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JP3508982B2 - AC motor control device - Google Patents
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JP3508982B2 - AC motor control device - Google Patents

AC motor control device

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Publication number
JP3508982B2
JP3508982B2 JP36483197A JP36483197A JP3508982B2 JP 3508982 B2 JP3508982 B2 JP 3508982B2 JP 36483197 A JP36483197 A JP 36483197A JP 36483197 A JP36483197 A JP 36483197A JP 3508982 B2 JP3508982 B2 JP 3508982B2
Authority
JP
Japan
Prior art keywords
magnetic flux
voltage
motor
phase
time
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
Application number
JP36483197A
Other languages
Japanese (ja)
Other versions
JPH11187695A (en
Inventor
洋一 大森
知明 桐谷
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.)
Toyo Electric Manufacturing Ltd
Original Assignee
Toyo Electric Manufacturing 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 Toyo Electric Manufacturing Ltd filed Critical Toyo Electric Manufacturing Ltd
Priority to JP36483197A priority Critical patent/JP3508982B2/en
Publication of JPH11187695A publication Critical patent/JPH11187695A/en
Application granted granted Critical
Publication of JP3508982B2 publication Critical patent/JP3508982B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は,交流電動機を駆動
するインバータの制御に関するもので,特に始動を滑ら
かにするものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to control of an inverter for driving an AC electric motor, and particularly to smooth start.

【0002】[0002]

【従来の技術】従来の技術を図3,図4,図5に基づい
て説明をする。まず図3について説明する。第1制御装
置40は電圧指令Vcを電力変換器1に出力し,電力変
換器1は交流電動機2に指令Vc通りの電圧を印加す
る。加減速度制限器3は,角周波数指令ωcを入力し,
加減速度を制限してそれに追従するように角周波数ωm
を出力する。例えば、ωcがステップ的に変化しても出
力ωmは制限された傾きで斜めに変化するようになる。
電圧大きさ指令発生器4は,角周波数ωmを入力し例え
ばそれに比例させた電圧大きさ指令Vmを出力する。積
分器5は角周波数ωmを積分して電圧位相θvを出力す
る。ベクトル変換器は,大きさが前記電圧大きさ指令V
mで位相が前記電圧位相θvである電圧指令Vcを求め
て出力する。以上の構成で,交流電動機2は角周波数指
令ωc相当の回転数で回転することになる。
2. Description of the Related Art A conventional technique will be described with reference to FIGS. First, FIG. 3 will be described. The first control device 40 outputs a voltage command Vc to the power converter 1, and the power converter 1 applies a voltage according to the command Vc to the AC motor 2. The acceleration / deceleration limiter 3 inputs the angular frequency command ωc,
The angular frequency ωm is set so that the acceleration / deceleration is limited and the acceleration / deceleration is followed.
Is output. For example, even if ωc changes stepwise, the output ωm changes obliquely with a limited inclination.
The voltage magnitude command generator 4 receives the angular frequency ωm and outputs a voltage magnitude command Vm proportional to it, for example. The integrator 5 integrates the angular frequency ωm and outputs the voltage phase θv. The size of the vector converter is the voltage magnitude command V
A voltage command Vc whose phase is the voltage phase θv at m is obtained and output. With the above configuration, the AC motor 2 rotates at a rotation speed corresponding to the angular frequency command ωc.

【0003】次に図4について説明する。第2制御装置
41は電圧指令Vcを電力変換器1に出力し,電力変換
器1は交流電動機2に指令Vc通りの電圧を印加する。
電流検出器14は電動機2の入力電流ベクトルiを検出
し,電圧検出手段15は入力電圧ベクトルvを検出また
は推定する。磁束演算器13は,電流検出器14と電圧
検出手段15との出力より積分演算で電動機2の回転子
の磁束ベクトルφを演算し出力する。トルク演算器12
は,磁束演算器13の出力のφと電流検出器14出力の
iより,電動機2の出力トルクTを演算して出力する。
トルク磁束制御器11は,磁束演算器13の出力のφの
大きさとトルク演算器12出力のトルクTがそれらの指
令値の磁束指令φcとトルク指令Tcに追従するような
電圧指令Vcを求めて出力する。以上の構成で,交流電
動機2は磁束指令φcの大きさの磁束状態でトルク指令
Tc通りのトルクを出力するようになる。
Next, FIG. 4 will be described. The second control device 41 outputs the voltage command Vc to the power converter 1, and the power converter 1 applies a voltage according to the command Vc to the AC motor 2.
The current detector 14 detects the input current vector i of the electric motor 2, and the voltage detection means 15 detects or estimates the input voltage vector v. The magnetic flux calculator 13 calculates and outputs the magnetic flux vector φ of the rotor of the electric motor 2 by an integral calculation from the outputs of the current detector 14 and the voltage detector 15. Torque calculator 12
Calculates the output torque T of the electric motor 2 from φ of the output of the magnetic flux calculator 13 and i of the output of the current detector 14, and outputs it.
The torque magnetic flux controller 11 obtains a voltage command Vc such that the output φ of the magnetic flux calculator 13 and the torque T output from the torque calculator 12 follow the magnetic flux command φc and the torque command Tc of those command values. Output. With the above configuration, the AC motor 2 comes to output the torque according to the torque command Tc in the magnetic flux state having the magnitude of the magnetic flux command φc.

【0004】最後に図5について説明する。第3制御装
置42は電圧指令Vcを電力変換器1に出力し,電力変
換器1は交流電動機2に指令Vc通りの電圧を印加す
る。電流指令変換器21は,トルク指令Tcと磁束指令
φcに相当する電流指令ベクトルicを出力する。周波
数指令変換器26はトルク指令Tcと磁束指令φcと速
度検出器27の出力の電動機2の回転角周波数ωrとを
入力して回転子磁束の回転角周波数指令ωc を出力す
る。積分器25は,回転子磁束の回転角周波数指令ωc
を時間積分して,回転子磁束の位相θを求める。周波数
指令変換器26と積分器25が磁束の位相を求める位相
演算手段28となる。回転座標変換24は,電流検出器
14の出力のiを回転子磁束の位相θの逆位相で回転座
標変換をして磁束と同期した座標上の電流ベクトルix
を出力する。電流制御器22は,電流指令ベクトルic
にixが追従するような電圧指令ベクトルVxを求めて
出力する。回転座標変換23は,回転子磁束の位相θで
Vxを回転座標変換して静止座標上の電圧指令ベクトル
Vcを出力する。以上の構成で,交流電動機2は磁束指
令φcの大きさの磁束状態でトルク指令Tc通りのトル
クを出力するようになる。
Finally, FIG. 5 will be described. The third control device 42 outputs a voltage command Vc to the power converter 1, and the power converter 1 applies a voltage according to the command Vc to the AC motor 2. The current command converter 21 outputs a current command vector ic corresponding to the torque command Tc and the magnetic flux command φc. The frequency command converter 26 inputs the torque command Tc, the magnetic flux command φc, and the rotational angular frequency ωr of the motor 2 which is the output of the speed detector 27, and outputs the rotational angular frequency command ωc of the rotor magnetic flux. The integrator 25 determines the rotation angular frequency command ωc of the rotor magnetic flux.
Is integrated over time to find the phase θ of the rotor magnetic flux. The frequency command converter 26 and the integrator 25 serve as the phase calculating means 28 for obtaining the phase of the magnetic flux. The rotational coordinate transformation 24 performs rotational coordinate transformation on the output i of the current detector 14 at the opposite phase of the phase θ of the rotor magnetic flux to obtain a current vector ix on the coordinate synchronized with the magnetic flux.
Is output. The current controller 22 uses the current command vector ic
To obtain and output a voltage command vector Vx such that ix follows. The rotational coordinate conversion 23 performs rotational coordinate conversion of Vx with the phase θ of the rotor magnetic flux and outputs a voltage command vector Vc on stationary coordinates. With the above configuration, the AC motor 2 comes to output the torque according to the torque command Tc in the magnetic flux state having the magnitude of the magnetic flux command φc.

【0005】[0005]

【発明が解決しようとする課題】図3における従来技術
では,加減速制限器3や積分器5を具備しており,これ
らはその性質上それぞれの初期値ω0とθ0を必要とす
る。しかしそれらの初期値を得ることが困難なため,ω
0=θ0=0としている。よって第1制御装置の始動時
点においては,角周波数ωmは必ず初期値ω0の値の0
の値から立ち上がることになる。もし電動機2が回転し
ている状態での始動においても角周波数ωmは0から立
ち上がるので,電動機2が誘導電動機の場合はωm相当
まで急減速から再度加速することになり危険である。ま
た電動機2が同期電動機の場合は,同期状態とならず脱
調状態となってしまう。また電圧位相θvの初期値にお
いても磁束の位相に合った電圧位相と必ずしもならない
ので過電流となる可能性がある。
In the prior art shown in FIG. 3, the acceleration / deceleration limiter 3 and the integrator 5 are provided, and these require their respective initial values ω0 and θ0. However, since it is difficult to obtain those initial values, ω
0 = θ0 = 0. Therefore, at the time of starting the first control device, the angular frequency ωm must be 0, which is the initial value ω0.
It will rise from the value of. If the electric motor 2 is an induction motor, the angular frequency ωm rises from 0 even when the electric motor 2 is started in a rotating state. Therefore, if the electric motor 2 is an induction motor, it is dangerous to accelerate from deceleration to ωm again. If the electric motor 2 is a synchronous electric motor, it will not be in a synchronous state and will be in a step-out state. Further, the initial value of the voltage phase θv does not always have a voltage phase that matches the phase of the magnetic flux, which may cause an overcurrent.

【0006】図4における従来技術では,磁束演算器1
3を具備しており,これは前述したように積分演算で磁
束を求めているので磁束の大きさの初期値φ0と磁束の
位相θ0を必要とする。しかしその初期値を得ることが
困難なため,φ0=0としている。しかし電動機2が同
期電動機の場合は,回転子の磁束は必ず存在するし,電
動機2が誘導電動機の場合でも残留磁束が存在すること
がある。よって磁束演算の初期値を間違うことになるの
で,間違った磁束演算をすることになり,それによって
トルクを演算しているので,トルク指令通りの出力トル
クが得られないことになる。
In the prior art shown in FIG. 4, the magnetic flux calculator 1
3, which requires the initial value φ0 of the magnitude of the magnetic flux and the phase θ0 of the magnetic flux because the magnetic flux is obtained by the integral calculation as described above. However, since it is difficult to obtain the initial value, φ0 = 0 is set. However, when the electric motor 2 is a synchronous electric motor, the magnetic flux of the rotor always exists, and even when the electric motor 2 is an induction motor, residual magnetic flux may exist. Therefore, since the initial value of the magnetic flux calculation is incorrect, an incorrect magnetic flux calculation is performed, and the torque is calculated accordingly, so that the output torque according to the torque command cannot be obtained.

【0007】図5における従来技術では,位相演算手段
28の中の積分器25を具備しており,初期値θ0を必
要とする。しかしその初期値を得ることが困難なため,
θ0=0としている。しかし回転子の磁束の位相が0か
ら始まることは希であるため位相演算手段28の出力の
磁束位相θは誤差を含むようになる。よって,トルク指
令通りの出力トルクが得られないことになる。本発明は
上述した点に鑑みて創案されたもので,その目的とする
ところは,各種制御装置内の初期値を提供し,問題のな
い制御装置の始動を可能とすることにある。
In the prior art shown in FIG. 5, the integrator 25 in the phase calculating means 28 is provided and an initial value θ0 is required. However, since it is difficult to obtain the initial value,
θ0 = 0. However, since the phase of the magnetic flux of the rotor rarely starts from 0, the magnetic flux phase θ of the output of the phase calculation means 28 includes an error. Therefore, the output torque according to the torque command cannot be obtained. The present invention has been made in view of the above-mentioned points, and an object thereof is to provide initial values in various control devices and enable the control device to be started without problems.

【0008】[0008]

【課題を解決するための手段】上述の問題点を解決する
ために本発明は,請求項1において,交流電動機に電力
を供給し始めてからの微少時間は,前記電動機の入力電
流が零またはそれに近い値となるように前記電力変換器
を制御する微少電流制御手段と,前記微少期間において
前記電動機の入力の電圧ベクトルを検出または推定する
電圧検出手段と,前記電圧検出手段の出力の電圧ベクト
ルより前記電動機の回転子の磁束の大きさと位相と回転
角周波数を推定演算する第1磁束推定手段とを具備し,
前記第1磁束推定手段の出力を、前記交流電動機制御装
置内で前記交流電動機の状態変数を演算又は出力する数
値の初期値とする。
In order to solve the above-mentioned problems, according to the present invention, in claim 1, the input current of the electric motor is zero or therefor during a minute time after the electric power is supplied to the AC electric motor. A minute current control means for controlling the power converter so as to have a close value, a voltage detection means for detecting or estimating the voltage vector of the input of the electric motor in the minute period, and a voltage vector of the output of the voltage detection means. A first magnetic flux estimating means for estimating and calculating the magnitude and phase of the magnetic flux of the rotor of the electric motor and the rotational angular frequency;
The output of the first magnetic flux estimating means is an initial value of a numerical value for calculating or outputting the state variable of the AC electric motor in the AC electric motor control device.

【0009】また請求項2において,交流電動機に電力
を供給し始めてからの微少時間は,前記電動機の入力電
流が零またはそれに近い値となるように前記電力変換器
を制御する微少電流制御手段と,前記微少期間において
前記電圧検出手段の出力の電圧ベクトルを時間積分演算
する電圧積分手段と,前記電圧積分手段の出力の電圧積
分ベクトルより前記電動機の回転子の磁束の大きさと位
相と回転角周波数を推定演算する第2磁束推定手段とを
具備し,前記第2磁束推定手段の出力を、前記交流電動
機制御装置内で前記交流電動機の状態変数を演算又は出
力する数値の初期値とする。
According to a second aspect of the present invention, there is provided a minute current control means for controlling the power converter so that an input current of the motor becomes zero or a value close to that during a minute time after the power is supplied to the AC motor. , A voltage integration means for time-integrating the voltage vector of the output of the voltage detection means in the minute period, and the magnitude and phase of the magnetic flux of the rotor of the electric motor and the rotation angular frequency from the voltage integration vector of the output of the voltage integration means. And a second magnetic flux estimating means for estimating and calculating, and an output of the second magnetic flux estimating means is an initial value of a numerical value for calculating or outputting a state variable of the alternating current motor in the alternating current motor control device.

【0010】また請求項3において,前記電動機の入力
電流が零またはそれに近い微少の大きさの直流となるよ
うに前記電力変換器を制御する微少電流制御手段を具備
する。
In the third aspect of the invention, there is provided a minute current control means for controlling the power converter so that the input current of the electric motor becomes zero or a minute magnitude of direct current close to zero.

【0011】請求項4において,前記第1磁束推定手段
または第2磁束推定手段の出力を,前記微少時間直後に
前記電動機に印加する電圧の周波数と位相の初期値とす
ることを特徴とする。
According to a fourth aspect of the present invention, the output of the first magnetic flux estimating means or the second magnetic flux estimating means is an initial value of the frequency and phase of the voltage applied to the electric motor immediately after the minute time.

【0012】請求項5において,前記電動機の回転子の
磁束を演算する磁束演算手段を具備し,前記磁束演算手
段の初期値として前記第1磁束推定手段または第2磁束
推定手段の出力を前記微少時間直後に用いることを特徴
とする。
According to a fifth aspect of the present invention, magnetic flux calculating means for calculating magnetic flux of the rotor of the electric motor is provided, and the output of the first magnetic flux estimating means or the second magnetic flux estimating means is used as an initial value of the magnetic flux calculating means. The feature is that it is used immediately after the time.

【0013】請求項6において,前記電動機のトルク指
令と磁束指令とに基づいて磁束の周波数指令を作り,該
周波数指令を積分することにより前記回転子の磁束の位
相を求める位相演算手段を具備し,前記位相演算手段の
初期値として前記第1磁束推定手段または第2磁束推定
手段の出力の磁束の位相を前記微少時間直後に用いるこ
とを特徴とする。
According to a sixth aspect of the present invention, there is provided a phase calculation means for generating a frequency command of the magnetic flux based on the torque command and the magnetic flux command of the electric motor and integrating the frequency command to obtain the phase of the magnetic flux of the rotor. The phase of the magnetic flux output from the first magnetic flux estimating means or the second magnetic flux estimating means is used immediately after the minute time as an initial value of the phase calculating means.

【0014】請求項7において,前記微少期間内の任意
の2つの時点の前記電圧検出手段の出力の電圧ベクトル
をV1,V2とし,V1とV2の位相差を前記V1検出
時点からV2検出時点までの経過時間で除することによ
り二次側の磁束の回転角周波数を求め,V1またはV2
の大きさ,またはV1とV2の大きさの平均値を前記回
転角周波数で除することにより回転子の磁束の大きさを
求め,V2の位相より90度だけ前記回転角周波数と逆
の方向に回転させた位相をV2の時点の回転子の磁束の
位相とする第1磁束推定手段を具備する。
According to a seventh aspect of the present invention, the voltage vector of the output of the voltage detecting means at any two points within the minute period is V1, V2, and the phase difference between V1 and V2 is from the V1 detecting point to the V2 detecting point. The rotational angular frequency of the magnetic flux on the secondary side is obtained by dividing by the elapsed time of
Or the average value of V1 and V2 is divided by the rotation angular frequency to obtain the magnitude of the magnetic flux of the rotor, and in the direction opposite to the rotation angular frequency by 90 degrees from the phase of V2. There is provided a first magnetic flux estimating means for making the rotated phase the phase of the magnetic flux of the rotor at the time of V2.

【0015】請求項8において,前記微少期間内の任意
の3つの時点の前記電圧積分手段の出力の電圧積分ベク
トルをF1,F2,F3とし,F1,F2,F3を通る
円の中心F0を求め,F1−F0とF3−F0との位相
差をF1検出時点からF3検出時点までの時間で除する
ことにより回転子の磁束の回転角周波数を求め,F3−
F0の位相をF3検出時点の回転子の磁束の位相とし,
F3−F0の大きさをF3検出時点の回転子の磁束の大
きさとする第2磁束推定手段を具備する。
In claim 8, the voltage integration vector of the output of the voltage integrating means at any three points within the minute period is F1, F2, F3, and the center F0 of the circle passing through F1, F2, F3 is obtained. , F1-F0 and F3-F0 are divided by the time from the F1 detection time to the F3 detection time to obtain the rotational angular frequency of the magnetic flux of the rotor, and F3-
Let the phase of F0 be the phase of the magnetic flux of the rotor at the time of detecting F3,
A second magnetic flux estimating means for setting the magnitude of F3-F0 to the magnitude of the magnetic flux of the rotor at the time of detecting F3 is provided.

【0016】[0016]

【発明の実施の形態】図1,図2に発明の実施例を示
し,これらの図に従って説明する。図1において,始動
関連信号発生器55は始動ONで1となり始動OFFで
0となる電力変換器始動信号S0と,始動ON後の微少
時間だけ1となる微少時間信号S1と始動ON後の微少
時間経過後に1となる制御器始動信号S2を出力する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Embodiments of the invention are shown in FIGS. 1 and 2 and will be described with reference to these drawings. In FIG. 1, the start-related signal generator 55 has a power converter start signal S0 that is 1 when the start is ON and 0 when the start is OFF, a minute time signal S1 that is 1 only for a minute time after the start is ON, and a minute signal after the start is ON. After the lapse of time, the controller start signal S2 which becomes 1 is output.

【0017】電力変換器1は前記電力変換器始動信号S
0が1となっている状態の時に交流電動機2に指令Vc
通りの電圧を印加する。スイッチ54は,前記微少時間
信号S1が0の時は,第1制御装置40または第2制御
装置41または第3制御装置42の出力の電圧指令Vc
1を選択しVc0として電力変換器1に出力する。一方
前記微少時間信号S1が1の時は,微少電流制御手段5
1の出力の電圧指令Vc2を選択しVc0として電力変
換器1に出力する。
The power converter 1 uses the power converter start signal S.
The command Vc is issued to the AC motor 2 when 0 is 1.
Apply the street voltage. When the minute time signal S1 is 0, the switch 54 outputs the voltage command Vc of the output of the first controller 40, the second controller 41, or the third controller 42.
1 is selected and output to the power converter 1 as Vc0. On the other hand, when the minute time signal S1 is 1, the minute current control means 5
The output voltage command Vc2 of 1 is selected and output to the power converter 1 as Vc0.

【0018】微少電流制御手段51は,電流検出器14
の出力の電動機2の入力電流ベクトルiが零またはそれ
に近い微少の大きさの直流となるような電圧指令Vc2
を出力する。
The minute current control means 51 includes a current detector 14
Voltage command Vc2 such that the input current vector i of the electric motor 2 of the output of 0 is a DC with a small magnitude of zero or close thereto.
Is output.

【0019】第1磁束推定手段53は,前記微少時間信
号S1が1の時の任意の2つの時点において電圧検出手
段15の出力の電圧ベクトルvを入力し,それらをV
1,V2とし,V1とV2の位相差をV1検出時点から
V2検出時点までの経過時間で除することにより回転子
の磁束の回転角周波数ω0を求め,V1またはV2の大
きさ,またはV1とV2の大きさの平均値を前記回転角
周波数で除することにより回転子の磁束の大きさφ0を
求め,V2の位相より90度だけ前記回転角周波数と逆
の方向に回転させた位相θ0を求め,前記ω0,φ0,
θ0を出力する。
The first magnetic flux estimating means 53 inputs the voltage vector v of the output of the voltage detecting means 15 at any two time points when the minute time signal S1 is 1, and outputs them as V
1, V2 and the phase difference between V1 and V2 is divided by the elapsed time from the V1 detection time to the V2 detection time to obtain the rotational angular frequency ω0 of the magnetic flux of the rotor, and the magnitude of V1 or V2 or V1 The magnitude φ0 of the magnetic flux of the rotor is obtained by dividing the average value of the magnitudes of V2 by the rotation angular frequency, and the phase θ0 rotated by 90 degrees in the direction opposite to the rotation angular frequency from the phase of V2 is obtained. Ω0, φ0,
Outputs θ0.

【0020】第1制御装置40は,前記制御器始動信号
S2が1になった時に,第1磁束推定手段の出力のω0
を図3における加減速度制限器3の初期値とし,第1磁
束推定手段の出力のθ0から90度位相を進ませた値を
図3における積分器5の初期値とする。
When the controller start signal S2 becomes 1, the first control device 40 outputs ω0 of the output of the first magnetic flux estimating means.
Is the initial value of the acceleration / deceleration limiter 3 in FIG. 3, and the value obtained by advancing the phase of 90 ° from the output of the first magnetic flux estimating means is the initial value of the integrator 5 in FIG.

【0021】第2制御装置41は,前記制御器始動信号
S2が1になった時に,第1磁束推定手段の出力のφ
0,θ0を図4における磁束演算器13の初期値とす
る。
The second control device 41 outputs the output φ of the first magnetic flux estimating means when the controller start signal S2 becomes 1.
0 and θ0 are initial values of the magnetic flux calculator 13 in FIG.

【0022】第3制御装置42は,前記制御器始動信号
S2が1になった時に,第1磁束推定手段の出力のθ0
を図5における積分器25の初期値とする。
When the controller start signal S2 becomes 1, the third controller 42 outputs θ0 of the output of the first magnetic flux estimating means.
Is the initial value of the integrator 25 in FIG.

【0023】図2においては,図1と同一部分の説明は
省略する。電圧積分手段56は,電圧検出手段15の出
力の電圧ベクトルvを入力して時間積分して電圧積分ベ
クトルFとして出力する。
In FIG. 2, description of the same parts as in FIG. 1 will be omitted. The voltage integration means 56 inputs the voltage vector v of the output of the voltage detection means 15, integrates it over time, and outputs it as a voltage integration vector F.

【0024】第2磁束推定手段57は,前記微少時間信
号S1が1の時の任意の3つの時点において前記電圧積
分手段56の出力の電圧積分ベクトルFを入力し,それ
らをF1,F2,F3とし,F1,F2,F3を通る円
の中心F0を求め,F1−F0とF3−F0との位相差
をF1検出時点からF3検出時点までの時間で除するこ
とにより回転子の磁束の回転角周波数ω0を求め,F3
−F0の位相をF3検出時点の回転子の磁束の位相θ0
とし,F3−F0の大きさをF3検出時点の回転子の磁
束の大きさφ0として出力する。
The second magnetic flux estimating means 57 inputs the voltage integration vector F of the output of the voltage integrating means 56 at any three points when the minute time signal S1 is 1, and inputs them to F1, F2 and F3. Then, the center F0 of the circle passing through F1, F2, and F3 is obtained, and the phase difference between F1-F0 and F3-F0 is divided by the time from the F1 detection time to the F3 detection time to determine the rotation angle of the magnetic flux of the rotor. Find the frequency ω0, F3
-The phase of F0 is the phase θ0 of the magnetic flux of the rotor at the time of detecting F3.
Then, the magnitude of F3−F0 is output as the magnitude φ0 of the magnetic flux of the rotor at the time of detecting F3.

【0025】第1制御装置40は,前記制御器始動信号
S2が1になった時に,第2磁束推定手段の出力のω0
を図3における加減速度制限器3の初期値とし,第2磁
束推定手段の出力のθ0から90度位相を進ませた値を
図3における積分器5の初期値とする。
When the controller start signal S2 becomes 1, the first controller 40 outputs ω0 of the output of the second magnetic flux estimating means.
Is the initial value of the acceleration / deceleration limiter 3 in FIG. 3, and the value obtained by advancing the phase of θ0 of the output of the second magnetic flux estimating means by 90 degrees is the initial value of the integrator 5 in FIG.

【0026】第2制御装置41は,前記制御器始動信号
S2が1になった時に,第2磁束推定手段の出力のφ
0,θ0を図4における磁束演算器13の初期値とす
る。
When the controller start signal S2 becomes 1, the second control unit 41 outputs the output φ of the second magnetic flux estimating means.
0 and θ0 are initial values of the magnetic flux calculator 13 in FIG.

【0027】第3制御装置42は,前記制御器始動信号
S2が1になった時に,第2磁束推定手段の出力のθ0
を図5における積分器25の初期値とする。
The third control device 42 outputs θ0 of the output of the second magnetic flux estimating means when the controller starting signal S2 becomes 1.
Is the initial value of the integrator 25 in FIG.

【0028】以下では,第1磁束推定手段53と第2磁
束推定手段57において磁束の大きさと位相と回転角周
波数が求めることができる理由を述べる。交流電動機は
一般的に v=R1・i+L・P(i)+P(φx) (1) で表される。ここでR1は一次の巻線抵抗,Lは漏れイ
ンダクタンス,vは入力電圧ベクトル,iは入力電流ベ
クトル,φxは二次磁束ベクトル,P()は時間微分を
表す。微少電流制御手段53で入力電流ベクトルiは,
零またはそれに近い微少の大きさの直流となるので,式
(1)の右辺の第1項と第2項は無視できる。また二次
磁束ベクトルがω0の角周波数で回転しているとする
と,φx=φ0・EXP(j・ω0・t)と表すことが
できる。ここでφ0は二次磁束ベクトルの大きさ,EX
P()は指数関数を表し,tは時間,jは虚数単位を表
している。すると式(1)は,φ0が一定ならば v=j・ω0・φ0・EXP(j・ω0・t) (2) と書き直すことができる。式(2)より,入力電圧ベク
トルvは,二次磁束ベクトルより90度位相が進んでお
り,その大きさはω0・φ0であり,その回転角周波数
はω0となることが分かる。よって第1磁束推定手段5
3の方法で,φ0,ω0,θ0を求めることが可能とな
る。
The reason why the magnitude and phase of the magnetic flux and the rotational angular frequency can be obtained by the first magnetic flux estimating means 53 and the second magnetic flux estimating means 57 will be described below. The AC motor is generally represented by v = R1 · i + L · P (i) + P (φx) (1). Here, R1 is the primary winding resistance, L is the leakage inductance, v is the input voltage vector, i is the input current vector, φx is the secondary magnetic flux vector, and P () is the time derivative. The input current vector i in the minute current control means 53 is
Since the direct current is zero or a very small value close to zero, the first and second terms on the right side of the equation (1) can be ignored. If the secondary magnetic flux vector rotates at an angular frequency of ω0, then φx = φ0 · EXP (j · ω0 · t) can be expressed. Where φ0 is the magnitude of the secondary magnetic flux vector, EX
P () represents an exponential function, t represents time, and j represents an imaginary unit. Then, equation (1) can be rewritten as v = j · ω0 · φ0 · EXP (j · ω0 · t) (2) if φ0 is constant. From equation (2), it can be seen that the input voltage vector v has a 90 ° phase advance from the secondary magnetic flux vector, its magnitude is ω0 · φ0, and its rotational angular frequency is ω0. Therefore, the first magnetic flux estimating means 5
By the method of 3, it is possible to obtain φ0, ω0, θ0.

【0029】前記と同様の理由により式(1)の第1項
と第2項を無視して両辺を積分すると, 積分(v)=φ0・EXP(j・ω0・t)+F0 (3) となる。積分(v)は,入力電圧ベクトルvを時間積分
することであり,電圧積分手段56の出力の電圧積分ベ
クトルFと同じものである。F0は積分の初期値であ
る。式(3)より,電圧積分ベクトルFは,中心がF0
で大きさがφ0で角周波数ω0で回転するベクトルとな
ることが分かる。よって第2磁束推定手段57の前記3
つの電圧積分ベクトルF1,F2,F3はF0を中心と
した円を通ることになり,第2磁束推定手段57の方法
で,φ0,ω0,θ0を求めることが可能となることが
分かる。
For the same reason as above, ignoring the first term and the second term of the equation (1) and integrating both sides, integration (v) = φ0 · EXP (j · ω0 · t) + F0 (3) Become. The integration (v) is to integrate the input voltage vector v with time, and is the same as the voltage integration vector F of the output of the voltage integration means 56. F0 is the initial value of integration. From the equation (3), the voltage integration vector F has a center F0.
It can be seen that the vector has a magnitude of φ0 and rotates at an angular frequency of ω0. Therefore, the 3 of the second magnetic flux estimating means 57
It is understood that the two voltage integration vectors F1, F2, F3 pass through a circle centered on F0, and φ0, ω0, θ0 can be obtained by the method of the second magnetic flux estimating means 57.

【0030】[0030]

【発明の効果】本発明により,交流電動機制御装置内の
数値の初期値を適切な値に設定する事ができるので,制
御装置の始動直後における急減速や過電流や制御精度悪
化などの様々な過渡現象を抑制することができる。
According to the present invention, the initial value of the numerical value in the AC motor control device can be set to an appropriate value, so that there are various problems such as sudden deceleration immediately after the control device is started, overcurrent and deterioration of control accuracy. The transient phenomenon can be suppressed.

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

【図1】本発明の1つの実施例である。FIG. 1 is one embodiment of the present invention.

【図2】本発明のもう1つの実施例である。FIG. 2 is another embodiment of the present invention.

【図3】従来技術の1例である。FIG. 3 is an example of a conventional technique.

【図4】第2番目の従来技術の例である。FIG. 4 is a second prior art example.

【図5】第3番目の従来技術の例である。FIG. 5 is a third prior art example.

【符号の説明】[Explanation of symbols]

1 電力変換器 2 交流電動機 3 加減速度制限器 4 電圧大きさ指令発生器 5 積分器 6 ベクトル変換器 11 トルク磁束制御器 12 トルク演算器 13 磁束演算器 14 電流検出器 15 電圧検出手段 21 電流指令変換器 22 電流制御器 23 回転座標変換器 24 回転座標変換器 25 積分器 26 周波数指令演算器 27 速度検出器 28 位相演算手段 40 第1制御装置 42 第2制御装置 43 第3制御装置 51 微少電流制御手段 53 第1磁束推定手段 54 スイッチ 55 始動関連信号発生器 56 電圧積分手段 57 第2磁束推定手段 1 power converter 2 AC motor 3 Acceleration / deceleration limiter 4 Voltage magnitude command generator 5 integrator 6 Vector converter 11 Torque flux controller 12 Torque calculator 13 Magnetic flux calculator 14 Current detector 15 Voltage detection means 21 Current command converter 22 Current controller 23 Rotational coordinate converter 24 rotary coordinate converter 25 integrator 26 Frequency command calculator 27 Speed detector 28 Phase calculation means 40 First control device 42 Second control device 43 Third control device 51 Micro current control means 53 First magnetic flux estimating means 54 switch 55 Start-related signal generator 56 voltage integrating means 57 Second magnetic flux estimating means

Claims (4)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 誘導電動機や同期電動機等の交流電動機
に電力を供給する電力変換器を制御する交流電動機制御
装置において,前記交流電動機に電力を供給し始めてか
らの微少時間は,前記交流電動機の入力電流が零となる
ように前記電力変換器を制御する微少電流制御手段と,
前記微少期間において前記交流電動機の入力の電圧ベク
トルを検出または推定する電圧検出手段と,前記電圧検
出手段の出力の電圧ベクトルより前記電動機の回転子の
磁束の大きさと位相と回転角周波数を推定演算する第1
磁束推定手段を具備する事を特徴とする交流電動機制御
装置。
1. An AC motor control device for controlling an electric power converter for supplying electric power to an AC motor such as an induction motor or a synchronous motor, wherein a minute time after starting to supply electric power to the AC motor is A minute current control means for controlling the power converter so that the input current becomes zero,
Voltage detection means for detecting or estimating the input voltage vector of the AC motor in the minute period, and the calculation of the magnitude and phase of the magnetic flux of the rotor of the motor and the rotation angular frequency from the voltage vector of the output of the voltage detection means. First to do
An AC motor control device comprising a magnetic flux estimating means.
【請求項2】 誘導電動機や同期電動機等の交流電動機
に電力を供給する電力変換器を制御する交流電動機制御
装置において,前記交流電動機に電力を供給し始めてか
らの微少時間は,前記交流電動機の入力電流が零となる
ように前記電力変換器を制御する微少電流制御手段と,
前記微少期間において前記電圧検出手段の出力の電圧ベ
クトルを時間積分演算する電圧積分手段と,該電圧積分
手段の出力の電圧積分ベクトルより前記交流電動機の回
転子の磁束の大きさと位相と回転角周波数を推定演算す
る第2磁束推定手段とを具備する事を特徴とする交流電
動機制御装置。
2. An AC motor control device for controlling a power converter that supplies power to an AC motor such as an induction motor or a synchronous motor, wherein a minute time after starting to supply power to the AC motor is A minute current control means for controlling the power converter so that the input current becomes zero,
The voltage integrating means for time-integrating the voltage vector of the output of the voltage detecting means in the minute period, and the magnitude and phase of the magnetic flux of the rotor of the AC motor and the rotational angular frequency from the voltage integrating vector of the output of the voltage integrating means. And a second magnetic flux estimating means for estimating and calculating.
【請求項3】 前記微少期間内の任意の2つの時点の前
記電圧検出手段の出力の電圧ベクトルをV1,V2と
し,V1とV2の位相差を前記V1検出時点からV2検
出時点までの経過時間で除することにより二次側の磁束
の回転角周波数を求め,V1またはV2の大きさ,また
はV1とV2の大きさの平均値を前記回転角周波数で除
することにより回転子の磁束の大きさを求め,V2の位
相より90度だけ前記回転角周波数と逆の方向に回転さ
せた位相をV2の時点の回転子の磁束の位相とする第1
磁束推定手段を具備することを特徴とする請求項1記載
の交流電動機制御装置。
3. The voltage vector of the output of the voltage detecting means at any two points in the minute period is V1, V2, and the phase difference between V1 and V2 is the elapsed time from the V1 detecting point to the V2 detecting point. The rotational angular frequency of the secondary side magnetic flux is obtained by dividing by, and the magnitude of V1 or V2, or the average value of the magnitudes of V1 and V2 is divided by the rotational angular frequency to determine the magnitude of the magnetic flux of the rotor. First, the phase is obtained by rotating the magnetic flux of the rotor at the time of V2 by determining the phase and rotating the phase by 90 degrees in the direction opposite to the rotational angular frequency from the phase of V2.
The AC motor control device according to claim 1, further comprising a magnetic flux estimating means.
【請求項4】 前記微少期間内の任意の3つの時点の前
記電圧積分手段の出力の電圧積分ベクトルをF1,F
2,F3とし,F1,F2,F3を通る円の中心F0を
求め,F1−F0とF3−F0との位相差をF1検出時
点からF3検出時点までの時間で除することにより回転
子の磁束の回転角周波数を求め,F3−F0の位相をF
3検出時点の回転子の磁束の位相とし,F3−F0の大
きさをF3検出時点の回転子の磁束の大きさとする第2
磁束推定手段を具備することを特徴とする請求項2記載
の交流電動機制御装置。
4. The voltage integration vectors of the outputs of the voltage integration means at arbitrary three points in the minute period are F1, F.
2, F3, the center F0 of the circle passing through F1, F2, and F3 is obtained, and the phase difference between F1-F0 and F3-F0 is divided by the time from the F1 detection time to the F3 detection time to determine the magnetic flux of the rotor. The rotation angular frequency of is calculated, and the phase of F3-F0 is F
The phase of the magnetic flux of the rotor at the time of 3 detection, and the magnitude of F3-F0 is the magnitude of the magnetic flux of the rotor at the time of F3 detection.
The AC motor control device according to claim 2, further comprising a magnetic flux estimating means.
JP36483197A 1997-12-22 1997-12-22 AC motor control device Expired - Lifetime JP3508982B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP36483197A JP3508982B2 (en) 1997-12-22 1997-12-22 AC motor control device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP36483197A JP3508982B2 (en) 1997-12-22 1997-12-22 AC motor control device

Publications (2)

Publication Number Publication Date
JPH11187695A JPH11187695A (en) 1999-07-09
JP3508982B2 true JP3508982B2 (en) 2004-03-22

Family

ID=18482772

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Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP3508982B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11223313B2 (en) 2016-09-05 2022-01-11 Toshiba Infrastructure Systems & Solutions Corporation Inverter control device and motor drive system

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000156497A (en) * 1998-11-20 2000-06-06 Toshiba Corp Method for manufacturing semiconductor device
JP4777051B2 (en) * 2005-11-22 2011-09-21 三菱電機株式会社 AC motor control device
US9281772B2 (en) * 2014-06-26 2016-03-08 Toshiba Mitsubishi-Electric Industrial Systems Corporation Controller for power converter

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11223313B2 (en) 2016-09-05 2022-01-11 Toshiba Infrastructure Systems & Solutions Corporation Inverter control device and motor drive system

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