JPS634148B2 - - Google Patents
Info
- Publication number
- JPS634148B2 JPS634148B2 JP7629280A JP7629280A JPS634148B2 JP S634148 B2 JPS634148 B2 JP S634148B2 JP 7629280 A JP7629280 A JP 7629280A JP 7629280 A JP7629280 A JP 7629280A JP S634148 B2 JPS634148 B2 JP S634148B2
- Authority
- JP
- Japan
- Prior art keywords
- gate
- integrator
- distribution line
- antenna
- high voltage
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R31/00—Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
- G01R31/08—Locating faults in cables, transmission lines, or networks
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Locating Faults (AREA)
Description
【発明の詳細な説明】
この発明は、高電圧パルス印加法による架空配
電線路の事故点の探査に使用する受信装置の改良
に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a receiving device used for detecting a fault point on an overhead power distribution line using a high voltage pulse application method.
架空配電線路に接地事故が生じたときは、高電
圧パルス印加法により事故点の探査を行つてい
る。これは停電状態の線路区間に高電圧パルスを
印加し、配電線路を流れるパルス電流をアンテナ
付きの受信装置により検出して接地事故点の探査
を行うものである。 When a grounding fault occurs on an overhead power distribution line, the point of fault is detected using a high-voltage pulse application method. This involves applying a high voltage pulse to a section of line that is in a power outage state, and detecting the pulse current flowing through the distribution line using a receiver equipped with an antenna to locate the point of a ground fault.
このような探査原理を以下説明する。第1図は
接地事故点を探査している状態を示す図である。
図において、1は高電圧パルス発生器、2は配電
線路、3は大地、4は接地事故点、Rgは接地事
故抵抗、Cgは接地事故点以降の対地静電容量、
5は配電線に近接するサーチコイル形アンテナ、
6は受信装置、7はアンテナ5と受信装置6を接
続するリード線である。 The principle of such exploration will be explained below. FIG. 1 is a diagram showing a state in which a grounding accident point is being searched.
In the figure, 1 is the high voltage pulse generator, 2 is the distribution line, 3 is the ground, 4 is the ground fault point, Rg is the ground fault resistance, Cg is the ground capacitance after the ground fault point,
5 is a search coil antenna close to the power distribution line;
6 is a receiving device, and 7 is a lead wire connecting the antenna 5 and the receiving device 6.
このような構成において、高電圧パルス発生器
1により配電線2と大地3との間に高電圧パルス
を印加し、アンテナ5付きの受信装置6で配電線
2に流れる電流を検出して接地事故点を探査す
る。すなわち、第2図は高電圧パルス発生器1が
発生する電圧パルスの波形であり、この高電圧パ
ルスの印加により線路に流れる電流を1回積分す
れば、(イ)線路に接地事故がない場合にはその積分
値は零に、(ロ)事故があつて、パルス発生器1から
その事故までの区間では、その積分値は事故電流
値に、(ハ)事故があつて、その事故を通り過ぎた後
の区間ではその積分値は零になるので一定時間後
に積分値を読み取ることにより上記3種類の値を
判別して事故点の探査を行う。 In such a configuration, a high voltage pulse generator 1 applies a high voltage pulse between the power distribution line 2 and the ground 3, and a receiving device 6 equipped with an antenna 5 detects the current flowing through the power distribution line 2, thereby preventing a grounding accident. Explore points. In other words, Figure 2 shows the waveform of the voltage pulse generated by the high voltage pulse generator 1, and if the current flowing through the line due to the application of this high voltage pulse is integrated once, (a) If there is no grounding fault on the line, (b) There is an accident, and in the section from pulse generator 1 to the accident, the integral value becomes zero, (c) There is an accident, and the integral value is the fault current value. In the section after the accident, the integral value becomes zero, so by reading the integral value after a certain period of time, the above three types of values are discriminated and the accident point is searched.
しかしながらサーチコイル形のアンテナではア
ンテナ出力が、線路電流波形を1回ある種の微分
回路を通したものと等価であることから、積分を
2回行なうことにより上記と同等の結果を得る。
第3図は従来の事故点探査用受信装置の一例で、
8は増幅器、9はゲート、10は第1積分器、1
1は第2積分器、12は検出表示ゲート、13は
検出メータ、14はゲート信号発生器である。 However, in the case of a search coil type antenna, the antenna output is equivalent to passing the line current waveform through a kind of differentiation circuit once, so by performing the integration twice, the same result as above can be obtained.
Figure 3 shows an example of a conventional receiving device for accident point detection.
8 is an amplifier, 9 is a gate, 10 is a first integrator, 1
1 is a second integrator, 12 is a detection display gate, 13 is a detection meter, and 14 is a gate signal generator.
このような、受信装置6の動作波形について説
明すると、第4図は線路に事故がない場合、第5
図は線路に事故があつて高電圧パルス発生器1か
らその事故までの区間の場合、第6図は事故点以
降の場合でそれぞれaは線路電流、bはアンテナ
出力、g1はゲート信号発生器14のゲート9への
信号、cは第1積分器10の出力、dは第2積分
器11の出力、g0はゲート信号発生器14の検出
表示ゲート12への信号、eは検出メータ13の
振れである。 To explain the operating waveforms of the receiving device 6, FIG. 4 shows that when there is no accident on the track,
The figure shows the section from the high voltage pulse generator 1 to the fault when there is an accident on the line, and Figure 6 shows the case after the fault point, where a is the line current, b is the antenna output, and g 1 is the gate signal generation. c is the output of the first integrator 10, d is the output of the second integrator 11, g0 is the signal to the detection display gate 12 of the gate signal generator 14, e is the detection meter It is a swing of 13.
次に、受信装置6の動作について説明する。ア
ンテナ5からの出力信号を増幅器8で充分な大き
さに増幅し、この信号の最初の時点をゲート信号
発生器14が検出し、高電圧パルスのパルス幅よ
り長い時間ゲート9を開き、第1、第2積分器1
0,11により2回積分を行う。次に一定時間後
検出表示ゲート12を開き、検出メータ13によ
り事故の状態を判別する。 Next, the operation of the receiving device 6 will be explained. The output signal from the antenna 5 is amplified to a sufficient magnitude by an amplifier 8, and the gate signal generator 14 detects the first point in time of this signal and opens the gate 9 for a time longer than the pulse width of the high voltage pulse. , second integrator 1
Integrate twice using 0 and 11. Next, after a certain period of time, the detection display gate 12 is opened, and the detection meter 13 determines the state of the accident.
ところで、数KΩ以上の高抵抗事故では、上記
配電線路電流の積分値が非常に小さくなるため、
増幅器の温度ドリフト及び近隣を流れる商用周波
電流の影響が無視できなくなるため高抵抗事故の
探査には難点があつた。 By the way, in a high resistance fault of several kilohms or more, the integrated value of the distribution line current becomes very small, so
Detecting high resistance faults was difficult because the effects of amplifier temperature drift and commercial frequency current flowing nearby could no longer be ignored.
したがつて、従来の受信装置は高抵抗事故の探
査を行うには探査前に受信装置の校正操作が必要
となつていた。さらに、大きな商用周波電流が流
れている場所(共同地線を流れる迷走電流が大き
な区間あるいは2重架線区間)では誤探査を招き
探査に多大の時間を費す欠点があつた。 Therefore, in order to search for high-resistance faults with conventional receiving devices, it has been necessary to calibrate the receiving device before the search. Furthermore, in areas where large commercial frequency currents are flowing (sections with large stray currents flowing through public ground lines or sections with double overhead wires), there is a drawback that erroneous detections may occur and a large amount of time is required for the search.
この発明は上記のような従来のものの欠点を除
去するためになされたもので受信装置に増幅器の
温度補償機能及び商用周波電流による誤動作除去
機能を設けて、校正操作を不用にし、さらに商用
周波電流の流れている区間でも高抵抗事故が極め
て良好に探査できる受信装置を提供することを目
的としている。 This invention was made in order to eliminate the above-mentioned drawbacks of the conventional system, and it provides a receiving device with an amplifier temperature compensation function and a function to remove malfunctions due to commercial frequency current, thereby eliminating the need for calibration operations and further reducing the need for commercial frequency current. The object of the present invention is to provide a receiving device that can extremely effectively detect high resistance faults even in sections where the wind is flowing.
以下、この発明の一実施例について説明する。
第7図はこの発明の配電線事故点探査用受信装置
の一実施例を示すブロツク図で、8は増幅器、9
は第1ゲート、15は第2ゲート、16は減算
器、10は第1積分器、11は第2積分器、12
は検出表示ゲート、13は検出メータ、14はゲ
ート信号発生器であり、これら全体を17で示し
ている。 An embodiment of the present invention will be described below.
FIG. 7 is a block diagram showing an embodiment of a receiving device for detecting a fault point in a distribution line according to the present invention, in which 8 is an amplifier;
is the first gate, 15 is the second gate, 16 is the subtracter, 10 is the first integrator, 11 is the second integrator, 12
13 is a detection display gate, 13 is a detection meter, and 14 is a gate signal generator, all of which are indicated by 17.
次にこの受信装置17の動作について説明す
る。アンテナ5からの出力信号を増幅器8で充分
な大きさに増幅して、この信号の最初の時点をゲ
ート信号発生器14が検出して、一連のゲート開
信号を発生する。まず、受信時点より商用周波数
の1周期の整数倍で、かつ高電圧パルスのパルス
幅より長い時間第1ゲート9を開き、増幅器8の
出力を通過させる。次に(第1ゲート出力)−(第
2ゲートの出力)の減算機能を持つた減算器16
を経由して、第1積分器10、第2積分器11で
2回積分をする。次に第1ゲート9を閉じた時点
から商用周波数の1周期または1周期より非常に
短い時間例えば10μs程度積分を休止して第1積分
器10の積分内容を初期状態に戻す。次に第1ゲ
ートと同じ時間第2ゲート15を開き増幅器8の
出力は減算器16により極性反転(第1ゲート9
が閉じているため)して、第1ゲート9が開のと
きと同様に2回積分する。次に高電圧パルス印加
周期より短かい時間検出表示ゲート12を開き検
出メータ13に第2積分器11の内容を指示す
る。第8図は上記の動作波形でaは線路電流、b
は増幅器8の出力、g1は第1ゲート開区間、cは
第1積分器10の出力、dは第2積分器11の出
力、g3は積分休止区間及び第1積分器10の初期
設定(リセツト)信号、g2は第2ゲート開区間、
g0は検出表示ゲート開区間、eは検出メータ13
の振れである。 Next, the operation of this receiving device 17 will be explained. The output signal from antenna 5 is amplified to a sufficient magnitude by amplifier 8, and the first instant of this signal is detected by gate signal generator 14 to generate a series of gate open signals. First, the first gate 9 is opened for a time that is an integral multiple of one cycle of the commercial frequency and longer than the pulse width of the high voltage pulse from the time of reception, and the output of the amplifier 8 is allowed to pass. Next, a subtractor 16 with a subtraction function of (first gate output) - (second gate output)
The first integrator 10 and the second integrator 11 perform integration twice. Next, from the time when the first gate 9 is closed, the integration is stopped for one period of the commercial frequency or for a period much shorter than one period, for example, about 10 μs, and the integration contents of the first integrator 10 are returned to the initial state. Next, the second gate 15 is opened for the same time as the first gate, and the output of the amplifier 8 is polarized by the subtracter 16 (first gate 9
is closed), and the integration is performed twice in the same way as when the first gate 9 is open. Next, the detection display gate 12 is opened for a time shorter than the high voltage pulse application period, and the content of the second integrator 11 is indicated to the detection meter 13. Figure 8 shows the above operating waveforms, where a is the line current and b
is the output of the amplifier 8, g1 is the first gate open period, c is the output of the first integrator 10, d is the output of the second integrator 11, g3 is the integration pause period and the initial setting of the first integrator 10. (reset) signal, g 2 is the second gate open section,
g 0 is the detection display gate open section, e is the detection meter 13
This is the fluctuation.
次に増幅器8が温度ドリフト等により出力に直
流成分が生じている場合の除去動作について第9
図の動作波形により説明する。なお、この図には
線路電流は含まれていない。第9図bは増幅器8
に入力信号が無いときの出力直流電圧Edである。
g1は第1ゲート9の開区間を示し、このときの第
1、第2積分器10,11の出力波形はc,dに
示すような波形となる。g3は積分休止区間及び第
1積分器10の初期設定で、これにより第1積分
器10の積分内容は、初期状態に戻される。g2は
第2ゲート15の開区間を示し、第1積分器10
は減算器16により逆極性に積分され、第2積分
器11の出力は零となる。このことから増幅器8
は、第1ゲート9開から第2ゲート15閉迄の区
間のみ安定に動作すれば探査性能に影響を与えな
いわけで、温度特性の様な周期の長いドリフトに
対しては極めて効果的である。 Next, Section 9 describes the removal operation when the amplifier 8 has a DC component in its output due to temperature drift, etc.
This will be explained using the operation waveforms shown in the figure. Note that this figure does not include line current. Figure 9b shows the amplifier 8
This is the output DC voltage Ed when there is no input signal.
g 1 indicates the open section of the first gate 9, and the output waveforms of the first and second integrators 10 and 11 at this time are waveforms as shown in c and d. g3 is an integration pause interval and an initial setting of the first integrator 10, whereby the integration contents of the first integrator 10 are returned to the initial state. g 2 indicates the open section of the second gate 15, and the first integrator 10
is integrated with opposite polarity by the subtracter 16, and the output of the second integrator 11 becomes zero. From this, amplifier 8
As long as it operates stably only in the section from the first gate 9 open to the second gate 15 closed, it will not affect exploration performance, and is extremely effective against long-period drifts such as temperature characteristics. .
次にアンテナ5が商用周波電流の誘導を受けた
場合の除去動作について第10図の動作波形によ
り説明する。なお、この図も第9図同様線路電流
は含まれていない。第10図bは増幅器8の出力
に現れる商用周波電流の誘導波形である。第1ゲ
ート9の開区間g1は商用周波数の周期の整数倍で
あるから第1、第2積分器10,11の出力は
c,dに示す様に位相は異なるが第1ゲート9が
閉じる時点では零となる。g3は積分休止区間でこ
のとき第1積分器10は初期状態に戻されるが積
分値が零であるため変化しない。第2ゲート15
の開区間g2も第1ゲート9の開区間g1と同一時間
であるため減算器16により極性が反転されても
第2ゲート15が閉じる時点では積分値は零とな
る。なおこの原理によりいかなる位相から積分開
始してもまた奇数、偶数高調波を含む歪み波にお
いても除去が可能である。 Next, the removal operation when the antenna 5 receives induction of a commercial frequency current will be explained using the operating waveforms shown in FIG. Note that, like FIG. 9, this figure also does not include the line current. FIG. 10b shows the induced waveform of the commercial frequency current appearing at the output of the amplifier 8. Since the open interval g 1 of the first gate 9 is an integral multiple of the period of the commercial frequency, the outputs of the first and second integrators 10 and 11 have different phases as shown in c and d, but the first gate 9 closes. It becomes zero at this point. g 3 is an integration pause interval, at which time the first integrator 10 is returned to its initial state, but since the integral value is zero, it does not change. 2nd gate 15
Since the open interval g 2 of is also the same time as the open interval g 1 of the first gate 9, even if the polarity is reversed by the subtracter 16, the integral value becomes zero at the time when the second gate 15 closes. Note that according to this principle, distortion waves including odd and even harmonics can be removed no matter what phase the integration starts from.
以上のように、この発明によれば、増幅器の温
度ドリフト補償機能及び商用周波電流による誤動
作除去機能を受信装置に具備させたので、探査前
の校正操作が不用でかつ、2重架線区間等商用周
波電流の影響を受けやすい場所でも極めて良好に
高抵抗事故の探査ができるようになるものであ
る。 As described above, according to the present invention, the receiving device is equipped with an amplifier temperature drift compensation function and a function to eliminate malfunctions caused by commercial frequency current. This makes it possible to very effectively search for high resistance faults even in places that are easily affected by frequency currents.
第1図は接地事故点を探査している状態を示す
図、第2図は第1図の高電圧パルス発生器の高電
圧パルスの波形を示す図、第3図は従来の事故点
探査用受信装置のブロツク図、第4図、第5図、
第6図は探査原理を示す動作波形図、第7図はこ
の発明の受信装置のブロツク図、第8図、第9
図、第10図はこの発明の原理を示す動作波形図
である。
図において5はアンテナ、17は受信装置、8
は増幅器、9は第1ゲート、15は第2ゲート、
16は減算器、10は第1積分器、11は第2積
分器、13は検出メータ、14はゲート信号発生
器である。なお図中同一符号は同一または相当部
分を示す。
Figure 1 is a diagram showing the state in which a ground fault point is being searched, Figure 2 is a diagram showing the waveform of the high voltage pulse of the high voltage pulse generator of Figure 1, and Figure 3 is a diagram showing the state in which the ground fault point is being searched. Block diagram of the receiving device, Fig. 4, Fig. 5,
FIG. 6 is an operating waveform diagram showing the principle of exploration, FIG. 7 is a block diagram of the receiving device of the present invention, and FIGS.
10 are operational waveform diagrams showing the principle of the present invention. In the figure, 5 is an antenna, 17 is a receiving device, and 8
is an amplifier, 9 is a first gate, 15 is a second gate,
16 is a subtracter, 10 is a first integrator, 11 is a second integrator, 13 is a detection meter, and 14 is a gate signal generator. Note that the same reference numerals in the figures indicate the same or corresponding parts.
Claims (1)
電線に繰返し印加される高電圧パルスにより上記
配電線に流れるパルス電流を検出するアンテナ付
きの配電線事故点探査用受信装置において、上記
アンテナで受信した信号を通過させ、並列配置さ
れた第1および第2のゲート、これら第1、第2
ゲートを通過してきた上記アンテナの受信信号を
減算する減算器、リセツト機能を持つた第1積分
器と、第2積分器とを直列に配置した積分器、上
記第2積分器の積分値を指示する指示器、上記ア
ンテナで受信した信号の開始時から商用電源周波
数の整数倍の周期に相当し、かつ上記高電圧パル
スのパルス幅より大である時間第1ゲートを開か
せ、続く1周期休止して、その後第1ゲートと同
じ時間第2ゲートを開かせるゲート信号発生器を
備えた受信装置。1. In a distribution line fault point detection receiver equipped with an antenna that detects pulse current flowing through the distribution line by high voltage pulses repeatedly applied to the distribution line in order to detect fault points on the distribution line, first and second gates arranged in parallel to pass the received signal;
A subtracter for subtracting the received signal of the antenna that has passed through the gate, an integrator having a reset function and a first integrator and a second integrator arranged in series, and an instruction for the integral value of the second integrator. An indicator to open the first gate for a period corresponding to an integral multiple of the commercial power frequency from the start of the signal received by the antenna and larger than the pulse width of the high voltage pulse, followed by one period of pause. and a gate signal generator for opening a second gate for the same time as the first gate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7629280A JPS573058A (en) | 1980-06-06 | 1980-06-06 | Radio receiver |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7629280A JPS573058A (en) | 1980-06-06 | 1980-06-06 | Radio receiver |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS573058A JPS573058A (en) | 1982-01-08 |
| JPS634148B2 true JPS634148B2 (en) | 1988-01-27 |
Family
ID=13601258
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7629280A Granted JPS573058A (en) | 1980-06-06 | 1980-06-06 | Radio receiver |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS573058A (en) |
-
1980
- 1980-06-06 JP JP7629280A patent/JPS573058A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS573058A (en) | 1982-01-08 |
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