Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JP3106471B2 - Vector control method of induction motor - Google Patents
[go: Go Back, main page]

JP3106471B2 - Vector control method of induction motor - Google Patents

Vector control method of induction motor

Info

Publication number
JP3106471B2
JP3106471B2 JP01307335A JP30733589A JP3106471B2 JP 3106471 B2 JP3106471 B2 JP 3106471B2 JP 01307335 A JP01307335 A JP 01307335A JP 30733589 A JP30733589 A JP 30733589A JP 3106471 B2 JP3106471 B2 JP 3106471B2
Authority
JP
Japan
Prior art keywords
magnetic flux
induction motor
constant
amount
secondary magnetic
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 - Fee Related
Application number
JP01307335A
Other languages
Japanese (ja)
Other versions
JPH03169293A (en
Inventor
秀紀 高崎
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.)
Yaskawa Electric Corp
Original Assignee
Yaskawa Electric Corp
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 Yaskawa Electric Corp filed Critical Yaskawa Electric Corp
Priority to JP01307335A priority Critical patent/JP3106471B2/en
Publication of JPH03169293A publication Critical patent/JPH03169293A/en
Application granted granted Critical
Publication of JP3106471B2 publication Critical patent/JP3106471B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Control Of Ac Motors In General (AREA)

Description

【発明の詳細な説明】 〔従来の技術〕 本発明は、電流形(ベクトル制御形)インバータで駆
動される誘導電動機のベクトル制御方法に関する。
Description of the Related Art [0001] The present invention relates to a vector control method for an induction motor driven by a current type (vector control type) inverter.

〔従来の技術〕[Conventional technology]

第1図は、従来の制御方法により誘導電動機が駆動さ
れる場合の制御指令系統図である。
FIG. 1 is a control command system diagram when an induction motor is driven by a conventional control method.

演算器8へ誘導電動機6の速度指令Nrefが与えられる
と、演算器8は、この速度指令Nrefと、誘導電動機6の
回転軸に連結した速度検出器7からの帰還速度Nとの速
度偏差を速度制御器1へ出力する。速度制御器1は、こ
の速度偏差の入力に基づき、誘導電動機6の二次電流指
令値I2*をベクトル制御器2へ出力する。帰還速度N
は、また、磁束指令器3に入力され、磁束指令器3は、
この帰還速度Nに対応したパターンでの誘導電動機6の
指令二次磁束量Φ*をベクトル制御器2へ出力する。
When the speed command Nref of the induction motor 6 is given to the calculator 8, the calculator 8 calculates the speed deviation between the speed command Nref and the feedback speed N from the speed detector 7 connected to the rotation shaft of the induction motor 6. Output to speed controller 1. The speed controller 1 outputs a secondary current command value I2 * of the induction motor 6 to the vector controller 2 based on the input of the speed deviation. Return speed N
Is also input to the magnetic flux commander 3, and the magnetic flux commander 3
The command secondary magnetic flux amount Φ * of the induction motor 6 in a pattern corresponding to the feedback speed N is output to the vector controller 2.

ベクトル制御器2は、これら二次電流指令値I2*及び
指令二次磁束量Φ*の入力に基づきベクトル演算を行
い、誘導電動機6の指令一次電流i1*を電流形(ベクト
ル制御形)インバータ4に出力する。これにより、交流
電源5からの誘導電動機6への一次電流i1が制御され、
誘導電動機6は指令速度Nrefで定トルクあるいは定出力
を保ちながら駆動される。
The vector controller 2 performs a vector operation based on the input of the secondary current command value I2 * and the command secondary magnetic flux amount Φ *, and converts the command primary current i1 * of the induction motor 6 into a current type (vector control type) inverter 4. Output to Thereby, the primary current i1 from the AC power supply 5 to the induction motor 6 is controlled,
The induction motor 6 is driven while maintaining a constant torque or a constant output at the command speed Nref.

ところで、一般的に誘導電動機の出力Pは次ぎの
(1)式で表される。
By the way, generally, the output P of the induction motor is expressed by the following equation (1).

P=K1・N・I2・Φ ……(1) ただし、 K1は定数、 Nは誘導電動機の回転速度、 I2は誘導電動機の二次電流値、 Φは誘導電動機の二次磁束量である。 P = K1, N, I2, Φ (1) where K1 is a constant, N is the rotation speed of the induction motor, I2 is the secondary current value of the induction motor, and Φ is the amount of secondary magnetic flux of the induction motor.

ここで、N>Nbのときに Φ=(Nb/N)・Φ0 ……(2) しかして、 Nbは誘導電動機の基底速度(固定)、 Nは誘導電動機の速度、 Φ0は誘導電動機の定格二次磁束量 とすれば、(1)式より P=K1・Nb・I2・Φ0 ……(3) となり、同一の誘導電動機の二次電流値I2であれば、誘
導電動機の出力Pは一定となる。
Here, when N> Nb, Φ = (Nb / N) · Φ0 (2) However, Nb is the base speed of the induction motor (fixed), N is the speed of the induction motor, and Φ0 is the rating of the induction motor. Assuming the amount of secondary magnetic flux, from equation (1), P = K1 · Nb · I2 · Φ0 (3), and if the secondary current value I2 of the same induction motor, the output P of the induction motor is constant. Becomes

第4図は、このときの磁束指令器における回転速度と
指令二次磁束量(指令磁束の大きさ)Φの特性図であ
る。
FIG. 4 is a characteristic diagram of the rotation speed and the command secondary magnetic flux amount (magnitude of the command magnetic flux) Φ * in the magnetic flux commander at this time.

誘導電動機6が正転において、起動[回転速度0]か
らは誘導電動機の定格二次磁束量Φ0を保ちながら、回
転速度Nを上昇させ、定トルク制御から定出力制御への
変換する演算の基底となる基底回転速度Nbに至ると[直
線21で移行する]、それからは二次曲線43に従い最高回
転速度NMaxまで定出力領域で駆動される。
When the induction motor 6 rotates forward, the rotation speed N is increased from the start [rotation speed 0] while maintaining the rated secondary magnetic flux amount Φ0 of the induction motor, and the basis of the calculation for converting from constant torque control to constant output control is maintained. When the rotation speed reaches the base rotation speed Nb (which shifts along the straight line 21), the motor is driven in the constant output region up to the maximum rotation speed NMax according to the quadratic curve 43.

このさい(2)式の条件Φ=(Nb/N)・Φ0であり、
最高回転速度NMaxではΦ=(Nb/NMax)・Φ0である。
In this case, the condition Φ = (Nb / N) · Φ0 in the equation (2) is satisfied.
At the maximum rotation speed NMax, Φ = (Nb / NMax) · Φ0.

なお、回転速度N=0から左行する特性曲線22,44は
同様にして、逆転の場合である。
The characteristic curves 22 and 44 going leftward from the rotation speed N = 0 are the same in the case of reverse rotation.

そして、この場合における誘導電動機の回転速度Nお
よび二次磁束量Φの時間微分のそれぞれについての時間
変化の特性図が第5図(a),(b)である。
FIGS. 5 (a) and 5 (b) show characteristic diagrams of the time change for each of the rotational speed N of the induction motor and the time derivative of the secondary magnetic flux amount Φ in this case.

すなわち、誘導電動機6の回転速度Nの時間tの変化
は曲線5aとなり、時点t1で基底回転速度Nbとなり、時点
t2で最高回転速度NMaxに到達する。
That is, the change of the rotation speed N of the induction motor 6 over time t becomes a curve 5a, and at time t1, it becomes the base rotation speed Nb.
At t2, the rotation speed reaches the maximum rotation speed NMax.

この駆動運転での二次磁束量Φの時間微分についての
時間変化は5bとなり、時点t1から時点t2までの変化が顕
著である。
The temporal change in the time derivative of the secondary magnetic flux amount Φ in this driving operation is 5b, and the change from the time point t1 to the time point t2 is remarkable.

〔発明が解決しようとする課題] ところが従来の制御方法では、誘導電動機6を短時間
で加速した場合は、第5図(b)の特性曲線5bの変化に
起因して定トルク領域から定出力領域に入った時点(t
1)で誘導電動機6の電圧,電流が振動し、その結果、
回転速度Nにも振動が生じる問題点があった。
[Problems to be Solved by the Invention] However, in the conventional control method, when the induction motor 6 is accelerated in a short time, the constant output from the constant torque region is caused by the change of the characteristic curve 5b in FIG. 5 (b). When entering the area (t
In 1), the voltage and current of the induction motor 6 oscillate, and as a result,
There is also a problem that vibration occurs in the rotation speed N.

そこで本発明は、急加減速時にも電圧,電流の振動が
発生しにくい定出力制御を行う方法を提供することを、
その目的とする。
Accordingly, the present invention provides a method for performing constant output control in which voltage and current oscillations are less likely to occur even during rapid acceleration / deceleration.
With that purpose.

〔課題を解決するための手段〕[Means for solving the problem]

上記目的を達成するために、本発明は、誘導電動機の
検出回転速度と速度指令との偏差に基づきこの誘導電動
機の2次電流を制御すると共に、この検出回転速度の入
力に基づき誘導電動機の2次磁束量を制御し、更にこれ
ら2次電流及び2次磁束量に基づき1次電流の制御を行
う場合に、前記2次磁束量に対する制御領域を定トルク
領域と定出力領域とに分け、定トルク領域では前記検出
回転速度の変化にかかわらず前記2次磁束量が一定とな
るように磁束一定制御を行い、定出力領域では前記検出
回転速度が増加するにしたがって前記2次磁束量が減少
するように磁束弱め制御を行う誘導電動機のベクトル制
御方法において、前記2次磁束量の減少が直線的なもの
となるようにし、この2次磁束量の時間微分値が一定と
なるように前記定出力領域での磁束弱め制御を行う、こ
とを特徴とする。
In order to achieve the above object, the present invention controls the secondary current of the induction motor based on the deviation between the detected rotation speed of the induction motor and the speed command, and controls the secondary current of the induction motor based on the input of the detected rotation speed. When controlling the amount of secondary magnetic flux and further controlling the primary current based on the secondary current and the amount of secondary magnetic flux, the control region for the amount of secondary magnetic flux is divided into a constant torque region and a constant output region, In the torque region, the magnetic flux constant control is performed so that the amount of the secondary magnetic flux is constant regardless of the change in the detected rotational speed. In the constant output region, the amount of the secondary magnetic flux decreases as the detected rotational speed increases. In the vector control method of the induction motor for performing the magnetic flux weakening control as described above, the decrease of the secondary magnetic flux amount is made linear, and the constant value is set so that the time differential value of the secondary magnetic flux amount becomes constant. Performing flux-weakening control in the region, characterized in that.

〔作用〕[Action]

本発明によれば、定出力制御での磁束弱め制御が、磁
束変化率が一定となるように行われるので、誘導電動機
の加減速時における電圧、電流の振動の発生を極力抑制
することができる。
According to the present invention, since the magnetic flux weakening control in the constant output control is performed so that the rate of change of the magnetic flux is constant, it is possible to minimize the occurrence of voltage and current vibrations during acceleration / deceleration of the induction motor. .

〔実施例〕〔Example〕

本発明の一実施例における指令二次磁束量(指令磁束
の大きさ)Φの回転速度Nについての特性曲線図を第
2図に表す。
FIG. 2 shows a characteristic curve diagram of the command secondary magnetic flux amount (magnitude of the command magnetic flux) Φ * with respect to the rotation speed N in one embodiment of the present invention.

また、その場合における誘導電動機の回転速度Nおよ
び二次磁束量Φの時間微分のそれぞれの時間tについて
の特性曲線図が第3図(a)および第3図(b)に示さ
れる。
3 (a) and 3 (b) show characteristic curves for the time t of the rotational speed N of the induction motor and the time derivative of the secondary magnetic flux amount Φ in that case.

すべての図面において、同一符号は同一要素を表す。 In all the drawings, the same reference numerals denote the same elements.

ところで、誘導電動機6の二次磁束量のベクトル表示
φは次式で示される。
By the way, the vector expression φ of the amount of secondary magnetic flux of the induction motor 6 is expressed by the following equation.

φ=Φεjωt ……(4) ただし、 εjωtは角速度ωt[ω=2πf fは周波数 t
は時間]で回転する単位ベクトルである。
φ = Φε jωt (4) where ε jωt is the angular velocity ωt [ω = 2πf f is the frequency t
Is a unit vector that rotates at time].

この誘導電動機6の二次磁束量φで誘起される電圧e
は e=dφ/dt =jωΦεjωt+(dφ/dt)εjωt ……(5) となる。また、この誘起電圧eは電流制御において外乱
の一つとして作用する。
The voltage e induced by the amount of secondary magnetic flux φ of the induction motor 6
Will be e = dφ / dt = jωΦε jωt + (dφ / dt) ε jωt ...... (5). Further, the induced voltage e acts as one of disturbances in the current control.

ここで、第4図に示す定出力パターン[正転では直線
21から曲線43であり、逆転では直線22から曲線44であ
る]で、誘導電動機6を停止状態[N=0]から最高回
転速度NMaxまで加速するときに、定トルク領域ではd
φ/dt=0であるため、(5)式の右辺第2項は零であ
るが、定出力領域に入った時点で最も変化が大きい。加
速中における(5)式の右辺第2項の変化を第5図
(b)[曲線5b]に示している。
Here, the constant output pattern shown in FIG.
When the induction motor 6 is accelerated from the stop state [N = 0] to the maximum rotation speed NMax in the constant torque region, the curve 43 is obtained from the curve 43 from the curve 21 and the curve 44 from the straight line 22 in the reverse rotation.
Since φ / dt = 0, the second term on the right side of the equation (5) is zero, but the change is the largest at the time when the constant output area is entered. The change of the second term on the right side of equation (5) during acceleration is shown in FIG. 5 (b) [curve 5b].

そこで本発明は、このような現象を適確に捕らえ、第
1図の回路構成図における磁束指令器3の指令二次磁束
量(指令磁束の大きさ)Φの回転速度Nについての特
性曲線図を第2図のように設定する。
Therefore, the present invention accurately captures such a phenomenon and obtains a characteristic curve of the command secondary magnetic flux amount (magnitude of the command magnetic flux) Φ * of the magnetic flux commander 3 in the circuit configuration diagram of FIG. The figure is set as shown in FIG.

従来例にみられた定出力領域での曲線43が直線23へ調
整して、ベクトル制御器2への磁束指令器3の指令磁束
の大きさΦを制御するのである。
The curve 43 in the constant output region as seen in the conventional example is adjusted to the straight line 23 to control the magnitude Φ * of the command magnetic flux of the magnetic flux commander 3 to the vector controller 2.

このように定出力領域での指令磁束の大きさΦの回
転速度Nパターンが調整されるのである。
In this manner, the rotation speed N pattern of the magnitude Φ * of the command magnetic flux in the constant output region is adjusted.

したがって、さきの誘導電動機6を停止状態[N=
0]から最高回転速度NMaxまで加速するときに、従来
と同様に、定トルク領域では磁束変化率がゼロ(dφ/d
t=0)であるため、(5)式の右辺第2項は零とな
る。そして、時間t1において定出力領域に入ると磁束変
化率はゼロでなくなるが、第3図(b)の直線3bとして
示すように、その値が一定となるため、磁束変化によっ
て誘導電動機6の電圧、電流が変化したとしても、その
振動の発生を回避することができる。また、磁束変化率
を一定にすることによって、第3図(b)からも明らか
なように、時刻t1における磁束変化率の値自体も従来よ
り小さくすることができるので、定トルク領域と定出力
領域との間での制御の移行をより円滑に行うことができ
る。
Therefore, the induction motor 6 is stopped (N =
0] to the maximum rotation speed NMax, the flux change rate is zero (dφ / d) in the constant torque region as in the conventional case.
(t = 0), the second term on the right side of the equation (5) becomes zero. Then, when entering the constant output region at time t1, the magnetic flux change rate is not zero, but its value becomes constant as shown by the straight line 3b in FIG. 3 (b). Even if the current changes, the occurrence of the vibration can be avoided. Further, by making the magnetic flux change rate constant, the value of the magnetic flux change rate at time t1 itself can be made smaller than in the conventional art, as is clear from FIG. 3 (b). The transition of the control to and from the area can be performed more smoothly.

〔発明の効果〕〔The invention's effect〕

かくして本発明によれば、誘導電動機のベクトルドラ
イブにおいて、定出力制御を行なう場合に、一般には定
出力範囲で磁束Φ(励磁電流)指令を誘導電動機の回転
速度Nに反比例(Φ∝1/N)の関数で制御していたが、
最近、要求の多い短時間での加減速で、定トルク領域か
ら定出力領域に入る時点での回転速度に振動が生じる現
象が現れ、この技術分野の大きな課題となっていたの
を、完全に払拭し、定出力制御の円滑運転に顕著な効果
を奏することができる。
Thus, according to the present invention, when performing constant output control in the vector drive of an induction motor, generally, a magnetic flux Φ (excitation current) command is inversely proportional to the rotation speed N of the induction motor (Φ∝1 / N) in a constant output range. ) Function,
Recently, the demand for acceleration and deceleration in a short time has caused a phenomenon in which the rotational speed at the point when the motor enters the constant output region from the constant torque region appears, which has been a major issue in this technical field. Wiping and a remarkable effect can be exerted on smooth operation of constant output control.

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

第1図は本発明の制御方法により誘導電動機が駆動され
る場合の制御指令系統図、第2図は本発明の一実施例に
おける指令二次磁束量(指令磁束の大きさ)Φの回転
速度Nについての特性曲線図、第3図(a),第3図
(b)はその誘導電動機の回転速度Nおよび二次磁束量
Φの時間微分のそれぞれの時間tについての特性曲線
図、第4図、第5図(a),第5図(b)は従来例の説
明図である。 1……速度制御器 2……ベクトル制御器 3……磁束指令器 4……電流形インバータ 5……交流電源 6……誘導電動機 7……速度検出器 8……演算器 N……誘導電動機回転速度(帰還速度) Nb……誘導電動機基底速度 NMax……誘導電動機最高速度。
FIG. 1 is a control command system diagram when an induction motor is driven by the control method of the present invention, and FIG. 2 is a rotation of a command secondary magnetic flux amount (magnitude of a command magnetic flux) Φ * in one embodiment of the present invention. FIG. 3 (a) and FIG. 3 (b) are characteristic curve diagrams for the speed N and the time derivative of the rotational speed N of the induction motor and the time derivative of the secondary magnetic flux amount Φ, respectively. FIG. 4, FIG. 5 (a) and FIG. 5 (b) are explanatory views of the conventional example. DESCRIPTION OF SYMBOLS 1 ... Speed controller 2 ... Vector controller 3 ... Magnetic flux commander 4 ... Current source inverter 5 ... AC power supply 6 ... Induction motor 7 ... Speed detector 8 ... Calculator N ... Induction motor Rotational speed (return speed) Nb: Induction motor base speed NMax: Induction motor maximum speed.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】誘導電動機の検出回転速度と速度指令との
偏差に基づきこの誘導電動機の2次電流を制御すると共
に、この検出回転速度の入力に基づき誘導電動機の2次
磁束量を制御し、更にこれら2次電流及び2次磁束量に
基づき1次電流の制御を行う場合に、前記2次磁束量に
対する制御領域を定トルク領域と定出力領域とに分け、
定トルク領域では前記検出回転速度の変化にかかわらず
前記2次磁束量が一定となるように磁束一定制御を行
い、定出力領域では前記検出回転速度が増加するにした
がって前記2次磁束量が減少するように磁束弱め制御を
行う誘導電動機のベクトル制御方法において、 前記2次磁束量の減少が直線的なものとなるようにし、
この2次磁束量の時間微分値が一定となるように前記定
出力領域での磁束弱め制御を行う、 ことを特徴とする誘導電動機のベクトル制御方法。
A secondary current of the induction motor is controlled based on a deviation between a detected rotation speed of the induction motor and a speed command, and a secondary magnetic flux amount of the induction motor is controlled based on an input of the detected rotation speed. Further, when controlling the primary current based on the secondary current and the secondary magnetic flux amount, the control region for the secondary magnetic flux amount is divided into a constant torque region and a constant output region,
In the constant torque region, the magnetic flux constant control is performed so that the amount of the secondary magnetic flux is constant irrespective of the change in the detected rotational speed. In the constant output region, the amount of the secondary magnetic flux decreases as the detected rotational speed increases. In the vector control method of the induction motor that performs the magnetic flux weakening control such that the decrease of the secondary magnetic flux amount becomes linear,
A vector control method for an induction motor, comprising: performing a magnetic flux weakening control in the constant output region so that a time differential value of the secondary magnetic flux amount becomes constant.
JP01307335A 1989-11-27 1989-11-27 Vector control method of induction motor Expired - Fee Related JP3106471B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP01307335A JP3106471B2 (en) 1989-11-27 1989-11-27 Vector control method of induction motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP01307335A JP3106471B2 (en) 1989-11-27 1989-11-27 Vector control method of induction motor

Publications (2)

Publication Number Publication Date
JPH03169293A JPH03169293A (en) 1991-07-22
JP3106471B2 true JP3106471B2 (en) 2000-11-06

Family

ID=17967893

Family Applications (1)

Application Number Title Priority Date Filing Date
JP01307335A Expired - Fee Related JP3106471B2 (en) 1989-11-27 1989-11-27 Vector control method of induction motor

Country Status (1)

Country Link
JP (1) JP3106471B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4730493B2 (en) * 2001-04-18 2011-07-20 株式会社安川電機 Synchronous motor controller

Also Published As

Publication number Publication date
JPH03169293A (en) 1991-07-22

Similar Documents

Publication Publication Date Title
JP3399156B2 (en) Control device for brushless DC motor
EP1729407B1 (en) Controller of permanent magnet synchronous motor
JPWO2009040884A1 (en) Electric motor control device
US20120306423A1 (en) Motor control system implementing field weakening
JP3765437B2 (en) Control system for synchronous motor for machine tool spindle drive
JP3106471B2 (en) Vector control method of induction motor
EP0616417B1 (en) Method for control of ac motor
JPH0223085A (en) Controlling method for induction motor
JP4144446B2 (en) Power converter
JP2018182938A (en) Servo motor control device and method
JP3053121B2 (en) Control method of induction motor
JPH037081A (en) Controller of rotating machine
JPH11235075A (en) Flat linear induction motor
JPH11150977A (en) Speed controller for series connected motors
JP3322088B2 (en) Induction motor control device
JP2831189B2 (en) Induction motor control device
JPH04322191A (en) Controller for synchronous motor
JPH0585470B2 (en)
JPH1118498A (en) Controller for servo motor
JPH06296386A (en) Servomotor control equipment
JPS63316687A (en) Vector controlling arithmetic device for induction motor
JPS61147787A (en) Vector control device for induction motor
JP2559197B2 (en) AC motor controller
JP6539538B2 (en) Electric car control device
JPS63140693A (en) Invertor device

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees