JPH02167484A - Measuring method for partial discharge - Google Patents
Measuring method for partial dischargeInfo
- Publication number
- JPH02167484A JPH02167484A JP32277088A JP32277088A JPH02167484A JP H02167484 A JPH02167484 A JP H02167484A JP 32277088 A JP32277088 A JP 32277088A JP 32277088 A JP32277088 A JP 32277088A JP H02167484 A JPH02167484 A JP H02167484A
- Authority
- JP
- Japan
- Prior art keywords
- electrodes
- calibration
- partial discharge
- detection
- connection part
- 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.)
- Granted
Links
- 238000000034 method Methods 0.000 title claims description 12
- 238000001514 detection method Methods 0.000 claims abstract description 29
- 125000000391 vinyl group Chemical group [H]C([*])=C([H])[H] 0.000 claims abstract description 14
- 229920002554 vinyl polymer Polymers 0.000 claims abstract description 14
- 230000035945 sensitivity Effects 0.000 claims abstract description 7
- 239000003990 capacitor Substances 0.000 abstract description 10
- 239000004020 conductor Substances 0.000 abstract description 10
- 238000009413 insulation Methods 0.000 abstract 3
- 239000002184 metal Substances 0.000 description 19
- 238000010586 diagram Methods 0.000 description 6
- 230000000694 effects Effects 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 230000002238 attenuated effect Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 239000013256 coordination polymer Substances 0.000 description 1
- 238000005260 corrosion Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 235000021419 vinegar Nutrition 0.000 description 1
- 239000000052 vinegar Substances 0.000 description 1
Landscapes
- Testing Relating To Insulation (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は電カケープル線路の絶縁接続部における部分放
電測定方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a method for measuring partial discharge in an insulated connection part of a power cable line.
第4図(a)は従来の部分放電測定方法を示す。電カケ
ープル21が絶縁接続部20を介して接続されており、
両端に終端接続部22が設けられている。終端接続部2
2には高電圧課電端子23が設けられており、絶縁接続
部20の近傍の金属シースは検出インピーダンス6を介
してアースされている。検出インピーダンス6の両端の
電位差を検出するために測定器7が接続されている。尚
、CKは結合コンデンサである。FIG. 4(a) shows a conventional partial discharge measuring method. A power cable 21 is connected via an insulated connection part 20,
Terminal connection portions 22 are provided at both ends. Termination connection part 2
2 is provided with a high voltage charging terminal 23, and the metal sheath near the insulated connection portion 20 is grounded via a detection impedance 6. A measuring device 7 is connected to detect the potential difference between both ends of the detection impedance 6 . Note that CK is a coupling capacitor.
以上の構成において、高電圧課電端子23に高電圧を課
電する。この状態において、絶縁体に部分放電が生じる
と、導体および金属シースに高周波パルスが誘起し、金
属シースの高周波パルスが検出インピーダンス6に流れ
てその両端に高周波パルスの大きさに比例した電位差が
生しる。その電位差を測定器7によって検出することに
より部分放電を測定する。In the above configuration, a high voltage is applied to the high voltage charging terminal 23. In this state, when a partial discharge occurs in the insulator, a high-frequency pulse is induced in the conductor and the metal sheath, and the high-frequency pulse in the metal sheath flows to the detection impedance 6, creating a potential difference at both ends proportional to the magnitude of the high-frequency pulse. Sign. The partial discharge is measured by detecting the potential difference with the measuring device 7.
測定器7の測定感度を較正するときは、高電圧端子23
の高電圧課電を停止し、較正信号発生器8を終端接続部
11の近傍に接続して電カケープル21の導体と金属シ
ースの間に較正用の高周波パルスを印加する。その等価
回路を第4図(b)に示す。第4図に示すように、較正
信号発生器8はv0ボルトの高周波パルスを静電容量C
8のコンデンサを介して電カケープル21の導体10と
金属シース12の間に加える。導体10と金属シース1
2の間には静電容量Cが形成され、静電容量Cのコンデ
ンサを流れた高周波パルスは検出インピーダンス6に分
流する。このようにして測定器7の感度較正が行われる
。ここで、静電容量Cのコンデンサによる見掛けの放電
電荷をQとし、電位をV、とすると、Q=VO・Co
=V+ ・c −−−−−−−−−−−(1)(1
)式より
O
v、 = VQ −−−−−(2)
が得られる。絶縁接続部20の絶縁筒の両側の金属シー
スの間に検出インピーダンスを接続しても略同様な効果
が得られる。When calibrating the measurement sensitivity of the measuring device 7, the high voltage terminal 23
The high voltage application is stopped, the calibration signal generator 8 is connected near the terminal connection part 11, and a high frequency pulse for calibration is applied between the conductor of the power cable 21 and the metal sheath. The equivalent circuit is shown in FIG. 4(b). As shown in FIG. 4, the calibration signal generator 8 sends a high frequency pulse of v0 volts to the capacitance
It is applied between the conductor 10 and the metal sheath 12 of the power cable 21 via a capacitor 8. Conductor 10 and metal sheath 1
A capacitance C is formed between the capacitance C and the high frequency pulse flowing through the capacitor having the capacitance C is shunted to the detection impedance 6. In this way, the sensitivity calibration of the measuring device 7 is performed. Here, if the apparent discharge charge by a capacitor with capacitance C is Q and the potential is V, then Q=VO・Co
=V+ ・c −−−−−−−−−−−(1)(1
) From the formula, O v, = VQ −−−−−(2)
is obtained. Substantially the same effect can be obtained by connecting a detection impedance between the metal sheaths on both sides of the insulating cylinder of the insulating connection part 20.
しかし、従来の部分放電測定方法によると、電カケープ
ル線路が数Kmというように長尺になると、較正用の高
周波パルスが部分放電測定位置に伝送されてくるまで、
そのレベル■。が減衰するため、また、通常はC>C,
であるため、(2)式のVIの値が小さくなり、所定の
較正操作を行うことができないという不都合がある。更
に、較正信号発生器を接続する終端接続部の位置と較正
操作を行う測定点の位置が離れているため作業性が悪い
という不都合がある。However, according to the conventional partial discharge measurement method, when the power cable line becomes long, such as several kilometers long, until the high-frequency pulse for calibration is transmitted to the partial discharge measurement position,
That level ■. is attenuated, and usually C>C,
Therefore, there is an inconvenience that the value of VI in equation (2) becomes small and a predetermined calibration operation cannot be performed. Furthermore, since the position of the terminal connection part to which the calibration signal generator is connected is far from the position of the measurement point where the calibration operation is performed, there is a problem that workability is poor.
従って、本発明の目的は所定のレベルの較正信号を得る
ことができる部分放電測定方法を提供することである。Therefore, it is an object of the present invention to provide a partial discharge measuring method that allows obtaining a calibration signal of a predetermined level.
本発明の他の目的は較正操作の作業性を改善した部分放
電測定方法を提供することである。Another object of the present invention is to provide a partial discharge measuring method that improves the workability of the calibration operation.
本発明は上記の目的を実現するため、部分放電によって
誘起される高周波パルスが流れる絶縁接続部の分離され
た金属シース上に防食ビニル層を介して一対の検出電極
を設け、その間に検出インピーダンスを挿入して接続す
るとともに検出インピーダンスと並列に較正信号発生器
を接続した部分放電測定方法を提供する。In order to achieve the above-mentioned object, the present invention provides a pair of detection electrodes via an anti-corrosion vinyl layer on a separated metal sheath of an insulated connection part through which high-frequency pulses induced by partial discharge flow, and a detection impedance is provided between them. A partial discharge measuring method is provided in which a calibration signal generator is connected in parallel with a detection impedance.
較正信号の注入は検出インピーダンスの両端に直接注入
しても良いが、前述した一対の検出電極に注入すること
もできる。また、絶縁接続部の防食ビニル層の外表面に
絶縁筒を介してその両側に一対の較正用電極を設け、そ
れに較正信号発生器を接続しても良い。The calibration signal may be injected directly to both ends of the detection impedance, but it can also be injected to the pair of detection electrodes described above. Alternatively, a pair of calibration electrodes may be provided on both sides of the outer surface of the anticorrosive vinyl layer of the insulating connection part via an insulating cylinder, and a calibration signal generator may be connected to the pair of calibration electrodes.
以下、本発明の部分放電測定方法を詳細に説明する。 Hereinafter, the partial discharge measuring method of the present invention will be explained in detail.
第1図は本発明の一実施例を示し、金属シース上の防食
ビニル11と絶縁接続部の金属胴管上の防食ビニル層2
は連続しており、金属胴管は絶縁筒3によって絶縁され
ている。金属胴管上の防食ビニル層2の外表面に一対の
検出電極4および一対の較正用電極5が設けられており
、これらの電極4.5に検出インピーダンス6および較
正信号発生器8が並列になるように接続されている。検
出インピーダンス6には測定器7が接続され、その両端
の電位差を検出するようになっている。FIG. 1 shows an embodiment of the present invention, in which an anticorrosion vinyl layer 11 on a metal sheath and an anticorrosion vinyl layer 2 on a metal trunk tube at an insulating connection part are shown.
is continuous, and the metal trunk tube is insulated by an insulating tube 3. A pair of detection electrodes 4 and a pair of calibration electrodes 5 are provided on the outer surface of the anticorrosive vinyl layer 2 on the metal trunk tube, and a detection impedance 6 and a calibration signal generator 8 are connected in parallel to these electrodes 4.5. connected so that A measuring device 7 is connected to the detection impedance 6 to detect the potential difference between both ends thereof.
第2図は第1図の実施例を回路的に示したものであり、
電カケープルの導体10は接続スリーブ11によって接
続され、導体10と金属胴管12の間に静電容量CI、
C2のコンデンサが形成され、金属胴管12は絶縁筒3
によって絶縁されている。金属胴管12上の防食ビニル
層2の外表面には検出電極4、および較正用電極5が設
けられている。検出インピーダンス6、測定器7、およ
び較正信号発生器5は第1図に示した通りである。FIG. 2 is a circuit diagram of the embodiment shown in FIG.
The conductor 10 of the power cable is connected by a connection sleeve 11, and there is a capacitance CI between the conductor 10 and the metal trunk tube 12.
A capacitor C2 is formed, and the metal body tube 12 is connected to the insulating tube 3.
insulated by. A detection electrode 4 and a calibration electrode 5 are provided on the outer surface of the anticorrosive vinyl layer 2 on the metal trunk tube 12. The detection impedance 6, measuring device 7, and calibration signal generator 5 are as shown in FIG.
第3図(a)は第2図の等価回路であり、同一部分は同
一の引用数字で示したので重複する説明は省略するが、
検出電極4によって静電容量C□、Cd2のコンデンサ
が、較正用電極5によって静電容量CP I、CPZの
コンデンサが形成される。ここで・CPI・CP2>
Co 。FIG. 3(a) is an equivalent circuit of FIG. 2, and the same parts are indicated by the same reference numerals, so redundant explanation will be omitted.
The detection electrode 4 forms a capacitor with capacitances C□ and Cd2, and the calibration electrode 5 forms a capacitor with capacitances CPI and CPZ. Here・CPI・CP2>
Co.
ス)。vinegar).
ス)、であるので、第3図(b)の等価回路が得られる
。この等価回路において、C,=C,。Therefore, the equivalent circuit shown in FIG. 3(b) is obtained. In this equivalent circuit, C,=C,.
C,>C,と仮定すると、
検出インピーダンス6の両端に加わる電圧V2は、
しI
ここで、C0、C1、C2、Voは既知、あるいは測定
可能である。従来の技術で説明した(2)式と、本発明
の(3)式を比較すると、
V 2 = 2 V l −−−−−(4)となる。Assuming that C, > C, the voltage V2 applied across the detection impedance 6 is: where C0, C1, C2, and Vo are known or can be measured. Comparing the equation (2) described in the related art and the equation (3) of the present invention, V 2 = 2 V l -----(4) is obtained.
ただし、C=C,とした。(4)式より明らかなように
、従来に比較して2倍のレベルで高周波パルスを検出す
ることになり、しかも、長尺の電カケープルを伝搬する
ことによって生じる減衰を考慮する必要はない。However, C=C. As is clear from equation (4), the high frequency pulse is detected at twice the level compared to the conventional method, and there is no need to take into account the attenuation caused by propagation through a long electric cable.
前述の実施例において、CPI、CPU>CGとしたが
、Coは10〜50PF程度であり、これを満たすため
に較正用電極5の面積を所定の値にすることにより50
0〜100OPF程度にすることはできる。In the above embodiment, CPI and CPU>CG were set, but Co is about 10 to 50PF, and to satisfy this, the area of the calibration electrode 5 is set to a predetermined value.
It is possible to set it to about 0 to 100 OPF.
ZcdI、Zcd2(Zについても同様である。ZcdI, Zcd2 (the same applies to Z).
また、較正用電極5を省略して検出用電極4に較正用信
号を注入する場合は、第3図(a)の等価回路において
cP、、 CP□が省略された形になるので第3図(
b)の等価回路と同一になる。ただし、較正精度を挙げ
るためには較正用電極5を設けた方が良い。Furthermore, if the calibration electrode 5 is omitted and the calibration signal is injected into the detection electrode 4, cP, CP□ will be omitted in the equivalent circuit of FIG. (
This is the same as the equivalent circuit of b). However, in order to improve the calibration accuracy, it is better to provide the calibration electrode 5.
更に、C,=C2、Z>Z、、を条件として説明したが
、この条件を満たさない場合でも、基本式をもとに補正
項を求めることにより較正は可能である。Further, the explanation has been made under the conditions that C,=C2, Z>Z, but even if this condition is not satisfied, calibration is possible by finding a correction term based on the basic equation.
以上説明した通り、本発明の部分放電測定方法によると
、絶縁接続部の金属胴管上に防食ビニル層を介して所定
の面積の電極を設け、その間に検出インピーダンスと較
正信号発生器を並列に接続して挿入したため、以下の効
果を奏することができる。As explained above, according to the partial discharge measuring method of the present invention, an electrode of a predetermined area is provided on the metal trunk tube of the insulated connection part through the anticorrosion vinyl layer, and a detection impedance and a calibration signal generator are connected in parallel between them. Since they are connected and inserted, the following effects can be achieved.
(1)長尺ケーブル線路の絶縁接続部において所定の感
度で部分放電の測定ができる。また、既設の線路にその
まま適用することができる。(1) Partial discharge can be measured with a predetermined sensitivity at an insulated connection part of a long cable line. Moreover, it can be applied to existing railway lines as is.
(2)較正用の高周波パルスの波形の歪みや減衰が生じ
ない。(2) No distortion or attenuation of the waveform of the high-frequency pulse for calibration occurs.
(3)較正信号発生器と測定器が同一の位置にあるため
、作業性が良い。(3) Workability is good because the calibration signal generator and measuring device are located at the same location.
(4)高圧導体に較正用の高周波パルスを注入する必要
がないので安全性が高い。(4) High safety because there is no need to inject high-frequency pulses for calibration into the high-voltage conductor.
(5)活線状態においても感度較正ができる。(5) Sensitivity calibration can be performed even in live line conditions.
【図面の簡単な説明】
第1図は本発明の一実施例を示す説明図。第2図は第1
図の回路的な説明図。第3図(a)、(b)は第2図の
等価回路図、第4図(a)、(b)は従来の部分放電測
定方法の説明図および等価回路図。
符号の説明
1−−−−−−−一金属シース上の防食ビニル層2−−
−−−−−−一金属胴管上の防食ビニル層3 絶縁
筒 4−−−−=−−−一検出電極5−−−−
−−−−−−一較正用電極
6−−−−−−−−−検出インピーダンス7−−−−−
−−−−一測定器 810 ケーブル導
体 11・−12−−−−−−−一金属胴管
較正信号発生器
終端スリーブBRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is an explanatory diagram showing one embodiment of the present invention. Figure 2 is the first
A circuit explanatory diagram of the figure. 3(a) and 3(b) are equivalent circuit diagrams of FIG. 2, and FIGS. 4(a) and 4(b) are explanatory diagrams and equivalent circuit diagrams of a conventional partial discharge measuring method. Explanation of symbols 1 --- Corrosion-proof vinyl layer on metal sheath 2 ---
--------1 Corrosion-proof vinyl layer 3 on the metal trunk tube 4--Insulating cylinder 4-------1 Detection electrode 5--
--------- One calibration electrode 6 --------- Detection impedance 7 ---
-------1 Measuring device 810 Cable conductor 11/-12--1 Metal barrel calibration signal generator termination sleeve
Claims (2)
放電測定方法において、 前記絶縁接続部の防食ビニル層の外表面に絶縁筒を介し
てその両側に一対の検出電極を設け、前記一対の検出電
極の間に測定器に接続される検出インピーダンスを接続
し、 前記検出インピーダンスの両端に前記測定器の感度較正
用の信号を注入することを特徴とする部分放電測定方法
。(1) In a method for measuring partial discharge in an insulated connection part of an underground power cable line, a pair of detection electrodes are provided on both sides of the anticorrosive vinyl layer of the insulated connection part via an insulating tube, and the pair of detection electrodes is A method for measuring partial discharge, characterized in that a detection impedance connected to a measuring device is connected between the electrodes, and a signal for sensitivity calibration of the measuring device is injected into both ends of the detection impedance.
一対の検出電極に隣接して一対の較正用電極を設け、 前記一対の較正用電極に前記感度較正用の信号を注入す
ることを特徴とする請求項第1項記載の部分放電測定方
法。(2) Providing a pair of calibration electrodes adjacent to the pair of detection electrodes on both sides of the outer surface via the insulating tube, and injecting the sensitivity calibration signal into the pair of calibration electrodes. The partial discharge measuring method according to claim 1, characterized in that:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63322770A JPH067148B2 (en) | 1988-12-21 | 1988-12-21 | Partial discharge measurement method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63322770A JPH067148B2 (en) | 1988-12-21 | 1988-12-21 | Partial discharge measurement method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH02167484A true JPH02167484A (en) | 1990-06-27 |
JPH067148B2 JPH067148B2 (en) | 1994-01-26 |
Family
ID=18147451
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63322770A Expired - Lifetime JPH067148B2 (en) | 1988-12-21 | 1988-12-21 | Partial discharge measurement method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH067148B2 (en) |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS57191568A (en) * | 1981-05-21 | 1982-11-25 | Toshiba Corp | Partial discharge measuring device |
JPS60146161A (en) * | 1984-01-11 | 1985-08-01 | Mitsubishi Electric Corp | Abnormality detector for electric insulation equipment |
JPS6140571A (en) * | 1984-07-31 | 1986-02-26 | Showa Electric Wire & Cable Co Ltd | Partial dischrge measurement of hot cable |
JPS62245976A (en) * | 1986-04-18 | 1987-10-27 | Mitsubishi Electric Corp | Detecting device for abnormality of electric equipment |
-
1988
- 1988-12-21 JP JP63322770A patent/JPH067148B2/en not_active Expired - Lifetime
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS57191568A (en) * | 1981-05-21 | 1982-11-25 | Toshiba Corp | Partial discharge measuring device |
JPS60146161A (en) * | 1984-01-11 | 1985-08-01 | Mitsubishi Electric Corp | Abnormality detector for electric insulation equipment |
JPS6140571A (en) * | 1984-07-31 | 1986-02-26 | Showa Electric Wire & Cable Co Ltd | Partial dischrge measurement of hot cable |
JPS62245976A (en) * | 1986-04-18 | 1987-10-27 | Mitsubishi Electric Corp | Detecting device for abnormality of electric equipment |
Also Published As
Publication number | Publication date |
---|---|
JPH067148B2 (en) | 1994-01-26 |
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