JPH0632256B2 - Method of measuring leakage current of lightning arrester - Google Patents
Method of measuring leakage current of lightning arresterInfo
- Publication number
- JPH0632256B2 JPH0632256B2 JP31714687A JP31714687A JPH0632256B2 JP H0632256 B2 JPH0632256 B2 JP H0632256B2 JP 31714687 A JP31714687 A JP 31714687A JP 31714687 A JP31714687 A JP 31714687A JP H0632256 B2 JPH0632256 B2 JP H0632256B2
- Authority
- JP
- Japan
- Prior art keywords
- leakage current
- fundamental wave
- zero point
- measuring
- point position
- 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
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- Testing Of Short-Circuits, Discontinuities, Leakage, Or Incorrect Line Connections (AREA)
- Testing Electric Properties And Detecting Electric Faults (AREA)
- Thermistors And Varistors (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、たとえば酸化亜鉛などを主成分とする非直
線性抵抗体を用いて構成した避雷器の前記抵抗体の劣化
の有無もしくは劣化の程度を判定するため、常時の運転
電圧のもとにこの抵抗体を通過する,いわゆる漏れ電流
を精度よく測定するための測定方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial application] The present invention relates to the presence or absence of deterioration of the resistor of a lightning arrester constituted by using a non-linear resistor containing zinc oxide as a main component, or the degree of deterioration. The present invention relates to a measuring method for accurately measuring a so-called leakage current that passes through this resistor under a constant operating voltage for determining.
酸化亜鉛などを主成分とした,非直線性の強い抵抗体を
用いることにより直列ギャップが省略された避雷器の等
価回路は、第2図に示すように、非直線性抵抗Rと、抵
抗体自体の静電容量を含む避雷器の静電容量Cとが並列
接続されたものとみなすことができる。従って避雷器の
接地線に流れる電流iOは非直線性抵抗Rを流れる抵抗分
漏れ電流iRと静電容量Cを流れる静電容量分電流iCとが
合成された電流となる。As shown in FIG. 2, the equivalent circuit of a lightning arrester in which the series gap is omitted by using a resistor having a strong non-linearity, which mainly contains zinc oxide, is shown in FIG. It can be considered that the arrester electrostatic capacitance C including the electrostatic capacitance of is connected in parallel. Therefore, the current i O flowing through the grounding wire of the lightning arrester becomes a current obtained by combining the resistance leakage current i R flowing through the non-linear resistance R and the capacitance current i C flowing through the capacitance C.
このうち、抵抗分漏れ電流iRは抵抗体の劣化の有無もし
くは劣化の程度を判定するのに重要であるため、従来か
ら、全漏れ電流iOから抵抗分漏れ電流iRを分離して測定
する種々の方法が考案されている。一例をあげれば、避
雷器と並列にコンデンサを接続し、抵抗体が劣化してい
ない状態では避雷器の静電容量分電流iCが抵抗分漏れ電
流iRよりもはるかに大きく従って全漏れ電流iOは実質的
に静電容量分電流iCに等しくなることを利用して、前記
並列に接続されたコンデンサを流れる電流が全漏れ電流
iOと等しくなるようにコンデンサ容量を調整した上で、
全漏れ電流と前記並列コンデンサを流れる電流との差電
流が得られる2次回路を構成して両電流の位相差に基づ
く抵抗分漏れ電流を得るものである。また、この方法に
よれば、抵抗体が劣化していても劣化の程度が小さけれ
ば、比較的良好な近似で抵抗分漏れ電流を求めることが
できる。Of these, since the resistance leakage current i R is important for determining the presence or absence of deterioration of the resistor or the degree of deterioration, conventionally, the resistance leakage current i R is separated from the total leakage current i O and measured. Various methods have been devised. As an example, when a capacitor is connected in parallel with the arrester and the resistance of the arrester is not deteriorated, the capacitance component current i C of the arrester is much larger than the resistance component leakage current i R , so the total leakage current i O Is substantially equal to the capacitance current i C , the current flowing through the capacitors connected in parallel is the total leakage current.
After adjusting the capacitor capacity to be equal to i O ,
A secondary circuit that obtains a difference current between the total leakage current and the current flowing through the parallel capacitor is configured to obtain a resistance leakage current based on the phase difference between the two currents. Further, according to this method, even if the resistor is deteriorated, if the degree of deterioration is small, the resistance leakage current can be obtained with a relatively good approximation.
また、上記の例によるコンデンサの代わりに計器用変圧
器を避雷器に並列に接続するとともに計器用変圧器の低
圧側にコンデンサを接続し、以下上記例と同様にして抵
抗分漏れ電流を得ることもできる。Also, instead of the capacitor according to the above example, connecting a voltage transformer for the lightning arrestor in parallel and connecting a capacitor on the low-voltage side of the voltage transformer, it is also possible to obtain the resistance leakage current in the same manner as in the above example. it can.
さらに、特開昭61−78086号公報に開示されているよう
に、全漏れ電流iOのピーク値位置を検出し、この位置か
ら90゜ずれた位置における電流瞬時値を抵抗分漏れ電流
として測定する方法もある。Further, as disclosed in JP-A-61-78086, the peak value position of the total leakage current i O is detected, and the instantaneous current value at a position deviated by 90 ° from this position is measured as a resistance leakage current. There is also a way to do it.
前記従来の測定方法のうち、避雷器と並列にコンデンサ
や計器用変圧器を接続する方法では、並列に接続される
コンデンサや計器用変圧器が高圧線路に接続される機器
故に高価となり、また既存の設備で避雷器と並列にコン
デンサや計器用変圧器が接続されていない場合には、こ
の方法の適用は困難である。Among the conventional measuring methods, in the method of connecting a capacitor or an instrument transformer in parallel with a lightning arrester, the capacitor or instrument transformer connected in parallel becomes expensive because it is a device connected to a high voltage line, and the existing This method is difficult to apply when the equipment does not have a capacitor or a transformer for instrument connected in parallel with the arrester.
また、特開昭61−78086号公報による測定方法では抵抗
分漏れ電流iRが全漏れ電流iOに比し十分に小さい場合す
なわち劣化が進行していない場合には有効であるが、抵
抗分漏れ電流iRが大きい場合には、全漏れ電流iOのピー
ク値位置と抵抗分漏れ電流iRのピーク値位置との位相差
は90゜より小さくなるため、抵抗分漏れ電流を十分な精
度で測定することができないという問題点がある。Further, the measuring method according to Japanese Patent Laid-Open No. 61-78086 is effective when the resistance component leakage current i R is sufficiently smaller than the total leakage current i O , that is, when the deterioration has not progressed, but the resistance component When the leakage current i R is large, the phase difference between the peak value position of the total leakage current i O and the peak value position of the resistance leakage current i R is smaller than 90 °, so the resistance leakage current is There is a problem that it cannot be measured at.
この発明の目的は、高価なコンデンサや計器用変圧器を
必要とせず、避雷器の全漏れ電流iOのみの測定により抵
抗分漏れ電流を簡易にかつ精度よく測定することのでき
る測定方法を提供することである。An object of the present invention is to provide a measuring method capable of easily and accurately measuring a resistance leakage current by measuring only a total leakage current i O of a lightning arrester without requiring an expensive capacitor or an instrument transformer. That is.
上記目的を達成するために、この発明によれば、非直線
性抵抗体を用いて構成した避雷器の接地線に流れる全漏
れ電流を基本波と高調波とに分離し、両者の位相差を、
前記分離された基本波波形の適宜に着目された零点位置
とこの零点位置以降に存在する,前記高調波中の最小次
数高調波の零点位置であって該零点を通過する波形の傾
斜方向が前記基本波波形の零点位置の傾斜方向と反対と
なる零点位置との間で求められる複数の位相差中の最小
位相差として基本波の電気角の尺度で求めるとともに、
この位相差と前記分離された基本のピーク値とから抵抗
分漏れ電流を測定するものとする。In order to achieve the above object, according to the present invention, the total leakage current flowing in the grounding wire of the arrester configured using a non-linear resistor is separated into a fundamental wave and a harmonic wave, and the phase difference between the two is
An appropriately focused zero point position of the separated fundamental wave waveform and a zero point position of the minimum order higher harmonic wave in the harmonics existing after this zero point position, and the inclination direction of the waveform passing through the zero point is Along with determining the electrical angle of the fundamental wave as the minimum phase difference among the multiple phase differences obtained between the zero point position and the opposite zero point position of the fundamental wave waveform,
The resistance leakage current is measured from this phase difference and the separated basic peak value.
本発明は、避雷器を構成する抵抗体の有する非直線特性
のため、抵抗分漏れ電流の半周期の波形が中央部に高い
ピーク値を有し、両裾野に向かって対称にかつ急速に減
衰する波形を有することに着目したものである。以下に
本発明による測定方法の原理につき説明する。According to the present invention, due to the non-linear characteristic of the resistor forming the lightning arrester, the waveform of a half cycle of the resistance leakage current has a high peak value in the central portion and is symmetrically and rapidly attenuated toward both skirts. It focuses on having a waveform. The principle of the measuring method according to the present invention will be described below.
抵抗分漏れ電流iRは、上述のように、その半周期の波形
が、中央部において高いピーク値を有し、このピーク値
から両裾野に向かって対称にかつ急速に減衰する波形を
有するから、基本波成分のほかに奇数次の高調波分を多
く含んでいる。各次数成分のピーク値をそれぞれR1,R
3,R5,…………とすると、iRは次式で表すことができ
る。As described above, the resistance leakage current i R has a waveform whose half cycle has a high peak value in the central portion and has a waveform which is symmetrically and rapidly attenuated from this peak value toward both skirts. , In addition to the fundamental wave component, it contains many odd harmonics. The peak value of each order component is R 1 , R
I R can be expressed by the following equation, where 3 , R 5 , ....
iR=R1 sin ωt+R3 sin 3ωt+ R5 sin 5ωt+ ……………(1) 一方、静電容量分電流iCはiRより位相が90゜進んでいる
から、ピーク値をC1 とすると次式で表すことができ
る。i R = R 1 sin ωt + R 3 sin 3ωt + R 5 sin 5ωt + ……………… (1) On the other hand, the capacitance component current i C is 90 ° ahead of i R , so the peak value is C 1 . Then, it can be expressed by the following equation.
iC=C1 sin (ωt +90゜) (2) 全漏れ電流iOはiRとiCとの合成されたものであるから、
次式で表される。i C = C 1 sin (ωt + 90 °) (2) Since the total leakage current i O is a combination of i R and i C ,
It is expressed by the following equation.
ここで、φは、合成後の基本波の波形の零点位置と、こ
の零点位置につづく合成前抵抗分漏れ電流零点位置との
間の時間差を電気角で表した位相差であり、次式で表す
ことができる。 Here, φ is the phase difference expressed in electrical angle between the zero point position of the waveform of the fundamental wave after the synthesis and the zero point position of the resistance leakage current before the synthesis that follows this zero point position. Can be represented.
φtan-1(C1 /R1) (4) また、前漏れ電流iO中の基本波のピーク値は(3)式から であるから、(4),(5)式をC1 について解くと、 が得られる。従って抵抗分漏れ電流iRが計測された全漏
れ電流から静電容量分電流C1 sin (ωt+90゜)=C
1 cos ωtを差し引くことにより求められる。このため
には、計測された全漏れ電流を基本波成分と高調波成分
とに分離して基本波成分の波高値を求めるとともに、こ
の基本波成分の零点位置と、この零点位置につづく,抵
抗分漏れ電流のみにおける基本波の零点位置との時間差
(位相差)を前記分離された波形から求めなければなら
ない。φtan -1 (C 1 / R 1 ) (4) In addition, the peak value of the fundamental wave in the front leakage current i O can be calculated from equation (3). Therefore, solving equations (4) and (5) for C 1 gives Is obtained. Therefore, the resistance leakage current i R is calculated from the total leakage current, and the capacitance current C 1 sin (ωt + 90 °) = C
It is obtained by subtracting 1 cos ωt. To this end, the measured total leakage current is divided into a fundamental wave component and a harmonic component to obtain the peak value of the fundamental wave component, and the zero point position of this fundamental wave component and the resistance following this zero point position The time difference (phase difference) from the zero point position of the fundamental wave only in the partial leakage current must be obtained from the separated waveform.
ところで、前述したように、抵抗分漏れ電流の波形は中
央部に高いピーク値を有し両裾野へ向かって対称にかつ
急速に減衰する波形であり、しかもこの波形は、基本波
成分と、この基本波成分の零点を基本波波形と逆方向の
傾斜をもって通過する第3次高調波成分とにより実質的
に定まるから、着目した基本波成分の零点位置と、分離
された第3次高調波成分の波形において前記着目した基
本波の零点位置における基本波波形の傾斜方向と逆方向
の傾斜となる,前記基本波の零点位置以降にある複数の
零点位置との間で時間差を求め、この時間差中の最小値
を基本波の電気角の目盛りで表せば、前記(4)式で表さ
れる位相角を得ることができる。By the way, as described above, the waveform of the resistance leakage current is a waveform that has a high peak value in the central portion and is symmetrically and rapidly attenuated toward both skirts. Since the zero point of the fundamental wave component is substantially determined by the third harmonic component that passes through the fundamental wave waveform with an inclination in the opposite direction, the zero point position of the focused fundamental wave component and the separated third harmonic component In the waveform of, the time difference is obtained between a plurality of zero point positions after the zero point position of the fundamental wave, which has a slope in the opposite direction to the inclination direction of the fundamental wave waveform at the zero point position of the focused fundamental wave, If the minimum value of is represented by the scale of the electrical angle of the fundamental wave, the phase angle represented by the above equation (4) can be obtained.
このように、全漏れ電流を基本波成分と高調波成分とに
分離することにより、全漏れ電流中の基本波成分波高値
と、直接測定では不可能な,全漏れ電流と抵抗分漏れ電
流とにおける基本波成分相互間の位相差とを求めること
が可能となり、従来のように高価なコンデンサや計器用
変圧器を用いることなく、かつ抵抗分漏れ電流が増大し
た場合にも精度よくこの抵抗分漏れ電流を求めことがで
きる。Thus, by separating the total leakage current into the fundamental wave component and the harmonic components, the peak value of the fundamental wave component in the total leakage current and the total leakage current and the resistance component leakage current that cannot be measured directly. It becomes possible to obtain the phase difference between the fundamental wave components in the, and the resistance component can be accurately measured even when the leakage current increases due to the resistance component without using the expensive capacitor and the transformer for instrument as in the past. The leakage current can be obtained.
第1図に、本発明の方法による漏れ電流測定を可能なら
しめる測定器構成の一実施例を示す。FIG. 1 shows an embodiment of a measuring instrument structure which enables the leakage current measurement by the method of the present invention.
避雷器1は高圧線路HVと大地Eとの間に挿入されてい
る。避雷器1の接地線2に流れる全漏れ電流iOは変流器
3によって検出され測定器4に入力される。変流器3と
して鉄心を2つ割り構造としたクランプ型変流器を用い
ると、接地線を着脱することなくiOを検出することがで
き好都合である。The lightning arrester 1 is inserted between the high voltage line HV and the ground E. The total leakage current i O flowing through the ground wire 2 of the lightning arrester 1 is detected by the current transformer 3 and input to the measuring device 4. If a clamp type current transformer having a split iron core structure is used as the current transformer 3, i O can be conveniently detected without attaching or detaching the ground wire.
測定器4は、入力された全漏れ電流iOの1サイクル分を
微小時間に分割し、この分割された各瞬時における電流
値を記憶するサンプリング手段4aと、この記憶された
各瞬時の電流値を用いて演算処理を行い、全漏れ電流iO
を基本波成分と高調波成分とに分離する,フィルタの役
目を果たす分離手段4bと、分離された基本波のピーク
値と、このピーク値につづく零点と、この零点位置にお
ける波形の傾斜方向とを検出する基本波データ検出手段
4cと、前記零点検出の信号を受けて波形の傾斜方向が
前記基本波の傾斜方向と逆になる第3高調波の零点位置
を検出する高調波データ検出手段4dと、基本波データ
検出手段4cにより検出された零点位置と高調波データ
検出手段4dにより検出された零点位置との時間差を求
めるとともにこの時間差中最小時間差を選択して基本波
の電気角の目盛で表して出力する位相差検出手段4e
と、前記基本波データ検出手段4cにより検出された基
本波のピーク値と前記位相差検出手段4eから出力され
た位相差とを用いて静電容量性電流のピーク値を求める
とともに、このピーク値を用いて抵抗分漏れ電流波形を
演算する演算手段4fと、演算手段4fにより得られた
抵抗分漏れ電流波形もしくはその波高値を表示する表示
手段4gとを用いて構成されている。従って、この測定
器4への全漏れ電流の入力から抵抗分漏れ電流の表示ま
での測定工程がすべけ自動的に進行するから、この測定
器4と、たとえばクランプ型変流器3とのみを用意する
ことにより、コンデンサや計器用変圧器が避雷器と並列
に接続されておらず、従って従来の方法では避雷器の劣
化判定が不可能な既存の設備においても測定準備のため
の運転中断を伴うことなく極めて容易にかつ精度高く避
雷器の抵抗分漏れ電流を測定することができる。The measuring device 4 divides one cycle of the input total leakage current i O into minute times and stores the current value at each divided moment, and a sampling means 4a and the stored current value at each moment. To calculate the total leakage current i O
Separating means 4b for separating a fundamental wave component and a harmonic wave component, which serves as a filter, a peak value of the separated fundamental wave, a zero point following the peak value, and a slope direction of the waveform at the zero point position. And a harmonic wave data detecting means 4d for detecting the zero point position of the third harmonic wave in which the inclination direction of the waveform is opposite to the inclination direction of the fundamental wave in response to the zero point detection signal. And the time difference between the zero point position detected by the fundamental wave data detecting means 4c and the zero point position detected by the harmonic wave data detecting means 4d is obtained, and the minimum time difference among the time differences is selected and the electrical angle scale of the fundamental wave is selected. Phase difference detecting means 4e for expressing and outputting
And the peak value of the fundamental wave detected by the fundamental wave data detecting means 4c and the phase difference output from the phase difference detecting means 4e, the peak value of the capacitive current is obtained, and the peak value is obtained. And a display means 4g for displaying the resistance leakage current waveform obtained by the calculation means 4f or the peak value thereof. Therefore, since the measuring process from the input of the total leakage current to the measuring device 4 to the display of the resistance leakage current is automatically performed, only the measuring device 4 and, for example, the clamp type current transformer 3 are connected. By preparing, the capacitor and the transformer for the instrument are not connected in parallel with the lightning arrester, and therefore the existing equipment, which cannot judge the deterioration of the lightning arrester by the conventional method, must be interrupted for the preparation for measurement. It is possible to measure the resistance component leakage current of the lightning arrester extremely easily and highly accurately.
以上に述べたように、本発明によれば、非直線性抵抗体
を用いて構成した避雷器の接地線に流れる全漏れ電流を
基本波と高調波とに分離し、両者の位相差を、前記分離
された基本波波形の適宜に着目された零点位置とこの零
点位置以降に存在する,前記高調波中の最小次数高調波
の零点位置であって該零点を通過する波形の傾斜方向が
前記基本波波形の零点位置の傾斜方向と反対となる零点
位置との間で求められる複数の位相差中の最小位相差と
して基本波の電気角の尺度で求めるとともに、この位相
差と前記分離された基本波のピーク値とから抵抗分漏れ
電流を測定するようにしたので、避雷器の劣化に直接関
係する抵抗分漏れ電流の大小にかかわらずこの漏れ電流
を精度よく測定することができ、従来のように高価なコ
ンデンサや計器用変圧器を用いることなく適確な劣化判
定が可能になる。また、この測定方法は、全漏れ電流の
入力から抵抗分漏れ電流の表示までの全測定工程をマイ
クロコンピュータを用いて自動的に進行させることが可
能な方法であるから、マイクロコンピュータを用いて構
成された測定器と、避雷器の接地線に流れる全漏れ電流
を測定するための,たとえばクランプ型変流器とを用意
するのみで、抵抗分漏れ電流測定手段を備えない既存の
設備に対しても、測定準備のための運転中断を伴うこと
なく、抵抗分漏れ電流の測定が可能になる。As described above, according to the present invention, the total leakage current flowing in the grounding wire of the arrester configured by using the non-linear resistor is separated into the fundamental wave and the harmonics, and the phase difference between them is An appropriately focused zero point position of the separated fundamental wave waveform and the zero point position of the minimum order higher harmonic wave in the higher harmonic wave existing after this zero point position, and the inclination direction of the waveform passing through the zero point is the basic point. The minimum phase difference among the multiple phase differences obtained between the zero point position and the opposite zero point position of the wave waveform is obtained on the scale of the electrical angle of the fundamental wave, and this phase difference and the separated basic Since the resistance leakage current is measured from the peak value of the wave, this leakage current can be accurately measured regardless of the magnitude of the resistance leakage current that is directly related to the deterioration of the arrester. For expensive capacitors and instruments Allowing accurately degradation determination without using the divider. In addition, this measurement method is a method that can automatically advance all measurement steps from the input of the total leakage current to the display of the resistance leakage current by using a microcomputer. For the existing equipment that does not have the resistance leakage current measuring means, only the prepared measuring instrument and the total leakage current flowing through the grounding wire of the arrester are prepared, for example, a clamp type current transformer. In addition, the resistance leakage current can be measured without interrupting the operation for preparation for measurement.
第1図は本発明の漏れ電流測定方法を可能ならしめる測
定器構成の一実施例を示す機能ブロック図、第2図は避
雷器の等価回路図である。 1……避雷器、2……接地線、3……変流器、4……測
定器、4a……サンプリング手段、4b……分離手段、
4c……基本波データ検出手段、4d……高調波データ
検出手段、4e……位相差検出手段、4f……演算手
段、4g……表示手段、iR……抵抗分漏れ電流、iO……
全漏れ電流。FIG. 1 is a functional block diagram showing an embodiment of a measuring device configuration that enables the leakage current measuring method of the present invention, and FIG. 2 is an equivalent circuit diagram of a lightning arrester. 1 ... Lightning arrester, 2 ... Ground wire, 3 ... Current transformer, 4 ... Measuring instrument, 4a ... Sampling means, 4b ... Separation means,
4c ...... fundamental data detecting means, 4d ...... harmonic data detecting means, 4e ...... phase difference detecting means, 4f ...... calculating means, 4g ...... Display unit, i R ...... resistive leakage current, i O ... …
Total leakage current.
Claims (2)
接地線に流れる全漏れ電流を基本波と高調波とに分離
し、両者の位相差を、前記分離された基本波波形の適宜
に着目された零点位置とこの零点位置以降に存在する,
前記高調波中の最小次数高調波の零点位置であって該零
点を通過する波形の傾斜方向が前記基本波波形の零点位
置の傾斜方向と反対となる零点位置との間で求められる
複数の位相差中の最小位相差として基本波の電気角の尺
度で求めるとともに、この位相差と前記分離された基本
波のピーク値とから抵抗分漏れ電流を測定することを特
徴とする避雷器の漏れ電流測定方法。1. A total leakage current flowing through a grounding wire of a lightning arrester constructed by using a non-linear resistor is separated into a fundamental wave and a harmonic wave, and a phase difference between the two is appropriately determined based on the waveform of the separated fundamental wave. Exists at the zero point position focused on and after this zero point position,
A plurality of positions determined between the zero point position of the zero-order position of the lowest order harmonic in the harmonic and the inclination direction of the waveform passing through the zero point is opposite to the inclination direction of the zero point position of the fundamental wave waveform. Measured as a minimum phase difference in the phase difference on the scale of the electrical angle of the fundamental wave, and measuring the leakage current of the surge arrester characterized by measuring the resistance component leakage current from this phase difference and the peak value of the separated fundamental wave Method.
方法において、接地線に流れる全漏れ電流の基本波と高
調波とへの分離から抵抗分漏れ電流測定に到る全測定工
程はマイクロコンピュータを用いて自動的に進められる
ことを特徴とする避雷器の漏れ電流測定方法。2. The leakage current measuring method according to claim 1, wherein all the measuring steps from the separation of the total leakage current flowing through the ground wire into the fundamental wave and the harmonic wave to the resistance leakage current measurement are performed. A method of measuring a leakage current of a lightning arrester, which is characterized by being automatically advanced by using a microcomputer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31714687A JPH0632256B2 (en) | 1987-12-15 | 1987-12-15 | Method of measuring leakage current of lightning arrester |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31714687A JPH0632256B2 (en) | 1987-12-15 | 1987-12-15 | Method of measuring leakage current of lightning arrester |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01159988A JPH01159988A (en) | 1989-06-22 |
| JPH0632256B2 true JPH0632256B2 (en) | 1994-04-27 |
Family
ID=18084953
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP31714687A Expired - Lifetime JPH0632256B2 (en) | 1987-12-15 | 1987-12-15 | Method of measuring leakage current of lightning arrester |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0632256B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4633513B2 (en) * | 2005-01-13 | 2011-02-16 | 関西電力株式会社 | Degradation diagnosis method for lightning arresters |
| CN113267726A (en) * | 2021-06-16 | 2021-08-17 | 江苏大学 | Fault harmonic current detection device and method for permanent magnet synchronous motor |
-
1987
- 1987-12-15 JP JP31714687A patent/JPH0632256B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01159988A (en) | 1989-06-22 |
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