JP4945727B2 - Leakage current interruption device and method - Google Patents

Leakage current interruption device and method Download PDF

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JP4945727B2
JP4945727B2 JP2007152754A JP2007152754A JP4945727B2 JP 4945727 B2 JP4945727 B2 JP 4945727B2 JP 2007152754 A JP2007152754 A JP 2007152754A JP 2007152754 A JP2007152754 A JP 2007152754A JP 4945727 B2 JP4945727 B2 JP 4945727B2
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insulation resistance
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豊次 阿閉
清 宮澤
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豊次 阿閉
頭本 頼数
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本発明は、漏洩電流を計測することにより被測定電線路を遮断する漏洩電流遮断装置及び方法に関する。   The present invention relates to a leakage current interrupting device and method for interrupting an electric line to be measured by measuring a leakage current.

日常生活の中で、電気の存在を意識することはあまりないが、周知のように、エネルギー源として、また、情報や通信を初めとする様々な分野に利用され、我々の社会にとって、なくてはならない存在となっている。   In everyday life, there is not much awareness of the existence of electricity, but as is well known, it is used as an energy source and in various fields such as information and communication. It has become a must not.

一方で、電気の利用は、便利な反面、適切な管理や使用を誤れば、大変危険な側面も兼ね備えており、電気火災や感電事故等の重大な事故を引き起こす可能性も少なくない。   On the other hand, the use of electricity is convenient, but if it is not properly managed and used, it also has very dangerous aspects, and there are many possibilities of causing serious accidents such as electric fires and electric shocks.

例えば、その重大事故の原因の一つとして、電路や機器の絶縁不良に深く関係しているのが漏洩電流である。しかし、この漏洩電流を調べるには、大変な時間を要するうえに、停電させて絶縁不良だけの数値を絶縁抵抗計により測定する必要がある。   For example, one of the causes of the serious accident is leakage current that is closely related to insulation failure of electric circuits and equipment. However, in order to investigate this leakage current, it takes a long time, and it is necessary to measure the value of insulation failure with an insulation resistance meter after a power failure.

しかしながら、現在の社会状況では、コンピュータが社会の各方面に利用され、インテリジェントビルの普及拡大及び工場のFA(ファクトリー・オートメーション)化により、24時間連続稼働するシステムが構築されており、漏洩電流を計測するために、一時的に停電状態にすることができない状況となっている。   However, in the current social situation, computers are used in various areas of society, and systems that operate continuously for 24 hours have been constructed by the spread of intelligent buildings and factory automation (FA). In order to measure, it is in a situation where it cannot temporarily be in a power failure state.

したがって、現在では、このような高度情報化による社会の無停電化の要請から、電路及び機器の絶縁不良管理が停電を伴う絶縁抵抗計による方法から、電気を切ることなく測定できる漏洩電流測定方法に移ってきており、漏洩電流遮断器や漏洩電流火災警報機等により漏洩電流を測定して絶縁状態を管理する通電中の予防策は種々提案されている(例えば、特許文献1及び特許文献2参照)。   Therefore, at present, due to the demand for uninterruptible socialization due to such advanced information technology, the leakage current measurement method that can measure the insulation failure of the electric circuit and equipment from the method using the insulation resistance meter with power failure without turning off the electricity Various preventive measures during energization that measure the leakage current with a leakage current breaker, a leakage current fire alarm, etc. and manage the insulation state have been proposed (for example, Patent Document 1 and Patent Document 2). reference).

ところで、漏洩電流Iには、対地静電容量に起因する漏洩電流(Igc)と、絶縁抵抗に直接関与している対地絶縁抵抗に起因する漏洩電流(Igr)とが含まれている。上述した漏電火災等を引き起こす原因は、絶縁抵抗の存在であり、この絶縁抵抗に起因する漏洩電流(Igr)のみを正確に検出することができれば、回路の絶縁状態をチェックすることができ、漏電火災等の大惨事を避けることができる。
特開2001−215247号公報 特開2002−98729号公報
By the way, the leakage current I includes a leakage current (Igc) caused by the ground capacitance and a leakage current (Igr) caused by the ground insulation resistance directly related to the insulation resistance. The cause of the above-mentioned leakage fire is the presence of insulation resistance. If only the leakage current (Igr) caused by this insulation resistance can be accurately detected, the insulation state of the circuit can be checked, A catastrophe such as a fire can be avoided.
JP 2001-215247 A JP 2002-98729 A

しかしながら、工場等で使用される電気機器は、機器同士を結線する際に電線路の長さが長大になることがあり、この電線路の長大化により、対地静電容量が増大化し、それに伴って対地静電容量に起因する漏洩電流(Igc)が大きくなってしまう。   However, electrical equipment used in factories or the like may have a long wire path when connecting the devices, and this increase in the length of the wire path increases the capacitance to the ground. As a result, the leakage current (Igc) due to the ground capacitance increases.

また、これらの電気機器は、電力用半導体素子を応用したインバータを搭載している。電気機器では、この搭載しているインバータを高速の電子スイッチとして使用しているため、必然的に、商用電源の基本周波数である50Hz若しくは60Hzの整数倍の正弦波である高調波歪み電流が発生する。高調波歪み電流には、高い周波数成分が含まれているため、電線路に自然分布している対地静電容量を通過し、電線路に流れてしまい、電線路に流れた高調波歪み電流により漏洩電流Iの値が大きくなってしまう。   Moreover, these electric devices are equipped with inverters using power semiconductor elements. In electrical equipment, this installed inverter is used as a high-speed electronic switch, so inevitably harmonic distortion current is generated that is a sine wave that is an integral multiple of 50 Hz or 60 Hz, which is the fundamental frequency of commercial power. To do. Since the harmonic distortion current contains high frequency components, it passes through the ground capacitance that is naturally distributed in the electric wire and flows into the electric wire, and due to the harmonic distortion current that flows in the electric wire. The value of the leakage current I becomes large.

したがって、絶縁の良否に直接関係する対地絶縁抵抗に起因する漏洩電流(Igr)が電線路の長大化及びインバータ等による高調波歪み電流の影響を受けてしまい、正確に検出することが困難となる。   Therefore, the leakage current (Igr) caused by the ground insulation resistance directly related to the quality of the insulation is affected by the length of the electric wire and the harmonic distortion current due to the inverter, and it is difficult to detect accurately. .

また、部品が高密度に実装された機器、例えば、電話機、ファクシミリ、プリンター及び複合機等では、絶縁箇所を調べるために、絶縁抵抗計等により計測を行った場合、注入する測定電圧により電子回路が影響を受けてしまう恐れがある。したがって、このような機器では、機能破壊を招く恐れがあることから、絶縁抵抗の測定自体ができない機器も多数存在する。   In addition, in equipment in which parts are mounted with high density, such as telephones, facsimiles, printers, and multi-function machines, when measuring with an insulation resistance meter or the like in order to check the insulation location, an electronic circuit is generated by the injected measurement voltage. May be affected. Accordingly, there is a large number of devices that cannot measure the insulation resistance because such devices may cause functional destruction.

そこで、本願発明では、上述した問題に鑑みて案出されたものであり、漏洩電流を計測し、検出のために電路及び機械設備等を停電状態にすることなく、かつ、被測定電線路に接続されている機器の機能を破壊することなく、外部から簡単かつ安全に絶縁の良否に直接関係する対地絶縁抵抗に起因する漏洩電流(Igr)のみを検出し、当該検出値に基づいて被測定電線路を遮断する漏洩電流遮断装置及び方法を提供する。   Therefore, in the present invention, it has been devised in view of the above-mentioned problems, and it is possible to measure the leakage current, without causing the electric circuit and mechanical equipment to be in a power failure state for detection, and to the electric line to be measured. Only the leakage current (Igr) due to ground insulation resistance directly related to the quality of insulation is detected easily and safely from the outside without destroying the function of the connected equipment, and measured based on the detected value Provided are a leakage current interrupting device and method for interrupting an electric line.

本発明に係る漏洩電流遮断装置は、電気方式が三相(R相、S相(接地相)、T相)三線式の被測定電線路に流れている漏洩電流を検出する漏洩電流検出手段と、上記漏洩電流検出手段により検出された漏洩電流を電圧に変換する変換手段と、上記変換手段により変換された電圧を増幅する増幅手段と、上記増幅手段で増幅された電圧に含まれている高調波成分を除去する第1の高調波成分除去手段と、上記被測定電線路の非接地相(R相−T相)間に発生している電圧を検出する電圧検出手段と、上記電圧検出手段で検出された電圧に含まれている高調波成分を除去する第2の高調波成分除去手段と、上記第1の高調波成分除去手段により高調波成分が除去された電圧の信号波形と、上記第2の高調波成分除去手段により高調波成分が除去された電圧の信号波形から位相差を検出する位相差検出手段と、上記位相差検出手段により検出された前記位相差が1サイクルの1/4以下かどうかを判定する判定手段と、上記第2の高調波成分除去手段により高調波成分が除去された電圧の信号波形に基づき、上記電圧検出手段で電圧を検出した電圧線路に発生している周波数を算出する周波数算出手段と、前記判定手段により1サイクルの1/4以下の位相差と、上記周波数算出手段で算出された周波数に基づき、上記被測定電線路に流れている漏洩電流の位相角度を算出する位相角度算出手段と、上記第1の高調波成分除去手段により高調波成分が除去された電圧の実効値を算出する実効値算出手段と、上記実効値算出手段で算出された実効値と、上記位相角度算出手段により算出された上記被測定電線路に流れている漏洩電流の位相角度に基づき、上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分を算出する対地絶縁抵抗漏洩電流成分算出手段と、上記対地絶縁抵抗漏洩電流成分算出手段で算出された上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分が、任意の値を超えたかどうかを判断する判断手段と、上記判断手段による判断に基づいて、上記被測定電線路を遮断する遮断手段とを備え、上記位相角度算出手段は、上記位相差検出手段により検出された位相パルス幅Wと、上記周波数算出手段で算出された周波数Fから、上記漏洩電流検出手段で検出された漏洩電流の位相角度θを
θ=360×W×F
により算出し、
上記実効値算出手段は、上記漏洩電流検出手段により検出された漏洩電流の平均値をIとし、その実効値I
=I×(π/2)/√2
により算出し、
上記対地絶縁抵抗漏洩電流成分算出手段は、上記実効値算出手段により算出された実効値Iと、上記位相角度算出手段により算出された上記被測定電線路のR相−S相間又はT相−S相間に流れている漏洩電流の位相角度θから、上記被測定電線路のR相−S相間又はT相−S相間に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分Igrを、
Igr=(I×sinθ)/cos30°
により算出することを特徴とする。
A leakage current interrupting device according to the present invention includes a leakage current detecting means for detecting a leakage current flowing in a three-wire electric line to be measured (R phase, S phase (ground phase), T phase) Conversion means for converting leakage current detected by the leakage current detection means into voltage; amplification means for amplifying the voltage converted by the conversion means; and harmonics included in the voltage amplified by the amplification means First harmonic component removing means for removing a wave component, voltage detecting means for detecting a voltage generated between ungrounded phases (R phase-T phase) of the measured electric line, and the voltage detecting means The second harmonic component removing means for removing the harmonic component contained in the voltage detected in step 1, the signal waveform of the voltage from which the harmonic component has been removed by the first harmonic component removing means, Harmonic components are removed by the second harmonic component removing means A phase difference detecting means for detecting a phase difference from the signal waveform of the detected voltage, a determining means for determining whether the phase difference detected by the phase difference detecting means is ¼ or less of one cycle, and the second A frequency calculating means for calculating a frequency generated in the voltage line in which the voltage is detected by the voltage detecting means based on the signal waveform of the voltage from which the harmonic component has been removed by the harmonic component removing means, and the judging means A phase angle calculating means for calculating a phase angle of a leakage current flowing in the measured electric line based on a phase difference equal to or less than ¼ of one cycle and the frequency calculated by the frequency calculating means; The effective value calculating means for calculating the effective value of the voltage from which the harmonic component has been removed by the harmonic component removing means, the effective value calculated by the effective value calculating means, and the phase angle calculating means. Based on the phase angle of the leakage current flowing through the measured electrical line, the ground insulation resistance leakage that calculates the leakage current component due to the ground insulation resistance included in the leakage current flowing through the measured electrical line The leakage current component due to the ground insulation resistance included in the leakage current flowing through the measured electric wire calculated by the current component calculation means and the ground insulation resistance leakage current component calculation means has an arbitrary value. A judgment means for judging whether or not it has exceeded, and a shut-off means for shutting off the electric wire to be measured based on the judgment by the judgment means, wherein the phase angle calculation means has a phase detected by the phase difference detection means. From the pulse width W and the frequency F calculated by the frequency calculation means, the phase angle θ of the leakage current detected by the leakage current detection means is set to θ = 360 × W × F
Calculated by
The effective value calculation means sets the average value of the leakage current detected by the leakage current detection means to I, and the effective value I 0 is I 0 = I × (π / 2) / √2
Calculated by
The ground insulation resistance leakage current component calculation means includes an effective value I 0 calculated by the effective value calculation means, and an R phase-S phase or a T phase of the measured electric wire calculated by the phase angle calculation means. From the phase angle θ of the leakage current flowing between the S phases, the leakage current caused by the ground insulation resistance included in the leakage current flowing between the R phase and the S phase or between the T phase and the S phase of the measured electric wire Ingredient Igr
Igr = (I 0 × sin θ) / cos 30 °
It is characterized by calculating by.

また、上記漏洩電流遮断装置では、上記任意の値を設定する設定手段を備え、上記判断手段は、上記対地絶縁抵抗漏洩電流成分算出手段で算出された上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分が、上記設定手段で設定された任意の値を超えたかどうかを判断することが好ましい。   The leakage current interrupting device further includes setting means for setting the arbitrary value, and the determination means is a leakage current flowing through the measured electric wire calculated by the ground insulation resistance leakage current component calculation means. It is preferable to determine whether or not the leakage current component caused by the ground insulation resistance included in the circuit exceeds an arbitrary value set by the setting means.

また、上記漏洩電流遮断装置では、上記対地絶縁抵抗漏洩電流成分算出手段により算出された上記漏洩電流成分を記録する記録手段を備えることが好ましい。   The leakage current interrupting device preferably includes recording means for recording the leakage current component calculated by the ground insulation resistance leakage current component calculation means.

また、上記漏洩電流遮断装置では、上記漏洩電流検出手段は、接地線路を含む被測定電線路をクランプし、上記被測定電線路に流れている漏洩電流を検出することが好ましい。   In the leakage current interrupting device, it is preferable that the leakage current detecting means clamps a measured electric wire including a ground line and detects a leakage current flowing through the measured electric wire.

また、上記漏洩電流遮断装置では、上記電圧検出手段は、上記被測定電線路に含まれている複数の電圧線路から検出した電圧を合成し、合成した電圧を上記第2の高調波成分除去手段に供給することが好ましい。   Further, in the leakage current interrupting device, the voltage detecting means synthesizes voltages detected from a plurality of voltage lines included in the measured electric line, and the synthesized voltage is added to the second harmonic component removing means. It is preferable to supply to.

本発明に係る漏洩電流遮断方法は、電気方式が三相(R相、S相(接地相)、T相)三線式の被測定電線路に流れている漏洩電流を検出する漏洩電流検出工程と、上記漏洩電流検出工程により検出された漏洩電流を電圧に変換する変換手段と、上記変換手段で変換された電圧を増幅する増幅工程と、上記増幅工程で増幅された電圧に含まれている高調波成分を除去する第1の高調波成分除去工程と、上記被測定電線路の非接地相(R相−T相)間に発生している電圧を検出する電圧検出工程と、上記電圧検出工程で検出された電圧に含まれている高調波成分を除去する第2の高調波成分除去工程と、上記第1の高調波成分除去工程により高調波成分が除去された電圧の信号波形と、上記第2の高調波成分除去工程により高調波成分が除去された電圧の信号波形から位相差を検出する位相差検出工程と、上記位相差検出工程により検出された前記位相差が1サイクルの1/4以下かどうかを判定する判定工程と、上記第2の高調波成分除去工程により高調波成分が除去された電圧の信号波形に基づき、上記電圧検出工程で電圧を検出した電圧線路に発生している電源周波数を算出する周波数算出工程と、前記判定工程により1サイクルの1/4以下の位相差と、上記周波数算出工程で算出された電源周波数に基づき、上記被測定電線路に流れている漏洩電流の位相角度を算出する位相角度算出工程と、上記第1の高調波成分除去工程により高調波成分が除去された電圧の実効値を算出する実効値算出工程と、上記実効値算出工程で算出された実効値と、上記位相角度算出工程により算出された上記被測定電線路に流れている漏洩電流の位相角度に基づき、上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分を算出する対地絶縁抵抗漏洩電流成分算出工程と、上記対地絶縁抵抗漏洩電流成分算出工程で算出された上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分が、任意の値を超えたかどうかを判断する判断工程と、上記判断工程による判断に基づいて、上記被測定電線路を遮断する遮断工程とを備え、
上記位相角度算出工程は、上記位相差検出工程により検出された位相パルス幅Wと、上記周波数算出工程で算出された周波数Fから、上記漏洩電流検出工程で検出された漏洩電流の位相角度θを
θ=360×W×F
により算出し、
上記実効値算出工程は、上記漏洩電流検出工程により検出された漏洩電流の平均値をIとし、その実効値I
=I×(π/2)/√2
により算出し、
上記対地絶縁抵抗漏洩電流成分算出工程は、上記実効値算出工程により算出された実効値Iと、上記位相角度算出工程により算出された上記被測定電線路のR相−S相間又はT相−S相間に流れている漏洩電流の位相角度θから、上記被測定電線路のR相−S相間又はT相−S相間に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分Igrを、
Igr=(I×sinθ)/cos30°
により算出することを特徴とする。
The leakage current interrupting method according to the present invention includes a leakage current detecting step for detecting a leakage current flowing in a three-wire electric line having a three-phase electrical system (R phase, S phase (ground phase), T phase), A conversion means for converting the leakage current detected by the leakage current detection step into a voltage; an amplification step for amplifying the voltage converted by the conversion means; and a harmonic included in the voltage amplified in the amplification step. A first harmonic component removing step of removing a wave component, a voltage detecting step of detecting a voltage generated between the non-grounded phases (R phase-T phase) of the measured electric line, and the voltage detecting step A second harmonic component removing step for removing the harmonic component contained in the voltage detected in step 1, a signal waveform of the voltage from which the harmonic component has been removed by the first harmonic component removing step, and Harmonic components are removed by the second harmonic component removal step A phase difference detection step of detecting a phase difference from a voltage signal waveform, a determination step of determining whether the phase difference detected by the phase difference detection step is ¼ or less of one cycle, and the second harmonic Based on the signal waveform of the voltage from which the harmonic component has been removed by the wave component removal step, a frequency calculation step for calculating the power supply frequency generated in the voltage line in which the voltage has been detected in the voltage detection step, and the determination step 1 A phase angle calculating step of calculating a phase angle of a leakage current flowing in the measured electric wire line based on a phase difference of ¼ or less of a cycle and the power supply frequency calculated in the frequency calculating step; The effective value calculating step for calculating the effective value of the voltage from which the harmonic component has been removed by the harmonic component removing step, the effective value calculated in the effective value calculating step, and the phase angle calculating step. Ground insulation resistance for calculating a leakage current component caused by ground insulation resistance included in the leakage current flowing through the measured electric wire based on the phase angle of the leakage current flowing through the measured electric wire The leakage current component due to the ground insulation resistance included in the leakage current flowing in the measured electric wire calculated in the leakage current component calculation step and the ground insulation resistance leakage current component calculation step is an arbitrary value. A judgment step for judging whether or not, and based on the judgment by the judgment step, a blocking step for cutting off the measured electric wire path,
The phase angle calculation step calculates the phase angle θ of the leakage current detected in the leakage current detection step from the phase pulse width W detected in the phase difference detection step and the frequency F calculated in the frequency calculation step. θ = 360 × W × F
Calculated by
In the effective value calculating step, the average value of the leakage current detected in the leakage current detecting step is I, and the effective value I 0 is I 0 = I × (π / 2) / √2
Calculated by
The ground insulation resistance leakage current component calculation step includes the effective value I 0 calculated by the effective value calculation step and the R phase-S phase or the T phase of the measured electric wire calculated by the phase angle calculation step. From the phase angle θ of the leakage current flowing between the S phases, the leakage current caused by the ground insulation resistance included in the leakage current flowing between the R phase and the S phase or between the T phase and the S phase of the measured electric wire Ingredient Igr
Igr = (I 0 × sin θ) / cos 30 °
It is characterized by calculating by.

本発明に係る漏洩電流遮断装置及び方法は、被測定電線路に流れている漏洩電流を検出し、検出した漏洩電流から高調波成分を除去したものと、被測定電線路の電圧線路に発生している電圧を検出し、検出した電圧から高調波成分を除去したものから位相差を検出し、検出した位相差と、高調波成分を除去した電圧から算出した電源周波数とから漏洩電流の位相角度を算出し、算出した漏洩電流の位相角度と、高調波成分を除去した漏洩電流の実効値から対地絶縁抵抗のみに起因する漏洩電流を算出し、算出された漏洩電流値が任意の値を超えている場合には、被測定電線路を遮断する。したがって、本発明に係る漏洩電流遮断装置及び方法は、高調波成分を除去した電圧から被測定電線路に流れている電源周波数(商用電源であれば50Hz若しくは60Hz)を正確に算出し、この電源周波数に基づいて、入力される高調波成分が除去された漏洩電流の信号波形と、高調波成分が除去された電圧の信号波形との位相差を正確に検出するので、正確な漏洩電流の位相角度を算出することができ、また、正確な位相角度と、高調波成分を除去した漏洩電流の実効値から対地絶縁抵抗のみに起因する漏洩電流を算出し、算出した漏洩電流の値が任意の値を超えている場合に、被測定電線路を遮断するので、被測定電線路の長大化により、又はインバータによる高調波歪み電流による影響を受けて、対地静電容量が増大しても、漏電火災等の大惨事を招く対地絶縁抵抗のみに起因する漏洩電流のみを検出し、この検出に基づいて被測定電線路を遮断することができる。   The leakage current interrupting device and method according to the present invention detects a leakage current flowing in a measured electric line, and removes a harmonic component from the detected leakage current, and occurs in the voltage line of the measured electric line. The phase angle of the leakage current is detected from the detected phase difference and the power supply frequency calculated from the voltage from which the harmonic component has been removed. Calculate the leakage current due to the ground insulation resistance only from the calculated leakage current phase angle and the effective value of the leakage current with the harmonic components removed, and the calculated leakage current value exceeds an arbitrary value. If so, shut off the line to be measured. Therefore, the leakage current interrupting apparatus and method according to the present invention accurately calculates the power frequency (50 Hz or 60 Hz for commercial power) flowing from the voltage from which the harmonic component has been removed to the line to be measured. Based on the frequency, the phase difference between the input signal waveform of the leakage current from which the harmonic component has been removed and the voltage signal waveform from which the harmonic component has been removed is accurately detected. The angle can be calculated, and the leakage current caused only by the ground insulation resistance is calculated from the accurate phase angle and the effective value of the leakage current from which harmonic components are removed. If the value exceeds the value, the line to be measured is interrupted, so even if the earth capacitance increases due to the length of the line to be measured or the influence of harmonic distortion current caused by the inverter, Only leakage current due to only ground insulation resistance lead to disaster detects such disaster, it is possible to cut off the measured electric line based on the detection.

また、本発明に係る漏洩電流遮断装置及び方法は、漏洩電流を計測検出のために電路・機械設備等を一時的な停電状態にすることなく、簡単かつ安全にIgrを測定することができる。   Moreover, the leakage current interrupting apparatus and method according to the present invention can measure Igr easily and safely without putting the electric circuit / mechanical equipment in a temporary power failure state for measuring and detecting the leakage current.

以下、本発明の実施の形態としての漏洩電流遮断装置及び方法について説明する。   Hereinafter, a leakage current interrupting apparatus and method as embodiments of the present invention will be described.

漏洩電流遮断装置1は、図1に示すように、被測定電線路Aの全体にクランプし、被測定電線路Aに流れている漏洩電流Iを検出するカレントトランスセンサ(以下CTセンサという。)部10と、CTセンサ部10により検出された漏洩電流Iを電圧に変換し、変換後の電圧(以下「変換後電圧」という。)V1を増幅する増幅部11と、増幅後の変換後電圧V1から高調波成分を除去するローパスフィルター(以下LPFという。)12と、LPF12で高調波成分が除去された変換後電圧V1を整流する全波整流部13と、被測定電線路Aの電圧線路から電圧V2を検出する電圧検出部14と、電圧検出部14で検出された電圧V2を所定の変圧比になるように変圧する変圧器15と、変圧器15で所定の電圧値に変圧された電圧V2から高調波成分を除去するローパスフィルター(以下LPFという。)16と、LPF16で高調波成分が除去された電圧V2を整流する全波整流部17と、LPF12により高調波成分が除去された変換後電圧V1の信号波形S1と、LPF16により高調波成分が除去された電圧V2の信号波形S2とを比較する比較部18と、比較部18により比較された結果に基づき所定の演算を行う演算部19と、演算部19による演算結果に基づき位相パルス幅を測定する位相パルス幅測定部20と、LPF16により高調波成分が除去された電圧V2の信号から被測定電線路Aの電圧線路に発生している電源周波数を測定する電源周波数測定部21と、位相パルス幅測定部20で測定された位相パルスと、電源周波数測定部21で測定された電源周波数から被測定電線路Aに流れる漏洩電流Iの位相角度を算出する位相角度算出部22と、全波整流部13で整流された変換後電圧V1をデジタル信号に変換するA/D変換部23と、A/D変換部23でデジタル信号に変換された変換後電圧V1の実効値を算出する実効値算出部24と、全波整流部17で整流された電圧V2をデジタル信号に変換するA/D変換部25と、A/D変換部25でデジタル信号に変換された電圧V2の実効値を算出する実効値算出部26と、位相角度算出部22で算出された漏洩電流Iの位相角度と、実効値算出部24で算出された変換後電圧V1の実効値から対地絶縁抵抗に起因する漏洩電流Igrを算出する漏洩電流算出部27と、位相角度算出部22で算出された漏洩電流Iの位相角度と、実効値算出部26で算出された電圧V2の実効値から対地絶縁抵抗の抵抗値を算出する抵抗値算出部28と、漏洩電流算出部27で算出された漏洩電流Igrが、任意の値を超えたかどうかを判断する判断部29と、判断部29による判断に基づいて、被測定電線路Aを遮断する遮断部30と、外部機器と通信する通信部33を備えてなる。   As shown in FIG. 1, the leakage current interrupting device 1 is clamped to the entire measured electrical line A, and detects a leakage current I flowing in the measured electrical line A (hereinafter referred to as “CT sensor”). Unit 10, the leakage current I detected by the CT sensor unit 10 is converted into a voltage, and the converted voltage (hereinafter referred to as "converted voltage") V1 is amplified, and the converted voltage after amplification A low-pass filter (hereinafter referred to as LPF) 12 that removes harmonic components from V1, a full-wave rectifier 13 that rectifies the converted voltage V1 from which harmonic components have been removed by the LPF 12, and a voltage line of the measured electric line A Voltage detector 14 for detecting voltage V2 from voltage transformer 15, transformer 15 for transforming voltage V2 detected by voltage detector 14 to a predetermined transformation ratio, and transformer 15 transformed to a predetermined voltage value. Voltage V2 Low-pass filter (hereinafter referred to as LPF) 16 for removing harmonic components, full-wave rectifying unit 17 for rectifying voltage V2 from which harmonic components have been removed by LPF 16, and post-conversion from which harmonic components have been removed by LPF 12 The comparison unit 18 that compares the signal waveform S1 of the voltage V1 with the signal waveform S2 of the voltage V2 from which the harmonic component has been removed by the LPF 16, and the calculation unit 19 that performs a predetermined calculation based on the comparison result by the comparison unit 18 And a phase pulse width measuring unit 20 that measures the phase pulse width based on the calculation result by the calculating unit 19 and a voltage V2 signal from which the harmonic component has been removed by the LPF 16 The power source frequency measuring unit 21 that measures the power source frequency being measured, the phase pulse measured by the phase pulse width measuring unit 20, and the power source measured by the power source frequency measuring unit 21 A phase angle calculation unit 22 that calculates the phase angle of the leakage current I flowing in the measured electrical line A from the frequency, and an A / D conversion unit 23 that converts the converted voltage V1 rectified by the full-wave rectification unit 13 into a digital signal. An effective value calculator 24 for calculating an effective value of the converted voltage V1 converted into a digital signal by the A / D converter 23, and an A for converting the voltage V2 rectified by the full-wave rectifier 17 into a digital signal. / D conversion unit 25, effective value calculation unit 26 for calculating the effective value of voltage V2 converted into a digital signal by A / D conversion unit 25, and phase angle of leakage current I calculated by phase angle calculation unit 22 A leakage current calculation unit 27 that calculates the leakage current Igr caused by the ground insulation resistance from the effective value of the converted voltage V1 calculated by the effective value calculation unit 24; and the leakage current I calculated by the phase angle calculation unit 22 Phase angle and RMS calculation Whether the resistance value calculation unit 28 that calculates the resistance value of the ground insulation resistance from the effective value of the voltage V2 calculated by the output unit 26 and whether the leakage current Igr calculated by the leakage current calculation unit 27 exceeds an arbitrary value Are determined, a blocking unit 30 that blocks the measured electrical line A, and a communication unit 33 that communicates with an external device.

また、遮断部30は、既存の漏電ブレーカに準じており、遮断スピードは概ね2サイクル(50Hzの場合には0.04秒)〜5サイクル(50Hzの場合には0.1秒)程度である。また、本願発明に係る漏洩電流遮断装置1では、図1中のB部分をチップ化し、既存のブレーカにおけるIの検出を行うブロック(回路)に置き換えて構成されるものを想定している。 Moreover, the interruption | blocking part 30 is based on the existing earth-leakage breaker, and interruption | blocking speed is about 2 cycles (0.04 second in the case of 50 Hz)-about 5 cycles (0.1 second in the case of 50 Hz). . Further, in the leakage current interrupting device 1 according to the present invention, it is assumed that the portion B in FIG. 1 is formed into a chip and replaced with a block (circuit) for detecting I 0 in an existing breaker.

CTセンサ部10は、被測定電線路Aに流れている漏洩電流成分から生じる磁気を検出し、検出した磁気から電流を生成する。CTセンサ部10は、生成した電流を漏洩電流Iとして増幅部11に供給する。なお、CTセンサ部10により生成された漏洩電流Iは、対地静電容量に起因する漏洩電流Igcと、絶縁抵抗に直接関与している対地絶縁抵抗に起因する漏洩電流Igrとが含まれている。なお、漏洩電流Igcは、被測定線路Aの長さに応じて容量が増大するだけでなく、電気機器に使用されているインバータやノイズフィルター等に起因する高調波歪み電流によっても容量が増大する。   The CT sensor unit 10 detects magnetism generated from a leakage current component flowing in the electric wire path A to be measured, and generates a current from the detected magnetism. The CT sensor unit 10 supplies the generated current as the leakage current I to the amplification unit 11. Note that the leakage current I generated by the CT sensor unit 10 includes a leakage current Igc caused by the ground capacitance and a leakage current Igr caused by the ground insulation resistance that is directly involved in the insulation resistance. . Note that the leakage current Igc not only increases in capacity according to the length of the line A to be measured, but also increases in capacity due to harmonic distortion current caused by an inverter, a noise filter, or the like used in the electrical equipment. .

増幅部11は、CTセンサ部10から供給された漏洩電流Iを電圧に変換し、変換後電圧V1を所定のレベルまで増幅する。また、増幅部11は、例えば、CTセンサ部10から供給された漏洩電流Iが0mA〜10mAのときには、二段で増幅し、また、CTセンサ部10から供給された漏洩電流Iが10mA〜300mAのときには、一段で増幅する。増幅部11は、増幅後の変換後電圧V1をLPF12に供給する。LPF12は、変換後電圧V1に含まれている高調波成分を除去する。LPF12は、高調波成分が除去された変換後電圧V1を全波整流部13と比較部18に供給する。全波整流部13は、供給された変換後電圧V1を整流し、整流後の変換後電圧V1をA/D変換部23に供給する。   The amplifying unit 11 converts the leakage current I supplied from the CT sensor unit 10 into a voltage, and amplifies the converted voltage V1 to a predetermined level. For example, when the leakage current I supplied from the CT sensor unit 10 is 0 mA to 10 mA, the amplification unit 11 amplifies in two stages, and the leakage current I supplied from the CT sensor unit 10 is 10 mA to 300 mA. In this case, it is amplified in one stage. The amplifying unit 11 supplies the converted voltage V1 after amplification to the LPF 12. The LPF 12 removes harmonic components contained in the converted voltage V1. The LPF 12 supplies the converted voltage V1 from which the harmonic component has been removed to the full-wave rectification unit 13 and the comparison unit 18. The full-wave rectification unit 13 rectifies the supplied converted voltage V <b> 1 and supplies the converted voltage V <b> 1 after rectification to the A / D conversion unit 23.

電圧検出部14は、被測定電線路Aに電圧プローブを接続することにより、電圧線路に発生している電圧を検出する。なお、電圧検出部14は、被測定電線路Aの電気方式が三相3線式(デルタ結線からなる方式)の場合には、S相(接地)以外のR相とT相間の電圧を検出する。また、電圧検出部14は、被測定電線路Aの電気方式が三相4線式(スター結線からなる方式)の場合には、接地線以外の相間から電圧を検出する。また、電圧検出部14は、被測定電線路Aの電気方式が単相2線式の場合には、N相とL相間の電圧を検出する。   The voltage detection unit 14 detects a voltage generated in the voltage line by connecting a voltage probe to the measured electric line A. The voltage detector 14 detects the voltage between the R phase and the T phase other than the S phase (ground) when the electrical system of the measured electrical line A is a three-phase three-wire system (a system comprising a delta connection). To do. Moreover, the voltage detection part 14 detects a voltage from between phases other than a grounding wire, when the electrical system of the to-be-measured electric wire A is a three-phase four-wire system (system which consists of star connection). Moreover, the voltage detection part 14 detects the voltage between N phase and L phase, when the electrical system of the to-be-measured electrical line A is a single phase 2 wire type.

そして、電圧検出部14は、被測定電線路Aから検出した電圧V2から基準点を求め、電圧V2を変圧器15に供給する。例えば、電圧検出部14は、被測定電線路Aから検出した電圧V2の0クロスする点を基準点とする。   Then, the voltage detection unit 14 obtains a reference point from the voltage V <b> 2 detected from the measured electric line A, and supplies the voltage V <b> 2 to the transformer 15. For example, the voltage detection unit 14 uses a point where the voltage V2 detected from the measured electric wire A crosses zero as a reference point.

変圧器15は、供給された電圧V2を所定の電圧値に変圧し、変圧後の電圧VをLPF16に供給する。変圧器15は、例えば、電圧比が20:1になるように変圧を行う。LPF16は、供給された電圧V2に含まれている高調波成分を除去する。LPF16は、高調波成分を除去した電圧V2を全波整流部17と、比較部18と、電源周波数測定部21に供給する。全波整流部17は、供給された電圧V2を整流し、整流後の電圧V2をA/D変換部25に供給する。   The transformer 15 transforms the supplied voltage V2 to a predetermined voltage value, and supplies the transformed voltage V to the LPF 16. For example, the transformer 15 performs voltage transformation so that the voltage ratio is 20: 1. The LPF 16 removes harmonic components contained in the supplied voltage V2. The LPF 16 supplies the voltage V <b> 2 from which the harmonic component has been removed to the full wave rectification unit 17, the comparison unit 18, and the power supply frequency measurement unit 21. The full-wave rectifier 17 rectifies the supplied voltage V <b> 2 and supplies the rectified voltage V <b> 2 to the A / D converter 25.

比較部18では、LPF12から供給された変換後電圧V1の0Vクロス点をとり、方形波変換を行い、方形波変換後の信号を演算部19に供給する。また、比較部18では、LPF16から供給された電圧V2の0Vクロス点をとり、方形波変換を行い、方形波変換後の信号を演算部19に供給する。   The comparison unit 18 takes a 0V cross point of the converted voltage V1 supplied from the LPF 12, performs square wave conversion, and supplies the square wave converted signal to the arithmetic unit 19. Further, the comparison unit 18 takes the 0V cross point of the voltage V <b> 2 supplied from the LPF 16, performs square wave conversion, and supplies the square wave converted signal to the calculation unit 19.

演算部19は、比較部18から供給される信号に基づき所定の演算を行い、演算後の信号を位相パルス幅測定部20に供給する。演算部19は、例えば、EXOR(排他的論理和)回路からなっており、比較部18から供給されてきた2つの方形波変換後の信号についてEXOR演算を実行する。   The calculation unit 19 performs a predetermined calculation based on the signal supplied from the comparison unit 18 and supplies the calculated signal to the phase pulse width measurement unit 20. The arithmetic unit 19 is composed of, for example, an EXOR (exclusive OR) circuit, and executes an EXOR operation on the two signals after square wave conversion supplied from the comparison unit 18.

位相パルス幅測定部20は、演算部19から供給される演算結果に基づき、変換後電圧V1と電圧V2の位相パルス幅を検出する。ここで、位相パルス幅測定部20の動作について説明する。   The phase pulse width measurement unit 20 detects the phase pulse widths of the converted voltage V1 and voltage V2 based on the calculation result supplied from the calculation unit 19. Here, the operation of the phase pulse width measurement unit 20 will be described.

電気方式が単相の場合には、図2Aに示すように、漏洩電流Igrの位相角θは0°、漏洩電流Igcの位相角θは90°となる。したがって、漏洩電流Igrと漏洩電流Igcの位相差は、90°(1/4サイクル)となる。また、電源が三相の場合には、図2Bに示すように、漏洩電流Igrの位相角θは60°、漏洩電流Igcの位相角θは0°となる。したがって、漏洩電流Igrと漏洩電流Igcの位相差は、60°(1/6サイクル)となる。そこで、位相パルス幅測定部20は、電源が単相のときでも、三相のときでも対応できるように、位相パルス幅を1サイクルの1/4以下のもののみ対象とする。   When the electrical system is a single phase, as shown in FIG. 2A, the phase angle θ of the leakage current Igr is 0 °, and the phase angle θ of the leakage current Igc is 90 °. Therefore, the phase difference between the leakage current Igr and the leakage current Igc is 90 ° (1/4 cycle). When the power source is three-phase, as shown in FIG. 2B, the phase angle θ of the leakage current Igr is 60 °, and the phase angle θ of the leakage current Igc is 0 °. Therefore, the phase difference between the leakage current Igr and the leakage current Igc is 60 ° (1/6 cycle). Therefore, the phase pulse width measuring unit 20 targets only a phase pulse width of ¼ or less of one cycle so that it can cope with a single-phase power supply or a three-phase power supply.

ゆえに、位相パルス幅測定部20は、演算部19から供給される演算結果に基づいて算出した、1サイクルの1/4以下の位相パルス幅を位相角度算出部22に出力する。なお、電源周波数が60Hzの場合には、1サイクルが16.6msであるので、位相パルス幅は、4.15ms以下となり、また、電源周波数が50Hzの場合には、1サイクルが20msであるので、5ms以下となる。   Therefore, the phase pulse width measurement unit 20 outputs to the phase angle calculation unit 22 a phase pulse width that is calculated based on the calculation result supplied from the calculation unit 19 and is ¼ or less of one cycle. When the power supply frequency is 60 Hz, one cycle is 16.6 ms, so the phase pulse width is 4.15 ms or less. When the power supply frequency is 50 Hz, one cycle is 20 ms. 5 ms or less.

電源周波数測定部21は、LPF16から供給された電圧V2に基づき、電源周波数を測定し、測定結果を位相角度算出部22に供給する。なお、被測定電線路Aが商用電源であれば、電源周波数測定部21の測定結果は、50Hz若しくは60Hzとなる。また、電源周波数測定部21は、LPF16から供給された電圧V2に基づき、50Hz又は60Hzの何れかを判定する構成であっても良い。   The power supply frequency measurement unit 21 measures the power supply frequency based on the voltage V <b> 2 supplied from the LPF 16 and supplies the measurement result to the phase angle calculation unit 22. In addition, if the to-be-measured electric line A is a commercial power supply, the measurement result of the power supply frequency measurement part 21 will be 50 Hz or 60 Hz. The power supply frequency measuring unit 21 may be configured to determine either 50 Hz or 60 Hz based on the voltage V2 supplied from the LPF 16.

位相角度算出部22は、位相パルス幅測定部20から供給された位相パルス幅Wと、電源周波数測定部21から供給された電源周波数Fに基づき、下記(1)式により被測定電線路Aに流れている漏洩電流Iの位相角度θを算出する。
θ=360×W×F・・・(1)
Based on the phase pulse width W supplied from the phase pulse width measurement unit 20 and the power supply frequency F supplied from the power supply frequency measurement unit 21, the phase angle calculation unit 22 is connected to the measured electrical line A according to the following equation (1). The phase angle θ of the flowing leakage current I is calculated.
θ = 360 × W × F (1)

位相角度算出部22は、算出した位相角度θを漏洩電流算出部27に供給する。   The phase angle calculation unit 22 supplies the calculated phase angle θ to the leakage current calculation unit 27.

A/D変換部23は、全波整流部13から供給された整流後の変換後電圧V1をデジタル信号に変換し、変換後の信号を実効値算出部24に供給する。実効値算出部24は、A/D変換部23から供給された信号に基づき、下記(2)式により変換後電圧V1の実効値Iを算出する。なお、実効値算出部24に供給される信号は、被測定電線路Aに流れている漏洩電流Iを電圧に変換した変換後電圧V1に基づくものであるので、便宜的にIとする。
=I×(π/2)/√2・・・(2)
The A / D converter 23 converts the rectified converted voltage V <b> 1 supplied from the full-wave rectifier 13 into a digital signal, and supplies the converted signal to the effective value calculator 24. Based on the signal supplied from the A / D conversion unit 23, the effective value calculation unit 24 calculates the effective value I 0 of the converted voltage V1 by the following equation (2). The signal supplied to the effective value calculating unit 24, since it is based on the converted voltage V1 obtained by converting the leakage current I flowing through the measured electric line A to the voltage, and convenience I 0.
I 0 = I × (π / 2) / √2 (2)

実効値算出部24は、算出した実効値Iを漏洩電流算出部27に供給する。 The effective value calculation unit 24 supplies the calculated effective value I 0 to the leakage current calculation unit 27.

また、A/D変換部25は、全波整流部17から供給された整流後の電圧V2をデジタル信号に変換し、変換後の信号を実効値算出部26に供給する。実効値算出部26は、A/D変換部25から供給された信号に基づき、下記(3)式により電圧V2の実効値V0を算出する。
V0=V×(π/2)√2・・・(3)
The A / D converter 25 converts the rectified voltage V <b> 2 supplied from the full-wave rectifier 17 into a digital signal and supplies the converted signal to the effective value calculator 26. Based on the signal supplied from the A / D converter 25, the effective value calculator 26 calculates an effective value V0 of the voltage V2 by the following equation (3).
V0 = V × (π / 2) √2 (3)

実効値算出部26は、算出した実効値V0を抵抗値算出部28に供給する。   The effective value calculation unit 26 supplies the calculated effective value V0 to the resistance value calculation unit 28.

漏洩電流算出部27は、位相角度算出部22から供給された位相角度θと、実効値算出部24から供給されたIに基づき、漏洩電流Igrを算出し、算出した漏洩電流Igrを抵抗値算出部28に供給する。なお、電源が単相電源の場合には、下記(4)式により漏洩電流Igrを算出し、電源が三相電源の場合には、下記(5)式により漏洩電流Igrを算出する。
Igr=I×cosθ・・・(4)
Igr=(I×sinθ)/cos30°・・・(5)
Leakage current calculator 27, a phase angle calculator 22 phase angle θ supplied from, based on I 0 supplied from the effective value calculating section 24 calculates the leakage current Igr, calculated leakage current Igr the resistance It supplies to the calculation part 28. When the power source is a single-phase power source, the leakage current Igr is calculated by the following equation (4). When the power source is a three-phase power source, the leakage current Igr is calculated by the following equation (5).
Igr = I 0 × cos θ (4)
Igr = (I 0 × sin θ) / cos 30 ° (5)

なお、漏洩電流算出部27は、電源が単相電源であるか三相電源であるかを、ロータリースイッチの選択状態に応じて判断することとする。   The leakage current calculation unit 27 determines whether the power source is a single-phase power source or a three-phase power source according to the selection state of the rotary switch.

抵抗値算出部28は、実効値算出部26から供給された実効値V0と、漏洩電流算出部27から供給された漏洩電流Igrに基づき、下記(6)式によりGrを算出する。
Gr=V0/Igr・・・(6)
Based on the effective value V0 supplied from the effective value calculating unit 26 and the leakage current Igr supplied from the leakage current calculating unit 27, the resistance value calculating unit 28 calculates Gr by the following equation (6).
Gr = V0 / Igr (6)

判断部29は、漏洩電流算出部27で算出された漏洩電流Igrが任意の値を超えている場合には、所定の遮断信号SCを生成し、生成した遮断信号SCを遮断部30に供給する。   When the leakage current Igr calculated by the leakage current calculation unit 27 exceeds an arbitrary value, the determination unit 29 generates a predetermined cutoff signal SC and supplies the generated cutoff signal SC to the cutoff unit 30. .

遮断部30は、判断部29から供給された遮断信号SCに基づき、被測定電線路Aを遮断する。また、遮断部30は、図3に示すように、引き外しコイルTC等により構成されており、判断部29から供給される遮断信号SCに基づいて被測定電線路Aを遮断する。   The blocking unit 30 blocks the measured electric line A based on the blocking signal SC supplied from the determination unit 29. Moreover, the interruption | blocking part 30 is comprised by the trip coil TC etc., as shown in FIG. 3, and interrupts | blocks the to-be-measured electric wire A based on the interruption | blocking signal SC supplied from the judgment part 29. FIG.

また、漏洩電流遮断装置1は、任意の値を設定する設定部31を備え、漏洩電流算出部27で算出された漏洩電流Igrが、設定部31で設定された任意の値を超えているかどうかを判断部29で判断する構成であっても良い。また、このような構成の場合、設定部31は、予め定められている複数の値をロータリースイッチで選択できるような構成であっても良い。また、値は、例えば、10mAステップで設定されている。   Further, the leakage current interrupting device 1 includes a setting unit 31 that sets an arbitrary value, and whether or not the leakage current Igr calculated by the leakage current calculation unit 27 exceeds an arbitrary value set by the setting unit 31. May be determined by the determination unit 29. In such a configuration, the setting unit 31 may be configured such that a plurality of predetermined values can be selected with a rotary switch. Also, the value is set, for example, in 10 mA steps.

また、漏洩電流遮断装置1は、漏洩電流算出部27により算出された漏洩電流Igrを記録する記録部32を備える構成であっても良い。記録部32では、漏洩電流算出部27により算出された漏洩電流Igrを経過時間ごとに記録するので、ユーザは、漏洩電流Igrの時間的な変化の様子を把握することができる。   Moreover, the leakage current interrupting device 1 may be configured to include a recording unit 32 that records the leakage current Igr calculated by the leakage current calculation unit 27. Since the recording unit 32 records the leakage current Igr calculated by the leakage current calculation unit 27 for each elapsed time, the user can grasp how the leakage current Igr changes with time.

例えば、ユーザは、通信コネクタを介してモニタ装置を漏洩電流遮断装置1に接続し、記録部32に記憶されているデータにアクセスする。なお、漏洩電流遮断装置1には、予め固有の識別番号をセットしておく。   For example, the user connects the monitor device to the leakage current interrupting device 1 via the communication connector, and accesses the data stored in the recording unit 32. The leakage current interrupting device 1 is set with a unique identification number in advance.

モニタ装置は、通信コネクタを介して、漏洩電流遮断装置1から、実効値算出部24で算出された実効値Iと、漏洩電流算出部27で算出された漏洩電流Igrと、電圧検出部14で検出した被測定電線路Aの電圧値Vと、電源周波数測定部21で測定された周波数と、漏洩電流遮断装置1の識別番号を読み出す。また、モニタ装置は、通信部33と接続されるコネクタの形状を丸形コネクタとし、通信部33との接触不良をなくすため、外れ防止機構を備えている。 The monitor device, through the communication connector, from the leakage current interrupting device 1, the effective value I 0 calculated by the effective value calculation unit 24, the leakage current Igr calculated by the leakage current calculation unit 27, and the voltage detection unit 14. The voltage value V of the line A to be measured detected in step 1, the frequency measured by the power frequency measuring unit 21 and the identification number of the leakage current interrupting device 1 are read out. In addition, the monitor device has a round connector as the shape of the connector connected to the communication unit 33, and is provided with a disconnection prevention mechanism in order to eliminate poor contact with the communication unit 33.

記録部32に記録されているデータを参照し、漏洩電流Igrの時間的な変化の様子から、例えば、瞬時に漏洩電流Igrが任意の値に達していることを把握した場合には、漏洩電流Igrが任意の値に達したときに起動させた機器、若しくは起動中の機器が漏電の原因である疑いが強いので、これを手がかりにして、漏電箇所の特定ができる。   With reference to the data recorded in the recording unit 32, for example, when it is grasped that the leakage current Igr instantaneously reaches an arbitrary value from the state of temporal change of the leakage current Igr, the leakage current Since there is a strong suspicion that the device activated when Igr reaches an arbitrary value or the activated device is the cause of the leakage, the leakage location can be specified using this as a clue.

また、漏洩電流Igrの時間的な変化の様子から、例えば、徐々に漏洩電流Igrが増えていることを把握した場合には、起動中の機器を検査することにより、漏電の原因となる機器を早期に発見することができる。   In addition, for example, when it is grasped from the state of the change of the leakage current Igr over time that the leakage current Igr is gradually increasing, by checking the activated device, the device that causes the leakage is detected. It can be discovered early.

上述のように構成される本願発明に係る漏洩電流遮断装置1では、例えば、被測定電線路Aの電源が三相式の場合、電源を単相式と同様の処理が可能な構成となっている。ここで、本願発明に係る漏洩電流遮断装置1の原理について述べる。   In the leakage current interrupting device 1 according to the present invention configured as described above, for example, when the power source of the measured electrical line A is a three-phase type, the power source can be processed in the same manner as the single-phase type. Yes. Here, the principle of the leakage current interrupting device 1 according to the present invention will be described.

CTセンサ部10は、被測定電線路Aをクランプし、図4Aに示すように、位相が120°ずつ異なるR相−S相間、S相−T相間及びT相−R相間の波形を検出する。なお、図4Aでは、便宜的にそれぞれの波形を示しているが、CTセンサ部10で検出される波形は合成波形である。CTセンサ部10により検出された合成波形は、増幅部11、LPF12及び比較部18を介して演算部19に入力される。   The CT sensor unit 10 clamps the electric wire A to be measured, and detects waveforms between the R phase and the S phase, between the S phase and the T phase, and between the T phase and the R phase, which are different in phase by 120 °, as shown in FIG. 4A. . In FIG. 4A, each waveform is shown for convenience, but the waveform detected by the CT sensor unit 10 is a synthesized waveform. The combined waveform detected by the CT sensor unit 10 is input to the calculation unit 19 via the amplification unit 11, the LPF 12, and the comparison unit 18.

また、電圧検出部14は、R相及びT相に電圧プローブを接続し、R相−T相間の電圧を検出し、検出した電圧を、図4Bに示すように、反転させる。電圧検出部14は、検出した電圧の所定の場所で0クロスする点を基準点aとして定める。このように基準点aが定まった電圧V2は、変圧器15、LPF16及び比較部18を介して演算部19に入力される。   Further, the voltage detection unit 14 connects voltage probes to the R phase and the T phase, detects a voltage between the R phase and the T phase, and inverts the detected voltage as shown in FIG. 4B. The voltage detector 14 determines a point at which the detected voltage crosses zero at a predetermined location as a reference point a. The voltage V2 with the reference point a determined in this way is input to the arithmetic unit 19 via the transformer 15, the LPF 16, and the comparison unit 18.

例えば、被測定電線路AのR相に漏洩電流Igr(以下「R相Igr」という。)のみが発生し、また、T相に漏洩電流Igr(以下「T相Igr」という。)のみが発生している場合には、図4Cに示すように、R相Igrは、基準点aから120°の位相差が生じ、T相Igrは、基準点aから60°の位相差が生じる。   For example, only the leakage current Igr (hereinafter referred to as “R phase Igr”) is generated in the R phase of the measured electrical line A, and only the leakage current Igr (hereinafter referred to as “T phase Igr”) is generated in the T phase. In this case, as shown in FIG. 4C, the R phase Igr has a phase difference of 120 ° from the reference point a, and the T phase Igr has a phase difference of 60 ° from the reference point a.

また、被測定電線路AのR相に漏洩電流Igc(以下「R相Igc」という。)のみが発生し、また、T相に漏洩電流Igc(以下「T相Igc」という。)のみが発生している場合には、図4Dに示すように、R相IgcとT相Igcの合成波形の基準点aからの位相差は、180°(0°)である。   Further, only the leakage current Igc (hereinafter referred to as “R phase Igc”) is generated in the R phase of the measured electrical line A, and only the leakage current Igc (hereinafter referred to as “T phase Igc”) is generated in the T phase. In this case, as shown in FIG. 4D, the phase difference from the reference point a of the combined waveform of the R phase Igc and the T phase Igc is 180 ° (0 °).

さらに、被測定電線路AのR相に漏洩電流Igrと漏洩電流Igcとが発生し、T相に漏洩電流Igrと漏洩電流Igcとが発生している場合には、図4Eに示すようになる。   Furthermore, when the leakage current Igr and the leakage current Igc are generated in the R phase of the electric wire A to be measured and the leakage current Igr and the leakage current Igc are generated in the T phase, the result is as shown in FIG. 4E. .

また、上述の説明をベクトルで表すと、以下のようになる。被測定電線路Aが三相式なので、図5Aに示すようになる。そして、電圧検出部14でR相−T相間の電圧を検出し、検出した電圧から基準点aを求めると、図5Bに示すように、単相式のベクトル図となる。なお、上述したように、R相Igrと基準点aとの位相差は、60°であり、また、T相Igrと基準点aとの位相差は、120°である。   Further, the above description can be expressed as a vector as follows. Since the wire A to be measured is a three-phase type, it is as shown in FIG. 5A. Then, when the voltage between the R phase and the T phase is detected by the voltage detection unit 14 and the reference point a is obtained from the detected voltage, a single-phase vector diagram is obtained as shown in FIG. 5B. As described above, the phase difference between the R phase Igr and the reference point a is 60 °, and the phase difference between the T phase Igr and the reference point a is 120 °.

また、単相式の場合には、図2Aを用いて既述したように、漏洩電流Igrと漏洩電流Igcの位相差は90°なので、R相Igrから90°回った位置にR相Igcを求めることができ、また、T相Igrから90°回った位置にT相Igcを求めることができる。さらに、基準点aから180°(0°)の位置に、R相IgcとT相Igcとの合成ベクトルIgcを求めることができる(図5C)。   In the case of the single-phase type, as already described with reference to FIG. 2A, since the phase difference between the leakage current Igr and the leakage current Igc is 90 °, the R-phase Igc is set at a position rotated 90 ° from the R-phase Igr. Further, the T phase Igc can be obtained at a position rotated by 90 ° from the T phase Igr. Furthermore, a combined vector Igc of the R phase Igc and the T phase Igc can be obtained at a position 180 ° (0 °) from the reference point a (FIG. 5C).

したがって、例えば、被測定電線路AにR相Igrのみが発生している場合には、R相IgrとIgcとの合成ベクトル、すなわち被測定電線路Aに流れている漏洩電流Iは、図5Dのように表すことができる。なお、図5Dから、R相Igrを算出する式として、上述した(5)式を導き出すことができる。また、漏洩電流Iの位相差θは、R相Igr及びIgcの大きさにより変化し、変化の幅は、基準点aから60°〜180°である。 Therefore, for example, when only the R phase Igr is generated in the measured electrical line A, the combined vector of the R phase Igr and Igc, that is, the leakage current I 0 flowing in the measured electrical line A is It can be expressed as 5D. Note that, from FIG. 5D, the above-described equation (5) can be derived as an equation for calculating the R phase Igr. Further, the phase difference θ of the leakage current I 0 changes depending on the magnitudes of the R phases Igr and Igc, and the range of change is 60 ° to 180 ° from the reference point a.

また、例えば、被測定電線路AにT相Igrのみが発生している場合には、T相IgrとIgcとの合成ベクトル、すなわち被測定電線路Aに流れている漏洩電流Iは、図5Eのように表すことができる。なお、図5Eから、T相Igrを算出する式として、上述した(5)式を導き出すことができる。また、漏洩電流Iの位相差θは、T相Igr及びIgcの大きさにより変化し、変化の幅は、120°〜180°である。 For example, when only the T-phase Igr is generated in the measured electrical line A, the combined vector of the T-phase Igr and Igc, that is, the leakage current I 0 flowing in the measured electrical line A is It can be expressed as 5E. Note that the above-described equation (5) can be derived from FIG. 5E as an equation for calculating the T-phase Igr. In addition, the phase difference θ of the leakage current I 0 changes depending on the magnitudes of the T phases Igr and Igc, and the range of change is 120 ° to 180 °.

ここで、上述に示した本願発明に係る漏洩電流遮断装置1により、被測定電線路Aに流れる漏洩電流Igrを検出し、検出した漏洩電流Igrに基づいて、被測定電線路Aを遮断する動作について図6に示すフローチャートを用いて説明する。なお、漏洩電流遮断装置1は、既存の漏電ブレーカ内に収納することを想定しているが、収納できない場合には、外付けであっても良い。   Here, the leakage current interruption device 1 according to the present invention shown above detects the leakage current Igr flowing through the measured electric line A, and based on the detected leakage current Igr, the operation of interrupting the measured electric line A Will be described with reference to the flowchart shown in FIG. The leakage current interrupting device 1 is assumed to be housed in an existing earth leakage breaker, but may be externally attached when it cannot be housed.

ステップST1において、ユーザは、被測定電線路Aの種類(単相2線式、単相3線式及び三相3線式等)に応じて、漏洩電流遮断装置1の図示しないロータリースイッチを切り換える。なお、ステップST1の工程では、被測定電線路Aは、遮断状態である。   In step ST1, the user switches a rotary switch (not shown) of the leakage current interrupting device 1 according to the type of the electric line A to be measured (single-phase two-wire system, single-phase three-wire system, three-phase three-wire system, etc.). . In addition, in the process of step ST1, the to-be-measured electric wire path A is a interruption | blocking state.

ステップST2において、ユーザは、設定部31を操作し、任意の値を設定する。   In step ST2, the user operates the setting unit 31 to set an arbitrary value.

ステップST3において、ユーザは、漏洩電流遮断装置1を通電状態にする。   In step ST3, the user turns on the leakage current interrupting device 1 in an energized state.

その後、漏洩電流遮断装置1は、漏洩電流算出部27により被測定電線路Aの漏洩電流Igrの算出を行い、判断部29により漏洩電流Igrが任意の値に達したかどうかの判断を行う。そして、漏洩電流遮断装置1は、判断部29により任意の値に達したと判断した場合に、遮断部30により被測定電線路Aを遮断する。   After that, the leakage current interrupting device 1 calculates the leakage current Igr of the measured electrical line A by the leakage current calculation unit 27 and determines whether the leakage current Igr has reached an arbitrary value by the determination unit 29. When the leakage current interrupting device 1 determines that the determination unit 29 has reached an arbitrary value, the leakage current interrupting device 1 interrupts the measured electrical line A by the interrupting unit 30.

ここで、本発明に係る漏洩電流遮断装置1により、実際に被測定電線路から漏洩電流成分を測定した第1の結果を図7に示す。図7は、屋上受配電キュービクル(高圧受電設備)の動力盤(電源周波数:50Hz、電圧:200V、被測定低電圧電路の種類:三相3線式、150kvA、室温:41℃、湿度:43%)を測定対象として行ったものである。   Here, FIG. 7 shows a first result of actually measuring the leakage current component from the measured electric wire line by the leakage current interrupting device 1 according to the present invention. FIG. 7 shows a power board (power frequency: 50 Hz, voltage: 200 V, type of low voltage circuit to be measured: three-phase three-wire system, 150 kvA, room temperature: 41 ° C., humidity: 43 of a rooftop distribution cubicle (high voltage power receiving equipment). %) Was measured.

また、実験では、測定開始から6分経過時〜9分経過前(3分間)に疑似絶縁抵抗としてR相に20kΩを接地し、測定開始から9分経過時〜11分経過前(2分間)に疑似絶縁抵抗としてT相に20kΩを接地し、測定開始から11分経過時〜12分経過前(1分間)に疑似絶縁抵抗を外し(接地解除)、測定開始から12分経過時〜13分経過前(1分間)に疑似絶縁抵抗としてR相に10kΩを接地し、測定開始から13分経過時〜15分経過前(2分間)に疑似絶縁抵抗としてT相に10kΩを接地し、測定開始から15分経過後に疑似絶縁抵抗を外した。
例えば、疑似絶縁抵抗としてR相に20kΩの抵抗を接地した場合には、理論的に、疑似絶縁抵抗成分の電流として、
Igr=V/R=200/(20×103)=10mA
の電流が被測定電線路に加算されて流れる。
In the experiment, 20 kΩ was grounded to the R phase as a pseudo-insulation resistance 6 minutes to 9 minutes before the start of measurement (3 minutes), and 9 minutes to 11 minutes before the start of measurement (2 minutes). As a pseudo-insulation resistance, ground 20 kΩ in the T phase, remove the pseudo-insulation resistance (11 minutes) after the elapse of 11 minutes to 12 minutes (1 minute) from the start of measurement, and 12 to 13 minutes after the start of measurement. 10kΩ is grounded to the R phase as the pseudo-insulation resistance before the passage (1 minute), and 10kΩ is grounded to the T phase as the pseudo-insulation resistance at the time of 13 minutes to 15 minutes (2 minutes) after the start of measurement. 15 minutes later, the pseudo-insulation resistance was removed.
For example, when a 20 kΩ resistor is grounded as the pseudo-insulation resistance in the R phase, theoretically, as the pseudo-insulation resistance component current,
Igr = V / R = 200 / (20 × 103) = 10 mA
Current is added to the line to be measured and flows.

漏洩電流遮断装置1は、図7に示すように、時間が6分経過時に、疑似絶縁抵抗としてR相に20kΩの抵抗を接地したら、12.3mAの漏洩電流Igrを検出した。疑似絶縁抵抗を接地していないとき(測定開始から6分経過前、測定開始から11分経過時〜12分経過前及び測定開始から15分経過後)の漏洩電流Igrが2mAであるので、R相に20kΩの疑似抵抗を接地した後の漏洩電流Igrから2mAを差し引くと、10.3mAとなる。したがって、本願発明に係る漏洩電流遮断装置1は、10.3mAの変化を測定できたことになる。この値は、上述した理論値(10mA)とほぼ一致している。   As shown in FIG. 7, the leakage current interrupting device 1 detected a leakage current Igr of 12.3 mA when a resistance of 20 kΩ was grounded to the R phase as a pseudo-insulation resistance when 6 minutes passed. Since the leakage current Igr is 2 mA when the pseudo-insulation resistance is not grounded (before 6 minutes from the start of measurement, 11 minutes after the start of measurement to 12 minutes before and 15 minutes after the start of measurement), R If 2 mA is subtracted from the leakage current Igr after grounding a pseudo resistance of 20 kΩ to the phase, it becomes 10.3 mA. Therefore, the leakage current interrupting device 1 according to the present invention can measure a change of 10.3 mA. This value almost coincides with the theoretical value (10 mA) described above.

また、R相に疑似絶縁抵抗を20kΩ接地したとき、接地前の抵抗値(Gr≒105.46kΩ(測定開始から6分経過前までのGrの平均値))との合成抵抗値は、
Gr=(20×103×105.46×103)/(20×103+105.46×103)≒16.3kΩ
となる。漏洩電流遮断装置1は、図7に示すように、測定開始から6分経過時の抵抗Grは17.2kΩを示しており、上述した理論値(16.3kΩ)とほぼ一致している。
In addition, when the pseudo insulation resistance is grounded to the R phase at 20 kΩ, the combined resistance value with the resistance value before grounding (Gr≈105.46 kΩ (average value of Gr from the start of measurement to 6 minutes before)) is
Gr = (20 × 103 × 105.46 × 103) / (20 × 103 + 105.46 × 103) ≈16.3 kΩ
It becomes. As shown in FIG. 7, the leakage current interrupting device 1 has a resistance Gr of 17.2 kΩ when 6 minutes have elapsed from the start of measurement, which is almost equal to the theoretical value (16.3 kΩ) described above.

また、疑似絶縁抵抗としてT相に20kΩの抵抗を接地した場合にも、上述と同様に、理論的には、疑似絶縁抵抗成分の電流は10mA増加する。漏洩電流遮断装置1では、図7に示すように、測定開始から9分経過時〜11分経過前に検出した漏洩電流Igrは、ほぼ12.4mAとなっており、該数値から2mAを差し引くと、10.4mAとなり、ほぼ理論値(10mA)と一致する。   Further, even when a 20 kΩ resistor is grounded as the pseudo-insulation resistance in the T phase, the current of the pseudo-insulation resistance component theoretically increases by 10 mA as described above. In the leakage current interrupting device 1, as shown in FIG. 7, the leakage current Igr detected from 9 minutes to 11 minutes after the start of measurement is approximately 12.4 mA, and when 2 mA is subtracted from the numerical value, 10.4 mA, which almost coincides with the theoretical value (10 mA).

また、T相に疑似絶縁抵抗を20kΩ接地したときの合成抵抗値Grは、上述と同様に、理論的には、16.3kΩであり、測定値は17.4kΩを示しており、ほぼ理論値と一致している。   Further, the combined resistance value Gr when the pseudo-insulation resistance is grounded to the T phase at 20 kΩ is theoretically 16.3 kΩ and the measured value is 17.4 kΩ, as described above. Is consistent with

また、漏洩電流遮断装置1は、図7に示すとおり、疑似絶縁抵抗としてR相又はT相に10kΩを接地したときの漏洩電流IgrとGrも理論値と実測値がほぼ一致している。   In addition, as shown in FIG. 7, in the leakage current interrupting device 1, the theoretical value and the actual measurement value of the leakage currents Igr and Gr when 10 kΩ is grounded as the pseudo-insulation resistance in the R phase or the T phase are substantially the same.

さらに、漏洩電流遮断装置1は、測定開始から11分経過後から12分経過前、及び15分経過時に疑似絶縁抵抗の接地状態を解除した場合、漏洩電流Igr、I及びGrの値が接地以前(測定開始から1分〜5分)の状態に戻った。 Furthermore, the leakage current cutoff device 1, prior to the expiration 12 minutes from the start of measurement after elapse of 11 minutes, and when releasing the ground state of the pseudo insulation resistance during the course 15-minute, leakage current Igr, the value of I 0 and Gr ground It returned to the previous state (from 1 minute to 5 minutes from the start of measurement).

また、本発明に係る漏洩電流遮断装置1により、実際に被測定電線路から漏洩電流成分を測定した第2の結果を図8に示す。図8は、受配電キュービクル(高圧受電設備)の動力盤(電源周波数:50Hz、電圧:200V、被測定低電圧電路の種類:三相3線式、150kvA)を測定対象として行ったものである。   Moreover, the 2nd result which actually measured the leakage current component from the to-be-measured electric wire line by the leakage current interrupting device 1 which concerns on this invention is shown in FIG. FIG. 8 shows a power board (power supply frequency: 50 Hz, voltage: 200 V, type of low-voltage circuit to be measured: three-phase three-wire system, 150 kvA) of a power distribution cubicle (high voltage power receiving equipment) as a measurement target. .

また、実験は、測定開始から1分経過時〜4分経過前(3分間)に疑似静電容量としてR相及びT相に0.22μFを接地し、測定開始から3分経過時〜4分経過前(1分間)に疑似絶縁抵抗としてT相に20kΩを接地し、測定開始から4分経過後に疑似静電容量及び疑似絶縁抵抗を外して行った。したがって、測定開始から3分経過時〜4分経過前は、R相及びT相に疑似静電容量を接地し、かつ、T相に疑似絶縁抵抗を接地して行った。   In the experiment, 1 minute elapsed from the start of measurement to 4 minutes before (3 minutes), 0.22 μF was grounded to the R phase and T phase as a pseudo capacitance, and 3 minutes elapsed from the start of measurement to 4 minutes. Before the lapse of time (1 minute), 20 kΩ was grounded to the T phase as a pseudo insulation resistance, and after 4 minutes from the start of measurement, the pseudo capacitance and the pseudo insulation resistance were removed. Therefore, from 3 minutes to 4 minutes before the start of measurement, the pseudo capacitance was grounded to the R phase and the T phase, and the pseudo insulation resistance was grounded to the T phase.

例えば、疑似静電容量としてR相及びT相に0.22μFの容量を接地した場合には、容量性リアクタンスXは、
X=1/2πfC=1/(2π×50×(0.22×10−6+0.22×10−6))
≒7.23×103
となる。
For example, when a capacitance of 0.22 μF is grounded to the R phase and the T phase as a pseudo capacitance, the capacitive reactance X is
X = 1 / 2πfC = 1 / (2π × 50 × (0.22 × 10 −6 + 0.22 × 10 −6))
≒ 7.23 × 103
It becomes.

したがって、被測定電線路には、
I=V/X=200/7.23×103≒27.6mA
の電流が加算されて流れる。
Therefore, the line to be measured has
I = V / X = 200 / 7.23 × 103≈27.6 mA
The current is added and flows.

また、絶縁抵抗としてT相に20kΩの抵抗を接地した場合には、理論的に、疑似絶縁抵抗成分の電流として、
Igr=V/R=200/(20×103)=10mA
の電流が被測定電線路に加算されて流れる。
In addition, when a 20 kΩ resistor is grounded to the T phase as an insulation resistance, theoretically, as a current of a pseudo insulation resistance component,
Igr = V / R = 200 / (20 × 103) = 10 mA
Current is added to the line to be measured and flows.

漏洩電流遮断装置1は、図8に示すように、時間が測定開始から1分経過時に、疑似静電容量としてR相及びT相に0.22μFの静電容量が接地されているときに、7.8mAの漏洩電流Igrを検出し、また、100.8mAのIを検出した。なお、Iは、上述したように絶縁抵抗に起因する漏洩電流Igrと、静電容量に起因する漏洩電流Igcの合成電流である。 As shown in FIG. 8, the leakage current interrupting device 1 has a time when 1 minute has elapsed from the start of measurement, and when a capacitance of 0.22 μF is grounded in the R phase and the T phase as a pseudo capacitance, detecting a leakage current Igr of 7.8 mA, also detected I 0 of 100.8MA. Note that I 0 is a combined current of the leakage current Igr caused by the insulation resistance and the leakage current Igc caused by the capacitance as described above.

疑似静電容量を接地していないときの漏洩電流Igrは、図8に示したとおり、7.6mA(測定開始から1分経過前の漏洩電流Igr)であるので、R相及びT相に疑似静電容量を接地した場合、漏洩電流Igrの変化は殆どない。   The leakage current Igr when the pseudo capacitance is not grounded is 7.6 mA (leakage current Igr 1 minute before the start of measurement) as shown in FIG. When the capacitance is grounded, there is almost no change in the leakage current Igr.

一方、疑似静電容量を接地していないときのIは、75.9mA(測定開始から1分経過前のI)である。疑似静電容量接地後のI(100.8mA)から疑似静電容量接地前のI(75.9mA)を差し引くと、24.9mAとなり、これが、加算された漏洩電流Igcである。この加算された漏洩電流Igcは、理論値(27.6mA)とほぼ等しい。 On the other hand, I 0 when not grounded pseudo capacitance is 75.9mA (I 0 before a lapse of one minute from the start of measurement). When the I 0 after the pseudo capacitance ground (100.8mA) subtracting the pseudo-capacitance ground before I 0 (75.9mA), 24.9mA next, which is summed leakage current Igc. This added leakage current Igc is substantially equal to the theoretical value (27.6 mA).

また、漏洩電流遮断装置1は、図8に示すように、R相及びT相に疑似静電容量が接地され、かつ、T相に疑似絶縁抵抗が接地されているとき(測定開始から3分経過時〜4分経過前)に、21.0mAの漏洩電流Igrを検出し、また、107.0mAのIを検出した。 In addition, as shown in FIG. 8, the leakage current interrupting device 1 is configured such that when the pseudo capacitance is grounded in the R phase and the T phase and the pseudo insulation resistance is grounded in the T phase (3 minutes from the start of measurement). Between the lapse of time and before the lapse of 4 minutes, a leakage current Igr of 21.0 mA was detected, and an I 0 of 107.0 mA was detected.

T相に絶縁抵抗を接地した後の漏洩電流Igr(21mA)から、絶縁抵抗を接地する前の漏洩電流Igr(8mA(測定開始から3分経過時の漏洩電流Igr))を差し引くと、13mAとなり、理論値(10mA)とほぼ等しくなる。   When the leakage current Igr (8 mA (leakage current Igr after 3 minutes from the start of measurement)) before grounding the insulation resistance is subtracted from the leakage current Igr (21 mA) after grounding the insulation resistance to the T phase, 13 mA is obtained. , Approximately equal to the theoretical value (10 mA).

また、R相に疑似絶縁抵抗として10kΩを接地したときの比較部18と演算部19の動作について図9〜図11を用いて説明する。   Further, the operations of the comparison unit 18 and the calculation unit 19 when 10 kΩ is grounded as a pseudo insulation resistance in the R phase will be described with reference to FIGS. 9 to 11.

比較部18は、図9に示すように、LPF12から変換後電圧V1が入力され、LPF16から電圧V2が入力される。変換後電圧V1と電圧V2の位相差は、120°である。比較部18は、図10Aに示すように、LPF12から入力された変換後電圧V1を方形波変換し、変換後の信号を演算部19に出力する。また、比較部18は、図10Bに示すように、LPF16から入力された電圧V2を方形波変換し、変換後の信号を演算部19に出力する。   As shown in FIG. 9, the comparison unit 18 receives the converted voltage V <b> 1 from the LPF 12 and receives the voltage V <b> 2 from the LPF 16. The phase difference between the converted voltage V1 and the voltage V2 is 120 °. As shown in FIG. 10A, the comparison unit 18 performs square wave conversion on the converted voltage V <b> 1 input from the LPF 12, and outputs the converted signal to the calculation unit 19. Further, as illustrated in FIG. 10B, the comparison unit 18 performs square wave conversion on the voltage V <b> 2 input from the LPF 16, and outputs the converted signal to the calculation unit 19.

演算部19は、図11に示すように、変換後電圧V2の方形波信号と、電圧V2の方形波信号に基づき、EXOR演算を実行する。演算部19は、EXOR演算後の信号に基づき、1サイクルの1/4以下の位相パルス幅を求め、求めた位相パルス幅を位相角度算出部22に出力する。   As shown in FIG. 11, the arithmetic unit 19 performs an EXOR operation based on the square wave signal of the converted voltage V2 and the square wave signal of the voltage V2. The computing unit 19 obtains a phase pulse width equal to or less than ¼ of one cycle based on the signal after the EXOR computation, and outputs the obtained phase pulse width to the phase angle calculating unit 22.

ステップST6において、ユーザは、測定が終了したら、漏洩電流遮断装置1の電源をOFFにする。   In step ST6, when the measurement is completed, the user turns off the power of the leakage current interrupter 1.

このように構成される本願発明に係る漏洩電流遮断装置1は、被測定電線路Aに流れている漏洩電流Iを検出し、検出した漏洩電流Iを電圧に変換し、変換後の電圧から高調波成分を除去し、高調波成分を除去した変換後電圧V1と、被測定電線路Aの電圧線路から電圧V2を検出し、検出した電圧V2から高調波成分を除去し、高調波成分を除去した電圧V2とに基づき、被測定電線路Aに流れている漏洩電流Iの位相角度θを正確に求め、その正確な位相角度θと、高調波成分が除去された変換後電圧V1の実効値Iとから対地絶縁抵抗に起因する漏洩電流Igrのみを算出し、算出した漏洩電流Igrを監視し、漏洩電流Igrが任意の値を超えた場合に、被測定電線路Aを遮断する。したがって、本願発明に係る漏洩電流遮断装置1は、被測定電線路Aの長大化により、また、高調波歪み電流を出力するインバータ等により対地静電容量に起因した漏洩電流Igcが増大しても、mA単位で確実に対地絶縁抵抗に起因する漏洩電流Igrのみを検出することができるので、漏洩電流Igrを監視し、漏洩電流Igrが任意の値を超えた場合のみに被測定電線路Aを遮断するように動作させることができる。ゆえに、本願発明に係る漏洩電流遮断装置1は、漏洩電流Igr以外の要素(漏洩電流Igcの増大)によって漏洩電流が増大しても従来装置のように被測定電線路Aを遮断することがない。 The leakage current interrupting device 1 according to the present invention configured as described above detects the leakage current I flowing in the electric line A to be measured, converts the detected leakage current I into a voltage, and generates a harmonic from the converted voltage. The converted voltage V1 from which the wave component is removed, the harmonic component is removed, and the voltage V2 are detected from the voltage line of the line A to be measured, and the harmonic component is removed from the detected voltage V2 to remove the harmonic component. On the basis of the measured voltage V2, the phase angle θ of the leakage current I flowing in the measured electrical line A is accurately determined, and the accurate phase angle θ and the effective value of the converted voltage V1 from which the harmonic component has been removed. Only the leakage current Igr caused by the ground insulation resistance is calculated from I 0 , the calculated leakage current Igr is monitored, and when the leakage current Igr exceeds an arbitrary value, the measured electrical line A is interrupted. Therefore, the leakage current interrupting device 1 according to the present invention can increase the leakage current Igc due to the ground capacitance due to the length of the electric line A to be measured and the inverter that outputs the harmonic distortion current. Since it is possible to reliably detect only the leakage current Igr caused by the ground insulation resistance in mA units, the leakage current Igr is monitored, and only when the leakage current Igr exceeds an arbitrary value, Can be operated to shut off. Therefore, the leakage current interrupting device 1 according to the present invention does not interrupt the measured electrical line A unlike the conventional device even if the leakage current increases due to an element other than the leakage current Igr (increase in the leakage current Igc). .

また、本願発明に係る漏洩電流遮断装置1は、電路・機械設備等を一時的に停電状態にすることなく漏洩電流Igrの検出を行うことができ、また、漏電火災等の大惨事に至る前に漏電箇所の発見に役立てることができる。   In addition, the leakage current interrupting device 1 according to the present invention can detect the leakage current Igr without temporarily turning off the electric circuit / mechanical equipment, and before the occurrence of a catastrophe such as a leakage fire. It can be used to find the location of electrical leakage.

また、本願発明に係る漏洩電流遮断装置1は、周波数注入式のように基準点を他から持ってくるのではなく、基準点を伝送線路に発生している電圧から求めるので、被測定電線路Aに流れている漏洩電流Igrを正確に測定することができる。   In addition, the leakage current interrupting device 1 according to the present invention does not bring in a reference point from another as in the frequency injection type, but obtains the reference point from the voltage generated in the transmission line. The leakage current Igr flowing through A can be accurately measured.

なお、本発明は、図面を参照して説明した上述の実施例に限定されるものではなく、添付の請求の範囲及びその主旨を逸脱することなく、様々な変更、置換又はその同等のものを行うことができることは当業者にとって明らかである。   The present invention is not limited to the above-described embodiments described with reference to the drawings, and various modifications, substitutions or equivalents thereof can be made without departing from the scope and spirit of the appended claims. It will be apparent to those skilled in the art that this can be done.

本発明に係る漏洩電流検出装置の構成を示すブロック図である。It is a block diagram which shows the structure of the leakage current detection apparatus which concerns on this invention. 電源が単相の場合と三相の場合における対地絶縁抵抗に起因する漏洩電流Igrと対地静電容量に起因する漏洩電流Igcの位相差を示す図である。It is a figure which shows the phase difference of the leakage current Igg resulting from the earth insulation resistance in the case of a single phase and a three-phase power supply, and the leakage current Igc resulting from an earth capacitance. 本発明に係る漏洩電流検出装置に備えられている遮断部の構成を示す図である。It is a figure which shows the structure of the interruption | blocking part with which the leakage current detection apparatus concerning this invention is equipped. 本発明に係る漏洩電流検出装置により行われる漏洩電流の検出する様子を波形で示した図である。It is the figure which showed a mode that the leakage current performed by the leakage current detection apparatus concerning this invention was detected. 本発明に係る漏洩電流検出装置により行われる漏洩電流の検出する様子をベクトルで示した図である。It is the figure which showed a mode that the leakage current performed by the leakage current detection apparatus based on this invention was detected with the vector. 本発明に係る漏洩電流検出装置の動作について説明するフローチャートである。It is a flowchart explaining the operation | movement of the leakage current detection apparatus which concerns on this invention. 本発明に係る漏洩電流検出装置により電線路を実際に測定したときの第1のデータ例を示す図である。It is a figure which shows the 1st data example when an electric wire path is actually measured by the leakage current detection apparatus which concerns on this invention. 本発明に係る漏洩電流検出装置により電線路を実際に測定したときの第2のデータ例を示す図である。It is a figure which shows the 2nd data example when an electric wire path is actually measured by the leakage current detection apparatus which concerns on this invention. 比較部に入力された変換後電圧V1と電圧V2の位相差を示す図である。It is a figure which shows the phase difference of the converted voltage V1 and the voltage V2 which were input into the comparison part. (a)は、比較部に入力されたときの変換後電圧V1の波形と、変換後電圧V1に基づき方形波変換したときの波形を示す図であり、(b)は、比較部に入力されたときの電圧V2の波形と、電圧V2に基づき方形波変換したときの波形を示す図である。(A) is a diagram showing a waveform of the converted voltage V1 when input to the comparison unit and a waveform when square wave conversion is performed based on the converted voltage V1, and (b) is an input of the comparison unit. It is a figure which shows the waveform when a square wave conversion is performed based on the waveform of voltage V2 at the time of voltage V2. 図10に示した変換後電圧V1に基づき方形波変換したときの波形と、電圧V2に基づき方形波変換したときの波形に基づきEXORを実行した際に形成される波形を示す図である。It is a figure which shows the waveform formed when EXOR is performed based on the waveform when square-wave conversion is performed based on the converted voltage V1 shown in FIG. 10, and the waveform when square-wave conversion is performed based on the voltage V2.

符号の説明Explanation of symbols

1 漏洩電流検出装置、A 被測定電線路、10 カレントトランスセンサ(CTセンサ)部、11 増幅部、12,16 ローパスフィルター(LPF)、13,17 全波整流部、14 電圧検出部、15 変圧器、18 比較部、19 演算部、20 位相パルス幅測定部、21 電源周波数測定部、22 位相角度算出部、23,25 A/D変換部、24,26 実効値算出部、27 漏洩電流算出部、28 抵抗値算出部、29 判断部、30 遮断部、31 設定部、32 記録部、33 通信部   DESCRIPTION OF SYMBOLS 1 Leakage current detection apparatus, A to-be-measured electric wire line, 10 Current transformer sensor (CT sensor) part, 11 Amplification part, 12, 16 Low-pass filter (LPF), 13, 17 Full wave rectification part, 14 Voltage detection part, 15 Transformer , 18 comparison unit, 19 calculation unit, 20 phase pulse width measurement unit, 21 power supply frequency measurement unit, 22 phase angle calculation unit, 23, 25 A / D conversion unit, 24, 26 effective value calculation unit, 27 leakage current calculation Unit, 28 resistance value calculation unit, 29 determination unit, 30 blocking unit, 31 setting unit, 32 recording unit, 33 communication unit

Claims (6)

電気方式が三相(R相、S相(接地相)、T相)三線式の被測定電線路に流れている漏洩電流を検出する漏洩電流検出手段と、
上記漏洩電流検出手段により検出された漏洩電流を電圧に変換する変換手段と、
上記変換手段により変換された電圧を増幅する増幅手段と、
上記増幅手段で増幅された電圧に含まれている高調波成分を除去する第1の高調波成分除去手段と、
上記被測定電線路の非接地相(R相−T相)間に発生している電圧を検出する電圧検出手段と、
上記電圧検出手段で検出された電圧に含まれている高調波成分を除去する第2の高調波成分除去手段と、
上記第1の高調波成分除去手段により高調波成分が除去された電圧の信号波形と、上記第2の高調波成分除去手段により高調波成分が除去された電圧の信号波形から位相差を検出する位相差検出手段と、
上記第2の高調波成分除去手段により高調波成分が除去された電圧の信号波形に基づき、上記電圧検出手段で電圧を検出した電圧線路に発生している周波数を算出する周波数算出手段と、
前記位相差検出手段で検出された位相差と、上記周波数算出手段で算出された周波数に基づき、上記被測定電線路に流れている漏洩電流の位相角度を算出する位相角度算出手段と、
上記第1の高調波成分除去手段により高調波成分が除去された電圧の実効値を算出する実効値算出手段と、
上記実効値算出手段で算出された実効値と、上記位相角度算出手段により算出された上記被測定電線路に流れている漏洩電流の位相角度に基づき、上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分を算出する対地絶縁抵抗漏洩電流成分算出手段と、
上記対地絶縁抵抗漏洩電流成分算出手段で算出された上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分が、所定の値を超えたかどうかを判断する判断手段と、
上記判断手段による判断に基づいて、上記被測定電線路を遮断する遮断手段とを備え、
上記実効値算出手段は、上記漏洩電流検出手段により検出された漏洩電流の平均値をIとし、その実効値I
=I×(π/2)/√2
により算出し、
上記対地絶縁抵抗漏洩電流成分算出手段は、上記実効値算出手段により算出された実効値Iと、上記位相角度算出手段により算出された上記被測定電線路に流れている漏洩電流の位相角度θから、上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分Igrを、
Igr=(I×sinθ)/cos30°
により算出することを特徴とする漏洩電流遮断装置。
Leakage current detection means for detecting a leakage current flowing in the three-phase (R-phase, S-phase (ground phase), T-phase) three-wire type electric wire to be measured;
Conversion means for converting the leakage current detected by the leakage current detection means into a voltage;
Amplifying means for amplifying the voltage converted by the converting means;
First harmonic component removal means for removing harmonic components contained in the voltage amplified by the amplification means;
Voltage detecting means for detecting a voltage generated between the non-grounded phases (R phase-T phase) of the measured electric wire;
Second harmonic component removing means for removing harmonic components contained in the voltage detected by the voltage detecting means;
A phase difference is detected from the signal waveform of the voltage from which the harmonic component has been removed by the first harmonic component removing means and the signal waveform of the voltage from which the harmonic component has been removed by the second harmonic component removing means. Phase difference detection means;
A frequency calculating means for calculating a frequency generated in the voltage line in which the voltage is detected by the voltage detecting means, based on the signal waveform of the voltage from which the harmonic component is removed by the second harmonic component removing means;
A phase angle calculating means for calculating a phase angle of a leakage current flowing through the measured electric line based on the phase difference detected by the phase difference detecting means and the frequency calculated by the frequency calculating means;
Effective value calculating means for calculating an effective value of the voltage from which the harmonic component has been removed by the first harmonic component removing means;
Based on the effective value calculated by the effective value calculating means and the phase angle of the leakage current flowing in the measured electric wire calculated by the phase angle calculating means, the leakage current flowing in the measured electric wire A ground insulation resistance leakage current component calculating means for calculating a leakage current component due to the ground insulation resistance included in
It is determined whether or not the leakage current component due to the ground insulation resistance included in the leakage current flowing through the measured electric wire calculated by the ground insulation resistance leakage current component calculation means exceeds a predetermined value. Judgment means,
Based on the determination by the determination means, and a blocking means for blocking the measured electric wire path,
The effective value calculation means sets the average value of the leakage current detected by the leakage current detection means to I, and the effective value I 0 is I 0 = I × (π / 2) / √2
Calculated by
The ground insulation resistance leakage current component calculation means includes an effective value I 0 calculated by the effective value calculation means, and a phase angle θ of the leakage current flowing through the measured electric wire calculated by the phase angle calculation means. From the leakage current component Igr caused by the ground insulation resistance included in the leakage current flowing through the measured electric line,
Igr = (I 0 × sin θ) / cos 30 °
A leakage current interrupting device characterized by the following calculation.
上記所定の値を設定する設定手段を備え、
上記判断手段は、上記対地絶縁抵抗漏洩電流成分算出手段で算出された上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分が、上記設定手段で設定された所定の値を超えたかどうかを判断することを特徴とする請求項1に記載の漏洩電流遮断装置。
Setting means for setting the predetermined value,
The determination means sets the leakage current component caused by the ground insulation resistance included in the leakage current flowing through the measured electric wire calculated by the ground insulation resistance leakage current component calculation means by the setting means. The leakage current interrupting device according to claim 1, wherein it is determined whether or not a predetermined value is exceeded.
上記対地絶縁抵抗漏洩電流成分算出手段により算出された上記漏洩電流成分を記録する記録手段を備えることを特徴とする請求項1に記載の漏洩電流遮断装置。   The leakage current interrupting device according to claim 1, further comprising recording means for recording the leakage current component calculated by the ground insulation resistance leakage current component calculation means. 上記漏洩電流検出手段は、接地線路を含む被測定電線路をクランプし、上記被測定電線路に流れている漏洩電流を検出することを特徴とする請求項1に記載の漏洩電流遮断装置。   2. The leakage current interrupting device according to claim 1, wherein the leakage current detecting means clamps a measured electric wire including a ground line and detects a leakage current flowing through the measured electric wire. 上記電圧検出手段は、上記被測定電線路に含まれている複数の電圧線路から検出した電圧を合成し、合成した電圧を上記第2の高調波成分除去手段に供給することを特徴とする請求項1に記載の漏洩電流遮断装置。   The voltage detection means synthesizes voltages detected from a plurality of voltage lines included in the electric line to be measured, and supplies the synthesized voltage to the second harmonic component removal means. Item 9. The leakage current interrupting device according to Item 1. 電気方式が三相(R相、S相(接地相)、T相)三線式の被測定電線路に流れている漏洩電流を検出する漏洩電流検出工程と、
上記漏洩電流検出工程により検出された漏洩電流を電圧に変換する変換工程と、
上記変換工程により変換された電圧を増幅する増幅工程と、
上記増幅工程で増幅された電圧に含まれている高調波成分を除去する第1の高調波成分除去工程と、
上記被測定電線路の非接地相(R相−T相)間に発生している電圧を検出する電圧検出工程と、
上記電圧検出工程で検出された電圧に含まれている高調波成分を除去する第2の高調波成分除去工程と、
上記第1の高調波成分除去工程により高調波成分が除去された電圧の信号波形と、上記第2の高調波成分除去工程により高調波成分が除去された電圧の信号波形から位相差を検出する位相差検出工程と、
上記第2の高調波成分除去工程により高調波成分が除去された電圧の信号波形に基づき、上記電圧検出工程で電圧を検出した電圧線路に発生している周波数を算出する周波数算出工程と、
前記位相差検出工程で検出された位相差と、上記周波数算出工程で算出された周波数に基づき、上記被測定電線路に流れている漏洩電流の位相角度を算出する位相角度算出工程と、
上記第1の高調波成分除去工程により高調波成分が除去された電圧の実効値を算出する実効値算出工程と、
上記実効値算出工程で算出された実効値と、上記位相角度算出工程により算出された上記被測定電線路に流れている漏洩電流の位相角度に基づき、上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分を算出する対地絶縁抵抗漏洩電流成分算出工程と、
上記対地絶縁抵抗漏洩電流成分算出工程で算出された上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分が、所定の値を超えたかどうかを判断する判断工程と、
上記判断工程による判断に基づいて、上記被測定電線路を遮断する遮断工程とを備え、
上記実効値算出工程は、上記漏洩電流検出工程により検出された漏洩電流の平均値をIとし、その実効値I
=I×(π/2)/√2
により算出し、
上記対地絶縁抵抗漏洩電流成分算出工程は、上記実効値算出工程により算出された実効値Iと、上記位相角度算出工程により算出された上記被測定電線路に流れている漏洩電流の位相角度θから、上記被測定電線路に流れている漏洩電流に含まれている対地絶縁抵抗に起因する漏洩電流成分Igrを、
Igr=(I×sinθ)/cos30°
により算出することを特徴とする漏洩電流遮断方法。
A leakage current detection step of detecting a leakage current flowing in a three-phase (R-phase, S-phase (grounding phase), T-phase) three-wire electric line to be measured;
A conversion step of converting the leakage current detected by the leakage current detection step into a voltage;
An amplification step of amplifying the voltage converted by the conversion step;
A first harmonic component removing step for removing harmonic components contained in the voltage amplified in the amplification step;
A voltage detection step of detecting a voltage generated between the non-grounded phases (R phase-T phase) of the measured electric line;
A second harmonic component removing step for removing harmonic components contained in the voltage detected in the voltage detecting step;
A phase difference is detected from the signal waveform of the voltage from which the harmonic component has been removed by the first harmonic component removal step and the signal waveform of the voltage from which the harmonic component has been removed by the second harmonic component removal step. A phase difference detection step;
Based on the signal waveform of the voltage from which the harmonic component has been removed by the second harmonic component removing step, a frequency calculating step for calculating the frequency generated in the voltage line that has detected the voltage in the voltage detecting step;
Based on the phase difference detected in the phase difference detection step and the frequency calculated in the frequency calculation step, a phase angle calculation step of calculating the phase angle of the leakage current flowing in the measured electric line,
An effective value calculating step of calculating an effective value of the voltage from which the harmonic component has been removed by the first harmonic component removing step;
Based on the effective value calculated in the effective value calculating step and the phase angle of the leakage current flowing in the measured electric wire calculated in the phase angle calculating step, the leakage current flowing in the measured electric wire A ground insulation resistance leakage current component calculation step for calculating a leakage current component due to the ground insulation resistance included in
It is determined whether or not the leakage current component due to the ground insulation resistance included in the leakage current flowing through the measured electric wire calculated in the ground insulation resistance leakage current component calculation step exceeds a predetermined value. A decision process;
Based on the determination by the determination step, including a blocking step of blocking the measured electrical line,
In the effective value calculating step, the average value of the leakage current detected in the leakage current detecting step is I, and the effective value I 0 is I 0 = I × (π / 2) / √2
Calculated by
The ground insulation resistance leakage current component calculation step includes the effective value I 0 calculated by the effective value calculation step and the phase angle θ of the leakage current flowing through the measured electric wire calculated by the phase angle calculation step. From the leakage current component Igr caused by the ground insulation resistance included in the leakage current flowing through the measured electric line,
Igr = (I 0 × sin θ) / cos 30 °
The leakage current interruption method characterized by calculating by this.
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