JPS62217860A - Control system for voltage-type pwm inverter - Google Patents

Control system for voltage-type pwm inverter

Info

Publication number
JPS62217860A
JPS62217860A JP61059376A JP5937686A JPS62217860A JP S62217860 A JPS62217860 A JP S62217860A JP 61059376 A JP61059376 A JP 61059376A JP 5937686 A JP5937686 A JP 5937686A JP S62217860 A JPS62217860 A JP S62217860A
Authority
JP
Japan
Prior art keywords
signal
phase
reference signal
rom
multiplied
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.)
Pending
Application number
JP61059376A
Other languages
Japanese (ja)
Inventor
Hiroshi Osawa
博 大沢
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP61059376A priority Critical patent/JPS62217860A/en
Publication of JPS62217860A publication Critical patent/JPS62217860A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To easily eliminate higher harmonic, by combining frequency component nfc+ or -mf0 (m, n are natural numbers) generated by switching action, with the signal of opposite phase, when each fundamental frequency of the modulation signal and the reference signal of a PWM inverter is fc, f0. CONSTITUTION:The phase theta0 of desired fundamental wave component and the phase thetac of modulation signal are directed to ROMs 11, 12 for input, and are multiplied 41 by m1 and multiplied 42 by n1 to be added 51 to each other. The phase is directed to a ROM 13 for input to obtain sine wave output. In the meantime, by a ROM 14, a non-linear function with the input of control factor lambda is produced, and higher harmonic DELTAe0 with the added output of the signal and of the ROM 13 multiplied 21 by each other is found out. To the reference signal e0 of a sine wave found out with the output of the ROM 11 and the control factor lambda multiplied 21 by each other, the higher harmonic signal DELTAe0 is added 52, and new reference signal e0 is produced and is compared with the modulation signal ec by a comparator 3. According to e0'>ec or e0'<ec, a switch on the positive side or on the negative side of a PWM inverter is turned ON. As a result, higher harmonic component is easily eliminated or reduced.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、直流電源から単相あるいは多相の交流電圧を
得る電圧形PWMインバータにおいて、出力電圧に含ま
れる特定次数の高調波を低減するための制御方式に関す
る。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention reduces harmonics of a specific order contained in the output voltage in a voltage source PWM inverter that obtains single-phase or multi-phase AC voltage from a DC power supply. Regarding the control method for

〔従来の技術〕[Conventional technology]

電圧形インバータの出力電圧波形は、一般に高調波成分
の少ない正弦波であることが望ましい。
It is generally desirable that the output voltage waveform of a voltage source inverter be a sine wave with few harmonic components.

出力電圧波形を改善する方法としては、例えばパルス幅
変調(以下、PWMとも略記する。)方式が一般的に知
られている。
As a method for improving the output voltage waveform, for example, a pulse width modulation (hereinafter also abbreviated as PWM) method is generally known.

第5図はトランジスタスイッチ(以下、単にスイッチと
呼ぶ。)で構成された3相出力電圧形インバ一タ主回路
を示す回路図である。こ\で、PWM制御を行なうには
、正側電位に接続されたスイッチT、〜TI3と負側電
位に接続されたスイッチT’z+〜T0の切換え操作を
行ない、交流電圧を出力する。例えば、U相の端子電圧
について云えば、中性点電位a点に対し正側スイッチ’
l”11がオンで負側スイッチTZIがオフのときはV
d/2に、スイッチT!IがオンでT、がオフのときは
−Vd/2になり、正側スイッチがオンしている期間と
負側スイッチがオンしている期間の比率を変えて交流電
圧を得る。従来、一般的に行なわれている正弦波PWM
ではこの比率を正弦波状に変えることにより、特に低い
次数の高調波成分の低減化を図るようにしている。第6
図に第5図におけるU相と■相の端子電圧波形と、両者
の相の線間電圧波形の一例を示す。なお、同図(イ)は
U相出力電圧、(ロ)はV相出力電圧、(ハ)はU−V
相線間電圧波形をそれぞれ示している。
FIG. 5 is a circuit diagram showing a three-phase output voltage type inverter main circuit composed of transistor switches (hereinafter simply referred to as switches). To perform PWM control, the switches T and TI3 connected to the positive potential and the switches T'z+ to T0 connected to the negative potential are operated to output an alternating current voltage. For example, regarding the terminal voltage of the U phase, the positive side switch'
When l”11 is on and the negative side switch TZI is off, V
Switch T on d/2! When I is on and T is off, it becomes -Vd/2, and an alternating current voltage is obtained by changing the ratio of the period when the positive side switch is on and the period when the negative side switch is on. Traditionally commonly used sine wave PWM
In this case, by changing this ratio into a sine wave shape, it is attempted to reduce particularly low-order harmonic components. 6th
The figure shows an example of the terminal voltage waveforms of the U phase and ■ phase in FIG. 5, and the line voltage waveforms of both phases. In addition, in the same figure (a) is the U-phase output voltage, (b) is the V-phase output voltage, and (c) is U-V.
Each phase-line voltage waveform is shown.

第7図に従来の正弦波pwMlil!11B方法の一例
を示す。同図において、11.12はそれぞれ正弦波、
三角波データが格納されているメモリ、21は掛算器、
3は比較器である。また、θ。は所望する出力電圧の基
本波成分の位相であり、これは読み出し専用メモリ (
以下、ROMとよぶ。)11に入力され、その出力は正
弦波となる。この信号と、出力電圧の大きさの目標値で
あるλ (以下、制御率と呼ぶ。)とが掛算器21で乗
算され、出力電圧の目標値eo  (以下、基準信号と
よぶ。)を得る。θゎはeoを変調する信号の位相であ
り、これはROM12に入力され、例えば三角波の信号
ec  (以下、変調信号とよぶ。)を得る。eoとe
cの大きさは比較器3で比岐され、eo >ecのとき
はPWMインバータの正側スイッチをオンし、e6<e
cのときは負側スイッチをオンする信号Sを得る。第8
図に基準信号e0、変調信号ecおよび出力電圧波形の
関係の一例を示す。
Figure 7 shows the conventional sine wave pwMlil! An example of the 11B method is shown. In the same figure, 11 and 12 are respectively sine waves,
A memory in which triangular wave data is stored; 21 is a multiplier;
3 is a comparator. Also, θ. is the phase of the fundamental component of the desired output voltage, which is stored in read-only memory (
Hereinafter, it will be referred to as ROM. ) 11, and its output becomes a sine wave. This signal is multiplied by λ (hereinafter referred to as the control rate), which is the target value of the output voltage magnitude, in a multiplier 21 to obtain the target value eo of the output voltage (hereinafter referred to as the reference signal). . θゎ is the phase of a signal that modulates eo, and this is input to the ROM 12 to obtain, for example, a triangular wave signal ec (hereinafter referred to as a modulation signal). eo and e
The magnitude of c is compared by comparator 3, and when eo > ec, the positive side switch of the PWM inverter is turned on, and e6<e
When c, a signal S is obtained that turns on the negative side switch. 8th
The figure shows an example of the relationship between the reference signal e0, the modulation signal ec, and the output voltage waveform.

第6図および第8図の出力電圧には、図から明らかな様
に少なからず高調波成分を含んでおり、この高調波成分
が例えば出力端子に接続される負荷や直流電源に好まし
くない影響を与えることはよ(知られている。また、各
高調波成分のうち特別の周波数成分が特に有害となる場
合がある。例えば、交流電動機を駆動する場合では負荷
がインダクタンス負荷であるため、低周波の高調波電圧
成分による高調波電流は比較的大きな値になり、巻線温
度を著しく上昇させたり、または大きな回転むらを生じ
させたりする。
As is clear from the figures, the output voltages in Figures 6 and 8 contain quite a few harmonic components, and these harmonic components can have an unfavorable effect on the load or DC power supply connected to the output terminal, for example. It is known that certain frequency components of each harmonic component can be particularly harmful. For example, when driving an AC motor, the load is an inductance load, so low frequency The harmonic current due to the harmonic voltage component becomes a relatively large value, which significantly increases the winding temperature or causes large rotational irregularities.

以下に、3相PWMインバータの場合を例にとって、出
力端子の線間電圧に含まれる高調波成分について詳しく
述べる。
The harmonic components included in the line voltage of the output terminal will be described in detail below, taking the case of a three-phase PWM inverter as an example.

すなわち、出力電圧は下記に示す各周波成分に分類する
ことができる。
That is, the output voltage can be classified into each frequency component shown below.

(a)基準信号e0の基本波と3の倍数を除く高調波成
分 (b)nfc+mf0成分(以下、側帯波とよぶ。)た
だし、fcは変調信号ecの基本波周波数であり、fo
は基準信号e0の基本波周波数である。また、nとmは
自然数である。
(a) Fundamental wave of reference signal e0 and harmonic components excluding multiples of 3 (b) nfc+mf0 component (hereinafter referred to as sideband). However, fc is the fundamental wave frequency of modulation signal ec, and fo
is the fundamental frequency of the reference signal e0. Further, n and m are natural numbers.

以上より、基準信号を正弦波とするならば上記(a)項
に属する高調波成分は存在しない。したがって、例えば
低周波の発生高調波を小さくしようとして、fcを高い
周波数にすれば、(b)項に属する高調波成分は高調波
となり、低周波の高調波成分は小さくなる。
From the above, if the reference signal is a sine wave, there are no harmonic components belonging to the above item (a). Therefore, for example, if fc is set to a high frequency in an attempt to reduce the harmonics generated at low frequencies, the harmonic components belonging to the (b) term become harmonics, and the harmonic components at low frequencies become small.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかしながら、fcを高くすると時間当たりのスイッチ
のスイッチング回数が増え、スイッチ素子の発生損失が
増加したり、あるいはスイッチ素子の動作遅れにより、
所望したスイッチングが行なえないなどの問題が生じる
。このため、PWMインバータの出力電圧高調波による
障害を低減する方法として、発生高調波と逆位相の電圧
や電流を発生する装置で高調波を補償したり、インバー
タを多重化して高調波を低減する方法が従来から採用さ
れているが、一般に高価であると云う問題がある。
However, when fc is increased, the number of times the switch is switched per time increases, the loss generated by the switch element increases, or the operation delay of the switch element increases.
Problems arise, such as not being able to perform desired switching. Therefore, as a method to reduce disturbances caused by output voltage harmonics of a PWM inverter, harmonics can be compensated for with a device that generates voltage or current that is in the opposite phase to the generated harmonics, or multiplexed inverters can be used to reduce harmonics. Although methods have been employed in the past, they generally have the problem of being expensive.

したがって、本発明は特別な主回路機器やスイッチのス
イッチング周波数を増加することなく、間車で安価な方
法によりスイッチのスイッチング動作を決め、特に負荷
等に対して有害となる高調波成分を低減する制御方式を
提供することを目的とする。
Therefore, the present invention determines the switching operation of the switch by an intermediate and inexpensive method without increasing the switching frequency of the special main circuit equipment or the switch, and reduces harmonic components that are harmful to the load in particular. The purpose is to provide a control method.

〔問題点を解決するための手段〕[Means for solving problems]

変調信号および基準信号の基本周波数をそれぞれfc、
foとするとき、該基準信号に対しそのスイッチング動
作にもとづいて発生するnfc±mfoなる周波数成分
と周波数および大きさが同じで位相が互いに逆の関係と
なる周波数成分を重畳して、PWM制御を行なう。
The fundamental frequencies of the modulation signal and the reference signal are respectively fc,
fo, PWM control is performed by superimposing frequency components nfc±mfo, which are generated based on the switching operation, on the reference signal, and frequency components that have the same frequency and magnitude but opposite phases. Let's do it.

〔作用〕[Effect]

変調信号と、所望する出力電圧に対応した基準信号の大
きさの比較により、スイッチのスイッチング動作を決定
するPWMにおいては、正弦波に近い出力電圧を得よう
とする場合、一般には基準信号を正弦波とする場合が多
い。しかし、スイッチング動作に基づいてnfc:tm
fo成分の側帯波が生じる。ところで、基準信号にある
周波数f。
In PWM, the switching operation of a switch is determined by comparing the magnitude of a modulation signal and a reference signal corresponding to the desired output voltage.When trying to obtain an output voltage close to a sine wave, the reference signal is generally set to a sine wave. Often called waves. However, based on the switching operation NFC:TM
A sideband wave of the fo component is generated. By the way, the frequency f in the reference signal.

を有した高調波Δe0を加算した信号を新たな基準信号
とするならば、高調波の周波数はf、とnfc±mfo
 きなる。本発明は周波数f、を特に有害となるn1f
(:!=mtfo (n+ + mzはそれぞれn、 
mの特定な値)の周波数に一致させ、しかも両高調波の
大きさが等しくかつ逆位相となる様に、基準信号に加算
すべき高調波を定める。このことにより、両高調波は互
いに打ち消され、インバータの出力端子には現れなくな
る。なお、正側スイッチと負側スイッチがオンしている
期間の比率で云うならば、本発明の方法はこの比率が正
弦波に消去したい高調波を含んだ波形となる様に制御す
ることにより、特定高調波が発生しない様にするものと
云うことができる。
If the signal obtained by adding the harmonic Δe0 with
Kinaru. The present invention reduces the frequency f to n1f, which is particularly harmful.
(:!=mtfo (n+ + mz are n, respectively)
The harmonics to be added to the reference signal are determined so as to match the frequency of the specific value of m), and so that both harmonics have equal magnitudes and opposite phases. As a result, both harmonics cancel each other out and no longer appear at the output terminal of the inverter. In terms of the ratio of the period during which the positive side switch and the negative side switch are on, the method of the present invention controls this ratio so that it becomes a sine wave containing the harmonics that you want to eliminate. It can be said that this prevents specific harmonics from being generated.

〔発明の実施例〕[Embodiments of the invention]

これ迄の種々の検討によれば、側帯波の大きさは制御率
λが一定ならば、変調周波数rcおよび基準周波数f0
に関係なく一定である。また、側帯波の位相は、変調信
号の位相θ。と基準信号の位相θ。のみによって与えら
れる。したがって、特定高調波の発生を抑制するために
eoに加算すべき高調波Δe0の大きさは制御率λのみ
の関数となり、またその位相はθゎとθ。によって求め
ることができる。
According to various studies so far, if the control rate λ is constant, the magnitude of the sideband wave depends on the modulation frequency rc and the reference frequency f0.
is constant regardless of Also, the phase of the sideband wave is the phase θ of the modulation signal. and the phase θ of the reference signal. given by only. Therefore, the magnitude of the harmonic Δe0 that should be added to eo in order to suppress the generation of a specific harmonic is a function only of the control rate λ, and its phase is θゎ and θ. It can be found by

第1図は発明の実施例を示すブロック図である。FIG. 1 is a block diagram showing an embodiment of the invention.

同図に符号If、12.21および3で示される各部は
第7図の場合と同様であるので説明を省略し、相違する
点について主として説明する。41゜42はそれぞれm
lおよびn3倍の逓倍器であり、m、およびn、はそれ
ぞれ低減したい高調波次数に相当する値に選ばれる。4
1.42の出力は加算器51で加算され、この位相を入
力としてROM13によって正弦波出力を得る。一方、
ROM14によって制御率λを人力として非線形関数か
つ(られ、この信号とROM13の出力が掛算器22で
乗算され、Δe0が求められる。Δe0は加算器52に
おいて正弦波の基準信号e0に加算され、この信号e 
0/を新たな基準信号として、e0′と変調信号e、の
大きさを比較器3で比較することにより、第7図の場合
と同様にスイッチのオン、オフが決められる。e、′は
正弦波にn、fc+m、f、成分の高調波が加算された
信号であり、この信号に従ってスイッチの動作状態を決
めることにより、n Hfe + m+fo成分の高調
波成分を持たない出力電圧波形を得ることができる。
The parts indicated by the symbols If, 12, 21, and 3 in the figure are the same as in the case of FIG. 7, so the explanation will be omitted, and the differences will be mainly explained. 41°42 are m respectively
It is a multiplier of l and n3 times, and m and n are respectively selected to values corresponding to the harmonic order to be reduced. 4
The outputs of 1.42 are added by an adder 51, and a sine wave output is obtained by the ROM 13 using this phase as an input. on the other hand,
The control rate λ is manually set as a nonlinear function by the ROM 14, and this signal and the output of the ROM 13 are multiplied by the multiplier 22 to obtain Δe0. Δe0 is added to the sine wave reference signal e0 in the adder 52, and this signal is signal e
By using 0/ as a new reference signal and comparing the magnitudes of e0' and modulation signal e with comparator 3, on/off of the switch is determined as in the case of FIG. e,' is a signal in which harmonics of n, fc + m, f components are added to a sine wave, and by determining the operating state of the switch according to this signal, an output that does not have harmonic components of n Hfe + m + fo components is obtained. A voltage waveform can be obtained.

また、本発明の原理によれば、eoに複数の高調波を加
算することによって、出力電圧に含まれる複数の高調波
も低減することが可能であることは云う迄もない。第2
図は本発明の別の実施例であり、変調周波数fcが基準
周波数の整数倍で表わされるときの例である。この場合
には、変調信号と基準信号ともにθ。から得ることがで
き、θ。
Further, according to the principle of the present invention, it goes without saying that by adding a plurality of harmonics to eo, it is also possible to reduce a plurality of harmonics included in the output voltage. Second
The figure shows another embodiment of the present invention, in which the modulation frequency fc is expressed as an integral multiple of the reference frequency. In this case, both the modulation signal and the reference signal are θ. can be obtained from θ.

はROM11.12に人力され、それぞれ正弦波と三角
波の出力を得る。基準信号e0に加算する信号Δe0も
θ。から得ることができ、このためθ。はROM13に
も入力される。ROM13の関数は基本波周波数の整数
倍の周波数を有する正弦波である。その他の各部14.
 21. 22. 3および52の機能は第1図の場合
と同様なので説明は省略する。
are manually input to ROM11 and 12 to obtain sine wave and triangular wave outputs, respectively. The signal Δe0 added to the reference signal e0 is also θ. and hence θ. is also input to the ROM 13. The function of the ROM 13 is a sine wave having a frequency that is an integral multiple of the fundamental wave frequency. Other parts 14.
21. 22. The functions of 3 and 52 are the same as in the case of FIG. 1, so a description thereof will be omitted.

以上の説明ではeoは正弦波として説明したが、3相出
力の場合に限れば、eoに3の倍数高調波を含んでいて
もこの高調波は出力端子の線間電圧には互いに相殺され
て現われない。例えば、電気学会研究会資料EPA−7
9−3rサイクロコンバータ給電交流可変速駆動方式と
変換装置容量」なる論文の如く、−相の出力電圧の目標
値、すなわちeoに3の倍数高調波を含ませてeoを台
形波状にする方式を採ることにすれば、同一の電源電圧
に対する出力電圧の基本波成分を増加させることができ
るので、更に好ましいものとなる。
In the above explanation, eo was explained as a sine wave, but in the case of three-phase output, even if eo contains harmonics that are multiples of 3, these harmonics will cancel each other out in the line voltage of the output terminal. Doesn't appear. For example, IEEJ Study Group Material EPA-7
9-3R Cycloconverter Power Supply AC Variable Speed Drive System and Converter Capacity", a method is proposed in which the target value of the -phase output voltage, that is, eo, includes harmonics that are multiples of 3 to make eo into a trapezoidal waveform. If adopted, the fundamental wave component of the output voltage for the same power supply voltage can be increased, which is even more preferable.

また、複数のPWMインバータを多重に接続して出力電
圧を低減する場合、例えば、2重化する場合において、
2重化では消去できない高調波成分を本発明では消去す
ることが可能であり、その結果、本発明は多重PWMイ
ンバータに対しても有効である。
In addition, when multiplexing multiple PWM inverters to reduce the output voltage, for example, when duplicating
The present invention can eliminate harmonic components that cannot be eliminated by duplication, and as a result, the present invention is also effective for multiple PWM inverters.

第3図は変調周波数fcを基準周波数f0の9倍にし、
従来の一般的な3相出力圧弦波PWMインバータで誘導
電動機を駆動した場合の一相の出力電圧、電流および誘
導電動機の発生トルクについて、ディジタルシミュレー
ションにより各部の波形を求めた例を示す。この場合、
出力電圧には低次の高調波成分としてfc−2f0成分
、すなわちre”9foであるので、9fo  2fo
−7fo成分(第7次高調波)が多く含まれ、従って電
流にも第7次高調波が多く含まれている。また、第7次
高調波電流は6倍のトルク脈動を発生することはよく知
られており、これはシミュレーション結果にも現われて
いる。これに対し、第4図は本発明により特に第7次高
調波電圧を低減した場合を示すもので、同図(イ)に点
線で示す基準信号には、第7次高調波電圧を低減する様
な大きさ、および位相を持った第7次高調波成分が含ま
れている。このとき、同図(ロ)や(ハ)に示す出力電
圧や電流には第7次高調波成分はほとんど含まれず、ま
た発生トルクの6倍のトルク脈動も同図(ニ)の如く低
減され、低次のトルク脈動はほとんど消去されている。
In Figure 3, the modulation frequency fc is set to nine times the reference frequency f0,
An example will be shown in which the waveforms of each part of the one-phase output voltage, current, and torque generated by the induction motor are obtained by digital simulation when the induction motor is driven by a conventional general three-phase output pressure sinusoidal PWM inverter. in this case,
The output voltage has an fc-2f0 component as a low-order harmonic component, that is, re"9fo, so 9fo 2fo
A large amount of −7fo component (seventh harmonic) is included, and therefore the current also contains a large amount of the seventh harmonic. Furthermore, it is well known that the seventh harmonic current generates six times as much torque pulsation, and this also appears in the simulation results. On the other hand, FIG. 4 shows a case in which the seventh harmonic voltage is particularly reduced according to the present invention, and the reference signal shown by the dotted line in FIG. 7th harmonic components with various magnitudes and phases are included. At this time, the output voltage and current shown in Figures (B) and (C) hardly contain the 7th harmonic component, and the torque pulsation, which is six times the generated torque, is reduced as shown in Figure (D). , low-order torque pulsations are almost eliminated.

高次のトルク脈動は、電動機の慣性モーメントの作用に
より回転むらになりにくいので、安定した回転を得るこ
とができる。
High-order torque pulsations are less likely to cause uneven rotation due to the effect of the moment of inertia of the electric motor, so stable rotation can be obtained.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、電圧形PWMインバータのスイッチの
動作を例えば三角波の変調信号と、出力電圧の所望値で
ある基準信号との大きさの比較により決定するものにお
いて、基準信号に少なくとも一つ以上の高調波成分を重
畳させることにより、それと同じ周波数を有する出力電
圧の高調波成分を消去あるいは低減することが可能とな
る利点がもたらされる。
According to the present invention, in a voltage-type PWM inverter in which the operation of a switch is determined by comparing the magnitude of a triangular wave modulation signal and a reference signal that is a desired value of output voltage, the reference signal has at least one or more The advantage of superimposing the harmonic components of the output voltage is that it is possible to eliminate or reduce the harmonic components of the output voltage having the same frequency.

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

第1図は本発明の実施例を示す構成図、第2図は本発明
の他の実施例を示す構成図、第3図は従来の一般的な3
相出力圧弦波インバータで誘導電動機を駆動した場合の
、−相の出力電圧、電流および電動機発生トルクを示す
波形図、第4図は本発明を適用した場合の第3図と同様
の各成分を示す波形図、第5図は3相出力電圧形PWM
インバータ主回路の一般的な例を示す回路図、第6図は
第5図におけるU相とV相の端子電圧波形と両者の相の
線間電圧波形を示す波形図、第7図はpwM制御方式の
一般的な例を示す構成図、第8図は第7図の動作を説明
するための各部波形図である。 符号説明 11〜14・・・リードオンリメモリ (ROM)、2
1.22・・・掛算器、3・・・比較器、41.42・
・・逓倍器、51.52・・・加算器、Tll〜T11
・・・正側スイッチ、T□〜T2.・・・負側スイッチ
、D、〜DI31D2.〜I)zt・・・ダイオード。 代理人 弁理士 並 木 昭 夫 代理人 弁理士 松 崎   清 第1図 1ム 第2図 第3図 第4図 第5図 第6図 第7N λ 第8図
Fig. 1 is a block diagram showing an embodiment of the present invention, Fig. 2 is a block diagram showing another embodiment of the present invention, and Fig. 3 is a conventional general 3
A waveform diagram showing the -phase output voltage, current, and motor generated torque when an induction motor is driven by a phase output pressure sinusoidal inverter. Figure 4 shows each component similar to Figure 3 when the present invention is applied. The waveform diagram shown in Figure 5 is a three-phase output voltage type PWM.
A circuit diagram showing a general example of an inverter main circuit, Fig. 6 is a waveform diagram showing the terminal voltage waveforms of the U phase and V phase in Fig. 5, and line voltage waveforms of both phases, and Fig. 7 is a pwM control A block diagram showing a general example of the system, and FIG. 8 is a waveform diagram of each part for explaining the operation of FIG. 7. Code explanation 11 to 14... Read only memory (ROM), 2
1.22... Multiplier, 3... Comparator, 41.42.
... Multiplier, 51.52 ... Adder, Tll to T11
... Positive side switch, T□~T2. ...Negative side switch, D, ~DI31D2. ~I) zt...diode. Agent Patent Attorney Akio Namiki Agent Patent Attorney Kiyoshi Matsuzaki Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7N λ Figure 8

Claims (1)

【特許請求の範囲】 変調信号と出力電圧指令値を代表する基準信号との大き
さの大小関係にもとづき正電位または負電位側に接続さ
れたスイッチング素子を切り換えて点弧することにより
出力電圧波形を制御する電圧形PWMインバータの制御
方式であって、前記変調信号および基準信号の基本周波
数をそれぞれf_c、f_oとするとき、該基準信号に
対しそのスイッチング動作にもとづいて発生するnf_
c±mf_o(n、mは自然数) なる周波数成分と同じ周波数および大きさをもちかつ逆
位相の関係となる周波数成分を重畳してPWM制御を行
なうことを特徴とする電圧形PWMインバータの制御方
式。
[Claims] The output voltage waveform is generated by switching and igniting a switching element connected to the positive potential or negative potential side based on the magnitude relationship between the modulation signal and a reference signal representing the output voltage command value. In this method, when the fundamental frequencies of the modulation signal and the reference signal are f_c and f_o, respectively, the nf_ that is generated based on the switching operation of the reference signal is
c±mf_o (n, m are natural numbers) A voltage source PWM inverter control method characterized by performing PWM control by superimposing a frequency component having the same frequency and magnitude as the frequency component and having an opposite phase relationship. .
JP61059376A 1986-03-19 1986-03-19 Control system for voltage-type pwm inverter Pending JPS62217860A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61059376A JPS62217860A (en) 1986-03-19 1986-03-19 Control system for voltage-type pwm inverter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61059376A JPS62217860A (en) 1986-03-19 1986-03-19 Control system for voltage-type pwm inverter

Publications (1)

Publication Number Publication Date
JPS62217860A true JPS62217860A (en) 1987-09-25

Family

ID=13111499

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61059376A Pending JPS62217860A (en) 1986-03-19 1986-03-19 Control system for voltage-type pwm inverter

Country Status (1)

Country Link
JP (1) JPS62217860A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02202397A (en) * 1989-01-31 1990-08-10 Fujitsu General Ltd Calculation of pwm waveform in inverter control
JP2011035991A (en) * 2009-07-30 2011-02-17 Hitachi Automotive Systems Ltd Power conversion device
JP2018126021A (en) * 2017-02-03 2018-08-09 株式会社豊田自動織機 Motor controller

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02202397A (en) * 1989-01-31 1990-08-10 Fujitsu General Ltd Calculation of pwm waveform in inverter control
JP2011035991A (en) * 2009-07-30 2011-02-17 Hitachi Automotive Systems Ltd Power conversion device
JP2018126021A (en) * 2017-02-03 2018-08-09 株式会社豊田自動織機 Motor controller

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