JPH0732538B2 - Three-phase circuit harmonic current detection method - Google Patents
Three-phase circuit harmonic current detection methodInfo
- Publication number
- JPH0732538B2 JPH0732538B2 JP60169203A JP16920385A JPH0732538B2 JP H0732538 B2 JPH0732538 B2 JP H0732538B2 JP 60169203 A JP60169203 A JP 60169203A JP 16920385 A JP16920385 A JP 16920385A JP H0732538 B2 JPH0732538 B2 JP H0732538B2
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- 230000010354 integration Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 230000001131 transforming effect Effects 0.000 description 1
Classifications
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- Y—GENERAL 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
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- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
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- Y02E40/40—Arrangements for reducing harmonics
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Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、平衡3相回路の各相の高調波電流を検出す
る3相回路の高調波電流検出方法に関する。Description: TECHNICAL FIELD The present invention relates to a three-phase circuit harmonic current detection method for detecting a harmonic current of each phase of a balanced three-phase circuit.
近年、産業用および家庭用の機器に、半導体整流装置な
どの高調波電流を多量に発生する装置を備えたものが多
く、このため電力会社の配電系統,需要家の所内電力系
統などの系統に高調波電流が増加し、高調波電流による
被害が問題となつている。In recent years, many industrial and household devices are equipped with a device that generates a large amount of harmonic current, such as a semiconductor rectifier device. Harmonic current is increasing and damage due to harmonic current is becoming a problem.
そして従来は、コンデンサとリアクトルあるいは抵抗か
らなる受動形フイルタ装置により、系統の負荷に供給さ
れる各相の相電流の特定の高調波電流を分路し、系統の
高調波電流を低減することが行なわれている。In the past, it was possible to reduce the harmonic current of the system by shunting a specific harmonic current of the phase current of each phase supplied to the load of the system with a passive filter device consisting of a capacitor and a reactor or resistor. Has been done.
しかし、前述の受動形フイルタ装置を用いる場合は、
(I)1台のフイルタ装置によつて複数の次数の高調波
電流の低減が行なえない,(II)フイルタ装置によつて
系統の周波数特性が変化する,(III)高調波電流が増
加するとフイルタ装置が過負荷になるなどの種々の不都
合がある。However, when using the passive filter device described above,
(I) The harmonic currents of a plurality of orders cannot be reduced by one filter device, (II) the frequency characteristic of the system is changed by the filter device, and (III) the filter current increases when the harmonic current increases. There are various inconveniences such as overloading of the device.
そこでインバータを備えたアクテイブフイルタ装置が考
案され、該アクテイブフイルタ装置は系統から負荷に供
給される角周波数ωoの基本波電流に、前記インバータ
によつて形成された高調波電流を注入し、系統の高調波
電流を低減する。Therefore, an active filter device provided with an inverter is devised, and the active filter device injects a harmonic current formed by the inverter into a fundamental current of an angular frequency ωo supplied from a system to a load, Reduce harmonic currents.
そしてアクテイブフイルタ装置の場合は、インバータに
よつて複数の次数の高調波電流を形成でき、また、フイ
ルタ装置が系統から独立しているため、受動形フイルタ
装置を用いた場合の前述の各不都合が解消される。In the case of an active filter device, harmonic currents of a plurality of orders can be formed by the inverter, and since the filter device is independent of the system, each of the inconveniences described above when using the passive filter device is eliminated. Will be resolved.
ところで前述のアクテイブフイルタ装置などにおいて
は、各相の高調波電流を正確に検出する必要がある。By the way, in the above-mentioned active filter device or the like, it is necessary to accurately detect the harmonic current of each phase.
一方、帯域除去フイルタ(ノッチフイルタ)は、一般
に、2次伝達関数 (ωxは除去する帯域の角周波数,Qは共振のするどさ,S
は複素変数)のフイルタであり、前記伝達関数を変形し
て得られる の式からも明らかなように、入力信号から角周波数ωx
の帯域の信号を減算除去して出力する。On the other hand, the band elimination filter (notch filter) is generally a quadratic transfer function. (Ωx is the angular frequency of the band to be removed, Q is the resonance frequency, S
Is a complex variable filter and is obtained by transforming the transfer function As is clear from the equation, the angular frequency ωx from the input signal
The signal in the band is removed by subtraction and output.
そして各相の基本波電流の角周波数がωoの一定周波数
であるため、各相の高調波電流の検出に、前記帯域除去
フイルタを用いることが考えられる。Since the angular frequency of the fundamental wave current of each phase is a constant frequency of ωo, it can be considered to use the band elimination filter for detecting the harmonic current of each phase.
ところで帯域除去フイルタは、産報出版株式会社の電子
科学シリーズ「アクテイブフイルタの設計」(1973年
12月10日初版発行)などに記載されているように、状態
変数形フイルタ回路を用いてたとえば第4図に示すよう
に構成される。By the way, the band elimination filter is the electronic science series “Designing an active filter” by Koho Publishing Co., Ltd. (1973
As described in, for example, the first edition issued on December 10, the state variable filter circuit is used, as shown in FIG. 4, for example.
そして第4図において(1)はフイルタ入力端子、
(2)は入力端子(1)の入力信号と後述の第2積分器
の出力信号とを加算する第1加算器、(3)は加算器
(2)の出力信号が入力される第1積分器、(4)は積
分器(3)の出力信号を1/Q(Qは共振のするどさ)に
低減して積分器(3)の入力側に帰還する定数回路、
(5)は積分器(3)の出力信号を積分して加算器
(2)に出力する第2積分器、(6)は加算器(2),
積分器(3),(5)および定数回路(4)が形成する
状態変数形フイルタ回路であり、定数回路(4)の出力
信号がフイルタ回路(6)の出力信号を形成する。And in FIG. 4, (1) is a filter input terminal,
(2) is a first adder that adds an input signal of the input terminal (1) and an output signal of a second integrator described later, and (3) is a first integration into which the output signal of the adder (2) is input. And (4) is a constant circuit that reduces the output signal of the integrator (3) to 1 / Q (Q is the resonance speed) and feeds it back to the input side of the integrator (3).
(5) is a second integrator that integrates the output signal of the integrator (3) and outputs it to the adder (2), (6) is the adder (2),
It is a state variable type filter circuit formed by the integrators (3), (5) and the constant circuit (4), and the output signal of the constant circuit (4) forms the output signal of the filter circuit (6).
(7)は定数回路(4)の出力信号を反転する反転アン
プ、(8)は入力端子(1)の入力信号とアンプ(7)
の出力信号とを加算する第2加算器、(9)は加算器
(8)に接続されたフイルタ出力端子である。(7) is an inverting amplifier that inverts the output signal of the constant circuit (4), and (8) is the input signal of the input terminal (1) and the amplifier (7).
Is a second adder for adding the output signal of the second output signal, and (9) is a filter output terminal connected to the adder (8).
そして入力端子(1)の入力信号が角周波数ωoの基本
波成分と高調波成分とからなる場合、基本波成分を除去
するために、フイルタ回路(6)の加算器(2),積分
器(3),(5)のループの共振角周波数ωxがωoに
設定され、このとき積分器(3)の出力信号が、2次伝
達関数 で設定されたバンドパスフイルタ信号になるとともに、
積分器(5)の出力信号が、2次伝達関数 で設定されたローパスフイルタ信号になる。When the input signal of the input terminal (1) is composed of the fundamental wave component and the harmonic component of the angular frequency ωo, in order to remove the fundamental wave component, the adder (2) and the integrator (2) of the filter circuit (6) The resonance angular frequency ωx of the loops 3) and (5) is set to ωo, and at this time, the output signal of the integrator (3) is the quadratic transfer function. With the bandpass filter signal set in,
The output signal of the integrator (5) is the quadratic transfer function It becomes the low pass filter signal set by.
また、定数回路(4)からアンプ(7)に出力される信
号は、積分器(3)の出力信号を1/Q倍した信号,すな
わち2次伝達関数 で設定された基本波成分の抽出信号になり、このとき定
数回路(4)の出力信号の位相は入力端子(1)の入力
信号の位相に一致する。The signal output from the constant circuit (4) to the amplifier (7) is a signal obtained by multiplying the output signal of the integrator (3) by 1 / Q, that is, a quadratic transfer function. It becomes the extraction signal of the fundamental wave component set in 1. At this time, the phase of the output signal of the constant circuit (4) matches the phase of the input signal of the input terminal (1).
さらに、アンプ(7)によつて定数回路(4)の出力信
号が反転され、アンプ(7)から加算器(8)に、定数
回路(4)の出力信号の符号反転信号が出力されるとと
もに、加算器(8)によつて符号反転信号と入力端子
(1)の入力信号とが加算され、これにより加算器
(8)から出力端子(9)に出力される信号が、入力端
子(1)の入力信号から基本波成分を減算除去した信
号,すなわち入力信号の高調波成分の信号になり、出力
端子(9)の信号により入力端子(1)の入力信号の高
調波成分が検出される。Further, the amplifier (7) inverts the output signal of the constant circuit (4), and the amplifier (7) outputs the sign inversion signal of the output signal of the constant circuit (4) to the adder (8). , The sign inversion signal and the input signal of the input terminal (1) are added by the adder (8), and the signal output from the adder (8) to the output terminal (9) is the input terminal (1 ) The signal obtained by subtracting and removing the fundamental wave component from the input signal, that is, the signal of the harmonic component of the input signal, and the harmonic component of the input signal of the input terminal (1) is detected by the signal of the output terminal (9). .
そして第4図の帯域除去フイルタを各相の高調波電流の
検出に用いる場合は、帯域除去フイルタを各相毎に設
け、各帯域除去フイルタの入力端子(1)に、各相の相
電流を、たとえば電流変成器などによつて検出して形成
された信号,すなわち各相の相電流それぞれの波形の相
電流検出信号を入力すればよい。When the band elimination filter of FIG. 4 is used to detect the harmonic current of each phase, a band elimination filter is provided for each phase, and the phase current of each phase is applied to the input terminal (1) of each band elimination filter. It suffices to input, for example, a signal formed by detection by a current transformer or the like, that is, a phase current detection signal of each waveform of the phase current of each phase.
ところで第4図の帯域除去フイルタの場合は、Q値の
大,小によつて過渡特性および定常特性が変化し、Q値
を1,5それぞれに設定して入力端子(1)に120°通電の
方形波信号を入力した場合は、過渡期にアンプ(7),
積分器(5)の出力信号が第5図,第6図それぞれに示
すようになる。なお、第5図(a),(b),(c)は
Q値が1に設定された場合の入力端子(1)の方形波信
号,アンプ(7),積分器(5)の出力信号を示し、第
6図(a),(b)(c)はQ値が5に設定された場合
の方形波信号,アンプ(7),積分器(5)の出力信号
を示す。By the way, in the case of the band elimination filter shown in Fig. 4, the transient characteristics and steady-state characteristics change depending on the Q value, and the Q value is set to 1 and 5, respectively, and the input terminal (1) is energized at 120 °. When the square wave signal of is input, the amplifier (7),
The output signal of the integrator (5) is as shown in FIGS. 5 and 6, respectively. 5 (a), (b), and (c) show the square wave signal of the input terminal (1), the output signal of the amplifier (7), and the integrator (5) when the Q value is set to 1. 6 (a), (b) and (c) show the square wave signal, the output signal of the amplifier (7) and the integrator (5) when the Q value is set to 5.
一方、定常時はアンプ(7),積分回路(5)の出力信
号が第7図,第8図それぞれに示すようになる。なお、
第7図(a),(b),(c)はQ値が1に設定された
場合の入力端子(1)の方形波信号,アンプ(7),積
分器(5)の出力信号を示し、第8図(a),(b),
(c)はQ値が5に設定された場合の方形波信号,アン
プ(7),積分器(5)の出力信号を示す。On the other hand, in the steady state, the output signals of the amplifier (7) and the integrating circuit (5) are as shown in FIGS. 7 and 8, respectively. In addition,
7 (a), (b) and (c) show the square wave signal of the input terminal (1), the output signal of the amplifier (7) and the integrator (5) when the Q value is set to 1. , FIG. 8 (a), (b),
(C) shows the square wave signal when the Q value is set to 5, the output signal of the amplifier (7) and the integrator (5).
そして第5図(b),第6図(b)の比較からも明らか
なように、Q値を大きくすれば過渡応答性が劣化する。As is clear from the comparison between FIG. 5 (b) and FIG. 6 (b), the transient response is deteriorated when the Q value is increased.
また、第7図(b),第8図(b)の比較からも明らか
なように、Q値を小さくすれば定常時の基本波成分の除
去率が低下して波形歪みが生じる。Further, as is clear from the comparison between FIG. 7 (b) and FIG. 8 (b), if the Q value is made smaller, the removal rate of the fundamental wave component in the steady state is lowered and waveform distortion occurs.
すなわち、第4図の帯域除去フイルタでは、応答速度を
早くするためにQ値を小さくすれば定常時に波形歪みが
生じ、逆に定常時の波形歪みを低減するためにQ値を大
きくすれば応答速度が遅くなり、過渡応答特性および基
本波成分の除去特性を共に良好にすることが困難にな
る。That is, in the band elimination filter shown in FIG. 4, if the Q value is made small in order to increase the response speed, waveform distortion occurs in the steady state, and conversely, if the Q value is made large in order to reduce the waveform distortion in the steady state, the response is made. The speed becomes slow, and it becomes difficult to improve both transient response characteristics and fundamental wave component removal characteristics.
したがつて、第4図の帯域除去フイルタを各相の高調波
電流の検出に用いた場合は、過渡応答特性および基本波
電流の除去特性のいずれか一方が劣化し、良好な検出が
行なえなくなる問題点がある。Therefore, when the band elimination filter of FIG. 4 is used to detect the harmonic current of each phase, either transient response characteristic or fundamental current elimination characteristic deteriorates, and good detection cannot be performed. There is a problem.
そしてこの発明は、とくに3相の平衡負荷の場合,すな
わち平衡3相回路の場合に、過渡応答特性および基本波
電流の除去特性を共に良好にし、迅速かつ波形歪みを少
なくして各相の高調波電流を検出することを技術的課題
とする。The present invention makes both transient response characteristics and fundamental current removal characteristics good, particularly in the case of a three-phase balanced load, that is, a balanced three-phase circuit, to quickly and reduce waveform distortion to improve harmonics of each phase. The technical problem is to detect the wave current.
この発明は、平衡3相回路の各相の相電流それぞれの波
形の相電流検出信号を、2次伝達関数 (ωoは基本波電流の角周波数,Qは共振のするどさ,Sは
複素変数)のフイルタ回路によりそれぞれ処理し、前記
伝達関数によつて設定された各相のローパスフイルタ信
号を得るとともに、各2相の前記ローパスフイルタ信号
の減算合成により各相の前記基本波電流それぞれの波形
の基本波電流検出信号を形成し、かつ各相の前記相電流
検出信号から各相それぞれの前記基本波電流検出信号を
減算して各相の高調波電流を検出することを特徴とする
3相回路の高調波電流検出方法である。According to the present invention, a phase current detection signal having a waveform of each phase current of each phase of a balanced three-phase circuit is converted into a secondary transfer function. (Ωo is the angular frequency of the fundamental wave current, Q is the resonance frequency, S is a complex variable), and low-pass filter signals of each phase set by the transfer function are obtained, A fundamental wave current detection signal of each waveform of the fundamental wave current of each phase is formed by subtractive synthesis of the low-pass filter signals of each two phases, and the fundamental wave current of each phase is formed from the phase current detection signal of each phase. A method for detecting a harmonic current of a three-phase circuit, which is characterized by detecting a harmonic current of each phase by subtracting a detection signal.
そして2次伝達関数 のフイルタ回路は、たとえば第4図のフイルタ回路
(6)の積分器(5)の出力信号を用いることによつて
形成され、この場合積分器(5)の出力信号が積分器
(3)の出力信号より位相が90°進んだ信号になるた
め、各フイルタ回路のローパスフイルタ信号は、各相の
基本波電流の位相を90°進めた波形の信号になる。And the quadratic transfer function Is formed by using, for example, the output signal of the integrator (5) of the filter circuit (6) of FIG. 4, in which case the output signal of the integrator (5) is of the integrator (3). Since the output signal has a phase advanced by 90 °, the low-pass filter signal of each filter circuit has a waveform obtained by advancing the phase of the fundamental current of each phase by 90 °.
また、第5図(c)および第7図(c)の波形からも明
らかなように、積分器(5)の出力信号は、Q値を小さ
くして過渡応答速度を速くしても、定常時の波形歪みが
少なく、基本波電流にしたがつて忠実に変化する。Further, as is clear from the waveforms of FIG. 5 (c) and FIG. 7 (c), the output signal of the integrator (5) remains constant even if the Q value is made small to increase the transient response speed. There is little waveform distortion at all times, and it changes faithfully according to the fundamental wave current.
一方、平衡3相回路の場合は、負荷に供給される3相の
相電流が120°ずつ位相のずれた電流になる。On the other hand, in the case of a balanced three-phase circuit, the phase currents of the three phases supplied to the load are 120 ° out of phase.
したがつて、各2相のローパスフイルタ信号を減算合成
して形成された信号が、各2相の基本波電流の位相を90
°進めた信号のベクトル合成信号,すなわち各相それぞ
れの基本波電流の波形の基本波電流検出信号になり、こ
の場合各フイルタ回路のQ値を小さくすることにより、
各相の基本波電流が過渡応答速度を速くして波形歪みな
く検出され、これにより各相の高調波電流が、過渡応答
特性および基本波電流の除去特性を共に良好にして検出
される。Therefore, the signal formed by subtracting and combining the low-pass filter signals of each two-phase has the phase of the fundamental current of each two-phase of 90.
° It becomes a vector composite signal of the advanced signal, that is, the fundamental current detection signal of the waveform of the fundamental current of each phase. In this case, by reducing the Q value of each filter circuit,
The fundamental wave current of each phase is detected with high transient response speed and without waveform distortion, whereby the harmonic current of each phase is detected with good transient response characteristics and fundamental wave current removal characteristics.
つぎに、この発明を、その1実施例を示した第1図ない
し第3図とともに詳細に説明する。Next, the present invention will be described in detail with reference to FIGS. 1 to 3 showing one embodiment thereof.
いま、平衡3相回路の負荷が高調波電流の発生源負荷を
形成しているとすれば、発生源負荷に供給される3相の
相電流は、位相が120°ずつずれるとともに、系統の基
本波電流に高調波電流が重畳した電流になる。Now, assuming that the load of the balanced three-phase circuit forms the source load of the harmonic current, the phase currents of the three phases supplied to the source load are 120 ° out of phase and The harmonic current is superimposed on the wave current.
そして各相の高調波電流を検出するために、まず、各相
の相電流を変流器によつてそれぞれ検出し、各相の相電
流それぞれの波形の相電流検出信号を形成する。Then, in order to detect the harmonic current of each phase, first, the phase current of each phase is detected by a current transformer to form a phase current detection signal of each waveform of the phase current of each phase.
つぎに、各相電流検出信号を、第1図(a),(b),
(c)に示すように、相電流検出信号入力端子(10
a),(10b),(10c)を介して各フイルタ回路(11
a),(11b),(11c)をそれぞれに入力する。Next, the current detection signals for each phase are shown in FIG. 1 (a), (b),
As shown in (c), the phase current detection signal input terminal (10
a), (10b), (10c) through each filter circuit (11
Input a), (11b), and (11c) respectively.
ところで各フイルタ回路(11a)〜(11c)は、第4図の
状態変数形フイルタ回路(6)と同一に形成され、図中
の(12a),(12b),(12c)は加算器(2)に相当す
る第3加算器、(13a),(13b),(13c)は積分器
(3)に相当する第3積分器、(14a),(14b),(14
c)は定数回路(4)に相当する1/Qの定数回路、(15
a),(15b),(15c)は積分器(5)に相当する第4
積分器である。By the way, each of the filter circuits (11a) to (11c) is formed in the same manner as the state variable type filter circuit (6) of FIG. 4, and (12a), (12b) and (12c) in the figure are adders (2 ) Corresponding to the third adder, (13a), (13b) and (13c) corresponding to the third integrator corresponding to the integrator (3), (14a), (14b) and (14).
c) is a 1 / Q constant circuit corresponding to the constant circuit (4), (15
a), (15b), (15c) are the fourth equivalent to the integrator (5)
It is an integrator.
なお、各フイルタ回路(11a)〜(11c)がフイルタ回路
(6)と異なる点は、積分器(15a)〜(15c)それぞれ
の出力信号,すなわちローパスフイルタ信号を、各フイ
ルタ回路(11a)〜(11c)の出力信号とした点である。Note that the filter circuits (11a) to (11c) differ from the filter circuit (6) in that the output signals of the integrators (15a) to (15c), that is, the low-pass filter signals are transferred to the filter circuits (11a) to (11a). (11c) is the output signal.
そして各フイルタ回路(11a)〜(11c)の加算器(12
a)〜(12c),積分器(13a)〜(13c),(15a)〜(1
5c)のループが各相の基本波電流の角周波数ωoに共振
し、このとき積分器(13a)〜(13c)から出力されるバ
ンドパスフイルタ信号が、2次伝達関数 によつて設定された信号になり、積分器(15a)〜(15
c)によつて積分器(13a)〜(13c)のバンドパスフイ
ルタ信号がさらに積分されるため、積分器(15a)〜(1
5c)のローパスフイルタ信号は、2次伝達関数 で設定される信号になる。The adder (12) of each of the filter circuits (11a) to (11c)
a) to (12c), integrators (13a) to (13c), (15a) to (1
The loop of 5c) resonates at the angular frequency ωo of the fundamental wave current of each phase, and at this time, the bandpass filter signals output from the integrators (13a) to (13c) are quadratic transfer functions. The signal is set by the integrator (15a) ~ (15a
c) further integrates the band pass filter signals of the integrators (13a) to (13c), so that the integrators (15a) to (1
The low-pass filter signal in 5c) is a quadratic transfer function It becomes the signal set by.
ところで第5図(c)および第7図(c)からも明らか
なように、積分器(15a)〜(15c)のローパスフイルタ
信号は、Q値を小さくして過渡応答速度を速くしても、
定常時に波形歪みが少なく、各相の基本波電流に忠実な
波形の信号になる。By the way, as is apparent from FIGS. 5 (c) and 7 (c), the low-pass filter signals of the integrators (15a) to (15c) can be obtained even if the Q value is reduced and the transient response speed is increased. ,
There is little waveform distortion in the steady state, and the signal has a waveform that is faithful to the fundamental current of each phase.
一方、積分器(13a)〜(13c)のバンドパスフイルタ信
号の位相が各相の基本波電流の位相に一致するため、積
分器(15a)〜(15c)のローパスフイルタ信号は、各相
の基本波電流の位相をそれぞれ90°進めた波形の信号に
なる。On the other hand, since the phase of the bandpass filter signals of the integrators (13a) to (13c) matches the phase of the fundamental wave current of each phase, the lowpass filter signals of the integrators (15a) to (15c) are The signal has a waveform that advances the phase of the fundamental current by 90 °.
また、各相の基本波電流の位相が120°ずつずれている
ため、積分器(15a)〜(15c)のローパスフイルタ信号
も、位相が120°ずつずれた信号になる。Further, since the phases of the fundamental wave currents of the respective phases are shifted by 120 °, the low-pass filter signals of the integrators (15a) to (15c) are also signals whose phases are shifted by 120 °.
したがつて、各相の相電流a,b,cおよびローパス
フイルタ信号a′,b′,c′のベクトル関係
は、第2図に示すようになる。Therefore, the vector relationship between the phase currents a, b, c of each phase and the low-pass filter signals a ', b', c'is as shown in FIG.
そしてたとえば、2相のローパスフイルタ信号b′,
c′を減算合成すると、その成分c′−b′は第
2図の破線矢印に示すように相電流aと同相になり、
相電流a中の基本波電流の波形の基本波電流検出信号
が得られる。Then, for example, a two-phase low-pass filter signal b ′,
When c'is subtractively combined, its component c'-b 'becomes in phase with the phase current a as shown by the broken line arrow in FIG.
A fundamental wave current detection signal having the waveform of the fundamental wave current in the phase current a is obtained.
同様に、2相のローパスフイルタ信号c′,a′,
を減算合成すると、相電流b中の基本波電流の波形の
基本波電流検出信号が得られ、2相のローパスフイルタ
信号a′,b′を減算合成すると、相電流c中の
基本波電流の波形の基本波電流検出信号が得られる。Similarly, two-phase low-pass filter signals c ′, a ′,
Is obtained by subtraction synthesis, a fundamental current detection signal of the waveform of the fundamental current in the phase current b is obtained, and by subtraction synthesis of the two-phase low-pass filter signals a ′ and b ′, A fundamental current detection signal having a waveform is obtained.
なお、減算合成のみを行なうと、 のレベルで基本波電流が検出されるため、実際には、減
算合成によつて得られた信号を に低減して各相の基本波電流検出信号を形成する。If only subtractive synthesis is performed, Since the fundamental current is detected at the level of, the signal obtained by subtractive synthesis is actually To form a fundamental current detection signal for each phase.
そして前述の減算合成によつて得られた各相の基本波電
流検出信号を、入力端子(10a)〜(10c)それぞれの相
電流検出信号から減算すれば、各相の高調波電流が検出
できるため、各相毎に第3図に示す演算回路(16)を設
ける。Then, the harmonic current of each phase can be detected by subtracting the fundamental wave current detection signal of each phase obtained by the above-mentioned subtractive synthesis from the phase current detection signal of each of the input terminals (10a) to (10c). Therefore, the arithmetic circuit (16) shown in FIG. 3 is provided for each phase.
なお、第3図において、(17)は相電流検出信号の入力
端子、(18),(19)は2相のローパスフイルタ信号そ
れぞれの入力端子、(20)は入力端子(19)のローパス
フイルタ信号の符号を反転するアンプ、(21)は入力端
子(18)のローパスフイルタ信号とアンプ(20)によつ
て符号が反転された入力端子(19)のローパスフイルタ
信号とを加算する加算器、(22)は加算器(21)の出力
信号を に低減する定数回路、(23)は入力端子(17)の相電流
検出信号から定数回路(22)の出力信号を減算する減算
器、(24)は減算器(24)に接続された高調波電流検出
信号出力端子である。In FIG. 3, (17) is the input terminal for the phase current detection signal, (18) and (19) are the input terminals for the two-phase low-pass filter signals, and (20) is the low-pass filter for the input terminal (19). An amplifier that inverts the sign of the signal, (21) is an adder that adds the low-pass filter signal of the input terminal (18) and the low-pass filter signal of the input terminal (19) whose sign is inverted by the amplifier (20), (22) is the output signal of the adder (21) A constant circuit for reducing the constant current, (23) a subtractor for subtracting the output signal of the constant circuit (22) from the phase current detection signal of the input terminal (17), (24) a harmonic connected to the subtractor (24) This is a current detection signal output terminal.
そして演算回路(16)によつて相電流aの高調波電流
を検出する場合は、入力端子(17)に入力端子(10a)
の相電流検出信号を入力するとともに入力端子(18),
(19)にフイルタ回路(11b),(11c)のローパスフイ
ルタ信号をそれぞれ入力し、このときアンプ(20)によ
つてフイルタ回路(11c)のローパスフイルタ信号の符
号が反転されるため、加算器(21)が両フイルタ回路
(11b),(11c)のローパスフイルタ信号を減算合成す
る。When the harmonic current of the phase current a is detected by the arithmetic circuit (16), the input terminal (17) is connected to the input terminal (10a).
Input the phase current detection signal of and input terminal (18),
The low-pass filter signals of the filter circuits (11b) and (11c) are input to (19), and at this time, the sign of the low-pass filter signals of the filter circuit (11c) is inverted by the amplifier (20). (21) subtracts and synthesizes the low-pass filter signals of both filter circuits (11b) and (11c).
さらに、加算器(21)の出力信号が定数回路(22)によ
つて に低減されるため、定数回路(22)から減算器(23)に
相電流aの基本波電流検出信号が出力される。Furthermore, the output signal of the adder (21) is fed by the constant circuit (22). As a result, the constant circuit (22) outputs the fundamental wave current detection signal of the phase current a to the subtractor (23).
そして減算器(23)によつて入力端子(17)の変流信号
から定数回路(23)の出力信号が減算されるため、出力
端子(16)に相電流a中の高調波電流の波形の高調波
電流検出信号が出力され、相電流a中の高調波電流が
検出される。Then, since the output signal of the constant circuit (23) is subtracted from the current transformation signal of the input terminal (17) by the subtractor (23), the waveform of the harmonic current in the phase current a is output to the output terminal (16). The harmonic current detection signal is output, and the harmonic current in the phase current a is detected.
なお、残りの相電流b,cそれぞれの高調波電流も、
前述と同様にしてそれぞれ検出される。The harmonic currents of the remaining phase currents b and c are also
Each is detected in the same manner as described above.
そしてフイルタ回路(11a)〜(11c)のQ値を小さく設
定し、過渡応答速度を速くしても、定常時に波形歪みの
少ない各相の基本波電流が検出されるため、Q値を小さ
く設定することにより、良好な過渡応答特性で各相の相
電流それぞれからほぼ完全に基本波電流が除去され、過
渡応答特性および基本波電流の除去特性を共に良好にし
て高調波電流が検出され、たとえばアクティブフイルタ
装置に適用すると、インバータによつて各相の高調波電
流が忠実に形成され、高調波電流の良好な低減が行なえ
る。Even if the Q values of the filter circuits (11a) to (11c) are set small and the transient response speed is increased, the fundamental wave current of each phase with less waveform distortion is detected in the steady state, so the Q value is set small. By doing so, the fundamental current is removed almost completely from each phase current of each phase with good transient response characteristics, both transient response characteristics and fundamental current removal characteristics are improved, and harmonic currents are detected. When applied to an active filter device, a harmonic current of each phase is faithfully formed by the inverter, and the harmonic current can be satisfactorily reduced.
なお、各フイルタ回路(11a)〜(11c)は、たとえば定
数回路(14a)〜(14c)の出力信号を符号反転して加算
器(12a)〜(12c)それぞれの入力側に帰還するように
構成してもよく、種々の構成のフイルタによつて形成で
きるのは勿論である。Each of the filter circuits (11a) to (11c), for example, inverts the output signals of the constant circuits (14a) to (14c) and feeds them back to the respective input sides of the adders (12a) to (12c). Of course, it may be configured, and it is needless to say that it can be formed by a filter having various configurations.
また、アクティブフイルタ装置だけでなく、高調波電流
の検出装置などの種々の装置に適用できるのも勿論であ
る。Further, it is needless to say that it can be applied not only to the active filter device but also to various devices such as a device for detecting a harmonic current.
以上のように、この発明の3相回路の高調波電流検出方
法によると、各フイルタ回路(11a)〜(11c)のQ値を
小さく設定することにより、過渡応答速度を速くし、か
つ波形歪みを少なくして平衡3相回路の各相の基本波電
流が検出され、過渡応答特性および基本波電流の除去特
性を共に良好にして各相の高調波電流を検出できるもの
である。As described above, according to the harmonic current detection method for a three-phase circuit of the present invention, the transient response speed is increased and the waveform distortion is increased by setting the Q value of each of the filter circuits (11a) to (11c) small. Is reduced to detect the fundamental wave current of each phase of the balanced three-phase circuit, improve both transient response characteristics and fundamental wave current removal characteristics, and detect the harmonic current of each phase.
第1図ないし第3図はこの発明の3相回路の高調波電流
検出方法の1実施例を示し、第1図(a)〜(c)はそ
れぞれフイルタ回路のブロック図、第2図は各相の相電
流と各相のローパスフイルタ信号のベクトル図、第3図
は演算回路のブロック図、第4図は従来の帯域除去フイ
ルタのブロック図、第5図(a)〜(c),第6図
(a)〜(c)はQ値を1,5それぞれに設定したときの
第4図の過渡特性説明用の波形図、第7図(a)〜
(c),第8図(a)〜(c)はQ値を1,5それぞれに
設定したときの第4図の定常特性説明用の波形図であ
る。 (11a),(11b),(11c)……フイルタ回路、(16)
……演算回路。1 to 3 show an embodiment of a method for detecting harmonic currents of a three-phase circuit according to the present invention. FIGS. 1 (a) to 1 (c) are block diagrams of a filter circuit, and FIG. Phase current of each phase and vector diagram of low-pass filter signal of each phase, FIG. 3 is a block diagram of an arithmetic circuit, FIG. 4 is a block diagram of a conventional band elimination filter, and FIGS. 5 (a) to 5 (c), 6 (a) to 6 (c) are waveform diagrams for explaining the transient characteristics of FIG. 4 when the Q value is set to 1, 5 respectively, and FIG. 7 (a) to
(C) and FIGS. 8 (a) to 8 (c) are waveform diagrams for explaining the steady-state characteristics of FIG. 4 when the Q value is set to 1,5, respectively. (11a), (11b), (11c) ... Filter circuit, (16)
…… Arithmetic circuit.
Claims (1)
形の相電流検出信号を、2次伝達関数 (ωoは基本波電流の角周波数,Qは共振のするどさ,Sは
複素変数)のフイルタ回路によりそれぞれ処理し、前記
伝達関数によつて設定された各相のローパスフイルタ信
号を得るとともに、各2相の前記ローパスフイルタ信号
の減算合成により各相の前記基本波電流それぞれの波形
の基本波電流検出信号を形成し、かつ各相の前記相電流
検出信号から各相それぞれの前記基本波電流検出信号を
減算して各相の高調波電流を検出することを特徴とする
3相回路の高調波電流検出方法。1. A phase transfer current detection signal of each phase current of each phase of a balanced three-phase circuit is converted into a quadratic transfer function. (Ωo is the angular frequency of the fundamental wave current, Q is the resonance frequency, S is a complex variable), and low-pass filter signals of each phase set by the transfer function are obtained, A fundamental wave current detection signal of each waveform of the fundamental wave current of each phase is formed by subtractive synthesis of the low-pass filter signals of each two phases, and the fundamental wave current of each phase is formed from the phase current detection signal of each phase. A method for detecting a harmonic current in a three-phase circuit, which comprises detecting a harmonic current of each phase by subtracting a detection signal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60169203A JPH0732538B2 (en) | 1985-07-31 | 1985-07-31 | Three-phase circuit harmonic current detection method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60169203A JPH0732538B2 (en) | 1985-07-31 | 1985-07-31 | Three-phase circuit harmonic current detection method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6231328A JPS6231328A (en) | 1987-02-10 |
| JPH0732538B2 true JPH0732538B2 (en) | 1995-04-10 |
Family
ID=15882114
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60169203A Expired - Lifetime JPH0732538B2 (en) | 1985-07-31 | 1985-07-31 | Three-phase circuit harmonic current detection method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0732538B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0638324B2 (en) * | 1987-06-03 | 1994-05-18 | 日本碍子株式会社 | Vertical array tension insulator device |
| JPH02262848A (en) * | 1989-02-27 | 1990-10-25 | Shinko Electric Co Ltd | Linked power generating system |
-
1985
- 1985-07-31 JP JP60169203A patent/JPH0732538B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6231328A (en) | 1987-02-10 |
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