JPH02176579A - Measurement of partial electric discharge - Google Patents
Measurement of partial electric dischargeInfo
- Publication number
- JPH02176579A JPH02176579A JP33155288A JP33155288A JPH02176579A JP H02176579 A JPH02176579 A JP H02176579A JP 33155288 A JP33155288 A JP 33155288A JP 33155288 A JP33155288 A JP 33155288A JP H02176579 A JPH02176579 A JP H02176579A
- Authority
- JP
- Japan
- Prior art keywords
- signal
- partial discharge
- frequency
- measurement
- amplifier
- 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
- 238000005259 measurement Methods 0.000 title claims abstract description 18
- 238000012935 Averaging Methods 0.000 claims description 6
- 239000012212 insulator Substances 0.000 claims description 5
- 230000006866 deterioration Effects 0.000 claims description 2
- 238000000691 measurement method Methods 0.000 claims description 2
- 238000001514 detection method Methods 0.000 abstract description 11
- 238000006243 chemical reaction Methods 0.000 abstract description 5
- 230000002238 attenuated effect Effects 0.000 abstract description 3
- 238000010408 sweeping Methods 0.000 abstract description 3
- 230000035945 sensitivity Effects 0.000 abstract description 2
- 238000000034 method Methods 0.000 description 10
- 230000010355 oscillation Effects 0.000 description 6
- 230000000903 blocking effect Effects 0.000 description 4
- 239000003990 capacitor Substances 0.000 description 4
- 230000008878 coupling Effects 0.000 description 4
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 238000001228 spectrum Methods 0.000 description 4
- 239000004020 conductor Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 230000000737 periodic effect Effects 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〕
本発明は絶縁体に高電圧が課電される電カケープル等の
部分放電測定方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a method for measuring partial discharge in a power cable or the like in which a high voltage is applied to an insulator.
第3図は従来の部分放電測定方法を示す。地中に布設さ
れた電カケープル1は金属シースが接地されており、終
端接続部2を介して高電圧課電端子3に接続されている
。終端接続部2と高電圧課電端子3の間にはブロッキン
グコイル4が設けられており、ブロッキングコイル4の
電カケープル1側には結合コンデンサ5が接続されてい
る。結合コンデンサ5は検出インピーダンス6を介して
接地されており、検出インピーダンス6は高域通過フィ
ルタフに接続され、高域通過フィルタ7は減衰器8に接
続されている。減衰器8は増幅器9に接続され、増幅器
9は信号メモリ処理部10に接続されている。FIG. 3 shows a conventional partial discharge measuring method. A power cable 1 laid underground has a metal sheath grounded and is connected to a high voltage charging terminal 3 via a terminal connection part 2. A blocking coil 4 is provided between the terminal connection portion 2 and the high voltage charging terminal 3, and a coupling capacitor 5 is connected to the power cable 1 side of the blocking coil 4. The coupling capacitor 5 is grounded via a detection impedance 6 , the detection impedance 6 is connected to a high-pass filter, and the high-pass filter 7 is connected to an attenuator 8 . The attenuator 8 is connected to an amplifier 9, and the amplifier 9 is connected to a signal memory processing section 10.
以上の構成において、高電圧課電端子3に交流高電圧(
例えば、275KV)を課電し、電力ケープル1によっ
て構成される地中送電線路を活線状態にする。この状態
で電カケープル1の絶縁体に部分放電が生じると、電カ
ケープル1の導体および金属シース間に高周波パルスが
誘起される。導体の高周波パルスはブロッキングコイル
4によって阻止され、交流課電電圧に基づく電流ととも
に結合コンデンサ5を介して検出インピーダンス6を流
れ、その両端に電位差が発生する。その電位差に基づく
信号の高域成分は高域通過フィルタ7を通過し、減衰器
8によって所定のレベルに減衰させられる。その後の信
号は増幅器9によって増幅され、信号メモリ処理部10
に入力し、そこで、所定の信号処理を受ける。この信号
処理では、高周波パルスの大きさ、単位時間当たりの個
数を検出することにより部分放電を測定し、電カケープ
ル1の絶縁劣化の診断が行われる。In the above configuration, the high voltage charging terminal 3 is connected to the AC high voltage (
For example, 275 KV) is applied to make the underground power transmission line constituted by the power cable 1 live. When a partial discharge occurs in the insulator of the power cable 1 in this state, a high frequency pulse is induced between the conductor of the power cable 1 and the metal sheath. The high frequency pulse of the conductor is blocked by the blocking coil 4 and flows through the detection impedance 6 via the coupling capacitor 5 together with a current based on the alternating current applied voltage, and a potential difference is generated across the impedance. A high-frequency component of the signal based on the potential difference passes through a high-pass filter 7 and is attenuated by an attenuator 8 to a predetermined level. The subsequent signal is amplified by an amplifier 9, and a signal memory processing section 10
, where it undergoes predetermined signal processing. In this signal processing, partial discharge is measured by detecting the magnitude of high-frequency pulses and the number of high-frequency pulses per unit time, and insulation deterioration of the power cable 1 is diagnosed.
しかし、従来の部分放電測定方法によると、部分放電に
基づく高周波パルスのレベルが小さいと、外部から侵入
するノイズおよび増幅器自身のノイズ等によってマスク
されてしまうため、部分放電の測定が困難になる場合が
ある。また、部分放電パルスの発生周期が一定でなく、
更に、交流電圧の課電時には、高周波パルスが交流電圧
の周期に応じて正および負に極性を変えるため、高周波
パルスを何周期かにわたって平均化すると出力が零にな
って部分放電の測定ができなくなる不都合がある。However, according to the conventional partial discharge measurement method, if the level of the high-frequency pulse based on partial discharge is small, it will be masked by noise entering from the outside and the noise of the amplifier itself, making it difficult to measure partial discharge. There is. In addition, the generation period of partial discharge pulses is not constant,
Furthermore, when AC voltage is applied, the high-frequency pulse changes polarity between positive and negative depending on the cycle of the AC voltage, so if the high-frequency pulse is averaged over several cycles, the output becomes zero and partial discharge cannot be measured. There is an inconvenience that it disappears.
従って、本発明の目的は外部から侵入するノイズ等によ
って測定結果が影響され難い部分放電測定方法を提供す
ることである。Accordingly, an object of the present invention is to provide a partial discharge measuring method in which the measurement results are not easily influenced by noise entering from the outside.
本発明の他の目的は高周波パルスの平均化処理によって
測定感度の向上を図る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 measurement sensitivity by averaging high-frequency pulses.
本発明は上記の目的を実現するため、部分放電に基づく
高周波パルス信号と周波数掃引型局部発振器より出力さ
れる局部発振信号とを混合して中間周波信号(ビート信
号)を発生し、この中間周波信号を検波することによっ
て部分放電を測定する部分放電測定方法を提供する。In order to achieve the above object, the present invention generates an intermediate frequency signal (beat signal) by mixing a high frequency pulse signal based on partial discharge and a local oscillation signal output from a frequency sweep type local oscillator, and generates an intermediate frequency signal (beat signal). A partial discharge measuring method is provided for measuring partial discharge by detecting a signal.
ここで、周波数掃引の周期をTとすると、nT(n=1
.2.3・・−m−−−・・・−)の時間にわたって測
定を行い、測定結果をnで除算することによって平均値
を算出すると測定精度が向上する。Here, if the frequency sweep period is T, then nT (n=1
.. If the measurement is performed over a period of time of 2.3...-m---...-) and the average value is calculated by dividing the measurement result by n, the measurement accuracy will be improved.
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(a)は本発明の一実施例を示し、第3図と共通
する部分は共通の引用数字で示したので重複する説明は
省略するが、第3図の構成に以下の構成が付加されてい
る。即ち、増幅器9の出力は周波数掃引型の局部発振器
15の出力とともに混合器11に接続され、混合器II
は中間周波信号を出力するために増幅器I2に接続され
ている。増幅器12は検波回路13に接続され、検波回
路13は検波信号をA/D変換するA/D変換回路14
に接続されている。A/D変換回路14は信号メモリ処
理部(デジタル信号を記憶するメモリを有し、そのデジ
タル信号を演算処理する)lOに接続され、信号メモリ
処理部10は制御部17に接続されている。局部発振器
I5、表示部16、および信号メモリ処理部10等は制
御部17によって制御される。局部発振器15は、例え
ば、第1図(b)に示すように、周期Tで変化する周波
数の局部発振信号を出力する。FIG. 1(a) shows an embodiment of the present invention, and parts common to FIG. 3 are indicated by common reference numerals, so duplicate explanations will be omitted, but the following configuration is added to the configuration of FIG. It has been added. That is, the output of the amplifier 9 is connected to the mixer 11 together with the output of the frequency sweep type local oscillator 15, and the output of the amplifier 9 is connected to the mixer 11.
is connected to amplifier I2 for outputting an intermediate frequency signal. The amplifier 12 is connected to a detection circuit 13, and the detection circuit 13 is connected to an A/D conversion circuit 14 that A/D converts the detected signal.
It is connected to the. The A/D conversion circuit 14 is connected to a signal memory processing section (having a memory for storing digital signals and performing arithmetic processing on the digital signals) lO, and the signal memory processing section 10 is connected to the control section 17. Local oscillator I5, display section 16, signal memory processing section 10, etc. are controlled by control section 17. The local oscillator 15 outputs a local oscillation signal having a frequency that changes with a period T, for example, as shown in FIG. 1(b).
以下、本発明の詳細な説明する。The present invention will be explained in detail below.
検出インピーダンス6の両端の電位差として表れる部分
放電に基づく高周波パルスは貰域通過フィルタ7を通過
しく低域成分および直流成分はカットされる)、減衰器
8で所定のレベルに減衰させられる。減衰器8の出力は
増幅器9で増幅され、混合器1工で局部発振器15から
の局部発振信号(例えば、第1図(1))に示すように
時間に対して周波数が直線的に変化する信号であるが、
これに限定しない)と混合される。混合器11における
この混合によって中間周波信号(ビート信号)が出力さ
れ、増幅器12で増幅された後、検波回路13で検波さ
れる。この検波信号は局部発振信号が周波数を掃引され
ているため、その掃引幅に応じた周波数帯域の高周波パ
ルスに対応するものであり、これがA/D変換回路14
でデジタル信号に変換される。そのデジタル信号が信号
メモリ処理部10で処理され、その大きさ、および単位
時間当たりの個数によって部分放電の判定が行われる。A high frequency pulse based on a partial discharge appearing as a potential difference between both ends of the detection impedance 6 passes through a band pass filter 7 (low frequency components and DC components are cut), and is attenuated to a predetermined level by an attenuator 8. The output of the attenuator 8 is amplified by the amplifier 9, and the mixer 1 generates a local oscillation signal from the local oscillator 15 (for example, as shown in FIG. 1 (1)), the frequency changes linearly with respect to time. Although it is a signal,
(including but not limited to). This mixing in the mixer 11 outputs an intermediate frequency signal (beat signal), which is amplified by the amplifier 12 and then detected by the detection circuit 13. Since this detection signal is a local oscillation signal whose frequency is swept, it corresponds to a high-frequency pulse in a frequency band corresponding to the sweep width, and this is the signal that is detected by the A/D conversion circuit 14.
is converted into a digital signal. The digital signal is processed by the signal memory processing section 10, and partial discharge is determined based on its magnitude and number per unit time.
測定結果は表示部16に表示される。The measurement results are displayed on the display section 16.
ここで、周期Tで周波数を掃引しながら、時間nTにわ
たって1回の部分放電の測定を行い、各回の測定結果を
信号メモリ処理部10で加算し、その加算値をnで除算
するとその平均値を算出することができる。このような
平均化処理によってランダムノイズのレベルは1/J]
口こ減衰することが判っている。例えば、n=10’と
すると、ランダムノイズ(7) L/<ルハ1 /、/
TO”r= 1 /100 トf、にる。従って、平均
化処理しないときに比較して1 /100のレベルの部
分放電まで測定が可能になる。Here, partial discharge is measured once over time nT while sweeping the frequency with period T, and the measurement results of each time are added up in the signal memory processing section 10, and when the added value is divided by n, the average value is obtained. can be calculated. Through such averaging processing, the level of random noise is reduced to 1/J]
It is known that the mouth is weakened. For example, if n=10', random noise (7) L/< Luha1 /, /
TO''r=1/100 f. Therefore, it is possible to measure partial discharges up to a level of 1/100 compared to when no averaging process is performed.
第2図(a)はこのようにして測定された部分放電に基
づく高周波パルスの周波数スペクトラムである。高周波
パルスの周波数をfs、局部発振信号の周波数をfLと
すると、f、、=f、−f、によって中間周波信号の周
波数ffiが定まり、f、を一定にしてf、を第1図(
b)のように掃引すると、第2図(b)に示す周波数ス
ペクトラムf、(0〜2000MH2’)が得られる。FIG. 2(a) shows the frequency spectrum of the high-frequency pulse based on the partial discharge measured in this manner. If the frequency of the high-frequency pulse is fs and the frequency of the local oscillation signal is fL, then the frequency ffi of the intermediate frequency signal is determined by f, , = f, -f, and when f is constant, f is shown in Fig. 1 (
By sweeping as shown in b), a frequency spectrum f (0 to 2000 MH2') shown in FIG. 2(b) is obtained.
第2図(b)は高電圧課電端子3に無課電の状態で測定
したノイズのスペクトラムである。その周波数スペクト
ラムより明らかなように、約700 MH2の近辺にU
HFテレビ放送の連続周期性の大きなノイズが混入して
いる。第2図(al、(blの比較から明らかなように
、100100O程度まで部分放電が発生しており、1
00100Oの近辺において約0.5目盛のレベル差が
検出されていることが判る。FIG. 2(b) shows a noise spectrum measured when no current is applied to the high voltage charging terminal 3. As is clear from the frequency spectrum, there is a U
Continuous periodic large noise from HF television broadcasting is mixed in. As is clear from the comparison of Figure 2 (al, (bl), partial discharge occurs up to about 100,100 O, and 1
It can be seen that a level difference of about 0.5 scale is detected near 00100O.
以上説明した通り、本発明の部分放電測定方法によると
、部分放電に基づく高周波パルス信号と周波数掃引型局
部発振器より出力される局部発振信号とを混合して中間
周波信号を発生し、この中間周波信号を検波することに
より部分放電を測定し、必要に応じて、1回の測定結果
の平均化処理によって部分放電を判定するため、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, a high frequency pulse signal based on partial discharge and a local oscillation signal output from a frequency sweep type local oscillator are mixed to generate an intermediate frequency signal, and this intermediate frequency Partial discharge is measured by detecting the signal, and if necessary, partial discharge is determined by averaging the results of one measurement, so that the following effects can be achieved.
(11外部から侵入するノイズによって影響されない精
度の高い測定結果を得ることができる。(11) It is possible to obtain highly accurate measurement results that are not affected by noise entering from the outside.
(2)1回の測定結果の平均化によって精度を更に向上
することができる。(2) Accuracy can be further improved by averaging the results of one measurement.
(3)時間に対してランダムに発生する部分放電をも適
確に測定することができる。(3) Even partial discharges that occur randomly over time can be accurately measured.
(4)部分放電によって絶縁体が劣化して寿命が短くな
るが、その初期の部分放電はレベルが小さ(、個数が少
ない。そのような状態においても、測定が可能になるの
で、処理までの時間的余裕が長くなり、対策がたて易く
なる。(4) Partial discharge deteriorates the insulator and shortens its lifespan, but the initial partial discharge is of low level (and the number of parts is small. Even in such a state, measurement is possible, so the process up to treatment can be You will have more time and it will be easier to take countermeasures.
第1図(a)、(blは本発明の一実施例を示し、(a
)はブロック図、(b)は局部発振器の周波数掃引特性
を示す説明図、第2図(al、(blは部分放電とノイ
ズの測定結果を示す説明図、第3図は従来の部分放電測
定方法を示すプロ、り図。
符号の説明
1〜・−・−電力ケーブル 2−・−−−−−−一終
端接続部3−−−−−−−・
5・−−−一−・
6−−−−−−−・
? −−−−−−−−−−
8−・−・−・
10−・−・・−・
14・・・−・
16−−−−・−−−一−
高電圧課電端子
ブロッキングコイル
結合コンデンサ
検出インピーダンス
高域通過フィルタ
減衰器
信号メモリ処理部
混合器
検波回路
A/D変換回路 15
表示部 17
9.12
増幅器
・局部発振器
制御部FIGS. 1(a) and 1(bl) show an embodiment of the present invention, and (a)
) is a block diagram, (b) is an explanatory diagram showing the frequency sweep characteristics of the local oscillator, Fig. 2 (al), (bl is an explanatory diagram showing the measurement results of partial discharge and noise, and Fig. 3 is a conventional partial discharge measurement A diagram illustrating the method. Explanation of symbols 1 - - - Power cable 2 - - - - - - - One end connection part 3 - - - - - - - - - - - - - - - - - - - - - - - - ------ - High voltage charging terminal blocking coil coupling capacitor detection impedance high pass filter attenuator signal memory processing section mixer detection circuit A/D conversion circuit 15 Display section 17 9.12 Amplifier/local oscillator control section
Claims (2)
て絶縁体の劣化を診断する部分放電測定方法において、 前記部分放電に基づく高周波パルス信号に所定の周期で
周波数が掃引される信号を混合して中間周波信号を発生
し、 前記中間周波信号を検波して前記部分放電を測定するこ
とを特徴とする部分放電測定測定信号。(1) In a partial discharge measurement method for diagnosing deterioration of an insulator by measuring partial discharge in an insulator to which a high voltage is applied, the frequency is swept at a predetermined period in a high-frequency pulse signal based on the partial discharge. A partial discharge measurement measurement signal, characterized in that the partial discharge is measured by mixing signals of the partial discharge to generate an intermediate frequency signal; and detecting the intermediate frequency signal to measure the partial discharge.
(n=1、2、3…………)、 n回の測定結果を平均化して部分放電の測定を行う請求
項第1項記載の部分放電測定方法。(2) The partial discharge is measured over n cycles (n=1, 2, 3...), and the partial discharge is measured by averaging the n measurement results. How to measure partial discharge.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP33155288A JPH067149B2 (en) | 1988-12-28 | 1988-12-28 | Partial discharge measurement method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP33155288A JPH067149B2 (en) | 1988-12-28 | 1988-12-28 | Partial discharge measurement method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH02176579A true JPH02176579A (en) | 1990-07-09 |
JPH067149B2 JPH067149B2 (en) | 1994-01-26 |
Family
ID=18244940
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP33155288A Expired - Lifetime JPH067149B2 (en) | 1988-12-28 | 1988-12-28 | Partial discharge measurement method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH067149B2 (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104267320A (en) * | 2014-10-08 | 2015-01-07 | 广西电网有限责任公司玉林供电局 | High-voltage switch cabinet partial discharge monitoring system based on ultrahigh-frequency electromagnetic wave detection |
JPWO2016157912A1 (en) * | 2015-03-31 | 2018-01-25 | 株式会社東芝 | Insulation diagnostic apparatus and insulation diagnostic method for power equipment |
JP2020101491A (en) * | 2018-12-25 | 2020-07-02 | 株式会社明電舎 | Partial discharge detector and partial discharge detection method |
-
1988
- 1988-12-28 JP JP33155288A patent/JPH067149B2/en not_active Expired - Lifetime
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104267320A (en) * | 2014-10-08 | 2015-01-07 | 广西电网有限责任公司玉林供电局 | High-voltage switch cabinet partial discharge monitoring system based on ultrahigh-frequency electromagnetic wave detection |
JPWO2016157912A1 (en) * | 2015-03-31 | 2018-01-25 | 株式会社東芝 | Insulation diagnostic apparatus and insulation diagnostic method for power equipment |
JP2020101491A (en) * | 2018-12-25 | 2020-07-02 | 株式会社明電舎 | Partial discharge detector and partial discharge detection method |
Also Published As
Publication number | Publication date |
---|---|
JPH067149B2 (en) | 1994-01-26 |
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