JPS61235755A - Detection electrode - Google Patents
Detection electrodeInfo
- Publication number
- JPS61235755A JPS61235755A JP7743985A JP7743985A JPS61235755A JP S61235755 A JPS61235755 A JP S61235755A JP 7743985 A JP7743985 A JP 7743985A JP 7743985 A JP7743985 A JP 7743985A JP S61235755 A JPS61235755 A JP S61235755A
- Authority
- JP
- Japan
- Prior art keywords
- detection electrode
- conductive fiber
- measured
- electrostatic voltmeter
- charge
- 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.)
- Granted
Links
Landscapes
- Measuring Leads Or Probes (AREA)
- Other Investigation Or Analysis Of Materials By Electrical Means (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は、帯電物の静電圧を測定するための検出電極
に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a detection electrode for measuring electrostatic voltage of a charged object.
帯電物の静電圧を測定するには二つの方法がある。その
一つは、被測定帯電物より電荷を集電し、その電荷が高
抵抗を通してアースに流れるときの電位差を測定するこ
とにより被測定帯電物の静電圧を知る方法(以下集電法
と云う)と、他の一つは、被測定帯電物のつくる電界中
に導体の電極を置き、その導体に生ずる誘導電荷を利用
して被測定帯電物の静電圧を測定する方法(以下静電誘
導法と云う]である。There are two methods to measure the electrostatic voltage of a charged object. One method is to collect electric charge from the charged object to be measured and measure the potential difference when the electric charge flows to the ground through a high resistance (hereinafter referred to as the current collection method). ), and the other method is to place a conductive electrode in the electric field created by the charged object to be measured, and use the induced charge generated in the conductor to measure the electrostatic voltage of the charged object to be measured (hereinafter referred to as electrostatic induction). It is called law.
コンデンサー型静電電圧計は、集電法による測定にも静
電誘導法による測定にも使用することのできる、クーロ
ン力を利用した、構造が簡単で、故障が少く、測定値に
対する信頼性の高い計器であるが、問題は、僅少ではあ
るが、漏洩コンダクタンスをもつことである。集電法に
よる測定の場合は、電荷が補給されるので問題はないが
、静電誘導法による測定は、漏洩電荷の無視できる短時
間内に限られる。Capacitor-type electrostatic voltmeters utilize Coulomb force, can be used for both current collection measurement and electrostatic induction measurement, and have a simple structure, less failure, and high reliability of measured values. Although it is a meter, the problem is that it has leakage conductance, although it is small. In the case of measurement using the current collection method, there is no problem since the charge is replenished, but the measurement using the electrostatic induction method is limited to a short time period in which leakage charge can be ignored.
しかしながら、集電法による測定は、被測定帯電物の電
圧変化に対する追随が一般に緩慢で敏速に帯電状態が変
化する被測定物に対しては静電誘導法を使用したい。コ
ンデンサー型静電電圧計を使用する場合、静電誘導法に
よる誘導電荷の発生が短時間で消滅し、次の測定に、そ
の誘導電荷が残らないような測定を継続して行う場合の
連続長期間測定は問題ないが、誘導電荷が常時連続的に
持続するような対象物に対する長期連続測定は、前述の
漏洩コンダクタンスのだめに、静電誘導法によっては、
不可能である。However, when measuring by the current collection method, it is generally slow to follow the voltage change of a charged object to be measured, and it is preferable to use the electrostatic induction method for a measured object whose charged state changes quickly. When using a capacitor-type electrostatic voltmeter, the induced charge generated by the electrostatic induction method disappears in a short period of time, and the induced charge does not remain in the next measurement for a continuous long period of time. There is no problem with measurements, but long-term continuous measurements on objects where induced charges are constantly sustained are difficult due to the leakage conductance mentioned above, depending on the electrostatic induction method.
It's impossible.
この発明は、被測定帯電物の帯電状態の変化に敏速に追
随でき、長期間の連続測定を可能にするコンデンサー型
静電電圧計用の検出電極を提供するものである。The present invention provides a detection electrode for a capacitor-type electrostatic voltmeter that can quickly follow changes in the charging state of a charged object to be measured and enables continuous measurement over a long period of time.
この発明の検出電極は、導電性の繊維層に導線の一端を
結合し、この導電性繊維層を、1個または、複数個の開
口部をもって絶縁物で被覆したもので、その導線の他の
一端をコンデンサー型静電電圧計に接続して被測定帯電
物の静電圧を測定するようにしたものである。The detection electrode of the present invention has one end of a conductive wire bonded to a conductive fiber layer, and this conductive fiber layer is covered with an insulating material with one or more openings. One end is connected to a capacitor-type electrostatic voltmeter to measure the electrostatic voltage of the charged object to be measured.
このような構造の検出電極を電界中に置くと絶縁物は誘
電分極を起し、この絶縁物に接している導電性繊細の部
分には、その誘電分極に応じた電荷が発生する。絶縁物
の開口部の導電性ll維層には直接に静電誘導による電
荷が発生しこれらの導電性繊維層に生じた電荷量と等量
で異種の極性をもった電荷が、その導線の他端に結合さ
れているコンデンサー型静電電圧計の電極に発生し、静
電電圧計が作動する。一方絶縁物に設けられた開口部に
は、微細な径の導電性繊維が露出しているので5被測定
帯電物との間にコロナ電流が流れ、静電電圧計の漏洩コ
ンダクタンスによる漏洩電荷を補給する。コロナ電流に
よる電荷の補給量は、絶縁物の孔の面積と検出電極の被
測定帯電物からの距離によって調整する。この発明を図
面を用いて、更に詳細に具体的に説明する。When a detection electrode with such a structure is placed in an electric field, dielectric polarization occurs in the insulator, and a charge corresponding to the dielectric polarization is generated in the delicate conductive portion that is in contact with the insulator. Charges are generated directly in the conductive fiber layers in the openings of the insulator due to electrostatic induction, and charges with a different polarity and an amount equal to the charge generated in these conductive fiber layers are generated in the conductive wire. It is generated at the electrode of the capacitor-type electrostatic voltmeter connected to the other end, and the electrostatic voltmeter is activated. On the other hand, since conductive fibers with a fine diameter are exposed in the opening provided in the insulator, a corona current flows between the charged object and the charged object to be measured, replenishing the leakage charge caused by the leakage conductance of the electrostatic voltmeter. do. The amount of charge replenishment by the corona current is adjusted by the area of the hole in the insulator and the distance from the charged object to be measured between the detection electrode. This invention will be specifically explained in more detail with reference to the drawings.
第1図は′、この発明の検出電極をコンデンサー型静電
電圧計に接続した場合の機能を説明するための略図であ
り、第2図は第1図の等価回路である。FIG. 1 is a schematic diagram for explaining the function when the detection electrode of the present invention is connected to a capacitor type electrostatic voltmeter, and FIG. 2 is an equivalent circuit of FIG. 1.
第1図において、1は被測定帯電物で、この場合、正に
帯電しているものとする。2は開口部3をもった絶縁物
で導電性繊維層4を覆っている。導電性繊維層4には導
線5の一端が結合され、他端はコンデンサー型静電電圧
計の固定電極に接続されている。コンデンサー型静電電
圧計の可動電極7は接地されている。In FIG. 1, reference numeral 1 denotes a charged object to be measured, which in this case is assumed to be positively charged. 2 covers the conductive fiber layer 4 with an insulator having openings 3. One end of a conductive wire 5 is connected to the conductive fiber layer 4, and the other end is connected to a fixed electrode of a capacitor type electrostatic voltmeter. The movable electrode 7 of the capacitor type electrostatic voltmeter is grounded.
被測定帯電物1の帯電電荷によって生じた電界中に、こ
の発明の検出電極を置くと、導電性繊維層4を覆ってい
る絶縁物は、誘導分極を起し、外側が負に、導電性繊維
層4に接している内側は正に分極し、従って導電性繊維
層4には負の電荷が生じ、絶縁物の開口部で被測定帯電
物よりの電気力線が直接到達する導電性繊維層も負に帯
電する。これらの導電性繊維層に生じた電荷と等量の正
の電荷が、導線5に接続されているコンデンサー型静電
電圧計の固定電極6に生じ、この電荷により静電電圧計
が作動する。When the detection electrode of the present invention is placed in an electric field generated by the charged charge of the charged object 1 to be measured, the insulating material covering the conductive fiber layer 4 causes induced polarization, and the outside becomes negative and the conductive The inner side that is in contact with the fiber layer 4 is positively polarized, so a negative charge is generated in the conductive fiber layer 4, and the conductive fiber is directly reached by the lines of electric force from the charged object to be measured at the opening of the insulator. The layer is also negatively charged. A positive charge equal to the charge generated in these conductive fiber layers is generated on the fixed electrode 6 of the capacitor-type electrostatic voltmeter connected to the conductive wire 5, and the electrostatic voltmeter is activated by this charge.
しかしながら、静電電圧計には漏洩コンダクタンスがあ
るため固定電極に生じた電荷は減少して行くので電荷の
補充がなげれば静電電圧計の指示は減少して行く。However, since the electrostatic voltmeter has leakage conductance, the charge generated on the fixed electrode decreases, and if the charge is not replenished, the reading on the electrostatic voltmeter will decrease.
この電荷の補充が、検出電極の被覆絶縁物2の開口部3
に露出している導電性繊維によって行われる。導電性繊
維は、その微細な寸度のため、電気力線の密度が大きく
、従ってコロナ電流が発生する。このコロナ電流によっ
て、コンデンサー型静電電圧計の固定電極6より逃げる
電荷が補給される。The replenishment of this charge is caused by the opening 3 of the insulating coating 2 of the detection electrode.
This is done by conductive fibers that are exposed to the Due to their fine size, conductive fibers have a high density of electric lines of force, thus generating corona currents. This corona current replenishes the charge that escapes from the fixed electrode 6 of the capacitor type electrostatic voltmeter.
これを等価回路で示すと第2図のようになる。This is shown in an equivalent circuit as shown in FIG.
第2図のC1は被測定帯電物と検出電極との間の静電容
量1glは被測定帯、型物と検出電極との間のコロナ電
流に対するコンダクタンス、C2およびg2はそれぞれ
コンデンサー型静電電圧計の静電容量および漏洩コンダ
クタンスである。In Figure 2, C1 is the electrostatic capacitance between the charged object to be measured and the detection electrode, 1 gl is the conductance for the corona current between the band to be measured and the molded object and the detection electrode, and C2 and g2 are each a capacitor-type electrostatic voltmeter. are the capacitance and leakage conductance of
被測定帯電物の静電圧をEとすればg++g2に −
電流が流れないときには静電電圧計は、lE
C5+ C2
の電圧を示すが最終的には静電電圧計の指示は。If the electrostatic voltage of the charged object to be measured is E, it becomes g++g2 −
When no current flows, the electrostatic voltmeter shows a voltage of lE C5+ C2, but the final reading of the electrostatic voltmeter is .
J
g+ + g2
となる。それ故、各コンダクタンスをそれぞれの静電容
量に比例するようにとれれば、静電誘導によって得られ
た指示は変化せず、迅速な指示が得られる。J g+ + g2. Therefore, if each conductance can be made proportional to each capacitance, the indication obtained by electrostatic induction will not change and a quick indication can be obtained.
コンデンサー型静電電圧計はそれ自体静電容量が変化す
るが、その変化量は比較的少いのでできるだけ各静電容
量に比例するようなコンダクタンスを持たせるようにす
ることにより、比較的迅速に最終指示値に近づけること
ができる。A capacitor type electrostatic voltmeter itself changes in capacitance, but the amount of change is relatively small, so by making the conductance proportional to each capacitance as much as possible, the final result can be determined relatively quickly. It is possible to get close to the indicated value.
コンダクタンスg1の調整は、・導電性繊維の種類、開
口部の大きさ、被測定帯電物よりの距離などにより行い
、コンダクタンスg2の調整は、調整用のコンダクタン
スを付加するなどの方法も採用することができる。また
静電容量CIは検出電極の大きさ、被測定帯電物と検出
電極との距離および導電性繊維の量などによって変化さ
せることができるので、測定現場の状況に応じて、適当
な検出電極を選定使用する。Adjustment of conductance g1 should be carried out by adjusting the type of conductive fiber, size of the opening, distance from the charged object to be measured, etc., and adjustment of conductance g2 should also be done by adding a conductance for adjustment. Can be done. In addition, the capacitance CI can be changed depending on the size of the detection electrode, the distance between the charged object to be measured and the detection electrode, the amount of conductive fibers, etc., so select an appropriate detection electrode depending on the situation at the measurement site. Use selectively.
従って、この発明の検出電極には色々の形状寸度のもの
が考えられるが、第3図に一実施例を示す。Therefore, the detection electrode of the present invention may have various shapes and sizes, and one embodiment is shown in FIG.
第3図の実施例において、電極形状を保持するための絶
縁体のバイブロの周囲に導電性繊維層4を設け、その外
側を開口部3をもった絶縁性の収縮チューブ2で被覆し
たもので、導電性繊維4の一端には導線5が結合されて
いる。In the embodiment shown in FIG. 3, a conductive fiber layer 4 is provided around the insulating vibro to maintain the electrode shape, and the outside of the conductive fiber layer 4 is covered with an insulating shrink tube 2 having an opening 3. , a conductive wire 5 is coupled to one end of the conductive fiber 4.
第1図は、この発明の検出電極コンデンサー型静電電圧
計に接続した場合の機能を説明するための略図であり、
第2図は第1図の等価回路図である。
第3図は、この発明の検出電極の一実施例を示す斜面図
である。FIG. 1 is a schematic diagram for explaining the function when connected to the detection electrode capacitor type electrostatic voltmeter of the present invention.
FIG. 2 is an equivalent circuit diagram of FIG. 1. FIG. 3 is a perspective view showing one embodiment of the detection electrode of the present invention.
Claims (1)
数個の開口部をもった絶縁物で被覆したコンデンサー型
静電電圧計によって静電圧を測定するための検出電極。A detection electrode for measuring static voltage with a capacitor-type electrostatic voltmeter, in which the outside of a conductive fiber layer bonded to a conductive wire is covered with an insulator having one or more openings.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7743985A JPH0623783B2 (en) | 1985-04-11 | 1985-04-11 | Detection electrode |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7743985A JPH0623783B2 (en) | 1985-04-11 | 1985-04-11 | Detection electrode |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS61235755A true JPS61235755A (en) | 1986-10-21 |
JPH0623783B2 JPH0623783B2 (en) | 1994-03-30 |
Family
ID=13634052
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7743985A Expired - Lifetime JPH0623783B2 (en) | 1985-04-11 | 1985-04-11 | Detection electrode |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0623783B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013234907A (en) * | 2012-05-09 | 2013-11-21 | Ulvac Japan Ltd | Surface potential measuring device |
-
1985
- 1985-04-11 JP JP7743985A patent/JPH0623783B2/en not_active Expired - Lifetime
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013234907A (en) * | 2012-05-09 | 2013-11-21 | Ulvac Japan Ltd | Surface potential measuring device |
Also Published As
Publication number | Publication date |
---|---|
JPH0623783B2 (en) | 1994-03-30 |
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