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JPH0625949B2 - Reactive power compensator - Google Patents
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JPH0625949B2 - Reactive power compensator - Google Patents

Reactive power compensator

Info

Publication number
JPH0625949B2
JPH0625949B2 JP60200010A JP20001085A JPH0625949B2 JP H0625949 B2 JPH0625949 B2 JP H0625949B2 JP 60200010 A JP60200010 A JP 60200010A JP 20001085 A JP20001085 A JP 20001085A JP H0625949 B2 JPH0625949 B2 JP H0625949B2
Authority
JP
Japan
Prior art keywords
phase
current
signal
reactive power
signals
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
JP60200010A
Other languages
Japanese (ja)
Other versions
JPS6260013A (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 JP60200010A priority Critical patent/JPH0625949B2/en
Priority to AU62349/86A priority patent/AU573101B2/en
Priority to US06/903,957 priority patent/US4698581A/en
Priority to CA000517797A priority patent/CA1300222C/en
Priority to EP86112529A priority patent/EP0214661B1/en
Priority to DE8686112529T priority patent/DE3684207D1/en
Publication of JPS6260013A publication Critical patent/JPS6260013A/en
Publication of JPH0625949B2 publication Critical patent/JPH0625949B2/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, which causes flicker of the lighting equipment and causes the utilization rate of the power supply equipment to decrease. 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," Special Committee for Permanent Rectifiers, 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 electric power of the arc furnace 10 is detected, the conduction angles of the thyristors 301U to 301W are adjusted according to the detected value, and the reactor current is controlled. That is, in the reactive power compensating apparatus 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
示されている方法であり、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. 6 shows the method disclosed in FIG. 2 of Japanese Patent Laid-Open No. 59-139416. First, when the product q of the 90 ° delayed waveform e 90 of the bus voltage e and the 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相変換して得られた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
御することを特徴とする。
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 connected to the load and a unit two-phase voltage signal having a frequency twice the frequency of the AC bus voltage are used, and the positive phase in the load current is calculated through the calculation of these signals. The reactive 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
(以後の説明の便のため、三相系で説明する)は第5図
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 (for the convenience of the following description, it will be described as a three-phase system) is the same as that in FIG. 5, and the elements referred to in the above description of the conventional example will be described. The description 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。30
0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 furnace transformer 9) bus voltage (e
RS , e ST , e TR ) are detected and guided to the control circuit 350. Thirty
Reference numeral 0 denotes a reactor portion, which is normally 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 and various calculations are performed, and a current command of DC value ▲ I * U for instructing the fundamental current that the reactor unit 300 should flow ▼, ▲ 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) designated by ▲ I * W ▼.
Ignition control of 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信号iRL,iSL,iTL
を式(1)の演算によりデルタ結線の相電流iUL,iVL
WLに変換する(式(1)の変換は第5図のリアクトル部
300がデルタ結線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 current signals i RL , i SL , and i TL detected as the line current in FIG.
Is calculated by the equation (1), the phase currents i UL , i VL of the delta connection,
i WL is converted (the conversion of the formula (1) is necessary for the reactor section 300 in FIG. 5 at the time of delta connection, and the star connection does not require this conversion).

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).

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)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▲e* 1d1▼と、それより
90°進んだ単位正弦波信号▲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5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)。
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
A two-phase signal generator obtained by configuring a circuit), and as its output, the first phase is the R phase and the second phase is the S phase in FIG.
Assuming that the phase and the third phase are T phases, 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 advanced by 90 ° * 1q1 ▼ and its phase signal ▲ θ * 1d1 ▼ are output, and ▲ e * 1d1 ▼, ▲ e * 1q1 ▼ are the formula
(3) (Note that when the reactor part 300 of FIG. 5 is star connected, ▲ e * 1d1 ▼, ▲ e * 1q1 ▼ are synchronized with the phase voltage of the first phase).

407も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周波数の2倍の周波数を持つ式
(4)の2相電圧信号▲e* 1d2▼,▲e* 1q2▼を発生す
る。
407 is also a two-phase generator, which operates by receiving the phase angle signal ▲ θ * 1d1 ▼ and has a frequency twice the AC bus voltage frequency.
(4) two-phase voltage signals ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ generates.

404は演算器であり信号i1dL,i1qL及び▲e
* 1d1▼,▲e* 1q1▼を入力し、式(5)により信号Q1N
1Nを演算する。
Reference numeral 404 denotes an arithmetic unit that outputs signals i 1dL , i 1qL and ▲ e
* 1d1 ▼, ▲ e * 1q1 ▼ is input, and the signal Q 1N ,
Calculate P 1N .

負荷電流iRL,iSL,iTLが正相分/逆相分を含む場
合、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 / a negative phase component, Q 1N and P 1N become a pulsating flow that includes a DC component and an AC component that oscillates at a frequency twice the fundamental wave. .

409は分離器であり、410,411の直流検出フィ
ルタと412,413の加算器で構成されており、信号
1N,P1Nを入力し、直流検出フィルタ410,411
によりQ1N,P1Nの直流分を検出し信号Q1ND,P1ND
して出力するとともに、加算器412,413の所で信
号Q1N,P1Nの中から直流分、即ちQ1ND,P1NDを取り
去り、交流成分だけを信号Q1NA,P1NAとして出力す
る。こうして得られた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)で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。
Reference numeral 409 denotes a separator, which is composed of the DC detection filters 410 and 411 and the adders 412 and 413, receives the signals Q 1N and P 1N , and receives the DC detection filters 410 and 411.
Detects the DC components of Q 1N and P 1N and outputs them as signals Q 1ND and P 1ND , and at the places of the adders 412 and 413, the DC components of the signals Q 1N and P 1N , that is, Q 1ND and P 1ND, are output. It is removed and only the AC component is output as the signals Q 1NA and P 1NA . The P 1ND and Q 1ND thus obtained are the components (P 1ND ) in phase with the reverse phase current included in the first phase current i UL of the equation (1) in the line voltage of the first phase and the second phase, and 90 ° Indicates the current of each component when it is decomposed by components with different phases (Q 1ND ), where P 1ND is the in-phase reverse-phase current signal of the first phase, Q 1ND
Will be referred to as a first-phase 90 ° anti-phase current signal.

408は演算器であり信号Q1NA,P1NA及び▲e
* 1d2▼,▲e* 1q2▼を入力し、式(6)により信号Q1PD
演算する。
Reference numeral 408 denotes an arithmetic unit which outputs signals Q 1NA , P 1NA and ▲ e
* 1d2 ▼, ▲ e * 1q2 ▼ enter a calculates the signal Q 1PD by equation (6).

1PD=▲e* 1d2▼・Q1NA−▲e* 1q2▼・P1NA ……
(6) 信号Q1PDは直流信号となり、このQ1PDは負荷電流
RL,iSL,iTLが含む正相無効電流を表わしている。
Q 1PD = ▲ e * 1d2 ▼ · Q 1NA - ▲ e * 1q2 ▼ · P 1NA ......
(6) The signal Q 1PD becomes a DC signal, and this Q 1PD represents the positive-phase reactive current included in the load currents i RL , i SL , and i TL .

420Aは分配器であり信号Q1PD,Q1ND,P1ND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▲I* U▼,▲I* V▼,
▲I* W▼を出力する。分配器420Aの詳細を第2図に
示す。
Reference numeral 420A denotes a distributor, which receives signals Q 1PD , Q 1ND and P 1ND to perform calculation, and current command values ▲ I * U ▼, ▲ I * V for instructing the current flowing through the reactor unit 300 shown in FIG. ▼ 、
Output ▲ I * W ▼. The details of the distributor 420A are shown in FIG.

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
1ND300が流すようサイリスタ301U,301V,3
01W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 ▼,
Thyristors 301U, 301V, 3 so that the current (fundamental wave component) instructed by ▲ I * W ▼ flows through reactor 1ND 300
Ignition control of 01W.

次に第2図により分配器420A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、421A,424Aは演算器であり、
第1相の90°逆相電流信号Q1NDと第1相の同相逆相
電流信号P1NDを入力し、それぞれ式(7),(8)の演算を通
して、第2相の90°逆相電流信号Q2ND、第2相の同
相逆相電流信号P2ND及び第3相の90°逆相電流信号
3ND,第3相の同相逆相電流信号P3NDを出力する。
Next, the distributor 420A 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, 421A and 424A are arithmetic units,
The first-phase 90 ° negative-phase current signal Q 1ND and the first-phase in-phase negative-phase current signal P 1ND are input, and the second-phase 90 ° negative-phase current is calculated through the equations (7) and (8), respectively. The signal Q 2ND , the second-phase in-phase reverse-phase current signal P 2ND, the third-phase 90 ° reverse-phase current signal Q 3ND , and the third-phase in-phase reverse-phase current signal P 3ND are output.

ここで、P2ND,Q2NDは式(1)の第2相電流iVLの逆相
成分を、第2相・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。
Here, P 2ND and Q 2ND are obtained by converting the opposite phase component of the second phase current i VL in the equation (1) into a component in phase with the line voltage of the second and third phases and a component having a 90 ° phase difference with it. The in-phase component current (P 2ND ) when decomposed and the current component (Q 2ND ) having a 90 ° phase difference are shown.

同様に、P3ND,Q3NDは式(1)の第3相電流iWLの逆相
成分を、第3相・第1相に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。
Similarly, P 3ND and Q 3ND are obtained by converting the negative phase component of the third phase current i WL of the equation (1) into the third phase and the first phase, which are in-phase with the line voltage, and different from the phase with 90 ° phase. The in-phase component current (P 3ND ) when decomposed and the current component (Q 3ND ) having a 90 ° phase difference are shown.

437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)の最大値を指示するための
無効電流設定信号Q1MAXを出力する。
A setter 437 outputs a reactive current setting signal Q 1MAX for instructing the maximum value of the reactive current (delay) to be generated by the reactor unit 300 in FIG.

430A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▲I* U▼、及び同様リア
クトル302Vのための第2相の電流指令▲I* V▼、及
びリアクトル302Wのための第3相の電流指令▲I* W
▼を出力する。ここで振分器430Aを構成するものと
して次の要素がある。即ち、431A,432A,43
3Aは係数器であり入力信号を 倍して出力する。434A,435A,436Aは加算
器であり係数器431A,432A,433Aの出力を
図示の極性で加算する。加算器434A,435A,436Aの
出力は式(9)の第3項の演算に相当する。438Aは加
算器であり設定信号Q1NAXと信号Q1PDを図示極性で演
算する。即ち、加算器438Aの出力は式(9)の第1項
の演算に相当する。439A,440A,441Aは加
算器であり信号Q1ND,Q2ND,Q3NDと加算器438Aの出
力信号、及び係数器434A,435A,436Aの出
力信号を図示の極性で加算する。
430A 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.
0 first phase current command ▲ I * U ▼ for indicating the current to be generated by the first phase reactor 302U, and second phase current command ▲ I * V ▼ for the reactor 302V, and Third-phase current command for reactor 302W ▲ I * W
Output ▼. Here, the following elements are included in the distributor 430A. That is, 431A, 432A, 43
3A is a coefficient unit for input signal Double and output. 434A, 435A and 436A are adders which add the outputs of the coefficient units 431A, 432A and 433A with the polarities shown. The outputs of the adders 434A, 435A and 436A correspond to the calculation of the third term of the equation (9). An adder 438A calculates the setting signal Q 1NAX and the signal Q 1PD with the polarities shown. That is, the output of the adder 438A corresponds to the calculation of the first term of Expression (9). Reference numerals 439A, 440A and 441A denote adders which add the signals Q 1ND , Q 2ND and Q 3ND and the output signal of the adder 438A and the output signals of the coefficient multipliers 434A, 435A and 436A with the polarities shown.

以上の演算で得られた信号▲I* U▼,▲I* V▼,▲I* W
▼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▲I* U▼,▲I* V▼,▲I* W▼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をも
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。
Signals obtained by the above calculation ▲ I * U ▼, ▲ I * V ▼, ▲ I * W
▼ is a DC amount signal, 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 part 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 reversed in addition to the positive phase component. Even when the phase component is included in a large amount, the current at point 4 in FIG. 5 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因線電圧も信号eRS,eST,e
TRとして検出され無効電力補償装置100制御回路に導
入される。
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 line 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 reactive power compensator 100 control circuit.

次に、第1図において、2相発生器406は信号eRS
ST,eTRを受けて式(3)に基づく2相信号▲e
* 1d1▼,▲e* 1q1▼とその位相角信号▲θ* 1d1▼を出力
し、次に2相発生器407は位相角信号▲θ* 1d1▼を受
けて式(4)に基づく2相信号▲e* 1d2▼,▲e* 1q2▼を
発生する。
Next, referring to FIG. 1, the two-phase generator 406 outputs the signal e RS ,
Two-phase signal ▲ e based on equation (3) in response to e ST and e TR
* 1d1 ▼, ▲ e * 1q1 ▼ and its phase angle signal ▲ θ * 1d1 ▼ are output, and then the two-phase generator 407 receives the phase angle signal ▲ θ * 1d1 ▼ and outputs the two-phase based on the equation (4). signal ▲ e * 1d2 ▼, to generate the e * 1q2 ▼.

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
UL,iVL,iWL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,i1qLが得られる。次
に演算器404の中で式(5)の演算を行い信号Q1N,P
1Nを得て、これを分離器409に通して直流成分の信号
1ND,P1ND及び交流成分の信号Q1NA,P1NAに分離す
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. 5).
Taking 0 as an example, Actors 302U, 302V, 302W
Corresponding to the current flowing in). The signals i UL , i VL , and i WL are converted by the equation (2) in the two-phase converter 403, and two-phase signals i 1dL and i 1qL are obtained. Next, the arithmetic operation of the equation (5) is performed in the arithmetic unit 404 to output the signals Q 1N , P
1N is obtained, and this is passed through a separator 409 to be separated into DC component signals Q 1ND and P 1ND and AC component signals Q 1NA and P 1NA .

こうして得られた信号Q1ND,P1ND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、各成分の電流、即ち、同相電流成分
(P1ND)及び90°位相の異なる電流成分(Q1ND)を
表わしている (P1ND:第1相の同相逆相電流、Q1ND:第1相の90
°逆相電流)。
The signals Q 1ND and P 1ND obtained in this way are such that the reverse phase current included in the first phase current i UL of the equation (1) is the same phase component as the line voltage of the first phase and the second phase and 90 ° phase with it. Represents the current of each component when decomposed into different components of P, ie, the in-phase current component (P 1ND ) and the current component with a 90 ° phase difference (Q 1ND ) (P 1ND : in-phase reverse phase of the first phase). Current, Q 1ND : 90 of the first phase
Reverse phase current).

一方、演算器408では信号▲e* 1d2▼,▲e* 1q2▼と
1NA,P1NAとで式(6)の演算が行われ直流信号のQ1PD
が得られるが、この信号は負荷電流信号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している。
On the other hand, the arithmetic unit 408 the signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ and Q 1NA, the operation is performed DC signal of formula (6) and P 1NA Q 1PD
Which is the load current signal 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)).

次に第2図の分配器420Aの中では演算器421A,
424Aの中で式(7),(8)の演算を行って、第2相の同
相逆相電流P2ND,90°逆相電流Q2ND、第3相の同相
逆相電流P3ND,90°逆相電流Q3NDが得られる。
Next, in the distributor 420A of FIG.
Equation (7) in 424A, performs an operation of (8), a second phase of the in-phase reverse-phase current P 2ND, 90 ° reverse-phase current Q 2ND, third phase of the in-phase reverse-phase current P 3ND, 90 ° A reverse phase current Q 3ND is 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(6)
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 contained in i TL and i TL . Further, if the positive-phase component current can be decomposed into an active current and a reactive current, it is only the reactive current. It is a signal that is relevant, ie, only the positive-phase reactive current.
Note that the calculation of various quantities related to the positive phase component of the current, for example, equation (6)
In the conversion of etc., the exact same amount 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、これらの信号は負荷電流式(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 are i in 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430Aの中で
式(9)に沿って振分け電流指令▲I* U▼,▲I* V▼,▲
* W▼を作るが、この電流指令▲I* U▼,▲I* V▼,▲
* 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、リアクリル部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,51
S,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 438A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5図の進相コンデンサの進み無効電
流がお互いに打消し合い、その結果、第5図の交流電流
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 430A 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 ▼, regarding the control of the anti-phase current, the anti-phase current of the current generated by the arc furnace and the compensation current generated by the rear acrylic part 300 are controlled. Since the opposite-phase currents are controlled so that their phases are exactly opposite to each other, these are the points 51R and 51 for the opposite-phase component.
Since they are combined at S and 51T and cancel each other out, the reverse-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 438A in 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 in 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 shown in FIG. 5 cancel each other out. As a result, the reactive current does not flow to the AC current 1 shown in FIG. Only the 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(即ち、無効電力を扱わ
なくてよい)向上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 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 suppressed and the utilization factor of the power source (that is, reactive power need not be handled) can be improved.

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図の分配器420Aの
変形例であり、第3図は第1図の分配器420A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 is a modification of the distributor 420A of FIG. 2 of the invention described above, and FIG. 3 is used by inserting it into the distributor 420A 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、421B,424Bは演算器であり、
前記した第1相の90°逆相電流信号Q1NDと第1相の
同相逆相電流信号P1NDを入力し、それぞれ式(10),(11)
の演算を通して第2相の90°逆相電流信号Q2ND,第
3相の90°逆相電流信号Q3NDを出力する。この
2ND,Q3NDは前記説明の式(7),(8)で得られた信号Q
2ND,Q3NDと同じものである。
In FIG. 3, 421B and 424B are arithmetic units,
The first-phase 90 ° anti-phase current signal Q 1ND and the first-phase in-phase anti-phase current signal P 1ND described above are input, and equations (10) and (11) are respectively inputted.
The second phase 90 ° anti-phase current signal Q 2ND and the third phase 90 ° anti-phase current signal Q 3ND are output through the above calculation. These Q 2ND and Q 3ND are the signals Q obtained by the equations (7) and (8) described above.
It is the same as 2ND and Q3ND .

437は設定器であり、無効電流設定信号Q1MAXを出力
する。430B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(12)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、446B,447B,44
8Bは係数器であり入力信号を2倍して出力する。ま
た、438A,439B,440B,441B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 437 outputs a reactive current setting signal Q 1MAX . 430B 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 (12) is performed based on these signals, and the first
Phase, second phase, third phase current command ▲ I * U ▼, ▲ I * V ▼, I
Output ▲ * W ▼. Here, 446B, 447B, 44
8B is a coefficient unit which doubles the input signal and outputs it. Further, reference numerals 438A, 439B, 440B, and 441B are adders, which add the illustrated signals with the illustrated polarities.

電流指令▲I* U▼,▲I* V▼,▲I* W▼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▲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 above-mentioned formulas.
It is exactly the same as the current command value obtained in (9). Therefore, based on this ▲ I * U ▼, ▲ I * V ▼, ▲ I * W
If the current of the reactor portion 300 in the figure is controlled, 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3図の演算器421B,424B
の演算が、第2図の演算器421A,424Aより簡略
化できる。
As described above, in this embodiment, the arithmetic units 421B and 424B shown in FIG.
Can be simplified by the arithmetic units 421A and 424A shown in FIG.

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図の分配器420Aに
挿入され使用される。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 FIG. 2 of the invention described above, and FIG. 4 is inserted into the distributor 420A of FIG. 1 for use. Therefore, the description of the same parts as those of the above-mentioned invention will be omitted.

第4図において、421C,424Cは演算器であり、
前記した第1相の90°逆相電流信号Q1NDと第1相の
同相逆相電流信号P1NDを入力し、それぞれ式(13),(14)
の演算を通して第2相の同相逆相電流信号P2ND、第3
相の同相逆相電流信号P3NDを出力する。このP2ND,P
3NDは前記説明式(7),(8)で得られた信号P2ND,P3ND
同じものである。
In FIG. 4, 421C and 424C are arithmetic units,
The first-phase 90 ° negative-phase current signal Q 1ND and the first-phase in-phase negative-phase current signal P 1ND described above are input, and the equations (13) and (14) are respectively inputted.
2nd phase in-phase current signal P 2ND , 3rd phase
The in-phase and out-of-phase current signal P 3ND of the phase is output. This P 2ND , P
3ND is the same as the signals P 2ND and P 3ND obtained by the above described equations (7) and (8).

437は設定器であり、無効電流設定信号Q1MAXを出力
する。430C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(15)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、431A,432A,4
33Aは係数器であり入力信号を 倍して出力する。446B,447B,448Bも係数
器であり入力信号を2倍して出力する。また、438A,4
39B,440B,441B,434A,435A,4
36A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 437 outputs a reactive current setting signal Q 1MAX . 430C 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 (15) based on these signals. The current command for the first phase, second phase, and third phase ▲ I * U ▼, ▲ I * V ▼,
Output ▲ I * W ▼. Here, 431A, 432A, 4
33A is a coefficient unit for input signal Double and output. 446B, 447B, 448B are also coefficient units, which double the input signal and output it. Also, 438A, 4
39B, 440B, 441B, 434A, 435A, 4
36A is an adder that adds the signals shown in the drawing with the polarities shown.

電流指令▲I* U▼,▲I* V▼,▲I* W▼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 the above-mentioned formulas.
It is exactly the same as the current command value obtained in (9). Therefore, the current of the reactor part 300 in FIG. 1 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421C,424C
の演算が第2図の演算器421A,424Aより簡略化
できる。
As described above, in this embodiment, the arithmetic units 421C and 424C shown in FIG.
Can be simplified by the arithmetic units 421A and 424A shown in FIG.

〔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 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 multiplier, 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. Also, because the circuit is simple,
The cost will be lower.

(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 demands for the reactive power compensation control which will become more 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な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…点弧制御回路、40
2…線/相変換器、403…2相変換器、404,40
8…演算器、406,407…2相発生器、409…分離
器、410,411…直流検出フィルタ、412,41
3…加算器、420A…分配器、500…点弧制御器、
421A,424A,421B,424B,421C,
424C…演算器、431A〜433A,446B〜4
48B…係数器、437…設定器、434A〜436
A,438A〜441A,439B〜441B…加算
器。
FIG. 1 is a block diagram showing an embodiment of the present invention, FIGS. 2 to 4 are block diagrams showing different embodiments of the present invention, and FIG. 5 is a reactive power compensation to which the present invention is applied. FIG. 6 is a main circuit diagram of the device, and FIG. 6 is a block diagram of a reactive power detection circuit adopted in a conventional reactive power compensating device. 1 ... AC power supply system, 3 ... System impedance, 9, 10
… Arc furnace equipment, 100… Reactive power compensator, 200…
Phase advancing capacitor, 300 ... Reactor part, 350 ... Control circuit, 400 ... Arithmetic circuit, 500 ... Firing control circuit, 40
2 ... Line / phase converter, 403 ... 2 phase converter, 404, 40
8 ... Operation unit, 406, 407 ... Two-phase generator, 409 ... Separator, 410, 411 ... DC detection filter, 412, 41
3 ... Adder, 420A ... Distributor, 500 ... Firing controller,
421A, 424A, 421B, 424B, 421C,
424C ... Operation unit, 431A to 433A, 446B to 4
48B ... Coefficient device, 437 ... Setting device, 434A to 436
A, 438A to 441A, 439B to 441B ... 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相に同期して位相が▲θ* 1d1
で変化する単位正弦波信号▲e* 1d1▼と、それより90
°位相が進んで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i1dL,i
1qLを得る手段と、 前記信号▲e* 1d1▼,▲e* 1q1▼とi1dL,i1qLを用いて P1N=▲e* 1d1▼・i1dL+▲e* 1q1▼・i1qL1N=▲e* 1d1▼・i1qL−▲e* 1q1▼・i1dL の演算により信号P1N,Q1Nを得る手段と、 前記信号P1N,Q1Nの交流成分を検出し信号P1NA,Q
1NAを得、及び、P1N,Q1Nの直流成分を検出し信号P
1ND,Q1NDを得る手段と、 前記位相角信号▲θ* 1d1▼に基づいて動作し、位相角が
▲2θ* 1d▼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P1NA,Q1NAに基
づいて Q1PD=▲e* 1d2▼・Q1NA−▲e* 1q2▼・P1NA の演算により信号Q1PDを得る手段と、 前記信号Q1PD,P1ND,Q1ND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 for 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 of an N-phase multi-phase AC power supply. θ * 1d1
Unit sine wave signal ▲ e * 1d1 ▼ that changes with
° Means to obtain a unit sine wave signal ▲ e * 1q1 ▼ whose phase advances and changes, and N-phase multi-phase load currents i 1L , i 2L …… i NL are detected, and the d-axis is aligned with the voltage of the first phase. The two-phase current signal i 1dL , i
Means for obtaining a 1QL, the signal ▲ e * 1d1 ▼, ▲ e * 1q1 ▼ and i 1 dL, with i 1qL P 1N = ▲ e * 1d1 ▼ · i 1dL + ▲ e * 1q1 ▼ · i 1qL Q 1N = ▲ e * 1d1 ▼ · i 1qL - ▲ e * 1q1 ▼ · i means for obtaining signals P 1N, the Q 1N by calculation of 1 dL, the signal P 1N, detects the AC component of the Q 1N signal P 1NA, Q
1NA is obtained and the DC component of P 1N and Q 1N is detected to obtain the signal P
A means for obtaining 1ND and Q 1ND , and a unit sine wave signal ▲ e * 1d2 ▼ and a 90 ° phase which operates based on the phase angle signal ▲ θ * 1d1 ▼ and whose phase angle changes by ▲ 2θ * 1d ▼ means for obtaining a unit sine wave signal e * 1q2 ▼ delayed, the signal ▲ e * 1d2 ▼, ▲ e * 1q2 ▼ and P 1NA, Q based on the Q 1NA 1PD = ▲ e * 1d2 ▼ · Q 1NA -▲ e * 1q2 ▼ Means for obtaining the signal Q 1PD by calculating P 1NA , and the first and second phases of N-phase polyphase alternating current by performing the calculation using the signals Q 1PD , P 1ND and Q 1ND as input signals A means for creating an N-th phase current command, 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▲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 signals P 1ND , Q Based on 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 current command signal ▲ I * U ▼, ▲ I * V ▼, ▲ I * W
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 ▲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 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 signals P 1ND , Q Based on 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 current command signal ▲ 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▲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。
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 signals P 1ND , Q Based on 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 And a means for producing current commands ▲ I * U ▼, ▲ I * V ▼, ▲ I * W ▼.
JP60200010A 1985-09-10 1985-09-10 Reactive power compensator Expired - Lifetime JPH0625949B2 (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP60200010A JPH0625949B2 (en) 1985-09-10 1985-09-10 Reactive power compensator
AU62349/86A AU573101B2 (en) 1985-09-10 1986-09-04 Reactive power compensation apparatus
US06/903,957 US4698581A (en) 1985-09-10 1986-09-05 Reactive power compensation apparatus
CA000517797A CA1300222C (en) 1985-09-10 1986-09-09 Reactive power compensation apparatus
EP86112529A EP0214661B1 (en) 1985-09-10 1986-09-10 Reactive power compensation apparatus
DE8686112529T DE3684207D1 (en) 1985-09-10 1986-09-10 BLIND POWER COMPENSATOR.

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60200010A JPH0625949B2 (en) 1985-09-10 1985-09-10 Reactive power compensator

Publications (2)

Publication Number Publication Date
JPS6260013A JPS6260013A (en) 1987-03-16
JPH0625949B2 true JPH0625949B2 (en) 1994-04-06

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Application Number Title Priority Date Filing Date
JP60200010A Expired - Lifetime JPH0625949B2 (en) 1985-09-10 1985-09-10 Reactive power compensator

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JP (1) JPH0625949B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5991327A (en) * 1995-10-26 1999-11-23 Inverpower Controls Ltd. Smart predictive line controller for AC and DC electric arc furnaces
CN105024389A (en) * 2015-08-07 2015-11-04 国网电力科学研究院武汉南瑞有限责任公司 Three-phase equilibrium based reactive compensation method for submerged arc furnace

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