[go: up one dir, main page]

JP2696513B2 - Electrical capacitance measurement method for ground - Google Patents

Electrical capacitance measurement method for ground

Info

Publication number
JP2696513B2
JP2696513B2 JP20723487A JP20723487A JP2696513B2 JP 2696513 B2 JP2696513 B2 JP 2696513B2 JP 20723487 A JP20723487 A JP 20723487A JP 20723487 A JP20723487 A JP 20723487A JP 2696513 B2 JP2696513 B2 JP 2696513B2
Authority
JP
Japan
Prior art keywords
phase
frequency
output
phase shifter
ground
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
JP20723487A
Other languages
Japanese (ja)
Other versions
JPS6449981A (en
Inventor
辰治 松野
俊二 柏崎
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.)
Filing date
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 JP20723487A priority Critical patent/JP2696513B2/en
Publication of JPS6449981A publication Critical patent/JPS6449981A/en
Application granted granted Critical
Publication of JP2696513B2 publication Critical patent/JP2696513B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Measurement Of Resistance Or Impedance (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は活線状態で電路等の対地静電容量を測定する
方法に関する。 (従来技術) 従来,漏電等の電路に於けるトラブルの発見には絶縁
抵抗を測定し,電路状態を監視するのが一般的であっ
た。しかし電路に負荷Zが接続されると該負荷の大地と
の間の静電容量より大地に漏洩する漏洩電流により正常
な電路及び負荷にもかかわらず絶縁抵抗が低下した如く
測定されるので正確な電路状態の監視には対地静電容
量,即ち電路自身と大地間の静電容量或は接続した負荷
のもつ容量とを測定し,前記絶縁抵抗と併せて監視する
必要がある。従来一般的に用いられている対地静電容量
を測定する方法を第2図に示す。 これは負荷Zを有する受電変圧器Tの接地線LEを,商
用電源周波とは異なる周波数なる低周波信号発振器
OSCに接続されたトランスOTに貫通せしめるか,或いは
前記接地線LEに直列に前記発振器を挿入接続する等して
電路1及び電路2に測定用低周波電圧を印加し,前記接
地線LEを貫通せしめた変流器ZCTによって電路と大地間
に存在する絶縁抵抗Ro及び対地浮遊容量Coを介して前記
接地線に帰還する前記低周波電圧により生ずる漏洩電流
を検出しこれを増幅器AMPで増幅したのち,フィルタFIL
によって周波数の成分のみを選択し,これを例えば
前記発振器OSCの出力信号を90゜移相器PSSに印加して得
られる電圧を用いて掛算器MULTで同期検波して該漏洩電
流中の無効分(即ち印加低周波電圧と90゜移相した成
分)を検出することにより電路の静電容量を測定するよ
う構成したものであった。 本発明の理解を助けるためにその測定理論を更に説明
する。 前記接地線LEに印加される低周波信号電圧を例えば正
弦波としてVsinω1t(ω=2π)とすれば,接地
点Eを介して接地線LEに帰還する周波数の漏洩電流
Iは と表わされ,印加する交流電圧と90゜移相した成分,即
ち上記(1)式の右辺第2項の成分に比例した値を同期
検波等の手段で検出すればこの値は静電容量Coに比例し
たものとなるから,これによって電路の静電容量を求め
ることができる。しかし,このように前記接地線に帰還
する漏洩電流を変流器ZCTで検出し,更に変流器出力に
含まれる周波数の漏洩電流成分をフィルタFILで選
択出力する従来の方法では通常,変流器→増幅器→フィ
ルタの系で周波数の漏洩電流の位相がずれるから,
これらの同期検波出力からCoに比例した値を得るために
はこの位相ずれを補償する必要がある。 このために同図に示す如く同期検波器MULTの第1の入
力端又は第2の入力端に固定の移相器PSを挿入し,これ
によって上記位相ずれを補正し互いの同期をとってい
た。 しかしながら上述の如き従来の方法では変流器ZCT,フ
ィルタFIL,移相器PS等の位相特性は温度変化または使用
部品特性の経年変化等によって変動するため,この結果
最初の設定値との位相誤差が発生し,正しい測定結果を
提供できなくなる欠点があった。これらに対処するため
に従来は特性変動の少ない極めて高品質な変流器或いは
フィルタ等を採用することによって位相誤差の影響を極
力小さくしていたが,それでもその影響を完全に除去す
ることは困難であった。 (発明の目的) 本発明は以上説明したような従来の対地静電容量の測
定方法の欠点を除去するためになされたものであって,
高価な部品を必要とせず安価に測定信号の位相ずれを常
時補正し,常に正確な測定結果をもたらしうる対地静電
容量測定方法を提供することを目的とする。 (発明の概要) この目的を達成する為に、本発明に係る電路の対地静
電容量測定方法の特許請求の範囲1記載の発明は、電路
の商用周波数とは異なる周波数f1の測定用低周波信号電
圧を印加し、電路の接地線に帰還する周波数f1の漏洩電
流を検出する電路の対地静電容量測定方法に於いて、前
記周波数f1の漏洩電流を検出する系で発生する漏洩電流
の位相推移をθ、移相器PSの位相推移をθ、該移相器
PSと移相器PSSSとを直列接続したときの位相推移をθ
(但し、θ≠θ)とした場合、 前記位相推移θと移相器PSにおける位相推移量θ
の関係を|θ−θ1|≪1、前記位相推移θと前記位相推
移θとの関係を|θ−θ2|≪1となるように前記移相
器PSの位相推移量を調整すると共に前記移相器PSSSの位
相推移量を設定し、前記周波数f1の漏洩電流成分と、前
記測定用低周波信号電圧を前記移相器PSに印加すること
により得た位相がθだけ推移した電圧とを用いて同期
検波することにより第1の出力を得、前記周波数f1の漏
洩電流成分と、前記測定用低周波信号電圧を前記移相器
PSを介して前記移相器PSSSに印加することにより得た位
相がθだけ推移した電圧とを用いて同期検波すること
により第2の出力を得、前記第1の出力及び第2の出力
との差を用いて電路の対地静電容量を測定したことを特
徴とする。 (発明の実施例) 以下図示した実施例に基づき本発明を詳細に説明す
る。 第1図は本発明の一実施例を示すブロック図であって
第2図と同一の記号は同一の意味をもつものとする。即
ち,同図に於てTは変圧器,1及び2はこの変圧器の2次
側低電路であって該電路2には第2種接地工事を施した
接地線LEが接続される。該接地線LEにはトランスOT及び
変流器ZCTとが結合され,該変流器ZCTの出力端は増幅器
AMPに接続し,該AMPの出力端はフィルタFILに接続す
る。該フィルタFILの出力は同期検波器MULT1の一入力端
に接続し,他の入力端には第1の移相器PSの出力端と接
続し,該PSの入力端は発振器OSCの出力端と接続する。
一方同期検波器MULT2の一入力端には前記フィルタFILの
出力端と接続し,他の入力端は前記移相器PSの出力端に
接続した第2の移相器PSSSの出力端の接続する。前記同
期検波器MULT1,MULT2の夫々の出力端を引算回路SUBの入
力端と接続する。 このように構成した回路に於て発振器OSCよりトラン
スOTを介して接地線に入力した信号は変流器ZCTを介し
て帰還し,増幅器AMP,フィルタFILの系を通過する時に
発生する位相のずれをθとすれば該フィルタFIL出力に
於ける周波数の漏洩電流成分は第1式より となり,同期検波器MULT1,MULT2の夫々の一方の入力端
に入力される。 一方,発振器OSCの出力は移相器PSを介して第1の同
期検波器MULT1の他の入力端に加える。この電圧をaosin
(ω1t+θ)とすれば前記第1の同期検波器の出力M1
となる。一方,位相器PSの出力を一定の固定位相量をも
つ移相器PSSSに加え,その出力をaocos(ω1t+θ
とすれば第2の同期検波器の出力M2となる。 更に移相器PSを調整して |θ−θ1|≪1,|θ−θ2|≪1 とすればcos(θ−θ)1,cos(θ−θ)1,sin
(θ−θ)θ−θ1,sin(θ−θ)θ−θ
なるから(3),(4)式のM1,M2 と近似される。なお、|θ−θ1|≪、|θ−θ2|≪1と
するため、上記PSの調整及びPSSSの設定の具体的方法
は、|θ−θ1|≪1の場合(3)式の右辺第二項が“0"
となり、同期検波器のMULT1の出力が最大となるので、
同期検波器MULT1の出力がほぼ最大となるように移送器P
Sを調整すると共に、|θ−θ2|≪の場合(4)式の右
辺第二項が“0"となり、同期検波器MULT2の出力が最大
となるので、同期検波器MULT2の出力が最大に近く、且
つθ≠θとなるように移送器PSSSの移送推移量を設
定すればよい。従って同期検波器MULT1,MULT2の夫々の
出力を引算器SUBに入力すれば,該SUBの出力にはに相当する値が得られる。 上記(7)式に於けるθ−θは移相器PSSSによる
固定位相推移量であり,更に角周波数ω1,電圧V,aoが一
定値であれば前記引算回路SUBの出力は対地静電容量Co
に比例した電圧を得ることができ,該電圧値により回路
中に於ける各部品の経年変化及び温度変化による位相特
性の影響を受けずに前記対地静電容量Coを算出すること
ができる。 尚,上記説明に於ては単相2線式電路の場合について
のみ説明したがこれに限るわけではなく,単相3線,3相
3線式電路にも適用可能なことは明らかであり,更に単
相2線式電路及び三相電路の各相について測定する場合
には商用周波電圧を測定用低周波信号電圧の代替として
使用することが可能なことは明らかである。 (発明の効果) 本発明は以上説明した如く構成し且つ動作するもので
あるから簡易な回路構成で対地静電容量測定回路に於け
る位相特性の変動の影響を補償し,正確な対地静電容量
を測定するうえで著効を奏するものである。
Description: TECHNICAL FIELD The present invention relates to a method for measuring a ground capacitance of an electric circuit or the like in a live state. (Prior Art) Conventionally, in order to find a trouble in an electric circuit such as an electric leakage, it has been general to measure an insulation resistance and monitor an electric circuit state. However, when the load Z is connected to the electric circuit, the measurement is made as if the insulation resistance was lowered despite the normal electric circuit and the load due to the leakage current leaking to the ground from the capacitance between the load and the ground. In order to monitor the state of the electric circuit, it is necessary to measure the electrostatic capacitance to the ground, that is, the capacitance between the electric circuit itself and the ground or the capacitance of the connected load, and to monitor the capacitance together with the insulation resistance. FIG. 2 shows a method of measuring the electrostatic capacitance generally used in the related art. Low frequency signal oscillator which the ground line L E of the power receiving transformer T having a load Z, becomes different frequency 1 from the commercial power source frequency
Or allowed to penetrate to the connected transformer OT to OSC, or by applying a low-frequency voltage measured by, for example connecting insert the oscillator in series with the path 1 and path 2 to the ground line L E, the ground line L E The leakage current generated by the low-frequency voltage that is fed back to the ground line via the insulation resistance Ro existing between the electric circuit and the ground and the ground stray capacitance Co is detected by the current transformer ZCT penetrating through the current transformer ZCT and amplified by the amplifier AMP. After that, filter FIL
Only the component of frequency 1 is selected, and this is synchronously detected by the multiplier MULT using the voltage obtained by applying the output signal of the oscillator OSC to the 90 ° phase shifter PSS, for example. The electrostatic capacitance of the electric circuit is measured by detecting the component (that is, the component shifted by 90 ° from the applied low frequency voltage). The measurement theory will be further described to assist in understanding the present invention. If Vsinomega 1 t and (omega 1 = 2 [pi 1) a low-frequency signal voltage applied to the ground line L E, for example, as a sine wave, the frequency 1 which returns to the ground line L E via the ground point E leakage current I is If a component that is 90 ° out of phase with the applied AC voltage, that is, a value proportional to the component of the second term on the right side of the above equation (1), is detected by means such as synchronous detection, this value is determined by the capacitance. Since it is proportional to Co, the capacitance of the electric circuit can be obtained from this. However, in the conventional method in which the leakage current returning to the ground line is detected by the current transformer ZCT and the leakage current component of frequency 1 included in the current transformer output is selected and output by the filter FIL, the current is usually changed. Since the phase of the leakage current at frequency 1 is shifted in the flower → amplifier → filter system,
In order to obtain a value proportional to Co from these synchronous detection outputs, it is necessary to compensate for this phase shift. For this purpose, a fixed phase shifter PS is inserted into the first input terminal or the second input terminal of the synchronous detector MULT as shown in the figure, thereby correcting the phase shift and synchronizing with each other. . However, in the conventional method as described above, the phase characteristics of the current transformer ZCT, filter FIL, phase shifter PS, etc. fluctuate due to temperature changes or aging of the characteristics of the parts used, and as a result, the phase error from the initial set value This has the disadvantage that correct measurement results cannot be provided. In order to cope with these, the influence of the phase error has been minimized by adopting an extremely high-quality current transformer or filter with little characteristic fluctuation, but it is still difficult to completely eliminate the influence. Met. (Object of the Invention) The present invention has been made in order to eliminate the disadvantages of the conventional method for measuring the capacitance to ground as described above.
It is an object of the present invention to provide a method for measuring the capacitance to ground that can always correct the phase shift of a measurement signal at low cost without requiring expensive components and can always provide accurate measurement results. SUMMARY OF THE INVENTION In order to achieve this object, the invention of claims 1, wherein in the earth capacitance measuring method of path according to the present invention, low for measurement of different frequencies f 1 and path of the commercial frequency applying a frequency signal voltage, at the earth capacitance measuring method path for detecting a leakage current of a frequency f 1 to return to the path of the ground line, generated in a system for detecting a leakage current of the frequency f 1 leakage The phase transition of the current is θ, the phase transition of the phase shifter PS is θ 1 ,
The phase transition when PS and phase shifter PSSS are connected in series is θ 2
(Where θ 1 ≠ θ 2 ), the relationship between the phase transition θ and the phase transition amount θ 1 in the phase shifter PS is | θ−θ 1 | ≪1, the phase transition θ and the phase transition θ 2 and of the relationship | θ-θ 2 | set the phase shift amount of the phase shifter PSSS with adjusting the phase shift amount of << 1 become as the phase shifter PS, the leakage current the frequency f 1 a component to obtain a first output by synchronous detection by using the voltage obtained phase remained only theta 1 by applying the low-frequency signal voltage for measurement to said phase shifter PS, the frequency f The leak current component of 1 and the low frequency signal voltage for measurement are
Via the PS obtain a second output by synchronous detection by using the voltage obtained phase remained only theta 2 by applying to the phase shifter PSSS, the first output and the second output And the capacitance of the electric circuit to ground was measured using the difference between (Embodiments of the Invention) Hereinafter, the present invention will be described in detail based on the illustrated embodiments. FIG. 1 is a block diagram showing one embodiment of the present invention, and the same symbols as those in FIG. 2 have the same meanings. Ie, T At a drawing transformers, 1 and 2 this transformer the electric path 2 a secondary low path ground line L E which has been subjected to second type grounding is connected. The grounding line L E are combined with trans OT and current transformer ZCT, the output end of the displacement current transformer ZCT an amplifier
Connected to AMP, the output of which is connected to filter FIL. The output of the filter FIL is connected to one input terminal of the synchronous detector MULT1, the other input terminal is connected to the output terminal of the first phase shifter PS, and the input terminal of the PS is connected to the output terminal of the oscillator OSC. Connecting.
On the other hand, one input terminal of the synchronous detector MULT2 is connected to the output terminal of the filter FIL, and the other input terminal is connected to the output terminal of a second phase shifter PSSS connected to the output terminal of the phase shifter PS. . The respective output terminals of the synchronous detectors MULT1 and MULT2 are connected to the input terminals of a subtraction circuit SUB. In the circuit configured in this way, the signal input from the oscillator OSC to the ground line via the transformer OT is fed back via the current transformer ZCT, and the phase shift that occurs when passing through the amplifier AMP and filter FIL system If θ is θ, the leakage current component at frequency 1 at the filter FIL output is And input to one input terminal of each of the synchronous detectors MULT1 and MULT2. On the other hand, the output of the oscillator OSC is applied to another input terminal of the first synchronous detector MULT1 via the phase shifter PS. This voltage is a o sin
1 t + θ 1 ), the output M 1 of the first synchronous detector
Is Becomes On the other hand, the output of the phase shifter PS is added to the phase shifter PSSS having a fixed fixed phase amount, and the output is a o cos (ω 1 t + θ 2 )
Then, the output M 2 of the second synchronous detector is Becomes If the phase shifter PS is further adjusted to | θ−θ 1 | ≪1, | θ−θ 2 | ≪1, cos (θ−θ 1 ) 1, cos (θ−θ 2 ) 1, sin
(Θ−θ 1 ) θ−θ 1 , sin (θ−θ 2 ) θ−θ 2 , M 1 and M 2 in the equations (3) and (4) are Is approximated. Note that, in order to satisfy | θ−θ 1 | ≪ and | θ−θ 2 | PS1, the specific method of adjusting the PS and setting the PSSS is given by the following equation (3) when | θ−θ 1 | ≪1 The second term on the right side of is "0"
Since the output of MULT 1 of the synchronous detector becomes the maximum,
Transfer device P so that the output of synchronous detector MULT 1 is almost maximum.
With adjusting S, | θ-θ 2 | « case (4) of the second term on the right-hand side becomes" 0 ", the output of the synchronous detector MULT 2 is maximum, the synchronous detector MULT 2 Output Should be set such that θ 1 is close to the maximum and θ 1 ≠ θ 2 . Therefore, if the outputs of the synchronous detectors MULT1 and MULT2 are input to the subtractor SUB, the output of the SUB Is obtained. Equation (7) in theta 1 - [theta] 2 to is a fixed phase shift amount by the phase shifter PSSS, further angular frequency omega 1, the voltage V, a o is the output of the subtraction circuit SUB if a constant value Is the ground capacitance Co
Can be obtained, and the ground capacitance Co can be calculated from the voltage value without being affected by the phase characteristics due to the aging and temperature change of each component in the circuit. In the above description, only the case of a single-phase two-wire circuit has been described. However, the present invention is not limited to this. Further, it is apparent that the commercial frequency voltage can be used as a substitute for the measurement low frequency signal voltage when measuring each phase of the single-phase two-wire circuit and the three-phase circuit. (Effects of the Invention) Since the present invention is constructed and operates as described above, it is possible to compensate for the influence of the fluctuation of the phase characteristic in the ground capacitance measuring circuit with a simple circuit configuration, and to obtain an accurate ground capacitance. This is very effective in measuring the capacity.

【図面の簡単な説明】 第1図は本発明の一実施例を示すブロック図,第2図は
従来の対地静電容量を測定する方法を示すブロック図で
ある。 T……トランス,1,2……電路,LE……接地線,E……接地
点,MULT,MULT1,MULT2……同期検波器, ZCT……変流器,AMP……増幅器,FIL……フィルタ, OSC……発振器,OT……注入トランス,PS,PSS,PSSS……移
相器。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a block diagram showing an embodiment of the present invention, and FIG. 2 is a block diagram showing a conventional method for measuring a ground capacitance. T… Transformer, 1,2… Electrical path, L E … Ground line, E… Ground point, MULT, MULT1, MULT2… Synchronous detector, ZCT… Current transformer, AMP… Amplifier, FIL… … Filter, OSC …… Oscillator, OT …… Injection transformer, PS, PSS, PSSS …… Phase shifter.

Claims (1)

(57)【特許請求の範囲】 1.電路の商用周波数とは異なる周波数f1の測定用低周
波信号電圧を印加し、電路の接地線に帰還する周波数f1
の漏洩電流を検出する電路の対地静電容量測定方法に於
いて、前記周波数f1の漏洩電流を検出する系で発生する
漏洩電流の位相推移をθ、移相器PSの位相推移をθ
該移相器PSと移相器PSSSとを直列接続したときの位相推
移をθ(但し、θ≠θ)とした場合、 前記位相推移θと移相器PSにおける位相推移量θとの
関係が|θ−θ1|≪1、前記位相推移θと前記位相推移
θとの関係が|θ−θ2|≪1となるように前記移相器
PSの位相推移量を調整すると共に前記移相器PSSSの位相
推移量を設定し、 前記周波数f1の漏洩電流成分と、前記測定用低周波信号
電圧を前記移相器PSに印加することにより得た位相がθ
だけ推移した電圧とを用いて同期検波することにより
第1の出力を得、 前記周波数f1の漏洩電流成分と、前記測定用低周波信号
電圧を前記移相器PSを介して前記移相器PSSSに印加する
ことにより得た位相がθだけ推移した電圧とを用いて
同期検波することにより第2の出力を得、 前記第1の出力と第2の出力との差を用いて電路の対地
静電容量を測定したことを特徴とする電路の対地静電容
量測定方法。
(57) [Claims] Applying a low-frequency signal voltage for the measurement of different frequencies f 1 and path of the commercial frequency, the frequency f 1 is fed back to the path of the ground line
Leakage current at the earth capacitance measuring method path for detecting the frequency f 1 of the phase transition of the leakage current generated in a system for detecting a leakage current theta, the phase shifter a phase transition of the PS theta 1 ,
If the phase shift when the phase shifter PS and the phase shifter PSSS are connected in series is θ 2 (where θ 1 ≠ θ 2 ), the phase shift θ and the phase shift amount θ 1 in the phase shifter PS relationship with the | θ-θ 1 | «1, the relationship between the phase shift theta and the phase shift theta 2 is | θ-θ 2 | «1 and the phase shifter so that
Set the phase shift amount of the phase shifter PSSS with adjusting the phase shift amount of PS, a leakage current component of the frequency f 1, by applying a low-frequency signal voltage the measurement to the phase shifter PS The phase obtained is θ
A first output is obtained by performing synchronous detection using the voltage shifted by 1 and the phase shift of the leakage current component of the frequency f 1 and the measurement low-frequency signal voltage via the phase shifter PS is performed. obtain a second output by synchronous detection by using the voltage obtained phase remained only theta 2 by applying to the vessel PSSS, path using a difference between the first output and the second output A method for measuring the capacitance of an electric circuit to ground, characterized by measuring the capacitance to ground.
JP20723487A 1987-08-20 1987-08-20 Electrical capacitance measurement method for ground Expired - Lifetime JP2696513B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20723487A JP2696513B2 (en) 1987-08-20 1987-08-20 Electrical capacitance measurement method for ground

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20723487A JP2696513B2 (en) 1987-08-20 1987-08-20 Electrical capacitance measurement method for ground

Publications (2)

Publication Number Publication Date
JPS6449981A JPS6449981A (en) 1989-02-27
JP2696513B2 true JP2696513B2 (en) 1998-01-14

Family

ID=16536449

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20723487A Expired - Lifetime JP2696513B2 (en) 1987-08-20 1987-08-20 Electrical capacitance measurement method for ground

Country Status (1)

Country Link
JP (1) JP2696513B2 (en)

Also Published As

Publication number Publication date
JPS6449981A (en) 1989-02-27

Similar Documents

Publication Publication Date Title
US4857830A (en) Method for measuring insulation resistance of electric line
US4851761A (en) Method for measuring insulation resistance of electric line
JP2696513B2 (en) Electrical capacitance measurement method for ground
JP2617324B2 (en) Insulation resistance measurement method
US4857855A (en) Method for compensating for phase of insulation resistance measuring circuit
JPH0552466B2 (en)
JPS61155869A (en) Measuring method of phase-compensated insulation resistance
JP2646089B2 (en) Method for measuring insulation resistance of low-voltage circuit
JP2696510B2 (en) Measurement method of insulation resistance of electric circuit
JP2612703B2 (en) Insulation resistance measurement method with canceling ground resistance
JP2896574B2 (en) Compensation method for phase characteristics of zero-phase current transformer
JP2764582B2 (en) Simple insulation resistance measurement method
JP2612719B2 (en) Simple insulation resistance measurement method for electrical circuits
JP2617325B2 (en) Insulation resistance measurement method
JPH0721523B2 (en) Insulation resistance measurement method that compensates for fluctuations in circuit constants
JP2614447B2 (en) Insulation resistance measurement method that compensates for the effect of ground resistance
JPH0721522B2 (en) Insulation resistance measurement method with phase compensation
JP2614449B2 (en) Insulation resistance measurement method compensated for ground resistance
JPH0721520B2 (en) Insulation resistance measurement method with phase compensation
JPH0731219B2 (en) Insulation resistance measuring device phase compensation method
JPH03218479A (en) Insulation degradation diagnostic method for cable
JP2750707B2 (en) Insulation resistance measurement method compensated for ground resistance
JPH0721519B2 (en) Method for measuring insulation resistance of phase-compensated circuit
JP2750705B2 (en) Insulation resistance measurement method
JPS58127172A (en) Insulation resistance measuring apparatus for electric line with suppressed stray capacity

Legal Events

Date Code Title Description
S111 Request for change of ownership or part of ownership

Free format text: JAPANESE INTERMEDIATE CODE: R313111

R360 Written notification for declining of transfer of rights

Free format text: JAPANESE INTERMEDIATE CODE: R360

R371 Transfer withdrawn

Free format text: JAPANESE INTERMEDIATE CODE: R371

S111 Request for change of ownership or part of ownership

Free format text: JAPANESE INTERMEDIATE CODE: R313111

R350 Written notification of registration of transfer

Free format text: JAPANESE INTERMEDIATE CODE: R350

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

EXPY Cancellation because of completion of term