JP2593669B2 - Method for locating defective electrical insulation - Google Patents

Method for locating defective electrical insulation

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Publication number
JP2593669B2
JP2593669B2 JP25561887A JP25561887A JP2593669B2 JP 2593669 B2 JP2593669 B2 JP 2593669B2 JP 25561887 A JP25561887 A JP 25561887A JP 25561887 A JP25561887 A JP 25561887A JP 2593669 B2 JP2593669 B2 JP 2593669B2
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JP
Japan
Prior art keywords
output
frequency
circuit
current
electric circuit
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 - Fee Related
Application number
JP25561887A
Other languages
Japanese (ja)
Other versions
JPH0197880A (en
Inventor
辰治 松野
俊 木下
Original Assignee
東洋通信機株式会社
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
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Publication date
Application filed by 東洋通信機株式会社 filed Critical 東洋通信機株式会社
Priority to JP25561887A priority Critical patent/JP2593669B2/en
Publication of JPH0197880A publication Critical patent/JPH0197880A/en
Application granted granted Critical
Publication of JP2593669B2 publication Critical patent/JP2593669B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は電路又は電路に接続された電気機器の絶縁不
良箇所を探査する方法に関する。
Description: FIELD OF THE INVENTION The present invention relates to a method for searching for a defective insulation portion of an electric circuit or an electric device connected to the electric circuit.

(従来技術) 活線状態で電路の絶縁不良を検出する方法として同一
出願人が提案した方法(特開56−63270)がある。
(Prior Art) There is a method proposed by the same applicant (Japanese Patent Application Laid-Open No. 56-63270) as a method for detecting insulation failure of an electric circuit in a live state.

この方法を第2図を用いて説明する。 This method will be described with reference to FIG.

同図に於て1及び2は互いに等なる周波数及び
をもつ交流電源であって,該信号を受電トランスの接
地線5を介して電路4に印加し,該電路4に存在する絶
縁抵抗R1,R2,……RN並びに対地浮遊容量c1,c2,……cN
介して接地線に帰還する電流を前記接地線を貫通せしめ
た変流器3にて検出する。
In the figure, 1 and 2 are frequencies 1 and 2 which are equal to each other.
An AC power source with a 2, the signal through the ground wire 5 of the power receiving transformer is applied to the path 4, the insulation resistance R 1 present in the electric path 4, R 2, ...... R N and ground stray capacitance c 1, c 2, for detecting a current which returns to the ground line via a ...... c N by the current transformer 3 which was allowed through the ground line.

例えば交流電源1,2の出力電圧を夫々Vsinω1t,Vsinω
2tとすれば(ここでω=2π1=2πf2)変流
器3の出力を増幅器AMPで増幅し,周波数の成分を
検出するフィルタF1に印加すれば,その出力iは となる。
For example, output voltages of AC power supplies 1 and 2 are respectively Vsinω 1 t and Vsinω
Assuming that 2 t (here, ω 1 = 2π 1 , ω 2 = 2πf 2 ), the output of the current transformer 3 is amplified by the amplifier AMP and applied to the filter F 1 for detecting the component of the frequency 1. i is Becomes

一方,周波数の成分を検出するフィルタF2の出力
i2となる。各フィルタF1,F2の出力を2乗検波回路SQ1,SQ2
に印加すれば,2乗検波回路SQ1の出力 となり,一方のSQ2の出力 となる。
On the other hand, the output of the filter F2 that detects the frequency 2 component
i 2 Becomes The output of each filter F1, F2 is squared detection circuit SQ1, SQ2
To the output of the square detection circuit SQ1 Is And the output of one SQ2 Is Becomes

更に前記2乗検波回路SQ1の出力を引算器SUBの一方の
入力とし,又同様にSQ2の出力を係数回路cにて(ω1
倍若しくは(1/倍した後に前記引
算器SUBの他方の入力端に印加することによって引算器
の出力は となり,該引算器出力を平方根をとる回路ROOTに印加す
れば,該ROOT出力OUTは となるので電路の一括した絶縁抵抗値を測定することは
可能である。
Further, the output of the square detection circuit SQ1 is used as one input of a subtractor SUB, and the output of SQ2 is similarly input to a coefficient circuit c (ω 1
/ omega 2) twice or (1/2) output of the subtracter by applying to the other input terminal of the subtracter SUB after 2 times If the output of the subtracter is applied to a circuit ROOT that takes the square root, the output ROOT of the ROOT becomes Therefore, it is possible to collectively measure the insulation resistance value of the electric circuit.

しかしながら,この方法による絶縁抵抗測定は,たと
え異常値を示しても電路上のどの点で絶縁不良が発生し
ているか検出することができないと云う欠点があった。
However, the insulation resistance measurement by this method has a drawback that it is not possible to detect at which point on the electrical circuit insulation failure has occurred even if an abnormal value is indicated.

(発明の目的) 本発明は上記に鑑みてなされたものであって活線状態
の電路上の任意の区間の絶縁不良箇所を探査し,早期に
絶縁不良箇所の修復を可能にする電路の絶縁不良箇所探
査方法を提供することを目的とする。
(Object of the Invention) The present invention has been made in view of the above, and has been made in consideration of the above-described problems. An object of the present invention is to provide a method for detecting a defective portion.

(発明の概要) 本発明は上記目的を達成する為に電路に互に異なる周
波数1,を発生する交流電源を印加し,上記電路の
探査すべき2点に第1,第2の変流器を結合させ,第1,第
2交流器出力電流の差に含まれる周波数の電流成分
並びに周波数の電流成分を検出すると共に該周波数
の成分の振幅の2乗値と,前記周波数の成分の
振幅の2乗値を(1/倍した値との差を求め,
該差域は該差の平方根を求めることによって,上記電路
上の2点間の絶縁抵抗を検出し,これにより電路の絶縁
不良箇所を探知する方法である。
(Summary of the Invention) In order to achieve the above object, the present invention applies an AC power supply that generates mutually different frequencies 1 and 2 to an electric circuit, and first and second current transformers are applied to two points of the electric circuit to be searched. To detect the current component of frequency 1 and the current component of frequency 2 included in the difference between the output currents of the first and second alternators.
And square value of the amplitude of the first component, the frequency 2 of the square value of the amplitude of the component (1/2) obtains the difference between twice the value,
The difference area is a method of detecting an insulation resistance between two points on the electric circuit by detecting a square root of the difference, thereby detecting a defective insulation of the electric circuit.

(実施例) 以下,本発明を図面に示した実施例に基づいて詳細に
説明する。
(Examples) Hereinafter, the present invention will be described in detail based on examples shown in the drawings.

第1図は本発明の実施にあたって用いる装置の一実施
例を示すブロック図である。
FIG. 1 is a block diagram showing an embodiment of an apparatus used in carrying out the present invention.

同図に於て前記第2図と同一の記号は同一の意味をも
つ。
2, the same symbols as those in FIG. 2 have the same meanings.

同図に於て電路上のA点に結合した分割型変流器の出
力は増幅器AMP2に入力し,該AMP2の出力は位相調整器PH
1,PH2及び振幅調整器AD1,AD2を介して引算回路SUB1,SUB
2に夫々入力され該SUB1,SUB2の他の入力には前記AMP1の
出力が入力する。
In this figure, the output of the split type current transformer coupled to point A on the circuit is input to an amplifier AMP2, and the output of AMP2 is a phase adjuster PH.
Subtraction circuit SUB1, SUB via 1, PH2 and amplitude adjuster AD1, AD2
2, and the output of the AMP1 is input to the other inputs of the SUB1 and SUB2.

前記SUB1の出力は周波数の成分を検出するフィル
タF1を介して2乗検波回路SQ1に入力し,一方前記SUB2
の出力は周波数の成分を検出するフィルタF2を介し
て2乗検波回路SQ2に入力する。更に前記SQ2出力を(ω
1倍の係数回路を介して引算回路SUB3の一入力
端に入力するとともに他の入力端には前記SQ1出力を入
力する。それにより得た値を平方根回路ROOTに入力する
ことにより,その出力としてOUT1を得る。
The output of the SUB1 is input to a square detection circuit SQ1 via a filter F1 for detecting a frequency 1 component.
Is input to a square detection circuit SQ2 via a filter F2 for detecting a frequency 2 component. Further, the SQ2 output is changed to (ω
1 / omega 2) to the other input terminal receives an input to one input terminal of the subtraction circuit SUB3 through twice the coefficient circuit for inputting said SQ1 output. By inputting the obtained value to the square root circuit ROOT, OUT1 is obtained as its output.

このように構成された回路に於て交流電流1及び2の
出力電圧をVsinω1t,Vsinω2t(ω=2π1
2πf2)とすれば,前記増幅器AMP2の出力には前記
(1)式に相当する周波数の電流iが含まれ,一方
前記増幅器AMP1の出力には周波数の電流▲i
▼,即ち が含まれる。従って前記増幅器AMP1とAMP2の出力を前記
引算器SUB1のそれぞれの入力端に印加し,その出力を前
記フィルタF1に印加すれば,フィルタF1の出力は前記
(1),(7)式より となる。これは変流器6,7の位相振幅特性が周波数
にて等しい時に得られるものであって,前記特性が周波
にて相異するときは増幅器AMP2の出力端に接続し
た位相調整器PH1及び該PH1の次段に接続した振幅調整器
AD1にて補正すればよい。
Thus the circuit configured Vsinomega 1 the output voltage of the alternating current 1 and 2 At a t, Vsinω 2 t (ω 1 = 2π 1, ω 2 =
2πf 2 ), the output of the amplifier AMP2 contains the current i of frequency 1 corresponding to the above equation (1), while the output of the amplifier AMP1 contains the current i of frequency 1
1 ▼, ie Is included. Therefore, if the outputs of the amplifiers AMP1 and AMP2 are applied to the respective input terminals of the subtractor SUB1 and the outputs are applied to the filter F1, the output of the filter F1 is calculated according to the equations (1) and (7). Becomes This is because the phase amplitude characteristics of current transformers 6 and 7 are frequency 1
When the characteristics are different at the frequency 1, the phase adjuster PH1 connected to the output terminal of the amplifier AMP2 and the amplitude adjuster connected to the next stage of the PH1 are obtained.
What is necessary is just to correct by AD1.

該補正とは変流器6,7を電路上の同一箇所に結合せし
め,この時のフィルタF1出力が零になるようにすればよ
い。
The correction may be performed by coupling the current transformers 6 and 7 to the same location on the electric circuit so that the output of the filter F1 at this time becomes zero.

更に周波数に関する出力として前記増幅器AMP2の
出力には前記(2)式で示された周波数の電流i2
含まれる一方前記増幅器AMP1の出力には周波数f2の電流
▲i ▼,即ち が含まれる。従って前記AMP1及びAMP2の出力を引算器SU
B2に夫々入力し,得た出力をフィルタF2に印加すれば,
該フィルタF2の出力は前記(2),(9)式より が得られる。上記フィルタF2出力は前記フィルタF1の場
合と同様に変流器6,7の位相振幅特性が周波数f2にて等
しくなければ得られないので,該位相振幅特性は位相調
整器PH2並びに振幅調整器AD2にて補正する。
Furthermore it said output of said amplifier AMP2 as an output related to the frequency 2 (2) of the frequency f 2 to the output of one the amplifiers AMP1 to include current i 2 of the frequency 2 shown in formula currents ▲ i '2 ▼, That is Is included. Therefore, the outputs of the AMP1 and AMP2 are subtracted by the SU
By inputting each to B2 and applying the obtained output to the filter F2,
The output of the filter F2 is obtained from the above equations (2) and (9). Is obtained. Since the filter F2 output phase amplitude characteristic of the case of the filter F1 as well as the current transformer 6 and 7 can not be obtained to be equal at a frequency f 2, the phase amplitude characteristic is phase adjuster PH2 and amplitude adjuster Correct with AD2.

フィルタF1の出力を2乗検波回路SQ1に印加すると,
その出力 となり,一方フィルタF2の出力を2乗検波回路SQ2に印
加すると,その出力 となる。前記2乗検波回路SQ2出力を係数回路に入力
し,(ω1倍することによって を得,該値を引算器SUB3の一入力端へ入力し,他の入力
端には前記2乗検波回路SQ2に入力する。
When the output of the filter F1 is applied to the square detection circuit SQ1,
Its output Is When the output of the filter F2 is applied to the square detection circuit SQ2, the output Is Becomes Enter the square-law detection circuit SQ2 output to the coefficient circuit, by multiplying (ω 1 / ω 2) 2 And input the value to one input terminal of the subtractor SUB3, and to the other input terminal to the square detection circuit SQ2.

斯くして引算器SUB3の出力には となる。即ち、前記(13)式から明らかな如く引算器SU
B3の出力は電路AB区間の絶縁抵抗R1の2乗に逆比例して
おり,これにより上記電路の所定区間に於ける絶縁抵抗
を知ることができる。
Thus, the output of the subtractor SUB3 is Becomes That is, as is apparent from the equation (13), the subtractor SU
B3 output is inversely proportional to the square of the insulation resistance R 1 of the path AB interval, thereby it is possible to know in insulation resistance in a predetermined section of the path.

更に前記引算器SUB3の出力を平方根回路ROOTに印加す
れば,その出力は(13)式より となるので絶縁抵抗R1を知ることができる。
Further, if the output of the subtracter SUB3 is applied to the square root circuit ROOT, the output is obtained from the equation (13). Since the can know the insulation resistance R 1.

尚,上記実施例では,電路上の区間ABの場合について
示したが,変流器6をB点に又,変流器7をc点に移設
すればBC区間の絶縁抵抗を測定することができることは
明らかである。更に変流器6,7の振幅位相特性が周波数
1,にて等しければ各変流器出力を逆相となるよう
に直列に接続し,これを増幅した後フィルタF1,F2に直
接入力してもよいことは明らかである。
In the above embodiment, the case of the section AB on the electric circuit is shown. However, if the current transformer 6 is moved to the point B and the current transformer 7 is moved to the point c, the insulation resistance in the section BC can be measured. Clearly what you can do. Furthermore, the amplitude and phase characteristics of current transformers 6 and 7
It is clear that if the currents are equal in 1 and 2 , the outputs of the current transformers may be connected in series so as to have opposite phases, amplified and then directly input to the filters F1 and F2.

(発明の効果) 本発明は上述の如き方法によって電路上の任意の区間
の絶縁抵抗をその区間前後の影響を受けずに測定できる
ため絶縁不良箇所の探知に著効を奏するものである。
(Effects of the Invention) The present invention makes it possible to measure the insulation resistance of an arbitrary section on an electric circuit without being affected before and after the section by the above-described method, so that the present invention is very effective in detecting a defective insulation.

【図面の簡単な説明】[Brief description of the drawings]

第1図は本発明の実施にあたって用いる装置の一実施例
を示すブロック図,第2図は従来の方法を示すブロック
図である。 1,2……交流電源,3,6,7……変流器,4……電路,5……接
地線,AMP,AMP1,AMP2……増幅器,PH1,PH2……位相調整
器,AD1,AD2……振幅調整器,SQ1,SQ2……2乗検波回路,c
……係数回路,SUB,SUB1,SUB2,SUB3……引算器,ROOT…
…平方根回路。
FIG. 1 is a block diagram showing an embodiment of an apparatus used in carrying out the present invention, and FIG. 2 is a block diagram showing a conventional method. 1,2 ... AC power supply, 3,6,7 ... Current transformer, 4 ... Electric circuit, 5 ... Ground line, AMP, AMP1, AMP2 ... Amplifier, PH1, PH2 ... Phase adjuster, AD1, AD2: Amplitude adjuster, SQ1, SQ2: Square detector circuit, c
…… Coefficient circuit, SUB, SUB1, SUB2, SUB3 …… Subtractor, ROOT…
... square root circuit.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】互いに相異なる周波数f1、f2(f2>f1)の
交流信号を電路に印加し、上記電路上の任意の2点にて
第1、第2の変流器を結合せしめ、該第1、第2の変流
器出力電流の差に含まれる周波数f1並びに周波数f2の電
流成分を検出し、該周波数f1の電流成分の振幅の2乗値
と、前記周波数f2の電流成分の振幅の2乗値を(f1/f
2)倍した値との差を求めることにより上記電路上の
2点間の絶縁抵抗を測定したことを特徴とする電気絶縁
不良箇所探査方法。
An AC signal having frequencies f1 and f2 (f2> f1) different from each other is applied to an electric circuit, and first and second current transformers are coupled at arbitrary two points on the electric circuit. A current component of the frequency f1 and a frequency f2 included in the difference between the first and second current transformer output currents are detected, and the square value of the amplitude of the current component of the frequency f1 and the amplitude of the current component of the frequency f2 are detected. To the squared value of (f1 / f
2) 2 times the value as an electrical insulation failure portion exploration method characterized by measured the insulation resistance between two points of the conductive path by obtaining a difference.
JP25561887A 1987-10-09 1987-10-09 Method for locating defective electrical insulation Expired - Fee Related JP2593669B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25561887A JP2593669B2 (en) 1987-10-09 1987-10-09 Method for locating defective electrical insulation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25561887A JP2593669B2 (en) 1987-10-09 1987-10-09 Method for locating defective electrical insulation

Publications (2)

Publication Number Publication Date
JPH0197880A JPH0197880A (en) 1989-04-17
JP2593669B2 true JP2593669B2 (en) 1997-03-26

Family

ID=17281248

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25561887A Expired - Fee Related JP2593669B2 (en) 1987-10-09 1987-10-09 Method for locating defective electrical insulation

Country Status (1)

Country Link
JP (1) JP2593669B2 (en)

Also Published As

Publication number Publication date
JPH0197880A (en) 1989-04-17

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