JPH0334316B2 - - Google Patents
Info
- Publication number
- JPH0334316B2 JPH0334316B2 JP56175710A JP17571081A JPH0334316B2 JP H0334316 B2 JPH0334316 B2 JP H0334316B2 JP 56175710 A JP56175710 A JP 56175710A JP 17571081 A JP17571081 A JP 17571081A JP H0334316 B2 JPH0334316 B2 JP H0334316B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic flux
- motor
- margin angle
- angle
- constant margin
- 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
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Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02P—CONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
- H02P6/00—Arrangements for controlling synchronous motors or other dynamo-electric motors using electronic commutation dependent on the rotor position; Electronic commutators therefor
- H02P6/34—Modelling or simulation for control purposes
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【発明の詳細な説明】
この発明は、直接式の位置検出器を持たない無
整流子電動機の定余裕角制御装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a constant margin angle control device for a commutatorless motor without a direct position detector.
かかる制御装置において、直接式の位置検出器
にかわるものとして電動機電圧を検出し、これか
ら磁束演算器により磁束波形を求め、この磁束波
形にて電動機側変換器(逆変換器)の位相制御パ
ルスを切り出す方法がある。この場合、磁束波形
の良し悪しが直接位相制御パルスの位相誤差を左
右するため、その演算には十分注意することが必
要である。特に、電動機の回転数の高いときトル
クが減少してもよい場合には、電動機の磁束を弱
めてその逆起電力があまり大きくならないように
する、いわゆる弱め磁束範囲をもつ制御において
は、その弱め磁束範囲において磁束演算波形の振
巾が減少することによる相対誤差が増大する傾向
にあることが知られている。したがつて、このよ
うな弱め磁束範囲においても位置検出器なし無整
流子電動機の定余裕角制御を安定に、しかも精度
よく行なうことが望ましい。 In such a control device, the motor voltage is detected as an alternative to a direct position detector, a magnetic flux waveform is determined from this using a magnetic flux calculator, and the phase control pulse of the motor side converter (inverter) is determined using this magnetic flux waveform. There is a way to cut it out. In this case, since the quality of the magnetic flux waveform directly affects the phase error of the phase control pulse, it is necessary to be very careful in its calculation. In particular, when the torque can be reduced when the rotational speed of the motor is high, control with a so-called flux-weakening range, which weakens the magnetic flux of the motor to prevent its back electromotive force from becoming too large, is used. It is known that the relative error tends to increase as the amplitude of the magnetic flux calculation waveform decreases in the magnetic flux range. Therefore, it is desirable to stably and accurately control the constant margin angle of a commutatorless motor without a position detector even in such a flux weakening range.
第1図はかかる磁束演算波形による無整流子電
動機の位置検出器なし定余裕角制御装置の従来例
を示す構成図である。 FIG. 1 is a block diagram showing a conventional example of a constant margin angle control device without a position detector for a non-commutator motor using such a magnetic flux calculation waveform.
同図において、1は速度調節器、2は電流調節
器、3は点弧角調整器、4はサイリスタ変換器、
5は速度起電力演算器、6は積分器、7は定余裕
角パルス発生器、8はパルス分配器、9は無整流
子電動機、10はタコジエネレータ(速度検出用
発電機)、SEは速度設定器、DCLは直流平滑用リ
アクトルである。 In the figure, 1 is a speed regulator, 2 is a current regulator, 3 is a firing angle regulator, 4 is a thyristor converter,
5 is a speed electromotive force calculator, 6 is an integrator, 7 is a constant margin angle pulse generator, 8 is a pulse distributor, 9 is a commutatorless motor, 10 is a tachogenerator (generator for speed detection), and SE is a speed setting The reactor and DCL are DC smoothing reactors.
交流電源(3φ)は電源側変換器41を介して
直流に変換された後、適宜平滑リアクトルDCL
を介し、さらに電動機側変換器42で交流に再変
換され、該交流電力により同期電動機9が駆動さ
れる。以上のように構成される無整流子電動機9
における速度制御は、速度設定器SEからの速度
設定信号n*と、電動機に直結した速度検出用発
電機10からの速度検出信号nとを比較して速度
調節器1に入力し、次いで速度調節器1の出力信
号、すなわち電流設定信号i*と電源側変換器41
の交流側入力電流検出信号iとを比較して電流調
節器2に入力し、得られた出力信号で点弧角調節
器3を介して電源側変換器41の位相制御を行な
うことにより達成される。一方、電動機側変換器
42の位相制御は、電動機電圧VMおよび電動機
電流IMから電動機速度起電力Eを求め、これを積
分演算して磁束Φの波形(有効磁束の各相成分)
を得た後、この磁束波形を定余裕角パルス発生器
7に入力し、出力される180゜el(電気角)幅の定
余裕角パルスをパルス分配器8に入力することに
より、その出力で行なわれる。 After the AC power supply (3φ) is converted to DC via the power supply side converter 41, it is connected to a smoothing reactor DCL as appropriate.
The AC power is then reconverted into AC power by the motor-side converter 42, and the synchronous motor 9 is driven by the AC power. Commutatorless motor 9 configured as above
Speed control is performed by comparing the speed setting signal n * from the speed setting device SE with the speed detection signal n from the speed detection generator 10 directly connected to the motor and inputting it to the speed regulator 1. The output signal of the converter 1, that is, the current setting signal i * and the power supply side converter 41
This is achieved by comparing the AC side input current detection signal i of Ru. On the other hand, the phase control of the motor-side converter 42 is performed by determining the motor speed electromotive force E from the motor voltage V M and the motor current I M , and integrating this to form the waveform of the magnetic flux Φ (each phase component of the effective magnetic flux).
After obtaining this magnetic flux waveform, input the constant margin angle pulse generator 7 to the constant margin angle pulse generator 7, and input the output constant margin angle pulse with a width of 180° EL (electrical angle) to the pulse distributor 8. It is done.
第1図に示された定余裕角パルス発生器7は、
第2図の如く構成される。なお、第2図は定余裕
角パルス発生器をより詳細に示すブロツク図であ
り、第3図は第2図の各部波形を示す波形図であ
り、第4図は定格磁束時、弱め磁束時における各
磁束波形と制御進み角および定余裕角との関係を
説明する波形図である。 The constant margin angle pulse generator 7 shown in FIG.
It is configured as shown in FIG. In addition, Fig. 2 is a block diagram showing the constant margin angle pulse generator in more detail, Fig. 3 is a waveform diagram showing the waveforms of each part in Fig. 2, and Fig. 4 is a waveform diagram showing the waveforms at rated magnetic flux and at weakening magnetic flux. It is a waveform diagram explaining the relationship between each magnetic flux waveform, control advance angle, and constant margin angle in .
第2図において、71は90゜el位相進め回路、
72はコンパレータ、73は転流重なり角(u)
演算器(以下、u演算器ともいう)、74は磁束
絶対値演算器S1〜S3はスイツチで磁束の各線間成
分Φuv,Φvw,Φwuが正のときは“1”側にあり、
負のときは“2”側に切り換わるものである。 In Figure 2, 71 is a 90°el phase advance circuit;
72 is a comparator, 73 is commutation overlap angle (u)
Arithmetic unit (hereinafter also referred to as u arithmetic unit), 74 is a magnetic flux absolute value arithmetic unit S 1 to S 3 is a switch that switches to the “1” side when each line component of magnetic flux Φ uv , Φ vw , Φ wu is positive. can be,
When it is negative, it switches to the "2" side.
その動作について、第2図および第3図を参照
して説明する。 Its operation will be explained with reference to FIGS. 2 and 3.
第3図イで示される如き有効磁束の各線間成分
(Φuv,Φvw,Φwu)は、まず90゜el位相進め回路7
1においてそれぞれ90゜elだけ進められる(Φuv→
Φ′uv,Φvw→Φ′vw,Φwu→Φ′wu)。なお、この位
相
進め回路71は、入力信号が3相平衡入力であれ
ば単純な加減算回路によつて構成することができ
る。このようにして得れるΦ′uv,Φ′vw,Φ′wuはそ
れぞれ速度起電力Euv,Evw,Ewu(例えば、Euvは
uv間の速度起電力)と同位相となる。一方、磁
束絶対値演算器74の出力を分圧して得られる余
裕角設定電圧V〓と、電流指令値(または検出値)
および磁束絶対値からu演算器73により得られ
る重なり角演算電圧Vuとが加算され、制御進み
角(β)指令電圧V〓が作成される。次いで、制
御進み角指令電圧V〓はスイツチS1〜S3により各
相の入力磁束波形の正負に応じて極性が切り換え
られる。このようにして得られた矩形波のβ指令
電圧(±V〓)は第3図ロの如くそれぞれΦ′uv,
Φ′vw,Φ′wuと大小比較すことより、電圧/角度の
変換が行なわれ、第3図ハの如き定余裕角パルス
(180゜el幅)が作り出される。ここで上述の大小
比較は、90゜el位相進め回路71の出力と制御進
み角指令電圧Vβとの差を減算回路によつて求め、
その差をコンパレータ72において定数と比較す
ることにより行われる。ところで、第1図に示さ
れるような定余裕角制御の場合に弱め磁束範囲が
あると、演算磁束波形の振幅はそれに応じて小さ
くなる。すると、定余裕角パルス発生器7内のコ
ンパレータ72による角度誤差が増大される恐れ
がある。すなわち、第4図からも明らかなよう
に、同じ誤差電圧ΔV〓をもつβ指令電圧V〓でも
コンパレータ72で角度変換した場合、弱め磁束
波形の時の角度誤差Δβ′(第4図ロ参照)の方が、
定格磁束波形のそれ(第4図イのΔβ参照)より
も大きくなる。これは弱め磁束範囲が大きいほど
問題となる。 Each line component (Φ uv , Φ vw , Φ wu ) of the effective magnetic flux as shown in FIG.
1, each is advanced by 90°el (Φ uv →
Φ′ uv , Φ vw →Φ′ vw , Φ wu →Φ′ wu ). Note that this phase advance circuit 71 can be constructed by a simple addition/subtraction circuit if the input signal is a three-phase balanced input. Φ′ uv , Φ′ vw , Φ′ wu obtained in this way are velocity electromotive forces E uv , E vw , E wu (for example, E uv is
It has the same phase as the velocity electromotive force between uv). On the other hand, the margin angle setting voltage V obtained by dividing the output of the magnetic flux absolute value calculator 74 and the current command value (or detected value)
and the overlap angle calculation voltage V u obtained by the u calculator 73 from the magnetic flux absolute value are added to create the control advance angle (β) command voltage V〓. Next, the polarity of the control advance angle command voltage V〓 is switched by switches S 1 to S 3 according to the positive or negative sign of the input magnetic flux waveform of each phase. The rectangular wave β command voltage (±V〓) obtained in this way is Φ′ uv and
By comparing the magnitudes of Φ′ vw and Φ′ wu , a voltage/angle conversion is performed, and a constant margin angle pulse (180°el width) as shown in FIG. 3C is created. Here, the above-mentioned magnitude comparison is performed by calculating the difference between the output of the 90°el phase advance circuit 71 and the control advance angle command voltage Vβ using a subtraction circuit.
This is done by comparing the difference with a constant in the comparator 72. By the way, if there is a flux weakening range in the case of constant margin angle control as shown in FIG. 1, the amplitude of the calculated magnetic flux waveform becomes smaller accordingly. Then, there is a possibility that the angular error caused by the comparator 72 in the constant margin angle pulse generator 7 will increase. In other words, as is clear from Fig. 4, even if the β command voltage V has the same error voltage ΔV, when the angle is converted by the comparator 72, the angular error Δβ' (see Fig. 4 b) when the flux is weakened is changed. It is better to
It becomes larger than that of the rated magnetic flux waveform (see Δβ in Fig. 4 A). This becomes a problem as the flux weakening range increases.
この発明は上記に鑑みなされたもので、弱め磁
束範囲においても無整流子電動機の定余裕角制御
を高精度に行ないうるようにすることを目的とす
るものである。 The present invention has been made in view of the above, and an object of the present invention is to enable constant margin angle control of a commutatorless motor to be performed with high precision even in the flux weakening range.
上記目的は、本発明によれば、少なくとも逆変
換器を含む電力変換装置によつて給電される無整
流子電動機の電動機電圧および電流に基づいて該
電動機に速度起電力を演算する起電力演算回路
と、該起電力を積分して磁束波形を演算する積分
回路と、該磁束波形を基準にして電動機の転流重
なり角を演算し、該重なり角と別途設定される電
動機の転流余裕角との和と位相を90度進められた
前記磁束波形との比較により決定された制御進み
角を有する定余裕角制御パルスを切り出す定余裕
角パルス発生回路と、を備え、切り出された前記
定余裕角制御パルスをゲート信号として前記電力
変換装置における逆変換器の点弧位相を制御する
ようにした無整流子電動機の定余裕角制御装置に
おいて、
前記積分回路により演算される磁束波形の振幅
を弱め磁束領域においても常に最大定格振幅に保
つ手段を設けたことにより達成される。 According to the present invention, the above object is an electromotive force calculation circuit that calculates a speed electromotive force for a non-commutator motor based on the motor voltage and current of the non-commutator motor supplied by a power conversion device including at least an inverter. , an integrating circuit that integrates the electromotive force to calculate a magnetic flux waveform, and calculates the commutation overlap angle of the motor based on the magnetic flux waveform, and calculates the overlap angle and the separately set commutation margin angle of the motor. a constant margin angle pulse generation circuit that cuts out a constant margin angle control pulse having a control advance angle determined by comparing the sum of the sum and the magnetic flux waveform whose phase is advanced by 90 degrees; In a constant margin angle control device for a commutatorless motor, the control pulse is used as a gate signal to control the firing phase of an inverter in the power conversion device, and the magnetic flux is weakened by weakening the amplitude of the magnetic flux waveform calculated by the integrating circuit. This is achieved by providing a means to always maintain the maximum rated amplitude even in this area.
以下、この発明の実施例を図面を参照して説明
する。 Embodiments of the present invention will be described below with reference to the drawings.
第5図はこの発明の要部実施例を示すブロツク
図、第6図は弱め磁束パターンと速度関数パター
ンとの関係を示す特性図、第7図はこの発明の他
の実施例を示すブロツク図である。 FIG. 5 is a block diagram showing an embodiment of the main part of the present invention, FIG. 6 is a characteristic diagram showing the relationship between the magnetic flux weakening pattern and the velocity function pattern, and FIG. 7 is a block diagram showing another embodiment of the present invention. It is.
第5図において、5〜8は第1図に示されたも
のと同じであり、11は乗算器、12は速度関数
発生器である。なお、同図は電動側変換器(逆変
換器)の制御回路のみを示すものである。 In FIG. 5, numerals 5 to 8 are the same as those shown in FIG. 1, 11 is a multiplier, and 12 is a speed function generator. Note that this figure shows only the control circuit of the electric side converter (inverse converter).
同図からも明らかなように、この発明は速度起
電力演算器5と積分器6との間に乗算器11が設
けられ、速度関数発生器12により得られる電動
機速度nに応じた信号f(n)と、速度起電力E
とを乗算して磁束信号Φを作るようにしている点
が特徴である。信号f(n)は弱め磁束のパター
ンに応じて決められ、例えば磁束パターンをΦ
(n)とすれば、f(n)=K・1/Φ(n)(Kは
比例定数)の如く表わされる。すなわち、第6図
の点線から右側に示されるような弱め磁束領域に
おいて同図のΦ(n)の如く速度に反比例して磁
束弱めを行なうものとすると、f(n)は同図に
示されるように直線的に増大するパターンとな
る。このようにすれば、弱め磁束範囲におても積
分器6の出力磁束波形は最大定格振幅をもつよう
になり、したがつて定余裕角パルス発生器におけ
る角度誤差の発生を極力抑止することができる。 As is clear from the figure, in the present invention, a multiplier 11 is provided between the speed electromotive force calculator 5 and the integrator 6, and a signal f( n) and speed electromotive force E
The feature is that the magnetic flux signal Φ is generated by multiplying the The signal f(n) is determined according to the pattern of magnetic flux weakening, for example, if the magnetic flux pattern is
(n), it is expressed as f(n)=K·1/Φ(n) (K is a proportionality constant). That is, in the flux weakening region shown on the right side of the dotted line in Figure 6, if the magnetic flux is weakened in inverse proportion to the speed as shown in Φ(n) in the figure, then f(n) is as shown in the figure. The pattern increases linearly. In this way, the output magnetic flux waveform of the integrator 6 will have the maximum rated amplitude even in the flux weakening range, and therefore the occurrence of angular errors in the constant margin angle pulse generator can be suppressed as much as possible. can.
乗算器の一方の入力として、上述の如き信号f
(n)のかわりに定余裕角パルス発生器(第2図
参照)によつて得られる磁束絶対値の逆関数信号
を導入してもよい。第7図はこのような場合の実
施例を示すブロツク図で、上記の如き磁束絶対値
の逆関数発生器13が設けられている点が特徴で
ある。 As one input of the multiplier, the signal f as described above
(n) may be replaced by an inverse function signal of the magnetic flux absolute value obtained by a constant margin angle pulse generator (see FIG. 2). FIG. 7 is a block diagram showing an embodiment in such a case, and is characterized in that it is provided with an inverse function generator 13 for the absolute value of magnetic flux as described above.
以上のように、この発明によれば、定余裕角パ
ルスを切り出すための磁束波形の振幅を弱め磁束
範囲においても常に最大定格振幅に保つようにし
たため、定余裕角パルス発生器での角度誤差発生
が少なくなり、高精度な位置検出器なし定余裕角
制御が可能となる。 As described above, according to the present invention, the amplitude of the magnetic flux waveform for extracting the constant margin angle pulse is always kept at the maximum rated amplitude even in the weakening magnetic flux range, so that an angular error occurs in the constant margin angle pulse generator. is reduced, and highly accurate constant margin angle control without a position detector is possible.
なお、この発明は直流式だけでなく交流式の無
整流子電動機制御システムの弱め磁束運転時に適
用することができる。 Note that the present invention can be applied to flux-weakening operation of not only DC type but also AC type commutatorless motor control systems.
第1図は位置検出器なし無整流子電動機の定余
裕角制御装置の従来例を示す構成図、第2図は定
余裕角パルス発生器を詳細に示すブロツク図、第
3図は第2図の各部の波形を示す波形図、第4図
は定格磁束時および弱め磁束時における各磁束波
形と、制御進み角および定余裕角との関係を説明
するための波形図、第5図はこの発明の実施例を
示す要部ブロツク図、第6図は弱め磁束パターン
と速度関数パターンとの関係を示す特性図、第7
図はこの発明の他の実施例を示す要部ブロツク図
である。
符号説明、1……速度調節器、2……電流調節
器、3……点弧パルス調整器、4……サイリスタ
変換器、5……速度起電力演算器、6……積分
器、7……定余裕角パルス発生器、71……
90゜el位相進め回路、72……コンパレータ、7
3……u演算器、74……磁束絶対値演算器、8
……パルス分配器、9……無整流子電動機、10
…タコジエネレータ、11……掛算器、12……
関数発生器、13……逆関数発生器。
Fig. 1 is a block diagram showing a conventional example of a constant margin angle control device for a commutatorless motor without a position detector, Fig. 2 is a block diagram showing details of a constant margin angle pulse generator, and Fig. 3 is a block diagram showing the details of a constant margin angle pulse generator. FIG. 4 is a waveform diagram showing the relationship between each magnetic flux waveform at rated magnetic flux and weakening flux, and the control advance angle and constant margin angle. FIG. 5 is a waveform diagram showing the waveform of each part of this invention. FIG. 6 is a characteristic diagram showing the relationship between the flux weakening pattern and the velocity function pattern, and FIG.
The figure is a main part block diagram showing another embodiment of the present invention. Description of symbols, 1...Speed regulator, 2...Current regulator, 3...Ignition pulse regulator, 4...Thyristor converter, 5...Speed electromotive force calculator, 6...Integrator, 7... ...Constant margin angle pulse generator, 71...
90°el phase advance circuit, 72...Comparator, 7
3... u computing unit, 74... magnetic flux absolute value computing unit, 8
... Pulse distributor, 9 ... Commutatorless motor, 10
...Tachogenerator, 11...Multiplier, 12...
Function generator, 13...Inverse function generator.
Claims (1)
つて給電される無整流子電動機の電動機電圧およ
び電流に基づいて該電動機の速度起電力を演算す
る起電力演算回路5と、該起電力を積分して磁束
波形を演算する積分回路6と、該磁束波形を基準
にして電動機の転流重なり角を演算し、該重なり
角と別途設定される電動機の転流余裕角との和と
位相を90度進められた前記磁束波形との比較によ
り決定された制御進み角を有する定余裕角制御パ
ルスを切り出す定余裕角パルス発生回路7と、を
備え、切り出された前記定余裕角制御パルスをゲ
ート信号として前記電力変換装置における逆変換
器の点弧位相を制御するようにした無整流子電動
機の定余裕角制御装置において、 前記積分回路6により演算される磁束波形の振
幅を弱め磁束領域においても常に最大定格振幅に
保つ手段11,12,13を設けたことを特徴と
する無整流子電動機のの定余裕角制御装置。[Scope of Claims] 1. An electromotive force calculation circuit 5 that calculates the speed electromotive force of a non-commutated motor based on the motor voltage and current of the non-commutated motor supplied by a power conversion device including at least an inverter; An integrating circuit 6 integrates the electromotive force to calculate a magnetic flux waveform, and calculates a commutation overlap angle of the motor based on the magnetic flux waveform, and combines the overlap angle with a separately set commutation margin angle of the motor. a constant margin angle pulse generation circuit 7 that extracts a constant margin angle control pulse having a control advance angle determined by comparison with the magnetic flux waveform whose sum and phase are advanced by 90 degrees; In a constant margin angle control device for a commutatorless motor, the firing phase of an inverter in the power converter is controlled using a control pulse as a gate signal, the amplitude of the magnetic flux waveform calculated by the integrating circuit 6 is weakened. A constant margin angle control device for a commutatorless motor, characterized in that means 11, 12, and 13 are provided to always keep the amplitude at the maximum rated amplitude even in the magnetic flux region.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56175710A JPS5879491A (en) | 1981-11-04 | 1981-11-04 | Constant marginal angle control system for commutatorless motor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56175710A JPS5879491A (en) | 1981-11-04 | 1981-11-04 | Constant marginal angle control system for commutatorless motor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5879491A JPS5879491A (en) | 1983-05-13 |
| JPH0334316B2 true JPH0334316B2 (en) | 1991-05-22 |
Family
ID=16000879
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56175710A Granted JPS5879491A (en) | 1981-11-04 | 1981-11-04 | Constant marginal angle control system for commutatorless motor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5879491A (en) |
-
1981
- 1981-11-04 JP JP56175710A patent/JPS5879491A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5879491A (en) | 1983-05-13 |
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