JP2750713B2 - Simple insulation resistance measurement method for low voltage wiring etc. - Google Patents

Simple insulation resistance measurement method for low voltage wiring etc.

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Publication number
JP2750713B2
JP2750713B2 JP31030988A JP31030988A JP2750713B2 JP 2750713 B2 JP2750713 B2 JP 2750713B2 JP 31030988 A JP31030988 A JP 31030988A JP 31030988 A JP31030988 A JP 31030988A JP 2750713 B2 JP2750713 B2 JP 2750713B2
Authority
JP
Japan
Prior art keywords
wiring
insulation resistance
current transformer
variable resistor
transformer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP31030988A
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Japanese (ja)
Other versions
JPH02193077A (en
Inventor
辰治 松野
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toyo Tsushinki KK
Original Assignee
Toyo Tsushinki KK
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Priority to JP31030988A priority Critical patent/JP2750713B2/en
Publication of JPH02193077A publication Critical patent/JPH02193077A/en
Application granted granted Critical
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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は電気配線の絶縁抵抗測定方法に関し,殊に一
般家庭等に於ける一般電気工作物の絶縁抵抗を局部的に
測定検知することのできる低圧配線等の絶縁抵抗測定方
法に関する。
Description: FIELD OF THE INVENTION The present invention relates to a method for measuring insulation resistance of electric wiring, and more particularly to a method of measuring and detecting the insulation resistance of a general electric work in a general household or the like locally. The present invention relates to a method for measuring insulation resistance of low-voltage wiring and the like that can be performed.

(従来の技術) 電力送電設備では通前絶縁監視が行なわれ,より安定
した電力供給がはかられている。
(Prior art) In power transmission equipment, insulation monitoring is performed before transmission, and more stable power supply is achieved.

しかし,一般家庭に於ける絶縁監視態勢は遅れており
極めて大ざっぱな計測を行なうための装置が設置されて
いるに止まっていた。
However, the monitoring system for insulation in ordinary households has been delayed, and only equipment for performing very rough measurements has been installed.

即ち,従来の一般家庭の負荷設備を含む屋内外配線の
絶縁抵抗測定方法としては,各家庭毎に分電盤にて給電
を停止し,被測定部分に高圧直流電圧を印加してそのリ
ーク電流を検知する所謂メカーを用いる方法が一般的で
あった。
That is, as a conventional method of measuring the insulation resistance of indoor and outdoor wiring including load equipment for general households, power supply is stopped at a distribution board in each household, a high-voltage DC voltage is applied to a portion to be measured, and the leakage current is measured. In general, a method using a so-called mecca for detecting the presence of a messenger is used.

又,給電を停止せずに測定する手段としては,配電線
に零相変流器をクランプし商用周波数成分の零相電流成
分を計測する方法が用いられていた。
As a means for measuring without stopping power supply, a method of measuring a zero-phase current component of a commercial frequency component by clamping a zero-phase current transformer on a distribution line has been used.

しかし一方,近年家庭内の電気設備はCPU等を搭載し
た精巧な各種エレクトロニクス回路を用いたものが多
く,絶縁抵抗測定のために給電を中断することあるいは
高圧を印加することは事故等の発生を生じる虞れもある
為,極力避けるべき状況となっている。
On the other hand, in recent years, many household electrical facilities use sophisticated electronic circuits equipped with a CPU and the like. Interrupting power supply or applying high voltage to measure insulation resistance may cause an accident, etc. It is a situation that should be avoided as much as possible because it may occur.

更には,各種電子機器に付設したノイズ除去用各種フ
ィルタの増加に伴ない,電路あるいは負荷機器と大地間
の対地静電容量が増加し単に商用周波の零相電流を測定
するのみでは正確に絶縁状況の良否を判定することが困
難となってきた。又絶縁抵抗測定のために測定者が屋内
に立入らず,屋外で一般家庭等の屋内配線の絶縁抵抗を
測定する方法の実用化がのぞまれていた。
Furthermore, with the increase of various filters for noise removal attached to various electronic devices, the capacitance to ground between the electric circuit or the load device and the ground increases, and accurate insulation can be obtained simply by measuring the zero-phase current of the commercial frequency. It has become difficult to determine whether the situation is good or bad. In addition, it has been desired that a method for measuring the insulation resistance of indoor wiring such as a general home outdoors be put to practical use, since a measurer does not enter indoors for measuring insulation resistance.

しかしながら,家庭等の一般電気工作物へ給電する低
圧電路例えば100Vあるいは200V等は柱上トランス又は地
下に埋設されたトランスで,一般に6.6KVから降圧され
たのち複数の家庭や電気設備へと配線されているが,こ
の受電トランスの低圧測出力電路の一端が,該受電変圧
トランスの設置場所付近で接地されるのが一般的であ
る。しかし,この接地抵抗は必ずしも十分低くないため
特定の家庭内の配線及びこれらに接続された電気機器に
関する絶縁抵抗を分離して測定するのが極めて困難であ
った。
However, low-voltage paths, such as 100 V or 200 V, that supply power to general electric works such as homes are pole transformers or transformers buried underground, which are generally stepped down from 6.6 KV and then wired to multiple homes and electrical equipment. However, one end of the low-voltage measurement output circuit of the power receiving transformer is generally grounded near the installation location of the power receiving transformer. However, since this ground resistance is not always sufficiently low, it has been extremely difficult to separate and measure the insulation resistance of the wiring in a specific home and the electric equipment connected thereto.

したがって,特定の家庭の電気絶縁抵抗測定に当って
は,他の家庭や他の電気設備の絶縁抵抗,対地静電容量
又上記トランスの低圧側電路接地抵抗の影響をうけない
方法でなければならない。
Therefore, when measuring the electrical insulation resistance of a particular household, the method must be one that is not affected by the insulation resistance of other households or other electrical equipment, the capacitance to ground, or the grounding resistance of the transformer on the low-voltage side. .

(発明の目的) 本発明は上記従来の問題点を解決すると同時に諸事情
に鑑みてなされたもので,一般家庭など一般用電気工作
物の電気絶縁抵抗の測定に当って屋内に立入ることな
く,無停電でしかも正確にかつ簡単に絶縁抵抗を測定す
る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 consideration of various circumstances at the same time as solving the above-mentioned conventional problems, and it is not necessary to enter indoors when measuring the electrical insulation resistance of a general electric work such as a general household. It is an object of the present invention to provide a method for accurately and easily measuring insulation resistance without interruption.

(発明の概要) この目的を達成するために、本発明にかかる簡易絶縁
抵抗測定方法は、一端が接地された配線の所要部に注入
トランス及び変流器を結合し、該注入トランスを介して
周波数f1なる測定用信号を配線に印加すると共に前記所
要部と大地との間に存在する電圧を検出し、該検出電圧
を可変抵抗器もしくは可変抵抗器と可変コンデンサとを
並列に接続した回路にて終端した導線に印加すると共
に、前記導線は前記配線に印加された測定用信号により
前記変流器に誘起される磁束と反対向きの磁束が前記変
流器に生じるように該変流器を貫通せしめ、更に、前記
変流器出力中に含まれる周波数f1成分が最小となるよう
に前記可変抵抗器の抵抗値もしくは前記可変抵抗値及び
可変コンデンサの抵抗値及び容量値を調整し、該抵抗値
或いは抵抗値及び容量値によって前記注入トランス及び
変流器を結合せしめた配線の所要部より端方部、即ち受
電トランスから見て前記所要部より遠方の配線及び配線
に接続した負荷機器等の絶縁抵抗を測定するよう手段を
講ずる。
(Summary of the Invention) In order to achieve this object, a simple insulation resistance measuring method according to the present invention comprises connecting an injection transformer and a current transformer to a required portion of a wire whose one end is grounded, and via the injection transformer. circuit for detecting a voltage present, and connects the detection voltage and a variable capacitor variable resistor or a variable resistor in parallel between the predetermined portions and ground to apply a measuring signal comprising a frequency f 1 to the wiring The current transformer is applied so that a magnetic flux in a direction opposite to a magnetic flux induced in the current transformer by the measurement signal applied to the wiring is generated in the current transformer. was allowed to penetrate further, by adjusting the resistance value and the capacitance value of the variable resistor a resistance value or the variable resistance and a variable capacitor so that the frequency f 1 component contained in the current transformer output is minimized, The resistance value or Insulation resistance of the wiring connecting the injection transformer and the current transformer at the end from the required part, that is, the wiring far from the required part as viewed from the power receiving transformer and the load device connected to the wiring by the resistance value and the capacitance value. Take steps to measure.

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

第1図は本発明の方法を実施するために用いる装置の
一実施例を示す構成図である。
FIG. 1 is a block diagram showing an embodiment of an apparatus used to carry out the method of the present invention.

即ち,第1図に於いてT,L1,L2及びLEは柱上あるいは
地下に埋設された受電トランスとその低圧電路及び該電
路の一方と大地(E2)との間に接続された接地線であ
る。
Ie, T In FIG. 1, L 1, L 2 and L E is connected between one and the earth of the low-pressure path and the power line and the power receiving transformer embedded in the pole or underground (E 2) Ground wire.

前記電路L1、L2は一般に複数に分岐し、多数の各家庭
に配布され、各電路の端方部、即ち受電トランスTから
見て夫々の分岐電路の分岐点より遠方には一般電気工作
物H1、H2、H0等が接続されており,これら一般電気工作
物(負荷設置への配線も含む)と大地との間には絶縁抵
抗R1,R3,R0が存在し,低圧電路と大地間には絶縁抵抗
R2,R4が存在する。又同時に該負荷設備(負荷設備の配
線も含む)及び前記低圧電路には夫々対地静電容量C1
C3,C0及びC2,C4等が存在する。
The electric lines L 1 and L 2 are generally branched into a plurality of parts and distributed to a large number of homes. General electric work is located at the end of each electric line, that is, farther than the branch point of each branch electric line when viewed from the power receiving transformer T. Objects H 1 , H 2 , H 0, etc. are connected, and insulation resistances R 1 , R 3 , R 0 exist between these general electric works (including wiring for load installation) and the ground. , Insulation resistance between low-voltage path and ground
R 2 and R 4 exist. At the same time, the load equipment (including the wiring of the load equipment) and the low-voltage path have a ground capacitance C 1 ,
There are C 3 , C 0 and C 2 , C 4, etc.

このような状態の配電線路のうち負荷機器H0に関する
絶縁抵抗を本発明の方法によって測定する場合を例示す
る。
It illustrates the case of measuring by the method of the present invention the insulation resistance on Load device H 0 of this state of the distribution line.

このために,この実施例においては同図に示す如く当
該負荷機器H0が設置された家庭の内部又は外部の電線
(電路)に注入トランスOTを結合すると共に該注入トラ
ンスOTに発振器OSCを接続し周波数1なる測定用信号を
前記電路L1,L2に注入する。
For this, connect the oscillator OSC to the infusion transformer OT with couples injection transformer OT inside or outside of the wire of the home where the load device H 0 as shown in the figure is installed (path) in this example Then, a measurement signal having a frequency of 1 is injected into the electric circuits L 1 and L 2 .

尚,この測定用信号周波数1は商用周波数並びにそ
の高調波成分の周波数とは異なるものとすることは云う
までもない。
It goes without saying that the measurement signal frequency 1 is different from the commercial frequency and the frequency of its harmonic component.

更に,前記配線電路には零相変流器ZCTをクランプ等
により貫通せしめ,その出力を周波数1成分を抽出す
るフィルタFILに入力し,該フィルタFIL出力を整流器DT
で整流した後メータMにて表示する。又,注入トランス
OTの結合点近くの電路と大地間の電圧を高入力インピー
ダンス増幅器A1にて検出し,該増幅器A1の出力を前記変
換器ZCTに貫通せしめた導線Lpに印加し,該導線Lpは可
変抵抗器RVにて終端する。
Further, a zero-phase current transformer ZCT is passed through the wiring circuit by a clamp or the like, and its output is input to a filter FIL for extracting one frequency component, and the output of the filter FIL is connected to a rectifier DT.
After the rectification, the value is displayed on the meter M. In addition, injection transformer
The voltage between the nearby tracks and the earth point of attachment OT detected by the high input impedance amplifier A 1, and applies the output of the amplifier A 1 at line L p which was allowed through the transducer ZCT, conductor lines L p Is terminated by a variable resistor RV.

尚、前記導線は測定用信号によって変流器に誘起され
る磁束と反対方向の磁束が生ずるように該変流器に貫通
せしめる。
The conducting wire is passed through the current transformer so that a magnetic flux in the opposite direction to the magnetic flux induced in the current transformer by the measurement signal is generated.

このように構成した回路に於いてメータMの値が最小
となるよう導線に接続した可変抵抗器RVの値を変化さ
せ,前記最小となった可変抵抗器RVの抵抗値から絶縁抵
抗R0を測定する。
In the circuit thus configured, the value of the variable resistor RV connected to the conducting wire is changed so that the value of the meter M is minimized, and the insulation resistance R0 is determined from the resistance value of the minimized variable resistor RV. Measure.

以下,図面と数式とを参照しつつ本発明の原理につい
て詳細に説明する。
Hereinafter, the principle of the present invention will be described in detail with reference to the drawings and mathematical expressions.

第1図の実施例の動作を理解しやすくするために印加
した測定用低周波電圧による電流の流れる系に関して等
価回路を描くと第2図の如くなる。
FIG. 2 shows an equivalent circuit for a system in which a current flows due to the applied low-frequency voltage for measurement in order to make the operation of the embodiment of FIG. 1 easier to understand.

即ち第2図でγは接地線LEとの接地抵抗である。R及
びCは低圧電路1,2に関する全絶縁抵抗と全対地静電容
量を示し各々 C=C1+C2+C3+C4であり,又C0,R0は測定対象家庭内
の負荷機器に於ける静電容量と絶縁抵抗であって,今測
定せんとするものはR0,更に必要があればC0をも測定可
能である。
That is γ in FIG. 2 is a ground resistance of a ground line L E. R and C represent the total insulation resistance and total ground capacitance for the low-voltage paths 1 and 2, respectively. C = C 1 + C 2 + C 3 + C 4 , and C 0 and R 0 are the capacitance and insulation resistance of the load equipment in the home to be measured, and R 0 , If necessary, C 0 can also be measured.

この図では測定用信号として1,即ち発振器OSC1
選定された場合を示しており,以下この状態を例にとり
数式を用いて説明する。周波数1の電圧V1が注入トラ
ンスを介して電路に印加されると,このときの周波数
1の漏洩電流I1となる。一般に接地抵抗γは絶縁抵抗Rと比較するとγ
《Rであるから(1)式は となり,ここで B1=ω1(C+C0γと置換すると前記(2)式は と表すことができる。
1 as the measurement signal in this figure, that is, shows the case where the oscillator OSC 1 is selected will be described using the following equation taking this state as an example. When the voltage V 1 of the frequency 1 is applied to the electric path through the injection transformer, a frequency at this time
1 of the leakage current I 1 is Becomes Generally, the ground resistance γ is γ as compared with the insulation resistance R.
<< Because R is a formula (1) Where Substituting B 1 = ω 1 (C + C 0 ) γ gives the above equation (2) It can be expressed as.

又,電路と大地間の周波数1の電圧E1と表され,前記(2)を代入して整理すると となる。ここでB2=ω1γと置換すると前記(5)式
と表すことができる。
The voltage E 1 at frequency 1 between the electric circuit and the ground is And substituting the above (2) and rearranging Becomes Here, if B 2 = ω 1 C γ is substituted, the above equation (5) becomes It can be expressed as.

ところで注入した測定用信号電圧V1を正弦波のν0sin
ω1tとしたときの電流I1をi1と表せば(3)式から となり,又この時の電圧E1をe1と表せば となる。
By the way, the injected measurement signal voltage V 1 is converted into a sine wave ν 0 sin
If the current I 1 when ω 1 t is expressed as i 1 , from equation (3) And the voltage E 1 at this time is expressed as e 1 Becomes

従って増幅器A1の入力端を例えば接地側電路L2と大地
E3間に接続し,該増幅器A1出力に得られる電圧e1を導線
Lpを介して可変抵抗器RVで終端し,該可変抵抗器の抵抗
値をRmとすると導線Lpに流れる電流はe1/Rmとなり,該
導線Lpを測定用信号によって変流器ZCTに誘起される磁
束と反対方向の磁束が生ずるように該変流器ZCTに貫通
させればフィルタFIL出力は(7)(8)式から となる。
Thus amplifier A 1 input terminal, for example, the ground-side electrical path L 2 and ground
Connect between E 3, a voltage e 1 obtained in the amplifier A 1 output wire
Through L p terminated by the variable resistor RV, the variable resistor of the current resistance value flowing through the conducting wire L p When Rm is e 1 / Rm, and the current transformer by measuring signal conductor lines L p ZCT If the current is passed through the current transformer ZCT so that a magnetic flux in the opposite direction to the magnetic flux induced in the filter is generated, the filter FIL output can be calculated from the equations (7) and (8). Becomes

図に示すようにフィルタFILの出力を整流器DTにて整流
するとその出力Xは となる。
When the output of the filter FIL is rectified by the rectifier DT as shown in the figure, the output X becomes Becomes

上記(10)式からも分かるように出力入が最小となる
のは であり該(11)式のA3,B2,B3を再置換すると である。即ち,Rm=R0であって,出力Xが最小となる可
変抵抗器の値から絶縁抵抗R0が測定される。
As can be seen from the above equation (10), the minimum output input is And A 3 , B 2 , and B 3 in equation (11) are re-substituted. It is. That is, Rm = R0 , and the insulation resistance R0 is measured from the value of the variable resistor that minimizes the output X.

第3図は可変抵抗器RVの抵抗値Rmを変化させたときの
整流器DTの出力Xの関係を示している。即ち,メーター
Mの指示が最小となるときの可変抵抗器の抵抗値で絶縁
抵抗を測定しうることになる。
FIG. 3 shows the relationship between the output X of the rectifier DT when the resistance value Rm of the variable resistor RV is changed. That is, the insulation resistance can be measured by the resistance value of the variable resistor when the indication of the meter M is minimum.

第4図は本発明の変形実施例を示すブロック図であっ
て,同図に示す如く変流器を貫通する導線に前記可変抵
抗器と並列に可変コンデンサを接続したものである。
FIG. 4 is a block diagram showing a modified embodiment of the present invention. As shown in FIG. 4, a variable capacitor is connected in parallel with the variable resistor to a conductor passing through a current transformer.

このように回路を構成することにより導線Lpに流れる
電流i2となり,フィルタFIL出力は前述した実施例同様にi1−i
2となるから と表すことができる。
By configuring the circuit in this way, the current i 2 flowing through the conductor L p is And the filter FIL output is i 1 −i as in the previous embodiment.
Because it becomes 2. It can be expressed as.

更に該フィルタFIL出力を次段の整流器DETにて整流す
ると該整流器DET出力X1であり,該出力Xが最小となるのは(14)式から のときであり(15),(16)式からω1Cmを消去すると と表され,(17)式に於けるA3,B2,B3を再置換すると となることが分かる。
Further, when the output of the filter FIL is rectified by the rectifier DET of the next stage, the rectifier DET output X 1 becomes And the output X is minimized according to equation (14). When ω 1 Cm is eliminated from Eqs. (15) and (16), When A 3 , B 2 , and B 3 in equation (17) are replaced, It turns out that it becomes.

即ち,出力Xが最小となるよう可変コンデンサ,可変
抵抗器を調整することにより可変抵抗器の値Rmから絶縁
抵抗値R0を測定することができる。
That is, by adjusting the variable capacitor and the variable resistor so that the output X is minimized, the insulation resistance value R 0 can be measured from the value Rm of the variable resistor.

尚,増幅器A1,AMPの出力には商用周波数成分も含まれ
るがフィルタFILで除去されるため本発明の方法に何ら
影響を与えないのでこれらの成分については数式上省略
して説明した。
The outputs of the amplifiers A 1 and AMP also include commercial frequency components, but since they are removed by the filter FIL and do not affect the method of the present invention, these components have been omitted from the mathematical expressions.

更に注入トランスOTと変流器ZCTは分割型とし,電路
と大地間の電圧検出用のプローブも非接触型,例えば近
年提案されている「光電圧センサー」等を用いることに
よりポータブルな測定器とすることができる。
Furthermore, the injection transformer OT and the current transformer ZCT are of a split type, and the probe for detecting the voltage between the electric circuit and the ground is a non-contact type, for example, a portable measuring instrument using the recently proposed "optical voltage sensor". can do.

又,本実施例では単相2線式電路の場合について説明
したが一端接地電路であれば単相3線式,3相3線式電路
等であってもよく,更に大地静電容量C0を測定する必要
がある場合には可変抵抗器RVを可変コンデンサCVに置換
し,同様の手法を用いればよういことは明らかである。
Further, the single-phase three-wire system if one ground path has been described for the case of single-phase two-wire path in this embodiment may be a three-phase three-wire path or the like, the earth capacitance C 0 It is clear that if it is necessary to replace the variable resistor RV with a variable capacitor CV and use a similar technique.

(発明の効果) 本発明は以上詳述に述べた如き方法によって絶縁抵抗
を求めるものであるから,多数に分岐する電路のうち一
部分あるいは該部に接続された負荷機器についての絶縁
抵抗を他の部分のそれに影響されることなく簡易な方法
で正確に測定することができ,殊に各家庭内の絶縁監視
を個別に行なう上で極めて有効な手段である。
(Effects of the Invention) Since the present invention determines the insulation resistance by the method as described in detail above, the insulation resistance of a part of the multi-branched electric circuit or the load equipment connected to the part is reduced by another method. It can be accurately measured in a simple manner without being affected by parts, and is a particularly effective means for individually monitoring insulation in each household.

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

第1図は本発明に係かる測定回路の一実施例を示すブロ
ック図,第2図は第1図に示した電路及び測定回路の等
価回路図,第3図は抵抗値と出力との関係を示す図,第
4図は本発明の変形実施例を示す図である。 T……トランス,OSC……発振器 A1,AMP……アンプ,FIL……フィルタ,OT……注入トラン
ス,ZCT……零相変流器,DT……整流器,M……メーター,CV
……可変コンデンサ,RV……可変抵抗器。
FIG. 1 is a block diagram showing an embodiment of a measuring circuit according to the present invention, FIG. 2 is an equivalent circuit diagram of the electric circuit and the measuring circuit shown in FIG. 1, and FIG. 3 is a relation between a resistance value and an output. FIG. 4 is a view showing a modified embodiment of the present invention. T ...... trans, OSC ...... oscillator A 1, AMP ...... amplifier, FIL ...... filter, OT ...... injection transformer, ZCT ...... ZCT, DT ...... rectifier, M ...... meters, CV
…… variable capacitor, RV …… variable resistor.

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】一端が接地された配線の所要部に注入トラ
ンス及び変流器を結合し、 該注入トランスを介して周波数f1なる測定用信号を配線
に印加すると共に前記所要部と大地との間に存在する電
圧を検出し、 該検出電圧を可変抵抗器にて終端した導線に印加すると
共に、前記導線は前記配線に印加された測定用信号によ
り前記変流器に誘起される磁束と反対向きの磁束が前記
変流器に生じるように該変流器を貫通せしめ、更に、 前記変流器出力中に含まれる周波数f1成分が最小となる
ように前記可変抵抗器の抵抗値を調整し、 該可変抵抗器の抵抗値によって前記注入トランス及び変
流器を結合せしめた配線の所要部より端方部の配線及び
配線に接続した負荷機器等の絶縁抵抗を測定したこと を特徴とした低圧配線等の簡易絶縁抵抗測定方法。
1. A one end is coupled an injection transformer and current transformer to a required portion of the ground line, and the required portion and ground to apply a measuring signal comprising a frequency f 1 via a infusion transformer wiring A voltage existing between the current transformer and the detected voltage is applied to a conductor terminated with a variable resistor, and the conductor is connected to a magnetic flux induced in the current transformer by a measurement signal applied to the wire. flux in the opposite direction is caused to penetrate the modified current transformer to produce the current transformer, further, the resistance value of the variable resistor such that the frequency f 1 component is minimum contained in the current transformer output Adjusting the resistance value of the variable resistor, and measuring the insulation resistance of the wiring connected to the injection transformer and the current transformer from the required part of the wiring to the end of the wiring and the load equipment connected to the wiring. Simple insulation resistance measurement method for low voltage wiring etc. .
【請求項2】前記可変抵抗器の代わりに、可変抵抗器と
可変コンデンサとを並列に接続した回路を用い、該可変
抵抗器及び可変コンデンサを調整することにより前記注
入トランス及び変流器を結合せしめた配線の所要部より
端方部の配線及び配線に接続した負荷機器等の絶縁抵抗
を測定すること を特徴とした低圧配線等の簡易絶縁抵抗測定方法。
2. A method in which a variable resistor and a variable capacitor are connected in parallel instead of the variable resistor, and the injection transformer and the current transformer are coupled by adjusting the variable resistor and the variable capacitor. A simple insulation resistance measuring method for low-voltage wiring and the like, characterized by measuring the insulation resistance of a wiring at an end from a required portion of the stiffened wiring and a load device connected to the wiring.
JP31030988A 1988-10-07 1988-12-08 Simple insulation resistance measurement method for low voltage wiring etc. Expired - Lifetime JP2750713B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP31030988A JP2750713B2 (en) 1988-10-07 1988-12-08 Simple insulation resistance measurement method for low voltage wiring etc.

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP25296788 1988-10-07
JP63-252967 1988-10-07
JP31030988A JP2750713B2 (en) 1988-10-07 1988-12-08 Simple insulation resistance measurement method for low voltage wiring etc.

Publications (2)

Publication Number Publication Date
JPH02193077A JPH02193077A (en) 1990-07-30
JP2750713B2 true JP2750713B2 (en) 1998-05-13

Family

ID=26540967

Family Applications (1)

Application Number Title Priority Date Filing Date
JP31030988A Expired - Lifetime JP2750713B2 (en) 1988-10-07 1988-12-08 Simple insulation resistance measurement method for low voltage wiring etc.

Country Status (1)

Country Link
JP (1) JP2750713B2 (en)

Also Published As

Publication number Publication date
JPH02193077A (en) 1990-07-30

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