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JPH0315707B2 - - Google Patents
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JPH0315707B2 - - Google Patents

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Publication number
JPH0315707B2
JPH0315707B2 JP20318681A JP20318681A JPH0315707B2 JP H0315707 B2 JPH0315707 B2 JP H0315707B2 JP 20318681 A JP20318681 A JP 20318681A JP 20318681 A JP20318681 A JP 20318681A JP H0315707 B2 JPH0315707 B2 JP H0315707B2
Authority
JP
Japan
Prior art keywords
cable
noise
pulse
measured
terminal
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
JP20318681A
Other languages
Japanese (ja)
Other versions
JPS58103672A (en
Inventor
Mitsugi Aihara
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
SWCC Corp
Original Assignee
Showa Electric Wire and Cable Co
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 Showa Electric Wire and Cable Co filed Critical Showa Electric Wire and Cable Co
Priority to JP20318681A priority Critical patent/JPS58103672A/en
Publication of JPS58103672A publication Critical patent/JPS58103672A/en
Publication of JPH0315707B2 publication Critical patent/JPH0315707B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R31/00Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
    • G01R31/12Testing dielectric strength or breakdown voltage ; Testing or monitoring effectiveness or level of insulation, e.g. of a cable or of an apparatus, for example using partial discharge measurements; Electrostatic testing
    • G01R31/1227Testing dielectric strength or breakdown voltage ; Testing or monitoring effectiveness or level of insulation, e.g. of a cable or of an apparatus, for example using partial discharge measurements; Electrostatic testing of components, parts or materials
    • G01R31/1263Testing dielectric strength or breakdown voltage ; Testing or monitoring effectiveness or level of insulation, e.g. of a cable or of an apparatus, for example using partial discharge measurements; Electrostatic testing of components, parts or materials of solid or fluid materials, e.g. insulation films, bulk material; of semiconductors or LV electronic components or parts; of cable, line or wire insulation
    • G01R31/1272Testing dielectric strength or breakdown voltage ; Testing or monitoring effectiveness or level of insulation, e.g. of a cable or of an apparatus, for example using partial discharge measurements; Electrostatic testing of components, parts or materials of solid or fluid materials, e.g. insulation films, bulk material; of semiconductors or LV electronic components or parts; of cable, line or wire insulation of cable, line or wire insulation, e.g. using partial discharge measurements

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Testing Relating To Insulation (AREA)

Description

【発明の詳細な説明】 本発明はケーブルの部分放電測定方法に関す
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring partial discharge in cables.

従来よりケーブルの管理試験の一つとしてケー
ブルの部分放電測定が第1図に示すようなパルス
回路を用いて行なわれている。該パルス回路は微
小パルスを扱うことから、ブロツキングコイルL
を介して高圧電源Eに接続したリード線l1と接地
したリード線l2上下に配置し、該リード線l1と大
地間に接続された結合コンデンサCと検出素子Z
を挿入して構成されており、被測定ケーブル1は
その一方の端末2でケーブルの導体にリード線l1
を、その下方でケーブルの金属シースにリード線
l2を接続して測定される。
BACKGROUND OF THE INVENTION Conventionally, partial discharge measurement of cables has been carried out as one of cable management tests using a pulse circuit as shown in FIG. Since the pulse circuit handles minute pulses, the blocking coil L
A lead wire L1 connected to a high-voltage power supply E via a lead wire L1 and a grounded lead wire L2 are arranged above and below, and a coupling capacitor C and a detection element Z are connected between the lead wire L1 and the ground.
The cable under test 1 is constructed by inserting the lead wire l 1 into the cable conductor at one terminal 2.
and the lead wire below it into the metal sheath of the cable.
l Measured by connecting 2 .

而して該パルス回路は上述のように構成され空
間的に組立てられているので、静電誘導や電磁誘
導による外来ノイズが入り込みやすい。該回路に
侵入するノイズとしては、第1図に模式的に示し
たようにリード線l1を通して高圧電源Eから入つ
てくるノイズV1、回路との漂遊容量を介して入
つてくる静電誘導によるノイズV2、高電圧課電
によりケーブル終端部1bに発生するコロナV3
および相互インダクタンスMを介して入つてくる
電磁誘導によるノイズV4がある。
Since the pulse circuit is configured and spatially assembled as described above, external noise due to electrostatic induction or electromagnetic induction is likely to enter. Noise that enters the circuit includes noise V 1 that enters from the high-voltage power supply E through the lead wire L 1 as schematically shown in Figure 1, and electrostatic induction that enters through stray capacitance with the circuit. Noise V 2 caused by high voltage charging, corona V 3 generated at the cable end 1b due to high voltage charging
There is also noise V 4 due to electromagnetic induction that enters through the mutual inductance M.

従来これらのノイズを除去するために次のよう
な方法が採られている。すなわち高圧電圧Eから
のノイズV1に対してはブロキングコイルL(第1
図)やバランス回路により相殺して除去する。ブ
ロキングコイルLによるときは1/100〜1/1000程
度に低減される。静電容量によるノイズV2に対
してはケーブルごとパルス回路をシールドルーム
中に収納し、金属体を近傍させないようにする。
この場合には占有空間が大きくなる上、設備費も
高くなる。コロナV3に対してはケーブル終端部
1bを大形化して沿面電界が小さくなるよう維持
する。電磁誘電によるノイズV4に対しては、ノ
イズV4が被測定ケーブル1と結合コンデンサC
の作る空間的ループが小さい程侵入は小さくなる
が、ほとんど無防備になつている。
Conventionally, the following methods have been adopted to remove these noises. In other words, the blocking coil L ( first
(Fig.) and a balance circuit. When using the blocking coil L, it is reduced to about 1/100 to 1/1000. To prevent noise V2 caused by capacitance, store the pulse circuit together with the cable in a shielded room and avoid placing any metal objects nearby.
In this case, not only the occupied space becomes large, but also the equipment cost becomes high. For corona V3 , the cable end portion 1b is enlarged to maintain a small creeping electric field. Regarding the noise V 4 caused by electromagnetic dielectric, the noise V 4 is caused by the cable under test 1 and the coupling capacitor C.
The smaller the spatial loop created, the smaller the intrusion, but it is almost defenseless.

従つて従来の測定方法では装置が大型化して設
備費が高価になる他、全てのノイズを有効に除去
できない欠点があつた。
Therefore, in the conventional measuring method, the equipment becomes large and the equipment cost becomes expensive, and there are also disadvantages in that all noise cannot be effectively removed.

本発明はかかる従来の難点に鑑みなされたもの
で、被測定ケーブルの一端を接地された金属ケー
スに装入すると共に他端を別の接地された金属ケ
ース内にてパルスセンサを介して結合コンデンサ
兼用課電ケーブルと接続し、該課電ケーブルを通
して被測定ケーブルに高電圧を印加し、その結果
被測定ケーブルに発生する部分放電を上記パルス
センサにて光信号で取出すようにしたケーブルの
部分放電測定方法を提供することを目的とする。
The present invention has been made in view of such conventional difficulties.One end of the cable to be measured is inserted into a grounded metal case, and the other end is connected to a coupling capacitor via a pulse sensor in another grounded metal case. Partial discharge of a cable that is connected to a dual-purpose charging cable, applies a high voltage to the cable under test through the charging cable, and as a result, the partial discharge generated in the cable under test is extracted as an optical signal by the above-mentioned pulse sensor. The purpose is to provide a measurement method.

以下本発明を図面に基づき実施例につき説明す
る。
The present invention will be described below with reference to the drawings.

第2図は本発明を実施するためのパルス回路の
一例を示したもので、被測定ケーブル3はその端
末3aでパルスセンサ4と介して課電ケーブル5
の端末5aと接続されており、これら導体の露出
した端末3a,5aおよびパルスセンサ4は漂遊
容量を無くすために接地された金属ケース6で電
気的にシールドされている。同様にケーブル3の
他方の開放された端末3bにも接地された金属ケ
ース7によるシールドが行なわれている。また該
端末3bはコロナV3の発生を抑制するために大
形に形成されている。課電ケーブル5の他方の端
末5b′には碍子8が被嵌され、これから引き出さ
れたケーブル5の導体9にはブロキングコイルL
を介して高圧電源Eが接続されている。ブロキン
グコイルLは高圧電源のノイズV1を除去するた
めのものである。また課電ケーブル5は結合コン
デンサCの役目もしており、課電ケーブル5自体
の金属シースにより該コンデンサCは電気的にシ
ールドされたものになつている。このように課電
ケーブル5を結合コンデンサC兼用とすることに
より、パルス回路の空間的構成を小さくすること
ができる。パルスセンサ4はインピーダンスZお
よび該インピーダンスZの両端に発生する電圧を
光信号に変換するE/O変換器からなつており、
ケーブル3に発生する部分放電は該センサ4から
光信号として光フアイバ10により取出される。
そしてモニタ11で電気信号に変換、増幅されて
オシロ12に電気波形として写し出されるように
なつている。
FIG. 2 shows an example of a pulse circuit for implementing the present invention, in which a cable to be measured 3 is connected to a power supply cable 5 via a pulse sensor 4 at its terminal 3a.
The exposed terminals 3a, 5a of these conductors and the pulse sensor 4 are electrically shielded with a grounded metal case 6 to eliminate stray capacitance. Similarly, the other open end 3b of the cable 3 is also shielded by a grounded metal case 7. Further, the terminal 3b is formed in a large size in order to suppress the generation of corona V3 . The other terminal 5b' of the charging cable 5 is fitted with an insulator 8, and the conductor 9 of the cable 5 drawn out from this is fitted with a blocking coil L.
A high-voltage power supply E is connected via the. The blocking coil L is for removing noise V1 of the high voltage power supply. The energizing cable 5 also serves as a coupling capacitor C, and the capacitor C is electrically shielded by the metal sheath of the energizing cable 5 itself. By using the energizing cable 5 also as the coupling capacitor C in this way, the spatial configuration of the pulse circuit can be made smaller. The pulse sensor 4 consists of an impedance Z and an E/O converter that converts the voltage generated across the impedance Z into an optical signal.
Partial discharge generated in the cable 3 is extracted from the sensor 4 as an optical signal by an optical fiber 10.
The signal is then converted into an electrical signal by the monitor 11, amplified, and displayed on the oscilloscope 12 as an electrical waveform.

本発明では以上のようにパルス回路を構成して
ケーブルの部分放電測定を行なうが、これによれ
ば各種のノイズは次のように除去される。
In the present invention, the pulse circuit is configured as described above to measure partial discharge of a cable, and various noises are removed as follows.

まず高電圧は高圧電源Eにより課電ケーブル5
を通して被測定ケーブル3の導体および金属シー
ス間に印加されるが、高圧電源EのノイズV1
ブロキングコイルLにより除去される。またケー
ブル3の開放端末3bに発生するコロナV3は端
末3bの大型化により抑制される。静電誘導によ
るノイズV2に対しては、接地された金属ケース
6,7によりケーブル3の端末3a,3b、課電
ケーブル5の端末5a、パルスセンサ4をシール
ドし、かつケーブル3,5自体は自己の金属シー
スでシールドされているので、パルス回路全体か
ら漂遊容量を除去され、その結果発生しなくな
る。また電磁誘導によるノイズV4に対しては、
結合コンデンサ兼用課電ケーブルを用いることに
よつて結合コンデンサを省略しパルス回路の空間
的構成を小さくしているので発生が抑えられる。
さらに部分放電の測定信号はパルスセンサ4で光
信号に変換して光フアイバ10により取出してい
るので、容易に外部からの電気的影響を受けない
でオシロ12に導くことができる。
First, the high voltage is applied to the power supply cable 5 by the high voltage power supply E.
The noise V 1 of the high-voltage power supply E is applied between the conductor of the cable 3 to be measured and the metal sheath through the blocking coil L. Further, corona V 3 generated at the open terminal 3b of the cable 3 is suppressed by increasing the size of the terminal 3b. To prevent noise V 2 caused by electrostatic induction, the terminals 3a and 3b of the cable 3, the terminal 5a of the charging cable 5, and the pulse sensor 4 are shielded by grounded metal cases 6 and 7, and the cables 3 and 5 themselves are shielded. Since it is shielded with its own metal sheath, stray capacitance is removed from the entire pulse circuit so that it no longer occurs. In addition, for noise V 4 due to electromagnetic induction,
By using a energizing cable that also serves as a coupling capacitor, the coupling capacitor is omitted and the spatial configuration of the pulse circuit is made small, thereby suppressing the occurrence.
Further, since the partial discharge measurement signal is converted into an optical signal by the pulse sensor 4 and taken out by the optical fiber 10, it can be easily guided to the oscilloscope 12 without being affected by external electrical influences.

第3図は本発明を実施するためのパルス回路の
他の例で、ここでは第2図のブロキングコイルL
が用いられない代りにバランス検出回路又は極性
判別回路を設けて高圧電源EからのノイズV1
除去しており、他のノイズV2,V3,V4は第2図
のパルス回路と同様な作用により除去される。す
なわちこのパルス回路では金属ケース6内で結合
コンデンサ兼用課電ケーブル5はその端末の先端
5aが分岐され、それぞれパルスセンサ4′,
4″を介して被測定ケーブル3の端末3aおよび
結合コンデンサ用ケーブル13の端末13aに接
続されている。結合コンデンサ用ケーブル13の
開放端末13bにはケーブル3の端末3bと同じ
ように接地された金属ケース14によるシールド
が施されている。そしてパルスコンデサ4′,
4″とモニタ11′,11″とバランス又は極性判
別を行なう検出器15とで検出回路を構成してい
る。なお10′,10″は光フアイバ、12はオシ
ロである。この検出回路では高圧電源Eからのノ
イズV1の他、被測定ケーブル3の開放端末3b
におけるコロナV3の除去にも有効である。
FIG. 3 shows another example of a pulse circuit for implementing the present invention, in which the blocking coil L shown in FIG.
Instead, a balance detection circuit or a polarity discrimination circuit is provided to remove the noise V 1 from the high-voltage power supply E, and the other noises V 2 , V 3 , and V 4 are the same as the pulse circuit in Figure 2. It is removed by a similar action. That is, in this pulse circuit, the terminal tip 5a of the energizing cable 5 which also serves as a coupling capacitor is branched within the metal case 6, and is connected to the pulse sensor 4', respectively.
4'' to the terminal 3a of the cable under test 3 and the terminal 13a of the coupling capacitor cable 13.The open terminal 13b of the coupling capacitor cable 13 is grounded in the same way as the terminal 3b of the cable 3. Shielding is provided by a metal case 14, and a pulse capacitor 4',
4'', monitors 11' and 11'', and a detector 15 for determining balance or polarity constitute a detection circuit. Note that 10' and 10'' are optical fibers, and 12 is an oscilloscope.In this detection circuit, in addition to the noise V1 from the high-voltage power supply E, the open terminal 3b of the cable under test 3 is detected.
It is also effective in removing corona V3 .

以上説明したように本発明によれば、被測定ケ
ーブルの一端を接地された金属ケースに装入する
と共に他端を別の接地された金属ケース内にてパ
ルスセンサを介して結合コンデンサ兼用課電ケー
ブルと接続し、該課電ケーブルを通して被測定ケ
ーブルに高電圧を印加し、その結果被測定ケーブ
ルに発生する部分放電を上記パルスセンサにて光
信号で取出すようにして測定しているので、測定
に伴なう高圧電源からのノイズ、静電誘導による
ノイズ、電磁誘導によるノイズ、コロナ放電を有
効に除去でき、シールドルームが不要になる。ま
た被測定ケーブルの端末の形成も簡単に行なえ、
さらに被測定ケーブルを含むパルス回路の組立て
も任意の場所でしかも簡単に行なえる利点があ
る。
As explained above, according to the present invention, one end of the cable to be measured is inserted into a grounded metal case, and the other end is placed in another grounded metal case and charged with a coupling capacitor via a pulse sensor. A high voltage is applied to the cable under test through the energizing cable, and the partial discharge generated in the cable under test is measured using the above-mentioned pulse sensor as an optical signal. It can effectively eliminate noise from high-voltage power supplies, noise caused by electrostatic induction, noise caused by electromagnetic induction, and corona discharge, eliminating the need for a shield room. It is also easy to form the terminal of the cable under test.
Another advantage is that the pulse circuit including the cable under test can be easily assembled at any location.

なお本発明はケーブルだけでなくケーブルの接
続部、ユニツトなどの部分放電測定にも適用でき
る。
Note that the present invention is applicable not only to cables but also to partial discharge measurements of cable connections, units, etc.

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

第1図は従来のパルス回路を示す概念図、第2
〜3図は本発明で使用するパルス回路を示す概念
図である。 3……被測定ケーブル、3a,3b……端末、
4,4′,4″……パルスセンサ、5……結合コン
デンサ兼用課電ケーブル、6,7,14……接地
された金属ケース。
Figure 1 is a conceptual diagram showing a conventional pulse circuit, Figure 2 is a conceptual diagram showing a conventional pulse circuit.
3 are conceptual diagrams showing pulse circuits used in the present invention. 3... Cable under test, 3a, 3b... Terminal,
4, 4', 4''... Pulse sensor, 5... Power supply cable that also serves as a coupling capacitor, 6, 7, 14... Grounded metal case.

Claims (1)

【特許請求の範囲】[Claims] 1 被測定ケーブルの一端を接地された金属ケー
スに挿入すると共に他端を別の接地された金属ケ
ース内にて電気信号を光信号に変換するE/O変
換器を備えたパルスセンサを介して結合コンデン
サ兼用課電ケーブルと接続し、該課電ケーブルを
通して被測定ケーブルに高電圧を印加し、その結
果被測定ケーブルに発生する部分放電を上記パル
スセンサにて光信号で取出すようにしたことを特
徴とするケーブルの部分放電測定方法。
1 One end of the cable to be measured is inserted into a grounded metal case, and the other end is inserted into another grounded metal case through a pulse sensor equipped with an E/O converter that converts electrical signals into optical signals. A high voltage is applied to the cable to be measured through the energizing cable that also serves as a coupling capacitor, and the partial discharge generated in the cable to be measured is extracted as an optical signal by the pulse sensor. Characteristic cable partial discharge measurement method.
JP20318681A 1981-12-16 1981-12-16 Partial discharge measuring method of cable Granted JPS58103672A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20318681A JPS58103672A (en) 1981-12-16 1981-12-16 Partial discharge measuring method of cable

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20318681A JPS58103672A (en) 1981-12-16 1981-12-16 Partial discharge measuring method of cable

Publications (2)

Publication Number Publication Date
JPS58103672A JPS58103672A (en) 1983-06-20
JPH0315707B2 true JPH0315707B2 (en) 1991-03-01

Family

ID=16469877

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20318681A Granted JPS58103672A (en) 1981-12-16 1981-12-16 Partial discharge measuring method of cable

Country Status (1)

Country Link
JP (1) JPS58103672A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6072578U (en) * 1983-10-21 1985-05-22 三菱電線工業株式会社 Cable partial discharge measuring device

Also Published As

Publication number Publication date
JPS58103672A (en) 1983-06-20

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