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JPH0625950B2 - Reactive power compensator - Google Patents
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JPH0625950B2 - Reactive power compensator - Google Patents

Reactive power compensator

Info

Publication number
JPH0625950B2
JPH0625950B2 JP60200011A JP20001185A JPH0625950B2 JP H0625950 B2 JPH0625950 B2 JP H0625950B2 JP 60200011 A JP60200011 A JP 60200011A JP 20001185 A JP20001185 A JP 20001185A JP H0625950 B2 JPH0625950 B2 JP H0625950B2
Authority
JP
Japan
Prior art keywords
phase
current
signal
signals
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
JP60200011A
Other languages
Japanese (ja)
Other versions
JPS6260014A (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 JP60200011A priority Critical patent/JPH0625950B2/en
Publication of JPS6260014A publication Critical patent/JPS6260014A/en
Publication of JPH0625950B2 publication Critical patent/JPH0625950B2/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

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  • Supply And Distribution Of Alternating Current (AREA)
  • Control Of Electrical Variables (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5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 / Harmonics Countermeasures", edited by the rectifier permanent technical committee, the configuration is the 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30
1u〜301wと、負荷電流検出器81R,81S,8
1T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,51S,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。従つて、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 thyristor 30 connected in series to it
1u to 301w and load current detectors 81R, 81S, 8
1T, voltage detection transformer 70, and its control circuit 350
The reactive power of the arc furnace 10 is detected, the conduction angles of the thyristors 301u to 301w are adjusted in accordance with the detected value, and the reactor current is controlled. That is, in the reactive power compensator 100, the currents of the reactors 302u to 302w are controlled in combination with the action of the phase advancing capacitor 200, 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, 51S, It is controlled to occur at 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 rate 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6図に示す。
In the reactive power compensator 100 having the above configuration, the control circuit 3
How accurately the reactive power generated by the load 10 is detected by 50 is a key to the device performance. An example of this reactive power detection circuit is shown in FIG.

即ち、第6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i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. 6 shows a circuit disclosed in FIG. 2 of JP-A-59-139416. First, a 90 ° delayed phase waveform e 90 of a bus voltage e.
When the product q of the load current i L and the load current i L is created, q becomes a form that includes a direct current component (reactive power component) and an alternating current component that oscillates at twice the fundamental wave frequency. The direct current component q VAR (amount indicating the reactive power) is detected through and the current of the reactor unit 300 is controlled based on the detected direct current component q VAR .

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 fluctuating power generated by an arc furnace (including active power and reactive power) is analyzed, the component of the DC amount that does not fluctuate (that is, positive phase power due to positive phase voltage and 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. , Could not be identified in principle, 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 new and accurate power detection method (including active and reactive components) based on a 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、それにより補償対策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、 負荷が接続されるN相多相交流母線の各々の相の電圧に
同期した単位2相電圧信号と、検出した負荷電流を各々
の相の電圧に合わせて2相変換して得られた2相電流信
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
電流指令に基づいて無効電力補償装置を制御することを
特徴とする。
In order to achieve the above object, the present invention provides a reactive power compensator for compensating the reactive power generated by a load connected to an AC power supply system, wherein the voltage of each phase of an N-phase multi-phase AC bus to which the load is connected is Using a synchronized unit two-phase voltage signal and a two-phase current signal obtained by converting the detected load current into two phases in accordance with the voltage of each phase, positive signals in the load current are calculated by calculating these signals. It is characterized in that the phase reactive component and the anti-phase component are separately detected, a current command of the reactive power compensator is created based on this detection signal, and the reactive power compensator is controlled based on this current command.

〔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5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 provided with the reactive power compensator of the present invention is the same as that of FIG. 5, and the description of the elements mentioned in the description of the conventional example is omitted here.

第5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1
0(炉用トランス9も含む)がつながる母線の電圧(e
RS,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. 5, reference numerals 81R, 81S and 81T denote 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. 70 is a voltage detector which is an arc furnace 1
0 (including the transformer 9 for the furnace) connected to the bus voltage (e
RS , e ST , e TR ) is detected and guided 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▲I* u▼,▲I
* v▼,▲I* w▼を出力する。
Reference numeral 400 is an arithmetic circuit incorporating the present invention.
RL , i SL , i TL and voltage signals e RS , e ST , e TR are input, various calculations are performed, and a current command of a direct current value for instructing the fundamental current that the reactor unit 300 should flow ▲ I * u ▼, ▲ I
Output * v ▼, ▲ I * w ▼.

500は点弧制御器であり、電流指令値▲I* u▼,▲I
* v▼,▲I* w▼を受けて動作し、▲I* u▼,▲I* v▼,
▲I* w▼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3
01u,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
Operates in response to * v ▼, ▲ I * w ▼, ▲ I * u ▼, ▲ I * v ▼,
Thyristor 3 so that reactors 302u, 302v, 302w flow the current (fundamental wave component) indicated by ▲ I * w ▼.
Ignition control is performed on 01u, 301v, and 301w.

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5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5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 the case where the reactor part 300 of FIG. 5 is delta-connected as an example. The same symbols in FIGS. 1 and 5 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5図の
線電流として検出した負荷電流iRS,iSL,iTLを式
(1)の演算によりデルタ結線の相電流iuL,ivL,iwL
に変換する(式(1)の変換は第5図のリアクトル部30
0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 is a line / phase converter, and the load currents i RS , i SL , and i TL detected as the line current in FIG.
Delta connection phase currents i uL , i vL , and i wL by the calculation of (1)
(The conversion of the formula (1) is performed by the reactor unit 30 in FIG.
0 is a necessary conversion when the delta connection is used, and this conversion is not necessary when the star connection is used).

406は第5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)等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5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▲e1d *▼とそれより9
0°位相が遅れた単位正弦波信号▲e1q *▼、及び第2
相と第3相の線間電圧eSTに同期した単位正弦波信号▲
2d *▼と90°位相が遅れた単位正弦波信号▲e
* 2q▼、及び第3相と第1相の線間電圧eTRに同期した
単位正弦波信号▲e* 3d▼と90°位相が遅れた単位正
弦波信号▲e* 3q▼をそれぞれ式(2)の如く発生する(な
お、第5図のリアクトル部300がスター結線の場合に
は、▲e* 1d▼,▲e* 1q▼は第1相の相電圧に、▲e*
2d▼,▲e* 2q▼は第2相の及び▲e* 3d▼,▲e* 3q
は第3相の相電圧にそれぞれ同期させる)。
406 inputs the AC bus voltage signals e RS , e ST , and e TR of FIG. 5, and based on them, the phase lock loop circuit (PLL
Circuit) and the like, and is a two-phase signal generator obtained as its output. As its output, in FIG. 5, the first phase is the R phase and the second phase is the S phase.
Assuming that the phase and the third phase are the T phase, the unit sine wave signal ▲ e 1d * ▼ synchronized with the line voltage e RS of the first phase and the second phase
Unit sine wave signal with 0 ° phase delay ▲ e 1q * ▼, and second
Unit sine wave signal synchronized with the phase-to-line voltage e ST of the third and third phases ▲
e 2d * ▼ and unit sine wave signal with 90 ° phase delay ▲ e
* 2q ▼, and the unit sine wave signal ▲ e * 3d ▼ synchronized with the line voltage e TR of the third and first phases and the unit sine wave signal ▲ e * 3q ▼ with a 90 ° phase delay (Eq. 2) (Note that when reactor part 300 in FIG. 5 is star connected, ▲ e * 1d ▼, ▲ e * 1q ▼ are the phase voltage of the first phase, and ▲ e *
2d ▼, ▲ e * 2q ▼ are for the second phase and ▲ e * 3d ▼, ▲ e * 3q
Are respectively synchronized with the phase voltage of the third phase).

403は2相変換器であり電流信号iuL,ivL,i
wLを、第1相と第2相の線間電圧eRS(即ち、式(2)の
▲e* 1d▼)にd軸を合わせた式(3)に基づく2相変換を
行い、第1相用の2相電流信号i1dL,i1qLを演算す
る。同様に404も2相変換器であり信号iuL,ivL
wLを、第2相と第3相の線間電圧eST(即ち、式(2)
の▲e2d *▼)にd軸を合わせた式(4)に基づく2相変換
を行い、第2相用の2相電流信号i2dL,i2qLを演算す
る。及び405も2相変換器であり信号iuL,ivL,i
wLを、第3相と第1相の線間電圧eTR(即ち式(2)の▲
3d *▼)にd軸を合わせた式(5)に基づく2相変換を行
い、第3相用の2相電流信号i3dL,i3qLを演算する。
Reference numeral 403 is a two-phase converter, which is a current signal i uL , i vL , i
The wL is subjected to a two-phase conversion based on the equation (3) in which the d axis is fitted to the line-to-line voltage e RS of the first phase and the second phase (that is, ▲ e * 1d ▼ of the equation (2)), and The two-phase current signals i 1dL and i 1qL for the phases are calculated. Similarly, 404 is also a two-phase converter and has signals i uL , i vL ,
i wL is the line voltage e ST of the second and third phases (that is, equation (2)
Roh ▲ e 2d * ▼) to perform two-phase conversion based on the formula (4) obtained by combining the d-axis, two-phase current signal i 2dL for the second phase, calculates the i 2qL. And 405 are also two-phase converters, and the signals i uL , i vL , i
wL is the line voltage e TR of the third phase and the first phase (that is, ▲ in equation (2)).
e 3d * ▼) is subjected to two-phase conversion based on the equation (5) in which the d axis is matched, and two-phase current signals i 3dL and i 3qL for the third phase are calculated.

410Aは演算分配器でありその詳細は後述の第2図で
説明するが、信号i1dL,i1qL,i2dL,i2qL
3dL,i3qL及び▲e* 1d▼,▲e* 1q▼,▲e2d *▼,
▲e2q *▼,▲e3d *▼,▲e3q *▼を受けて演算を行な
い、第5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。
Reference numeral 410A is an arithmetic distributor, the details of which will be described later with reference to FIG. 2, but the signals i 1dL , i 1qL , i 2dL , i 2qL ,
i 3dL , i 3qL and ▲ e * 1d ▼, ▲ e * 1q ▼, ▲ e 2d * ▼,
Current command values I u *, I v *, for instructing the current flowing through the reactor unit 300 shown in FIG. 5 by performing calculations upon receiving ▲ e 2q * ▼, ▲ e 3d * ▼, ▲ e 3q * ▼. Output I w *.

500は点孤制御器であり、電流指令値▲Iu *▼,▲I
v *▼,▲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を点孤制
御する。
Reference numeral 500 denotes an ignition controller, which is a current command value ▲ I u * ▼, ▲ I.
v * ▼, ▲ I w * ▼ operates by receiving the, ▲ I u * ▼, ▲ I v * ▼,
▲ I w * ▼ at the indicated current thyristor to (fundamental component) of the reactor 300 is passed 301u, 301V, to Tenko control 301W.

次に第2図により演算分配器410A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411Aは演算器であり信号
1dL,i1qL及び▲e1d *▼,▲e1q *▼を入力し、式
(6)により信号Q1P,Q1N,P1Nを演算する。
Next, the operation distributor 410A will be described with reference to FIG. First
Signals having the same symbols in the drawings and FIG. 2 are connected according to the symbols. In FIG. 2, 411A is an arithmetic unit which inputs signals i 1dL , i 1qL and ▲ e 1d * ▼, ▲ e 1q * ▼,
The signals Q 1P , Q 1N and P 1N are calculated by (6).

負荷電流iRL,iSL,iTLが正相分と逆相分を含む場
合、Q1P,Q1N,P1N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 and a negative phase component, Q 1P , Q 1N , and P 1N are pulses that include a DC component and an AC component that oscillates at twice the fundamental frequency. It becomes a flow.

412A,413Aも演算器であり、それぞれ信号i
2dL,i2qLと▲e* 2d▼,▲e* 2q▼及びi3dL,i3qL
▲e* 3d▼,▲e* 3q▼を受けて式(7),(8)の演算により
信号Q2N,P2N,及びQ3N,P3Nを出力する。これらの
信号Q2N,P2N及びQ3N,P3Nも、負荷電流iRL
SL,iTLが正相分と逆相分を含む場合、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。
412A and 413A are also arithmetic units, each of which has a signal i
2dL , i 2qL and ▲ e * 2d ▼, ▲ e * 2q ▼ and i 3dL , i 3qL and ▲ e * 3d ▼, ▲ e * 3q ▼ are received and the signal Q is calculated by the equations (7) and (8). 2N , P 2N , and Q 3N , P 3N are output. These signals Q 2N , P 2N and Q 3N , P 3N also have load currents i RL ,
When i SL and i TL include a positive phase component and a negative phase component, the pulsating flow includes a direct current component and an alternating current component that oscillates at twice the frequency of the fundamental wave.

421〜427は直流検出フィルタであり、それぞれ信
号Q1P,Q1N,P1N,Q2N,P2N,Q3N,P3Nの直流成
分を検出し、それぞれ信号Q1PD,Q1ND,P1ND
2ND,P2ND,Q3ND,P3NDとして出力する。このよう
にして得られた直流量の信号は次の量を表わす。即ち、
信号Q1PDは負荷電流iRL,iSL,iTLが含む正相無効
電流を表わす。及び、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、Q
1NDを第1相の90°逆相電流信号と呼ぶことにする。
同様に、信号P2ND,Q2NDは式(1)の第2相電流ivL
逆相成分を、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),90°位相の異なる電流成分(Q2ND
を表わしている。及び、信号P3ND,Q3NDは式(1)の第
3相電流iwLの逆相成分を、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),90°位相の異なる電
流成分(Q3ND)を表わしている。ここではP2ND,Q
2ND及びP3ND,Q3NDを第2相の同相逆相電流信号(P
2ND)、第2相の90°逆相電流信号(Q2ND)、及び、
第3相の同相逆相電流信号(P3ND)、第3相の90°
逆相電流信号(Q3ND)と呼んでおく。
Reference numerals 421 to 427 denote direct-current detection filters, which detect the direct-current components of the signals Q 1P , Q 1N , P 1N , Q 2N , P 2N , Q 3N , P 3N , respectively, and output the signals Q 1PD , Q 1ND , P 1ND , respectively.
Output as Q 2ND , P 2ND , Q 3ND , P 3ND . The DC amount signal thus obtained represents the following amount. That is,
The signal Q 1PD represents the positive phase reactive current contained in the load currents i RL , i SL , and i TL . And the signals P 1ND and Q 1ND are the first signals of the equation (1).
The reverse-phase current contained in the phase current i uL is decomposed into a component (P 1ND ) in phase with the line voltage of the first phase and the second phase and a component (Q 1ND ) different in phase from it by 90 °. Current, where P 1ND is the in-phase and in-phase current signal of the first phase, Q 1
1ND will be referred to as the first-phase 90 ° anti-phase current signal.
Similarly, the signals P 2ND and Q 2ND are the components in phase with the opposite phase component of the second phase current i vL of the equation (1) in the line voltage of the second phase and the third phase, and the component different in 90 ° phase from it. In-phase component current (P 2ND ) when decomposed into two, 90 ° phase difference current component (Q 2ND )
Is represented. Also, the signals P 3ND and Q 3ND convert the antiphase component of the third phase current i wL of the equation (1) into the in-phase component of the line voltage of the third phase and the first phase and the component of 90 ° phase difference from that. The in-phase component current (P 3ND ) when decomposed and the current component (Q 3ND ) having a 90 ° phase difference are shown. Here, P 2ND , Q
2ND, P 3ND , and Q 3ND are connected to the second phase in-phase current signal (P
2ND ), 90 ° negative phase current signal of the second phase (Q 2ND ), and
Third-phase in-phase reverse-phase current signal (P 3ND ), third-phase 90 °
It is called a reverse-phase current signal (Q 3ND ).

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5図のリアクトル部300
が発生すべき無効電流(遅れ)の最下値を指示するため
の無効電流設定信号Q1MAXを出力する。
Next, 447 is a setting device, which is the reactor unit 300 shown in FIG.
Outputs a reactive current setting signal Q 1MAX for instructing the lowest 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,Q
3ND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5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,4
46Aの出力は式(9)の第3項の演算に相当する。44
8Aは加算器であり設定信号Q1MAXと信号Q1PD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,44
6A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 ° negative-phase current signals Q 1ND , Q 2ND , Q
Input 3ND , in-phase and out-of-phase current signals P 1ND , P 2ND , P 3ND and 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.
No. 0 first phase current command ▲ I u * ▼ for indicating the current to be generated by the first phase reactor 302u, and similarly, second phase current command ▲ I v * ▼ for the reactor 302v and It outputs the third-phase current command I w * for the reactor 302w. Here, the following elements are included in the distributor 440A. That is, 441A, 442A, 443A
Is a coefficient unit and 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. Adders 444A, 445A, 4
The output of 46A corresponds to the calculation of the third term of Expression (9). 44
Reference numeral 8A is an adder that calculates the setting signal Q 1MAX and the signal Q 1PD with the polarities shown in the figure. 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
48A output signal and adders 444A, 445A, 44
The output signals of 6 A 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5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おも多量に含む場合
であっても第5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 includes all the information about the positive-phase current and the information about the negative-phase current. Therefore,
By controlling the reactor unit 300 of FIG. 5 based on these ▲ I u * ▼, ▲ I v * ▼, and ▲ I w * ▼, the load current of the arc furnace or the like is added to the positive phase component and the negative phase component. The current at point 4 in FIG. 5 can be freely balanced even if it contains a large amount.

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5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も信号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406
は信号eRS,eST,eTRを受けて式(2)に基づく2相信
号▲e* 1d▼,▲e1q *▼(第1相と第2相の線間電圧e
RSに同期)、及び信号▲e2d *▼,▲e2q *▼(第3相と
第1相の線間電圧eSTに同期)を発生する。
First, in FIG. 5, 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 power source bus voltage to which the arc furnace is connected is also the signal e RS , e ST , e.
It is detected as TR and is introduced into the control circuit of the reactive power compensator 100. Next, referring to FIG. 1, a two-phase generator 406
Is a two-phase signal ▲ e * 1d ▼, ▲ e1q * ▼ (the line voltage e of the first phase and the second phase e based on the equation (2) in response to the signals e RS , e ST , e TR.
(Synchronized with RS ) and signals ▲ e 2d * ▼, ▲ e 2q * ▼ (synchronized with the line voltage e ST of the third phase and the first phase).

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5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,302
wに流れる電流に相当する)に変換される。この信号i
uL,ivL,iwLは次の2相変換器403,404,40
5の中で式(3),(4),(5)による変換が行われ、第1相と
第2相の線間電圧eRSにd軸を合わせた2相電流信号i
1dL,i1qL、及び第2相と第3相の線間電圧eSTにd軸
を合わせた2相電流信号i2dL,i2qL、及び、第3相と
第1相の線間電圧eTRにd軸を合わせた2相電流信号i
3dL,i3qLが得られる。こうして得られた信号i1dL
1qL,i2dL,i2qL,i3dL,i3qL及び▲e* 1d▼,▲
* 1q▼,▲e* 2d▼,▲e* 2q▼,▲e* 3d▼,▲e* 3q
▼は演算分配器410Aに入力される。
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, the reactor section 30 in the delta connection of FIG. 5 for example).
Taking 0 as an example, the reactors 302u, 302v, 302
corresponding to the current flowing through w). This signal i
uL , i vL , and i wL are the following two-phase converters 403 , 404 , and 40.
5 is converted by the equations (3), (4) and (5), and the two-phase current signal i in which the d axis is aligned with the line voltage e RS of the first phase and the second phase
1dL , i 1qL , two-phase current signals i 2dL , i 2qL in which the d axis is aligned with the line voltage e ST of the second and third phases, and the line voltage e TR of the third and first phases Two-phase current signal i with d axis aligned to
3dL and i3qL are obtained. The signal i 1dL thus obtained,
i 1qL , i 2dL , i 2qL , i 3dL , i 3qL and ▲ e * 1d ▼, ▲
e * 1q ▼, ▲ e * 2d ▼, ▲ e * 2q ▼, ▲ e * 3d ▼, ▲ e * 3q
▼ is input to the arithmetic distributor 410A.

次に、第2図の演算分配器410Aの中では、演算器4
11Aでは信号▲e1d *▼,▲e1q *▼,i1dL,i1qL
入力され式(6)の演算により信号Q1P,Q1N,P1Nが得
られ、及び演算器412Aでは信号▲e2d *▼,▲e2q *
▼,i2dL,i2qLが入力された式(7)の演算により信号
2N,P2Nが得られ、及び、演算器413Aでは信号▲
* 3d▼,▲e3q *▼,i3dL,i3qLが入力され式(8)の
演算により信号Q3N,P3Nが得られる。これらの信号Q
1P,Q1N,P1N,Q2N,P2N,Q3N,P3Nは次の直流検
出フィルタ421,422,423,424,425,
426,427に入力され信号の中の直流成分が検出さ
れ直流量の信号Q1PD,Q1ND,P1ND,Q2ND,P2ND
3ND,P3NDが得られる。
Next, in the operation distributor 410A shown in FIG.
In 11A, the signals ▲ e 1d * ▼, ▲ e 1q * ▼, i 1dL , i 1qL are input to obtain the signals Q 1P , Q 1N , P 1N by the calculation of the equation (6), and in the calculator 412A, the signal ▲ e 2d * ▼, ▲ e 2q *
The signals Q 2N and P 2N are obtained by the calculation of the equation (7) to which ▼, i 2dL and i 2qL are input, and the signal ▲ is calculated by the calculator 413A.
e * 3d ▼, ▲ e 3q * ▼, it 3dL, signal Q 3N by calculation of i 3QL is input expression (8), P 3N is obtained. These signals Q
1P , Q 1N , P 1N , Q 2N , P 2N , Q 3N , P 3N are the following DC detection filters 421, 422, 423, 424, 425.
426, 427, the DC component in the signal is detected, and the DC amount signals Q 1PD , Q 1ND , P 1ND , Q 2ND , P 2ND ,
Q 3ND and P 3ND are obtained.

こうして得られた直流量の信号Q1PDは負荷電流信号i
RL,iSL,iTL(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分電流を表わ
し、また、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相の線間電圧と同相の
成分とそれと90°位相の異なる成分に分解した場合の
各成分電流即ち、同相電流成分P1ND(第1相の同相逆
相電流)及び90°位相の異なる電流成分Q1ND(第1
相の90°逆相電流)を表わしている。及びP2ND,Q
2NDは第2相の同相逆相電流P2ND,第2相の90°逆相
電流Q2NDである。同様に、P3ND,Q3NDは第3相の同
相逆相電流P3ND、第3相の90°逆相電流Q3NDであ
る。
The signal Q 1PD of the DC amount thus obtained is the load current signal i
RL , i SL , i TL (or may be paraphrased as i uL , i vL , i wL in the equation (1)) represent the positive-phase reactive current, and the signals P 1ND and Q 1ND are First phase current i uL of equation (1)
Each of the component currents when the negative-phase current included in is decomposed into a component having the same phase as the line voltage of the first phase and the second phase and a component having a 90 ° phase difference from that, that is, the common-mode current component P 1ND (of the first phase In-phase and anti-phase currents) and 90 ° phase-different current components Q 1ND (first
90 ° reverse-phase current of the phase). And P 2ND , Q
2ND is the in-phase reverse-phase current P 2ND of the second phase and the 90 ° reverse-phase current Q 2ND of the second phase. Similarly, P 3ND and Q 3ND are a third-phase in-phase reverse-phase current P 3ND and a third-phase 90 ° reverse-phase current Q 3ND .

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(6)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 in the equation (6), 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及び及びP
3ND,Q3NDに着目すると、これらの信号は負荷電流式
(1)のiuL,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
逆相分のみに、P2ND,Q2NDはivLの逆相分のみに、P
3ND,Q3ND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、P
1NDは電流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
Focusing on 3ND and Q 3ND , these signals are
It is a signal related only to the negative-phase component current contained in i uL , i vL , and i wL (or may be paraphrased as i RL , i SL , and i TL ) in (1), and further, P 1ND , Q 1ND is only for the antiphase component of the current i uL , P 2ND , Q 2ND is only for the antiphase component of i vL , P
3ND and Q 3ND are signals 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 is a current component in phase with the line voltage in the antiphase component of the current i uL , 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 *▼,▲
* w▼を作るが、この電流指令▲Iu *▼,▲Iv *▼,▲
w *▼に基づいて第5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51
R,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5図のリアクトル部300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5
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5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 signals thus obtained are distributed along the equation (9) in the distributor 440A of FIG. 2 and the current commands ▲ I u * ▼, ▲ I v * ▼, ▲
I * w ▼ is made, but this current command ▲ I u * ▼, ▲ I v * ▼, ▲
When the current of the reactor part of FIG. 5 is controlled on the basis of I w * , the anti-phase current is controlled by the anti-phase current of the current generated by the arc furnace and the compensation current generated by the reactor part 300. Since the phases of the anti-phase currents are controlled so that they are exactly opposite to each other, these are the points 51 for the anti-phase currents.
R, 51S, and 51T are combined at the R, 51S, and 51T and cancel each other, so that the negative-phase current does not flow toward 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 generation of the reactor unit 300 of FIG. The sum of the compensation current and the positive-phase reactive component (delay) is controlled to be exactly equal to the reactive current setting signal Q 1MAX (delay) in FIG. Fifth
The leading reactive currents of the phase advancing capacitor 200 in the figure cancel each other out, and as a result, the reactive current no longer flows toward the AC power supply 1 in FIG. 5, and only the positive phase active current generated by the load flows in the AC power supply. 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 compensator 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.

次に本発明の他の実施例を第3図により説明する。即
ち、第3図は前述した発明の第2図の演算分配器410
Aの変形例であり、第3図は第1図の演算分配器410
A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, another embodiment of the present invention will be described with reference to FIG. That is, FIG. 3 shows the operation distributor 410 of FIG.
FIG. 3 is a modification of A, and FIG. 3 shows the operation distributor 410 of FIG.
It is inserted in A and used. 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、411Bは演算器であり前記した第1
相の2相電流信号i1dL,i1qL及び第1相の2相電圧信
号▲e1d *▼,▲e1q *▼を入力し式(10)により信号
1P,Q1Nが演算される。
In FIG. 3, 411B is a computing unit, which is the first unit described above.
The two-phase current signals i 1dL and i 1qL of the phase and the two-phase voltage signals ▲ e 1d * ▼ and ▲ e 1q * ▼ of the first phase are input, and the signals Q 1P and Q 1N are calculated by the equation (10).

このQ1P,Q1Nは前記説明の式(6)で得られた信号
1P,Q1Nと同じものである。412B,413Bも演
算器であり、それぞれ前記した第2相の2相電流信号i
2dL,i2qL,2相電圧信号▲e2d *▼・▲e2q *▼と第3
相の2相電流信号i3dL,i3qL,2相電圧信号▲e3d *
▼,▲e3q *▼が入力され、式(11),(12)により信号
2N,Q3Nが演算される。
These Q 1P and Q 1N are the same as the signals Q 1P and Q 1N obtained by the above-mentioned equation (6). Reference numerals 412B and 413B are also arithmetic units, and each of the above-mentioned second-phase two-phase current signal i
2dL , i 2qL , two-phase voltage signal ▲ e 2d * ▼ ・ ▲ e 2q * ▼ and the third
Two-phase current signal i 3dL , i 3qL , two-phase voltage signal ▲ e 3d *
▼ and ▲ e 3q * are input, and the signals Q 2N and Q 3N are calculated by the equations (11) and (12).

2N=▲e2d *▼・i2qL−(−▲e2q *▼)・i2dL…(1
1) Q3N=▲e3d *▼・i3qL−(−▲e* 3q▼)・i3dL…(1
2) このQ2N,Q3Nは前記説明の式(7),(8)で得られた信号
2N,Q3Nと同じものである。
Q 2N = ▲ e 2d * ▼ ・ i 2qL − (-▲ e 2q * ▼) ・ i 2dL … (1
1) Q 3N = ▲ e 3d * ▼ ・ i 3qL − (− ▲ e * 3q ▼) ・ i 3dL … (1
2) These Q 2N and Q 3N are the same as the signals Q 2N and Q 3N obtained by the equations (7) and (8) described above.

次にこれらの信号Q1P,Q1N,Q2N,Q3Nを直流検出フ
ィルタ421,422,424,426に通して直流成
分の信号Q1PD,Q1ND,Q2ND,Q3NDが得られる。
Next, these signals Q 1P , Q 1N , Q 2N and Q 3N are passed through DC detection filters 421, 422, 424 and 426 to obtain DC component signals Q 1PD , Q 1ND , Q 2ND and Q 3ND .

ここでQ1PDは正相無効電流信号であり、Q1NDは第1相
の90°逆相電流信号、Q2NDは第2相の90°逆相電
流信号、Q3NDは第3相の90°逆相電流信号である。
Here, Q 1PD is a positive-phase reactive current signal, Q 1ND is the first-phase 90 ° negative-phase current signal, Q 2ND is the second-phase 90 ° negative-phase current signal, and Q 3ND is the third-phase 90 ° This is a negative-phase current signal.

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Q
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 *▼,▲
w *▼を出力する。
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 , 1st phase, 2nd phase, 3rd phase 90 ° negative phase current signal Q
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
Phase, second phase, third phase current command ▲ I u * ▼, ▲ I v * ▼, ▲
Output I w * ▼.

ここで453B,454B,455Bは係数器であり入
力信号を2倍して出力する。また、448A,449
B,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。
Here, 453B, 454B, and 455B are coefficient multipliers, which double the input signal and output it. Also, 448A, 449
B, 450B, and 451B are adders, which add the illustrated signals with the illustrated polarities.

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 *▼,▲Iv *▼,▲Iw *▼に基づいて第5
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 the expressions described above.
It is exactly the same as the current command value obtained in (9). Therefore, the fifth value is obtained based on these ▲ I u * ▼, ▲ I v * ▼, and ▲ I w * ▼.
If the current of the reactor portion 300 in the figure is controlled, 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411B,412
B,413Bの演算が、第2図の演算器411A,41
2A,413Aより簡略化できる。
As described above, in this embodiment, the arithmetic units 411B and 412 shown in FIG.
The calculation of B and 413B is performed by the calculators 411A and 41 of FIG.
2A and 413A can be simplified.

次に本発明のもう1つの実施例を第4図により説明す
る。本実施例もやはり前述した発明の第2図の変形例に
関するものであり、第4図は第1図の演算分配器410
Aに挿入される。従って前述した発明と重複する部分は
その説明を省略する。
Next, another embodiment of the present invention will be described with reference to FIG. This embodiment also relates to the modification of the above-mentioned invention shown in FIG. 2, and FIG. 4 shows the arithmetic distributor 410 shown in FIG.
Inserted in A. Therefore, the description of the same parts as those of the above-mentioned invention will be omitted.

第4図において、411Cは演算器であり第1相の2相
電流信号i1dL,i1qL及び第1相の2相電圧信号▲e1d
*▼,▲e* 1q▼を入力し式(14)により信号Q1P,Q1N
演算される。
In FIG. 4, reference numeral 411C denotes an arithmetic unit, which is a first-phase two-phase current signal i 1dL , i 1qL and a first-phase two-phase voltage signal ▲ e 1d.
Input signals * ▼ and ▲ e * 1q ▼, and the signals Q 1P and Q 1N are calculated by the equation (14).

このQ1P,P1Nは前記説明の式(6)で得られた信号
1P,P1Nと同じものである。412C,413Cも演
算器であり、それぞれ前記した第2相の2相電流信号i
2dL,i2qL,2相電圧信号▲e* 2d▼,▲e* 2q▼と第3
相の2相電流信号i3dL,i3qL,2相電圧信号▲e* 3d
▼,▲e* 3q▼が入力され、式(15),(16)により信号
2N,P3Nが演算される。
These Q 1P and P 1N are the same as the signals Q 1P and P 1N obtained by the above-mentioned equation (6). Reference numerals 412C and 413C are also arithmetic units, and each of the above-mentioned second-phase two-phase current signals i
2dL , i 2qL , two-phase voltage signal ▲ e * 2d ▼, ▲ e * 2q ▼ and the third
Two-phase current signal i 3dL , i 3qL , two-phase voltage signal ▲ e * 3d
▼ and ▲ e * 3q ▼ are input, and the signals P 2N and P 3N are calculated by the equations (15) and (16).

2N=▲e2d *▼・i2dL+(−▲e2q *▼)・i2qL…(1
5) P3N=▲e3d *▼・i3dL+(−▲e3q *▼)・i3qL…(1
6) このP2N,P3Nは前記説明の式(7),(8)で得られた信号
2N,P3Nと同じものである。
P 2N = ▲ e 2d * ▼ ・ i 2dL + (-▲ e 2q * ▼) ・ i 2qL … (1
5) P 3N = ▲ e 3d * ▼ ・ i 3dL + (-▲ e 3q * ▼) ・ i 3qL … (1
6) The P 2N and P 3N are the same as the signals P 2N and P 3N obtained by the equations (7) and (8) described above.

次にこれらの信号Q1P,P1N,P2N,P3Nを直流検出フ
ィルタ421,423,425,427に通して直流成
分の信号Q1PD,P1ND,P2ND,P3NDが得られる。
Next, these signals Q 1P , P 1N , P 2N and P 3N are passed through DC detection filters 421, 423, 425 and 427 to obtain DC component signals Q 1PD , P 1ND , P 2ND and P 3ND .

ここでQ1PDは正相無効電流信号であり、P1NDは第1相
の同相逆相電流信号、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る。
Here, Q 1PD is a positive-phase reactive current signal, P 1ND is a first-phase in-phase reverse-phase current signal, P 2ND is a second-phase in-phase reverse-phase current signal, and P 3ND is a third-phase in-phase reverse-phase current signal. It is a signal.

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Q
1PD、第1相、第2相、第3相の同相逆相電流信号
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▲I* u▲,▲I* v▲,
▲I* w▲を出力する。ここで、441A,442A,4
43Aは係数器であり入力信号を 倍して出力する。453B,454B,455Bも係数
器であり入力信号を2倍して出力する。また、444
A,445A,446A,448A,449B,450
B,451Bは加算器であり図示の信号を図示の極性で
加算する。
A setter 447 outputs a reactive current setting signal Q 1MAX . 440C is a distributor, which is a positive-phase reactive current signal Q
Input 1PD , first-phase, second-phase, third-phase in-phase reverse-phase current signals P 1ND , P 2ND , P 3ND and reactive current setting signal Q 1MAX, and calculate equation (17) based on these signals. The current command for the first phase, the second phase, and the third phase ▲ I * u ▲, ▲ I * v ▲,
Output ▲ I * w ▲. Here, 441A, 442A, 4
43A is a coefficient unit for input signal Double and output. 453B, 454B and 455B are also coefficient units, which double the input signal and output it. Also, 444
A, 445A, 446A, 448A, 449B, 450
Reference numerals B and 451B denote adders that add the illustrated signals with the illustrated polarities.

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▲I* u▼,▲I* v▼,▲I* w▼に基づいて第5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 the expressions described above.
It is exactly the same as the current command value obtained in (9). Therefore, the current of the reactor part 300 of FIG. 5 is controlled based on these ▲ I * u ▼, ▲ I * v ▼, and ▲ I * w ▼. Then, the above-mentioned first
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4図の演算器411C,412
C,413Cの演算が第2図の演算器411A,412
A,413Aより簡略化できる。
As described above, in this embodiment, the arithmetic units 411C and 412 shown in FIG.
The calculation of C and 413C is performed by the calculators 411A and 412 of FIG.
A, 413A can be simplified.

〔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 reverse phase components together with the positive phase components, but in the present invention, these positive phase components and reverse 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 on only the negative-phase current, or the current balancing control (negative-phase control). Current compensation) can be prioritized and positive-phase reactive power compensation can be performed only when there is remaining capacity in the device (priority control), etc. can be freely configured, and more advanced compensation control can be performed easily compared to the conventional control. realizable.

(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. Only the desired signal is obtained, and an accurate and highly accurate signal (regarding the positive phase component and the negative phase component) can be obtained without any ambiguity in the detection 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/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 / negative-phase current is accurately separated and detected, 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
入れられているため、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 them" 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4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5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6図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…点孤制御回路、40
2…線/相変換器、403〜405…2相変換器、40
6…2相発生器、410A…演算分配器、500…点孤
制御器、411A〜413A,411B〜413B,4
11C〜413C…演算器、421〜427…直流検出
フィルタ、447…設定器、441A〜443A,45
3B〜455B…係数器、444A〜446A,448
A〜451A……加算器。
1 is a block diagram showing an embodiment of the present invention, FIGS. 2 to 4 are block diagrams showing other embodiments of the present invention, and FIG. 5 is an invalidity to which the present invention is applied. FIG. 6 is a main circuit diagram of the power compensator, and FIG. 6 is a block diagram of a reactive power detection circuit adopted in a conventional reactive power compensator. 1 ... AC power supply system, 3 ... System impedance, 9, 10
… Arc furnace equipment, 100… Reactive power compensator, 200…
Phase advancing capacitor, 300 ... Reactor section, 350 ... Control circuit, 400 ... Arithmetic circuit, 500 ... Firing control circuit, 40
2 ... Line / phase converter, 403-405 ... 2 phase converter, 40
6 ... Two-phase generator, 410A ... Arithmetic distributor, 500 ... Pointing controller, 411A-413A, 411B-413B, 4
11C to 413C ... Operation unit, 421 to 427 ... DC detection filter, 447 ... Setting device, 441A to 443A, 45
3B to 455B ... Coefficient unit, 444A to 446A, 448
A to 451A ... Adder.

Claims (4)

【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、第2相、第3相〜第N相
の電圧に同期した単位正弦波信号▲e* 1d▼,▲e
* 2d▼,▲e* 3d▼…▲e* Nd▼と、それに対して90°
位相の遅れた単位正弦波信号▲e* 1q▼,▲e* 2q▼,▲
* 3q▼…▲e* Nq▼を得る手段と、 N相・多相負荷電流i1L,i2L,i3L……iNLを検出
し、これら負荷電流から、それぞれ、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i1dL,i1qL
を得て、第2相の電圧にd軸を合わせた2相変換により
2相電流信号i2dL,i2qLを得て、第3相の電圧にd軸
を合わせた2相変換により2相電流信号i3dL,i3qL
得て、及び、同様の変換を順次行い第N相の2相電流信
号iNdL,iNqLまで得る手段と、 前記信号▲e* 1d▼,▲e* 2d▼,▲e* 3d▼〜▲e
* Nd▼,▲e* 1q▼,▲e* 2q▼,▲e* 3q▼〜▲e* Nq
及びi1dL,i1qL,i2dL,i2qL,i3dL,i3qL〜i
NdL,iNqL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3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 polyphase AC power supply system, comprising: a first phase, a second phase, and a first phase of an N-phase / polyphase AC power supply. Unit sine wave signals ▲ e * 1d ▼, ▲ e synchronized with 3rd to Nth phase voltage
* 2d ▼, ▲ e * 3d ▼ ... ▲ e * Nd ▼ and 90 ° to it
Unit sine wave signal with phase delay ▲ e * 1q ▼, ▲ e * 2q ▼, ▲
e * 3q ▼ ... ▲ e * Nq ▼ means and N-phase / multi-phase load currents i 1L , i 2L , i 3L・ ・ ・ i NL are detected, and from these load currents, the voltage of the first phase is respectively detected. To d
Two-phase current signals i 1dL and i 1qL are performed by performing two-phase conversion with the axes aligned.
To obtain the two-phase current signals i 2dL and i 2qL by the two-phase conversion in which the d-axis is adjusted to the second-phase voltage, and the two-phase current is obtained by the two-phase conversion in which the d-axis is adjusted to the third-phase voltage. Means for obtaining the signals i 3dL , i 3qL and sequentially performing the same conversion to obtain the N-phase two-phase current signals i NdL , i NqL , and the signals ▲ e * 1d ▼, ▲ e * 2d ▼, ▲ e * 3d ▼ 〜 ▲ e
* Nd ▼, ▲ e * 1q ▼, ▲ e * 2q ▼, ▲ e * 3q ▼ ~ ▲ e * Nq
And i 1dL , i 1qL , i 2dL , i 2qL , i 3dL , i 3qL to i
And means for creating current commands for the first phase, second phase, third phase to Nth phase of N-phase / multi-phase alternating current by performing calculation with NdL and i NqL as input signals. A reactive power compensator for controlling the reactive power compensator based on a current command.
【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、 前記信号▲e* 1d▼,▲e* 1q▼とi1dL,i1qLを用いて Q1P=▲e* 1d▼・i1qL−▲e* 1q▼・i1dL1N=▲e* 1d▼・i1dL−▲e* 1q▼・i1qL1N=▲e* 1d▼・i1qL+▲e* 1q▼・i1dL の演算を行い信号Q1P,P1N,Q1Nを得る手段と、 前記信号▲e* 2d▼,▲e* 2q▼とi2dL,i2qLを用いて P2N=▲e* 2d▼・i2dL−▲e* 2q▼・i2qL2N=▲e* 2d▼・i2qL+▲e* 2q▼・i2dL の演算を行い信号P2N,Q2Nを得る手段と、 前記信号▲e* 3d▼,▲e* 3q▼とi3dL,i3qLを用いて P3N=▲e* 3d▼・i3dL−▲e* 3q▼・i3qL3N=▲e* 3d▼・i3qL+▲e* 3q▼・i3dL の演算を行い信号P3N,Q3Nを得る手段と、 前記信号Q1P,P1N,Q1N,P2N,Q2N,P3N,Q3N
直流成分を検出し信号Q1PD,P1ND,Q1ND,P2ND,Q
2ND,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▲I* u▼,▲I* v▼,▲I* w
▼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 signal ▲ e * 1d. Using ▼, ▲ e * 1q ▼ and i 1dL , i 1qL , Q 1P = ▲ e * 1d ▼ ・ i 1qL − ▲ e * 1q ▼ ・ i 1dL P 1N = ▲ e * 1d ▼ ・ i 1dL − ▲ e * 1q ▼ ・ i 1qL Q 1N = ▲ e * 1d ▼ ・ i 1qL + ▲ e * 1q ▼ ・ i 1dL means for obtaining the signals Q 1P , P 1N , Q 1N , and the signal ▲ e * 2d Using ▼, ▲ e * 2q ▼ and i 2dL , i 2qL , P 2N = ▲ e * 2d ▼ ・ i 2dL − ▲ e * 2q ▼ ・ i 2qL Q 2N = ▲ e * 2d ▼ ・ i 2qL + ▲ e * 2q ▼ · i 2dL is calculated to obtain signals P 2N and Q 2N , and P 3N = ▲ e * 3d using the signals ▲ e * 3d ▼, ▲ e * 3q ▼ and i 3dL , i 3qL ▼ · i 3dL - ▲ e * 3q ▼ · i 3qL Q 3N = ▲ e * 3d ▼ i 3qL + ▲ e * 3q ▼ · i 3dL signal P 3N performs an operation of, the means for obtaining the Q 3N, the signal Q 1P, P 1N, Q 1N , P 2N, Q 2N, DC P 3N, Q 3N The components are detected and the signals Q 1PD , P 1ND , Q 1ND , P 2ND , Q
Means for obtaining 2ND , P 3ND , Q 3ND , and said signals Q 1MAX , Q 1PD , Q 1ND , Q 2ND , Q 3ND ,
Based on P 1ND , P 2ND , P 3ND The current command signals ▲ I * u ▼, ▲ I * v ▼, ▲ I * w are calculated.
3. The reactive power compensator according to claim 1, further comprising: means for creating ▼.
【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、 前記信号▲e* 1d▼,▲e* 1q▼とi1dL,i1qLを用いて Q1P=▲e* 1d▼・i1qL−▲e* 1q▼・i1dL1N=▲e* 1d▼・i1qL+▲e* 1q▼・i1dL の演算を行い信号Q1P,Q1Nを得る手段と、 前記信号▲e* 2d▼,▲e* 2q▼とi2dL,i2qL、及び▲
* 3d▼,▲e* 3q▼とi3dL,i3qLを用いて Q2N=▲e* 2d▼・i2qL+▲e* 2q▼・i2dL3N=▲e* 3d▼・i3qL+▲e* 3q▼・i3dL の演算を行い信号Q2N,Q3Nを得る手段と、 前記信号Q1P,Q1N,Q2N,Q3Nの直流成分を検出し信
号Q1PD,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 ▲I* v▼=−Q1MAX+Q1PD−2Q2ND ▲I* w▼=−Q1MAX+Q1PD−2Q3ND の演算をし、電流指令信号▲I* u▼,▲I* v▼,▲I* w
▼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 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 signal ▲ e * 1d. Using ▼, ▲ e * 1q ▼ and i 1dL , i 1qL , Q 1P = ▲ e * 1d ▼ ・ i 1qL − ▲ e * 1q ▼ ・ i 1dL Q 1N = ▲ e * 1d ▼ ・ i 1qL + ▲ e * 1q ▼ · i 1dL calculation means to obtain signals Q 1P and Q 1N , and the signals ▲ e * 2d ▼, ▲ e * 2q ▼ and i 2dL , i 2qL , and ▲.
Using e * 3d ▼, ▲ e * 3q ▼ and i 3dL , i 3qL , Q 2N = ▲ e * 2d ▼ ・ i 2qL + ▲ e * 2q ▼ ・ i 2dL Q 3N = ▲ e * 3d ▼ ・ i 3qL + ▲ e * 3q ▼ · i signal Q 2N performs an operation of 3 dL, means for obtaining the Q 3N, the signal Q 1P, Q 1N, Q 2N , Q 3N of the DC component to detect a signal Q 1PD, Q 1ND, Q 2ND, Q means for obtaining 3ND, the signal Q 1MAX, Q 1PD, Q 1ND , Q 2ND, Q 3ND, on the basis ▲ 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 current command signals ▲ I * u ▼, ▲ I * v ▼, ▲ I * w
3. The reactive power compensator according to claim 1, further comprising: means for creating ▼.
【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、 前記信号▲e* 1d▼,▲e* 1qL▼とi1q,i1qLを用いて Q1P=▲e* 1dL▼・i1qL−▲e* 1q▼・i1dL1N=▲e* 1d▼・i1dL−▲e* 1q▼・i1qL の演算を行い信号Q1P,P1Nを得る手段と、 前記信号▲e* 2d▼,▲e* 2q▼とi2dL,i2qL、及び▲
* 3d▼,▲e* 3q▼とi3dL,i3qLを用いて P2N=▲e* 2d▼・i2dL−▲e* 2q▼・i2qL3N=▲e* 3d▼・i3dL−▲e* 3q▼・i3qL の演算を行い信号P2N,P3Nを得る手段と、 前記信号Q1P,P1N,P2N,P3Nの直流成分を検出し信
号Q1PD,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▲I* u▼,▲I* v▼,▲I* w
▼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, 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 signal ▲ e *. Using 1d ▼, ▲ e * 1qL ▼ and i 1q , i 1qL , Q 1P = ▲ e * 1dL ▼ ・ i 1qL − ▲ e * 1q ▼ ・ i 1dL P 1N = ▲ e * 1d ▼ ・ i 1dL − ▲ e * 1q ▼ · i 1qL operation was carried out signals Q 1P, the means for obtaining a P 1N, the signal ▲ e * 2d ▼, ▲ e * 2q ▼ and i 2dL, i 2qL, and ▲
e * 3d ▼, ▲ e * 3q ▼ and i 3dL, P using the i 3qL 2N = ▲ e * 2d ▼ · i 2dL - ▲ e * 2q ▼ · i 2qL P 3N = ▲ e * 3d ▼ · i 3dL - ▲ e * 3q ▼ and · i signal P 2N performs an operation of 3QL, means for obtaining a P 3N, the signal Q 1P, P 1N, P 2N , P 3N of the DC component of the detected signal Q 1PD, P 1ND, P 2ND, means for obtaining a P 3ND, the signal Q 1MAX, Q 1PD, P 1ND , P 2ND, based on P 3ND The current command signals ▲ I * u ▼, ▲ I * v ▼, ▲ I * w are calculated.
5. The reactive power compensator according to claim 1, further comprising:
JP60200011A 1985-09-10 1985-09-10 Reactive power compensator Expired - Lifetime JPH0625950B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60200011A JPH0625950B2 (en) 1985-09-10 1985-09-10 Reactive power compensator

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Application Number Priority Date Filing Date Title
JP60200011A JPH0625950B2 (en) 1985-09-10 1985-09-10 Reactive power compensator

Publications (2)

Publication Number Publication Date
JPS6260014A JPS6260014A (en) 1987-03-16
JPH0625950B2 true JPH0625950B2 (en) 1994-04-06

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JPS6260014A (en) 1987-03-16

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