JPH0750143B2 - Partial discharge position locator - Google Patents
Partial discharge position locatorInfo
- Publication number
- JPH0750143B2 JPH0750143B2 JP23341387A JP23341387A JPH0750143B2 JP H0750143 B2 JPH0750143 B2 JP H0750143B2 JP 23341387 A JP23341387 A JP 23341387A JP 23341387 A JP23341387 A JP 23341387A JP H0750143 B2 JPH0750143 B2 JP H0750143B2
- Authority
- JP
- Japan
- Prior art keywords
- partial discharge
- ultrasonic
- waveform
- difference
- waveforms
- 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 - Lifetime
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- Locating Faults (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は部分放電位置標定装置に関する。The present invention relates to a partial discharge position locator.
(従来の技術) 絶縁体にある値以上の電圧を印加すると絶縁破壊を生じ
部分放電が起こる。従来から、部分放電が生じた際の急
激な電圧又は電流の変化を電気的な方法により測定し、
部分放電の位置を決定することが広く行われている。
又、部分放電により発生する機械的振動に起因して発生
する超音波を複数の超音波センサで検出してその時間差
を求め、部分放電の位置を算出する方法も行われてい
る。(Prior Art) When a voltage higher than a certain value is applied to an insulator, dielectric breakdown occurs and partial discharge occurs. Conventionally, an abrupt change in voltage or current when partial discharge occurs is measured by an electrical method,
It is widely practiced to determine the location of partial discharges.
There is also a method in which ultrasonic waves generated due to mechanical vibration generated by partial discharge are detected by a plurality of ultrasonic sensors, the time difference between them is calculated, and the position of partial discharge is calculated.
(発明が解決しようとする問題点) しかしながら、従来の電気的方法では、種々のノイズの
多い現場環境では部分放電を精度良く測定することが困
難であり、まして部分放電の位置を正確に標定すること
は極めて難しいという問題点がある。一方、超音波セン
サを用いる方法でも、周囲の種々のノイズの中から該当
する超音波信号を選択して、2つの超音波信号波形の時
間差を精度良く求めることは難しく、部分放電の位置を
標定することは不可能に近いという問題点がある。(Problems to be Solved by the Invention) However, it is difficult for the conventional electrical method to accurately measure the partial discharge in various noisy field environments, and much more, the position of the partial discharge is accurately located. This is extremely difficult. On the other hand, even with the method using the ultrasonic sensor, it is difficult to accurately select the time difference between the two ultrasonic signal waveforms by selecting the corresponding ultrasonic signal from various ambient noises, and the position of the partial discharge is located. There is a problem that it is almost impossible to do.
本発明は、上記事情に鑑みてなされたものであり、部分
放電の際に発生する超音波を複数の超音波センサで検出
して、信号波形間の相互相関係数を求めて部分放電の位
置を標定する部分放電位置標定装置を提供することを目
的とする。The present invention has been made in view of the above circumstances, and detects ultrasonic waves generated during partial discharge with a plurality of ultrasonic sensors, and obtains a cross-correlation coefficient between signal waveforms to determine the position of partial discharge. It is an object of the present invention to provide a partial discharge position locating device for locating.
(問題点を解決するための手段) 上記目的を達成するために本発明によれば、異なった位
置に設置され部分放電により発生する超音波を検出し電
気信号に変換する複数の超音波センサと、該超音波セン
サの各々の出力電気信号波形をデジタル電気信号波形に
変換して記憶する波形記憶装置と、前記デジタル信号波
形を読み取り2つのデジタル信号波形毎に相互相関係数
を計算しその最大値から超音波の超音波センサへの到達
時間差を計算し、前記到達時間差に超音波の速度を乗算
して距離差を算出し前記部分放電の位置を算出判定する
演算装置とから成る部分放電位置標定装置が提供され
る。(Means for Solving the Problems) In order to achieve the above object, according to the present invention, a plurality of ultrasonic sensors installed at different positions for detecting ultrasonic waves generated by partial discharge and converting them into electric signals A waveform storage device that converts the output electric signal waveform of each of the ultrasonic sensors into a digital electric signal waveform and stores the digital electric signal waveform, and reads the digital signal waveform to calculate a cross-correlation coefficient for each of the two digital signal waveforms. Partial discharge position consisting of an arithmetic unit for calculating the arrival time difference of the ultrasonic wave from the value to the ultrasonic sensor, calculating the distance difference by multiplying the arrival time difference by the ultrasonic velocity, and calculating the position of the partial discharge An orienting device is provided.
(作用) 複数の超音波センサが部分放電の際に発生する超音波を
夫々検出し電気信号波形に変換し、波形記憶装置がこれ
らのアナログ電気信号波形をデジタル信号波形に変換し
て記憶し、演算装置が各デジタル信号波形の1サイクル
ないし数サイクル分を読み取って、相互相関係数を計算
しその最大値から超音波の各超音波センサへの到達時間
差を求め、部分放電の位置を算出判定する。(Function) A plurality of ultrasonic sensors each detect an ultrasonic wave generated during partial discharge and convert it into an electric signal waveform, and the waveform storage device converts these analog electric signal waveforms into digital signal waveforms and stores them. The arithmetic unit reads one cycle or several cycles of each digital signal waveform, calculates the cross-correlation coefficient, finds the difference in the arrival time of ultrasonic waves to each ultrasonic sensor from the maximum value, and calculates the position of partial discharge. To do.
(実施例) 以下、本発明の実施例を添付図面に基づいて詳細に説明
する。(Example) Hereinafter, an example of the present invention will be described in detail with reference to the accompanying drawings.
第1図は本発明の部分放電位置標定装置の一実施例を示
すブロック図である。本発明の部分放電位置標定装置は
この実施例では4個の超音波センサ3a,3b,3c,3d,波形記
憶装置5,及び演算装置6から構成されている。4個の超
音波センサ3a,3b,3c,3dは電力ケーブル1の接続部2の
部分放電位置例えば4で発生した部分放電に伴う機械的
振動による超音波を検出しやすい位置に取り付けられ、
接続部2内で発生した超音波を検出して電気信号として
出力する。波形記憶装置5はA−D変換器とデジタルメ
モリとから成り、超音波接続部3a,3b,3c,3dからのアナ
ログ電気信号波形をデジタル電気信号波形に変換して、
デジタルメモリに各波形の到達時刻と共に記憶する。演
算装置6は波形記憶装置5に記憶されている1サイクル
ないし数サイクル分のデジタル電気信号波形を読み取
り、後述する相互相関係数ρxy(j)(j=0,1,2,…N−
1)最大値を計算して、超音波の部分放電位置4から各
超音波センサ3a,3b,3c,3dへの到達時間差を求め、接続
部2内の部分放電の位置を算出判定する。FIG. 1 is a block diagram showing an embodiment of the partial discharge position locating device of the present invention. In this embodiment, the partial discharge position locating device of the present invention comprises four ultrasonic sensors 3a, 3b, 3c, 3d, a waveform storage device 5, and a computing device 6. The four ultrasonic sensors 3a, 3b, 3c, 3d are attached at the partial discharge position of the connection portion 2 of the power cable 1, for example, at the position where it is easy to detect ultrasonic waves due to mechanical vibration associated with the partial discharge generated at 4,
The ultrasonic wave generated in the connection portion 2 is detected and output as an electric signal. The waveform storage device 5 is composed of an AD converter and a digital memory, and converts the analog electric signal waveform from the ultrasonic wave connecting portions 3a, 3b, 3c, 3d into a digital electric signal waveform,
The time of arrival of each waveform is stored in the digital memory. The arithmetic unit 6 reads the digital electric signal waveform for one cycle or several cycles stored in the waveform storage unit 5, and cross-correlation coefficient ρ xy (j) (j = 0, 1, 2, ...
1) The maximum value is calculated, the arrival time difference from the partial discharge position 4 of the ultrasonic waves to the ultrasonic sensors 3a, 3b, 3c, 3d is calculated, and the position of the partial discharge in the connection portion 2 is calculated and determined.
次に、第1図及び第2図を参照して本発明の部分放電位
置標定装置の作用について説明する。Next, the operation of the partial discharge position locating device of the present invention will be described with reference to FIGS. 1 and 2.
第2図は超音波センサの出力波形xi及びyi,及びその相
互相関係数ρxyの波形を示す図である。一般に、2つの
時系列データの内の2つのデジタルデータ波形をxi(i
=1,2,…N)及びyi(i=1,2,…N)とすると、これら
の2つの波形の相互相関係数ρxy(j)は次式で定義され
る。FIG. 2 is a diagram showing the output waveforms x i and y i of the ultrasonic sensor and the waveform of the cross-correlation coefficient ρ xy thereof. In general, two digital data waveforms of two time series data are calculated as x i (i
= 1,2, ... N) and y i (i = 1,2, ... N), the cross-correlation coefficient ρ xy (j) of these two waveforms is defined by the following equation.
ここで、 (2)式で与えられる相互共分散係数Rxy(j)は波形xmと
波形ym+jの類似度を示すもので両波形が最も類似してい
るときに最大値をとる。この相互共分散係数Rxy(j)は
(2)式から直接演算して求めることができるが、相互
共分散係数Rxy(j)のフーリエ変換がクロスパワースペク
トルの各成分に対応することが証明されていることから
通常は波形xmと波形ym+jのクロスパワースペクトルを求
めて、これをフーリエ逆変換して相互共分散係数Rxy(j)
を求めることが行われる。フーリエ変換及びフーリエ逆
変換は夫々高速フーリエ変換(FFT)及び高速フーリエ
逆変換が用いられる。また、Rx(0)及びRy(0)は夫々次式
で与えられる自己共分散係数Rx(j)及びRy(j)のj=0の
時の値である。 here, The mutual covariance coefficient R xy (j) given by the equation (2) indicates the similarity between the waveform x m and the waveform y m + j , and takes the maximum value when the two waveforms are the most similar. The mutual covariance coefficient R xy (j) can be obtained by directly calculating from the equation (2), but the Fourier transform of the mutual covariance coefficient R xy (j) may correspond to each component of the cross power spectrum. Since it has been proved, the cross power spectrum of the waveform x m and the waveform y m + j is usually obtained, and the inverse covariance coefficient R xy (j) is obtained by inverse Fourier transforming this.
Is asked. Fast Fourier transform (FFT) and fast Fourier inverse transform are used as the Fourier transform and the inverse Fourier transform, respectively. Further, R x (0) and R y (0) are the values of the autocovariance coefficients R x (j) and R y (j) when j = 0, respectively, given by the following equations.
この自己共分散係数Rx(j)及びRy(j)も波形xm及びymのパ
ワースペクトルを算出し、このパワースペクトルをフー
リエ逆変換することによって能率的に求められる。
(1)式で与えられる相互相関係数ρxy(j)は相互共分
散係数Rxy(j)を自己共分散係数Rx(0),Ry(0)で規準化し
たものであり、両波形xmとym+jが最も類似している時に
最大値1をとる。 The self-covariance coefficients R x (j) and R y (j) are also efficiently obtained by calculating the power spectrum of the waveforms x m and y m and subjecting this power spectrum to the inverse Fourier transform.
The cross-correlation coefficient ρ xy (j) given by the equation (1) is obtained by normalizing the cross-covariance coefficient R xy (j) by the self-covariance coefficients R x (0) and R y (0) , It takes a maximum value of 1 when both waveforms x m and y m + j are most similar.
実際に電圧ケーブル1の接続部2の部分放電により発生
した超音波を超音波センサ3a及び3bで夫々検出した結
果、各超音波センサ3a及び3bで夫々検出した結果、各超
音波センサ3a及び3bの出力波形が第2図(a)の波形xi
及び第2図(b)の波形yiとなり、相互相関係数ρ
xy(j)は演算装置6により第2図(c)に示す如く計算
された。相互相関係数ρxy(j)の最大値を与える時間、
つまり、波形xiと波形yiとが超音波センサ3a及び3bへ到
達する時間差ΔTが48μsであると計算された。As a result of actually detecting the ultrasonic waves generated by the partial discharge of the connection portion 2 of the voltage cable 1 by the ultrasonic sensors 3a and 3b, respectively, and by the ultrasonic sensors 3a and 3b respectively, the ultrasonic sensors 3a and 3b are detected. The output waveform of is the waveform x i of Fig. 2 (a)
And the waveform y i in FIG. 2 (b), the cross-correlation coefficient ρ
xy (j) was calculated by the arithmetic unit 6 as shown in FIG. The time that gives the maximum value of the cross-correlation coefficient ρ xy (j) ,
That is, it was calculated that the time difference ΔT between the waveforms x i and the waveform y i reaching the ultrasonic sensors 3a and 3b was 48 μs.
この時間差ΔTにこの接続部2の材料中の音速v、例え
ば、1900m/secを乗算すれば、部分放電発生位置4から
超音波センサ3aと超音波センサ3bとの距離差ΔS=ΔT
×vが求められる。従って、第2図の例では距離差ΔS
はΔS=48×10-6×1900=0.0912(m)=9.12(cm)と
なる。この距離差ΔSは第1図における超音波の伝搬経
路Aと伝搬経路Bの長さの差を示している。If this time difference ΔT is multiplied by the sound velocity v in the material of the connecting portion 2, for example, 1900 m / sec, the distance difference ΔS = ΔT from the partial discharge occurrence position 4 to the ultrasonic sensor 3a and the ultrasonic sensor 3b.
Xv is required. Therefore, in the example of FIG. 2, the distance difference ΔS
Is ΔS = 48 × 10 −6 × 1900 = 0.0912 (m) = 9.12 (cm). This distance difference ΔS indicates the difference in length between the ultrasonic wave propagation path A and the ultrasonic wave propagation path B in FIG.
以上述べた時間差の計算を超音波センサ3cと超音波セン
サ3dとの間でも行って距離差を求め、超音波の伝搬経路
Cとの差及び伝搬経路Dとの長さの差を求めれば、部分
放電位置4を正確に算出し判定することができる。The calculation of the time difference described above is also performed between the ultrasonic sensor 3c and the ultrasonic sensor 3d to obtain the distance difference, and if the difference between the ultrasonic wave propagation path C and the propagation path D is obtained, The partial discharge position 4 can be accurately calculated and determined.
(発明の効果) 以上説明したように、本発明によれば、異なった位置に
設置され部分放電により発生する超音波を検出し電気信
号に変換する複数の超音波センサと、該超音波センサの
各々の出力電気信号波形をデジタル電気信号波形に変換
して記憶する波形記憶装置と、前記デジタル信号波形を
読み取り2つのデジタル信号波形毎に相互相関係数を計
算しその最大値から超音波の超音波センサへの到達時間
差を計算し、前記到達時間差に超音波の速度を乗算して
距離差を算出し前記部分放電の位置を算出判定する演算
装置とから成ることにより、特別に熟練を必要とせずに
ノイズの多い超音波センサの出力から正確迅速に2つの
波形間の時間差を算出し、これを用いて部分放電の位置
標定ができ、部分放電を確実に測定することができるた
めに絶縁破壊事故を未然に防止でき、手作業によって調
整する必要がないために完全な自動化が可能であるとい
う効果が得られる。(Effects of the Invention) As described above, according to the present invention, a plurality of ultrasonic sensors installed at different positions to detect ultrasonic waves generated by partial discharge and convert them into electric signals, and the ultrasonic sensor A waveform storage device that converts each output electric signal waveform into a digital electric signal waveform and stores the converted waveform, and a cross-correlation coefficient is calculated for each of the two digital signal waveforms by reading the digital signal waveforms. It requires a special skill by being composed of an arithmetic unit that calculates the arrival time difference at the sound wave sensor, calculates the distance difference by multiplying the arrival time difference by the ultrasonic velocity, and calculates and determines the position of the partial discharge. Instead, the time difference between the two waveforms can be calculated accurately and quickly from the output of a noisy ultrasonic sensor, and the position of the partial discharge can be located using this, and the partial discharge can be reliably measured. In addition, it is possible to prevent a dielectric breakdown accident in advance, and there is no need for manual adjustment, so that it is possible to achieve complete automation.
第1図は本発明の部分放電位置標定装置の一実施例を示
すブロック図、第2図は超音波センサの出力波形xi、yi
及び相互相関係数ρxyの波形を示す図である。 1……電圧ケーブル、2……接続部、3a,3b,3c,3d……
超音波センサ、4……部分放電位置、5……波形記憶装
置、6……演算装置。FIG. 1 is a block diagram showing an embodiment of the partial discharge position locating device of the present invention, and FIG. 2 is an output waveform x i , y i of an ultrasonic sensor.
FIG. 7 is a diagram showing a waveform of a cross correlation coefficient ρ xy . 1 ... voltage cable, 2 ... connection part, 3a, 3b, 3c, 3d ...
Ultrasonic sensor, 4 ... Partial discharge position, 5 ... Waveform storage device, 6 ... Computing device.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 丸山 義雄 千葉県市原市八幡海岸通6 古河電気工業 株式会社千葉電線製造所内 (72)発明者 山下 泰浩 千葉県市原市八幡海岸通6 古河電気工業 株式会社千葉電線製造所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Yoshio Maruyama 6 Yawata Kaigan Dori, Ichihara City, Chiba Furukawa Electric Co., Ltd. Chiba Cable Manufacturing Co., Ltd. (72) Yasuhiro Yamashita 6 Hachiman Kaido Dori, Ichihara City, Chiba Furukawa Electric Co., Ltd. Company Chiba Electric Wire Works
Claims (1)
生する超音波を検出し電気信号に変換する複数の超音波
センサと、該超音波センサの各々の出力電気信号波形を
デジタル電気信号波形に変換して記憶する波形記憶装置
と、前記デジタル信号波形を読み取り2つのデジタル信
号波形毎に相互相関係数を計算しその最大値から超音波
の超音波センサへの到達時間差を計算し、前記到達時間
差に超音波の速度を乗算して距離差を算出し前記部分放
電の位置を算出判定する演算装置とから成ることを特徴
とする部分放電位置標定装置。1. A plurality of ultrasonic sensors installed at different positions to detect ultrasonic waves generated by partial discharge and convert them into electric signals, and output electric signal waveforms of the ultrasonic sensors are converted into digital electric signal waveforms. A waveform storage device that converts and stores the digital signal waveform, calculates a cross-correlation coefficient for each of the two digital signal waveforms, calculates a difference in arrival time of ultrasonic waves from the maximum value to the ultrasonic sensor, A partial discharge position locating device, comprising: an arithmetic unit for calculating and determining the position of the partial discharge by calculating a distance difference by multiplying the time difference by the ultrasonic velocity.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23341387A JPH0750143B2 (en) | 1987-09-17 | 1987-09-17 | Partial discharge position locator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23341387A JPH0750143B2 (en) | 1987-09-17 | 1987-09-17 | Partial discharge position locator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6474465A JPS6474465A (en) | 1989-03-20 |
| JPH0750143B2 true JPH0750143B2 (en) | 1995-05-31 |
Family
ID=16954671
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP23341387A Expired - Lifetime JPH0750143B2 (en) | 1987-09-17 | 1987-09-17 | Partial discharge position locator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0750143B2 (en) |
Families Citing this family (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE19617243A1 (en) * | 1996-04-30 | 1997-11-06 | Horstmann Gmbh Dipl Ing H | Method and device for determining the distance of a cable fault |
| BR112013033908A2 (en) * | 2011-07-05 | 2017-12-12 | Koninklijke Philips Nv | Method and device for determining when an artery of interest under changing pressure changes from open to closed or vice versa |
| CN110865286A (en) * | 2019-11-25 | 2020-03-06 | 武汉三相电力科技有限公司 | Discharge phase calculation method |
| CN112327108A (en) * | 2020-10-09 | 2021-02-05 | 国网冀北电力有限公司检修分公司 | A method for denoising and time difference identification of partial discharge ultrasonic signal of tank circuit breaker |
| JPWO2025004394A1 (en) * | 2023-06-28 | 2025-01-02 | ||
| CN116973702B (en) * | 2023-07-31 | 2024-04-05 | 上海莫克电子技术有限公司 | Signal identification method and system applied to GIS partial discharge test |
| CN118673392B (en) * | 2024-08-13 | 2025-01-21 | 国网上海市电力公司 | A switch cabinet partial discharge diagnosis method and system |
-
1987
- 1987-09-17 JP JP23341387A patent/JPH0750143B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6474465A (en) | 1989-03-20 |
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