Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0625948B2 - Reactive power compensator - Google Patents
[go: Go Back, main page]

JPH0625948B2 - Reactive power compensator - Google Patents

Reactive power compensator

Info

Publication number
JPH0625948B2
JPH0625948B2 JP60200009A JP20000985A JPH0625948B2 JP H0625948 B2 JPH0625948 B2 JP H0625948B2 JP 60200009 A JP60200009 A JP 60200009A JP 20000985 A JP20000985 A JP 20000985A JP H0625948 B2 JPH0625948 B2 JP H0625948B2
Authority
JP
Japan
Prior art keywords
phase
signal
signals
current
reactive power
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
Application number
JP60200009A
Other languages
Japanese (ja)
Other versions
JPS6260012A (en
Inventor
武夫 嶋村
広 内野
良一 黒沢
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP60200009A priority Critical patent/JPH0625948B2/en
Publication of JPS6260012A publication Critical patent/JPS6260012A/en
Publication of JPH0625948B2 publication Critical patent/JPH0625948B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/30Reactive power compensation

Landscapes

  • Control Of Electrical Variables (AREA)
  • Supply And Distribution Of Alternating Current (AREA)

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は無効電力補償装置に係り、交流電源系統から交
流母線を介して無効電力変動の激しい負荷に電力を供給
するシステムにおいて、効果的な無効電力補償を行うた
めの無効電力補償装置に関する。
Description: TECHNICAL FIELD [0001] The present invention relates to a reactive power compensator, and an effective reactive power compensation system in a system for supplying power from an AC power supply system to an AC power bus to a load with a large fluctuation of reactive power. The present invention relates to a reactive power compensator for performing power compensation.

〔発明の技術的背景とその問題点〕[Technical background of the invention and its problems]

近年、大容量のアーク炉設備が交流電源系統に接続され
運転されるようになった。周知の如く、アーク炉は炉中
の溶解物の状態により急変動する無効電力を電源側に発
生する。この急変動する無効電力は電源系統インピーダ
ンスとの相互作用で電圧波形を歪ませ照明器具のフリッ
カの原因になり、及び、電源設備の利用率を低下させる
原因になっている。このため、大容量のアーク炉等を設
備する時にはアーク炉に並置して無効電力補償装置を備
え、これによりアーク炉の発生する急変動する無効電力
を補償し、交流電源系統の無効電力の変動を抑制してい
る。
In recent years, large-capacity arc furnace equipment has been connected to an AC power supply system and operated. As is well known, the arc furnace generates reactive power on the power supply side that fluctuates abruptly depending on the state of the melt in the furnace. This abruptly changing reactive power distorts the voltage waveform due to the interaction with the power supply system impedance and causes flicker of the lighting equipment, and also causes a reduction in the utilization rate of the power supply equipment. Therefore, when installing a large-capacity arc furnace, etc., a reactive power compensator is installed in parallel with the arc furnace to compensate for the rapidly fluctuating reactive power generated by the arc furnace and to fluctuate the reactive power of the AC power system. Is suppressed.

このような無効電力補償装置については、例えば〔文
献〕電気学会技術報告(II部),昭和54年4月第76
号P26〜P31,「無効電力・高調波対策のための電
力変換技術」,整流器常置専門委員会編,に詳述されて
おり、その構成は第8図に示すような電力供給システム
となる。
For such a reactive power compensator, see [Reference] Technical Report of The Institute of Electrical Engineers of Japan (Part II), April 1979, 76th edition.
Nos. P26 to P31, "Power Conversion Technology for Reactive Power / Harmonic Countermeasures", edited by the Special Committee for Permanent Rectifiers, the configuration is a power supply system as shown in FIG.

即ち、同図において、10はアーク炉等の負荷であり、
炉12の中に鉄等を入れ電極11を通して放電により電
流を流し、内部の鉄を加熱溶解している。9は炉用トラ
ンスである。
That is, in the figure, 10 is the load of the arc furnace,
Iron or the like is put into the furnace 12, and an electric current is caused to flow through the electrode 11 by electric discharge to heat and melt the iron inside. 9 is a transformer for the furnace.

100は無効電力補償装置であり、リアクトル部300
と高調波フィルタを兼ねた進相コンデンサ部200で構
成される。リアクトル部300はリアクトル302U〜302W
とそれに直列接続された逆並列サイリスタ301U〜301W
と、負荷電流検出器81R,81S,81Tと電圧検出
用トランス70と、その制御回路350よりなり、アーク
炉10の無効電力を検出し、その検出値に応じてサイリ
スタ301U〜301Wの導通角が調整され、リアクトルの電流
が制御されている。即ち、無効電力補償装置100で
は、進相コンデンサ200の作用と相まってリアクトル
302U〜302Wの電流が制御され、アーク炉10の発生無効
電力(遅れ)と等しい量の進み無効電力を線51R,5
1S,51Tに発生するよう制御され、三相母線4の点
では無効電力は無くなり負荷の有効電力だけが流れるよ
うになる。従って、母線4の電圧歪は低減され、また電
源設備の利用率が向上することとなる。3は三相交流電
源系統に存在する系統インピーダンス、1は三相交流電
源系統又は送配電母線などの電力供給源である。
Reference numeral 100 is a reactive power compensator, which is a reactor unit 300.
And a phase advancing capacitor section 200 that also serves as a harmonic filter. Reactor section 300 is reactor 302U-302W
And anti-parallel thyristors 301U to 301W connected in series with it
The load current detectors 81R, 81S, 81T, the voltage detecting transformer 70, and the control circuit 350 thereof detect the reactive power of the arc furnace 10, and the conduction angles of the thyristors 301U to 301W are detected according to the detected value. Adjusted and the reactor current is controlled. That is, in the reactive power compensator 100, the reactor is coupled with the action of the phase advance capacitor 200.
The electric current of 302U to 302W is controlled, and the amount of lead reactive power equal to the generated reactive power (delay) of the arc furnace 10 is applied to the lines 51R, 5R.
It is controlled to occur in 1S and 51T, and the reactive power disappears at the point of the three-phase bus 4 and only the active power of the load flows. Therefore, the voltage distortion of the bus bar 4 is reduced, and the utilization factor of the power supply equipment is improved. Reference numeral 3 is a system impedance existing in a three-phase AC power supply system, and 1 is a power supply source such as a three-phase AC power supply system or a transmission and distribution bus.

以上の構成の無効電力補償装置(100)では、制御回路3
50により、負荷(10)の発生する無効電力をいかに正確
に検出するかが装置性能を左右するポイントになってい
る。この無効電力検出回路の一例を第9図に示す。
In the reactive power compensator (100) having the above configuration, the control circuit 3
According to 50, how accurately the reactive power generated by the load (10) is detected is the key to the device performance. An example of this reactive power detection circuit is shown in FIG.

即ち、第9図は特開昭59−139416の第2図に開
示されている回路であり、まず母線電圧eの90°遅相
波形e90と負荷電流iLとの積qをつくると、qには直
流成分(無効電力成分)とそれに基本波周波数の2倍で
振動する交流成分が含まれる形になり、この信号を低域
通過フィルタに通し直流分qVAR(無効電力を示す量)
を検出し、これに基づいてリアクトル部300の電流を
制御している。
That is, FIG. 9 is a circuit disclosed in FIG. 2 of Japanese Patent Laid-Open No. 59-139416. First, when a product q of a 90 ° delayed waveform e 90 of a bus voltage e and a load current i L is created, q has a form in which a direct current component (reactive power component) and an alternating current component that oscillates at twice the fundamental frequency are included. This signal is passed through a low-pass filter, and the direct current component q VAR (amount of reactive power)
Is detected, and the current of the reactor part 300 is controlled based on this.

その他、種々の無効電力検出法が提案されているが、そ
の主旨は特開昭59-139416に開示されている原理に帰着
できる。
Besides, various reactive power detection methods have been proposed, but the gist thereof can be reduced to the principle disclosed in Japanese Patent Laid-Open No. 59-139416.

以上が従来の無効電力補償装置の説明であるが、この装
置では次のような欠点がある。即ち、アーク炉等の発生
する変動電力(有効電力・無効電力も含めて)を分析す
ると、その中には変動しない直流量の成分(即ち、正相
電圧と正相電流に起因する正相電力)と変動する成分
(即ち、正相電圧と逆相電流に起因する逆相電力)とを
含んでいるが、従来の無効電力検出法はこれら正相電力
と逆相電力を明確に分離するという概念がなく、そのた
め電力を正相電力と逆相電力が渾然一体と混った形の単
なる変動分としてのみとらえ、それに基づいてリアクト
ル電流を制御している。そのため、従来の無効電力補償
装置では補償対象を何にするか、即ち、正相無効電力
(変動しない成分)を制御しているのか、逆相無効電力
(変動する成分)を制御しているのか、の識別が原理的
にできず、より高度な制御への展開が不可能であった。
The above is the description of the conventional reactive power compensator, but this device has the following drawbacks. That is, when the fluctuating power (including active power and reactive power) generated by an arc furnace is analyzed, the component of the DC amount that does not fluctuate (that is, the positive phase power due to the positive phase voltage and the positive phase current) ) And a fluctuating component (that is, the negative phase power caused by the positive phase voltage and the negative phase current), the conventional reactive power detection method clearly separates these positive phase power and negative phase power. There is no concept, therefore, the electric power is regarded only as a fluctuation component in which the positive-phase electric power and the negative-phase electric power are mixed together, and the reactor current is controlled based on the fluctuation. Therefore, what is to be compensated in the conventional reactive power compensator, that is, whether the positive-phase reactive power (component that does not fluctuate) is controlled or the negative-phase reactive power (component that fluctuates) is controlled. In principle, it was not possible to discriminate between, and it was impossible to develop into more advanced control.

近年、交流電力系統の電力の品質向上が強く求められ、
これに応ずるためのアーク炉等のフリッカ対策用の無効
電力補償装置、及び、交流電力系統の安定化対策用の無
効電力補償装置のより高度な制御が強く求められてお
り、この要求を満すための新規な制御概念に基づく精度
の良い電力検出法(有効分,無効分を含めて)を備えた
無効電力補償装置の出現が望まれている。
In recent years, there has been a strong demand for improving the quality of power in the AC power system,
In order to meet this demand, there is a strong demand for more advanced control of reactive power compensators for flicker countermeasures in arc furnaces, etc., and reactive power compensators for AC power system stabilization measures, and this requirement is satisfied. Therefore, the emergence of a reactive power compensator equipped with a highly accurate power detection method (including active and reactive components) based on a new control concept is desired.

〔発明の目的〕[Object of the Invention]

本発明は上記従来技術の問題点に鑑みなされたもので、
その目的はアーク炉等の負荷の発生する無効電力の補償
を行う装置において、負荷電流の中の正相分と逆相分を
分離検出し、それにより補償対象を明確にして制御を行
うことにより、高精度の補償制御を行えるようにした無
効電力補償装置を提供することにある。
The present invention has been made in view of the above-mentioned problems of the prior art,
The purpose is to separate and detect the positive-phase component and the negative-phase component in the load current in a device that compensates the reactive power generated by the load of an arc furnace, etc. Another object of the present invention is to provide a reactive power compensator capable of performing highly accurate compensation control.

〔発明の概要〕[Outline of Invention]

本発明は上記目的を達成するために交流電源系統に接続
される負荷が発生する無効電力を補償する無効電力補償
装置において、 検出した負荷電流を2相変換して得られる2相電流信号
と、負荷がつながる交流母線電圧に同期した単位2相電
圧信号と、交流母線電圧の周波数の2倍の周波数の単位
2相電圧信号とを用い、これらの信号の演算を通じて負
荷電流の中の正相無効分及び逆相成分を分離検出し、こ
の検出信号に基づいて無効電力補償装置の電流指令を作
成し、この電流指令値に基づいて無効電力補償装置を制
御するようにしたものである。
In order to achieve the above object, the present invention relates to a reactive power compensator for compensating reactive power generated by a load connected to an AC power system, and a two-phase current signal obtained by converting a detected load current into two phases, A unit two-phase voltage signal synchronized with the AC bus voltage to which the load is connected and a unit two-phase voltage signal having a frequency twice the frequency of the AC bus voltage are used, and the positive phase invalid in the load current is calculated through the calculation of these signals. The component and the anti-phase component are separately detected, a current command for the reactive power compensator is created based on this detection signal, and the reactive power compensator is controlled based on this current command value.

〔発明の実施例〕Example of Invention

本発明の無効電力補償装置を備えた電力供給システムは
第8図のものと同一であり、前述の従来例の説明で言及
した要素については、ここでは説明を省略する。
The power supply system including the reactive power compensator of the present invention is the same as that of FIG. 8, and the description of the elements mentioned in the description of the conventional example is omitted here.

第8図において81R,81S,81Tは電流検出器で
ありアーク炉10の電流(iRL,iSL,iTL)を検出し
制御回路350に導く。70は電圧検出器でありアーク
炉10(炉用トランス9も含む)がつながる母線の電圧
(eRS,eST,eTR)を検出し制御回路350に導く。
300はリアクトル部であり通常はデルタ結線され、サ
イリスタ301U〜301Wの点弧角の調整により電流の大きさ
が調整される。リアクトル電流は通常、基本波の他に高
調波を含んだ歪波形となる。
In FIG. 8, 81R, 81S, and 81T are current detectors, which detect the currents (i RL , i SL , i TL ) of the arc furnace 10 and guide them to the control circuit 350. Reference numeral 70 denotes a voltage detector that detects the voltage (e RS , e ST , e TR ) of the busbar to which the arc furnace 10 (including the furnace transformer 9) is connected and guides it to the control circuit 350.
Reference numeral 300 denotes a reactor portion, which is usually delta-connected, and the magnitude of the current is adjusted by adjusting the firing angle of the thyristors 301U to 301W. The reactor current usually has a distorted waveform including harmonics in addition to the fundamental wave.

400は本発明を盛込んだ演算回路であり、電流信号i
RL,iSL,iTLと電圧信号eRS,eST,eTRを入力し種
々の演算を行い、リアクトル部300が流すべき基本波
電流を指示するための直流値の電流指令IU *,IV *,I
W *を出力する。
Reference numeral 400 is an arithmetic circuit incorporating the present invention.
RL , i SL , i TL and the voltage signals e RS , e ST , e TR are input, various calculations are performed, and the current command I U * of the direct current value for instructing the fundamental wave current that the reactor unit 300 should flow, I V * , I
Output W * .

500は点弧制御器であり、電流指令値IU *,IV *,I
W *を受けて動作し、IU *,IV *,IW *で指示された電流
(基本波成分)をリアクトル302U,302V,302Wが流すよ
うサイリスタ301U,301V,301Wを点弧制御する。
Reference numeral 500 denotes an ignition controller, which is a current command value I U * , I V * , I
It operates by receiving W * and controls the firing of thyristors 301U, 301V, 301W so that reactors 302U, 302V, 302W flow the current (fundamental wave component) indicated by I U * , IV * , I W *. .

演算回路400と点弧制御器500を合わせたものを制
御回路350と称し、この回路の詳細を第1図に示す。
A combination of the arithmetic circuit 400 and the ignition controller 500 is called a control circuit 350, and the details of this circuit are shown in FIG.

次に本発明の主要部を第1図,第2図により説明する。
なお、本発明では第8図のリアクトル部300がデルタ
結線された場合を例にして以下の説明を進める。第1図
と第8図の同一記号カ所は同一要素同一信号を表わす。
Next, the main part of the present invention will be described with reference to FIGS.
In the present invention, the following description will be given by taking as an example the case where the reactor portion 300 of FIG. 8 is delta-connected. The same symbols in FIGS. 1 and 8 represent the same elements and the same signals.

第1図において402は線/相変換器であり、第8図の
線電流として検出した負荷電流信号iRL,iSL,iTL
式(1)の演算によりデルタ結線の相電流iUL,iVL,i
WLに変換する(式(1)の変換は第8図のリアクトル部3
00がデルタ結線の時に必要な変換であり、スター結線
ではこの変換は不要となる)。
In FIG. 1, reference numeral 402 denotes a line / phase converter, and the load current signals i RL , i SL , and i TL detected as the line currents in FIG. 8 are calculated by the equation (1), and the phase current i UL of the delta connection, i VL , i
Convert to WL (Conversion of formula (1) is performed by reactor part 3 in Fig. 8)
00 is a necessary conversion when the delta connection is used, and this conversion is not necessary when the star connection is used).

403は2相変換器であり電流信号iUL,iVL,iWL
式(2)の演算により2相電流信号i1dL,i1qLに変換す
る。
Reference numeral 403 denotes a two-phase converter which converts the current signals i UL , i VL , i WL into two-phase current signals i 1dL , i 1qL by the calculation of the equation (2).

405は第8図の交流母線電圧信号eRS・eST・eTR
入力し、それをもとにフェイズロックループ回路(PLL
回路)を構成して得られる2相信号発生器であり、その
出力として、第8図において第1相をR相,第2相をS
相,第3相をT相とすると、第1相と第2相の線間電圧
RSに同期した単位正弦波信号▲e* 1d1▼と、それより
90゜遅れた単位正弦波信号▲e* 1q1▼、及びそれの位相
信号▲θ* 1d1▼を出し、▲e* 1d1▼,▲e* 1q1▼は式
(3)で表わせる(なお、第8図のリアクトル部300が
スター結線の場合には▲e* 1d1▼,▲e* 1q1▼は第1相
の相電圧に同期させる)。
405 inputs the AC bus voltage signals e RS , e ST, and e TR shown in FIG. 8, and based on this, the phase lock loop circuit (PLL
A two-phase signal generator obtained by constructing a circuit), and as its output, the first phase is the R phase and the second phase is the S phase in FIG.
If the phase and the third phase are the T phase, the unit sine wave signal ▲ e * 1d1 ▼ synchronized with the line voltage e RS of the first and second phases, and
The unit sine wave signal ▲ e * 1q1 ▼ delayed by 90 ° and its phase signal ▲ θ * 1d1 ▼ are output, and ▲ e * 1d1 ▼ and ▲ e * 1q1 ▼ are expressed by
(3) (Note that when the reactor part 300 in FIG. 8 is star connected, ▲ e * 1d1 ▼, ▲ e * 1q1 ▼ are synchronized with the phase voltage of the first phase).

404は演算器であり、信号i1dL,i1q1及び▲e* 1d1
▼,▲e* 1q1▼を入力し、式(4)により信号Q1P,P1P
を演算する。
Reference numeral 404 denotes an arithmetic unit, which outputs signals i 1dL , i 1q1 and ▲ e * 1d1.
Input ▼, ▲ e * 1q1 ▼, and use the formula (4) to input signals Q 1P and P 1P
Is calculated.

負荷電流iRL,iSL,iTLが正相分/逆相分を含む場
合、Q1P,P1Pは直流分と基本波の2倍の周波数で振動
する交流分を含んだ脈流となる。
When the load currents i RL , i SL , and i TL include a positive phase component / a negative phase component, Q 1P and P 1P become a pulsating flow that includes a direct current component and an alternating current component that oscillates at twice the frequency of the fundamental wave. .

407は分離器であり、408,409の直流検出フィ
ルタと410,411の加算器で構成されており、信号
1P,P1Pを入力し、直流検出フィルタ408,409
によりQ1P,P1Pの直流分を検出し信号Q1PD,P1PD
して出力するとともに、加算器410,411の所で信
号Q1P,P1Pの中から直流分、即ちQ1PD,P1PDを取り
去り、交流成分だけを信号Q1PA,P1PAとして出力す
る。ここで得られた直流量の信号Q1PD,P1PDは負荷電
流iRL,iSL,iTLが含む正相無効電流(Q1PD)と正相有
効電流(P1PD)を表わしている。
Reference numeral 407 denotes a separator, which is composed of direct current detection filters 408 and 409 and adders 410 and 411, receives the signals Q 1P and P 1P, and outputs direct current detection filters 408 and 409.
Detects the DC components of Q 1P and P 1P and outputs them as signals Q 1PD and P 1PD . At the adders 410 and 411, the DC components, that is, Q 1PD and P 1PD, are output from the signals Q 1P and P 1P. It is removed and only the AC component is output as the signals Q 1PA and P 1PA . The DC amount signals Q 1PD and P 1PD obtained here represent the positive phase reactive current (Q 1PD ) and the positive phase active current (P 1PD ) included in the load currents i RL , i SL , and i TL .

415Aは分配器であり信号Q1PD,Q1PA,P1PA及び
位相角信号▲θ* 1d1▼を受けて演算を行ない、第8図の
リアクトル部300が流す電流を指示するための電流指
令値IU *,IV *,IW *を出力する。分配器415Aの詳
細を第2図に示す。
Reference numeral 415A denotes a distributor, which receives signals Q 1PD , Q 1PA , P 1PA and a phase angle signal ▲ θ * 1d1 ▼ to perform an operation, and a current command value I for instructing a current flowing by the reactor unit 300 in FIG. U * , IV * , and IW * are output. The details of the distributor 415A are shown in FIG.

500は点弧制御器であり電流指令値IU *,IV *,IW *
を受けて動作し、IU *,IV *,IW *で指示された電流
(基本波成分)をリアクトル部300が流すようサイリ
スタ301U,301V,301Wを点弧制御する。
Reference numeral 500 denotes an ignition controller, which is a current command value I U * , I V * , I W *.
The thyristors 301U, 301V, 301W are ignited and controlled so that the reactor unit 300 causes the current (fundamental wave component) designated by I U * , I V * , I W * to flow.

次に第2図により分配器415Aを説明する。第1図と
第2図の同一記号の信号は記号に合わせて接続される。
第2図において416Aは2相発生器であり、位相角信
号▲θ* 1d1▼を受けて動作し交流母線電圧の周波数の2
倍の周波数を持つ式(5)の2相電圧信号▲e* 1d2▼,▲
* 1q2▼,▲e* 2d2▼,▲e* 2q2▼,▲e* 3d2▼,▲e
* 3q2▼を発生する。
Next, the distributor 415A will be described with reference to FIG. Signals having the same symbols in FIGS. 1 and 2 are connected according to the symbols.
In FIG. 2, reference numeral 416A is a two-phase generator, which operates by receiving the phase angle signal ▲ θ * 1d1 ▼ and has a frequency of 2 of the AC bus voltage.
Two-phase voltage signal of formula (5) with double frequency ▲ e * 1d2 ▼, ▲
e * 1q2 ▼, ▲ e * 2d2 ▼, ▲ e * 2q2 ▼, ▲ e * 3d2 ▼, ▲ e
* Generates 3q2 ▼.

417Aは演算器であり、信号Q1PA,P1PAおよび▲e
* 1d2▼,▲e* 1q2▼を入力し式(6)により信号Q1ND,P
1NDを演算する。同様に、418A,419Aも演算器
であり、それぞれ信号Q1PA,P1PAと▲e* 2d2▼,▲e
* 2q2▼、及びQ1PA,P1PAと▲e* 3d2▼,▲e* 3q2▼を
入力し式(7),(8)により信号Q2ND,P2ND、及び
3ND,P3NDを演算する。
Reference numeral 417A is an arithmetic unit, which outputs signals Q 1PA , P 1PA and ▲ e.
* 1d2 ▼, ▲ e * 1q2 ▼ input expression (6) by a signal Q 1ND, P
Calculate 1ND . Similarly, the 418A and 419A are also arithmetic units, and the signals Q 1PA and P 1PA and ▲ e * 2d2 ▼ and ▲ e, respectively.
* 2q2 ▼, Q 1PA , P 1PA and ▲ e * 3d2 ▼, ▲ e * 3q2 ▼ are input and the signals Q 2ND , P 2ND , and Q 3ND , P 3ND are calculated by equations (7) and (8). .

こうして得られた信号P1ND,Q1NDは式(1)の第1相電
流iULが含む逆相電流を、第1相と第2相の線間電圧に
同相の成分(P1ND)とそれと90゜位相の異なる成分(Q1ND)
に分解した時の各成分の電流を表わしており、ここで
は、P1NDを第1相の同相逆相電流信号、Q1NDを第1相
の90゜逆相電流信号と呼ぶことにする。同様に、P2ND
2NDは式(1)の第2相電流iVLが含む逆相電流を、第2
相と第3相の線間電圧に同相の成分とそれと90゜位相の
異なる成分に分解した時の同相成分電流(P2ND:第2
相の同相逆相電流)、90゜位相の異なる電流成分
(Q2ND:第2相の90゜逆相電流)を表わしている。同様
に、P3ND,Q3NDは式(1)の第3相電流iWLが含む逆相
電流を、第3相と第1相の線間電圧に同相の成分とそれ
と90゜位相の異なる成分に分解した時の同相成分電流
(P3ND:第3相の同相逆相電流)、90゜位相の異なる電
流成分(Q3ND:第3相の90゜逆相電流)を表わしてい
る。これらの信号P1ND,Q1ND,P2ND,Q2ND
3ND,Q3NDは直流量の信号である。
The signals P 1ND and Q 1ND thus obtained include the negative phase current included in the first phase current i UL of the equation (1) as the in-phase component (P 1ND ) in the line voltage of the first and second phases and 90 ° phase difference component (Q 1ND )
The currents of the respective components when decomposed into are represented as follows. Here, P 1ND is referred to as a first-phase in-phase reverse-phase current signal, and Q 1ND is referred to as a first-phase 90 ° reverse-phase current signal. Similarly, P 2ND ,
Q 2ND is the negative phase current included in the second phase current i VL in equation (1)
In-phase component current (P 2ND : second phase) when it is decomposed into the in-phase component and the 90 ° phase difference component in the line voltage of the third phase
Phase in-phase current) and 90 ° phase difference current components (Q 2ND : second phase 90 ° anti-phase current). Similarly, P 3ND and Q 3ND are components of the same phase in the line voltage of the third phase and the first phase and a component different in 90 ° phase from the reverse phase current included in the third phase current i WL of the equation (1). 2 shows the in-phase component current (P 3ND : third-phase in-phase reverse-phase current) and the 90 ° -phase different current component (Q 3ND : third-phase 90-degree reverse-phase current). These signals P 1ND , Q 1ND , P 2ND , Q 2ND ,
P 3ND and Q 3ND are DC signals.

こうして得られた信号Q1PD,Q1ND,P1ND,Q2ND,P
2ND,Q3ND,P3NDは次の振分器440Aに入力される。
The signals Q 1PD , Q 1ND , P 1ND , Q 2ND and P thus obtained
2ND , Q 3ND and P 3ND are input to the next distributor 440A.

次に447は設定器であり、第8図のリアクトル部30
0が発生すべき無効電流(遅れ)の最大値を指示するた
めの無効電流設定信号Q1MAXを出力する。
Next, reference numeral 447 is a setting device, which is the reactor unit 30 shown in FIG.
0 outputs a reactive current setting signal Q 1MAX for instructing the maximum value of the reactive current (delay) that should be generated.

440Aは振分器であり、この中ではアーク炉等の負荷
電流から検出された正相無効電流信号Q1PD、第1相,
第2相,第3相の90゜逆相電流信号Q1ND,Q2ND,Q3ND
と同相逆相電流信号P1ND,P2ND,P3ND及び無効電流
設定信号Q1MAXを入力し、これらの信号に基づいて式
(9)の演算を行い、それぞれ第8図のリアクトル部30
0の第1相のリアクトル302Uの発生すべき電流を指
示するための第1相の電流指令IU *、及び同様にリアク
トル302Vのための第2相の電流指令IV *、及びリア
クトル302Wのための第3相の電流指令IW *を出力す
る。ここで振分器440Aを構成するものとして次の要
素がある。即ち、441A,442A,443Aは係数器であり入力
信号を 倍して出力する。444A,445A,446Aは加算器であり係数
器441A,442A,443Aの出力を図示の極性で加算する。加
算器444A,445A,446Aの出力は式(9)の第3項の演算に
相当する。448Aは加算器であり設定信号Q1MAXと信号Q
1PDを図示極性で演算する。即ち、加算器448Aの出
力は式(9)の第1項の演算に相当する。449A,450A,451
Aは加算器であり、信号Q1ND,Q2ND,Q3NDと加算器4
48Aの出力信号、及び加算器444A,445A,446Aの出力
信号を図示の極性で加算する。
440A is a distributor, in which the positive phase reactive current signal Q 1PD detected from the load current of the arc furnace, the first phase,
Second-phase and third-phase 90 ° reverse-phase current signals Q 1ND , Q 2ND , Q 3ND
Input the in-phase and out-of-phase current signals P 1ND , P 2ND , P 3ND and the reactive current setting signal Q 1MAX , and formula based on these signals.
The calculation of (9) is performed, and the reactor unit 30 of FIG.
0 for the first phase reactor 302U to indicate the current to be generated by the first phase current command I U * , and similarly for the reactor 302V second phase current command I V * , and for the reactor 302W. To output a third-phase current command I W * for Here, the following elements are included in the distributor 440A. That is, 441A, 442A, 443A are coefficient multipliers, Double and output. 444A, 445A and 446A are adders which add the outputs of the coefficient units 441A, 442A and 443A with the polarities shown. The outputs of the adders 444A, 445A, and 446A correspond to the calculation of the third term of Expression (9). 448A is an adder, which is used for setting signal Q 1MAX and signal Q
Calculate 1PD with the indicated polarity. That is, the output of the adder 448A corresponds to the calculation of the first term of the equation (9). 449A, 450A, 451
A is an adder, and signals Q 1ND , Q 2ND , Q 3ND and adder 4
The output signal of 48A and the output signals of the adders 444A, 445A and 446A are added with the polarities shown.

以上の演算で得られた信号IU *,IV *,IW *は直流量の
信号となり、この信号の中には正相電流に関する情報及
び逆相電流に関する情報が全て含まれている。従って、
このIU *,IV *,IW *に基づいて第8図のリアクトル部
300を制御することにより、アーク炉等の負荷電流が
正相分に加えて逆相分をも多量に含む場合であっても第
8図の点4の所の電流を自在に平衡化できる。
The signals I U * , I V * , and I W * obtained by the above calculation are DC amount signals, and this signal contains all the information about the positive-phase current and the information about the negative-phase current. Therefore,
When the reactor 300 shown in FIG. 8 is controlled based on these I U * , I V * , and I W * so that the load current of the arc furnace or the like contains a large amount of the negative phase component in addition to the positive phase component. However, the current at point 4 in FIG. 8 can be freely balanced.

以上が本発明の代表的構成である。The above is a typical configuration of the present invention.

次に本発明の作用を説明する。Next, the operation of the present invention will be described.

まず、第8図においてアーク炉の電流が信号iRL
SL,iTLとして検出されるが、この電流は通常、正相
分と逆相分を含んだ不平衡電流となっている。一方、ア
ーク炉の接続される電源母線電圧を信号eRS,eST,e
TRとして検出され無効電力補償装置100の制御回路に導
入される。次に、第1図において、2相発生器405は信
号eRS,eST,eTRを受けて式(3)に基づく2相信号▲
* 1d1▼,▲e* 1q1▼とその位相角信号▲θ* 1d1▼を出
力する。
First, in FIG. 8, the electric current of the arc furnace is the signal i RL ,
Although detected as i SL and i TL , this current is usually an unbalanced current including a positive phase component and a negative phase component. On the other hand, the signals e RS , e ST , e
It is detected as TR and introduced into the control circuit of the reactive power compensator 100. Next, in FIG. 1, the two-phase generator 405 receives the signals e RS , e ST , and e TR, and outputs the two-phase signal ▲ based on the equation (3)
e * 1d1 ▼, ▲ e * 1q1 ▼ and its phase angle signal ▲ θ * 1d1 ▼ are output.

一方、線電流として検出された信号iRL,iSL,iTL
線/相変換器402の中で式(1)による変換が行われ、
その結果、デルタ結線の相電流iUL,iVL,iWL(即
ち、例えば第8図のデルタ結線されたリアクトル部30
0を例にするとリアクトル302U,302V,302Wに流れる電
流に相当する)に変換される。この信号iUL,iVL,i
WLは2相変換器403の中で式(2)による変換が行わ
れ、2相信号i1dL,iqLが得られる。次に演算器40
4の中で式(4)の演算を行い信号Q1P,P1Pを得て、こ
れを分離器407に通して直流成分の信号Q1PD,P1PD
及び交流成分の信号Q1PA,P1PAに分離する。こうして
得られた信号Q1PDは負荷電流信号iRL,iSL,i
TL(又は式(1)のiUL,iVL,iWLと言い換えてもよ
い)の中に含まれる正相無効電流を表わしている。
On the other hand, the signals i RL , i SL , and i TL detected as the line currents are converted by the equation (1) in the line / phase converter 402,
As a result, the phase currents i UL , i VL , and i WL of the delta connection (that is, for example, the reactor section 30 in the delta connection of FIG. 8).
If 0 is taken as an example, it is converted into a current flowing through the reactors 302U, 302V, 302W). This signal i UL , i VL , i
The WL is converted by the equation (2) in the two-phase converter 403, and two-phase signals i 1dL and i qL are obtained. Next, arithmetic unit 40
4 to obtain the signals Q 1P and P 1P , and pass them through the separator 407 to obtain the DC component signals Q 1PD and P 1PD.
And AC component signals Q 1PA and P 1PA . The signal Q 1PD thus obtained is the load current signals i RL , i SL , i
It represents the positive-phase reactive current contained in TL (or may be paraphrased as i UL , i VL , and i WL in Expression (1)).

信号Q1PD,Q1PA,Q1NA及び位相角信号▲θ* 1d1▼は
次の分配器415Aに導入される。
The signals Q 1PD , Q 1PA , Q 1NA and the phase angle signal ▲ θ * 1d1 ▼ are introduced to the next distributor 415A.

第2図の分配器415Aの中では2相発生器416Aは
位相角信号▲θ* 1d1▼を受けて交流母線電圧の周波数の
2倍の周波数を持つ式(5)の単位2相電圧信号を発生す
る。また、演算器417A,418A,419Aの中では式(6),(7),
(8)の演算が行われ、第1相,第2相,第3相の同相逆
相電流信号P1ND,P2ND,P3ND、及び第1相,第2
相,第3相の90゜逆相電流信号Q1ND,Q2ND,Q3NDが得
られる。
In the distributor 415A of FIG. 2, the two-phase generator 416A receives the phase angle signal ▲ θ * 1d1 ▼ and outputs the unit two-phase voltage signal of the formula (5) having a frequency twice that of the AC bus voltage. Occur. Further, in the arithmetic units 417A, 418A, and 419A, equations (6), (7),
The calculation of (8) is performed, and the in-phase reverse-phase current signals P 1ND , P 2ND , P 3ND of the first phase, the second phase, and the third phase, and the first phase, the second phase
The 90 ° negative phase current signals Q 1ND , Q 2ND and Q 3ND of the first and third phases are obtained.

以上のようにして得られた信号Q1PDは負荷電流iRL
SL,iTLの中に含まれる正相分電流だけに関係する信
号であり、さらに言えばその正相分電流が有効電流と無
効電流とに分解できるとすれば、その無効電流だけに関
係し、即ち正相無効電流だけに関係する信号である。な
お、電流の正相分に関する諸量の演算、例えば式(4)の
1P等の変換では、どの相に基準を合わせて演算を行っ
ても全く同じ量が演算される。従って正相分に関する演
算は1つの相について行えばよい。
The signal Q 1PD obtained as described above is the load current i RL ,
i SL , i TL is a signal related only to the positive-phase component current, and further, if the positive-phase component current can be decomposed into an active current and a reactive current, it is only related to the reactive current. I.e., a signal related only to the positive-phase reactive current. In the calculation of various quantities related to the positive phase of the current, for example, the conversion of Q 1P or the like in Expression (4), the same quantity is calculated regardless of which phase the calculation is performed. Therefore, the calculation for the positive phase component may be performed for one phase.

また、信号P1ND,Q1ND及びP2ND,Q2ND及びP3ND
3NDに着目すると、これらの信号に負荷電流式(1)のi
UL,iVL,iWL(又はiRL,iSL,iTLと言い換えても
よい)の中に含まれる逆相分電流だけに関係する信号で
あり、さらに言えばP1ND,Q1NDは電流iULの逆相分の
みに、P2ND,Q2NDはiVLの逆相分のみに、P3ND,Q
3NDは電流iWLの逆相分のみに関係する信号であり、さ
らに詳しく言えばP1ND,Q1NDを例にすると、P1ND
電流iULの逆相分の中の線間電圧と同相の電流成分であ
り、Q1NDは電圧と90゜位相のずれた電流成分のみに関係
する信号である。
Also, the signals P 1ND , Q 1ND and P 2ND , Q 2ND and P 3ND ,
Focusing on Q 3ND , these signals can be applied to i of load current equation (1).
UL , i VL , and i WL (or i RL , i SL , and i TL may be paraphrased) are signals related only to the negative-phase component current, and further, P 1ND and Q 1ND are currents. i UL 's reverse phase component only, P 2ND , Q 2ND only i VL 's reverse phase component P 3ND , Q
3ND is a signal related only to the reverse phase component of the current i WL . More specifically, taking P 1ND and Q 1ND as an example, P 1ND has the same phase as the line voltage in the reverse phase component of the current i UL . It is a current component, and Q 1ND is a signal related only to the current component that is 90 ° out of phase with the voltage.

以上、負荷電流iRL,iSL,iTLのあらゆる情報が直流
の信号Q1PD,P1ND,P2ND,P3ND,Q1ND,Q2ND,Q
3NDの形で独立して分離検出されていることが明らかで
あろう。
As described above, all the information of the load currents i RL , i SL , and i TL are DC signals Q 1PD , P 1ND , P 2ND , P 3ND , Q 1ND , Q 2ND , Q.
It will be clear that they are separately detected in the form of 3ND .

こうして得られた信号を第2図の振分器440Aの中で式
(9)に沿って振分け電流指令IU *,IV *,IW *を作る
が、この電流指令IU *,IV *,IW *に基づいて第8図の
リアクトル部の電流を制御すると、逆相電流の制御に関
してはアーク炉の発生する電流の逆相分電流と、リアク
トル部300の発生する補償電流の中の逆相分電流の位
相が丁度反対になるよう制御されるから、従って逆相分
に関してはこれらが点51R、51S、51Tのところ
で合成されお互いに打消し合い、従って逆相電流は電源
1の方へ流れなくなり、電源1の電流が平衡化されるこ
ととなる。次に、正相無効電流に関しては、第2図の加
算器448Aの出力信号が作用し、その結果、負荷の発生す
る電流の正相無効分(遅れ)と第8図のリアクトル部3
00の発生する補償電流の正相無効分(遅れ)との和
が、丁度、第2図の無効電流設定信号Q1MAX(遅れ)に
等しくなるように制御されるから、従ってこれらの一定
の遅れ無効電流と第8図の進相コンデンサ200の進み
無効電流がお互いに打消し合い、その結果、第8図の交
流電源1の方へは無効電流は流れなくなり、交流電源に
は負荷の発生する正相有効電流だけが流れることとな
る。
The signal thus obtained is expressed in the distributor 440A shown in FIG.
Distributing current commands I U * , I V * , and I W * are made along (9). Based on these current commands I U * , I V * , and I W * , the current of the reactor part in FIG. 8 is calculated. When controlled, the anti-phase current is controlled so that the phase of the anti-phase component current of the current generated by the arc furnace and the phase of the anti-phase component current of the compensation current generated by the reactor unit 300 are exactly opposite to each other. Therefore, regarding the anti-phase component, these are combined at points 51R, 51S, 51T and cancel each other, so that the anti-phase current does not flow to the power source 1 and the current of the power source 1 is balanced. . Next, regarding the positive-phase reactive current, the output signal of the adder 448A of FIG. 2 acts, and as a result, the positive-phase reactive component (delay) of the current generated by the load and the reactor unit 3 of FIG.
00 is controlled so that the sum of the compensation current generated by 00 and the positive-phase reactive component (delay) is exactly equal to the reactive current setting signal Q 1MAX (delay) shown in FIG. The reactive current and the advance reactive current of the phase advancing capacitor 200 shown in FIG. 8 cancel each other out. As a result, the reactive current stops flowing to the AC power supply 1 shown in FIG. 8 and a load is generated in the AC power supply. Only the positive-phase active current will flow.

以上の説明から、本発明の無効電力補償装置が作動する
とアーク炉等の負荷が正相分,逆相分を含んだ不平衡電
流を発生しても、無効電流の補償が行われ、及び逆相電
流の補償が行われるため交流電源には正相有効電流だけ
が流れるようになり、従って電圧変動(即ちフリッカ)
を抑制できしかも電源の利用率向上(即ち、無効電力を
扱わなくてよいため)が図れることが分る。
From the above description, when the reactive power compensating device of the present invention operates, even if the load of the arc furnace or the like generates an unbalanced current including a positive phase component and a negative phase component, the reactive current is compensated and the reverse current is compensated. Since the phase current is compensated, only the positive-phase active current flows through the AC power supply, and therefore the voltage fluctuation (that is, flicker).
It can be seen that the power consumption can be improved (that is, reactive power does not have to be handled) and the power consumption can be suppressed.

以上が本発明の代表的な実施例である。The above is a typical embodiment of the present invention.

次に本発明の第2の実施例を第3図により説明する。即
ち、第3図は前述の発明の第2図の分配器415Aの変
形例であり、第3図は第1図の分配器415Aの中に挿
入され使用される。従って、本変形例は前に説明した発
明と重複する部分が多々あり、重複する部分については
説明を省略する。第3図と第1図の同一記号カ所は記号
に合わせて接続される。
Next, a second embodiment of the present invention will be described with reference to FIG. That is, FIG. 3 is a modification of the distributor 415A of FIG. 2 of the above-mentioned invention, and FIG. 3 is inserted and used in the distributor 415A of FIG. Therefore, this modified example has many parts that overlap with the invention described above, and the description of the overlapping parts will be omitted. The same symbols in FIGS. 3 and 1 are connected according to the symbols.

第3図において、416Aは2相発生器であり第2図の
発明と同様に位相角信号▲θ* 1d1▼を受けて式(5)に示
す単位2相電圧信号▲e* 1d2▼,▲e* 1q2▼,▲e* 2d2
▼,▲e* 2q2▼,▲e* 3d2▼,▲e* 3q2▼を発生する。
In FIG. 3, reference numeral 416A denotes a two-phase generator, which receives the phase angle signal ▲ θ * 1d1 ▼ like the invention of FIG. 2 and receives the unit two-phase voltage signal ▲ e * 1d2 ▼, ▲ shown in the equation (5). e * 1q2 ▼, ▲ e * 2d2
▼, ▲ e * 2q2 ▼, ▲ e * 3d2 ▼, ▲ e * 3q2 ▼ are generated.

417Bは演算器であり、前記した信号Q1PA,P1PA
び▲e* 1d2▼,▲e* 1q2▼を入力し式(10)により信号Q
1ND(第1相の90゜逆相電流信号)を演算する。このQ
1NDは前記説明の式(6)で得られた信号Q1NDと同じもの
である。418B,419Bも演算器であり、それぞれ前記信号
1PA,P1PA,▲e* 2d2▼,▲e* 2q2▼及び前記信号Q
1PA,P1PA,▲e* 3d2▼,▲e* 3q2▼を入力し、式(1
1),(12)により信号Q2ND,Q3ND(第2相,第3相の90
゜逆相電流信号)を演算する。ここでもQ2ND,Q3ND
前記説明式(7),(8)で得られた信号Q2ND,Q3NDと同じ
ものである。
417B is a calculator, the signal Q 1PA, P 1PA and ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ signals by input (10) and Q
Calculate 1ND (90 ° reverse-phase current signal of the first phase). This Q
1ND is the same as the signal Q 1ND obtained by the equation (6) described above. Reference numerals 418B and 419B are also arithmetic units, and the signals Q 1PA , P 1PA , ▲ e * 2d2 ▼, ▲ e * 2q2 ▼ and the signal Q, respectively.
Input 1PA , P 1PA , ▲ e * 3d2 ▼, ▲ e * 3q2 ▼, and enter the formula (1
Signals Q 2ND , Q 3ND (second phase, third phase 90
Calculate the negative-phase current signal). Also here, Q 2ND and Q 3ND are the same as the signals Q 2ND and Q 3ND obtained by the above-mentioned equations (7) and (8).

1ND=▲e* 1d2▼・Q1PA+▲e* 1q2▼・P1PA …(1
0) Q2ND=▲e* 2d2▼・Q1PA+▲e* 2q2▼・P1PA …(1
1) Q3ND=▲e* 3d2▼・Q1PA+▲e* 3q2▼・P1PA …(1
2) 447は設定器であり無効電流設定信号Q1MAXを出力す
る。440Bは振分器であり、正相無効電流信号
1PD、第1相,第2相,第3相の90゜逆相電流信号Q
1ND,Q2ND,Q3ND及び無効電流設定信号Q1MAXを入力
し、これらの信号に基づいて式(13)の演算を行い、第1
相,第2相,第3相の電流指令IU *,IV *,IW *を出力
する。ここで、453B,454B,455Bは係数器でも、入力信
号を2倍して出力する。また、448A,449B,450B,451B
は加算器であり図示の信号を図示の極性で加算する。
Q 1ND = ▲ e * 1d2 ▼ · Q 1PA + ▲ e * 1q2 ▼ · P 1PA ... (1
0) Q 2ND = ▲ e * 2d2 ▼ ・ Q 1PA + ▲ e * 2q2 ▼ ・ P 1PA … (1
1) Q 3ND = ▲ e * 3d2 ▼ ・ Q 1PA + ▲ e * 3q2 ▼ ・ P 1PA … (1
2) 447 is a setter which outputs a reactive current setting signal Q 1MAX . 440B is a distributor, which is a positive-phase reactive current signal Q 1PD , a 90 ° negative-phase current signal Q of the first phase, the second phase, and the third phase.
1ND , Q 2ND , Q 3ND and reactive current setting signal Q 1MAX are input, and the calculation of formula (13) is performed based on these signals, and the first
The current commands I U * , I V * , and I W * of the phase, the second phase, and the third phase are output. Here, the coefficient units of 453B, 454B, and 455B also double the input signal and output it. Also, 448A, 449B, 450B, 451B
Is an adder that adds the signals shown in the drawing with the polarities shown.

電流指令IU *,IV *,IW *は前述した式(9)で得られる
電流指令値と全く同一のものであり、従ってこのIU *
V *,IW *に基づいて第8図のリアクトル部300の電
流を制御すると、前述した第1図,第2図による発明と
全く同じ補償効果が得られる。
The current commands I U * , I V * , and I W * are exactly the same as the current command values obtained by the above-mentioned equation (9), and therefore I U * ,
When the current of the reactor part 300 of FIG. 8 is controlled on the basis of I V * and I W * , the same compensation effect as that of the invention according to FIGS. 1 and 2 described above can be obtained.

以上、本実施例では第3図の演算器417B,418B,419Bの
演算が、第2図に示す発明の演算器417A,418A,419Aよ
り簡略化でき、コスト低減出来る。
As described above, in this embodiment, the arithmetic operations of the arithmetic units 417B, 418B, 419B in FIG. 3 can be simplified and the cost can be reduced as compared with the arithmetic units 417A, 418A, 419A of the invention shown in FIG.

次に本発明の第3の実施例を第4図により説明する。第
4図は前記発明の第2図の分配器415Aの変形例であ
り、第1図の分配器415Aの中に挿入される。第4図と第
1図の同一信号カ所は記号に合わせて接続される。
Next, a third embodiment of the present invention will be described with reference to FIG. FIG. 4 is a modification of the distributor 415A of FIG. 2 of the above invention, which is inserted into the distributor 415A of FIG. The same signal points in FIGS. 4 and 1 are connected according to the symbols.

第4図において、416Aは2相発生器であり第2図の
発明と同様に位相角信号▲θ* 1d1▼を受けて式(5)に示
す単位2相電圧信号▲e* 1d2▼,▲e* 1q2▼,▲e* 2d2
▼,▲e* 2q2▼,▲e* 3d2▼,▲e* 3q2▼を発生する。
417C,418C,419Cは演算器であり、前記信号Q1PA,P
1PA及び▲e* 1d2▼,▲e* 1q2▼及び▲e* 2d2▼,▲e*
2q2▼及び▲e* 3d2▼,▲e* 3q2▼を入力し式(14)(15)
(16)により信号P1ND(第1相の同相逆相電流信号)、
2ND(第2相の同相逆相電流信号)、P3ND(第3相の
同相逆相電流信号)を演算する。これら得られた信号P
1ND,P2ND,P3NDは前記説明の式(6),(7),(8)で得られ
たP1ND,P2ND,P3NDと同じものである。
In FIG. 4, 416A is a two-phase generator, which receives the phase angle signal ▲ θ * 1d1 ▼ like the invention of FIG. 2 and receives the unit two-phase voltage signal ▲ e * 1d2 ▼, ▲ shown in the equation (5). e * 1q2 ▼, ▲ e * 2d2
▼, ▲ e * 2q2 ▼, ▲ e * 3d2 ▼, ▲ e * 3q2 ▼ are generated.
417C, 418C, 419C are arithmetic units, and the signals Q 1PA , P
1PA and ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ and ▲ e * 2d2 ▼, ▲ e *
Input 2q2 ▼ and ▲ e * 3d2 ▼, ▲ e * 3q2 ▼ and formula (14) (15)
According to (16), the signal P 1ND (first-phase in-phase reverse-phase current signal),
P 2ND (second-phase in-phase reverse-phase current signal) and P 3ND (third-phase in-phase reverse-phase current signal) are calculated. These obtained signals P
1ND , P 2ND , and P 3ND are the same as P 1ND , P 2ND , and P 3ND obtained by the equations (6), (7), and (8) described above.

1ND=▲e* 1d2▼・P1PA−▲e* 1q2▼・Q1PA …(1
4) P2ND=▲e* 2d2▼・P1PA−▲e* 2q2▼・Q1PA …(1
5) P3ND=▲e* 3d2▼・P1PA−▲e* 3q2▼・Q1PA …(1
6) 447は設定器であり無効電流設定信号Q1MAXを出力す
る。440Cは振分器であり、正相無効電流信号
1PD、第1相,第2相,第3相の同相逆相電流信号P
1ND,P2ND,P3ND及び無効電流設定信号Q1MAXを入力
し、これらの信号に基づいて式(17)の演算を行い、第1
相,第2相,第3相の電流指令IU *,IV *,IW *を出力
する。ここで、441A,442A,443Aは係数器であり入力信
号を 倍して出力する。また、453B,454B,455Bも係数器であ
り入力信号を2倍して出力する。及び、444A,445A,44
6A,448A,449B,450B,451Bは加算器であり、図示の信
号を図示の極性で加算する。
P 1ND = ▲ e * 1d2 ▼ · P 1PA - ▲ e * 1q2 ▼ · Q 1PA ... (1
4) P 2ND = ▲ e * 2d2 ▼ ・ P 1PA − ▲ e * 2q2 ▼ ・ Q 1PA … (1
5) P 3ND = ▲ e * 3d2 ▼ ・ P 1PA − ▲ e * 3q2 ▼ ・ Q 1PA … (1
6) 447 is a setter which outputs the reactive current setting signal Q 1MAX . 440C is a distributor, which is a positive-phase reactive current signal Q 1PD , a first-phase, a second-phase, and a third-phase in-phase reverse-phase current signal P
1ND , P 2ND , P 3ND and reactive current setting signal Q 1MAX are input, and the calculation of formula (17) is performed based on these signals, and the first
The current commands I U * , I V * , and I W * of the phase, the second phase, and the third phase are output. Here, 441A, 442A, 443A are coefficient multipliers, Double and output. Further, 453B, 454B and 455B are also coefficient units, which double the input signal and output it. And 444A, 445A, 44
6A, 448A, 449B, 450B and 451B are adders, which add the signals shown in the drawing with the polarities shown.

電流指令IU *,IV *,IW *は前述した式(9)で得た電流
指令値と全く同一のものであり、従って、このIU *,I
V *,IW *に基づいて第1図のリアクトル部300の電流
を制御すると、前述した第1図,第2図による発明と全
く同じ補償効果が得られる。
The current commands I U * , I V * , and I W * are exactly the same as the current command values obtained by the above-mentioned equation (9). Therefore, I U * , I W *
When the current of the reactor part 300 of FIG. 1 is controlled on the basis of V * and I W * , exactly the same compensation effect as that of the invention shown in FIGS. 1 and 2 can be obtained.

以上、本実施例では第4図の演算器417C,418C,419Cの
演算が第2図の演算器417A,418A,419Aより簡略化で
き、コスト低減出来る。
As described above, in this embodiment, the arithmetic operations of the arithmetic units 417C, 418C and 419C in FIG. 4 can be simplified and the cost can be reduced as compared with the arithmetic units 417A, 418A and 419A in FIG.

さらに本発明の実施例として次のものがある。即ち、本
発明の第4の実施例を第5図により説明する。第5図は
前記発明の第2図の分配器415Aの変形例であり、第
1図の分配器415Aの中に挿入され使用される。第5図と
第1図の同一記号カ所は記号に合わせて接続される。
Further examples of the present invention are as follows. That is, a fourth embodiment of the present invention will be described with reference to FIG. FIG. 5 shows a modified example of the distributor 415A of FIG. 2 of the invention, which is inserted and used in the distributor 415A of FIG. The same symbols in FIGS. 5 and 1 are connected according to the symbols.

第5図において、422Eは2相発生器であり第2図の
発明と同様に位相角信号▲θ* 1d1▼を受けて式(18)に示
す単位2相電圧信号▲e* 1d2▼,▲e* 1q2▼を発生す
る。信号▲e* 1d2▼,▲e* 1q2▼は前記説明の式(5)で
得られた信号▲e* 1d2▼,▲e* 1q2▼と同じものであ
る。423Eは演算器であり、前記信号Q1PA,P1PA
び▲e* 1d2▼,▲e* 1q2▼を入力し、式(19)の演算によ
り信号P1ND(第1相の同相逆相電流信号)、Q1ND(第
1相の90゜逆相電流信号)を出力する。信号P1ND,Q
1NDは前記説明の式(6)で得た信号P1ND,Q1NDと同じも
のである。
In FIG. 5, 422E is a two-phase generator, which receives the phase angle signal ▲ θ * 1d1 ▼ like the invention of FIG. 2 and receives the unit two-phase voltage signal ▲ e * 1d2 ▼, ▲ shown in the equation (18). e * 1q2 ▼ is generated. Signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ is the signal obtained by the equation (5) Description ▲ e * 1d2 ▼, is the same as the e * 1q2 ▼. 423E is a calculator, the signal Q 1PA, P 1PA and ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ enter a, calculated by the signal P 1ND (phase negative sequence current signal of the first phase of the formula (19) ), Q 1ND (first-phase 90 ° reverse-phase current signal) is output. Signal P 1ND , Q
1ND is the same as the signals P 1ND and Q 1ND obtained by the equation (6) described above.

次に424E,425Eは演算器であり、信号P1ND,Q1NDを入
力し、それぞれ式(20)(21)の演算を行い信号Q2ND,P
2ND、及びQ3ND,P3NDを出力する。
Next, 424E and 425E are arithmetic units, which input the signals P 1ND and Q 1ND and perform the arithmetic operations of the equations (20) and (21) respectively to output the signals Q 2ND and P
Outputs 2ND , Q 3ND and P 3ND .

ここでP2NDは第2相の同相逆相電流信号、Q2NDは第2
相の90゜逆相電流信号、P3NDは第3相の同相逆相電流信
号、Q3NDは第3相の90゜逆相電流信号であり、これらの
信号は前記説明の式(7)(8)で得られた信号P2ND
2ND,P3ND,Q3NDと同じものである。
Here, P 2ND is the second-phase in-phase and reverse-phase current signal, and Q 2ND is the second
90 ° anti-phase current signal of the phase, P 3ND is the in-phase anti-phase current signal of the third phase, Q 3ND is the 90 ° anti-phase current signal of the third phase, and these signals are expressed by the equation (7) ( The signal P 2ND obtained in 8),
It is the same as Q 2ND , P 3ND , and Q 3ND .

447は設定器であり無効電流設定信号Q1MAXを出力す
る。440Aは振分器であり、正相無効電流信号
1PD、及び第1相,第2相,第3相の同相逆相電流信
号P1ND,P2ND,P3ND、90゜逆相電流信号Q1ND
2ND,Q3ND、及び無効電流設定信号Q1MAXを入力し、
これらの信号に基づいて前述説明の式(9)の演算を行
い、第1相,第2相,第3相の電流指令IU *,IV *,I
W *を出力する。ここで本変形例第5図の振分器440A
は前記説明の第2図の振分器440Aと同一構成である
ので要素の説明を省略する。
A setter 447 outputs a reactive current setting signal Q 1MAX . Reference numeral 440A denotes a distributor, which has a positive-phase reactive current signal Q 1PD and first-phase, second-phase, and third-phase in-phase negative-phase current signals P 1ND , P 2ND , P 3ND , and a 90 ° negative-phase current signal Q. 1ND ,
Input Q 2ND , Q 3ND , and reactive current setting signal Q 1MAX ,
Based on these signals, the calculation of the equation (9) described above is performed, and the first-phase, second-phase, and third-phase current commands I U * , I V * , I
Output W * . Here, the distributor 440A of FIG.
Has the same configuration as that of the distributor 440A shown in FIG.

電流指令値IU *,IV *,IW *は前述説明した第2図で得
られる電流指令値IU *,IV *,IW *と全く同一のもので
あり、従ってこのIU *,IV *,IW *に基づいて第8図の
リアクトル部300の電流を制御すると、前述の第8
図,第1図,第2図による発明と全く同じ補償効果が得
られる。
The current command value I U *, I V *, I W * the second current command value obtained in Figure I U described above explained *, I V *, are of exactly the same as I W *, thus the I U If the current of the reactor part 300 shown in FIG. 8 is controlled based on * , I V * , and I W * ,
The exactly same compensation effect as the invention according to FIGS. 1, 2 and 3 can be obtained.

以上、本実施例では第5図の演算器424E,425Eの演
算が、第2図の演算器418A,419Aより簡略化でき、従っ
てコスト低減出来る。
As described above, in this embodiment, the arithmetic operations of the arithmetic units 424E and 425E shown in FIG. 5 can be simplified as compared with the arithmetic units 418A and 419A shown in FIG. 2, and the cost can be reduced accordingly.

さらに本発明の実施例として次のものがある。即ち、本
発明の第5の実施例を第6図により説明する。第6図は
前記発明の第2図の分配器415Aの変形例であり、第
1図の分配器415Aの中に挿入され使用される。第6図と
第1図の同一記号カ所は記号に合わせて接続される。
Further examples of the present invention are as follows. That is, a fifth embodiment of the present invention will be described with reference to FIG. FIG. 6 shows a modified example of the distributor 415A of FIG. 2 of the above invention, which is inserted and used in the distributor 415A of FIG. 6 and FIG. 1 are connected according to the same symbols.

第6図において、422Eは2相発生器であり第2図の
発明と同様に位相角信号▲θ* 1d1▼を受けて式(18)に示
す単位2相電圧信号▲e* 1d2▼,▲e* 1q2▼を発生す
る。信号▲e* 1d2▼,▲e* 1q2▼は前記説明の式(5)で
得られた信号▲e* 1d2▼,▲e* 1q2▼と同じものであ
る。423Eは演算器であり、前記信号Q1PA,P1PA
び▲e* 1d2▼,▲e* 1q2▼を入力し、式(19)の演算によ
り信号P1ND(第1相の同相逆相電流信号)、Q1ND(第
1相の90゜逆相電流信号)を出力する。信号P1ND,Q
1NDは前記説明の式(6)で得た信号P1ND,Q1NDと同じも
のである。
In FIG. 6, 422E is a two-phase generator, which receives the phase angle signal ▲ θ * 1d1 ▼ like the invention of FIG. 2 and receives the unit two-phase voltage signal ▲ e * 1d2 ▼, ▲ shown in the equation (18). e * 1q2 ▼ is generated. Signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ is the signal obtained by the equation (5) Description ▲ e * 1d2 ▼, is the same as the e * 1q2 ▼. 423E is a calculator, the signal Q 1PA, P 1PA and ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ enter a, calculated by the signal P 1ND (phase negative sequence current signal of the first phase of the formula (19) ), Q 1ND (first-phase 90 ° reverse-phase current signal) is output. Signal P 1ND , Q
1ND is the same as the signals P 1ND and Q 1ND obtained by the equation (6) described above.

次に424F,425Fは演算器であり、信号P1ND,Q1NDを入
力し、それぞれ式(22)(23)の演算を行い信号Q2ND及び
3NDを出力する。
Next, 424F and 425F are arithmetic units, which receive the signals P 1ND and Q 1ND , respectively, perform the calculations of the equations (22) and (23), and output the signals Q 2ND and Q 3ND .

ここで、Q2NDは第2相の90゜逆相電流信号、Q3NDは第
3相の90゜逆相電流信号であり、これらの信号は前記説
明の式(7)(8)で得られた信号Q2ND,Q3NDと同じもので
ある。
Here, Q 2ND is the second-phase 90 ° negative-phase current signal, and Q 3ND is the third-phase 90 ° negative-phase current signal. These signals are obtained by the equations (7) and (8) described above. The signals Q 2ND and Q 3ND are the same.

447は設定器であり無効電流設定信号Q1MAXを出力す
る。440Bは振分器であり、正相無効電流信号
1PD、及び第1相,第2相,第3相の90゜逆相電流信号
1ND,Q2ND,Q3ND、及び無効電流設定信号Q1MAX
入力し、これらの信号に基づいて前述説明の式(13)の演
算を行い、第1相,第2相,第3相の電流指令IU *,I
V *,IW *を出力する。ここで本変形例の第6図の振分器
440Bは前記説明の第3図の振分器440Bと同一構
成であるので要素の説明を省略する。
A setter 447 outputs a reactive current setting signal Q 1MAX . 440B is a distributor, which is a positive-phase reactive current signal Q 1PD , and 90 ° negative-phase current signals Q 1ND , Q 2ND , Q 3ND of the first phase, the second phase, and the third phase, and a reactive current setting signal Q. 1MAX is input, the above-mentioned equation (13) is calculated based on these signals, and the first-phase, second-phase, and third-phase current commands I U * , I
Outputs V * and IW * . Here, the distributor 440B of FIG. 6 of the present modification has the same configuration as the distributor 440B of FIG. 3 described above, and therefore the description of the elements is omitted.

電流指令値IU *,IV *,IW *は前述説明した第2図で得
られる電流指令値IU *,IV *,IW *と全く同一のもので
あり、従ってこのIU *,IV *,IW *に基づいて第8図の
リアクトル部300の電流を制御すると、前述の第1
図,第2図による発明と全く同じ補償効果が得られる。
The current command value I U *, I V *, I W * the second current command value obtained in Figure I U described above explained *, I V *, are of exactly the same as I W *, thus the I U If the current of the reactor part 300 shown in FIG. 8 is controlled based on * , I V * , and I W * ,
The same compensation effect as the invention according to FIGS. 2 and 3 can be obtained.

以上、本実施例では第6図の演算器424F,425Fの演算
が、第2図発明の演算器418A,419Aより簡略化でき、従
ってコスト低減出来る。
As described above, in this embodiment, the arithmetic operations of the arithmetic units 424F and 425F shown in FIG. 6 can be simplified as compared with the arithmetic units 418A and 419A shown in FIG.

さらに本発明の実施例として次のものがある。即ち、本
発明の第6の実施例を第7図により説明する。第7図は
前記発明の第2図の分配器415Aの変形例であり、第
1図の分配器415Aの中に挿入され使用される。第7図と
第1図の同一記号カ所は記号に合わせて接続される。
Further examples of the present invention are as follows. That is, the sixth embodiment of the present invention will be described with reference to FIG. FIG. 7 shows a modified example of the distributor 415A of FIG. 2 of the above invention, which is inserted and used in the distributor 415A of FIG. 7 and FIG. 1 are connected in accordance with the same symbols.

第7図において、422Eは2相発生器であり第2図の
発明と同様に位相角信号▲θ* 1d1▼を受けて式(18)に示
す単位2相電圧信号▲e* 1d2▼,▲e* 1q2▼を発生す
る。信号▲e* 1d2▼,▲e* 1q2▼は前記説明の式(5)で
得られた信号▲e* 1d2▼,▲e* 1q2▼と同じものであ
る。423Eは演算器であり、前記信号Q1PA,P1PA
び▲e* 1d2▼,▲e* 1q2▼を入力し、式(19)の演算によ
り信号P1ND(第1相の同相逆相電流信号)、Q1ND(第
1相の90゜逆相電流信号)を出力する。信号P1ND,Q
1NDは前記説明の式(6)で得た信号P1ND,Q1NDと同じも
のである。
In FIG. 7, 422E is a two-phase generator, which receives the phase angle signal ▲ θ * 1d1 ▼ like the invention of FIG. 2 and receives the unit two-phase voltage signal ▲ e * 1d2 ▼, ▲ shown in the equation (18). e * 1q2 ▼ is generated. Signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ is the signal obtained by the equation (5) Description ▲ e * 1d2 ▼, is the same as the e * 1q2 ▼. 423E is a calculator, the signal Q 1PA, P 1PA and ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ enter a, calculated by the signal P 1ND (phase negative sequence current signal of the first phase of the formula (19) ), Q 1ND (first-phase 90 ° reverse-phase current signal) is output. Signal P 1ND , Q
1ND is the same as the signals P 1ND and Q 1ND obtained by the equation (6) described above.

次に424G,425Gは演算器であり、信号P1ND,Q1NDを入
力し、それぞれ式(24)(25)の演算を行い信号P2ND及び
3NDを出力する。
Next, 424G and 425G are arithmetic units, which input the signals P 1ND and Q 1ND , perform the arithmetic operations of the equations (24) and (25), respectively, and output the signals P 2ND and P 3ND .

ここで、P2NDは第2相の同相逆相電流信号、P3NDは第
3相の同相逆相電流信号であり、これらの信号は前記説
明の式(7)(8)で得られた信号P2ND,P3NDと同じもので
ある。
Here, P 2ND is a second-phase in-phase reverse-phase current signal, P 3ND is a third-phase in-phase reverse-phase current signal, and these signals are signals obtained by the above-described equations (7) and (8). It is the same as P 2ND and P 3ND .

447は設定器であり無効電流設定信号Q1MAXを出力す
る。440Cは振分器であり、正相無効電流信号
1PD、及び第1相,第2相,第3相の同相逆相電流信
号P1ND,P2ND,P3ND、及び無効電流設定信号Q1MAX
を入力し、これらの信号に基づいて前述説明の式(17)の
演算を行い、第1相,第2相,第3相の電流指令IU *
V *,IW *を出力する。ここで本変形例第7図の振分器
440Cは前記説明の第4図の振分器440Cと同一構
成であるので要素の説明を省略する。
A setter 447 outputs a reactive current setting signal Q 1MAX . 440C is a sorting device, the positive-phase reactive current signal Q 1PD, and the first phase, second phase, third phase of the in-phase reverse-phase current signals P 1ND, P 2ND, P 3ND , and reactive current setting signal Q 1MAX
Is input, and the calculation of the above-described equation (17) is performed based on these signals, and the first-phase, second-phase, and third-phase current commands I U * ,
I V * and I W * are output. Here, since the distributor 440C of FIG. 7 of the present modification has the same configuration as the distributor 440C of FIG. 4 described above, the description of the elements is omitted.

電流指令値IU *,IV *,IW *は前述説明した第2図で得
られる電流指令値IU *,IV *,IW *と全く同一のもので
あり、従ってこのIU *,IV *,IW *に基づいて第8図の
リアクトル部300の電流を制御すると、前述の第1
図,第2図による発明と全く同じ補償効果が得られる。
The current command value I U *, I V *, I W * the second current command value obtained in Figure I U described above explained *, I V *, are of exactly the same as I W *, thus the I U If the current of the reactor part 300 shown in FIG. 8 is controlled based on * , I V * , and I W * ,
The same compensation effect as the invention according to FIGS. 2 and 3 can be obtained.

以上、本実施例では第7図の演算器424G,425Gの演
算が、第2図の演算器418A,419Aより簡略化でき、
従ってコスト低減出来る。
As described above, in this embodiment, the arithmetic operations of the arithmetic units 424G and 425G shown in FIG. 7 can be simplified as compared with the arithmetic units 418A and 419A shown in FIG.
Therefore, the cost can be reduced.

〔発明の効果〕〔The invention's effect〕

以上の説明から明らかなように、本発明の無効電力補償
装置では次のような効果が得られる。即ち、 (1)アーク炉等の変動する負荷が発生する電流は正相分
とともに多量の逆相分を含んだ不平衡電流となるが、本
発明ではこれら正相分,逆相分を明確に分離検出できる
ことから、無効電力補償装置の補償すべき対象が明確に
なり、即ち、正相無効電力だけに着目した制御、逆相電
流にだけに着目した制御、又は、電流の平衡化制御(逆
相電流補償)を優先させ装置に余力がある場合にのみ正
相無効電力補償を行う(優先度制御)、等々の制御が自
在に構成でき、従来のものに比し、より高度な補償制御
が簡単に実現できる。
As is clear from the above description, the reactive power compensator of the present invention has the following effects. That is, (1) the current generated by a fluctuating load such as an arc furnace is an unbalanced current containing a large amount of positive phase components and a large amount of negative phase components, but in the present invention, these positive phase components and negative phase components are clearly defined. Since it can be detected separately, the target to be compensated by the reactive power compensator becomes clear, that is, the control focusing only on the positive phase reactive power, the control focusing only on the negative phase current, or the current balancing control (reverse control). Phase current compensation) is prioritized, and positive phase reactive power compensation is performed only when there is extra capacity in the device (priority control), etc. can be freely configured, and more advanced compensation control than the conventional one can be performed. Easy to achieve.

(2)負荷電流に変動があっても、また進み力率/遅れ力
率にかかわりなく、正相分・逆相分を直流信号の形で連
続的に検出でき、従って制御に不連続性が入り込まない
ことから安定な補償制御が実現できる。
(2) Even if the load current fluctuates, the positive phase component and the negative phase component can be continuously detected in the form of a DC signal regardless of the lead power factor / lag power factor. Since it does not enter, stable compensation control can be realized.

(3)また、制御回路においては負荷電流の正相分,逆相
分を検出する場合、信号処理手段として係数器,加算
器,乗算器等々の簡単な素子を用い、単純な演算を行っ
て所用の信号を得るだけであり、検出信号にあいまいさ
が入り込まず、正確で高精度の信号(正相分,逆相分に
関する)を得ることができる。また回路が簡単なためコ
ストも安くなる。
(3) In the control circuit, when detecting the positive-phase component and the negative-phase component of the load current, simple elements such as a coefficient unit, an adder, and a multiplier are used as signal processing means to perform a simple calculation. It is possible to obtain an accurate and high-accuracy signal (regarding the positive phase component and the negative phase component) without any ambiguity in the detection signal, only by obtaining the required signal. In addition, the cost is low because the circuit is simple.

(4)従って、本発明による無効電力補償装置では、正相
電流と逆相電流に関する情報を正確に分離検出している
ことから、従ってアーク炉のように急変動する負荷であ
っても、その補償対象(即ち、正相無効電流を制御する
のか、逆相電流を制御するのか、等々)を明確にして制
御を行うことができるから、安定で高精度の無効電力補
償が可能となる。
(4) Therefore, in the reactive power compensator according to the present invention, since the information regarding the positive-phase current and the negative-phase current is accurately separated and detected, therefore, even if the load fluctuates rapidly like an arc furnace, Since it is possible to perform control by clarifying the target of compensation (that is, whether to control the positive-phase reactive current, the negative-phase current, etc.), stable and highly accurate reactive power compensation can be performed.

以上述べたように本発明の無効電力補償装置では、従来
の制御には無い、“正相分と逆相分を分離検出しそれに
基づいて補償制御を行う”という全く新しい制御概念が
取込れられているため、よって今後の複雑・高度化する
無効電力補償制御への要求にも充分答えることができ
る。
As described above, the reactive power compensator of the present invention incorporates a completely new control concept that "the positive phase component and the negative phase component are separately detected and the compensation control is performed based on that" which is not in the conventional control. Therefore, it is possible to sufficiently meet the demand for the reactive power compensation control which will be complicated and sophisticated in the future.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明の一実施例を示すブロック図、第2図乃
至第7図は本発明のそれぞれ異る他の実施例を示すブロ
ック図、第8図は本発明が適用される無効電力補償装置
の主回路図、第9図は従来は従来の無効電力補償装置に
採用されている無効電力検出回路のブロック図である。 1……交流電源系統、3……系統インピーダンス、9,
10……アーク炉設備、100……無効電力補償装置、
200……進相コンデンサ、300……リアクトル部、
350……制御回路、400……演算回路、500……
点弧制御回路、402……線/相変換器、403……2
相変換器、404……演算器、405……2相発生器、
408,409……直流検出フィルタ、410,411……加算器、4
15A……分配器、500……点弧制御器、416A,422E
……2相発生器、417A〜419A,471B〜419B,417C〜419C,4
23E,424E,425E,424F,425F,424G,425G……演算器、441A
〜443A,453B〜455B……係数器、444A〜446A,448A〜45
1A,449B〜451B……加算器、447……設定器。
FIG. 1 is a block diagram showing an embodiment of the present invention, FIGS. 2 to 7 are block diagrams showing different embodiments of the present invention, and FIG. 8 is a reactive power to which the present invention is applied. FIG. 9 is a main circuit diagram of the compensator, and FIG. 9 is a block diagram of a reactive power detection circuit conventionally used in a conventional reactive power compensator. 1 ... AC power supply system, 3 ... system impedance, 9,
10 ... Arc furnace equipment, 100 ... Reactive power compensation device,
200 ... Phase advancing capacitor, 300 ... Reactor section,
350 ... control circuit, 400 ... arithmetic circuit, 500 ...
Firing control circuit, 402 ... Line / phase converter, 403 ... 2
Phase converter, 404 ... Calculator, 405 ... 2-phase generator,
408,409 …… DC detection filter, 410,411 …… Adder, 4
15A ... Distributor, 500 ... Ignition controller, 416A, 422E
...... 2-phase generator, 417A to 419A, 471B to 419B, 417C to 419C, 4
23E, 424E, 425E, 424F, 425F, 424G, 425G ... Calculator, 441A
〜443A 、 453B〜455B …… Coefficient multiplier, 444A〜446A 、 448A〜45
1A, 449B to 451B ... Adder, 447 ... Setting device.

Claims (7)

【特許請求の範囲】[Claims] 【請求項1】多相交流電源系統に接続される負荷が発生
する不平衡電力及び無効電力を補償する無効電力補償装
置において、N相多相交流電源の第1相の電圧に同期し
て位相角が▲θ* 1d1▼と変化する単位正弦波信号▲e*
1d1▼と、それより90°位相が遅れて変化する単位正
弦波信号▲e* 1q1▼を得る手段と、 N相多相負荷電流i1L,i2L…iNLを検出し、第1相の
電圧にd軸を合わせた2相変換を行い2相電流信号i
1dL,i1qLを得る手段と、 前記信号▲e* 1d1▼,▲e* 1q1▼とi1dL,i1qLを用い
て P1P=▲e* 1d1▼・i1dL+▲e* 1q1▼・i1qL1P=▲e* 1d1▼・i1qL−▲e* 1q1▼・i1dL の演算を行い信号P1P,Q1pを得る手段と、 前記信号P1p,Q1pの交流成分を取り出し信号P1PA
1PA、及びQ1pの直流成分を取り出し信号Q1PDを得る
手段と、 前記信号▲θ* 1d1▼,Q1PD,P1PA,Q1PAを入力信号
として演算を行いN相・多相交流の第1相,第2相〜第
N相の電流指令を作成する手段とを備え、 該手段により得られた電流指令に基づいて前記無効電力
補償装置を制御することを特徴とする無効電力補償装
置。
1. A reactive power compensator for compensating unbalanced power and reactive power generated by a load connected to a multi-phase AC power supply system, wherein a phase is synchronized with a first phase voltage of an N-phase poly-phase AC power supply. Unit sine wave signal ▲ e * whose angle changes as ▲ θ * 1d1
1d1 ▼ and, means for obtaining a unit sine wave signal e * 1q1 ▼ varying delays from 90 ° phase it, N-phase multi-phase load current i 1L, detects the i 2L ... i NL, the first phase Two-phase current signal i
1 dL, means for obtaining i 1QL, the signal ▲ e * 1d1 ▼, ▲ e * 1q1 ▼ and i 1 dL, P 1P using i 1qL = ▲ e * 1d1 ▼ · i 1dL + ▲ e * 1q1 ▼ · i 1qL Q 1P = ▲ e * 1d1 ▼ ・ i 1qL − ▲ e * 1q1 ▼ ・ i 1dL to obtain the signals P 1P and Q 1p , and the AC component of the signals P 1p and Q 1p 1PA ,
A means for extracting the DC components of Q 1PA and Q 1p to obtain a signal Q 1PD , and a calculation of N-phase / multi-phase AC using the signals ▲ θ * 1d1 ▼, Q 1PD , P 1PA , Q 1PA as input signals. A reactive power compensator comprising: means for generating current commands for the first phase, second phase to Nth phase, and controlling the reactive power compensator based on the current command obtained by the means.
【請求項2】前記電流指令を作成する手段が、 無効電力補償装置が補償すべき無効電力の最大値を指示
するための、無効電流設定信号Q1MAXを設定する手段
と、 前記位相角信号▲θ* 1d1▼に基づいて動作し、位相角が
2▲θ* 1d1▼で変化する単位正弦波信号▲e* 1d2▼とそ
れより90°位相が遅れた単位正弦波信号▲e* 1q2▼、
及び同様に位相が(2▲θ* 1d1▼+2/3π)で変化す
る2相の単位正弦波信号▲e* 2d2▼,▲e* 2q2▼、及び
同様に位相が(2▲θ* 1d1▼−2/3π)で変化する2
相の単位正弦波信号▲e* 3d2▼,▲e* 3q2▼を得る手段
と 前記信号▲e* 1d2▼,▲e* 1q2▼,▲e* 2d2▼,▲e*
2q2▼,▲e* 3d2▼,▲e* 3q2▼及び信号P1PA,Q1PA
に基づいて P1ND=▲e* 1d2▼・P1PA−▲e* 1q2▼・Q1PA1ND=▲e* 1d2▼・Q1PA+▲e* 1q2▼・P1PA2ND=▲e* 2d2▼・P1PA−▲e* 2q2▼・Q1PA2ND=▲e* 2d2▼・Q1PA+▲e* 2q2▼・P1PA3ND=▲e* 3d2▼・P1PA−▲e* 3q2▼・Q1PA3ND=▲e* 3d2▼・Q1PA+▲e* 3q2▼・P1PA の演算を行い信号P1ND,Q1ND,P2ND,Q2ND
3ND,Q3NDを得る手段と、 前記信号Q1MAX,Q1PD,Q1ND,Q2ND,Q3ND
1ND,P2ND,P3NDに基づいて の演算をし、電流指令信号IU *,IV *,IW *を作成する
手段とから成ることを特徴とする特許請求の範囲第1項
記載の無効電力補償装置。
2. A means for creating the current command, means for setting a reactive current setting signal Q 1MAX for instructing the maximum value of the reactive power to be compensated by the reactive power compensator, and the phase angle signal ▲ theta * 1d1 operates based on ▼, phase angle 2 ▲ theta * 1d1 unit sine wave signal varies ▼ ▲ e * 1d2 ▼ the unit sine wave signal delayed from the 90 ° phase it e * 1q2 ▼,
And the two-phase unit sine wave signals ▲ e * 2d2 ▼, ▲ e * 2q2 ▼, and similarly the phase changes by (2 ▲ θ * 1d1 ▼ + 2 / 3π) and (2 ▲ θ * 1d1 ▼). -2 / 3π) changes 2
Unit sine wave signal phase ▲ e * 3d2 ▼, ▲ e * 3q2 ▼ to obtain means and the signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼, ▲ e * 2d2 ▼, ▲ e *
2q2 ▼, ▲ e * 3d2 ▼, ▲ e * 3q2 ▼ and signals P 1PA , Q 1PA
P 1ND = ▲ e * 1d2 ▼ · P 1PA based on the - ▲ e * 1q2 ▼ · Q 1PA Q 1ND = ▲ e * 1d2 ▼ · Q 1PA + ▲ e * 1q2 ▼ · P 1PA P 2ND = ▲ e * 2d2 ▼ ・ P 1PA − ▲ e * 2q2 ▼ ・ Q 1PA Q 2ND = ▲ e * 2d2 ▼ ・ Q 1PA + ▲ e * 2q2 ▼ ・ P 1PA P 3ND = ▲ e * 3d2 ▼ ・ P 1PA − ▲ e * 3q2 ▼・ Q 1PA Q 3ND = ▲ e * 3d2 ▼ ・ Q 1PA + ▲ e * 3q2 ▼ ・ P 1PA is calculated and signals P 1ND , Q 1ND , P 2ND , Q 2ND ,
Means for obtaining P 3ND , Q 3ND , said signals Q 1MAX , Q 1PD , Q 1ND , Q 2ND , Q 3ND ,
Based on P 1ND , P 2ND , P 3ND The means for calculating the current command signals I U * , I V * , and I W *, and the reactive power compensator according to claim 1.
【請求項3】前記電流指令を作成する手段が、 無効電力補償装置が補償すべき無効電力の最大値を指示
するための、無効電流設定信号Q1MAXを設定する手段
と、 前記位相角信号▲θ* 1d1▼に基づいて動作し、位相角が
2▲θ* 1d1▼で変化する単位正弦波信号▲e* 1d2▼とそ
れより90°位相が遅れた単位正弦波信号▲e* 1q2▼、
及び、同様に位相が(2▲θ* 1d1▼+2/3π)で変化
する2相の単位正弦波信号▲e* 2d2▼,▲e* 2q2▼、及
び、同様に位相が(2▲θ* 1d1▼−2/3π)で変化す
る2相の単位正弦波信号▲e* 3d2▼,▲e* 3q2▼を得る
手段と、 前記信号▲e* 1d2▼,▲e* 1q2▼,▲e* 2d2▼,▲e*
2q2▼,▲e* 3d2▼,▲e* 3q2▼及びP1PA,Q1PAに基
づいて Q1ND=▲e* 1d2▼・Q1PA+▲e* 1q2▼・P1PA2ND=▲e* 2d2▼・Q1PA+▲e* 2q2▼・P1PA3ND=▲e* 3d2▼・Q1PA+▲e* 3q2▼・P1PA の演算を行い信号Q1ND,Q2ND,Q3NDを得る手段と、 前記信号Q1MAX,Q1PD,Q1ND,Q2ND,Q3NDに基づい
て I* U=−Q1MAX+Q1PD−2Q1ND* V=−Q1MAX+Q1PD−2Q2ND* W=−Q1MAX+Q1PD−2Q3ND の演算をし、電流指令信号IU *,IV *,IW *を作成する
手段とから成ることを特徴とする特許請求の範囲第1項
記載の無効電力補償装置。
3. A means for generating the current command, means for setting a reactive current setting signal Q 1MAX for instructing the maximum value of the reactive power to be compensated by the reactive power compensator, and the phase angle signal ▲ theta * 1d1 operates based on ▼, phase angle 2 ▲ theta * 1d1 unit sine wave signal varies ▼ ▲ e * 1d2 ▼ the unit sine wave signal delayed from the 90 ° phase it e * 1q2 ▼,
Similarly, the two-phase unit sine wave signals ▲ e * 2d2 ▼, ▲ e * 2q2 ▼, which similarly change the phase by (2 ▲ θ * 1d1 ▼ + 2 / 3π), and the phase (2 ▲ θ * 1d1 ▼ -2 / 3π) unit sine wave signals of two phases which changes in ▲ e * 3d2 ▼, ▲ e * 3q2 ▼ means for obtaining the signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼, ▲ e * 2d2 ▼, ▲ e *
2q2 ▼, ▲ e * 3d2 ▼ , ▲ e * 3q2 ▼ and P 1PA, Q based on the Q 1PA 1ND = ▲ e * 1d2 ▼ · Q 1PA + ▲ e * 1q2 ▼ · P 1PA Q 2ND = ▲ e * 2d2 ▼ ・ Q 1PA + ▲ e * 2q2 ▼ ・ P 1PA Q 3ND = ▲ e * 3d2 ▼ ・ Q 1PA + ▲ e * 3q2 ▼ ・ P 1PA The means to obtain the signals Q 1ND , Q 2ND and Q 3ND the signal Q 1MAX, Q 1PD, Q 1ND , Q 2ND, I based on the Q 3ND * U = -Q 1MAX + Q 1PD -2Q 1ND I * V = -Q 1MAX + Q 1PD -2Q 2ND I * W = -Q The reactive power compensator according to claim 1, further comprising means for calculating 1MAX + Q 1PD -2Q 3ND and creating current command signals I U * , IV * , and I W *. .
【請求項4】前記電流指令を作成する手段が、 無効電力補償装置が補償すべき無効電力の最大値を指示
するための、無効電流設定信号Q1MAXを設定する手段
と、 前記位相角信号▲θ* 1d1▼に基づいて動作し、位相角が
2▲θ* 1d1▼で変化する単位正弦波信号▲e* 1d2▼とそ
れより90°位相が遅れた単位正弦波信号▲e* 1q2▼、
及び、同様に位相が(2▲θ* 1d1▼+2/3π)で変化
する2相単位正弦波信号▲e* 2d2▼,▲e* 2q2▼、及び
同様に位相が(2▲θ* 1d1▼−2/3π)で変化する2
相の単位正弦波信号▲e* 3d2▼,▲e* 3q2▼を得る手段
と、 前記信号▲e* 1d2▼,▲e* 1q2▼,▲e* 2d2▼,▲e*
2q2▼,▲e* 3d2▼,▲e* 3q2▼及びP1PA,Q1PAに基
づいて P1ND=▲e* 1d2▼・P1PA−▲e* 1q2▼・Q1PA2ND=▲e* 2d2▼・P1PA−▲e* 2q2▼・Q1PA3ND=▲e* 3d2▼・P1PA−▲e* 3q2▼・Q1PA の演算を行い、信号P1ND,P2ND,P3NDを得る手段
と、 前記信号Q1MAX,Q1PD,P1ND,P2ND,P3NDに基づい
の演算をし、電流指令信号IU *,IV *,IW *を作成する
手段とから成ることを特徴とする第1項記載の無効電力
補償装置。
4. A means for generating the current command, a means for setting a reactive current setting signal Q 1MAX for instructing a maximum value of reactive power to be compensated by the reactive power compensator, and the phase angle signal ▲ theta * 1d1 operates based on ▼, phase angle 2 ▲ theta * 1d1 unit sine wave signal varies ▼ ▲ e * 1d2 ▼ the unit sine wave signal delayed from the 90 ° phase it e * 1q2 ▼,
Also, a two-phase unit sine wave signal ▲ e * 2d2 ▼, ▲ e * 2q2 ▼, which similarly changes in phase by (2 ▲ θ * 1d1 ▼ + 2 / 3π), and similarly, phase (2 ▲ θ * 1d1 ▼) -2 / 3π) changes 2
Unit sine wave signal phase ▲ e * 3d2 ▼, ▲ e * 3q2 ▼ means for obtaining the signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼, ▲ e * 2d2 ▼, ▲ e *
2q2 ▼, ▲ e * 3d2 ▼ , ▲ e * 3q2 ▼ and P 1PA, P based on the Q 1PA 1ND = ▲ e * 1d2 ▼ · P 1PA - ▲ e * 1q2 ▼ · Q 1PA P 2ND = ▲ e * 2d2 ▼ ・ P 1PA − ▲ e * 2q2 ▼ ・ Q 1PA P 3ND = ▲ e * 3d2 ▼ ・ P 1PA − ▲ e * 3q2 ▼ ・ Q 1PA means to obtain the signals P 1ND , P 2ND , P 3ND And based on the signals Q 1MAX , Q 1PD , P 1ND , P 2ND and P 3ND And a means for producing the current command signals I U * , I V * , I W * , the reactive power compensator according to claim 1.
【請求項5】前記電流指令を作成する手段が、 無効電力補償装置が補償すべき無効電力の最大値を指示
するための無効電流設定信号Q1MAXを設定する手段と、 前記位相信号▲θ* 1d1▼に基づいて動作し位相角が2▲
θ* 1d1▼で変化する単位正弦波信号▲e* 1d2▼とそれよ
り90°位相が遅れた単位正弦波信号▲e* 1q2▼を得る
手段と、 前記信号▲e* 1d2▼,▲e* 1q2▼及びP1PA,Q1PAに基
づいて P1ND=▲e* 1d2▼・P1PA−▲e* 1q2▼・Q1PA1ND=▲e* 1d2▼・Q1PA+▲e* 1q2▼・P1PA の演算を行い信号P1ND,Q1NDを得る手段と、 前記信号P1ND,Q1NDに基づいて の演算を行い信号P2ND,Q2ND,P3ND,Q3NDを得る手
段と、 前記信号Q1MAX,Q1PD,Q1ND,Q2ND,Q3ND
1ND,P2ND,P3NDに基づいて の演算をし、電流指令信号IU *,IV *,IW *を作成する
手段とから成ることを特徴とする特許請求の範囲第1項
記載の無効電力補償装置。
5. A means for creating the current command, means for setting a reactive current setting signal Q 1MAX for instructing a maximum value of reactive power to be compensated by the reactive power compensator, and the phase signal ▲ θ *. Operates based on 1d1 ▼ and phase angle is 2 ▲
theta * 1d1 ▼ and unit sine wave signal e * 1q2 obtain ▼ means unit sine wave signal ▲ e * 1d2 ▼ and it than 90 ° phase change is delayed in the signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ and P 1PA, P based on the Q 1PA 1ND = ▲ e * 1d2 ▼ · P 1PA - ▲ e * 1q2 ▼ · Q 1PA Q 1ND = ▲ e * 1d2 ▼ · Q 1PA + ▲ e * 1q2 ▼ · P signal P 1ND performs an operation of 1PA, means for obtaining the Q 1ND, the signal P 1ND, based on the Q 1ND To obtain the signals P 2ND , Q 2ND , P 3ND , Q 3ND , and the signals Q 1MAX , Q 1PD , Q 1ND , Q 2ND , Q 3ND ,
Based on P 1ND , P 2ND , P 3ND The means for calculating the current command signals I U * , I V * , I W *, and the reactive power compensator according to claim 1.
【請求項6】前記電流指令を作成する手段が、 無効電力補償装置が補償すべき無効電力の最大値を指示
するための無効電流設定信号Q1MAXを設定する手段と、 前記位相信号▲θ* 1d1▼に基づいて動作し位相角が2▲
θ* 1d1▼で変化する単位正弦波信号▲e* 1d2▼とそれよ
り90°位相が遅れた単位正弦波信号▲e* 1q2▼を得る
手段と、 前記信号▲e* 1d2▼,▲e* 1q2▼及びP1PA,Q1PAに基
づいて P1ND=▲e* 1d2▼・P1PA−▲e* 1q2▼・Q1PA1ND=▲e* 1d2▼・Q1PA+▲e* 1q2▼・P1PA の演算を行い信号P1ND,Q1NDを得る手段と、 前記信号P1ND,Q1NDに基づいて の演算を行い信号Q2ND,Q3NDを得る手段と、 前記信号Q1MAX,Q1PD,Q1ND,Q2ND,Q3NDに基づい
て I* U=−Q1MAX+Q1PD−2Q1ND* V=−Q1MAX+Q1PD−2Q2ND* W=−Q1MAX+Q1PD−2Q3ND の演算をし、電流指令信号IU *,IV *,IW *を作成する
手段とから成ることを特徴とする特許請求の範囲第1項
記載の無効電力補償装置。
6. A means for creating the current command, means for setting a reactive current setting signal Q 1MAX for instructing the maximum value of the reactive power to be compensated by the reactive power compensator, and the phase signal ▲ θ *. Operates based on 1d1 ▼ and phase angle is 2 ▲
theta * 1d1 ▼ and unit sine wave signal e * 1q2 obtain ▼ means unit sine wave signal ▲ e * 1d2 ▼ and it than 90 ° phase change is delayed in the signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ and P 1PA, P based on the Q 1PA 1ND = ▲ e * 1d2 ▼ · P 1PA - ▲ e * 1q2 ▼ · Q 1PA Q 1ND = ▲ e * 1d2 ▼ · Q 1PA + ▲ e * 1q2 ▼ · P signal P 1ND performs an operation of 1PA, means for obtaining the Q 1ND, the signal P 1ND, based on the Q 1ND Signal Q 2ND performs an operation of, the means for obtaining the Q 3ND, the signal Q 1MAX, Q 1PD, Q 1ND , Q 2ND, based on the Q 3ND I * U = -Q 1MAX + Q 1PD -2Q 1ND I * V = -Q 1MAX + Q 1PD -2Q 2ND I * W = -Q 1MAX + Q 1PD -2Q 3ND and means for generating current command signals I U * , IV * , I W *. The reactive power compensator according to claim 1.
【請求項7】前記電流指令を作成する手段が、 無効電力補償装置が補償すべき無効電力の最大値を指示
するための無効電流設定信号Q1MAXを設定する手段と、 前記位相信号▲θ* 1d1▼に基づいて動作し位相角が2▲
θ* 1d1▼で変化する単位正弦波信号▲e* 1d2▼とそれよ
り90°位相が遅れた単位正弦波信号▲e* 1q2▼を得る
手段と、 前記信号▲e* 1d2▼,▲e* 1q2▼及びP1PA,Q1PAに基
づいて P1ND=▲e* 1d2▼・P1PA−▲e* 1q2▼・Q1PA1ND=▲e* 1d2▼・Q1PA+▲e* 1q2▼・P1PA の演算を行い信号P1ND,Q1NDを得る手段と、 前記信号P1ND,Q1NDに基づいて の演算を行い信号P2ND,P3NDを得る手段と、 前記信号Q1MAX,Q1PD,P1ND,P2ND,P3NDに基づい
の演算をし、電流指令信号IU *,IV *,IW *を作成する
手段とから成ることを特徴とする特許請求の範囲第1項
記載の無効電力補償装置。
7. A means for creating the current command, means for setting a reactive current setting signal Q 1MAX for instructing a maximum value of reactive power to be compensated by the reactive power compensator, and the phase signal ▲ θ *. Operates based on 1d1 ▼ and phase angle is 2 ▲
theta * 1d1 ▼ and unit sine wave signal e * 1q2 obtain ▼ means unit sine wave signal ▲ e * 1d2 ▼ and it than 90 ° phase change is delayed in the signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ and P 1PA, P based on the Q 1PA 1ND = ▲ e * 1d2 ▼ · P 1PA - ▲ e * 1q2 ▼ · Q 1PA Q 1ND = ▲ e * 1d2 ▼ · Q 1PA + ▲ e * 1q2 ▼ · P signal P 1ND performs an operation of 1PA, means for obtaining the Q 1ND, the signal P 1ND, based on the Q 1ND Based on the signals Q 1MAX , Q 1PD , P 1ND , P 2ND , P 3ND , and means for obtaining the signals P 2ND , P 3ND The means for calculating the current command signals I U * , I V * , I W *, and the reactive power compensator according to claim 1.
JP60200009A 1985-09-10 1985-09-10 Reactive power compensator Expired - Lifetime JPH0625948B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60200009A JPH0625948B2 (en) 1985-09-10 1985-09-10 Reactive power compensator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60200009A JPH0625948B2 (en) 1985-09-10 1985-09-10 Reactive power compensator

Publications (2)

Publication Number Publication Date
JPS6260012A JPS6260012A (en) 1987-03-16
JPH0625948B2 true JPH0625948B2 (en) 1994-04-06

Family

ID=16417273

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60200009A Expired - Lifetime JPH0625948B2 (en) 1985-09-10 1985-09-10 Reactive power compensator

Country Status (1)

Country Link
JP (1) JPH0625948B2 (en)

Also Published As

Publication number Publication date
JPS6260012A (en) 1987-03-16

Similar Documents

Publication Publication Date Title
EP0214661B1 (en) Reactive power compensation apparatus
EP0259805A2 (en) Reactive power compensation apparatus
JPS6122791A (en) 12-pulse ac motor drive device
JPH06233464A (en) Voltage fluctuation and harmonic suppression device
JPH0625951B2 (en) Reactive power compensator
JP3181859B2 (en) Power converter
JPH0625948B2 (en) Reactive power compensator
JPH0625949B2 (en) Reactive power compensator
JP3343711B2 (en) Static var compensator
JPH0625950B2 (en) Reactive power compensator
JPH01270791A (en) Speed controller for induction motor
JPH08322153A (en) Control method of three-phase power converter for reactive power compensation
JP2575682B2 (en) Reactive power compensator
RU2677628C1 (en) Three-phase reactive power compensator
JPH073803Y2 (en) Compensation current detection circuit for power compensator
JPH01152518A (en) Control system for reactive power compensator
JPH0789715B2 (en) Reactive power compensator
JPH0682305B2 (en) Reactive power compensator
JPS6369430A (en) Reactive power compensator
JPH0866032A (en) Cycloconverter control device
JPS63277427A (en) Active type reactive-power compensator
Jiao Novel Control Algorithms for Power Quality Improvement Using Four-Leg Converter
JPH08149824A (en) Inverter parallel operation device
JPH0568343A (en) Inverter constant voltage control circuit for independent and interconnection operation
JPH0130163B2 (en)