JPH0425648Y2 - - Google Patents

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Publication number
JPH0425648Y2
JPH0425648Y2 JP1986110548U JP11054886U JPH0425648Y2 JP H0425648 Y2 JPH0425648 Y2 JP H0425648Y2 JP 1986110548 U JP1986110548 U JP 1986110548U JP 11054886 U JP11054886 U JP 11054886U JP H0425648 Y2 JPH0425648 Y2 JP H0425648Y2
Authority
JP
Japan
Prior art keywords
current density
sensor
liquid
conductor
cylindrical body
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
JP1986110548U
Other languages
Japanese (ja)
Other versions
JPS6319260U (en
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 filed Critical
Priority to JP1986110548U priority Critical patent/JPH0425648Y2/ja
Publication of JPS6319260U publication Critical patent/JPS6319260U/ja
Application granted granted Critical
Publication of JPH0425648Y2 publication Critical patent/JPH0425648Y2/ja
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 〔考案の目的〕 産業上の利用分野 本考案は電気メツキ等の電解処理を施す被処理
面を局所的電流密度を測定する装置に関する。
[Detailed Description of the Invention] [Purpose of the Invention] Industrial Application Field The present invention relates to an apparatus for measuring the local current density of a surface to be treated which is subjected to an electrolytic treatment such as electroplating.

従来の技術 電気メツキや電解研磨等の電解処理を行なうに
当つて、被処理面の電流密度を適切な範囲内に調
整することは、良好な電解処理面を得るためには
欠くことができない。このような電解処理におい
て電流密度を知るために、被処理面の面積と通電
全電流値とから算出する方法があるが、被処理面
の形状が一様でないときにはその凸部や端部など
に電流が集中し、また凹部や裏面などには少しし
か電流が廻らないという問題があり、前記のよう
な平均電流密度を知るのみでは良好な電解処理面
は得られない。
Prior Art When performing electrolytic treatments such as electroplating and electrolytic polishing, it is essential to adjust the current density of the surface to be treated within an appropriate range in order to obtain a good electrolytically treated surface. In order to know the current density in such electrolytic treatment, there is a method of calculating it from the area of the surface to be treated and the total current value. There is a problem in that the current is concentrated and only a small amount of current flows to the recesses or the back surface, so it is not possible to obtain a good electrolytically treated surface just by knowing the average current density as described above.

そこで、電解処理を行なうに当つて、被処理導
電体と電解浴との接液面におけるそれぞれ異つた
場所での局所的電流密度を知ることができれば、
これによつて電解処理条件や対極の形状あるいは
対極との相対的位置関係等を調整し、効率的かつ
優れた成績が得られる電解処理を実施することが
可能となる筈である。ところがこのような接液面
の局所的電流密度を知る手段としては、実験室的
に測定する方法はあつたとしても、工業的に操業
現場で利用し得る測定方法は未だに無いのが現実
であつた。
Therefore, when performing electrolytic treatment, it would be possible to know the local current density at different locations on the contact surface between the conductor to be treated and the electrolytic bath.
This should make it possible to perform electrolytic treatment efficiently and with excellent results by adjusting the electrolytic treatment conditions, the shape of the counter electrode, the relative positional relationship with the counter electrode, etc. However, even if there is a laboratory measurement method for determining the local current density of a liquid-contacted surface, the reality is that there is still no measurement method that can be used in industrial operations. Ta.

これに対して本考案者の1人は、対になつて互
いに絶縁された導電体電極を所定距離を隔てて対
向配置したバイポーラ電極型センサを電流密度測
定対象導電体の接液面に近接させて電解液中に位
置させ、電解液中を流れる電流によつて液中に発
生する液中電流密度に比例した電位傾度を前記セ
ンサの電極間の電位差として検出し、この電位差
信号をあらかじめ同じ電解液について測定して得
た電位差−電流密度の関数に代入することによつ
て測定対象導電体の接液面付近の液中電流密度を
求め、これによって該接液面の特定箇所を通過す
る電流の密度を近似的に測定する手段が、工業的
に実用可能であることを見出した。そして、この
原理に基づく電流密度測定装置を発明し、別途特
許出願している(特開昭62−27655号)。
In contrast, one of the inventors of the present invention proposed a bipolar electrode type sensor in which a pair of mutually insulated conductor electrodes are arranged facing each other at a predetermined distance, and the sensor is placed close to the wetted surface of the conductor to be measured for current density. The sensor is placed in an electrolytic solution, and the potential gradient proportional to the current density in the solution generated by the current flowing through the electrolytic solution is detected as the potential difference between the electrodes of the sensor. The current density in the liquid near the liquid contact surface of the conductor to be measured is determined by substituting it into the potential difference-current density function obtained by measuring the liquid, and from this, the current passing through a specific point on the liquid contact surface is determined. It has been found that a means for approximately measuring the density of is industrially practical. He then invented a current density measuring device based on this principle and filed a separate patent application (Japanese Patent Laid-Open No. 62-27655).

解決しようとする問題点 かかる電流密度測定装置は、先端に導電体を離
間対向して配置したセンサと、該導電体間の電位
差を信号として導出する電線と、該信号を増幅し
て表示する出力装置とからなつている。そして、
かかる測定装置によつて得た電流傾度の測定精度
は、センサに設けた電極を被測定導電体の接液面
に対して接近した位置で電位傾度が最大となるよ
うな姿勢に固定して測定を実施することによつ
て、はじめて確保される。
Problems to be Solved This current density measuring device includes a sensor having a conductor disposed at its tip facing each other at a distance, an electric wire that derives the potential difference between the conductors as a signal, and an output that amplifies and displays the signal. It consists of equipment. and,
The measurement accuracy of the current gradient obtained by such a measuring device is determined by fixing the electrode attached to the sensor in a position that maximizes the potential gradient at a position close to the wetted surface of the conductor to be measured. This can only be ensured by implementing the following.

ところが、被測定導電体の形状は必ずしも単純
なものばかりではなく、複雑な表面形状の導電体
の多くの部位の電流傾度を正確に測定しようとす
ると、センサの位置決めが容易でない。またセン
サを電位傾度が最大となる姿勢となるよう固定す
るのも容易でなく、場合によつてはセンサの電極
を測定対象の部位に接近させることさえ不可能の
ことがあつた。
However, the shape of the conductor to be measured is not necessarily simple, and positioning the sensor is not easy when attempting to accurately measure current gradients in many parts of a conductor with a complex surface shape. Furthermore, it is not easy to fix the sensor in a position where the potential gradient is maximum, and in some cases, it has been impossible to even bring the electrode of the sensor close to the part to be measured.

また更に、センサの電極を測定対象部位に過度
に接近させると電流分布を乱すことになり、結局
電流密度測定値の精度が低下する結果を招く。
Furthermore, if the electrode of the sensor is brought too close to the measurement target site, the current distribution will be disturbed, resulting in a decrease in the accuracy of the current density measurement value.

そこで、本考案は、複雑な表面形状の導電体に
おける接液面の電流密度を測定するに当つて、多
様の部位のそれぞれに容易に電極を接近させるこ
とができ、また接近させても測定の精度を低下さ
せることのない電流密度測定用センサを提供しよ
うとするものである。
Therefore, when measuring the current density on the liquid contact surface of a conductor with a complex surface shape, the present invention allows electrodes to be easily brought close to each of various parts, and even if the electrodes are brought close, measurement is not possible. The present invention aims to provide a sensor for measuring current density without reducing accuracy.

〔考案の構成〕[Structure of the idea]

問題点を解決するための手段 上述のような本考案の目的は、絶縁性の筒状体
の先端部に2個の接液電極を互に絶縁された状態
で設けてなり、該接液電極は筒状体の長さ方向に
所定距離を隔てて対設されると共に、少くともい
ずれか一方が該筒状体を環状にとりまいて設けら
れていることを特徴とする導電体接液面の電流密
度測定用センサを用いることによつて達成され
る。
Means for Solving the Problems The object of the present invention as described above is to provide two wetted electrodes insulated from each other at the tip of an insulating cylindrical body. are arranged oppositely at a predetermined distance in the length direction of a cylindrical body, and at least one of them is provided so as to surround the cylindrical body in an annular manner. This is achieved by using a sensor for measuring current density.

以下、図面によつて本考案のセンサを説明す
る。1は電気絶縁性の筒状体の基部であり、2は
同じく筒状体の延長部である。延長部2は相互に
絶縁された2本の導線3,3′を軟質の絶縁材料
4で包埋して細長く形成されている。延長部2の
先細に形成された先端2aから5mmおよび10mm離
れた位置には、環状の接液電極5および6がその
外面を延長部2の側面に現わすように嵌着されて
おり、それぞれ導線3および3′に接続されてい
る。
Hereinafter, the sensor of the present invention will be explained with reference to the drawings. 1 is the base of an electrically insulating cylindrical body, and 2 is an extension of the cylindrical body. The extension part 2 is formed into an elongated shape by embedding two mutually insulated conductive wires 3 and 3' in a soft insulating material 4. Annular liquid contact electrodes 5 and 6 are fitted at positions 5 mm and 10 mm away from the tapered tip 2a of the extension part 2 so that their outer surfaces are exposed on the side surfaces of the extension part 2, respectively. It is connected to conductors 3 and 3'.

筒状体の基部1は中空筒状であつてその内部の
空間を貫通して2芯の絶縁電線7が設けられ、そ
れぞれの芯線は先端においてそれぞれ導線3,
3′に接続されている。絶縁電線7は基部1の後
端から引き出されて、外部の計器に電極電位を達
成することができるようになつている。
The base 1 of the cylindrical body has a hollow cylindrical shape, and a two-core insulated wire 7 is provided passing through the inner space of the base 1, and each core wire has a conductive wire 3,
3'. An insulated wire 7 is led out from the rear end of the base 1 so that an electrode potential can be achieved for an external instrument.

これらの接液電極5,6は、いずれも軸からみ
て側方に接液面を有しているが、先端に近い電極
5は、側面に設ける代わりに先端に設けられてい
てもよい。この場合は液中における電位差を測定
できるほか、該測定導電体に電極5を接触させる
ことにより被測定導電体と液との電気差をも測定
できる利点があるが、一方、被測定導電体の接液
面から電流密度測定点までの距離の正確さを期し
難いという不利がある。
These liquid contact electrodes 5 and 6 both have a liquid contact surface on the side when viewed from the axis, but the electrode 5 near the tip may be provided at the tip instead of on the side. In this case, there is an advantage that in addition to being able to measure the potential difference in the liquid, it is also possible to measure the electrical difference between the conductor to be measured and the liquid by bringing the electrode 5 into contact with the conductor to be measured. There is a disadvantage that it is difficult to ensure the accuracy of the distance from the liquid contact surface to the current density measurement point.

かかる接液電極5,6は、たとえば白金などの
ような耐食性金属か、または電解液に含有される
イオンと同種の金属などで構成され、たとえ溶出
しても電解液を汚染しないような金属であること
が望ましい。
The wetted electrodes 5 and 6 are made of a corrosion-resistant metal such as platinum, or a metal of the same type as the ions contained in the electrolyte, and are made of a metal that will not contaminate the electrolyte even if eluted. It is desirable that there be.

また、延長部2は可撓性であることが望まし
く、一旦屈曲したときにその状態が内部摩擦によ
つてそのまま維持されるものであるときは、延長
部2のみを種々の角度に屈曲することにより複雑
な形状の接液面に対する測定が一層容易となる。
Further, it is preferable that the extension part 2 is flexible, and if once bent, the state is maintained by internal friction, only the extension part 2 can be bent at various angles. This makes it easier to measure liquid contact surfaces with complex shapes.

作 用 本考案の電流密度測定用センサは、以上の如く
構成されているから、接液電極5,6を設けた先
端部を測定対象の導電体接液面に対して垂直とな
るようにして液中電気差の測定を行なうものであ
り、先端が絶縁体で形成されている場合は、先端
を接液面に接触させて測定を実施することにより
測定位置が正確に規制され、一定位値での電流密
度を容易に知ることができる。
Function Since the current density measuring sensor of the present invention is constructed as described above, the tip portion provided with the liquid contact electrodes 5 and 6 is arranged perpendicular to the liquid contact surface of the conductor to be measured. This device measures the electrical difference in a liquid, and if the tip is made of an insulator, the measurement position is accurately regulated by making the measurement with the tip in contact with the wetted surface, and a constant value is measured. The current density at can be easily determined.

〔考案の効果〕[Effect of idea]

本考案の導電体接液面の電流密度測定用センサ
は、筒状センサの先端部をとりまいて環状の接液
電極が設けられているので、電流密度測定に当つ
て測定位置を正確に規制することができるばかり
でなく、センサの先端部を導電体接液面に対して
垂直に位置させ得るので液中の電流分布を乱すこ
とがない。従つて、局所的な電流密度を高精度で
測定すことが可能となつたものである。
The sensor for measuring current density on the surface of a conductor in contact with liquid according to the present invention has a ring-shaped liquid contact electrode surrounding the tip of the cylindrical sensor, so the measurement position can be accurately regulated when measuring current density. In addition, the tip of the sensor can be positioned perpendicular to the surface of the conductor in contact with the liquid, so that the current distribution in the liquid is not disturbed. Therefore, it has become possible to measure local current density with high precision.

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

図面は、本考案の導電体接液面の電流密度測定
用センサの部分的な断面を示した正面図である。 1……筒状体基部、2……筒状体延長部、3,
3′……導線、4……絶縁被覆、5,6……接液
電極、7……絶縁電線。
The drawing is a front view showing a partial cross section of a sensor for measuring current density on a surface of a conductor in contact with liquid according to the present invention. 1... Cylindrical body base, 2... Cylindrical body extension, 3,
3'...Conducting wire, 4...Insulating coating, 5, 6...Wetted electrode, 7...Insulated wire.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 絶縁性の筒状体の先端部に2個の接液電極を互
に絶縁された状態で設けてなり、該接液電極は筒
状体の長さ方向に所定距離を隔てて対設されると
共に、少くともいずれか一方が該筒状体を環状に
とりまいて設けられていることを特徴とする導電
体接液面の電流密度測定用センサ。
Two liquid-contacted electrodes are provided at the tip of an insulating cylindrical body in a mutually insulated state, and the liquid-contacted electrodes are arranged opposite each other at a predetermined distance in the length direction of the cylindrical body. A sensor for measuring current density of a surface in contact with a conductor, characterized in that at least one of the two is provided annularly surrounding the cylindrical body.
JP1986110548U 1986-07-18 1986-07-18 Expired JPH0425648Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1986110548U JPH0425648Y2 (en) 1986-07-18 1986-07-18

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1986110548U JPH0425648Y2 (en) 1986-07-18 1986-07-18

Publications (2)

Publication Number Publication Date
JPS6319260U JPS6319260U (en) 1988-02-08
JPH0425648Y2 true JPH0425648Y2 (en) 1992-06-19

Family

ID=30989651

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1986110548U Expired JPH0425648Y2 (en) 1986-07-18 1986-07-18

Country Status (1)

Country Link
JP (1) JPH0425648Y2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4968491U (en) * 1972-09-27 1974-06-14

Also Published As

Publication number Publication date
JPS6319260U (en) 1988-02-08

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