JPH0522458B2 - - Google Patents
Info
- Publication number
- JPH0522458B2 JPH0522458B2 JP24147285A JP24147285A JPH0522458B2 JP H0522458 B2 JPH0522458 B2 JP H0522458B2 JP 24147285 A JP24147285 A JP 24147285A JP 24147285 A JP24147285 A JP 24147285A JP H0522458 B2 JPH0522458 B2 JP H0522458B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- zero
- circuit breaker
- shunt reactor
- reactor
- 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 - Fee Related
Links
- 239000003990 capacitor Substances 0.000 claims description 7
- 230000005540 biological transmission Effects 0.000 description 13
- 230000000694 effects Effects 0.000 description 3
- 230000001052 transient effect Effects 0.000 description 3
- 238000001514 detection method Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000002159 abnormal effect Effects 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000001681 protective effect Effects 0.000 description 1
Landscapes
- Emergency Protection Circuit Devices (AREA)
Description
【発明の詳細な説明】
本発明は、静電容量の大きい送電線に接地さ
れ、系統の電流零なしの解消に好適な充電電流補
償装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a charging current compensator that is grounded to a power transmission line with a large capacitance and is suitable for eliminating zero current in a system.
例えば、昭和55年電気学会全国大会論文No.875
「故障電流のゼロミス発生予測」に示されるよう
に、電力系統事故時に発生する直流が交流の振幅
よりも大きいと、交流の数サイクルにわたつて電
流の零点が生じないという現象の発生し得ること
が知られている。
For example, 1981 National Institute of Electrical Engineers of Japan Conference Paper No.875
As shown in "Prediction of Zero Miss Occurrence of Fault Current", if the amplitude of the DC generated during a power system fault is greater than the amplitude of the AC, a phenomenon may occur in which the zero point of the current does not occur over several cycles of the AC. It has been known.
現状は、この電流零なし現象の発生にもかかわ
らず事故の検出による遮断器の開放指令が遮断器
に与えられている。 Currently, a command to open the circuit breaker is given to the circuit breaker due to the detection of an accident despite the occurrence of this no-current phenomenon.
この場合、遮断器は機械的に極間を開放してい
るが、電気的には直流が印加され続けており、ア
ークで接続された状態となり、接点溶解などの遮
断器破損を引き起す可能性がある。また、このこ
と以上に、長時間事故除去できないことにより電
力系統の安定度低下が問題である。 In this case, the circuit breaker mechanically opens the poles, but electrically DC continues to be applied, creating an arc-connected state that may cause circuit breaker damage such as contact melting. There is. Further, more than this, the problem is that the stability of the power system decreases due to the inability to eliminate faults for a long time.
この電流零なし現象の発生をいかにして阻止
し、発生後はいかにしてこれと速やかに減衰せし
め、遮断器、あるいは、保護継電器をいかに対応
せしめるかといつた観点から種々の検討が成され
ている。しかし、これといつた決めてのないのが
実情である。 Various studies have been conducted from the viewpoints of how to prevent this no-current phenomenon from occurring, how to quickly attenuate it after it occurs, and how to respond to it with circuit breakers or protective relays. There is. However, the reality is that there is no fixed answer.
この電流零なし現象は、超高圧系統で発生し易
いといわれている。 This non-zero current phenomenon is said to easily occur in ultra-high voltage systems.
以上のことから本発明の目的は、静電容量の大
きい送電線において、電流零なしを速やかに解消
することのできる充電電流補償装置を提供するこ
とにある。
In light of the above, an object of the present invention is to provide a charging current compensator that can quickly eliminate the problem of zero current in a power transmission line with a large capacitance.
超高圧送電系統においては、充電電流補償及び
不平衡事故時の異常電圧の抑制等のために、母線
や送電線と大地間に分路リアクトルを設置するこ
とが不可欠である。本発明では、分路リアクトル
に直列にコンデンサを設置することにより、送電
線事故時に分路リアクトルより流出する電流に低
次周波数振動をおこさせ、この電流により、遮断
器を通過する電流に零点を生ぜしめ、速やかに遮
断動作を可能にしようとするものである。
In ultra-high voltage power transmission systems, it is essential to install a shunt reactor between the bus bar or transmission line and the ground in order to compensate for charging current and suppress abnormal voltage in the event of an unbalanced accident. In the present invention, by installing a capacitor in series with the shunt reactor, a low-order frequency oscillation is caused in the current flowing out from the shunt reactor in the event of a transmission line fault, and this current causes a zero point in the current passing through the circuit breaker. This is to enable quick shutoff operation.
本発明の適用される従来の超高圧系統の一例を
第2図により説明する。同図は電気所S1が変圧器
Tr1,Tr2、送電線L1〜L3を介して電気所S2に電
力を送つている例を示したものであり、送電線
L1〜L3の両端には遮断器CB1〜CB6が設置されて
いる。その上、送電線の静電容量を補償するた
め、上記遮断器CBの母線側に分路リアクトルLh1
〜Lh6が設置されている。このような系統におい
て、送電線L1〜L3の受電側の点、この図では例
えば地点Fで2線短絡が生ずると、送電線の遅れ
相、すなわち、遮断器CB2を通過する電流に電流
零なしが生ずる。この理由は、事故前潮流により
定まる直流分及び事故発生時の電圧により定まる
直流分及び送電線の静電容量により生ずる直流分
が相加わる方向に作用するためである。母線側に
分路リアクトルを設置した場合には、第4図に示
すように、過渡的には、分路リアクトルLに事故
時に流れていた電流が事故点Fを介して流出する
(図中のil)ため、事故発生位相によつては、過
渡直流分電流の増大をまねき、電流零なしは発生
しやすくなる。同図でE,Leは各各等価電源及
び電源側の等価リアクタンスを示す。このため、
事故の検出により遮断器CBに遮断指令を発して
も、遮断器は開放できず、遮断器が破損すること
が懸念されている。本発明は前記の欠点を補なお
うとするものである。第1図は、本発明の実施例
を示したものであり、分路リアクトルLh1〜Lh6に
直列に静電容量C1〜C5を設けてあることが本発
明の特徴である。
An example of a conventional ultra-high pressure system to which the present invention is applied will be explained with reference to FIG. In the figure, electric station S 1 is a transformer.
This shows an example in which power is sent to the electric station S2 via T r1 , T r2 , and power transmission lines L 1 to L 3 .
Circuit breakers CB 1 to CB 6 are installed at both ends of L 1 to L 3 . Moreover, in order to compensate for the capacitance of the transmission line, a shunt reactor L h1 is installed on the bus side of the circuit breaker CB.
~L h6 is installed. In such a system, if a two-wire short circuit occurs at a point on the receiving side of power transmission lines L 1 to L 3 , for example at point F in this figure, the current passing through the lagging phase of the transmission line, that is, circuit breaker CB 2 , will No current zero occurs. The reason for this is that the DC component determined by the power flow before the accident, the DC component determined by the voltage at the time of the accident, and the DC component generated by the capacitance of the power transmission line act in the direction of adding to each other. When a shunt reactor is installed on the busbar side, as shown in Figure 4, the current that was flowing through the shunt reactor L at the time of the accident flows out through the fault point F (as shown in Figure 4). il), depending on the phase in which the fault occurs, this may lead to an increase in the transient DC current, making it more likely that the current will not reach zero. In the figure, E and Le indicate each equivalent power supply and the equivalent reactance on the power supply side. For this reason,
Even if a shutdown command is issued to the circuit breaker CB upon detection of an accident, the circuit breaker cannot be opened, and there is concern that the circuit breaker may be damaged. The present invention seeks to compensate for the aforementioned drawbacks. FIG. 1 shows an embodiment of the present invention, and a feature of the present invention is that capacitances C 1 to C 5 are provided in series with the shunt reactors L h1 to L h6 .
第3図は本発明で提案する分路リアクトルの効
果を説明するためのものであり、同図でCは静電
容量である。 FIG. 3 is for explaining the effect of the shunt reactor proposed by the present invention, and in the same figure, C is the capacitance.
第3図の場合には、F点の事故によりリアクト
ルL及びコンデンサCに印加されていた電圧によ
り、遮断器通過電流に低次調波電流が生ずる。こ
の時の周波数は
で定まり、この電流の大きさは、次のように定ま
る。 In the case of FIG. 3, due to the voltage applied to the reactor L and capacitor C due to the fault at point F, a low-order harmonic current is generated in the current passing through the circuit breaker. The frequency at this time is The magnitude of this current is determined as follows.
ここで、Vは分路リアクトル端子電圧とする。 Here, V is the shunt reactor terminal voltage.
この電流ioが潮流より定まる過渡直流分電流ip、
充電電流より定まる過渡直流分icの和より大きく
なつた場合に、合成電流は零点を有し零なしは解
消する。これらの関係より零なしの解消する条件
は、
となる。 This current i o is determined by the power flow as a transient DC current i p ,
When the current becomes larger than the sum of the transient direct current components i c determined by the charging current, the composite current has a zero point and is no longer zero. From these relationships, the conditions for eliminating zero are: becomes.
次に、分路リアクトルに直列に設けるコンデン
サの値につき述べる。 Next, we will discuss the value of the capacitor installed in series with the shunt reactor.
分路リアクトルの補償度をγ、分路リアクトル
のリアクタンス分に対するコンデンサの系統周波
数におけるインピーダンスの比をηとすると、
ω0L=1/ω0Clγ ……(4)
ω0Lη=1/ω0C ……(5)
ここで、Cl;送電線の対値静電容量、ω0=2πf
とする。 If the compensation degree of the shunt reactor is γ, and the ratio of the capacitor's impedance at the system frequency to the reactance of the shunt reactance is η, then ω 0 L=1/ω 0 Clγ ……(4) ω 0 Lη=1/ω 0 C ……(5) Here, Cl: Pairwise capacitance of the transmission line, ω 0 = 2πf
shall be.
(3)〜(5)式からηを求めると、
η<1/(2πf0Lip/V+r)2 ……(6)
となる。(6)式に示す条件を満足すれば、零なしは
急速に消滅する。 When η is obtained from equations (3) to (5), η<1/(2πf 0 Li p /V+r) 2 ...(6). If the condition shown in equation (6) is satisfied, the non-zero condition disappears rapidly.
本発明によれば、分路リアクトルに直列に潮
流、端子電圧、分路リアクトル補償度より定まる
コンデンサを設置するのみで、電流零なしを解消
することができ、経済的効果は極めて大きい。
According to the present invention, by simply installing a capacitor determined by power flow, terminal voltage, and shunt reactor compensation degree in series with the shunt reactor, it is possible to solve the problem of no current zero, and the economic effect is extremely large.
第1図は本発明に係る超高圧送電系統、第2図
は従来の系統、第3図は本発明に係る系統図、第
4図は従来の解析図である。
S1,S2……電気所、Tr1,Tr2……変圧器、L1
〜L3……送電線、CB1〜CB6……遮断器、Lh1〜
Lh6……分路リアクトル。
FIG. 1 is an ultra-high voltage power transmission system according to the present invention, FIG. 2 is a conventional system, FIG. 3 is a system diagram according to the present invention, and FIG. 4 is a conventional analysis diagram. S 1 , S 2 ... Electrical station, T r1 , T r2 ... Transformer, L 1
~L 3 ...Transmission line, CB 1 ~CB 6 ...Breaker, L h1 ~
L h6 ...Shunt reactor.
Claims (1)
地間に設けられる充電電流補償装置において、 この充電電流補償装置は、リアクトルとコンデ
ンサとの直列回路を線路と大地間に設けられ、前
記コンデンサは、線路の最大潮流をip、リアクト
ルの端子電圧をV、前記リアクトルの補償度をγ
とするとき、次式により定まるリアクトルとの比
率ηのコンデンサとされる充電電流補償装置。 η<1/(2πfoLip/V+r)2 [Claims] 1. A charging current compensator installed between the line and the ground to compensate for the charging current of the line. The capacitor has a maximum current of the line as ip, a terminal voltage of the reactor as V, and a compensation degree of the reactor as γ.
When , the charging current compensator is a capacitor with a ratio η to the reactor determined by the following equation. η<1/(2πfoLip/V+r) 2
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24147285A JPS62104427A (en) | 1985-10-30 | 1985-10-30 | Charging current compensator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24147285A JPS62104427A (en) | 1985-10-30 | 1985-10-30 | Charging current compensator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62104427A JPS62104427A (en) | 1987-05-14 |
| JPH0522458B2 true JPH0522458B2 (en) | 1993-03-29 |
Family
ID=17074822
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP24147285A Granted JPS62104427A (en) | 1985-10-30 | 1985-10-30 | Charging current compensator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62104427A (en) |
-
1985
- 1985-10-30 JP JP24147285A patent/JPS62104427A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62104427A (en) | 1987-05-14 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |