JPH0732539B2 - Harmonic current detection method - Google Patents
Harmonic current detection methodInfo
- Publication number
- JPH0732539B2 JPH0732539B2 JP60169204A JP16920485A JPH0732539B2 JP H0732539 B2 JPH0732539 B2 JP H0732539B2 JP 60169204 A JP60169204 A JP 60169204A JP 16920485 A JP16920485 A JP 16920485A JP H0732539 B2 JPH0732539 B2 JP H0732539B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- current
- phase
- filter
- current detection
- 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
Links
- 238000001514 detection method Methods 0.000 title claims description 29
- 230000003111 delayed effect Effects 0.000 claims description 3
- 230000001052 transient effect Effects 0.000 description 15
- 230000008030 elimination Effects 0.000 description 11
- 238000003379 elimination reaction Methods 0.000 description 11
- 238000010586 diagram Methods 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 230000003247 decreasing effect Effects 0.000 description 2
- 239000003990 capacitor Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 230000001131 transforming effect Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Classifications
-
- 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
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/40—Arrangements for reducing harmonics
Landscapes
- Measurement Of Current Or Voltage (AREA)
- Supply And Distribution Of Alternating Current (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、負荷に供給される相電流の高周波電流を検
出する高調波電流の検出方法に関する。Description: TECHNICAL FIELD The present invention relates to a harmonic current detection method for detecting a high frequency current of a phase current supplied to a load.
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われている。Conventionally, a passive filter device consisting of a capacitor and a reactor or a resistor is used to shunt a specific harmonic current of the phase current of each phase that is supplied to the load of the system and reduce the harmonic current of the system. It is being appreciated.
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ィブフイルタ装置が考
案され、該アクティ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 wave current of an angular frequency ωo supplied from a system to a load, Reduce harmonic currents.
そしてアクティ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 the active filter device, the inverters can form harmonic currents of a plurality of orders, and since the filter device is independent of the system, each of the inconveniences described above when the passive filter device is used occurs. Will be resolved.
ところで前述のアクティブフイルタ装置などにおいて
は、負荷に供給される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 supplied to the load.
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それぞれ一定であ
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 constant, it is conceivable 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「アクティブフイルタの設計」(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2図に示すよう
に構成される。By the way, the band elimination filter is the electronic science series “Design of Active Filter” by Sangpo Publishing Co., Ltd. (1973
As described in, for example, the first edition issued on December 10, the state variable filter circuit is used, for example, as shown in FIG.
そして第2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. 2, (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)の変流信号とアンプ(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 a current-transformed signal at the input terminal (1) and an 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2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、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. 2 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. A signal formed by being detected by a current transformer, that is, a phase current detection signal having a waveform of each phase current of each phase may be input.
ところで第2図の帯域除去フイルタの場合は、Q値の
大,小によつて過渡応答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3図,第4図それ
ぞれに示すようになる。なお、第3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4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. 2, the transient response characteristic and the steady characteristic vary depending on the Q value.
When the Q value is set to 1, 5 and a square wave signal of 120 ° conduction is input to the input terminal (1), the output signals of the amplifier (7) and integrator (5) are shown in Fig. 3 during the transition period. , As shown in FIG. 4, respectively. In addition, FIG. 3 (a), (b),
(C) shows 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, and FIGS. 4 (a) and 4 (b). , (C) are square wave signals when the Q value is set to 5, amplifier (7), integrator (5)
The output signal of is shown.
一方、定常時は、アンプ(7),積分回路(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。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. 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.
そして第3図(b),第4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. 3 (b) and FIG. 4 (b), increasing the Q value deteriorates the transient response.
また、第5図(b),第6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. 5 (b) and FIG. 6 (b), when the Q value is reduced, the removal rate of the fundamental wave component in the steady state is lowered and waveform distortion occurs.
すなわち、第2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. 2, if the Q value is reduced to increase the response speed, waveform distortion occurs in the steady state, and conversely, if the Q value is increased to reduce the waveform distortion in the steady state, the response is increased. 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2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
行えなくなる問題点がある。Therefore, when the band elimination filter shown in FIG. 2 is used to detect the harmonic current of each phase, either the transient response characteristic or the fundamental current elimination characteristic deteriorates, and good detection cannot be performed. There is a problem.
そしてこの発明は、単相あるいは多相の負荷に供給され
る相電流の高調波電流を、良好な過渡応答特性および基
本波電流の除去特性で迅速かつ波形歪みを少なくして検
出することを技術的課題とする。The present invention provides a technique for detecting a harmonic current of a phase current supplied to a single-phase or multi-phase load quickly, with good transient response characteristics and fundamental wave current removal characteristics, with reduced waveform distortion. Subject.
この発明は、負荷に供給される相電流の波形の相電流検
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処理し、前記伝達関数
によつて設定されたローパスフイルタ信号を得るととも
に、該ローパスフイルタ信号を90°遅延して前記基本波
電流の波形の基本波電流検出信号を形成し、かつ前記相
電流検出信号から前記基本波電流検出信号を減算して高
調波電流を検出することを特徴とする高調波電流の検出
方法である。According to the present invention, a phase current detection signal having a waveform of a phase current supplied to a load 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 a low-pass filter signal set by the transfer function is obtained, and the low-pass filter signal is obtained. Is delayed by 90 ° to form a fundamental current detection signal of the waveform of the fundamental current, and the harmonic current is detected by subtracting the fundamental current detection signal from the phase current detection signal. This is a method of detecting harmonic current.
そして2次伝達関数 のフイルタ回路は、たとえば第2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、フイルタ回路のローパスフイルタ信号は、相電流中
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. 2, in which case the output signal of the integrator (5) is of the integrator (3). Since the phase of the output signal is advanced by 90 °, the low-pass filter signal of the filter circuit is a signal of which the phase of the fundamental current in the phase current is advanced by 90 °.
また、第3図(c)および第5図(c)の波形からも明
らかなように、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 FIGS. 3 (c) and 5 (c), the low-pass filter signal has little waveform distortion in the steady state even if the Q value is made small and the transient response speed is made fast. It changes faithfully according to the fundamental wave current.
したがつてローパスフイルタ信号を90°遅延して得られ
た基本波電流検出信号が、基本波電流と同一位相かつ同
一波形の信号になり、相電流検出信号から基本波電流を
減算することにより相電流中の高調波電流が検出され
る。Therefore, the fundamental current detection signal obtained by delaying the low-pass filter signal by 90 ° becomes a signal with the same phase and waveform as the fundamental current, and the fundamental current is subtracted from the phase current detection signal to obtain the phase current. The harmonic current in the current is detected.
そしてフイルタ回路のQ値を小さくすることにより、基
本波電流が過渡応答速度を速くして低波形歪みで検出さ
れ、これにより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。By reducing the Q value of the filter circuit, the fundamental current increases the transient response speed and is detected with low waveform distortion, which makes the harmonic current improve both the transient response characteristics and the fundamental current removal characteristics. Detected.
つぎに、この発明を、その1実施例を示した第1図とと
もに詳細に説明する。Next, the present invention will be described in detail with reference to FIG. 1 showing one embodiment thereof.
第1図において、(10)は相電流検出信号が入力される
フイルタ入力端子、(11)は第2図の状態変数形フイル
タ回路(6)と同一に構成されたフイルタ回路、
(7),(8),(9),(10)は第2図の加算器
(2),積分器(3),定数回路(4),積分器(5)
に相当する第3加算器,第3積分器,1/Qの定数回路,第
4積分器である。In FIG. 1, (10) is a filter input terminal to which a phase current detection signal is input, (11) is a filter circuit configured the same as the state variable filter circuit (6) of FIG. 2,
(7), (8), (9) and (10) are the adder (2), integrator (3), constant circuit (4) and integrator (5) of FIG.
Corresponding to the third adder, the third integrator, the 1 / Q constant circuit, and the fourth integrator.
そしてフイルタ回路(11)がフイルタ回路(6)と異な
る点は、積分器(10)の出力信号,すなわちローパスフ
イルタ信号をフイルタ回路(11)の出力信号とした点で
ある。The filter circuit (11) is different from the filter circuit (6) in that the output signal of the integrator (10), that is, the low-pass filter signal is used as the output signal of the filter circuit (11).
また、(12)は積分器(10)のローパスフイルタ信号の
位相を90°遅延して出力する遅延素子であり、BBD(バ
ケットプリガードデバイス)などにより形成されてい
る。Further, (12) is a delay element for delaying the phase of the low-pass filter signal of the integrator (10) by 90 ° and outputting it, and is formed by a BBD (bucket preguard device) or the like.
(13)は遅延素子(12)の出力信号を符号反転して出力
する反転アンプ、(14)はアンプ(13)の出力信号と入
力端子(1)の相電流検出信号とを加算する第4加算器
である。(15)は加算器(14)に接続されたフイルタ出
力端子である。(13) is an inverting amplifier for inverting and outputting the output signal of the delay element (12), and (14) is a fourth addition circuit for adding the output signal of the amplifier (13) and the phase current detection signal of the input terminal (1). It is an adder. (15) is a filter output terminal connected to the adder (14).
そして負荷に供給される相電流を電流変成器などによつ
て検出して形成された検出信号,すなわち相電流の波形
の相電流検出信号が入力端子(1)に入力される。Then, a detection signal formed by detecting the phase current supplied to the load by a current transformer or the like, that is, a phase current detection signal having a waveform of the phase current is input to the input terminal (1).
ところで相電流に含まれた基本波電流の角周波数がωo
であれば、フイルタ回路(11)はフイルタ回路(6)と
同様に、加算器(7),積分器(8),(10)のループ
が基本波電流の角周波数ωoに共振し、このとき積分器
(8)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(10)によつて
積分器(8)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(8)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。By the way, the angular frequency of the fundamental current included in the phase current is ωo
If so, the loop of the adder (7), the integrators (8), and (10) of the filter circuit (11) resonates at the angular frequency ωo of the fundamental current, as in the filter circuit (6). The bandpass filter signal output from the integrator (8) is a quadratic transfer function. Since the bandpass filter signal of the integrator (8) is further integrated by the integrator (10), the lowpass filter signal of the integrator (8) becomes 2
Transfer function It becomes the signal set by.
ところで第3図(c)および第5図(c)からも明らか
なように、積分器(10)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、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. 3 (c) and 5 (c), the low-pass filter signal of the integrator (10) is Q
Even if the value is made small and the transient response speed is made fast, there is little waveform distortion in the steady state, and the signal has a waveform faithful to the fundamental current.
一方、積分器(8)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(10)
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 signal of the integrator (8) matches the phase of the fundamental wave current of each phase, the integrator (10)
The low-pass filter signal of is a signal having a waveform obtained by advancing the phase of the fundamental current of each phase by 90 °.
すなわち、積分器(10)のローパスフイルタ信号は、入
力端子(1)の相電流検出信号の基本波電流成分の90°
位相が進んだ信号になる。That is, the low-pass filter signal of the integrator (10) is 90 ° of the fundamental wave current component of the phase current detection signal of the input terminal (1).
The signal has advanced phase.
そして積分器(10)のローパスフイルタ信号の位相が遅
延素子(12)によつて90°遅延されるため、遅延素子
(12)の出力信号は、相電流検出信号の基本波電流成分
の信号,すなわち基本波電流と同一波形かつ同一位相の
基本波電流検出信号になる。Since the phase of the low-pass filter signal of the integrator (10) is delayed by 90 ° by the delay element (12), the output signal of the delay element (12) is the signal of the fundamental wave current component of the phase current detection signal, That is, the fundamental wave current detection signal has the same waveform and the same phase as the fundamental wave current.
さらに、アンプ(13)によつて基本波電流検出信号の符
号が反転されるとともに、加算器(14)によりアンプ
(13)の出力信号と入力端子(1)の相電流検出信号と
が加算されるため、加算器(14)から出力端子(15)に
は、入力端子(1)の相電流検出信号から遅延素子(1
2)の基本波電流検出信号を減算した信号,すなわち高
調波電流の波形の高調波電流検出信号が出力され、出力
端子(15)の高調波電流検出信号によつて高調波電流が
検出される。Further, the sign of the fundamental wave current detection signal is inverted by the amplifier (13), and the output signal of the amplifier (13) and the phase current detection signal of the input terminal (1) are added by the adder (14). Therefore, from the adder (14) to the output terminal (15), the delay element (1
A signal obtained by subtracting the fundamental wave current detection signal of 2), that is, a harmonic current detection signal of the waveform of the harmonic current is output, and the harmonic current is detected by the harmonic current detection signal of the output terminal (15). .
そしてフイルタ回路(11)のQ値を小さくして過渡応答
速度を速くしても、定常時にローパスフイルタ信号に波
形歪みなどが生じないため、Q値を小さくすることによ
り、良好な過渡応答特性で波形歪みを少なくして基本波
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 value of the filter circuit (11) is decreased to increase the transient response speed, the low-pass filter signal will not be distorted in a steady state. Therefore, by decreasing the Q value, good transient response characteristics can be obtained. The harmonic current is detected by reducing the waveform distortion, the transient response characteristic and the fundamental current removal characteristic are both improved, and the harmonic current is detected. For example, when applied to an active filter device, the harmonic current is detected by the inverter. Is faithfully formed, and the harmonic current can be satisfactorily reduced.
ところで自相の相電流のみを用いて自相の高調波電流が
検出されるため、負荷が単相あるいは多相の平衡負荷,
不平衡負荷であつても、各相毎に第1図のブロックを設
けることにより、各相の高調波電流がそれぞれ検出され
る。By the way, since the self-phase harmonic current is detected using only the self-phase current, the load is a single-phase or multi-phase balanced load,
Even with an unbalanced load, the harmonic current of each phase is detected by providing the block of FIG. 1 for each phase.
なお、フイルタ回路(11)は、たとえば定数回路(9)
の出力信号を符号反転して加算器(7)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。The filter circuit (11) is, for example, a constant circuit (9).
The output signal may be inverted in sign and fed back to the input side of the adder (7), and it goes without saying 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、この発明の高調波電流の検出方法による
と、フイルタ回路(11)のQ値を小さく設定し、良好な
過渡応答特性で波形歪みを少なくして自相の相電流検出
信号から自相の基本波電流が検出できるため、負荷の種
類にかかわらず、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を検出することができ
るものである。As described above, according to the harmonic current detection method of the present invention, the Q value of the filter circuit (11) is set to a small value, the waveform distortion is reduced with good transient response characteristics, and the phase current detection signal of its own phase is detected. Since the fundamental wave current of its own phase can be detected, it is possible to detect the harmonic current by improving both the transient response characteristic and the fundamental wave current removal characteristic regardless of the type of load.
第1図はこの発明の高調波電流の検出方法の1実施例の
ブロック図、第2図は従来の帯域除去フイルタのブロッ
ク図、第3図(a)〜(c),第4図(a)〜(c)は
Q値を1,5それぞれに設定したときの第2図の過渡応答
特性説明用の波形図、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2図の定常特性説明用の波形図である。 (11)……フイルタ回路、(12)……遅延素子、(13)
……反転アンプ、(14)……加算器。FIG. 1 is a block diagram of one embodiment of a method for detecting a harmonic current according to the present invention, FIG. 2 is a block diagram of a conventional band elimination filter, and FIGS. 3 (a)-(c) and 4 (a). ) To (c) are waveform diagrams for explaining the transient response characteristic of FIG. 2 when the Q value is set to 1, 5 respectively, FIG. 5 (a) to (c), and FIG. 6 (a) to ( 3C is a waveform diagram for explaining the steady-state characteristic of FIG. 2 when the Q value is set to 1, 5 respectively. (11) …… Filter circuit, (12) …… Delay element, (13)
…… Inverting amplifier, (14) …… Adder.
Claims (1)
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処理し、前記伝達関数
によつて設定されたローパスフイルタ信号を得るととも
に、該ローパスフイルタ信号を90°遅延して前記基本波
電流の波形の基本波電流検出信号を形成し、かつ前記相
電流検出信号から前記基本波電流検出信号を減算して高
調波電流を検出することを特徴とする高調波電流の検出
方法。1. A phase transfer current detection signal having a waveform of a phase current supplied to a load 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 a low-pass filter signal set by the transfer function is obtained, and the low-pass filter signal is obtained. Is delayed by 90 ° to form a fundamental current detection signal of the waveform of the fundamental current, and the harmonic current is detected by subtracting the fundamental current detection signal from the phase current detection signal. Harmonic current detection method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60169204A JPH0732539B2 (en) | 1985-07-31 | 1985-07-31 | Harmonic current detection method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60169204A JPH0732539B2 (en) | 1985-07-31 | 1985-07-31 | Harmonic current detection method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6231329A JPS6231329A (en) | 1987-02-10 |
| JPH0732539B2 true JPH0732539B2 (en) | 1995-04-10 |
Family
ID=15882133
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60169204A Expired - Lifetime JPH0732539B2 (en) | 1985-07-31 | 1985-07-31 | Harmonic current detection method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0732539B2 (en) |
-
1985
- 1985-07-31 JP JP60169204A patent/JPH0732539B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6231329A (en) | 1987-02-10 |
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