れる電流の値は、前放電物質の混入にかかわらず
正確に検出することができ、その電流値の積分値から物
質の含有量を定量できる。
In the present invention, the voltage applied between the working electrode 3 and the reference electrode 5 is further changed as shown in FIG. In the waveform of this applied voltage, a DC component V0 is always applied, and a pulse wave in which a pulse whose amplitude increases as V1, V2, ... To be done. Such a measuring method is called a normal pulse method. By applying the voltage between the working electrode 3 and the reference electrode 5 by the above method, the value of the current flowing between the two electrodes can be accurately detected regardless of the mixture of the pre-discharge substance. , The content of the substance can be quantified from the integrated value of the current value.

たとえば第4図は、本発明の実験結果を示すグラフであ
り、作用電極に銀を用いたときの2×10-4MBr
(0.1MKNO)の電極上への析出波における正
常パルス法により記録した電位−電流曲線を示したもの
である。本実施例において作用電極3と参照電極5との
間に第3図のV0として前放電物質としてのヨウ素イオ
ンIの限界電圧−0.05Vを、またV1=0.15
V,V2=0.3V,…と時間経過とともに一次関数で
増大するパルスとパルス相互間のパルス休止期間とが交
互に1秒間隔で繰返される矩形波電圧を印加したとき
に、分析物質として臭素イオンBrとヨウ素イオンI
を含んでいるときは、l1の波形が与えられる。l1
のV0に相当する点l11と電流が急上昇するまでの点
l12の間のW1の範囲の電流値はヨウ素イオンI
対応するものであり、l1の電流が次に一定になつてい
るl13とl14との間のW2の範囲の電流値は臭素イ
オンBrとヨウ素イオンIに対応するものである。
すなわちヨウ素イオンIと臭素イオンBrとを含む
場合、l1をW1の間で積分したAがIの量であり、
l1をW2の間で積分したBがBr-+I-の量であるから
Br=B−Aとなる。この検体が臭素イオンBr
みを含むときは、l2で示される波形が得られる。前放
電物質であるヨウ素イオンIが含まれていないときに
は、ヨウ素イオンIによる妨害がないので、電流が一
定になるW2の間が明確になる。l2の波形から予めW
2の範囲を決めておくとl1からW2の範囲を決めるよ
りも正確にできる。またl2で示されるように電圧V0
になつたときに電流が流れ始めることになる。本発明で
は、この第3図のように電圧V0を常時加えて、さらに
時間経過とともにピーク値V1,V2,…を有するパル
スを重畳しているので、ヨウ素イオンIによる妨害が
あつても臭素イオンBrの電量を測定することができ
る。
For example, FIG. 4 is a graph showing the experimental results of the present invention, which is 2 × 10 −4 MBr when silver is used for the working electrode.
- recorded potential by normal pulse method in precipitation wave to (0.1MKNO 3) of the electrode on the - shows the current curve. In the present embodiment, the limit voltage −0.05V of iodine ion I − serving as the pre-discharge material is used as V0 in FIG. 3 between the working electrode 3 and the reference electrode 5, and V1 = 0.15.
Bromine was used as an analyte when a rectangular wave voltage was applied in which V, V2 = 0.3 V, ... Ion Br and iodine ion I
If it contains a-, the waveform of l1 is given. l1
The current value in the range of W1 between the point l11 corresponding to V0 and the point l12 until the current sharply rises corresponds to the iodine ion I , and the current of l1 becomes constant next to l13. The current value in the range of W2 between 114 and 114 corresponds to bromine ion Br and iodine ion I .
That is, when iodine ion I and bromine ion Br are included, A obtained by integrating 11 with W1 is the amount of I ,
Since B obtained by integrating 11 over W2 is the amount of Br + I , Br = BA. When this sample contains only bromide ions Br , a waveform indicated by 12 is obtained. When iodine ion I which is the pre-discharge substance is not contained, there is no interference by iodine ion I −, so that the period during W2 when the current becomes constant becomes clear. W from the waveform of l2
If the range of 2 is determined, it can be more accurate than the range of 11 to W2. Also, as indicated by l2, the voltage V0
The current will start to flow when it reaches. In the present invention, in addition to voltage V0 as the FIG. 3 always further peak value V1, V2 as time elapses, since the superimposing pulse having a ..., iodide ion I - bromine even thickness interference by The charge of the ion Br can be measured.

第5図は、電圧V2を一定として検出すべき物質すなわ
ち臭素イオンに混入される妨害物質ヨウ素イオンの濃度
を変化させて、拡散電流を測定したグラフである。l
3,l4,l5,l6,l7はそれぞれヨウ素イオン濃
度10−4M、2×10−4M、5×10−4M、10
−3M、2×10−3Mに対応したものである。
FIG. 5 is a graph in which the diffusion current was measured while changing the concentration of the substance to be detected, that is, the interfering substance iodine ion mixed in the bromine ion, with the voltage V2 kept constant. l
3, l4, l5, l6 and l7 are iodine ion concentrations of 10 −4 M, 2 × 10 −4 M, 5 × 10 −4 M and 10 respectively.
-3 M, 2 * 10 -3 M.

以上のように本発明によれば、電極反応が行われる電極
表面11は、回転子13によつて摺擦されるので、電極
表面11の付着物や酸化皮膜は除去され、検水中に含ま
れる被測定イオンの濃度を正確に定量することができ
る。
As described above, according to the present invention, since the electrode surface 11 on which the electrode reaction is performed is rubbed by the rotor 13, the deposits and oxide film on the electrode surface 11 are removed and included in the test water. The concentration of the measured ion can be accurately quantified.

さらに参照電極5と作用電極3との間に、前放電物質の
限界電流域に予め定められる直流成分V1と、時間経過
とともに振幅V2が増大するパルスとパルス相互間のパ
ルス休止期間が交互に繰返される矩形波電圧とを印加す
るので、前放電物質による電量の誤差をなくして、定量
すべき物質の正確な電量分析を行うことができる。
Further, between the reference electrode 5 and the working electrode 3, a direct current component V1 which is predetermined in the limiting current region of the pre-discharge substance, and a pulse pause period between the pulses in which the amplitude V2 increases with the passage of time are alternately repeated. Since a rectangular wave voltage is applied, it is possible to eliminate the error of the coulombic quantity due to the pre-discharged material and to perform accurate coulometric analysis of the material to be quantified.

また、回転子13は、マグネチツクスターラ14によつ
て回転駆動されるので、簡単な機構で容易に電極表面1
1の研磨を行うことができる。
Further, since the rotor 13 is rotationally driven by the magnetic stirrer 14, the electrode surface 1 can be easily driven by a simple mechanism.
1 polishing can be performed.

また、回転子13は、円形磁石の全周面および軸線方向
の両端面を耐磨耗性材料で被覆して形成されるので、電
極面11の研磨を十分に行うことができる。
Further, since the rotor 13 is formed by covering the entire circumferential surface of the circular magnet and both end surfaces in the axial direction with a wear resistant material, the electrode surface 11 can be sufficiently polished.

さらに、作用電極3は円柱状であり、対極4は同心的に
配置され、この軸線方向に垂直な端面11を回転子13
によつて研磨するので、電極表面11の研磨は均一にか
つ効率的に行うことができる。
Further, the working electrode 3 has a cylindrical shape, the counter electrode 4 is concentrically arranged, and the rotor 11 has an end face 11 perpendicular to the axial direction.
Since the polishing is performed by the method described above, the polishing of the electrode surface 11 can be performed uniformly and efficiently.

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

第1図は本発明に従つて構成される分析装置の一実施例
の断面図、第2図は第1図示の回転子13付近の平面
図、第3図は作用電極3と参照電極5の間に印加した電
圧の波形図、第4図は作用電極と参照電極間に正常パル
ス電圧を印加した際の電位ー電流曲線、第5図は前放電
物質共存下における拡散電流を示したグラフである。 1…電解セル、3…作用電極、4…対極、5…参照電
極、13…回転子、14…マグネチツクスターラ、21
…電流測定手段
FIG. 1 is a cross-sectional view of an embodiment of an analyzer constructed according to the present invention, FIG. 2 is a plan view of the vicinity of the rotor 13 shown in FIG. 1, and FIG. 3 shows a working electrode 3 and a reference electrode 5. Fig. 4 is a waveform diagram of the voltage applied between them, Fig. 4 is a potential-current curve when a normal pulse voltage is applied between the working electrode and the reference electrode, and Fig. 5 is a graph showing a diffusion current in the presence of a pre-discharge substance. is there. DESCRIPTION OF SYMBOLS 1 ... Electrolytic cell, 3 ... Working electrode, 4 ... Counter electrode, 5 ... Reference electrode, 13 ... Rotor, 14 ... Magnetic stirrer, 21
... Current measuring means

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】電解セル1内に設けられた一対の電極3,
4間に流れる電流を測定することによつて、電解セル1
内の検水中に含まれる被測定イオンの濃度を定量するよ
うにした電量分析方法において、 前記電極3,4は円柱状の作用電極3と、作用電極3の
周囲に同軸に配置される円筒状の対極4とを有し、電極
3,4間の間隙には絶縁部材15が設けられ、電極3,
4における電極反応が行われる平面状の表面11には、
円柱状の永久磁石の全外周面および軸線方向の両端面を
耐摩耗性材料によって被覆して形成される回転子13を
設け、回転子13をマグネチツクスターラ14によつて
作用電極3の軸線まわりに摺動回転させ、 参照電極5と作用電極3との間に、前放電物質の限界電
流域に予め定められる直流成分V0と、時間経過ととも
に振幅がV1,V2,…と増大するパルスとパルス相互
間のパルス休止期間とが交互に繰返される矩形波電圧と
を印加することを特徴とする電量分析方法。
1. A pair of electrodes 3, provided in an electrolysis cell 1.
By measuring the current flowing between the four electrolysis cells 1
In the coulometric analysis method for quantifying the concentration of ions to be measured contained in the sample water, the electrodes 3 and 4 are a cylindrical working electrode 3 and a cylindrical cylinder arranged coaxially around the working electrode 3. Counter electrode 4, and an insulating member 15 is provided in the gap between the electrodes 3 and 4,
In the flat surface 11 on which the electrode reaction in 4 is performed,
A rotor 13 formed by covering the entire outer peripheral surface of the cylindrical permanent magnet and both end surfaces in the axial direction with a wear-resistant material is provided, and the rotor 13 is rotated around the axis of the working electrode 3 by a magnetic stirrer 14. Pulses and pulses that are slidably rotated to a direct current component V0 predetermined between the reference electrode 5 and the working electrode 3 in the limiting current region of the pre-discharge substance, and the amplitude increases to V1, V2, ... With time. A coulometric analysis method comprising applying a rectangular wave voltage in which pulse rest periods are alternately repeated.
JP58089519A 1983-05-20 1983-05-20 Coulometric analysis method Expired - Lifetime JPH0617895B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58089519A JPH0617895B2 (en) 1983-05-20 1983-05-20 Coulometric analysis method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58089519A JPH0617895B2 (en) 1983-05-20 1983-05-20 Coulometric analysis method

Publications (2)

Publication Number Publication Date
JPS59214753A JPS59214753A (en) 1984-12-04
JPH0617895B2 true JPH0617895B2 (en) 1994-03-09

Family

ID=13973042

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58089519A Expired - Lifetime JPH0617895B2 (en) 1983-05-20 1983-05-20 Coulometric analysis method

Country Status (1)

Country Link
JP (1) JPH0617895B2 (en)

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5555181Y2 (en) * 1977-07-16 1980-12-20
JPS54102189U (en) * 1977-12-28 1979-07-18
JPS55146036A (en) * 1979-05-02 1980-11-14 Masashi Goto Polarograph of step wave semidifferentiation and integration
JPS5615568U (en) * 1979-07-16 1981-02-10

Also Published As

Publication number Publication date
JPS59214753A (en) 1984-12-04

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