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JPS593773B2 - Reactive power fluctuation compensator - Google Patents
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JPS593773B2 - Reactive power fluctuation compensator - Google Patents

Reactive power fluctuation compensator

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Publication number
JPS593773B2
JPS593773B2 JP51070030A JP7003076A JPS593773B2 JP S593773 B2 JPS593773 B2 JP S593773B2 JP 51070030 A JP51070030 A JP 51070030A JP 7003076 A JP7003076 A JP 7003076A JP S593773 B2 JPS593773 B2 JP S593773B2
Authority
JP
Japan
Prior art keywords
reactive power
voltage
igniter
load
current
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
JP51070030A
Other languages
Japanese (ja)
Other versions
JPS52151847A (en
Inventor
惇 西台
信一郎 西村
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.)
Nissin Electric Co Ltd
Original Assignee
Nissin Electric Co Ltd
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 Nissin Electric Co Ltd filed Critical Nissin Electric Co Ltd
Priority to JP51070030A priority Critical patent/JPS593773B2/en
Publication of JPS52151847A publication Critical patent/JPS52151847A/en
Publication of JPS593773B2 publication Critical patent/JPS593773B2/en
Expired legal-status Critical Current

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  • Control Of Electrical Variables (AREA)

Description

【発明の詳細な説明】 この発明は誘導性の負荷の無効電力変動を速やかに補償
し得るようにした無効電力変動補償装置に関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a reactive power fluctuation compensator capable of quickly compensating for reactive power fluctuations of an inductive load.

5 例えばアーク炉のアーク抵抗の変化等による負荷イ
ンピーダンスの変動によつて無効電力変動を生じ、これ
が電源電圧の急速な変化、すなわち電圧フリッカと称さ
れる現象を呈する。
5. Fluctuations in load impedance due to, for example, changes in arc resistance in an arc furnace cause reactive power fluctuations, which cause rapid changes in power supply voltage, a phenomenon called voltage flicker.

この電圧フリッカ対策として第1図に示すような装置が
既に、0この発明者らによつて提案されている。第1図
において、1及び2は交流電源3に接続された人力端子
、4及び5は出力電圧をとり出す出力端子で、この出力
端子4及び5の間に変動負荷12が接続されている。6
は直列リアクトル、75Tは前記直列リアクトル6を介
して入力端子1、2間に接続された点弧子付スイッチ装
置で、サイリスタなどのような点弧位相制御のできるス
イッチ要素71、72により構成されている。
As a measure against this voltage flicker, a device as shown in FIG. 1 has already been proposed by the present inventors. In FIG. 1, 1 and 2 are human power terminals connected to an AC power supply 3, 4 and 5 are output terminals for taking out an output voltage, and a variable load 12 is connected between these output terminals 4 and 5. 6
is a series reactor, and 75T is a switch device with an igniter connected between the input terminals 1 and 2 via the series reactor 6, and is composed of switch elements 71 and 72 that can control the ignition phase, such as a thyristor. ing.

8は変圧器で、1次巻線81は前記スイッチ装置Tの端
ノO 子間に接続され、2次巻線82はその一端が後述
するインピーダンス例えばリアクトル10に、他端は後
述する検出制御装置11に接続されている。
8 is a transformer, a primary winding 81 is connected between the terminals of the switch device T, and a secondary winding 82 has one end connected to an impedance, for example, a reactor 10, which will be described later, and the other end connected to a detection control, which will be described later. It is connected to the device 11.

9は変流器で、1次巻線91は入出力端子1、4間に接
続され、2次巻線92にはリアクトル10ノ5 が接続
されている。
9 is a current transformer, a primary winding 91 is connected between input and output terminals 1 and 4, and a secondary winding 92 is connected to a reactor 10/5.

検出制御装置11は、スイッチ装置Tの端子電圧VTと
、前記リアクトル10に負荷電流ILが流れた時に生ず
る、このリアクトル10の端子電圧に比例する電圧との
差電圧りを検出し、この差電圧Vの平均値を一定化させ
る30よう、半サイクル毎にその積分値が一定値となつ
たときに基準電圧Esと比較して前記スイッチ装置7を
点弧させるように構成されている。なお、前記変圧器8
、及び変流器9の巻数比はそれぞれ1:1に巻回されて
いるものとして図示してある35が、これはその動作の
説明を簡略化する為であつて実際には、変圧器8は1:
nに変流器9は1■n’の巻数比に巻回されているもの
である。第v図に示す装置において、変動負荷12の無
効電力分のみを例示して説明すると、であり、(2)式
に(1)式を代入するととなり、(3)式においてX=
XBとすれば(4)式でE及びXBは一定と見做し得る
ので差電圧Vの平均値、即ち積分値を毎半サイクルごと
に基準電圧Esと比較しながら一致した時点で検出制御
装置11から点弧パルスを出しスイツチ装置7を点弧導
通させると端子電圧VTは差電圧vの半サイクル毎の平
均値即ち積分値が一定になる如く制御され(4)式から
してIT+ILは平均値に於いて一定となる如く制御さ
れることとなる。
The detection control device 11 detects a voltage difference between the terminal voltage VT of the switching device T and a voltage proportional to the terminal voltage of the reactor 10 that occurs when the load current IL flows through the reactor 10, and detects this difference voltage. In order to keep the average value of V constant 30, when the integral value becomes a constant value every half cycle, it is compared with the reference voltage Es and the switch device 7 is turned on. Note that the transformer 8
, and the current transformer 9 are shown in the figure as having a winding ratio of 1:1, but this is to simplify the explanation of their operation, and in reality, the transformer 8 is 1:
The current transformer 9 is wound at a turns ratio of 1 n'. In the device shown in FIG.
If XB, E and XB can be regarded as constant in equation (4), so the average value of the differential voltage V, that is, the integral value, is compared with the reference voltage Es every half cycle, and the detection control device detects it when they match. When an ignition pulse is issued from 11 to ignite and conduct the switch device 7, the terminal voltage VT is controlled so that the average value, that is, the integral value of the differential voltage v every half cycle is constant, and from equation (4), IT+IL is the average value. It is controlled so that the value remains constant.

しかし、上述の構成では無負荷の条件即ちXIL−XB
IT=Oの場合V=VTであることから、制御回路81
→8→82→11→7→81がEsを基準電圧とするV
Tに対する定電圧制御系を構成し、そのバツフアリアク
タンスとして電源側リアクタンスより比較的大きなリア
クタンスを有する直列リアクトル6を介しているので、
負荷電流1Lの急激な変化、特に電源周波数の2倍以上
速い周波数を持つ急変に対してはスイツチ装置7が応答
出来ないので正饋還が上述の制御閉ループにかかりハン
チングすることがある。
However, in the above configuration, the no-load condition, that is, XIL-XB
Since V=VT when IT=O, the control circuit 81
→8→82→11→7→81 is V with Es as the reference voltage
A constant voltage control system for T is configured, and its buffer reactance is via the series reactor 6, which has a relatively larger reactance than the reactance on the power supply side.
Since the switch device 7 cannot respond to a sudden change in the load current 1L, especially a sudden change with a frequency that is twice or more faster than the power supply frequency, the positive feedback may be involved in the above-mentioned control closed loop and hunting may occur.

従つてこれを抑制するには一般の制御理論からすれば制
御回路に遅れ要素をもつたフイルタ一回路を主とするハ
ンチング防止回路を設ければよいが、その回路を付加す
ることにより無効電力変動補償装置はその生命とも云う
べき速応性が失なわれてしまうことになる。さらに負荷
電流1Lに含まれる高調波分に依つてこのハンチング現
象が拡大されるといつた不都合を生じる。この発明は上
述の事柄に鑑み、速応性を失なうことなく負荷電流に含
まれる高調波による制御誤差を少なくした無効電力変動
補償装置を得ることを目的として提案されたもので、以
下この発明の一実施例を第2図〜第5図に基ずいて説明
する。
Accordingly, in order to suppress this, according to general control theory, it is sufficient to provide the control circuit with an anti-hunting circuit consisting mainly of a filter circuit with a delay element, but by adding this circuit, reactive power fluctuations The compensation device will lose its quick response, which can be called its life. Furthermore, this hunting phenomenon is amplified by the harmonic components contained in the load current 1L, resulting in a disadvantage. In view of the above-mentioned matters, this invention was proposed for the purpose of obtaining a reactive power fluctuation compensator that reduces control errors due to harmonics contained in load current without losing quick response. One embodiment of this will be explained based on FIGS. 2 to 5.

なお、第2図において第1図と同一符号を付したものは
略々同一のものを示す。ただし、変圧器8は点弧子付ス
イツチ装置7の両端のVTからでなく、入力端子1,2
又は出力端子4,5の両端の電源電圧食をその1次巻線
81に印加している。又、検出制御装置11は検出信号
電圧Vを毎半サイクル毎に或時点にてりセツトした後積
分を開始する時分割積分器111と、この時分割積分器
111の積分出力値が或るレベルに達した時にパルスを
発するレベル比較器112と、このレベル比較器112
からのパルスを増巾して点弧子付スイツチ装置7を点弧
せしめるパルス増巾器113とからなつている。なお、
前記変圧器8及び変流器9の巻数比はそれぞれ1:1に
巻回されているものとして図示してあるが、これは第1
図に示すものと同様その動作の説明を簡略化する為であ
つて、実際には変圧器8は1:nに変流器9は1:n′
の巻線比に巻回されている。次に本発明の動作について
、誘導性の変動負荷の無効電力分のみを例示して説明す
ると、交流電源3の電圧をE、直列リアクトル6のリア
クタンスをXBlこの直列リアクトル6に流れる電流を
IT、負荷電流をIL、スイツチ装置7の端子電圧をV
Tlリアクトル10のリアクタンスをXとする。
In FIG. 2, the same reference numerals as in FIG. 1 indicate substantially the same components. However, the transformer 8 is connected not from the VT at both ends of the switch device 7 with igniter, but from the input terminals 1 and 2.
Alternatively, a power supply voltage difference across the output terminals 4 and 5 is applied to the primary winding 81 thereof. Further, the detection control device 11 includes a time division integrator 111 that starts integration after resetting the detection signal voltage V at a certain point in every half cycle, and a time division integrator 111 that starts integration after resetting the detection signal voltage V at a certain point in time every half cycle, and a time division integrator 111 that sets the detection signal voltage V at a certain point in time in every half cycle. a level comparator 112 that emits a pulse when the level is reached, and this level comparator 112
and a pulse amplifier 113 that amplifies the pulses from the igniter and ignites the igniter-equipped switch device 7. In addition,
The transformer 8 and the current transformer 9 are shown with a turns ratio of 1:1, but this is different from the first one.
Similar to the one shown in the figure, this is to simplify the explanation of the operation, and in reality, the transformer 8 is 1:n and the current transformer 9 is 1:n'.
It is wound to a winding ratio of . Next, to explain the operation of the present invention by illustrating only the reactive power component of an inductive variable load, the voltage of the AC power supply 3 is E, the reactance of the series reactor 6 is XBl, the current flowing through the series reactor 6 is IT, The load current is IL, and the terminal voltage of the switch device 7 is V.
Let X be the reactance of the Tl reactor 10.

(1)先づ、無負荷時(IL=0のとき)には、検出制
御装置11により電圧V即ち電源電圧亡を角度一βから
積分を開始し、その積分値FtVCOSOdθがfつβ
ECldθに到達した瞬間の角度θ(即ち+β)に点弧
パルスを発し、スィッチ装置7の例えばスイツチ要素7
2を点弧するように制御している(即ち第3図の斜線の
面積が点弧パルスを発生するための比較レベルErtC
OSOdθに等しくなつている)。
(1) First, when there is no load (when IL=0), the detection control device 11 starts integrating the voltage V, that is, the power supply voltage, from an angle of 1β, and the integral value FtVCOSOdθ is
An ignition pulse is emitted at an angle θ (i.e. +β) at the moment when ECldθ is reached, and the switch element 7 of the switch device 7, for example,
2 (that is, the area of the diagonal line in FIG. 3 is the comparison level ErtC for generating the ignition pulse).
(is equal to OSOdθ).

この動作によりリアクトル6にはITなる電流が流れる
。また次の半サイクルにおいても極性に逆転するが全く
同様の制御によりスイツチ要素71に点弧パルスが与え
られリアクトル6にTなる電流が流れる。(2)いま変
動負荷12として力率0の最大の遅れ電流1Lmaxが
流れる場合を想定するとき、変流器9の二次回路のリア
クトル10の端子にはJILmaxxなる端子電圧を生
じ、第4図に示す如く積分される。
This operation causes a current IT to flow through the reactor 6. In the next half cycle as well, the polarity is reversed, but an ignition pulse is applied to the switch element 71 under exactly the same control, and a current of T flows through the reactor 6. (2) Now assuming that the maximum lagging current 1Lmax with a power factor of 0 flows as the variable load 12, a terminal voltage of JILmaxx is generated at the terminal of the reactor 10 of the secondary circuit of the current transformer 9, as shown in FIG. It is integrated as shown in .

入力電圧は(E一JILmOx)であるのでこれは角度
一βから積分が開始されyβ(?−JILmaxX)d
θなる積分値が比較レペルEK3cOsOdθに達した
時に点弧パルスを生ずることは明らかである。
Since the input voltage is (E - JILmOx), the integration starts from the angle - β and becomes yβ (? - JILmaxX) d
It is clear that an ignition pulse is generated when the integral value θ reaches the comparison level EK3cOsOdθ.

今、リアクトル10のリアクタンスXの値を次のように
選定すると遅れ零力率の負荷電流の最大値1Lmaxに
対して点弧パルス発生角度βが一になる。
Now, if the value of the reactance X of the reactor 10 is selected as follows, the ignition pulse generation angle β will be equal to the maximum value 1Lmax of the load current at the delayed zero power factor.

即ち負荷電流1Lの影響によりサイリスタ電流を零なら
しめるものである。即ち )?β(ILmaxX)COsOdθは第4図の縦線の
面積SECOSOdθは第4図の斜線の面積 これが等しくなる様にリアクトル10を選定するOもし
ILが上記最大値1Lmaxより小さい場合は!)にβ
(L−JiLX)dθの積分はθが一に達する以前に点
弧し上記のようにILが零からILが最大に至るまでの
変化に対し電流ITは、IL−0に対応する電流から零
まで連続的?ヨントロールできる。
That is, the thyristor current is brought to zero under the influence of the load current 1L. i.e.)? β (ILmax ) to β
(L-JiLX) The integral of dθ is fired before θ reaches one, and as mentioned above, as IL changes from zero to the maximum, current IT changes from the current corresponding to IL-0 to zero. Continuously? You can roll.

(3)次に負荷電流の力率が100%の場合を考えると
、第5図に示すように一β点より(EjXIL)は積分
を開始されるが明らかに−j×1Lの積分値は第5図の
縦線で図示する面積でみられるよう一βから+βまでで
零となり結局乙(屓−JXiL)dθ一几?dθ即ち(
1)における説明の無負荷時と同じ位相角βにおいて上
記積分値は比較レベルに達してスイツチ装置7にTなる
電流を通電せしめる。
(3) Next, if we consider the case where the power factor of the load current is 100%, as shown in Figure 5, integration starts from the 1β point (EjXIL), but clearly the integral value of -j x 1L is As can be seen in the area indicated by the vertical line in Figure 5, it becomes zero from 1β to +β, and in the end, dθ1L? dθ, i.e. (
At the same phase angle β as in the no-load state described in 1), the above-mentioned integral value reaches the comparison level, causing the switch device 7 to conduct a current of T.

即ち無効電力を含まない、100%力率の負荷に対して
は負荷電流の大小を問わず、このスイツチ装置7の電流
制御は感応しないことを示す。
In other words, this shows that the current control of the switch device 7 is not sensitive to a load with a power factor of 100% that does not include reactive power, regardless of the magnitude of the load current.

(4)任意遅れ力率の負荷に対してはこの負荷電流は1
00%力率とO%力率遅れの二つの電流ベクトルに分解
して考える事ができるのは、よく知られた所で前者に対
応する有効電流成分に対しては感応せず、後者の無効電
力成分負荷電流に対してのみ、前記(2)で説明したよ
うに無効電力負荷の増大に伴ないスイツチ装置7により
リアクトル6の電流を減少させる。
(4) For a load with an arbitrary lagging power factor, this load current is 1
It is well known that the current vectors can be separated into two current vectors, 00% power factor and 0% power factor lag. As explained in (2) above, only for the power component load current, the switch device 7 reduces the current of the reactor 6 as the reactive power load increases.

即ちリアクトル6で消費する無効電力を減少させる。以
上の説明から明らかなように、無負荷時のスイツチ装置
の点弧角βに対し積分開始を一βなる点におき、一βか
ら一までのVの積分出力をレベル比較する事により負荷
の無効電力の増減に半サイクル毎に逆対応した時分割無
効電力調整が可能となり電源への無効電力変動の影響を
平坦化することができる。
That is, the reactive power consumed by the reactor 6 is reduced. As is clear from the above explanation, by setting the integration start at the point 1β for the firing angle β of the switch device under no load, and comparing the level of the integral output of V from 1β to 1, the load can be adjusted. It is possible to perform time-division reactive power adjustment that inversely responds to increases and decreases in reactive power every half cycle, and it is possible to flatten the influence of reactive power fluctuations on the power supply.

別言すれば系を開ループとし、電源周波数の半サイクル
毎に合成電圧を積分し、この積分値を設定レベルと比較
した後はりセツトする如く時分割積分して成るので、無
効電力変動補償装置としての速応性を損なうことなく負
荷電流に含まれる高調波による制御誤差を少なくできる
ことが分る。なお、角度βの選定には、(1)ILの波
形に歪が多いとき−JXILの波形も歪むがβが大きい
程積分期間が拡がるため、誤差に及ぼす影響が小さくな
るという利屯があり、また(2)βが小なる程ITでコ
ントロールできる無効電力の大きさに対応するITの波
形歪率が小となり有利である、という相反する特徴を有
するため、変動負荷の性質により適当な値を選ぶべきで
あるが、一般にアーク炉のようにILの波形歪の大なる
ものはβ一300程度整流器負荷のようにILの波形歪
が比較的小さいものにはβ−10に位が適当である。
In other words, the system is open-loop, the composite voltage is integrated every half cycle of the power supply frequency, and this integrated value is compared with a set level and then integrated in a time-division manner, so that the reactive power fluctuation compensation device It can be seen that control errors due to harmonics contained in the load current can be reduced without impairing the quick response of the load current. Note that the selection of the angle β has the following advantages: (1) When the IL waveform has a lot of distortion - the JXIL waveform will also be distorted, but the larger β is, the wider the integration period will be, so the effect on the error will be smaller; In addition, (2) the smaller β is, the smaller the waveform distortion factor of IT corresponding to the amount of reactive power that can be controlled by IT is advantageous. Generally speaking, in cases where the IL waveform distortion is large, such as an arc furnace, β-300 is appropriate.For cases where the IL waveform distortion is relatively small, such as a rectifier load, β-10 is appropriate. .

以上述べた如く、本発明によれば速応性を失なうことな
く負荷電流に含まれる高調波成分による制御誤差を少な
くすることができ、常時消費される無効電力を必要最小
限にして経済的に無効電力変動を防止し得る。又、ハン
チング現象を生じることもなく負荷電流に含まれる高調
波成分によつてハンチング現象が拡大されるおそれもな
いといつた効果を奏する。なお、本発明の点弧子付スイ
ツチ装置としては、前述の実施例で用いたサイリスタに
代えて、イグナイトロンのようなものでもよく、要は点
弧位相の調整が可能なスイツチ要素であればよい。
As described above, according to the present invention, it is possible to reduce control errors due to harmonic components contained in load current without losing quick response, and to reduce the constantly consumed reactive power to the necessary minimum, resulting in an economical It is possible to prevent reactive power fluctuations. Further, there is an effect that no hunting phenomenon occurs and there is no fear that the hunting phenomenon will be amplified by harmonic components contained in the load current. The igniter-equipped switch device of the present invention may be replaced by an ignitron or the like in place of the thyristor used in the above-mentioned embodiments.In short, any switch element that can adjust the ignition phase may be used. good.

また、前述の実施例においては本発明を単相回路に適用
した場合について説明したが、三相回路に本発明を適用
しても同様の効果を奏するのは勿論である。
Further, in the above-mentioned embodiments, the case where the present invention is applied to a single-phase circuit has been described, but it goes without saying that the same effect can be achieved even when the present invention is applied to a three-phase circuit.

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

第1図は従来例を示す結線図、第2図は本発明の一実施
例を示す結線図、第3図〜第5図は本発明を説明するた
めの波形図である。 3・・・・・・交流電源、6・・・・・・直列リアクト
ル、7.・・・・・点弧子付スイツチ装置、8・・・・
・・変圧器、9・・・・・・変流器、10・・・・・・
インピーダンス、11・・・・・・検出制御装置、11
1・・・・・・時分割積分器、112・・・・・・レベ
ル比較器、113・・・・・・パルス増巾器、12・・
・・・・変動負荷。
FIG. 1 is a wiring diagram showing a conventional example, FIG. 2 is a wiring diagram showing an embodiment of the present invention, and FIGS. 3 to 5 are waveform diagrams for explaining the present invention. 3...AC power supply, 6...Series reactor, 7. ...Switch device with igniter, 8...
...Transformer, 9...Current transformer, 10...
Impedance, 11...Detection control device, 11
1... Time division integrator, 112... Level comparator, 113... Pulse amplifier, 12...
...Fluctuating load.

Claims (1)

【特許請求の範囲】[Claims] 1 電源につながれた誘導性の変動負荷に並列に、点弧
位相制御のできる点弧子付スイッチ装置と直列リアクト
ルを直列に接続し、前記点弧子付スイッチ装置の点弧位
相角度を制御して前記直列リアクトルを速動可変インダ
クタンスとして動作させる無効電力変動補償装置におい
て、電源の電圧と変動負荷の電流に比例した電圧とを合
成し、この合成電圧を電源零点に同期し且つ電源零点か
ら(π/2)−βだけ位相の遅れた時点より積分を開始
し、その値を設定レベルと比較してπ迄に前記積分値を
リセットする如く時分割積分し、前記積分値が前記設定
レベルに達した時に発するパルスにより前記点弧子付ス
イッチ装置の点弧位相角度を制御して前記変動負荷の無
効電力分の増減に半サイクル毎に逆対応した時分割積分
の無効電力制御を行なわしめてなることを特徴とする無
効電力変動補償装置。
1. A switching device with an igniter that can control the ignition phase and a series reactor are connected in series in parallel to an inductive variable load connected to a power source, and the ignition phase angle of the switching device with an igniter is controlled. In a reactive power fluctuation compensator that operates the series reactor as a fast-moving variable inductance, the voltage of the power supply and the voltage proportional to the current of the fluctuating load are combined, and this combined voltage is synchronized with the power supply zero point and Integration is started from a point in time when the phase is delayed by π/2)-β, the value is compared with the set level, and time-division integration is performed so as to reset the integral value by π, so that the integral value reaches the set level. The ignition phase angle of the igniter-equipped switch device is controlled by the pulse emitted when the igniter is reached, thereby performing time-division integral reactive power control that inversely corresponds to the increase or decrease of the reactive power of the fluctuating load every half cycle. A reactive power fluctuation compensator characterized by:
JP51070030A 1976-06-14 1976-06-14 Reactive power fluctuation compensator Expired JPS593773B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP51070030A JPS593773B2 (en) 1976-06-14 1976-06-14 Reactive power fluctuation compensator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP51070030A JPS593773B2 (en) 1976-06-14 1976-06-14 Reactive power fluctuation compensator

Publications (2)

Publication Number Publication Date
JPS52151847A JPS52151847A (en) 1977-12-16
JPS593773B2 true JPS593773B2 (en) 1984-01-26

Family

ID=13419775

Family Applications (1)

Application Number Title Priority Date Filing Date
JP51070030A Expired JPS593773B2 (en) 1976-06-14 1976-06-14 Reactive power fluctuation compensator

Country Status (1)

Country Link
JP (1) JPS593773B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5914023A (en) * 1982-07-15 1984-01-24 Chugoku Denki Seizo Kk Method for controlling suppressing device of flicker

Also Published As

Publication number Publication date
JPS52151847A (en) 1977-12-16

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