JPS5930490Y2 - Electric charge measuring device for transformer insulating oil - Google Patents

Electric charge measuring device for transformer insulating oil

Info

Publication number
JPS5930490Y2
JPS5930490Y2 JP2035380U JP2035380U JPS5930490Y2 JP S5930490 Y2 JPS5930490 Y2 JP S5930490Y2 JP 2035380 U JP2035380 U JP 2035380U JP 2035380 U JP2035380 U JP 2035380U JP S5930490 Y2 JPS5930490 Y2 JP S5930490Y2
Authority
JP
Japan
Prior art keywords
transformer
probe
oil
charge
electrode
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
Application number
JP2035380U
Other languages
Japanese (ja)
Other versions
JPS55149923U (en
Inventor
新一 毛受
正己 本多
仁 大久保
Original Assignee
株式会社東芝
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 株式会社東芝 filed Critical 株式会社東芝
Priority to JP2035380U priority Critical patent/JPS5930490Y2/en
Publication of JPS55149923U publication Critical patent/JPS55149923U/ja
Application granted granted Critical
Publication of JPS5930490Y2 publication Critical patent/JPS5930490Y2/en
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 この考案は強制送油冷却型の変圧器の絶縁油中に蓄積さ
れた電荷量を測定する装置に関する。
[Detailed Description of the Invention] This invention relates to a device for measuring the amount of charge accumulated in the insulating oil of a forced oil cooling type transformer.

大型の大容量変圧器に於ては変圧器絶縁油(以下変圧器
油という)を電動ポンプで冷却器を通して高速循環させ
変圧器の巻線を冷却している。
In large, large-capacity transformers, transformer insulating oil (hereinafter referred to as transformer oil) is circulated at high speed through a cooler using an electric pump to cool the transformer windings.

一方変圧器油はそれ自身が非常に良い絶縁物であるため
に、変圧器の巻線及び鉄心並びに冷却器の内面に接触し
て高速で通過するときに摩擦電気を生ずることがあり、
これによって変圧器油中に電荷が蓄積されることがあり
、且この電荷は四散しにくい状態におかれる。
On the other hand, since transformer oil itself is a very good insulator, it can generate triboelectricity when it comes into contact with the transformer windings and core as well as the inner surface of the cooler and passes through it at high speed.
This may cause charge to accumulate in the transformer oil, and this charge is placed in a state where it is difficult to dissipate.

即ち更に詳説すると、変圧器油は1013〜1014.
Qcmの高い体積抵抗率を有しており、変圧器の構成物
との接触摩擦により多量の電荷を発生することがある。
That is, to explain in more detail, the transformer oil is 1013 to 1014.
It has a high volume resistivity of Qcm, and can generate a large amount of electric charge due to contact friction with transformer components.

そしてこの電荷は変圧器油の高い体積抵抗率のために四
散せず次第に油中に蓄積され一種の空間電荷として存在
したり、あるいは内部絶縁物の表面などに偏在したりし
て最終的には相当の電荷量即ち電圧値に達することとな
り、これが限界値をこえると内部放電や絶縁破壊を引き
おこすことになる。
Due to the high volume resistivity of the transformer oil, this charge is not dispersed but gradually accumulates in the oil and exists as a kind of space charge, or it is unevenly distributed on the surface of internal insulators and eventually A considerable amount of charge, ie, a voltage value, will be reached, and if this exceeds a limit value, internal discharge or dielectric breakdown will occur.

このような現象は大容量変圧器などのように変圧器油を
大量に使用し、しかも冷却のために強制的に流動させて
いる機器においてはもはや無視できなくなってきた。
This phenomenon can no longer be ignored in equipment such as large-capacity transformers that use a large amount of transformer oil and are forced to flow for cooling purposes.

然しなから、これまで油入変圧器においてはその流動帯
電現象ははっきりつかめていなかった事などの理由によ
り変圧器油の帯電に関するなんらの対策も考慮されてい
なかった。
However, for reasons such as the fact that the flow charging phenomenon in oil-immersed transformers has not been clearly understood, no countermeasures have been taken to prevent charging of transformer oil.

そこで、変圧器油中に電荷検出プローブの一端を侵し、
このプローブの端と変圧器油とをほぼ等電位とし、この
プローブの電位を検出することにより変圧器油中の電荷
量を求めることが考えられる。
Therefore, one end of the charge detection probe was immersed in the transformer oil.
It is conceivable to make the end of this probe and the transformer oil approximately equal potential, and to determine the amount of charge in the transformer oil by detecting the potential of this probe.

すなわち、第1図において、11は変圧器タンクで内部
に変圧器本体12及び変圧器油13を収納している。
That is, in FIG. 1, 11 is a transformer tank which houses a transformer body 12 and transformer oil 13 inside.

変圧器油13は変圧器本体12の巻線12 a及び鉄心
12 bを冷却して上昇し、変圧器タンク11の図示し
ない上部開口から冷却器14に流入して冷却され再び変
圧器タンク11内に下部開口11aから流入する循環系
路を流れる。
The transformer oil 13 cools the windings 12a and the iron core 12b of the transformer body 12, rises, flows into the cooler 14 from the upper opening (not shown) of the transformer tank 11, is cooled, and returns to the inside of the transformer tank 11. The water flows through a circulation path that flows into the lower opening 11a.

この変圧器油13の循環は冷却器14及び変圧器タンク
11の下部開口11 aの途中に設けられたポンプ15
により強制的に行われる。
The circulation of the transformer oil 13 is carried out by a cooler 14 and a pump 15 provided midway through the lower opening 11a of the transformer tank 11.
This will be done forcibly.

16・・・・・・は冷却器14、ポンプ15及び変圧器
タンク11を連通ずる配管である。
16... are piping that connect the cooler 14, the pump 15, and the transformer tank 11.

このような変圧器において、高速で流動する変圧器油1
3が配管16・・・・・・、内部絶縁物等との間で接触
、摩擦を生じ帯電し変圧器油13中に電荷が蓄積すると
、この電荷量は配管16に設けたプローブ17を介して
測定される。
In such a transformer, transformer oil 1 flowing at high speed
3 comes into contact with the piping 16, internal insulators, etc., causing friction and charging, and when electric charge accumulates in the transformer oil 13, this amount of electric charge is transferred via the probe 17 installed in the piping 16. It is measured by

この部を第2図を参照して更に詳細に説明する。This section will be explained in more detail with reference to FIG.

プローブ17は検出端が銅等の良導体で形成されたロッ
ド17 aとその先端に取付けられた球状電極17bと
で構成され、球状電極17 bは変圧器油13中に配設
される。
The probe 17 is composed of a rod 17a whose detection end is made of a good conductor such as copper and a spherical electrode 17b attached to the tip thereof, and the spherical electrode 17b is disposed in the transformer oil 13.

このプローブ17のロッド17 aはテフロンとして市
販されている高抵抗絶縁物の蓋18によって配管16の
開口を貫通して絶縁支持される。
The rod 17a of this probe 17 is insulated and supported by a lid 18 made of a high-resistance insulator commercially available as Teflon and passed through the opening of the pipe 16.

絶縁物の蓋18は配管16に形成されたプローブ取付は
用フランジ19にボルト及びナラ) 20により油密に
取付けられる。
The insulating lid 18 is oil-tightly attached to the probe mounting flange 19 formed on the pipe 16 with bolts and nuts 20.

プローブ17のロッド17 aの外部端子17 Cはブ
ローブリード線21を介してコンデンサCを形成する一
方の電極となるアルミ導電板22に接続され、プローブ
23の他方の電極23は超大入力インピーダンスを持つ
電位計24に接続される。
The external terminal 17C of the rod 17a of the probe 17 is connected via a blow bleed wire 21 to an aluminum conductive plate 22 which becomes one electrode forming a capacitor C, and the other electrode 23 of the probe 23 has an extremely large input impedance. It is connected to an electrometer 24.

このように構成された電荷量測定装置に於てはプローブ
17が外部に対して絶縁されているために絶縁油中とプ
ローブ17とはほぼ等電位になる。
In the charge amount measuring device configured in this manner, the probe 17 is insulated from the outside, so that the insulating oil and the probe 17 have approximately the same potential.

そこでプローブロッド17 aの電位をブローブリード
線21を介してアルミ導体板22に導き、ここで一定の
容量Cを介して電位計24により測定することができる
Therefore, the potential of the probe rod 17a is guided through the blow bleed wire 21 to the aluminum conductor plate 22, where it can be measured by the electrometer 24 through a certain capacitance C.

今例えば絶縁油中の電荷が(刊であYばアルミ導体板2
2は(ト)、プローブ電極23は(−)になるので、電
位計24は(ト)の電位値を表示し、また逆に電荷が(
→の場合は(→の電位値が表示される。
For example, if the electric charge in the insulating oil is
2 becomes (g) and the probe electrode 23 becomes (-), so the electrometer 24 displays the potential value of (g), and conversely, the electric charge becomes (g).
In the case of →, the potential value of (→ is displayed.

そしてこの電位値により電荷密度を求めれば変圧器油中
の電荷量を測定することができる。
Then, by determining the charge density from this potential value, the amount of charge in the transformer oil can be measured.

そして、この測定は周囲の影響をさけるためにシールド
ボックス25あるいはシールドルームで行なうことが好
ましい。
This measurement is preferably performed in the shield box 25 or in a shield room to avoid the influence of the surroundings.

以上のように変圧器油中の電荷量及び極性を測定するた
めにはプローブによって測定すればよいが、その際にシ
ールドボックスを使用したり測定器を校正したりしてい
ては変圧器の保守上不便である。
As mentioned above, in order to measure the amount of charge and polarity in transformer oil, it is sufficient to measure it with a probe, but if a shield box is used or the measuring device is calibrated at that time, it is difficult to maintain the transformer. This is extremely inconvenient.

本考案は上述の点を考慮したもので、変圧器絶縁油の電
荷量をシールドケース等を用いずに簡単に測定できる装
置を得ることを目的とする。
The present invention takes the above-mentioned points into consideration, and aims to provide a device that can easily measure the amount of charge in transformer insulating oil without using a shield case or the like.

以下本考案の一実施例を図面を参照して説明する。An embodiment of the present invention will be described below with reference to the drawings.

即ち、第3図に示すようにプローブの外部端子17 C
をブローブリード線21を介してガス密閉容器27内に
収納された電極組立26の一方の電極26 aに接続し
、電極組立26の他方の電極26 bを電流検出器28
を介して接地した装置を用いる。
That is, as shown in FIG.
is connected to one electrode 26a of an electrode assembly 26 housed in a gas-tight container 27 via a blow bleed wire 21, and the other electrode 26b of the electrode assembly 26 is connected to a current detector 28.
Use equipment that is grounded through the

この場合、プローブの電位がある予定の電位に達したと
きに電極組立25のギャップが絶縁破壊するように設定
しておけば変圧器油中の電荷がある値に達した時に絶縁
破壊が生じて電流検出器28に信号が表われることにな
る。
In this case, if the gap in the electrode assembly 25 is set so that dielectric breakdown occurs when the potential of the probe reaches a certain predetermined potential, dielectric breakdown will occur when the charge in the transformer oil reaches a certain value. A signal will appear on current detector 28.

従ってこの信号を利用して油中の電荷の量を自動的に検
出するようにすれば、きわめて簡単に電荷量が測定でき
るとともにシールドボックス等を用いることがないので
保守の手数を低減することができる。
Therefore, if this signal is used to automatically detect the amount of charge in oil, the amount of charge can be measured extremely easily, and maintenance work can be reduced since there is no need to use a shield box. can.

尚、上記実施例においては冷却器配管系統または変圧器
内部に電荷量測定装置を設ける場合について説明したが
冷却器の前後、ポンプの前後あるいは変圧器タンクの上
部と下部のように変圧器油循環系統の上流及び下流にそ
れぞれ電荷測定装置を設けて測定値の相対比較をすれば
冷却器、ポンプあるいは変圧器本体中での電荷の発生量
をそれぞれ測定することができる。
In the above embodiments, the charge measurement device is installed in the cooler piping system or inside the transformer, but it is also used in the transformer oil circulation system, such as before and after the cooler, before and after the pump, or at the top and bottom of the transformer tank. By installing charge measuring devices upstream and downstream of the system and making a relative comparison of the measured values, it is possible to measure the amount of charge generated in the cooler, pump, or transformer body.

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

第1図は変圧器絶縁油の電荷量を測定する装置の一実施
例を示す一部破断断面図、第2図は第1図の要部を拡大
して示す部分図、第3図は本考案の一実施例による電荷
量測定装置を示す断面図、第4図は本考案の他の実施例
を示す断面図、第5図はその側面図である。 17・・・・・・プローブ、18・・・・・・絶縁物、
22.23・・・・・・電極、24・・・・・・電位計
、C・・・・・・コンデンサ、26・・・・・・電極組
立、27・・・・・・ガス密閉容器、28・・・・・・
電流検出器。
Figure 1 is a partially cutaway cross-sectional view showing an embodiment of a device for measuring the amount of charge in transformer insulating oil, Figure 2 is a partial view showing an enlarged main part of Figure 1, and Figure 3 is a partial view of the main part of Figure 1. FIG. 4 is a sectional view showing another embodiment of the invention, and FIG. 5 is a side view thereof. 17...Probe, 18...Insulator,
22.23... Electrode, 24... Electrometer, C... Capacitor, 26... Electrode assembly, 27... Gas sealed container. , 28...
Current detector.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 変圧器絶縁油の循環系統の少なくとも一部に設けた開口
を閉じる高抵抗絶縁物の蓋と、この蓋を貫通して油中に
置かれる一端を持つプローブと、このプローブの外部端
子に接続された第1の電極及びこの電極から離しておか
れた第2の電極を有する電極組立と、電極組立の第2の
電極及び大地間に接続された電流検出器とからなる変圧
器絶縁油の電荷量測定装置。
A high-resistance insulating lid that closes an opening provided in at least a portion of a transformer insulating oil circulation system, a probe having one end that passes through the lid and is placed in the oil, and a probe that is connected to an external terminal of the probe. an electrode assembly having a first electrode spaced apart from the second electrode; and a current detector connected between the second electrode of the electrode assembly and ground. Quantity measuring device.
JP2035380U 1980-02-21 1980-02-21 Electric charge measuring device for transformer insulating oil Expired JPS5930490Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2035380U JPS5930490Y2 (en) 1980-02-21 1980-02-21 Electric charge measuring device for transformer insulating oil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2035380U JPS5930490Y2 (en) 1980-02-21 1980-02-21 Electric charge measuring device for transformer insulating oil

Publications (2)

Publication Number Publication Date
JPS55149923U JPS55149923U (en) 1980-10-29
JPS5930490Y2 true JPS5930490Y2 (en) 1984-08-31

Family

ID=28851165

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2035380U Expired JPS5930490Y2 (en) 1980-02-21 1980-02-21 Electric charge measuring device for transformer insulating oil

Country Status (1)

Country Link
JP (1) JPS5930490Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010118242A (en) * 2008-11-12 2010-05-27 Sumitomo Chemical Co Ltd Bodily sensing device of flow electrification, and experiment method for bodily sensing flow electrification

Also Published As

Publication number Publication date
JPS55149923U (en) 1980-10-29

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