JP2593668B2 - Insulation fault detection method for electric circuit - Google Patents

Insulation fault detection method for electric circuit

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Publication number
JP2593668B2
JP2593668B2 JP25561787A JP25561787A JP2593668B2 JP 2593668 B2 JP2593668 B2 JP 2593668B2 JP 25561787 A JP25561787 A JP 25561787A JP 25561787 A JP25561787 A JP 25561787A JP 2593668 B2 JP2593668 B2 JP 2593668B2
Authority
JP
Japan
Prior art keywords
output
electric circuit
circuit
square
filter
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
JP25561787A
Other languages
Japanese (ja)
Other versions
JPH0197879A (en
Inventor
辰治 松野
俊 木下
Original Assignee
東洋通信機株式会社
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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 JP25561787A priority Critical patent/JP2593668B2/en
Publication of JPH0197879A publication Critical patent/JPH0197879A/en
Application granted granted Critical
Publication of JP2593668B2 publication Critical patent/JP2593668B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Measurement Of Resistance Or Impedance (AREA)
  • Locating Faults (AREA)

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=2π)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 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 frequency 1 , the output i becomes 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。
While the output i 2 of the filter F2 for detecting the component of the frequency 2
Is 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
るの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 electric circuit an insulation failure has occurred even if it shows an abnormal value.

(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,電路に互いに相異
なる周波数1,)を発生する交流電源
を印加するとともに,上記電路上の任意の2点にて第1
及び第2の変流器を結合させ、上記第1,第2の変流器の
出力に夫々得られる周波数の漏洩電流成分の振幅の
2乗値 と周波数の漏洩電流成分の振幅の2乗値 とを検出し, の演算を行なうことにより上記電路上の2点間の絶縁抵
抗を測定する方法である。
(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 ( 2 > 1 ) to an electric circuit, and also applies an AC power source to any two points on the electric circuit. First
And the second current transformer, and the square value of the amplitude of the leakage current component of frequency 1 obtained at the output of each of the first and second current transformers And the square of the amplitude of the leakage current component at frequency 2 And detect Is a method of measuring the insulation resistance between two points on the electric circuit by performing the above calculation.

(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当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 one embodiment of an apparatus used in carrying out the present invention.

同図に於て前記第2図と同一の意味を表し,前記第2
図と異なる点は変流器を含む漏洩電流成分検出系を二系
統備え,該二系統の出力を引算器SUB3に入力することに
より,その出力を検出した点である。
In the same figure, the same meaning as in FIG.
The difference from the figure is that two systems of a leakage current component detection system including a current transformer are provided, and the outputs of the two systems are input to a subtractor SUB3 to detect the output.

同図に於て,電路上Aで電路4を分割型変流器6に貫
通せしめ,該出力は増幅器AMP2に入力され,該AMP2出力
は周波数成分を検出するフィルタF3並びに周波数
成分を検出するフィルタF4に印加される。斯くしてフ
ィルタF3の出力には前記(1)式で示される電流が得ら
れ,これを2乗検波回路SQ3に印加すると,その出力は
前記(3)式で示される に相当する。一方フィルタF4の出力i2は前記(2)式で
示される電流となり,これを2乗検波回路SQ4に印加す
ると,その出力は前記(4)式で示される に相当する値を得る。
In this figure, an electric circuit 4 is passed through a split-type current transformer 6 on an electric circuit A, the output of which is input to an amplifier AMP2, and the output of AMP2 is a filter F3 for detecting one frequency component and a frequency.
It is applied to a filter F4 that detects two components. Thus, a current represented by the above equation (1) is obtained at the output of the filter F3. When this current is applied to the square detection circuit SQ3, the output is represented by the above equation (3). Is equivalent to While the output i 2 of the filter F4 becomes the current represented by the equation (2), applying this to the square-law detection circuit SQ4, the output is represented by the equation (4) Is obtained.

前記2乗検波回路SQ4の出力を係数回路cにて
(ω1=(1/倍し,その出力を引算
器SUB2の一入力端に,他の入力端には前記2乗検波回路
SQ3の出力を入力することによって該引算回路SUB2の出
力には(5)式に相当する出力が得られ,更に該出力を
平方根回路ROOT2に入力すれば該ROOT2出力は前記(6)
式に相当するA点から電路の末端までの総合絶縁抵抗が
測定される。
The square-law detection circuit outputs at the coefficient circuit c 2 of SQ4 (ω 1 / ω 2) 2 = (1/2) 2 multiplied by its output to one input terminal of the subtractor SUB2, the other input terminal Is the square detection circuit
By inputting the output of SQ3, an output corresponding to the equation (5) is obtained as the output of the subtraction circuit SUB2. If the output is further input to the square root circuit ROOT2, the output of the ROOT2 becomes the above (6).
The total insulation resistance from the point A corresponding to the equation to the end of the circuit is measured.

一方,電路上のB点で電路が貫通する変流器7の出力
を増幅器AMP1に入力し,該AMP1の出力を周波数成分
を検出するフィルタF1並びに周波数成分を検出する
フィルタF2に入力する。
On the other hand, the output of the current transformer 7 through which the electric circuit penetrates at point B on the electric circuit is input to the amplifier AMP1, and the output of the AMP1 is input to the filter F1 for detecting the frequency 1 component and the filter F2 for detecting the frequency 2 component. .

前記フィルタF1の出力▲i ▼は となり,一方フィルタF2の出力▲i ▼は となる。前記フィルタF1及びF2の出力を2乗検波回路SQ
1,SQ2に夫々入力すれば該SQ1の出力として 及び該SQ2の出力として を得る。
The output ▲ i 1 ▼ of the filter F1 is On the other hand, the output ▲ i 2 ▼ of the filter F2 is Becomes The output of the filters F1 and F2 is squared detection circuit SQ
1, if input to SQ2, output as SQ1 And the output of the SQ2 Get.

更に前記2乗検波回路SQ2の出力▲i′2 ▼を係数
回路cで(ω1若しくは(1/
し,その出力を引算回路SUB1の一入力端に入力すると共
に他の入力端には前記2乗検波回路SQ1出力を入力する
ことにより引算器SUB1の出力は となり,該SUB1出力を平方根回路ROOT1に印加すればそ
の出力として となる。これはB点から電路の末端までの総合絶縁抵抗
であって,該値と前記平方根回路ROOT2出力とを夫々引
算器SUB3に入力すれば,該SUB3出力OUT1は(6),(1
2)式から となり電路上の区間ABの絶縁抵抗を測定しうることにな
る。
Further first input terminal of the square-law detection output of the circuit SQ2 ▲ i '2 2 ▼ at the coefficient circuits c 1 (omega 1 / omega 2) 2 or (1/2) is doubled, subtraction circuit SUB1 its output And the other input terminal receives the output of the square detection circuit SQ1 so that the output of the subtractor SUB1 is And applying the SUB1 output to the square root circuit ROOT1 produces the output Becomes This is the total insulation resistance from point B to the end of the circuit. If this value and the output of the square root circuit ROOT2 are input to the subtractor SUB3, the output SUB3 OUT1 becomes (6), (1)
2) From equation Thus, the insulation resistance of the section AB on the electric circuit can be measured.

尚,上記実施例では電路上の区間ABについて説明を行
ない示したが,これに限るわけでなく変流器6をB点に
又変流器7をC点に移設し測定すれば区間BCの絶縁抵抗
を測定することが可能なことは明らかである。
In the above embodiment, the section AB on the electric circuit has been described and shown. However, the present invention is not limited to this. If the current transformer 6 is moved to the point B and the current transformer 7 is moved to the point C and measured, the section BC of the section BC is measured. It is clear that the insulation resistance can be measured.

(発明の効果) 本発明は上述の如き方法によって作用するものである
から電路の上の任意の区間の絶縁抵抗(電路に接続され
ている電子機器のそれをも含む)をその区間の前後の影
響を受けずに測定できるため,絶縁不良箇所の探査に著
効を奏するものである。
(Effect of the Invention) Since the present invention operates by the method as described above, the insulation resistance (including that of the electronic device connected to the electric circuit) in an arbitrary section on the electric circuit is determined before and after the section. Since the measurement can be performed without being affected, it is extremely effective in searching for 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当って用いる装置の一実施例を
示す図,第2図は従来の測定方法を示す図である。 1,2……交流電源,3,6,7……変流器,AMP,AMP1,AMP2……
増幅器,F1,F2,F3,F4……フィルタ,SQ1,SQ2,SQ3,SQ4……
2乗検波回路,SUB,SUB1,SUB2,SUB3……引算器,c1,c
……係数回路,ROOT1,ROOT2……平方根回路。
FIG. 1 is a view showing an embodiment of an apparatus used in carrying out the present invention, and FIG. 2 is a view showing a conventional measuring method. 1,2 …… AC power supply, 3,6,7 …… Current transformer, AMP, AMP1, AMP2 ……
Amplifier, F 1, F 2, F 3, F 4 ...... filter, SQ1, SQ2, SQ3, SQ4 ......
Square-law detection circuit, SUB, SUB1, SUB2, SUB3 ...... subtractor, c 1, c
2 ...... Coefficient circuit, ROOT1, ROOT2 ... 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
器の出力に夫々得られる周波数f1の漏洩電流成分の振幅
の2乗値 と、周波数f2の漏洩電流成分の振幅の2乗値 とを検出し、 の演算を行う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路の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. The square value of the amplitude of the leakage current component of the frequency f1 obtained at each of the outputs of the first and second current transformers And the square of the amplitude of the leakage current component at frequency f2 And detect A method for detecting an insulation failure portion of an electric circuit, wherein an insulation resistance between two points on the electric circuit is measured by performing the above calculation.
JP25561787A 1987-10-09 1987-10-09 Insulation fault detection method for electric circuit Expired - Fee Related JP2593668B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25561787A JP2593668B2 (en) 1987-10-09 1987-10-09 Insulation fault detection method for electric circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25561787A JP2593668B2 (en) 1987-10-09 1987-10-09 Insulation fault detection method for electric circuit

Publications (2)

Publication Number Publication Date
JPH0197879A JPH0197879A (en) 1989-04-17
JP2593668B2 true JP2593668B2 (en) 1997-03-26

Family

ID=17281233

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25561787A Expired - Fee Related JP2593668B2 (en) 1987-10-09 1987-10-09 Insulation fault detection method for electric circuit

Country Status (1)

Country Link
JP (1) JP2593668B2 (en)

Also Published As

Publication number Publication date
JPH0197879A (en) 1989-04-17

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