JPS58769A - Method of detecting dielectric resistance, insulation thereof is insufficient, of electrodynamic machine winding - Google Patents
Method of detecting dielectric resistance, insulation thereof is insufficient, of electrodynamic machine windingInfo
- Publication number
- JPS58769A JPS58769A JP57070159A JP7015982A JPS58769A JP S58769 A JPS58769 A JP S58769A JP 57070159 A JP57070159 A JP 57070159A JP 7015982 A JP7015982 A JP 7015982A JP S58769 A JPS58769 A JP S58769A
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- frequency
- measuring
- detection device
- amplitude
- 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.)
- Pending
Links
- 238000009413 insulation Methods 0.000 title claims description 26
- 238000004804 winding Methods 0.000 title claims description 21
- 238000000034 method Methods 0.000 title claims description 8
- 230000005520 electrodynamics Effects 0.000 title 1
- 238000005259 measurement Methods 0.000 claims description 31
- 238000001514 detection method Methods 0.000 claims description 21
- 150000002500 ions Chemical class 0.000 claims description 14
- 230000004888 barrier function Effects 0.000 claims description 6
- 239000003990 capacitor Substances 0.000 claims description 4
- 239000004020 conductor Substances 0.000 claims description 3
- 238000005070 sampling Methods 0.000 claims description 3
- 206010011224 Cough Diseases 0.000 claims 1
- 241000206754 Palmaria palmata Species 0.000 claims 1
- 239000001921 dulse Substances 0.000 claims 1
- 239000003921 oil Substances 0.000 claims 1
- 238000010408 sweeping Methods 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 7
- 238000011156 evaluation Methods 0.000 description 6
- CBENFWSGALASAD-UHFFFAOYSA-N Ozone Chemical compound [O-][O+]=O CBENFWSGALASAD-UHFFFAOYSA-N 0.000 description 3
- 230000015556 catabolic process Effects 0.000 description 3
- 239000011148 porous material Substances 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 210000003127 knee Anatomy 0.000 description 2
- 238000000691 measurement method Methods 0.000 description 2
- 230000003071 parasitic effect Effects 0.000 description 2
- 241001385733 Aesculus indica Species 0.000 description 1
- 208000018583 New-onset refractory status epilepticus Diseases 0.000 description 1
- 240000002834 Paulownia tomentosa Species 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- 241001255854 Teras Species 0.000 description 1
- 241000700605 Viruses Species 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 239000003048 aphrodisiac agent Substances 0.000 description 1
- 230000002509 aphrodisiac effect Effects 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 125000004122 cyclic group Chemical group 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000002939 deleterious effect Effects 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000001627 detrimental effect Effects 0.000 description 1
- 238000010494 dissociation reaction Methods 0.000 description 1
- 230000005593 dissociations Effects 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 238000005868 electrolysis reaction Methods 0.000 description 1
- 230000001667 episodic effect Effects 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 241000894007 species Species 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/34—Testing dynamo-electric machines
- G01R31/346—Testing of armature or field windings
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Tests Of Circuit Breakers, Generators, And Electric Motors (AREA)
- Testing Relating To Insulation (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
高電圧電気機械の巻線の絶縁の品質?評価する問題は以
紡から知られている。しかし巻線の絶縁を劣化させる原
因は1つではないので、従来Fi耐験に軸らざるを得な
かったが、このM験による評価がうまくゆかないと、電
気機械の巻線分完全な状態に巻直すことが必要になるた
め、メーカーシてとって損失になり、オた経験による評
価に使用される方法が電気機械の絶縁の差迫った穿孔を
予想することを可能にしないため、使用渚にとっても損
失になる。[Detailed Description of the Invention] Quality of insulation of high-voltage electric machine windings? The problem to be evaluated is known from Ibo. However, since there is more than one cause for the deterioration of the winding insulation, conventionally we had no choice but to focus on the Fi test, but if the evaluation using the M test does not go well, the winding of the electrical machine will be in perfect condition. This is a loss to the manufacturer due to the need for rewinding, and the method used for empirical evaluation does not allow predicting impending perforation of the electrical machine insulation, so it is not recommended to use it. It would also be a loss for Nagisa.
従来の知見の総合により、外見上は完全な巻線の絶縁の
不充分な絶縁耐力が、成る閾値電圧以降に現出される絶
縁内部の局所部分放電の成立による本のであることが最
近WAHされた。しかし絶縁内部の局所部分放電は直接
測定ができない几め、この知見によっては、間曙が単に
移されるにすき′ない。A recent study by WAH has shown that the insufficient dielectric strength of apparently perfect winding insulation is due to the formation of local partial discharges inside the insulation that appear after a threshold voltage of Ta. However, since local partial discharges inside the insulation cannot be directly measured, there is no way that this knowledge can simply be transferred.
一般に承蛯されている従来技術の見解によれば。According to the generally accepted view of the prior art.
絶縁の内部の局所部分数tFi、特に高電圧の絶瞭中に
多少分布されたガス吸収箇所に生ずる。部分放電の成る
電圧値以降において、電圧値の増大に伴って相当大きな
数の気孔の内部に部分放電が成立すると、巻線の容量は
、放電の座である気孔の内部が導体になるので、印加電
圧の関数として変化する。この昭識により、TERAS
E(El@ctr。A local fraction tFi within the insulation occurs, especially at more or less distributed gas absorption points during the high voltage gap. If a partial discharge occurs inside a considerably large number of pores as the voltage increases beyond the voltage value at which a partial discharge occurs, the capacity of the winding will change as the inside of the pores, which is the seat of the discharge, becomes a conductor. Varies as a function of applied voltage. With this enlightenment, TERAS
E(El@ctr.
En@、 Jap、、1973年2月)i−t、印加電
圧の関数としての巻線容量の曲線の推移に基づい九絶繰
の品質の規準を提案した。この特性は容量測定ブリッジ
例えばシェリングブリッジの助けを借りて定めることが
できる。TERASE法によれば、成る場合にけ、有益
な結絢を引出すことができる。En@, Jap, February 1973) it proposed a nine-point quality criterion based on the course of the curve of the winding capacitance as a function of the applied voltage. This characteristic can be determined with the help of a capacitance measuring bridge, for example a Schelling bridge. According to the TERASE method, beneficial knots can be drawn out only when this occurs.
しかし他の多くの場合には、評価の重弗な特徴を定める
精賓が充分ではない。I!に別の場合Ku、所畳の効果
が他の現象により完全にマスキングされふ。However, in many other cases, there are not enough distinguished guests to define the critical features of the evaluation. I! In other cases, the effect of Ku is completely masked by other phenomena.
本発明の目的は、非常に感度が高く、既存の測定装置に
より実施でき、有害な部分放電とイオン可動實とのうち
どちらか一方又は両方に基づいた物理的な側面から有用
な評価基準を与え得る検出方法を提供することにあふ。It is an object of the present invention to provide useful evaluation criteria from physical aspects based on harmful partial discharge and/or ion mobility, which is very sensitive and can be carried out with existing measurement equipment. We aim to provide a detection method to obtain the desired results.
本発明け、容量測定ブリッジの測定道中に、巻線の導体
と、巻線の範囲に配設された電気機械の質量部分とを接
続し、所定の電圧範囲内に含オれる各々の測定交流電圧
について、測定ブリッジを平衡させ、交流電圧の周波数
は電a:に機械の使用条件において巻@に生ずる周波数
の中から運ぶこ七により、電気機械の巻線の絶縁の不充
分な絶縁耐力を検出する方法において、敗る1つの所定
の媚tIN数を通過させる電流ノ奢ルス又は電流の高選
択性測定装置又は各々が異なる所定の周波数を!l!l
過させる電tlllJ−4ルス又は電流の高選択性の複
数の測定装fを相#後させて、平衡指示器に代るように
、側?ブリッジの平衡対角辺中に配設することと。In the measuring path of the capacitance measuring bridge, the conductor of the winding and the mass part of the electric machine arranged in the area of the winding are connected, and each measured alternating current contained within a predetermined voltage range is connected. For voltage, the measuring bridge is balanced, and the frequency of the alternating voltage is calculated from the frequencies occurring in the windings under the conditions of use of the machine. In the method of detecting, a high selectivity measuring device of current flow or current passing through one predetermined number of aphrodisiacs or each different predetermined frequency! l! l
A high-selectivity multiple measuring device f of the electric current tllllJ-4 pulse or current to be passed is placed after the phase, and the side? and placed in the balanced diagonal side of the bridge.
使用電圧よりも低い傭と電気機械の最大許容電圧に叫し
いか又けこれより高い値との間において、測定電圧の値
tスイープすbことを特徴とする検出方法に存する。好
ましくけ、印加電圧の関数と □して、高選択性測
定要素ないしFi測定装曾により測定される電流又はノ
々ルスの繰返し頻度ないし周波数と振幅とのうちどちら
か一方又は両方を記鈴し、これらの量の曲線の形状から
、電気機械の巻線の絶縁が不児全か否かを評価する。The detection method is characterized in that the value of the measured voltage is swept between a value lower than the working voltage and a value at least equal to or higher than the maximum permissible voltage of the electric machine. Preferably, as a function of the applied voltage, one or both of the repetition rate or frequency and the amplitude of the current or the Norms measured by the highly selective measuring element or Fi measuring device are recorded. , from the shapes of the curves of these quantities, it is evaluated whether the insulation of the windings of the electric machine is poor or not.
次に添付図面に示した本発明の一実施例を参照して更に
説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, an embodiment of the present invention will be further described with reference to the accompanying drawings.
第1図に示した測定ブリッジは、4つの側辺と1の平衡
対角辺とを備えている。4つの側辺は、被測容量1(こ
の例では、電動機の固定子巻線の電動機質量に対する容
量)と、基準コンデンサー2と、平衡抵抗3と、平衡コ
ンデンサー4(可変抵抗5と並列に接続される)とを備
えている。測定対角辺には切替スイッチ6が配設してあ
り、スイッチ6Fi平衡指示器7Kか又はフェライトコ
アの可飽和高−波変圧器8に接続されており、高闇波変
圧1ls8の2次巻線は波高電圧計9に給電する。The measuring bridge shown in FIG. 1 has four side edges and one balanced diagonal edge. The four sides are the capacitance to be measured 1 (in this example, the capacitance of the stator winding of the motor relative to the motor mass), the reference capacitor 2, the balance resistor 3, and the balance capacitor 4 (connected in parallel with the variable resistor 5). ). A changeover switch 6 is arranged on the measurement diagonal side, and is connected to the switch 6Fi balance indicator 7K or the ferrite core saturable high-wave transformer 8, and the secondary winding of the high-dark wave transformer 1ls8 is Power is supplied to the wave height voltmeter 9.
スイッチ6を設ける代りに変圧器8を測定対角辺中に恒
久的Km続し、ローノ青スフイルターを平衡指示器7と
直列に結線してもよい、変圧器8−電圧針9の代妙に、
部分放電に基づく電流ノ々ルスの最大振幅管高選択賓で
測定する他の全ての装置を使用することもできる。振幅
最大の電aノeルスは明らかに有害なp4ルスである。Instead of providing the switch 6, a transformer 8 may be permanently connected in the measuring diagonal, and the Ronso blue filter may be connected in series with the balance indicator 7. To,
All other devices that measure the maximum amplitude of current flow based on partial discharges can also be used. The electron pulse with the largest amplitude is clearly the deleterious p4 pulse.
測定は次のように行う、電動機の公称電圧の同勢の成る
範囲の各測定電圧について、平衡指示器7の助けを借り
て53 Hz の−波数につきブリッジをひと先ず平衡
させる。これにより電#IJ1mの質量に対する固定子
巻線の容量を測定する6絶1図に示したブリッジの給電
状態においては、電動機の固定子質量は大地から絶縁さ
れていなけれげならない、接地された機械の固定子@@
の各iを測定する場合には、測定辺(複数)Kよりプリ
ツノに給電するか又は第2図に例示したような別の形式
のブリッジを使用することが必!PKなる。The measurements are carried out as follows: for each measured voltage in the range of the nominal voltage of the motor, the bridge is first balanced with the aid of the balance indicator 7 at a wavenumber of 53 Hz. This measures the capacitance of the stator winding with respect to the mass of electric current #IJ1m. In the bridge power supply state shown in Figure 1, the stator mass of the motor must be insulated from the ground, and the Stator of @@
When measuring each i of , it is necessary to supply power to the Pritsuno from the measurement sides K or to use another type of bridge as illustrated in Figure 2. It becomes PK.
ブリッジの平衡が得られたら、平衡指示器7全回路から
速断して測定対角辺に変圧vs8を挿入す石ように、ス
イッチ6の可動接点の位置を切替える。変圧5SFi、
局所部分放電の平均パルス1の後縁の持続時間Oの逆数
にはt!対応する周波数tK高選択性をもつ高選択性変
圧器である。第5図においてt4ルス1け、矢験部分を
代表する成分1p と後縁を代表する成分:9 とに
分解される。When the balance of the bridge is obtained, the position of the movable contact of the switch 6 is changed so that all the circuits of the balance indicator 7 are quickly disconnected and the transformer vs8 is inserted on the diagonal side for measurement. Transformation 5SFi,
The reciprocal of the duration O of the trailing edge of the average pulse 1 of the local partial discharge is t! It is a high selectivity transformer with a corresponding frequency tK high selectivity. In FIG. 5, t4 is decomposed into a component 1p representing the arrow part and a component 9 representing the trailing edge.
msされるように成分1.は振部は小さいが持続時間は
非常に長く、従って持続時間の非常に短かい成分1.よ
りも絶縁破壊効果により多く寄与する。後縁の持続時間
は、成分1.の波高値の半分の高さの・fシス1.の持
続時間である。変圧器8−波高電圧計9のユニットの通
過帯は好ましくは周波数f=」−の回りの非常に狭い範
囲である。Component 1. The vibration part is small but the duration is very long, so the duration is very short.1. contributes more to the dielectric breakdown effect. The trailing edge duration is component 1.・fsis of half the height of the wave height of 1. is the duration of The passband of the transformer 8-voltmeter 9 unit is preferably a very narrow range around the frequency f=''-.
0
この通過帯は成分1.並びにあらゆる種類の寄生パルス
?:除去し得るように選定される。0 This passband is component 1. as well as all kinds of parasitic pulses? : Selected so that it can be removed.
変圧器8の選択によシ所定の周波数fを、l!I択した
場合、検出装置は、その持続時間0が周波数1の逆数に
対応するところの平均パルスに感応する。Depending on the selection of the transformer 8, a predetermined frequency f, l! In the case of option I, the detection device is sensitive to an average pulse whose duration 0 corresponds to the reciprocal of the frequency 1.
即ち局所部分放電の平均パルスの形状は、印加された電
圧の1141数として変化でき、また1つの絶縁部から
別の絶縁部にかけて変化でき、電圧の関数としての変化
は、遭遇される変化の中で最も大きい、S分放電を容易
に測定するには、基準コンデ/+−2の容量と平衡抵抗
3の抵抗との積は、平均ノ4ルスの持続時間Oよりも短
かい成る時間に等しくなければならない。これによりノ
9ルスの急峻な波頭の影響を測定から排除できる。この
急峻な波頭ないしは成分子、tL絶縁内部には荷を発生
させるのに必要なエネルゼーを表わし、これはそれ自身
として有害ではない。有害なのは、成分1゜によって表
わされるこれらの電荷の排除ないしは除去の動力学であ
る。変圧器8の141i選択性のため、その平均放電ノ
4ルスが持続時間0を号するところの測定電圧値を定め
ることができる。その理由は、#lJ定電圧の関数とし
て波高電圧計9により測定される値を表わす曲線は上記
電圧値において極大になるからである。その反対に、測
定された曲線が顕著な極大値を示さなければ、局所部分
放電に関連し九絶縁を劣化させない池の現象が気孔の1
所に現出されているものと推定しなければならない。That is, the shape of the average pulse of a local partial discharge can vary as a number of applied voltages, and can vary from one insulation to another, and the variation as a function of voltage is among the variations encountered. To easily measure the discharge of S minutes, which is the largest in There must be. This makes it possible to eliminate the influence of the steep wave crest of the Norse from the measurement. This steep wave front or element represents the energy necessary to generate a charge within the tL insulation, which is not harmful in itself. What is detrimental is the kinetics of removal of these charges represented by component 1°. Due to the 141i selectivity of the transformer 8, it is possible to determine the measured voltage value at which the average discharge voltage has a duration of zero. The reason is that the curve representing the value measured by the peak voltmeter 9 as a function of the #lJ constant voltage reaches a maximum at the above voltage value. On the contrary, if the measured curve does not show significant local maxima, then the phenomenon of ponding, which is related to local partial discharges and does not degrade the insulation, is likely to occur in the pores.
It must be assumed that it appears in the location.
従ってこの場合は絶縁は正常と見てもよい。変圧器8F
i不飽和焚圧器であり、変圧IS8の1次舎線の両端間
の電荷量が局所部分放電現象と見合う成る値よりも大き
な成る@値を超過した時から飽和が作用し始める。従っ
てこの@値が超過された場合に記録される現象は、表面
放電のように局所部分放電と共通のなにものももたない
ものとなる。Therefore, in this case, the insulation can be considered normal. Transformer 8F
It is an unsaturated compressor, and saturation begins to occur when the amount of charge between both ends of the primary wire of the transformer IS8 exceeds a value that is greater than the value that is commensurate with the local partial discharge phenomenon. Therefore, the phenomenon recorded when this @ value is exceeded has nothing in common with a local partial discharge, such as a surface discharge.
波高電圧計9の代りに有害なパルスの計数器分使用して
もよい。成るノ!ルスの有害性は、その大きさと繰返し
頻度とにより評価される。成るパルスが測定交流電圧の
周波数の各々の交番について現出された場合、多少とも
短かい期間内に絶縁を破壊するべき恒久的な現象が存在
する。その反対に、有害な・9ルスの繰返しs度が測定
5!:流電圧の1交番ごとに0.5又はそれ以下であれ
ば、そのパルスは、短期間内に絶縁の破壊をもたらすこ
とのない14@的なパルスないし不規則なパルスと兇る
ことができる。In place of the wave height voltmeter 9, a counter for harmful pulses may be used. Naru no! The harmfulness of a virus is evaluated by its size and repetition frequency. If a pulse consisting of the following occurs for each alternation of the frequency of the measured alternating current voltage, there is a permanent phenomenon that should break down the insulation within a more or less short period of time. On the contrary, the degree of repetition of harmful 9 russ is measured at 5! : If it is 0.5 or less for each alternation of current voltage, the pulse can be considered as a regular pulse or an irregular pulse that does not lead to breakdown of the insulation within a short period of time. .
有害なパルスの計数器は、この計at行う目的で、好ま
しくはgm可能な・−1直をもった人力段を有し、調節
0Tjfl!な閾値以下の強さの・平ルスのみがこの人
力段を通過する。他方ではこの計数器のサンブリング周
期は、測定電圧の周波数の50〜10005!IFの範
囲内に好ましくは選定される。For the purpose of this counting, the counter of harmful pulses preferably has a manual stage with gm possible -1 shift and adjustment 0Tjfl! Only Heirusu whose strength is below the threshold will pass through this human power stage. On the other hand, the sampling period of this counter is 50 to 10,005 times the frequency of the measured voltage! It is preferably selected within the range of IF.
測定時間を無用にひき延ばさな^ように、上記周期を1
000交醤よりも小さくすることが彎ましい、また迩断
器のオンオフ時などに回路中に生ずる寄生パルスに基づ
くノイズの影響を少くする目的で、50交番という上期
周期の最小値を遵守すべきである。To avoid unnecessarily prolonging the measurement time, set the above period to 1.
It is advisable to keep the value smaller than 000 alternations.Also, in order to reduce the influence of noise due to parasitic pulses that occur in the circuit when switching on and off the switch, it is recommended to observe the minimum value of the first half cycle of 50 alternations. Should.
測定寸法が、全測定範囲に対する単一の閾値の選択、各
々の測定電圧に対する閾値の相異なる一連の調節の選択
又は測定電圧の関数として、例え#−1′測定電圧に比
例するように選択された各々の測定電圧についての単一
の閾値の選択に存することがあり得る。The measurement dimensions may be selected such as the selection of a single threshold value for the entire measurement range, the selection of a series of different adjustments of the threshold value for each measurement voltage, or as a function of the measurement voltage, e.g. proportional to the #-1' measurement voltage. may consist in selecting a single threshold value for each measured voltage.
%に有利な測定方法は、波高電圧計による測定とノダル
ス計数器の測定との組合せによる方法である。その場合
閾値入力段のパルス計数器は、波高電圧計9に対し並列
に分路される。ノヤルス計数器の閾値は、波高電圧計に
印加されるパルスの最大振幅より少し小さな振幅の電圧
例えば#最大振幅の98〜80参の振幅の電圧に勢しぐ
なるようK、手動又は自動調節される。波高電圧計及び
ノヤルス計数器によって記帰されるそれぞれの測定債の
比較により、試験している機械の巻線の絶線破壊を4ま
たらし得ふ現象の最も信頼で舞る評価が可能になる。An advantageous measuring method for % is the combination of measurement with a pulse height voltmeter and measurement with a nodalus counter. The pulse counter of the threshold input stage is then shunted in parallel to the pulse height voltmeter 9. The threshold value of the Noyals counter is adjusted manually or automatically so that the voltage has an amplitude slightly smaller than the maximum amplitude of the pulse applied to the pulse height voltmeter, for example, a voltage with an amplitude of 98 to 80 cm of the maximum amplitude. Ru. Comparison of the respective measurement values recorded by the pulse height voltmeter and the Noyals counter allows the most reliable evaluation of the phenomena that can lead to failure of the windings of the machine under test.
上述した測定方法の利点け、内部放電の検出の場合にも
失われない、この内部放電の検出は、本発明による内部
放電についての測定方法の選択性により1表面放電又は
切欠放電のような他の性質の放電が存在する場合に本容
易になる。しかし成る測定電圧レベル以降では表面放電
と切欠放電とのうちどちらか一方又は両方によって内部
放電の測定がマスキングされる。しかしこれは絶縁の良
否を定めることのみが重要になる実際の場合には不つど
うではない、実際に良い状轄の絶縁は、使用電圧より低
い電圧及びそれより少し高い電圧において表面放電又は
切欠放電を示し得ない。The advantages of the measurement method described above are not lost even in the case of the detection of internal discharges, which, due to the selectivity of the measurement method for internal discharges according to the invention, can be used for detecting one surface discharge or another, such as a notch discharge. This becomes easier if there is a discharge of this nature. However, below the measurement voltage level, the measurement of internal discharges is masked by surface discharges and/or notch discharges. However, this is not indispensable in practical cases where it is only important to determine the quality of the insulation. cannot be shown.
波高電圧計9により測定された電圧値の増大が、内部放
電と表面放電と切欠放電とのうちのどれKより生じ喪か
を判定することもできる。実際に、測定電圧の関数とし
て波高電圧計9により測定され九電圧値の増大速度は最
大である1表ml放電の場合KF−1操作者は、特有の
オゾン臭を感仰し、表面放電によって生じた騒音を聞き
わけることができる。操作者が各々の測定において少し
手間取った場合には、%に高電圧においての表面放電の
繰返し鋼重は、少くとも1分以内に、1交番当り例えば
1放電から50交番当り1放*VCW少する。It is also possible to determine which of internal discharge, surface discharge, and notch discharge causes an increase in the voltage value measured by the wave height voltmeter 9. In fact, the rate of increase in the voltage value measured by the wave height voltmeter 9 as a function of the measured voltage is the highest.In the case of a 1ml discharge, the KF-1 operator was impressed by the characteristic ozone odor, and due to the surface discharge. I can hear the noises that occur. If the operator takes a little time in each measurement, the cyclic steel weight of surface discharges at high voltages in % may vary from e.g. 1 discharge per alternation to 1 discharge per 50 alternations*VCW less than do.
切欠放電が現出した場合には、騒音が聞き分けられたり
、オゾン臭が感じられたりするこ々けない、しかしいろ
いろの付帯的な表われから、*気機械の絶縁の絶縁耐力
の良否の評価に役立ち得る一連の特性的な現象を明らか
にすることができる、第4図は、本発明の検出装置によ
り析われたいろいろの測定曲線を重ね合せて示した線図
であり、すべての測定曲線について測定電圧H横軸にプ
ロットされ、いろいろの量の測定値は縦軸Kfプロット
れている。告白@により示されたtけ次の通りであゐ、
10ち曲1110H1電気機械の質量に対するコイル
の容量の相対的な増大、曲@11け絶縁のtgJ 、曲
線12Fi波高電圧針により測定された電圧値、曲線1
:lj有害なノダルスの計数量により計数された1交番
当りの放電数である0曲線10.11け絶縁欠陥を示さ
ないが1曲@12.13についてはそうで#′i々い、
1ull定している電気機械の公称電圧LJn よ
りも相当低い電圧において、振幅の小さな多数の内部放
電が波高電圧計によ妙測定され、はぼ各Rの交番におい
て現出されるが、測定電圧が増大するにつれて、より大
きな振幅の放電が発生し、それが波高電圧針により測定
され、計数器により記鐘される。これが曲1!13の減
少形状の理由である。しかし波高電圧計9により測定さ
れた放電の最大条幅は公称電圧のところで極大値管通過
する。曲、1112d公称電圧より少し高い電圧におい
てニーを示し、そのニーから、表面放電による増大曲線
部分が延長している。このニーに対応する測定電圧以降
については操作者はオゾン特有の臭気を感じるので、表
面放電が発生している。有害なパルスの計数器によシ測
定された放電の繰返し頻度は、2つの極大を示し、これ
らの極大は、表面放電を生ずるいくつかの小さな箇所が
成る高電圧以降は燃焼除去されたことを示している。最
も有害な内部放電が未だ偶発的性質しかもたず、を比表
面放電が機械の公称電圧よりも相当高い測定電圧のみに
おいて生ずることから、菓4図に従う曲線を有する絶縁
は、比較的良好と見ることができる。しかし曲線12の
極太点が公称電圧のところにあるという事実け、この絶
縁が比較的短かい期間ごとに検査されねばならないこと
を示している。When notch discharge appears, there are subtle but incidental manifestations such as audible noise and the smell of ozone. *Evaluation of the dielectric strength of mechanical insulation. FIG. 4 is a superimposed diagram of various measurement curves analyzed by the detection device of the present invention, which can reveal a series of characteristic phenomena that can be useful for The measured voltage H is plotted on the horizontal axis, and the measured values of various quantities are plotted on the vertical axis Kf. As indicated by the confession @,
10th track 1110H1 Relative increase in the capacitance of the coil to the mass of the electrical machine, curve @ tgJ of 11-insulation, curve 12Fi wave Voltage value measured by high voltage needle, curve 1
:lj The 0 curve, which is the number of discharges per alternating cycle counted by the counting amount of harmful nodalus, does not show insulation defects by 10.11, but the same is true for 1 song @12.13.
At voltages considerably lower than the nominal voltage LJn of the electrical machine, which is fixed at 1ull, a large number of internal discharges with small amplitudes are measured by a pulse-height voltmeter, appearing approximately at the alternation of each R, but the measured voltage As the voltage increases, a discharge of larger amplitude occurs, which is measured by the crest voltage needle and recorded by the counter. This is the reason for the decreasing shape of songs 1!13. However, the maximum width of the discharge measured by the wave height voltmeter 9 passes through the tube at a maximum value at the nominal voltage. Curve 1112d shows a knee at a voltage slightly higher than the nominal voltage, from which an increasing curve portion due to surface discharge extends. Since the operator senses the odor peculiar to ozone at the measured voltage corresponding to this knee, surface discharge occurs. The repetition frequency of the discharges, measured by a counter of harmful pulses, shows two maxima, which are burnt out after the high voltage, which consists of several small spots that give rise to surface discharges. It shows. Since the most harmful internal discharges are still only of an episodic nature and specific surface discharges occur only at measured voltages considerably higher than the nominal voltage of the machine, an insulation with a curve according to Figure 4 is considered relatively good. be able to. However, the fact that the thickest point of curve 12 is at the nominal voltage indicates that this insulation must be checked at relatively short intervals.
tIXs図に示した測定ブリッジは、第1図しζ示した
ものと類似しているが、その平衡辺にeゴ、%帽ノfル
ス又は電流を高選択度で測定するための籾数の測定II
P票(各々別の所定の#i11波数を通過させる)が含
まれている。これらの油1定要素は、1.2図について
既に説明した要素と同一でもよいが、そのほかに1例え
ば5QHz の測定電圧の回@(資)波数(商用周波数
)についてフィルター15に接続され圧変圧器14と、
平衡指示器として役立つオシログラフ指示!1gとして
もよい。The measuring bridge shown in the tIXs diagram is similar to the one shown in Figure 1, but with a number of grains on its equilibrium side for measuring the ego, % cap, or current with high selectivity. Measurement II
P votes (each passing a different predetermined #i11 wave number) are included. These oil constant elements may be the same as the elements already explained with respect to Figure 1.2, but in addition, they may also be connected to the filter 15 and connected to the filter 15 for the frequency of the measurement voltage (commercial frequency), for example 5QHz. Vessel 14 and
Oscillograph indication useful as an equilibrium indicator! It may be 1g.
波高電圧針9に接続されると共に可調節閾値の入力段1
+つた計数器10に並列に接続されている高選択性の変
圧器SFi、有害な部分放電の後縁の持続時間に対応す
る例えば100〜500 Hzの範囲内の周波数に感応
する。an input stage 1 connected to the peak voltage needle 9 and with an adjustable threshold;
A highly selective transformer SFi, connected in parallel to the counter 10, is sensitive to frequencies, for example in the range from 100 to 500 Hz, corresponding to the duration of the trailing edge of the harmful partial discharge.
変圧器18.可費利得のlテンシミメーター19、例え
ば200〜800Hz の範囲内Ktすれる商用−波数
の戚る整倍倍に*Lい所定m波数について高選択性のフ
ィルター20及び容量入力段増幅1)21からなる別の
測定要素は、波高電圧計22に接続されている。これけ
イオンll11:又は可動賓に関連した現象の検出に用
いられる。波高電圧計22Fi、 fi高電圧計9が適
当な測定範囲の好ましくけ自動式の選択器を備えていれ
ば、波高電圧計9と同一のものでもよい。これらの検出
回路を次々に回路に入れるのけ、第1図に示すように接
続したスイッチ6又けf85図に示すように接続した2
傭の可動接点つきのスイッチ6.6’により、第1図に
ついて説明したように行われる。Transformer 18. A tensimeter 19 with an expensable gain, e.g. commercially available with Kt in the range 200-800 Hz - a filter 20 with high selectivity for a given m wavenumber and a capacitive input stage amplifier 1) Another measuring element consisting of 21 is connected to a peak voltmeter 22. This ion ll11: Or used to detect phenomena related to moving guests. The wave height voltmeter 22Fi may be the same as the wave height voltmeter 9, as long as the fi high voltmeter 9 is preferably equipped with an automatic selector for an appropriate measurement range. In order to insert these detection circuits one after another into the circuit, 6 switches are connected as shown in Figure 1, and 2 switches are connected as shown in Figure 85.
By means of a switch 6.6' with a separate movable contact, this is carried out as explained in connection with FIG.
成る場合に汀、変圧flag、14.18の1次側を恒
久的に直列に平衡辺(II数)中に接続し、可動スイッ
チ6′のみにより測定の選択1行なってもよい。In this case, the primary side of the voltage transformer flag 14.18 may be permanently connected in series to the balanced side (number II), and one measurement selection line may be performed using only the movable switch 6'.
!圧器18、Iテンシミメーター19.フィルター20
及び増幅器21からなる測定要素について以下に詳述す
る。変圧器18は恒久的に平衡辺に分路させてよ(、選
択された周波数においての測定要素の選択性がそれによ
り失われることけない、実際に商用周波数においては抵
抗日が4テンシヨメーター19の中間タッグに入れられ
、その先端は、増幅器の入力段中にあるコンデンサーの
インピーダンスに比べて小さい、それに反し、選択され
た周波数においてはこの抵抗R#′i増幅器21の入力
段中のコンデンサーCのインピーダンスに比べて小さい
。そのため商用同波数よりも著しく高い周波数について
のフィルター20の場合、増幅器21の応答は、平衡辺
の端子電圧に比例せず、平衡辺t−流れる電流に比例す
る。W流に、電気機械に印加された交流測定電圧によっ
て電気機械の絶轍部中t11動すゐイオンにより生じ、
波高電圧計22によp検知される測定電圧?生成させる
。! Pressure gauge 18, I tensimeter 19. filter 20
The measuring element consisting of the amplifier 21 and the amplifier 21 will be explained in detail below. The transformer 18 is permanently shunted to the balanced side (so that the selectivity of the measuring element at the selected frequency is not thereby lost; in fact at commercial frequencies the resistance is 4 tensiometers). 19, whose tip is small compared to the impedance of the capacitor in the input stage of the amplifier, whereas at the selected frequency this resistor R#'i Therefore, in the case of the filter 20 for a frequency significantly higher than the commercial frequency, the response of the amplifier 21 is not proportional to the terminal voltage on the balanced side, but proportional to the current flowing through the balanced side t. In the W flow, caused by ions moving in the isolated part of the electric machine due to the alternating current measuring voltage applied to the electric machine,
The measured voltage p detected by the wave height voltmeter 22? Generate.
商用−波数において測定電圧Uの関数として波高電圧針
22により検知される電圧Vの曲@230例が第6図に
示されている。 Un は電気機械の公称電圧である。An example of the curve @230 of the voltage V detected by the peak voltage needle 22 as a function of the measured voltage U in the commercial wavenumber is shown in FIG. Un is the nominal voltage of the electrical machine.
曲線の形状は、低電圧側では、2つの隣接する障壁の間
の可動イオンの密度と、これらのイオンの可動度従って
一方の障壁から他の障壁へのこれらのイオンの走行時間
とによって主に定まる。これら2つの量の積は、増大曲
線部分に始まって最大値を通過し漸近的にWLルベルに
至る曲線23の形状を宇める。その後の第2レベルは、
新しいea部の場合、高電圧の影響の下においての成る
種の錯体の解離と電荷による局所電解の成立によるイオ
ン濃度の増大によって説明される。すべての絶縁部につ
いて、閾値電圧Us 以後に、絶縁の破11に先行する
繊細電流が上記局所電界のために発生し、この電流発生
け、波高電圧計22により測定された電圧の指数関数的
増大の開始により説明される。この電圧増大開始以降は
試験は中止しなければならない。The shape of the curve, on the low voltage side, is mainly determined by the density of mobile ions between two adjacent barriers and the mobility of these ions and hence the transit time of these ions from one barrier to the other. Determined. The product of these two quantities determines the shape of the curve 23, starting from the increasing curve section, passing through the maximum value and asymptotically reaching the WL level. After that, the second level is
In the case of the new ea part, it is explained by the dissociation of the complexes of the species under the influence of high voltage and the increase in the ion concentration due to the formation of local electrolysis due to the charge. For all insulation parts, after the threshold voltage Us, a delicate current is generated due to the local electric field, which precedes the breakdown of the insulation 11, and this current generation causes an exponential increase in the voltage measured by the wave height voltmeter 22. This is explained by the beginning of . The test shall be discontinued after this voltage increase begins.
波高電圧計22に測定のために選定される同波数は、測
定に対する印加電圧の直接の影響を回避するために、商
用周波数と異なった値とすべきである。他方では可動イ
オンは、障壁間の空間中においての各々の可動闇に対応
する連間で、 15111定交流電圧により各々移動さ
れるので、ブリツノ平衡道中Kit起される電流は、測
定電圧がそれから導出されたところの回線め周波数(商
用周波数)の整数倍に郷しい周波数の交流電流(置数)
を重畳したものからなる。しかしω=−(ここKTけ、
2つの隣接障壁間の可動イオンの平均走行時間である)
に等しい[波数についてけwtltのS幅は零になる。The same wave number selected for measurement by the wave height voltmeter 22 should be different from the commercial frequency to avoid direct influence of the applied voltage on the measurement. On the other hand, the mobile ions are each moved by a constant alternating voltage in the space between the barriers in the space corresponding to each mobile ion, so that the current induced during the Britno equilibrium path is such that the measured voltage is derived from it. Alternating current (number) with a frequency that is an integral multiple of the line frequency (commercial frequency)
Consists of a superposition of . But ω=-(KT here,
is the average transit time of a mobile ion between two adjacent barriers)
[The S width of wtlt becomes zero with respect to the wave number.
そのため、商用周波数よりも光分高い商用8波数の整数
倍に#I、(’且つwR波数−より相当低い周波数、実
際Ktf 200〜800 H2の(資)波数を通過さ
せるフィルター201−便用すふ。Therefore, the filter 201 is used to pass the wave number #I, which is an integer multiple of the commercial 8 wave number which is higher than the commercial frequency by an amount of light, and the frequency considerably lower than the wR wave number, in fact KTF 200 to 800 H2. debt.
曲線23により、新しい?3縁部の場合Klt気機械の
作用の許容限界電圧を定めることを可能にする繊細電流
の開始及びイオン濃度による2つのしペルを見出すこと
ができるため、絶一部の正常さについての補助的な計画
が得られる。古い絶縁部の場合Kに、使用されたプラス
チック桐料の脱型台などにより、イオンの接続時間が更
に長くなる。By curve 23, new? In the case of three edges, we can find two thresholds due to the onset of the delicate current and the ion concentration, which makes it possible to determine the permissible limit voltage for the operation of the Klt-air machine, so that it is possible to find an auxiliary explanation about the normality of the absolute part. You can get a good plan. In the case of old insulating parts, the ion connection time becomes longer due to the mold removal table of the plastic paulownia material used.
そのため電圧Us ij減少し、第2のレベルは生じ得
ない。Therefore, the voltage Us ij decreases and the second level cannot occur.
第1図は本発明の一実施例による測定ブリッジの電気回
路図、第2図は本発明の別の実施例による測定ブリッジ
の電気(司略図、第3図1n/4ルス妓形図、第4図F
i 11圧波形図、第5図は本発明の別の実施例シてよ
る測定プリツノの電気回路図、躯6図は第5図に対応す
る重圧ffI影図である。
符号の説明
7・・・平衡指示器、8・・・高S波賛圧器(測定装置
)、9.22・・・波高電圧計(測定値W7t)、14
゜18・・・変圧器(測定値fi)、15・・・フィル
ター(+III)定M# ) 、 16・・・オシログ
ラフ指示器(測定値!11)、20・・・高選択性フィ
ルター(御;電装fi11)。
21・・・増幅器(測定装置)
代理人
弁理士 中 村 捻回 山
本 部同 串
岡 八 即問 大 塚 文
開園 宍 戸 嘉 −
手 続 禎 IF 書(方式)
昭和57年特 許 +1J1 第70159号3、補
正をする者
事件との関係 山−人
4、代理人1 is an electrical circuit diagram of a measuring bridge according to an embodiment of the invention, FIG. 2 is an electrical schematic diagram of a measuring bridge according to another embodiment of the invention, and FIG. Figure 4F
i11 pressure waveform diagram, FIG. 5 is an electric circuit diagram of a measurement circuit according to another embodiment of the present invention, and FIG. 6 is a heavy pressure ffI shadow diagram corresponding to FIG. Explanation of symbols 7... Balance indicator, 8... High S wave pressure booster (measuring device), 9.22... Wave height voltmeter (measured value W7t), 14
゜18...Transformer (measured value fi), 15...Filter (+III) constant M#), 16...Oscillograph indicator (measured value! 11), 20...High selectivity filter ( control; electric equipment fi11). 21...Amplifier (measuring device) Representative Patent Attorney Nakamura Nerui Yama
Honbu Dokushi
Oka Hachi Immediate Question Aya Otsuka Opening Shishi To Yoshi −
Procedure Tei IF document (method) 1984 patent +1J1 No. 70159 No. 3, Relationship with the case of the person making the amendment Yamato 4, Agent
Claims (1)
巻線の周囲に配設され良電気機械O貿量部分とを接続し
、所定の電圧範囲内において堆っ大台々の測定交流電圧
について、測定ブリッジを平衝させ、交流電圧の周波数
は電気機械の使用条件においてl1lK生ずる周波数の
中から選ぶことにより、電気機械の巻線の絶縁の不充分
な絶縁耐力を検出する方法において、成る1つの所定の
周波数を通過させる電流・ダルス又は電#IO高選択4
&測定装置8.9又は各々が異なる所定の周波数を通過
させる電流パルス又は電流の高選択性の複数Oill
j!値装14,15,16:8.9:17.18.20
.21.22を相前後させて、平衡指示器7に代わるよ
うK、測定ブリッジの平衡対角辺中に配設する仁とと、
使用電圧よ抄も低い値と電気機械の最大許容電圧に等し
いか又はこれより高い値との間において、[定電圧の値
をスイープすることとを特徴とする検出方法。 (2)高選択性の測定装置の1つが、OSの絶縁中0部
分放電による振幅に対応する振幅並びに巻IIO絶II
O内部に起こる局所部分放電の平均電流の後III、0
持続時間に対応するように1足され九周波数を通過させ
るようにすることを特徴とする特許請求の範囲111(
1)項記載の検出方法。 (3)高選択性の測定装置の1つが、測定電圧の周波数
0**倍に等しいように選定壊れた、該測定電圧の周波
数よ抄も相当高く且つ周波数−(■ ここにTは2つの障壁間のイオンO平均走行時間である
)よ#)4相i低い周波数を通過させるようにすること
を特徴とする特許請求の範囲第(1)項記載の検出方法
。 (4)複数の抵抗とコンデンサーとを含む容量測定ブリ
ッジ0III定対角辺中に配設し九平衡指示器7を1選
択装置6と直列に4111L、また複数の電流パルス又
は電流の周波数についての11[1以上の高選択性測定
要素と並列に接続し良ことを特徴とする特許請求の範囲
第(1)項から第(3)項までのうちいずれか1項記載
の検出方法を実施する丸めの検出装置。 (5)複数の成る電流パルス又は電流の周波数について
高選択性の測定装置が巻線の絶縁内部の局所部分放電に
より生じ食・櫂ルスに対応する振幅及び周波数に感応す
るようにし九ことを特徴とする特許請求の範囲第(4)
項記載の検出装置。 16)電流パルスの所定振幅の測定装置が成る周波数に
対し高選択性の変圧器8を含むことを特徴とする特許請
求の範囲第(5)項記載の検出装置。 ())高選択性の変圧lI8が可飽和の変圧器であるこ
とを1tlI徽とする特許請求の#Il!l第(6)項
記載の検出装置。 (8) 電flAルス又は電流の所定振幅O測定装置
が波高電圧針であ抄、この波高電圧針はそれに加わる電
流パルス又は電流の最大の波高の振幅を測定することを
特徴とする特許請求の範囲第(6)項記載の検出装置。 (9)電RΔルスの所定振幅の測定装置が、所定サンプ
リング周期を含み、成る閾値振幅以上の・ヤルスを通過
させる人力段により前置され九計数器であることを特徴
とする特許請求の範囲第(5)項から第())項までの
うちいずれか1gi記鐵の検出装置。 a@ サンプリング周期を測定電圧の周波数の50〜1
000交番の範囲に定め良ことを特徴とする特許請求の
範囲第(9)項記載の検出装置。 α力 所定振幅O測定装置を、成る閾値振幅以上のパル
スを通過させる入力段を前置した波高電圧針と計数器と
の並列回路により形成したことを特徴とする特許請求O
SS第(8)項からg舖項まてのうちいずれか1項記載
の検出装置。 (ロ)波高電圧計において測定された電圧値の関数とし
て動作する計数器の人力部に閾値調節装置を配設し友こ
とを特徴とする特許請求の範囲第a事項記載の検出装置
。 (ロ)高選択性0III定装置が、測定周波数よりも相
当に高く周波数−=−(ことKTは2つの隣接■ 障壁間の可動イオノ0平均走行時間である)よりも相当
に低い咳測定周波数の成る整数倍に感応するようにした
ことを特徴とする特許請求の範i!!第(4)項記載の
検出装置。[Claims] α) During the measurement path of the capacitance measuring bridge, the winding 0 conductor and
The measuring bridge is placed around the winding and connected to a good electrical machine, and the frequency of the alternating voltage is In a method for detecting insufficient dielectric strength of the insulation of the windings of an electrical machine by selecting from among the frequencies occurring in the conditions of use of the machine, a current dulse or voltage passing one predetermined frequency consisting of High selection 4
& Measuring device 8.9 or a plurality of highly selective oils of current pulses or currents each passing a different predetermined frequency.
j! Price tag 14, 15, 16: 8.9: 17.18.20
.. 21 and 22 one after the other, K to replace the balance indicator 7, and a holder arranged in the balance diagonal side of the measuring bridge;
A detection method characterized by sweeping the value of a constant voltage between a value lower than the working voltage and a value equal to or higher than the maximum permissible voltage of the electric machine. (2) One of the highly selective measurement devices can measure the amplitude corresponding to the amplitude due to the zero partial discharge in the insulation of the OS as well as the winding IIO and the winding II
After the average current of local partial discharges occurring inside O III, 0
Claim 111(
Detection method described in section 1). (3) One of the highly selective measuring devices is selected so that the frequency of the measured voltage is equal to 0** times the frequency of the measured voltage, and the frequency of the measured voltage is also quite high and the frequency - (■ Here T is two times 2. The detection method according to claim 1, wherein the average transit time of ions between the barriers is passed. (4) A capacitance measuring bridge 0III containing a plurality of resistors and capacitors is disposed in the constant diagonal side, and nine balance indicators 7 are connected in series with one selection device 6 4111L, and a plurality of current pulses or current frequency 11 [Implementing the detection method according to any one of claims (1) to (3), which can be connected in parallel with one or more highly selective measurement elements. Rounding detection device. (5) characterized in that the measuring device is highly selective with respect to the frequency of the current pulses or currents and is sensitive to the amplitude and frequency corresponding to the eclipses caused by local partial discharges within the insulation of the winding; Claim No. (4)
Detection device described in section. 16) Detection device according to claim 5, characterized in that it comprises a transformer 8 with high selectivity for the frequency of which the device for measuring the predetermined amplitude of the current pulse is comprised. ()) #Il of the patent claim in which the highly selective transformer II8 is a saturable transformer! 1. The detection device according to item (6). (8) The device for measuring the predetermined amplitude of the electric flA pulse or current is formed by a wave-high voltage needle, and the wave-high voltage needle measures the amplitude of the maximum wave height of the current pulse or current applied thereto. Detection device according to scope item (6). (9) The device for measuring the predetermined amplitude of the electric RΔrus includes a predetermined sampling period and is a nine counter preceded by a manual stage that passes the RΔrus with a threshold amplitude or more. A detection device according to any one of paragraphs (5) to ()). a@ The sampling period is 50 to 1 of the frequency of the measuring voltage.
The detection device according to claim (9), characterized in that the detection device can be set within a range of 000 police boxes. A patent claim O characterized in that the alpha force predetermined amplitude O measuring device is formed by a parallel circuit of a pulse voltage needle and a counter, which is preceded by an input stage through which pulses having an amplitude equal to or greater than a threshold value are passed.
The detection device according to any one of SS paragraphs (8) to g. (b) The detection device according to item (a) of the claims, characterized in that a threshold value adjustment device is disposed in the manual section of the counter that operates as a function of the voltage value measured by the wave height voltmeter. (b) The high selectivity 0III constant device has a cough measurement frequency that is considerably higher than the measurement frequency and considerably lower than the frequency -=- (where KT is the average transit time of the movable ion between two adjacent barriers). Claim i! is sensitive to an integer multiple of ! ! Detection device according to paragraph (4).
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| BE888875 | 1981-05-20 | ||
| BE888875 | 1981-05-20 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS58769A true JPS58769A (en) | 1983-01-05 |
Family
ID=3861925
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57070159A Pending JPS58769A (en) | 1981-05-20 | 1982-04-26 | Method of detecting dielectric resistance, insulation thereof is insufficient, of electrodynamic machine winding |
Country Status (2)
| Country | Link |
|---|---|
| JP (1) | JPS58769A (en) |
| BE (1) | BE888875A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101738567B (en) * | 2008-11-25 | 2012-05-30 | 上海市电力公司 | The Method of Using Constant Current Sweep Frequency Power Supply to Excite and Detect the State of Transformer Winding |
-
1981
- 1981-05-20 BE BE1/10227A patent/BE888875A/en not_active IP Right Cessation
-
1982
- 1982-04-26 JP JP57070159A patent/JPS58769A/en active Pending
Also Published As
| Publication number | Publication date |
|---|---|
| BE888875A (en) | 1981-11-20 |
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