JPH0645270Y2 - Insulation resistance measuring device - Google Patents
Insulation resistance measuring deviceInfo
- Publication number
- JPH0645270Y2 JPH0645270Y2 JP7806588U JP7806588U JPH0645270Y2 JP H0645270 Y2 JPH0645270 Y2 JP H0645270Y2 JP 7806588 U JP7806588 U JP 7806588U JP 7806588 U JP7806588 U JP 7806588U JP H0645270 Y2 JPH0645270 Y2 JP H0645270Y2
- Authority
- JP
- Japan
- Prior art keywords
- distribution line
- phase
- voltage
- resistance
- impedance
- 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
Links
Landscapes
- Measurement Of Resistance Or Impedance (AREA)
Description
【考案の詳細な説明】 〔産業上の利用分野〕 本考案は、3相低圧配電線路などの多相低圧配電線路の
絶縁抵抗を測定する絶縁抵抗測定装置に関する。[Detailed Description of the Invention] [Industrial field of application] The present invention relates to an insulation resistance measuring device for measuring the insulation resistance of a multi-phase low-voltage distribution line such as a 3-phase low-voltage distribution line.
従来、多相低圧配電線路である3相低圧配電線路の絶縁
劣化の監視は、多くの場合、絶縁抵抗計を用いた手動計
測によつて配電線路の絶縁抵抗を測定するとともに、そ
の測定結果にもとづき、絶縁抵抗の良,不良を判別して
行われ、この場合、煩雑かつ危険を伴う測定作業,測定
結果の判別作業などを要する。Conventionally, for monitoring insulation deterioration of a three-phase low-voltage distribution line, which is a multi-phase low-voltage distribution line, in many cases, the insulation resistance of the distribution line is measured by manual measurement using an insulation resistance meter, and First, the insulation resistance is judged to be good or bad. In this case, complicated and dangerous measurement work and measurement result judgment work are required.
そこで、配電線路の中性点に低周波の電圧信号を注入し
て配電線路の絶縁抵抗を自動測定し、絶縁劣化の自動監
視を行う絶縁監視装置が考案されている。Therefore, an insulation monitoring device has been devised which injects a low-frequency voltage signal into the neutral point of the power distribution line to automatically measure the insulation resistance of the power distribution line and automatically monitors the insulation deterioration.
そして、前記監視装置に用いられる従来の絶縁抵抗測定
装置は、マイクロプロセツサの自動制御により、配電線
路の送電交流(50Hz又は60Hz)と異なる所定周波数fの
低周波の電配信号を配電線路の非接地の中性点に零相電
圧として注入するとともに、零相変成器(ZCT)などを
用いて配電線路の零相電流を検出し、前記電圧信号の注
入にもとづく配電線路の零相電圧,電流を測定する。Then, the conventional insulation resistance measuring device used for the monitoring device, by automatic control of the microprocessor, transmits a low-frequency distribution signal of a predetermined frequency f different from the transmission AC (50 Hz or 60 Hz) of the distribution line to the distribution line. While injecting as a zero-phase voltage to the ungrounded neutral point, the zero-phase transformer (ZCT) is used to detect the zero-phase current of the distribution line, and the zero-phase voltage of the distribution line based on the injection of the voltage signal, Measure the current.
さらに、零相電圧,電流の測定値(ベクトル値),
にもとづき、その実効値V,I及び,の位相角θを算
出するとともに、実効値V,I及び位相角θにもとづき、
配電線路のインピーダンスの抵抗成分r,リアクタンス成
分xをr=V/(Icosθ),x=1/(2πfC)=V/(Isin
θ):(Cは容量)の式から算出し、抵抗成分rを絶縁
抵抗の測定値として出力する。In addition, zero-phase voltage and current measurement values (vector values),
Based on the effective value V, I and the phase angle θ of the, and based on the effective value V, I and the phase angle θ,
The resistance component r and the reactance component x of the impedance of the distribution line are r = V / (Icosθ), x = 1 / (2πfC) = V / (Isin
θ): (C is the capacity), and the resistance component r is output as the measured value of the insulation resistance.
なお、電圧信号を配電線路の中性点に注入して零相電
圧,電流から配電線路のインピーダンスを測定するた
め、配電線路のコイル成分を無視し、リアクタンス成分
xを容量成分とみなすことができる。Since the voltage signal is injected into the neutral point of the distribution line and the impedance of the distribution line is measured from the zero-phase voltage and current, the coil component of the distribution line can be ignored and the reactance component x can be regarded as the capacitance component. .
また、絶縁抵抗の測定にもとづき、監視装置は絶縁抵抗
の良,不良を自動判別して絶縁劣化の表示,報知などを
行う。Also, based on the measurement of the insulation resistance, the monitoring device automatically determines whether the insulation resistance is good or bad, and displays and informs of the insulation deterioration.
ところで、前述のように電圧信号を注入して絶縁抵抗を
測定する場合、前記零相変成器のインピーダンスなどの
装置の回路インピーダンスにもとづく信号の測定位相ず
れ(回転)により、測定値,が真のインピーダンス
座標(直交する抵抗軸とリアクタンス軸の座標)を前記
位相ずれに相当する角度回転したインピーダンス座標
(以下測定インピーダンス座標と称する)にもとづいて
得られる。By the way, when the insulation resistance is measured by injecting the voltage signal as described above, the measurement value is true due to the measurement phase shift (rotation) of the signal based on the circuit impedance of the device such as the impedance of the zero-phase transformer. The impedance coordinates (coordinates of the resistance axis and the reactance axis orthogonal to each other) are obtained by rotating the impedance coordinates (hereinafter referred to as measured impedance coordinates) by an angle corresponding to the phase shift.
そして、測定値,から算出された実効値V,I及び位
相角θにもとづき、たとえば第5図の抵抗軸R*,リア
クタンス軸X*の測定インピーダンス座標から抵抗成分
r,リアクタンス成分xが算出され、このとき、同図の抵
抗軸R,リアクタンス軸Xの真のインピーダンス座標から
の角度の測定位相ずれにより、算出された抵抗成分r,
リアクタンス成分xが配電線路の真の抵抗成分ro(=絶
縁抵抗),リアクタンス成分xoそれぞれから角度に相
当する量だけずれ、絶縁抵抗の測定誤差が生じる。Then, based on the effective values V and I and the phase angle θ calculated from the measured values, for example, from the measured impedance coordinates of the resistance axis R * and the reactance axis X * in FIG.
r and the reactance component x are calculated. At this time, the resistance component r, which is calculated from the measured phase shift of the angle from the true impedance coordinate of the resistance axis R and the reactance axis X in FIG.
The reactance component x deviates from the true resistance component ro (= insulation resistance) of the distribution line and the reactance component xo by an amount corresponding to the angle, and an insulation resistance measurement error occurs.
したがつて、従来の絶縁抵抗測定装置の場合、絶縁抵抗
の正確な測定が行えず、絶縁劣化の正確な監視などが行
えない問題点がある。Therefore, in the case of the conventional insulation resistance measuring device, there is a problem that the insulation resistance cannot be accurately measured and the insulation deterioration cannot be accurately monitored.
なお、絶縁抵抗計を用いた場合も、抵抗計の回路インピ
ーダンスにもとづく測定位相ずれにより、絶縁抵抗を正
確に測定することはできない。Even when the insulation resistance meter is used, the insulation resistance cannot be accurately measured due to the measurement phase shift based on the circuit impedance of the resistance meter.
本考案は、中性点に低周波の電圧信号を注入したときの
配電線路の零相電圧,電流から配電線路の絶縁抵抗を測
定位相ずれの誤差なく正確に測定する絶縁抵抗測定装置
を提供することを目的としている。The present invention provides an insulation resistance measuring device for accurately measuring the insulation resistance of a distribution line from the zero-phase voltage and current of the distribution line when a low-frequency voltage signal is injected into the neutral point without error in phase shift. Is intended.
前記目的を達成するための手段を以下に説明する。 Means for achieving the above object will be described below.
本考案は、多相低圧配電線路の絶縁抵抗を測定する絶縁
抵抗測定装置において、 前記配電線路の非接地の中性点に送電交流と異なる2周
波数の低周波の電圧信号を順に注入する電圧注入手段
と、 前記配電線路の零相電流を検出する電流検出手段と、 前記検出手段の検出結果にもとづき前記両電圧信号それ
ぞれの注入時の前記配電線路の零相電圧,電流の実効値
及び位相角を算出するとともに該両実効値及び位相角か
ら前記両電圧信号それぞれにもとづく前記配電線路のイ
ンピーダンスの抵抗成分,リアクタンス成分の測定値を
算出するインピーダンス演算手段と、 前記両電圧信号の前記抵抗成分,リアクタンス成分の測
定値にもとづく幾何学演算から前記インピーダンスの測
定位相ずれを補正し,前記配電線路の絶縁抵抗を算出す
る補正演算手段と を備えるという技術的手段を講じている。The present invention relates to an insulation resistance measuring device for measuring the insulation resistance of a multi-phase low-voltage distribution line, wherein voltage injection is performed by sequentially injecting low-frequency voltage signals of two frequencies different from the transmission AC into an ungrounded neutral point of the distribution line. Means, a current detecting means for detecting a zero-phase current of the distribution line, and an effective value and a phase angle of the zero-phase voltage and current of the distribution line at the time of injecting each of the both voltage signals based on the detection result of the detecting means. And impedance calculation means for calculating the resistance value of the impedance of the distribution line based on the voltage signals and the measured value of the reactance component from the RMS value and the phase angle, and the resistance component of the voltage signals, A correction operation that corrects the measured phase shift of the impedance from the geometric calculation based on the measured value of the reactance component and calculates the insulation resistance of the distribution line. We have taken technical measures to equip them with arithmetic means.
したがつて、2周波数の電圧信号の注入にもとづき、配
電線路の零相電圧,電流が零相電圧の周波数を変えて2
回測定されるとともに、それぞれの測定結果にもとづ
き、インピーダンス演算手段によつて配電線路のインピ
ーダンスの抵抗成分,リアクタンス成分が算出される。Therefore, based on the injection of the voltage signal of 2 frequencies, the frequency of the zero phase voltage and the current of the distribution line are changed to 2
The impedance component is used to calculate the resistance component and the reactance component of the impedance of the power distribution line based on the measurement results.
このとき、測定位相ずれにもとづき、両電圧信号それぞ
れにもとづく抵抗成分,リアクタンス成分の演算が、真
のインピーダンス座標を所定角度回転した同一の測定イ
ンピーダンス座標によつて行われる。At this time, the calculation of the resistance component and the reactance component based on both the voltage signals based on the measurement phase shift is performed by the same measurement impedance coordinate obtained by rotating the true impedance coordinate by a predetermined angle.
そして、前記2回の測定にもとづき、抵抗成分,リアク
タンス成分がr1,x1及びr2,x2として算出されたとする
と、測定位相ずれにより、抵抗成分r1,r2が異なるとと
もに、測定位相ずれが90°又は270°になつてリアクタ
ンス成分x1,x1が等しくなる特別な場合を除き、点(r1,x
1),(r1,x2)を結ぶ線分が真のインピーダンス座標のリア
クタンス軸に平行になるとともに該線分と真のインピー
ダンス座標の抵抗軸との交点が真の抵抗成分の点にな
る。If the resistance component and the reactance component are calculated as r 1 , x 1 and r 2 , x 2 based on the above two measurements, the resistance components r 1 and r 2 are different due to the measurement phase shift, and Except in the special case where the reactance components x 1 and x 1 become equal as the phase shift becomes 90 ° or 270 °, the point (r 1 , x
The line segment connecting ( 1 ) and (r 1 , x 2 ) is parallel to the reactance axis of the true impedance coordinate, and the intersection of the line segment and the resistance axis of the true impedance coordinate is the point of the true resistance component. .
そのため、点(r1,x1),(r1,x2)を結ぶ線分の傾きなどに
もとづき、補正演算手段により、幾何学演算から測定位
相ずれの補正が行われ、真のインピーダンス座標にもと
づく配電線路の絶縁抵抗が算出される。Therefore, based on the inclination of the line segment connecting the points (r 1 , x 1 ), (r 1 , x 2 ), the correction calculation means corrects the measured phase shift from the geometric calculation to obtain the true impedance coordinates. Based on this, the insulation resistance of the distribution line is calculated.
なお、前記特別な場合は、リアクタンス成分x1,x2が真
のインピーダンス座標にもとづく配電線路の絶縁抵抗と
して算出される。In the special case, the reactance components x 1 and x 2 are calculated as the insulation resistance of the distribution line based on the true impedance coordinates.
つぎに、本考案を、その1実施例を示した第1図ないし
第4図とともに詳細に説明する。Next, the present invention will be described in detail with reference to FIGS. 1 to 4 showing one embodiment thereof.
第1図において、(1)は中性点(1)′が非接地の3
相低圧配電線路であり、50Hz又は60Hzの送電交流が流れ
る。(2)は絶縁抵抗測定装置を用いて形成された絶縁
監視装置、(3)は装置(2)の制御,演算などを行う
マイクロプロセツサであり、後述のインピーダンス演算
手段,補正演算手段を形成する。In Fig. 1, (1) is a neutral point (1) 'where 3 is not grounded.
It is a low voltage phase distribution line, and 50Hz or 60Hz transmission AC flows. (2) is an insulation monitoring device formed by using an insulation resistance measuring device, (3) is a microprocessor that controls and calculates the device (2), and forms an impedance calculating means and a correction calculating means described later. To do.
(4)はプロセツサ(3)によつて発振周波数が可変さ
れる電圧発生器であり、測定時に2周波数f1,f2に順に
変化する低周波の電圧信号V(f)を形成して出する。
(5)はプロセツサ(3)によつてオン,オフする注入
用スイツチ、(6)は1次側にスイツチ(5)を介した
電圧信号V(f)が供給される注入用変圧器であり、2
次側が中性点(1)′とアースとの間に設けられ、発生
器(4),スイツチ(5)とともに電圧注入手段を形成
し、電圧信号V(f)を中性点(1)′に注入する。(4) is a voltage generator whose oscillating frequency is variable by the processor (3), which forms a low-frequency voltage signal V (f) which sequentially changes to two frequencies f 1 and f 2 at the time of measurement and outputs the voltage signal V (f). To do.
(5) is an injection switch that is turned on and off by the processor (3), and (6) is an injection transformer that is supplied with the voltage signal V (f) through the switch (5) on the primary side. Two
The secondary side is provided between the neutral point (1) 'and the ground, and forms a voltage injection means together with the generator (4) and the switch (5) to transfer the voltage signal V (f) to the neutral point (1)'. Inject.
(7)は配電線路(1)の零相電流を検出する零相変成
器(ZCT)であり、電流検出手段を形成し、零相電流に
比例した電圧の検出信号I(f)を出力する。(8),
(9)は電圧信号V(f),検出信号I(f)それぞれ
を増幅する2個の入力増幅器、(10)は増幅器(9)の
入力側に設けられたバイアス用の抵抗である。Reference numeral (7) is a zero-phase transformer (ZCT) for detecting a zero-phase current of the distribution line (1), which forms a current detecting means and outputs a detection signal I (f) having a voltage proportional to the zero-phase current. . (8),
(9) is two input amplifiers for amplifying each of the voltage signal V (f) and the detection signal I (f), and (10) is a bias resistor provided on the input side of the amplifier (9).
(11)は増幅器(8),(9)の出力信号を選択出力す
るマルチプレクサであり、プロセツサ(3)によつて動
作制御される。(12)はマルチプレクサ(11)の出力信
号をデジタル変換するA/D変換器であり、電圧信号V
(f),検出信号I(f)のデジタルデータをプロセツ
サ(3)に出力する。Reference numeral (11) is a multiplexer for selectively outputting the output signals of the amplifiers (8) and (9), and its operation is controlled by the processor (3). (12) is an A / D converter for converting the output signal of the multiplexer (11) into a digital signal, and the voltage signal V
(F), digital data of the detection signal I (f) is output to the processor (3).
(13)はプロセツサ(3)の測定結果の表示信号が入力
される抵抗値表示器であり、測定された絶縁抵抗の値を
表示する。(14),(15)はプロセツサ(3)の判別結
果の報知信号が入力される絶縁正常表示器,絶縁不良表
示器であり、点,消灯などにもとづき、配電線(1)の
絶縁劣化の有,無を表示する。(16)はプロセツサ
(3)の判別結果の報知信号によつて駆動される劣化接
点信号発生器であり、絶縁劣化の識別時に報知,制御の
外部出力用の接点信号を発生する。(13) is a resistance value indicator into which the display signal of the measurement result of the processor (3) is input, and displays the measured insulation resistance value. (14) and (15) are an insulation normality indicator and an insulation defect indicator to which a notification signal of the determination result of the processor (3) is input. Displays Yes and No. A deterioration contact signal generator (16) is driven by a notification signal of the determination result of the processor (3) and generates a contact signal for notification and control external output when insulation deterioration is identified.
なお、プロセツサ(3),発生器(4),スイツチ
(5),変成器(6),(7),増幅器(8),(9)
及びマルチプレクサ(11),変換器(12)により、絶縁
抵抗測定装置が形成されている。A processor (3), a generator (4), a switch (5), a transformer (6), (7), an amplifier (8), (9).
The multiplexer (11) and the converter (12) form an insulation resistance measuring device.
そして、プロセツサ(3)のタイマ動作又は手動起動に
より、たとえば1日に1回程度の比較的長い間隔をあけ
て装置(2)が動作し、絶縁抵抗の測定を実行する。Then, by the timer operation of the processor (3) or manual activation, the device (2) operates at a relatively long interval, for example, about once a day, and the insulation resistance is measured.
このとき、プロセツサ(3)の制御にもとづき、発生器
(4)が比較的短い時間に所定の2周波数f1,f2の電圧
信号V(f)を順に出力するとともに、スイツチ(5)
が2周波数f1,f2の電圧信号V(f)それぞれの安定な
期間にオンし、2周波数f1,f2の電圧信号V(f)が変
成器(6)を介して中性点(1)′に零相電圧として順
に注入される。At this time, based on the control of the processor (3), the generator (4) sequentially outputs the voltage signals V (f) of the predetermined two frequencies f 1 and f 2 in a relatively short time, and the switch (5).
Is turned on during a stable period of each of the voltage signals V (f) of the two frequencies f 1 and f 2, and the voltage signal V (f) of the two frequencies f 1 and f 2 is passed through the transformer (6) to the neutral point. (1) 'is sequentially injected as a zero-phase voltage.
なお、2周波数f1,f2は送電交流の周波数と異なる低周
波の異なる2周波数に設定され、たとえば、送電交流が
50Hzのときに60Hz,62Hzそれぞれに設定され、送電交流
が60Hzのときに50Hz,52Hzそれぞれに設定される。Note that the two frequencies f 1 and f 2 are set to two different low frequencies, which are different from the frequency of the power transmission AC.
It is set to 60Hz and 62Hz respectively at 50Hz, and is set to 50Hz and 52Hz respectively when the transmission AC is 60Hz.
そして、電圧信号V(f)の注入にもとづき、配電線路
(1)の零相電流が電圧信号V(f)の周波数に応じて
変化するとともに、配電線路(1)の零相電流が変成器
(7)によつて検出される。Then, based on the injection of the voltage signal V (f), the zero-phase current of the distribution line (1) changes according to the frequency of the voltage signal V (f), and the zero-phase current of the distribution line (1) changes. It is detected by (7).
さらに、電圧信号V(f)及び変成器(7)の検出信号
I(f)が一定利得の増幅器(8),(9)を介してマ
ルチプレクサ(11)に入力され、このとき、プロセツサ
(3)の制御にもとづき、周波数f1,f2それぞれの電圧
信号V(f)の注入時の1又は数周期分の電圧信号V
(f),検出信号I(f)がマルチプレクサ(11)から
変換器(12)に時系列に出力される。Further, the voltage signal V (f) and the detection signal I (f) of the transformer (7) are input to the multiplexer (11) via the amplifiers (8) and (9) of constant gain, and at this time, the processor (3) ), The voltage signal V for one or several cycles at the time of injecting the voltage signal V (f) of each of the frequencies f 1 and f 2
(F), the detection signal I (f) is output from the multiplexer (11) to the converter (12) in time series.
そして、変換器(12)により、入力された電圧信号V
(f),検出信号I(f)それぞれが微小な周期でデジ
タル変換され、周波数f1,f2それぞれの零相電圧,電流
の1周期当りN個の瞬時値(t),(t)(t=1,
…,N)のサンプリングデータがプロセツサ(3)に出力
される。Then, the converter (12) inputs the input voltage signal V
(F) and the detection signal I (f) are digitally converted in a minute cycle, and N instantaneous values (t), (t) (zero-phase voltage and current per cycle of the frequencies f 1 and f 2 respectively) t = 1,
, N) sampling data is output to the processor (3).
このとき、プロセツサ(3)のインピーダンス演算手段
により、周波数,f1,f2それぞれの零相電圧,電流の1
周期分の瞬時値(t),(t)にもとづくフーリエ
変換処理から、周波数f1,f2にそれぞれの電圧信号V
(f)が注入されたときの零相電圧,電流の測定値,
の実効値V,I及び,の位相角θが算出される。At this time, the impedance calculation means of the processor (3) controls the frequency, the zero phase voltage of each of f 1 and f 2 and the current of 1
From the Fourier transform processing based on the instantaneous values (t) and (t) for a period, the voltage signals V at the frequencies f 1 and f 2 are obtained.
(F) Zero phase voltage when injected, current measurement,
The effective values V, I of and the phase angle θ of are calculated.
ところで、周波数f1の電圧信号V(f)にもとづく測定
値,を1,1とし、周波数f2の電圧信号V(f)
にもとづく測定値,を2,2とした場合、配電線
路(1)のインピーダンスは、つぎの(1),(2)の
ベクトル演算それぞれから求まる。1 /1=1=r1+jx1 ……(1)式2 /2=2=r2+jx2 ……(2)式 なお、1,2は演算から求められた配電線路(1)の
インピーダンスを示し、r1,r2はインピーダンス1,
2の抵抗成分を示し、x1,x2はインピーダンス1,2の
リアクタンス成分を示す。By the way, the measured value based on the voltage signal V (f) of the frequency f 1 is set to 1 , 1, and the voltage signal V (f) of the frequency f 2 is set.
When the measured value based on the above is 2 , 2 , the impedance of the distribution line (1) can be obtained from the vector operations of (1) and (2) below. 1/1 = 1 = r 1 + jx 1 ...... (1) Formula 2/2 = 2 = r 2 + jx 2 ...... (2) Equation Incidentally, 1, 2 was determined from the arithmetic distribution line (1) Where r 1 and r 2 are impedances 1 and
2 shows the resistance component, and x 1 and x 2 show the reactance components of impedances 1 and 2 .
そして、変成器(7),増幅器(8),(9)などにも
とづく装置(2)の回路インピーダンスによる測定位相
ずれがなく、測定値1,1及び2,2が真のインピ
ーダンス座標から得られたとすると、このとき、配電線
路(1)の抵抗成分が周波数によつて変化しないため、
抵抗成分r1,r2は共に配電線路(1)の真の抵抗成分
r0,すなわち真の絶縁抵抗になつて等しくなる。And there is no measurement phase shift due to the circuit impedance of the device (2) based on the transformer (7), amplifier (8), (9), etc., and the measured values 1 , 1 and 2 , 2 can be obtained from the true impedance coordinates. Then, at this time, since the resistance component of the distribution line (1) does not change with frequency,
Resistance components r 1 and r 2 are both true resistance components of the distribution line (1)
r 0 , that is, the true insulation resistance becomes equal.
しかし、実際には、装置(2)の回路インピーダンスに
もとづく測定位相ずれにより、測定値1,1及び
2,2が、真のインピーダンス座標から位相ずれに相
当する所定角度回転した測定インピーダンス座標から得
られ、このとき、抵抗成分r1,r2は真のインピーダンス
座標上の抵抗成分r0からずれた異なる値になる。However, in reality, due to the measurement phase shift based on the circuit impedance of the device (2), the measured values 1 , 1 and
2 and 2 are obtained from the measured impedance coordinates rotated by a predetermined angle corresponding to the phase shift from the true impedance coordinates, and at this time, the resistance components r 1 and r 2 are displaced from the resistance component r 0 on the true impedance coordinates. Will have different values.
すなわち、第2図に示すように抵抗軸R*,リアクタンス
軸X*の測定インピーダンス座標が、測定位相ずれにもと
づき、抵抗軸R,リアクタンス軸Xの真のインピーダンス
座標から角度だけ回転し、その測定インピーダンス座
標を基準にした測定値1,1及び2,2からインピ
ーダンス1=(r1,x1)及び2=(r2,x2)それぞれが得ら
れたとすると、同図からも明らかなように、抵抗成分
r1,r2は真の抵抗成分r0からずれた異なる値になる。That is, as shown in FIG. 2, the measured impedance coordinates of the resistance axis R * and the reactance axis X * are rotated by an angle from the true impedance coordinates of the resistance axis R and the reactance axis X based on the measurement phase shift, and the measurement is performed. Assuming that impedances 1 = (r 1 , x 1 ) and 2 = (r 2 , x 2 ) are obtained from the measured values 1 , 1 and 2 , 2 based on the impedance coordinates, respectively, it is clear from the figure. To the resistance component
r 1 and r 2 have different values deviated from the true resistance component r 0 .
ところで、前述したように真のインピーダンス座標から
点(r1,x1),(r1,x2)をみると、その抵抗成分r1,r2が必ず
等しくなるため、点(r1,x1),(r1,x2)を結ぶ線分は、測
定位相ずれによつて角度が90°又は270°になる特別
な場合,すなわち抵抗軸R*がリアクタンス軸Xに一致し
てリアクタンス軸X*が抵抗軸Rに一致する特別な場合を
除き、第2図からも明らかなように、真のインピーダン
ス座標のリアクタンス軸Xに平行になり、しかも、その
線分と真のインピーダンス座標の抵抗軸Rとの交点が、
真の成功成分r0,すなわち真の絶縁抵抗の点になる。By the way, looking at the points (r 1 , x 1 ), (r 1 , x 2 ) from the true impedance coordinates as described above, the resistance components r 1 , r 2 are always equal, and therefore the points (r 1 , The line segment connecting (x 1 ), (r 1 , x 2 ) has a special case where the angle becomes 90 ° or 270 ° due to the measurement phase shift, that is, the resistance axis R * coincides with the reactance axis X and the reactance As is clear from FIG. 2, except for the special case where the axis X * coincides with the resistance axis R, it becomes parallel to the reactance axis X of the true impedance coordinate, and the line segment and the true impedance coordinate The intersection with the resistance axis R is
It is the point of the true success component r 0 , that is, the true insulation resistance.
そして、抵抗軸R*,リアクタンス軸X*を直交する2軸
α,βとし、点(r1,X1),(r2,x2)を結ぶ線分をつぎの
(3)式とした場合、2軸α,βの座標からみた抵抗軸
Rは(4)式で示すことができる。なお、式中のK,Mは
定数である。Then, the resistance axis R * and the reactance axis X * are two axes α and β orthogonal to each other, and the line segment connecting the points (r 1 , X 1 ), (r 2 , x 2 ) is defined as the following equation (3). In this case, the resistance axis R viewed from the coordinates of the two axes α and β can be expressed by the equation (4). Note that K and M in the formula are constants.
β=Kα−M ……(3)式 β=−(1/K)α ……(4)式 さらに、(3)式の線分が点(r1,x1),(r1,x2)を通るた
め、定数K,Mはつぎの(5),(6)式それぞれから求
まる。β = Kα−M (3) Equation β = − (1 / K) α (4) Further, the line segment of Equation (3) is a point (r 1 , x 1 ), (r 1 , x 2 ), the constants K and M are obtained from the following equations (5) and (6), respectively.
K=(x1-x2)/(r1-r2) …(5)式 M=(x1r2-r1x2)/(r1-r2) ……(6)式 また、(3)式と(4)との交点を(α1,β1)とする
と、α1,β1はつぎの(7),(8)式それぞれから求
まる。K = (x 1 -x 2 ) / (r 1 -r 2 ) ... (5) Formula M = (x 1 r 2 -r 1 x 2 ) / (r 1 -r 2 ) ... (6) Formula , (3) and the intersection of (4) with (α 1 , β 1 ), α 1 , β 1 can be obtained from the following equations (7), (8), respectively.
α1=MK/(K2+1) ……(7)式 β1=−M/(K2+1) ……(8)式 そして、α1,β1が第2図のr0′,x0′になるため、抵
抗成分r0は、つぎの(9)式に(5),(6)式のK,M
を代入して求めることができる。α 1 = MK / (K 2 +1) (7) Formula β 1 = −M / (K 2 +1) (8) Formula α 1 and β 1 are r 0 ′, x in FIG. Since it becomes 0 ′, the resistance component r 0 can be expressed by the following equations (9), K and M in equations (5) and (6).
Can be obtained by substituting.
なお、前記特別な場合は、点(r1,x1),(r1,x2)を、結ぶ
線分がリアクタンス軸Xに平行になつて抵抗軸Rに直角
になり、このとき、リアクタンス成分x1,x2が必ず抵抗
成分r0に等しい同一値になるため、リアクタンス成分が
x1,x1から抵抗成分r0が求まる。 In the special case, the line segment connecting the points (r 1 , x 1 ) and (r 1 , x 2 ) is parallel to the reactance axis X and is perpendicular to the resistance axis R. At this time, Since the components x 1 and x 2 always have the same value equal to the resistance component r 0 , the reactance component is
The resistance component r 0 is obtained from x 1 and x 1 .
したがつて、プロセツサ(3)のインピーダンス演算手
段により、周波数f1,f2の電圧信号V(f)それぞれに
もとづく実効値,及び位相角θのベクトル演算から
前述のインピーダンス1,2それぞれの抵抗成分,リ
アクタンス成分r1,x1及びr2,x2が測定値として算出され
る。Therefore, the impedance calculation means of the processor (3) calculates the effective values based on the voltage signals V (f) of the frequencies f 1 and f 2 and the vector calculation of the phase angle θ to calculate the resistances of the impedances 1 and 2 described above. The components and reactance components r 1 , x 1 and r 2 , x 2 are calculated as the measured values.
さらに、プロセツサ(3)の補正演算手段により、イン
ピーダンス1の両成分r1,x1及びインピーダンス2の
両成分r2,x2にもとづき、前記(5),(6),(9)
式の幾何学演算から測定位相ずれを補正して真の抵抗成
分r0が算出され、算出された抵抗成分r0のデータ値が絶
縁抵抗の測定値として出力される。Furthermore, by the correction computing means processor (3), based on both components r 2, x 2 of the two-component r 1, x 1 and impedance second impedance 1, wherein (5), (6), (9)
The true resistance component r 0 is calculated by correcting the measured phase shift from the geometrical calculation of the equation, and the data value of the calculated resistance component r 0 is output as the measured value of the insulation resistance.
なお、前記特別な場合は、リアクタンス成分x1,x2が等
しくなることから検出され、この場合、リアクタンス成
分x1又はx2が真の抵抗成分r0として算出される。The special case is detected because the reactance components x 1 and x 2 are equal, and in this case, the reactance component x 1 or x 2 is calculated as the true resistance component r 0 .
そして、補正演算手段から出力された絶縁抵抗の測定値
にもとづき、表示器(13)に求められた絶縁抵抗の値が
数値表示されるとともに、プロセツサ(3)の劣化判別
手段により、予め設定された判別基準値rsと測定値r0と
の大,小比較から配電線路(1)の絶縁劣化の有,無が
判別される。Then, the value of the insulation resistance obtained on the display (13) is displayed numerically based on the measurement value of the insulation resistance output from the correction calculation means, and is preset by the deterioration determination means of the processor (3). The presence or absence of insulation deterioration of the distribution line (1) can be determined from the comparison between the determination reference value rs and the measured value r 0 .
さらに、劣化判別手段の判別結果にもとづき、絶縁劣化
のない正常なときには、表示器(14)の点灯などによつ
て劣化のないことが表示され、絶縁劣化のあるときに
は、表示器(15)の点灯などによつて絶縁劣化が表示さ
れるとともに、発生器(16)から外部に接点信号が出力
される。Further, based on the determination result of the deterioration determining means, when the insulation is normal and there is no deterioration, it is displayed that the display (14) is not deteriorated, and when the insulation is deteriorated, the display (15) is displayed. Insulation deterioration is displayed by lighting, and a contact signal is output from the generator (16) to the outside.
なお、装置(2)の動作をフローチヤートで示すと、第
3図に示すようになる。The flow chart of the operation of the device (2) is as shown in FIG.
また、測定位相ずれの大きさを測定系の誤差として求め
る場合などには、たとえば第4図に示すように、インピ
ーダンス1の抵抗成分r1,リアクタンス成分x1と真の
抵抗成分r0,リアクタンス成分x0とにもとづき、インピ
ーダンス1のベクトルと抵抗軸R*とのなす角δ及び抵
抗成分r0を示すつぎの(10),(11)式から角度を算
出すればよい。The measurement in the example, when determining the magnitude of the phase shift as an error of the measurement system, for example, as shown in FIG. 4, the resistance component r 1 of the impedance 1, the reactance component x 1 and the true resistive component r 0, the reactance Based on the component x 0 , the angle may be calculated from the following equations (10) and (11) indicating the angle δ formed by the vector of the impedance 1 and the resistance axis R * and the resistance component r 0 .
δ=tan-1(x1/r1) ……(10)式 そして、前記実施例では絶縁監視に適用した場合につい
て説明したが、たとえば、絶縁抵抗の測定のみを行う場
合にも適用できるのは勿論である。δ = tan -1 (x 1 / r 1 ) …… (10) Formula Further, in the above-described embodiment, the case where the present invention is applied to the insulation monitoring has been described, but it is needless to say that the present invention can be applied to the case where only the insulation resistance is measured.
また、4相以上の多相低圧配電線路についても、実施例
と同様にして測定が行えるのも勿論である。Further, it is needless to say that the multi-phase low voltage power distribution line having four or more phases can be measured in the same manner as in the embodiment.
以上のように、本考案の絶縁抵抗測定装置によると、2
周波数の低周波の電圧信号を零相電圧として配電線路の
中性点に注入するとともに、両電圧信号それぞれの注入
時の配電線路の零相電流を検出し、両電圧信号にもとづ
く2周波数の零相電圧,電流それぞれから配電線路のイ
ンピーダンスの抵抗成分及びリアクタンス成分を算出
し、かつ、算出した2種の抵抗成分,リアクタンス成分
にもとづく幾何学演算により、前記インピーダンスの測
定位相ずれを補正して配電線路の絶縁抵抗を算出したこ
とにより、多相低圧配電線路の絶縁抵抗を測定位相ずれ
なく正確に測定することができる。As described above, according to the insulation resistance measuring device of the present invention, 2
A low-frequency voltage signal with a low frequency is injected as a zero-phase voltage into the neutral point of the distribution line, and the zero-phase current of the distribution line at the time of injection of both voltage signals is detected, and two frequency zeros based on both voltage signals are detected. The resistance component and the reactance component of the impedance of the distribution line are calculated from the phase voltage and the current, respectively, and the measured phase shift of the impedance is corrected by geometric calculation based on the calculated two types of resistance component and reactance component. By calculating the insulation resistance of the line, it is possible to accurately measure the insulation resistance of the multi-phase low-voltage distribution line without a measurement phase shift.
第1図は本考案の絶縁抵抗測定装置の1実施例のブロツ
ク図,第2図,第4図は第1図の測定説明用のインピー
ダンス座標、第3図は第1図の動作説明用のフローチヤ
ート、第5図は従来の絶縁抵抗測定装置の測定説明用の
インピーダンス座標である。 (1)……3相低圧配電線路、(1)′……中性点、
(3)……マイクロプロセツサ、(4)……電圧発生
器、(5)……注入用スイツチ、(6)……注入用変成
器、(7)……零相変成器、(8),(9)……入力増
幅器、(11)……マルチプレクサ、(12)……A/D変換
器。FIG. 1 is a block diagram of one embodiment of the insulation resistance measuring device of the present invention, FIG. 2 and FIG. 4 are impedance coordinates for the measurement description of FIG. 1, and FIG. 3 is a description of the operation of FIG. The flow chart, FIG. 5, is impedance coordinates for explaining the measurement of the conventional insulation resistance measuring device. (1) …… 3-phase low voltage distribution line, (1) ′ …… Neutral point,
(3) -Microprocessor, (4) -Voltage generator, (5) -Injection switch, (6) -Injection transformer, (7) -Zero-phase transformer, (8) , (9) …… Input amplifier, (11) …… Multiplexer, (12) …… A / D converter.
Claims (1)
縁抵抗測定装置において、 前記配電線路の非接地の中性点に送電交流と異なる2周
波数の低周波の電圧信号を順に注入する電圧注入手段
と、 前記配電線路の零相電流を検出する電流検出手段と、 前記検出手段の検出結果にもとづき前記両電圧信号それ
ぞれの注入時の前記配電線路の零相電圧,電流の実効値
及び位相角を算出するとともに該両実効値及び位相角か
ら前記両電圧信号それぞれにもとづく前記配電線路のイ
ンピーダンスの抵抗成分,リアクタンス成分の測定値を
算出するインピーダンス演算手段と、 前記両電圧信号の前記抵抗成分,リアクタンス成分の測
定値にもとづく幾何学演算から前記インピーダンスの測
定位相ずれを補正し,前記配電線路の絶縁抵抗を算出す
る補正演算手段と を備えた絶縁抵抗測定装置。1. An insulation resistance measuring device for measuring insulation resistance of a multi-phase low-voltage distribution line, wherein a voltage for sequentially injecting low-frequency voltage signals of two frequencies different from the transmission AC to a non-grounded neutral point of the distribution line. Injection means, current detection means for detecting a zero-phase current of the distribution line, and zero-phase voltage and current effective value and phase of the distribution line at the time of injection of each of the voltage signals based on the detection result of the detection means. Impedance calculating means for calculating an angle and calculating a measured value of a resistance component and a reactance component of the impedance of the distribution line based on the voltage signals from the RMS value and the phase angle, and the resistance component of the voltage signals. A correction for correcting the measured phase shift of the impedance from the geometric calculation based on the measured value of the reactance component to calculate the insulation resistance of the distribution line Insulation resistance measuring device equipped with a calculating means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7806588U JPH0645270Y2 (en) | 1988-06-13 | 1988-06-13 | Insulation resistance measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7806588U JPH0645270Y2 (en) | 1988-06-13 | 1988-06-13 | Insulation resistance measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02668U JPH02668U (en) | 1990-01-05 |
| JPH0645270Y2 true JPH0645270Y2 (en) | 1994-11-16 |
Family
ID=31303015
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7806588U Expired - Lifetime JPH0645270Y2 (en) | 1988-06-13 | 1988-06-13 | Insulation resistance measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0645270Y2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR101483952B1 (en) * | 2013-06-14 | 2015-01-21 | 광주과학기술원 | Wire harness inspection method |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2577825B2 (en) * | 1990-11-20 | 1997-02-05 | 三菱電機株式会社 | Non-power failure insulation diagnostic device |
| JP6128921B2 (en) * | 2013-04-09 | 2017-05-17 | 三菱電機ビルテクノサービス株式会社 | Non-interruptible insulation diagnosis device and non-interruptible insulation diagnosis method |
| US10203364B2 (en) * | 2017-02-17 | 2019-02-12 | Doble Engineering Company | System and method for performing transformer diagnostics |
| JP7533275B2 (en) * | 2021-02-24 | 2024-08-14 | 富士電機機器制御株式会社 | Electrical line monitoring device, electric line monitoring system, and electric line monitoring method |
-
1988
- 1988-06-13 JP JP7806588U patent/JPH0645270Y2/en not_active Expired - Lifetime
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR101483952B1 (en) * | 2013-06-14 | 2015-01-21 | 광주과학기술원 | Wire harness inspection method |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02668U (en) | 1990-01-05 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US5514978A (en) | Stator turn fault detector for AC motor | |
| US8405417B2 (en) | Method and device for off-line testing of electric motors | |
| US5144226A (en) | Multi-mode measuring system | |
| US4472676A (en) | Leakage impedance measuring system including a superimposed measuring voltage having a frequency differing slightly from system frequency | |
| JP3405407B2 (en) | Earth leakage detector, earth leakage alarm and earth leakage breaker using the same | |
| WO2019048537A1 (en) | Method and apparatus for current measurement in polyphase electricity supply | |
| JPH0645270Y2 (en) | Insulation resistance measuring device | |
| US7750663B2 (en) | Method and apparatus for testing an electronic motor | |
| EP2017631A1 (en) | Methods and systems for detecting DC influence in a current sensor | |
| JP2000028671A (en) | Insulation detector | |
| CN100385761C (en) | Electronic trip device with phase reconfiguration function and circuit breaker including the trip device | |
| JP2010060329A (en) | Apparatus and method for measuring leakage current of electrical path and electric instrument | |
| JPH0894683A (en) | Insulation monitoring system for low voltage ungrounded system | |
| JP3964538B2 (en) | Impedance measuring device | |
| JPH04109174A (en) | Impedance measuring device | |
| JP2942893B2 (en) | Method for measuring insulation resistance of single-phase three-wire circuit | |
| JPH0566988B2 (en) | ||
| JPH09304453A (en) | Simple impedance measuring device and simple impedance measuring method for low-voltage distribution line | |
| WO2021082036A1 (en) | Power system frequency measurement method, bus voltage correction method and devices | |
| JPH03122573A (en) | Apparatus for detecting deterioration of lightning arrester | |
| SU911395A1 (en) | Device for testing ac measuring instruments | |
| JP2750716B2 (en) | Insulation resistance measurement method for low voltage wiring etc. | |
| JPH02190769A (en) | Wattmeter | |
| JP2008145155A (en) | Apparatus for detecting resistance component current of zero-phase current and leakage monitoring apparats | |
| JPH01223363A (en) | Fault point locator |