JPWO2012153794A1 - Position sensorless control device for permanent magnet synchronous motor - Google Patents

Position sensorless control device for permanent magnet synchronous motor Download PDF

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JPWO2012153794A1
JPWO2012153794A1 JP2013514047A JP2013514047A JPWO2012153794A1 JP WO2012153794 A1 JPWO2012153794 A1 JP WO2012153794A1 JP 2013514047 A JP2013514047 A JP 2013514047A JP 2013514047 A JP2013514047 A JP 2013514047A JP WO2012153794 A1 JPWO2012153794 A1 JP WO2012153794A1
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山本 康弘
康弘 山本
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P27/00Arrangements or methods for the control of AC motors characterised by the kind of supply voltage
    • H02P27/04Arrangements or methods for the control of AC motors characterised by the kind of supply voltage using variable-frequency supply voltage, e.g. inverter or converter supply voltage
    • H02P27/06Arrangements or methods for the control of AC motors characterised by the kind of supply voltage using variable-frequency supply voltage, e.g. inverter or converter supply voltage using dc to ac converters or inverters
    • H02P27/08Arrangements or methods for the control of AC motors characterised by the kind of supply voltage using variable-frequency supply voltage, e.g. inverter or converter supply voltage using dc to ac converters or inverters with pulse width modulation
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P21/00Arrangements or methods for the control of electric machines by vector control, e.g. by control of field orientation
    • H02P21/14Estimation or adaptation of machine parameters, e.g. flux, current or voltage
    • H02P21/18Estimation of position or speed
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P21/00Arrangements or methods for the control of electric machines by vector control, e.g. by control of field orientation
    • H02P21/24Vector control not involving the use of rotor position or rotor speed sensors
    • H02P21/26Rotor flux based control

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  • Control Of Ac Motors In General (AREA)
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Abstract

基本波電流検出部8はPWM制御の零電圧ベクトル期間V7またはV0における電流を検出する。電流変化分検出部11は電流検出値から電流微分に相当する実電流の電流差分を演算する。電流差分成分演算部12は、電流検出値とモータ抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ω*より起電力を演算し、インダクタンスLと電流差分の時間差ΔTpを利用してその電圧成分により生じる電流差分成分に変換する。補正角周波数指令演算部13〜15は、実電流の電流差分と電流差分成分を加算し、フィルタと補正ゲインを乗算し、角周波数指令成分を除算することに近似した角周波数重み関数Kωを乗じることにより補正角周波数Δωp*を演算する。The fundamental wave current detector 8 detects a current in the zero voltage vector period V7 or V0 of PWM control. The current change detection unit 11 calculates the current difference of the actual current corresponding to the current differentiation from the detected current value. The current difference component calculation unit 12 calculates an electromotive force from the current detection value, the voltage drop due to the motor resistance R, the inductance L, and the angular frequency command ω *, and uses the time difference ΔTp between the inductance L and the current difference to generate the voltage component. The current difference component generated by The corrected angular frequency command calculation units 13 to 15 add the current difference and the current difference component of the actual current, multiply the filter by the correction gain, and multiply by the angular frequency weighting function Kω approximated to dividing the angular frequency command component. Thus, the correction angular frequency Δωp * is calculated.

Description

本発明は、永久磁石を界磁源とする同期電動機(以下、PMモータ)の位置センサレス制御装置に係り、特に磁気的に突極性のないPMモータを電流引込法で始動制御するときのモータ速度の振動抑制に関する。   The present invention relates to a position sensorless control device for a synchronous motor (hereinafter referred to as PM motor) using a permanent magnet as a field source, and in particular, a motor speed when starting control of a PM motor having no magnetic saliency by a current drawing method. Related to vibration suppression.

PMモータの界磁磁石を配置する構造には、界磁鉄心の表面に磁石を張り付ける構造(SPMSM:Surface Permanent Magnet Synchronous Motor)と鉄心内部に埋め込む構造(IPMSM:Interior Permanent Magnet Synchronous Motor)とに大別することができる。   The structure for arranging the field magnet of the PM motor includes a structure in which a magnet is attached to the surface of the field core (SPMSM: Surface Permanent Synchronous Motor) and a structure in which the magnet is embedded in the core (IPMSM: Interior Permanent Magnet). It can be divided roughly.

永久磁石同期機では、永久磁石の比透磁率が約1程度と低いため、SPM構造とIPM構造では特性が異なる。一般的には、SPM構造ではd軸インダクタンスとq軸インダクタンスがほぼ等しい非突極性を有することが多く、IPM構造ではd軸よりq軸インダクタンスの方が小さいという逆突極特性を有することが多い。   In the permanent magnet synchronous machine, since the relative permeability of the permanent magnet is as low as about 1, the SPM structure and the IPM structure have different characteristics. In general, the SPM structure often has non-saliency in which the d-axis inductance and the q-axis inductance are almost equal, and the IPM structure often has a reverse salient pole characteristic in which the q-axis inductance is smaller than the d-axis. .

ここでは、界磁極(N極)を基準とする直交座標系における固定子巻線のd軸とq軸のインダクタンス成分がほぼ等しい場合を“磁気的に非突極性を有する”と定義する。   Here, the case where the inductance components of the d-axis and the q-axis of the stator winding in the orthogonal coordinate system with the field pole (N pole) as a reference are substantially equal is defined as “having magnetic non-saliency”.

基本となる記号の定義
d軸:界磁軸
q軸:界磁軸に対して直交であり、d軸から電気角で90°だけ正転方向に移動した軸
Ld:電機子巻線のd軸インダクタンス
Lq:電機子巻線のq軸インダクタンス
R:電機子巻線抵抗
θ:U相巻線軸からd軸までの位相角(電気角、正転方向を正とする)
ω:角速度(dθ/dt)(電気角、正転側方向を正とする)
ここで、突極性に関しては次のように定義する。
Definition of basic symbols d axis: field axis q axis: axis orthogonal to the field axis and moved in the forward rotation direction by 90 ° in electrical angle from the d axis Ld: d axis of the armature winding Inductance Lq: q-axis inductance of armature winding R: Armature winding resistance θ: Phase angle from U-phase winding axis to d-axis (electrical angle, normal rotation direction is positive)
ω: angular velocity (dθ / dt) (electrical angle, forward rotation direction is positive)
Here, the saliency is defined as follows.

“磁気的に非突極性を有する同期機”または“非突極機”:Ld≒Lqの場合
“磁気的に突極性を有する同期機”または“突極機”:Ld≠Lqの場合
本発明が制御対象としているPMモータは、非突極機でかつダンパ巻線の存在していないPMモータである。
“Synchronous machine with magnetic non-saliency” or “non-saliency machine”: Ld≈Lq “Synchronous machine with magnetic saliency” or “saliency machine”: Ld ≠ Lq Is a PM motor that is a non-salient pole machine and has no damper winding.

PMモータの磁極位置を位置センサで検出することなく、PMモータの速度やトルクを制御する手法として、PMモータの速度起電力から磁極位置情報を得る方式など、位置センサを不要にしてPMモータの回転速度、回転位相を制御する位置センサレス制御方式が提案されている。このうち、PMモータの速度起電力から磁極位置情報を得る方式は、PMモータの定格速度の10%以下付近の速度になると、前記の速度起電力がPMモータの定格電圧よりも相対的に小さくなるため、速度起電力の電圧誤差の影響が相対的に大きくなる。そのため、速度起電力情報を利用した位置センサレス制御方式では、低速域の正確な磁極位相が得られなくなる。この低速域のセンサレス制御による磁極位相精度の対策として、突極機などではモータ駆動電流に高周波成分を重畳した磁極位相推定方法などが開発されている(例えば、特許文献1参照)。   As a method for controlling the speed and torque of the PM motor without detecting the magnetic pole position of the PM motor by using a position sensor, the position sensor is not required, such as a method of obtaining magnetic pole position information from the speed electromotive force of the PM motor. A position sensorless control method for controlling the rotation speed and the rotation phase has been proposed. Among these, the method of obtaining magnetic pole position information from the speed electromotive force of the PM motor is such that the speed electromotive force is relatively smaller than the rated voltage of the PM motor when the speed is near 10% or less of the rated speed of the PM motor. Therefore, the influence of the voltage error of the speed electromotive force becomes relatively large. Therefore, in the position sensorless control method using the speed electromotive force information, an accurate magnetic pole phase in the low speed range cannot be obtained. As a countermeasure for the magnetic pole phase accuracy by sensorless control in the low speed region, a magnetic pole phase estimation method in which a high frequency component is superimposed on a motor drive current has been developed for salient pole machines and the like (see, for example, Patent Document 1).

しかし、磁気的に非突極性を有する非突極機では、高調波の電圧と電流のベクトルには位相差が生じないため、位相推定方法を適用できないという問題があった。そのため、非突極機では、ステッピングモータにおける駆動制御のように、任意の大きさとなる振幅の電流を流し、この電流の周波数を徐々に変化させて同期引込状態を維持させながら強制的に磁極位相を電流位相に追従させて始動する方式(電流引込法と呼ぶ)が利用されている。   However, a non-salient pole machine having non-saliency magnetically has a problem that a phase estimation method cannot be applied because a phase difference does not occur between harmonic voltage and current vectors. Therefore, in a non-salient pole machine, a current of an arbitrary amplitude is passed as in the drive control of a stepping motor, and the magnetic phase is forcibly maintained while maintaining the synchronous pull-in state by gradually changing the frequency of this current. Is started (followed by the current phase) (referred to as current drawing method).

しかし、この電流引込法による始動方式は下記のような課題がある。   However, the starting method by the current drawing method has the following problems.

(1)磁極軸と電流軸の位相差(起磁力相差角ψ)のsin関数としてトルクが変動するため、このトルク特性が固定子と回転子間にあたかも弾性軸が存在しているものと似た振る舞いをする。そして、負荷トルク変動などにより、回転子や負荷の慣性モーメントと共振するような速度振動(軸ねじれ振動)が生じるが、ダンパ巻線が無いPMモータでは振動抑制効果が無く、軸ねじれ振動(以下、軸振動と称する)が継続する問題がある。この軸振動は負荷に出力するトルク品質を低下させ、さらにカップリングなどでは軸振動により金属疲労などを起こす問題がある。   (1) Since the torque fluctuates as a sin function of the phase difference between the magnetic pole axis and the current axis (magnetomotive force phase difference angle ψ), this torque characteristic is similar to that in which an elastic axis exists between the stator and the rotor. Behave. Then, speed vibration (shaft torsional vibration) that resonates with the rotor and load inertia moment occurs due to load torque fluctuation, etc. However, a PM motor without a damper winding has no vibration suppression effect and shaft torsional vibration (hereinafter referred to as “torsional torsion vibration”) , Referred to as axial vibration). This shaft vibration lowers the quality of torque output to the load, and there is a problem that coupling causes metal fatigue due to shaft vibration.

(2)電流引込法では、上記の軸振動が生じると軸ねじれ分のトルク脈動が出力軸のトルクに加算されるため、電流振幅を大きく設定しておかないと最大トルクを超えて脱調が発生する。この脱調を防止するためには通常のベクトル制御で必要な電流よりも、1.5〜2倍の大きな電流を流さねばならない。その結果、大きな容量の電力変換器が必要になる。   (2) In the current pull-in method, torque pulsation corresponding to shaft torsion is added to the torque of the output shaft when the above-mentioned shaft vibration occurs, so if the current amplitude is not set large, step-out will occur exceeding the maximum torque. Occur. In order to prevent this step-out, a current that is 1.5 to 2 times larger than that required for normal vector control must be supplied. As a result, a large capacity power converter is required.

これらの課題があるため、電流引込法はファン・ポンプなどの始動時や低速時のトルクが小さい二乗低減負荷特性などに応用範囲が限定されている。   Because of these problems, the scope of application of the current pull-in method is limited to the square reduction load characteristics with a small torque at the time of starting or low speed of a fan / pump.

もし、電流引込法を突極機に適用するのであれば、特許文献2のように、高周波法を振動抑制に応用する方法もある。また、高周波成分を利用しないで磁極位相を推定する方法として非特許文献1の方式などもある。   If the current drawing method is applied to the salient pole machine, there is a method of applying the high frequency method to vibration suppression as disclosed in Patent Document 2. Further, as a method for estimating the magnetic pole phase without using a high frequency component, there is a method of Non-Patent Document 1.

この非特許文献1の方式における特徴は、PWM制御によるスイッチングモードにおいて、三相のスイッチング素子が全相とも上アームのみが導通(ON)する期間(V7)と全相とも下アームのみが導通(ON)する期間(V0)に電流微分情報を得て磁極位相を推定する。このV7とV0の期間は通常零電圧ベクトル期間と呼ばれている。PMモータの定格速度の10%以下という低速では零電圧ベクトル期間V7とV0の発生比率が大きいため、電流微分情報を得るために複数の電流を検出する時間間隔もPWMキャリア周期の1/4以上に設定できるため、2点以上の時刻で電流検出が可能である。   The feature of the method of Non-Patent Document 1 is that in the switching mode by PWM control, the three-phase switching element has a period (V7) in which only the upper arm is conductive (ON) for all phases and only the lower arm is conductive for all phases ( ON) Current differential information is obtained during the period (V0) during which the magnetic pole phase is estimated. This period of V7 and V0 is usually called a zero voltage vector period. Since the generation ratio of the zero voltage vector periods V7 and V0 is large at a low speed of 10% or less of the rated speed of the PM motor, the time interval for detecting a plurality of currents to obtain current differential information is also ¼ or more of the PWM carrier period. Current can be detected at two or more times.

特開2008−295220号公報JP 2008-295220 A 特開2006−353025号公報JP 2006-353025 A 特開2000−236694号公報JP 2000-236694 A

J.−L.Chen, T.−H.Uu,and C.−L.Chen:“Implementation of a Novel High−Paformance Sensorless IPMSM Control System”、ICIT 2010,pp.361−366(2010)J. et al. -L. Chen, T.A. -H. Uu, and C.I. -L. Chen: "Implementation of a Novel High-Performance Sensor IPMSM Control System", ICIT 2010, pp. 361-366 (2010)

PMモータの位置センサレス制御における磁極位相推定方法を大別すると、次の3種類がある。   The magnetic pole phase estimation method in the position sensorless control of the PM motor is roughly classified into the following three types.

(a)速度起電力を利用した磁極位相推定方法
(b)磁気的な突極性を利用した磁極位相推定方法
(c)鉄心の磁気飽和特性がN極とS極方向で異なることを利用した磁極位相推定方法
これら位相推定方法のうち、零電圧ベクトル期間における電流微分情報を利用する方法の非特許文献1では、磁気的な突極性を利用した(b)の成分だけでなく、(a)の速度起電力の成分も複合して位相推定に利用している。
(A) Magnetic pole phase estimation method using velocity electromotive force (b) Magnetic pole phase estimation method using magnetic saliency (c) Magnetic pole using the fact that the magnetic saturation characteristics of the iron core are different in the N-pole and S-pole directions Phase estimation method Among these phase estimation methods, Non-Patent Document 1, which uses current differential information in a zero voltage vector period, includes not only the component (b) but also the magnetic saliency. The component of velocity electromotive force is also used for phase estimation.

(b)の磁気的な突極性を利用する方法では、d軸の位相を推定できても、N極とS極の区別ができない欠点がある。ある程度の速度に達すれば(a)の起電力情報によってN極とS極を判定することが可能になるが、それまではN極とS極の推定に誤りがあるとPMモータは異常な動作をすることがある。   The method using the magnetic saliency of (b) has a drawback that even if the d-axis phase can be estimated, the N pole and the S pole cannot be distinguished. If the speed reaches a certain level, it becomes possible to determine the N pole and the S pole based on the electromotive force information in (a). Until then, the PM motor operates abnormally if there is an error in the estimation of the N pole and the S pole. Sometimes

(c)の鉄心の磁気飽和を利用する方法では、モータの設計時点で磁気飽和をしやすい設計にする必要があり、さらに過大な電流を流す必要がある。   In the method (c) using the magnetic saturation of the iron core, it is necessary to make the design easy to perform magnetic saturation at the time of designing the motor, and it is necessary to pass an excessive current.

以上のように、従来のPMモータの位置センサレス制御方法は、(a)の速度起電力を利用した磁極位相推定方法だけでは正確な磁極位相を推定できない。また、(b)の方法は磁気的な突極性を利用するため、磁気的に突極性のない非突極機にはそのまま適用することができない。また、電流引込法を適用した場合には軸ねじれ振動を招く問題が残る。また、(c)の方法は、脱調防止のためには大容量の電力変換器を必要とするなどの問題がある。   As described above, the conventional PM motor position sensorless control method cannot accurately estimate the magnetic pole phase only by the magnetic pole phase estimation method using the speed electromotive force of (a). Further, since the method (b) uses magnetic saliency, it cannot be applied as it is to a non-salient pole machine having no magnetic saliency. Further, when the current drawing method is applied, there remains a problem that causes shaft torsional vibration. Further, the method (c) has a problem that a large-capacity power converter is required to prevent step-out.

本発明の目的は、磁気的に突極性のないPMモータの磁極位相を定格速度の10%以下などの低い速度まで精度良く推定でき、この磁極位相の推定を基にした電流引込法による速度振動(軸振動)の抑制および脱調を防止できる永久磁石同期電動機の位置センサレス制御装置を提供することにある。   It is an object of the present invention to accurately estimate the magnetic pole phase of a PM motor having no magnetic saliency up to a low speed such as 10% or less of the rated speed, and to perform velocity oscillation by a current drawing method based on the estimation of the magnetic pole phase. An object of the present invention is to provide a position sensorless control device for a permanent magnet synchronous motor that can suppress (shaft vibration) and prevent step-out.

本発明に用いる前記の零電圧ベクトル期間の電流微分情報は、デッドタイムの影響を受けないため、従来のPWM制御に入力する電圧指令などを利用する磁極位相推定方法よりも、より低い速度から速度起電力情報が得られる可能性があることに着目し、零電圧ベクトル期間の電流微分情報を検出して速度起電力情報を取得し、この速度起電力を利用した磁極位相推定方法で磁極位相を推定し、この推定した磁極位相を基に磁気的に突極性のないPMモータに電流引込法を適用した場合の速度振動(軸振動)の抑制をするようにしたもので、以下の構成を特徴とする。   Since the current differential information of the zero voltage vector period used in the present invention is not affected by the dead time, the speed is reduced from a lower speed than the magnetic pole phase estimation method using a voltage command or the like input to the conventional PWM control. Focusing on the possibility that electromotive force information can be obtained, current differential information during zero voltage vector period is detected to obtain speed electromotive force information, and the magnetic pole phase is estimated by the magnetic pole phase estimation method using this speed electromotive force. Based on this estimated magnetic pole phase, velocity vibration (shaft vibration) is suppressed when the current drawing method is applied to a PM motor with no magnetic saliency. And

(1)非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θを推定する位相推定手段を有する永久磁石同期電動機の位置センサレス制御装置であって、
前記位相推定手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、各前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記2点以上の時刻t2n、t(2n+1)の電流検出値から電流差分を演算する電流差分検出部(11)と、
前記時刻t2n,t2n+1の時間差ΔTpと前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ω*より速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した除算値と前記速度起電力との乗算値となる電流差分成分に変換する電流差分成分演算部(12)と、
前記電流差分検出部の出力と前記電流差分成分演算部の出力を加算し、この加算値をフィルタで直流分を除去して補正ゲインKpを乗算し、さらに前記補正ゲインKpを乗算した出力に角周波数重み関数Kωを乗じることにより補正角周波数Δωp *を演算し、これを前記角周波数指令ω*に加算して新しい角周波数指令ωp *を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする。
(1) Phase estimation means for starting the magnetic pole phase θ of a synchronous motor that uses a permanent magnet that is a non-salient pole machine and does not have a damper winding as a field source to follow the current phase and estimates the magnetic pole phase θ A position sensorless control device for a permanent magnet synchronous motor having:
The phase estimation means includes
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental wave current detector (8) for detecting currents at times t 2n and t (2n + 1) at least two points during each of the zero voltage vector periods;
A current difference detector (11) that calculates a current difference from current detection values at times t 2n and t (2n + 1) at two or more points;
A speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L, and the angular frequency command ω * , and the time difference ΔTp is divided by the inductance L. A current difference component calculation unit (12) that converts a current difference component that is a product of the value and the speed electromotive force;
An output obtained by adding the output of the current difference detection unit and the output of the current difference component calculation unit, removing the DC component by a filter, multiplying the sum by a correction gain K p , and further multiplying the correction gain K p angular frequency weight multiplied by the function K omega calculates the correction angle frequency [Delta] [omega p *, the correction angular frequency command calculator for calculating the angular frequency command omega * to a new angular frequency command omega p * by adding this to the ( 13-15)
It is provided with.

(2)非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θを推定する位相推定手段を有する永久磁石同期電動機の位置センサレス制御装置であって、
前記位相推定手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記2点以上の時刻t2n、t(2n+1)の電流検出値から電流差分を演算する電流差分検出部(11)と、
前記電流差分をフィルタにより直流分を除去して補正ゲインを乗算し、さらに前記補正ゲインKpを乗算した出力に角周波数重み関数Kωを乗じることにより補正角周波数Δωp *を演算し、これを前記角周波数指令ω*に加算して新しい角周波数指令ωp *を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする。
(2) Phase estimation means for starting the magnetic pole phase θ of a synchronous motor that uses a permanent magnet that is a non-salient pole machine and has no damper winding as a field source to follow the current phase and estimate the magnetic pole phase θ A position sensorless control device for a permanent magnet synchronous motor having:
The phase estimation means includes
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental current detector (8) for detecting currents at times t 2n and t (2n + 1) at least two points during the zero voltage vector period;
A current difference detector (11) that calculates a current difference from current detection values at times t 2n and t (2n + 1) at two or more points;
A correction angular frequency Δω p * is calculated by multiplying an output obtained by removing the DC component from the current difference by a filter and multiplying the correction gain by the filter, and multiplying the output multiplied by the correction gain K p by an angular frequency weighting function K ω. the was added to the angular frequency command omega * calculates a new angular frequency command omega p * corrected angular frequency command calculation section (13 to 15),
It is provided with.

(3)非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θを推定する位相推定手段を有する永久磁石同期電動機の位置センサレス制御装置であって、
前記位相推定手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、前記零電圧ベクトル期間中に三角波キャリア信号の上下限の頂点に対して対称な少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記上アームと下アーム2種類の零電圧ベクトル期間(V7,V0)の頂点に対して対称な2点以上の時刻t2n、t(2n+1)の電流検出値の電流差分の平均値を求め、前記時刻t2n,t2n+1の時間差ΔTpと、前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ω*より速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した除算値と前記速度起電力との乗算値となる電流差分成分に変換する電流差分成分の平均値演算部(12A)と、
前記電流検出部の電流差分の平均値出力と電流差分成分演算部の出力を加算(12C)し、この加算値をフィルタで直流分を除去して補正ゲインKpを乗算し、さらに前記補正ゲインKp乗算した出力に角周波数重み関数Kωを乗じることにより補正角周波数Δωp *を演算し、これを前記角周波数指令ω*に加算して新しい角周波数指令ωp *を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする。
(3) Phase estimation means for starting the magnetic pole phase θ of a synchronous motor that uses a permanent magnet that is a non-salient pole machine and does not have a damper winding as a field source to follow the current phase and estimates the magnetic pole phase θ A position sensorless control device for a permanent magnet synchronous motor having:
The phase estimation means includes
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental wave current detector (8) for detecting currents at times t 2n and t (2n + 1) at least two points symmetrical with respect to the upper and lower vertices of the triangular wave carrier signal during the zero voltage vector period;
The average value of the current difference of the current detection values at time t 2n and t (2n + 1) at two or more points symmetrical with respect to the vertices of the zero voltage vector period (V7, V0) of the upper arm and the lower arm. The speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L, and the angular frequency command ω * , and the time difference ΔTp is calculated by the inductance L. An average value calculation unit (12A) of a current difference component that is converted into a current difference component that is a multiplication value of the divided value divided by the speed electromotive force;
The average value output of the current difference of the current detection unit and the output of the current difference component calculation unit are added (12C), the DC value is removed by a filter, and the correction gain Kp is multiplied. K p calculates the correction angle frequency [Delta] [omega p * by multiplying the angular frequency weighting function K omega output multiplication, it calculates the angular frequency command omega * to a new angular frequency command omega p * by adding this correction angle A frequency command calculation unit (13 to 15);
It is provided with.

(4)非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θを推定する位相推定手段を有する永久磁石同期電動機の位置センサレス制御装置であって、
前記位相推定手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記2点以上の時刻t2n、t(2n+1)の電流検出値から電流差分を演算する電流差分検出部(11)と、
前記上アームの零電圧ベクトル期間(V7)と下アームの零電圧ベクトル期間(V0)の2種類の検出期間における前記2点以上の時刻t2n、t(2n+1)の電流差分を移動平均し、前記時刻t2n、t2n+1の時間差ΔTpと、前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ω*より速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した除算値と前記速度起電力との乗算値となる電流差分成分に変換する電流差分成分の平均値演算部(12B)と、
前記電流検出部の電流差分と電流差分成分演算部の出力を加算(12C)し、この加算値をフィルタで直流分を除去して補正ゲインKpを乗算し、さらに前記補正ゲインKp乗算した出力に角周波数重み関数Kωを乗じることにより補正角周波数Δωp *を演算し、これを前記角周波数指令ω*に加算して新しい角周波数指令ωp *を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする。
(4) Phase estimating means for starting the magnetic pole phase θ of a synchronous motor that uses a permanent magnet that is a non-salient pole machine and does not have a damper winding as a field source to follow the current phase and estimate the magnetic pole phase θ A position sensorless control device for a permanent magnet synchronous motor having:
The phase estimation means includes
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental current detector (8) for detecting currents at times t 2n and t (2n + 1) at least two points during the zero voltage vector period;
A current difference detector (11) that calculates a current difference from current detection values at times t 2n and t (2n + 1) at two or more points;
A moving average of current differences at times t 2n and t (2n + 1) at two or more points in two types of detection periods of the upper arm zero voltage vector period (V7) and the lower arm zero voltage vector period (V0). Then, the speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L and the angular frequency command ω * , and the time difference ΔTp is calculated by the inductance L. An average value calculation unit (12B) of current difference components to be converted into a current difference component that is a multiplication value of the divided value divided by the speed electromotive force;
Wherein adding the output of the current difference and the current difference component calculation unit of the current detecting portion (12C), the added value by removing the DC component in the filter multiplied by the correction gain K p, multiplied further the correction gain Kp Output angular frequency weight multiplied by the function K omega calculates the correction angle frequency [Delta] [omega p *, the correction angular frequency command calculator for calculating the angular frequency command omega * to a new angular frequency command omega p * by adding this to the ( 13-15)
It is provided with.

以上のとおり、本発明によれば、零電圧ベクトル期間の電流微分情報を利用して速度起電力情報を取得し、この速度起電力を利用した磁極位相推定方法で磁極位相を推定し、この推定した磁極位相を基に磁気的に突極性のないPMモータの磁極位相θを電流位相に追従させて始動する電流引込法を適用した場合の振動抑制を追加したことにより、磁気的に突極性のないPMモータの磁極位相を低い速度まで精度良く推定でき、この磁極位相の推定を基にした電流引込法による速度振動(軸振動)の抑制および脱調を防止できる。   As described above, according to the present invention, the speed electromotive force information is obtained using the current differential information in the zero voltage vector period, and the magnetic pole phase is estimated by the magnetic pole phase estimation method using the speed electromotive force. Vibration suppression when applying the current pull-in method to start the PM motor by following the current phase with the magnetic pole phase θ of a PM motor that has no magnetic saliency based on the magnetic pole phase. It is possible to accurately estimate the magnetic pole phase of a non-PM motor to a low speed, and to suppress the speed vibration (shaft vibration) and the step-out by the current drawing method based on the estimation of the magnetic pole phase.

本発明の実施形態1を示す装置構成図。The apparatus block diagram which shows Embodiment 1 of this invention. 本発明の実施形態2を示す装置構成図。The apparatus block diagram which shows Embodiment 2 of this invention. 本発明の実施形態3を示す装置構成図。The apparatus block diagram which shows Embodiment 3 of this invention. 本発明の実施形態4を示す装置構成図。The apparatus block diagram which shows Embodiment 4 of this invention. V0電圧ベクトル時の短絡電流の例。The example of the short circuit current at the time of V0 voltage vector. V7電圧ベクトル時の短絡電流の例。The example of the short circuit current at the time of V7 voltage vector. 零電圧ベクトルV0,V7の定義期間。Definition period of zero voltage vectors V0 and V7. 零電圧ベクトルV0,V7と電流検出の関係図。The relationship diagram of zero voltage vectors V0 and V7 and current detection. 図1中の周波数重み関数の特性例。The characteristic example of the frequency weight function in FIG. 従来の基本的な電流引込法によるシミュレーション波形図。The simulation waveform figure by the conventional basic current drawing method. 本発明の実施形態によるシミュレーション波形図。The simulation waveform diagram by embodiment of this invention.

(1)発明の基本的な説明
本発明の実施形態を示す前に、本発明の基本的な原理や関係式を先に説明する。まず、同期機が呈する電圧、電流等の関係は、磁極軸をd軸とする直交2軸座標系(d−q座標)の方程式を(1)式として表すことができる。
(1) Basic description of the invention Before showing an embodiment of the present invention, the basic principle and relational expression of the present invention will be described first. First, the relationship between the voltage, current, and the like exhibited by the synchronous machine can be expressed as an equation (1) in an orthogonal biaxial coordinate system (dq coordinate) having the magnetic pole axis as the d axis.

Figure 2012153794
Figure 2012153794

ここで、
d、Vq:d軸、q軸電圧成分
d、iq:d軸、q軸電流成分
φd:界磁磁束による固定子巻線鎖交磁束(界磁磁束はd軸のみと仮定)
R:巻線抵抗
d、Lq:界磁軸(d軸)とそれより90°位相の進んだ軸におけるインダクタンス成分
p:微分演算子(=d/dt)
θ:U相巻線軸からみた界磁軸(d軸)の位相角(電気角)
ω:角周波数(電気角)dθ/dt
次に、本発明は、非突極機を対象とするため、インダクタンスをLd=Lq=Lとおくと、(2)式のように行列が対称な要素になる。
here,
V d , V q : d-axis, q-axis voltage component i d , i q : d-axis, q-axis current component φ d : stator winding interlinkage magnetic flux by field magnetic flux (assuming that field magnetic flux is only d-axis )
R: Winding resistance L d , L q : Inductance component on the field axis (d axis) and an axis advanced by 90 ° phase p: Differential operator (= d / dt)
θ: Phase angle (electrical angle) of field axis (d-axis) viewed from U-phase winding axis
ω: angular frequency (electrical angle) dθ / dt
Next, since the present invention is intended for non-salient pole machines, when the inductance is set to L d = L q = L, the matrix becomes an element that is symmetric as shown in equation (2).

Figure 2012153794
Figure 2012153794

このd−q座標成分を固定座標から、位相角θγでかつ角速度ωγで回転している電流ベクトルを基準とする回転座標(γ−δ座標)に変換するには、d軸からみた電流ベクトルの発生軸(γ軸)までの位相角を起磁力相差角ψ=θγ−θと定義して(3)式〜(5)式を適用すればよい。In order to convert this dq coordinate component from a fixed coordinate to a rotational coordinate (γ-δ coordinate) based on a current vector rotating at a phase angle θ γ and an angular velocity ω γ , the current viewed from the d axis The phase angle to the vector generation axis (γ axis) is defined as magnetomotive force phase difference angle ψ = θ γ −θ, and equations (3) to (5) may be applied.

また、電流引込法では電流指令Iγ *のみに設定しており、さらに電流制御の応答も高いので正確にIγ *とIδ *=0に等しい実電流が角速度指令ω*どおり流れているものと仮定する。Further, in the current drawing method, only the current command I γ * is set, and the current control response is also high, so that an actual current exactly equal to I γ * and I δ * = 0 flows according to the angular velocity command ω * . Assume that

Figure 2012153794
Figure 2012153794

Figure 2012153794
Figure 2012153794

Figure 2012153794
Figure 2012153794

この(3)式〜(5)式を(1)式と(2)式に代入し、電圧項の変換行列を消去するためにその逆行列を両辺の左から掛けると、(6)式のようになり、さらにまとめると(7)式になる。   Substituting these formulas (3) to (5) into formulas (1) and (2) and multiplying the inverse matrix from the left of both sides to eliminate the conversion matrix of the voltage term, the formula (6) When it is further summarized, the equation (7) is obtained.

Figure 2012153794
Figure 2012153794

Figure 2012153794
Figure 2012153794

さらに、PWMパターンの零電圧ベクトル期間のみに限定すれば、左辺の電圧成分は(8)式のように零に置き換えられる。ここで、PWMインバータなどの主回路の半導体素子の電圧降下成分は無視しており、またd軸とγ軸の位相角の変化量が少ないものとみなして、d軸とγ軸の角速度差(dψ/dt)も微小であるとしてdψ/dt≒0を代入して無視する。   Furthermore, if limited to the zero voltage vector period of the PWM pattern, the voltage component on the left side is replaced with zero as shown in equation (8). Here, the voltage drop component of the semiconductor element of the main circuit such as the PWM inverter is ignored, and it is considered that the change amount of the phase angle between the d axis and the γ axis is small, and the angular velocity difference between the d axis and the γ axis ( Assuming that dψ / dt) is also very small, dψ / dt≈0 is substituted and ignored.

Figure 2012153794
Figure 2012153794

(8)式の関係を(7)式に代入して、γ軸成分のみ取り出すとφd・sinψを求める式が得られる。By substituting the relationship of equation (8) into equation (7) and extracting only the γ-axis component, an equation for obtaining φ d · sin ψ is obtained.

Figure 2012153794
Figure 2012153794

発生トルクは電流と直交な鎖交磁束成分との積であるので、トルクTorqueはこれらの直交成分の積で求められる。   Since the generated torque is a product of the current and the orthogonal flux linkage component, the torque Torque is obtained by the product of these orthogonal components.

Figure 2012153794
Figure 2012153794

ここで、正のトルクとは回転子を正転方向に加速するトルク成分としたので、磁束に対して電流が90゜進んだ方向の場合に正のトルクが発生する。このトルクが推定できれば、特許文献2および特許文献3などのV/F形PMモータの位置センサレス制御方式において採用した安定化原理を適用することができる。   Here, since the positive torque is a torque component that accelerates the rotor in the forward rotation direction, positive torque is generated when the current is in a direction advanced by 90 ° with respect to the magnetic flux. If this torque can be estimated, the stabilization principle adopted in the position sensorless control method of the V / F type PM motor such as Patent Document 2 and Patent Document 3 can be applied.

特許文献3では電圧ベクトルと同相成分のq軸電流成分をフィードバック信号に利用しているが、トルクに比例する成分という観点でみれば等価であり、ほぼ同様な振動抑制効果が得られることになる。また、特許文献2では入力電圧ベクトルの軸と界磁磁束による電圧ベクトルの軸との位相差(負荷角δ)をフィードバックしている。どちらの構成においてもモータトルクに関連した検出値をフィードバック量としており、それぞれ、その情報を利用した安定化原理が説明されているので、ここでは安定化に必要な周波数補償についての原理的な説明は省略する。   In Patent Document 3, the q-axis current component having the same phase component as that of the voltage vector is used for the feedback signal. However, this is equivalent from the viewpoint of a component proportional to the torque, and substantially the same vibration suppressing effect can be obtained. . In Patent Document 2, the phase difference (load angle δ) between the axis of the input voltage vector and the axis of the voltage vector due to the field magnetic flux is fed back. In both configurations, the detected value related to the motor torque is used as the feedback amount, and the stabilization principle using each information is explained. Here, the principle explanation about the frequency compensation necessary for stabilization is explained. Is omitted.

結論としては、電流引込法における周波数をトルクに比例した(11)式で補正したωp *として補正すればよい。In conclusion, the frequency in the current drawing method may be corrected as ω p * corrected by the equation (11) proportional to the torque.

Figure 2012153794
Figure 2012153794

(11)式の電流微分p・iγを離散系として表すため、時刻t2n、t(2n+1)の電流検出値iγ2n、iγ(2n+1)の差分とその時間差ΔTp=t(2n+1)−t2nにより近似し、電流差分iγ(2n+1)−iγ(2n)に掛かっていた係数を他の項に移動する。また、負の符号もまとめてしまうと(12)式に変形できる。この時刻t2n、t(2n+l)と電流検出値iγ(2n)、iγ(2n+l)については、後述の図8やトリガ信号発生部9の説明で詳細に記載することにする。In order to express the current differential p · i γ in the equation (11) as a discrete system, the difference between the detected current values i γ2n and i γ (2n + 1) at time t 2n and t (2n + 1) and the time difference ΔTp = t Approximate by (2n + 1) −t 2n, and move the coefficient applied to the current difference i γ (2n + 1) −i γ (2n) to another term. Further, if negative signs are also collected, it can be transformed into equation (12). The times t 2n and t (2n + l) and the current detection values i γ (2n) and i γ (2n + l) will be described in detail in FIG. 8 and the description of the trigger signal generator 9 described later. To do.

Figure 2012153794
Figure 2012153794

(12)式には分母に角周波数指令ω*の項があるため、周波数が零付近では補償量は過大になってしまう。この零の除算を防止するため、周波数の正負の極性を考慮し、周波数が零付近では補償量の大きさを零に抑圧する角周波数重みゲインKω(ω*)に近似して(13)式として取り扱うことにする。Since the expression (12) has a term of the angular frequency command ω * in the denominator, the compensation amount becomes excessive when the frequency is near zero. In order to prevent this division of zero, the polarity of the frequency is taken into consideration and approximated to an angular frequency weight gain K ω* ) that suppresses the magnitude of the compensation amount to zero near the frequency (13) I will treat it as an expression.

Figure 2012153794
Figure 2012153794

さらに、位相や回転速度の振動を抑制するためには(13)式の過渡成分だけを補償すればよいので、特許文献3を参照して高周波成分と直流成分を遮断するバンドパスフィルタ関数BPF{}を適用する。   Further, in order to suppress the vibration of the phase and the rotational speed, it is only necessary to compensate for the transient component of the equation (13), so that a bandpass filter function BPF { } Is applied.

Figure 2012153794
Figure 2012153794

(2)装置の基本構成
本発明を実現するための基本構成例を図1、図2、図3、図4に装置構成図として示す。図1〜図4の装置構成およびこれら構成における要部機能および動作を以下に概略説明する。
(2) Basic Configuration of Apparatus An example of a basic configuration for realizing the present invention is shown in FIG. 1, FIG. 2, FIG. 3, and FIG. The apparatus configuration shown in FIGS. 1 to 4 and the main functions and operations in these configurations will be schematically described below.

図5は、V0電圧ベクトル時の短絡電流の例であり、零電圧ベクトル期間V0におけるインバータのスイッチング状態と、(+Iu、−Iv、−Iw)極性の三相電流における電流通流路の例を示す。これにより、モータの端子電流がインバータの直流リンク電圧源(Vdc)と無関係であり、三相端子が短絡された状態と等価であることが分かる。Figure 5 is an example of a short-circuit current when the voltage V0 vector, the switching state of the inverter in the zero voltage vector period V0, (+ I u, -I v, -I w) current flow path in the polarity of the three-phase current An example of Thus, it can be seen that the motor terminal current is independent of the DC link voltage source (V dc ) of the inverter and is equivalent to a state where the three-phase terminals are short-circuited.

図6は、V7電圧ベクトル時の短絡電流の例であり、零電圧ベクトル期間V7におけるインバータのスイッチング状態と、(+Iu、−Iv、−Iw)極性の三相電流における電流通流路の例を示す。これにより、モータの端子電流がインバータの直流リンク電圧源(Vdc)と無関係であり、三相端子が短絡された状態と等価であることが分かる。FIG. 6 is an example of a short-circuit current at the time of the V7 voltage vector, and the current flow path in the switching state of the inverter in the zero voltage vector period V7 and the three-phase current of (+ I u , −I v , −I w ) polarity. An example of Thus, it can be seen that the motor terminal current is independent of the DC link voltage source (V dc ) of the inverter and is equivalent to a state where the three-phase terminals are short-circuited.

図7は、零電圧ベクトルV0,V7の定義期間であり、三角波キャリア比較法によるPWM制御パルス生成例を利用して、図5と図6における零電圧ベクトル期間V0とV7を示す。   FIG. 7 shows the definition periods of the zero voltage vectors V0 and V7, and shows the zero voltage vector periods V0 and V7 in FIGS. 5 and 6 using an example of PWM control pulse generation by the triangular wave carrier comparison method.

図8は零電圧ベクトル期間V0,V7と電流検出の関係を示し、図7のPWMパターンと電流検出時期の関係を示す。このように、零電圧ベクトル期間の電流微分を応用する方法をここではCurrent−Slope法と呼ぶ。   FIG. 8 shows the relationship between zero voltage vector periods V0 and V7 and current detection, and shows the relationship between the PWM pattern of FIG. 7 and current detection timing. Thus, the method of applying the current differentiation of the zero voltage vector period is referred to herein as the Current-Slope method.

図1は、Current−Slope法を適用した電流引込法によって振動抑制をする装置構成図であり、図8の電流サンプルを利用した制御システムの全体構成図を示す。   FIG. 1 is an apparatus configuration diagram for suppressing vibration by a current drawing method to which a current-slope method is applied, and shows an overall configuration diagram of a control system using the current sample of FIG.

図9は、図1中の角周波数重み関数の特性例を示し、これは図11で使用した例である。   FIG. 9 shows an example of the characteristics of the angular frequency weighting function in FIG. 1, which is the example used in FIG.

図2は、Current−Slope法を適用した電流引込法によって振動抑制をする装置構成図であり、図1の構成に対して、位相や回転速度の変動が小さいものとみなして簡素化した場合の構成例である。   FIG. 2 is a configuration diagram of a device that suppresses vibration by a current drawing method to which the current-slope method is applied. In the configuration shown in FIG. It is a structural example.

図3は、Current−Slope法を適用した電流引込法によって振動抑制をする装置構成図であり、図1の構成に対して、電流サンプル情報のうち、電流微分以外に使用する電流成分を、電流差分演算用の複数の検出電流値から合成した電流に修正した場合の構成を示す。   FIG. 3 is a configuration diagram of an apparatus that suppresses vibration by a current drawing method using the Current-Slope method. Compared to the configuration of FIG. The structure at the time of correcting to the electric current synthesize | combined from the some detected electric current value for difference calculation is shown.

図4は、Current−Slope法を適用した電流引込法によって振動抑制をする装置構成図であり、図3の構成に対して、電流差分値は三角波キャリアの上限の頂点(V7)と下限の頂点(V0)の2種類存在するので、2種類の平均値を移動平均して求めることにより、統計的な外乱抑制を適用した例を示す。   FIG. 4 is a configuration diagram of an apparatus that suppresses vibration by a current drawing method to which the Current-Slope method is applied. In contrast to the configuration of FIG. 3, the current difference value is the upper limit vertex (V7) and lower limit vertex of the triangular wave carrier. Since there are two types of (V0), an example in which statistical disturbance suppression is applied by obtaining a moving average of two types of average values is shown.

図10は、Current−Slope法による振動抑制を適用しない場合の、電流引込法による低速領域での始動および逆転動作のタイムチャート例であり、図4の制御構成例に対して、補償を適用していない動作チャートを示す。補償が無いため、速度が振動している例を示している。   FIG. 10 is a time chart example of start-up and reverse rotation operation in the low speed region by the current drawing method when vibration suppression by the Current-Slope method is not applied, and compensation is applied to the control configuration example of FIG. An operation chart is shown. Since there is no compensation, an example in which the speed is oscillating is shown.

図11は、Current−Slope法による振動抑制を適用した場合の、電流引込法による低速領域での始動および逆転動作のタイムチャート例であり、図4の制御構成例を適用することにより、図10の持続的な振動成分が減衰しながら抑制されている効果を示す。   FIG. 11 is a time chart example of starting and reversing operation in a low speed region by a current drawing method when vibration suppression by the Current-Slope method is applied. By applying the control configuration example of FIG. This shows the effect that the continuous vibration component of is suppressed while being attenuated.

(3)実施形態1
本実施形態は、図1に示す装置構成とする。同図は、電流制御部1による回転座標(γ−δ座標)の電流指令とそのフィードバック信号との偏差を基にした電流制御系を構成し、この電流制御部1からの電圧指令(γ−δ座標)を座標変換部2により推定位相(θ^)を使って電圧va *とvb *の固定座標に変換し、さらに2相/3相変換部3により3相電圧vu *,vv *,vw *に変換し、これら電圧を3相電圧指令としてPWM制御部4と三角波発振部5により三角波キャリア比較法によりPWM波形を生成し、このPWM波形を電圧形3相インバータ6の各相ゲート指令としてインバータ6にPMモータ7のPWM電流出力を得る。
(3) Embodiment 1
This embodiment has the apparatus configuration shown in FIG. The figure shows a current control system based on the deviation between the current command of the rotation coordinate (γ-δ coordinate) by the current control unit 1 and its feedback signal, and the voltage command (γ− δ coordinate) is converted into fixed coordinates of voltages v a * and v b * by the coordinate conversion unit 2 using the estimated phase (θ ^), and the two-phase / three-phase conversion unit 3 further converts the three-phase voltage v u * , The PWM waveform is converted into v v * and v w * , and these voltages are used as a three-phase voltage command to generate a PWM waveform by the triangular wave carrier comparison method using the PWM control unit 4 and the triangular wave oscillation unit 5. The PWM current output of the PM motor 7 is obtained in the inverter 6 as each phase gate command.

次に、図1の装置構成で利用するモータ電流の検出について図5等を参照して説明する。図5はモータ電流の検出期間である零電圧ベクトル期間V0における電流の流路の例を示す。同図では、6アーム構成による電圧形3相インバータにおいて、3相とも下アームのスイッチング側(Sx、Sy、Sz)を導通(ON)状態にした場合をV0期間と呼ぶ。モータの端子電流がU相は正でありV相とW相は負の場合であれば、モータ内部のインダクタンス成分が電流を流れ続けるように働くため、点線で示したようにスイッチング素子と逆導通ダイオードを経由してモータ端子が短絡されたように電流が流れる。   Next, detection of a motor current used in the apparatus configuration of FIG. 1 will be described with reference to FIG. FIG. 5 shows an example of a current flow path in the zero voltage vector period V0, which is a motor current detection period. In the figure, in a voltage-type three-phase inverter having a six-arm configuration, the case where the switching side (Sx, Sy, Sz) of the lower arm is turned on (ON) in all three phases is called a V0 period. If the terminal current of the motor is positive in the U phase and negative in the V and W phases, the inductance component inside the motor will continue to flow, so reverse conduction with the switching element as shown by the dotted line A current flows as if the motor terminal is short-circuited via the diode.

図6はモータ電流のもう一つの検出期間である零電圧ベクトル期間V7における電流路の例を示す。同図では、上アームのスイッチング素子(Su、Sv、Sw)が導通(ON)状態となるので、電流路は異なるが、やはり図5と同様にモータ端子を短絡した状態になる。これにより、(8)式で電圧成分を零に近似したことが理解できる。   FIG. 6 shows an example of a current path in the zero voltage vector period V7 which is another detection period of the motor current. In the figure, since the switching elements (Su, Sv, Sw) of the upper arm are in the conductive (ON) state, the current paths are different, but the motor terminals are also short-circuited as in FIG. Thereby, it can be understood that the voltage component is approximated to zero in the equation (8).

次に、三角波キャリア比較法におけるPWM波形作成の場合を例にとって、この場合の零電圧ベクトルV0とV7の期間を示したものが図7である。三角波キャリア信号に対して、図のようなU相電圧指令vu(実線)、V相電圧指令vv(破線)、W相電圧指令vw(一点鎖線)が与えられた場合の、Su〜Szの6個のゲート信号の動作例を示す。前述の3相とも下アームのスイッチング素子(Sx、Sy、Sz)が導通(ON)しているV0期間と、上アームのスイッチング素子(Su、Sv、Sw)が導通(ON)しているV7期間をこの図に具体的に示している。低速では電圧指令が小さいため、三相の各電圧指令もほぼ三角波キャリア波形の振幅に対してほぼ中央レベルに集中している。そのため、V0期間もV7期間も他の電圧ベクトル期間に比べて長いことも読み取れる。Next, FIG. 7 shows the period of zero voltage vectors V0 and V7 in this case, taking as an example the case of PWM waveform generation in the triangular wave carrier comparison method. When a U-phase voltage command v u (solid line), a V-phase voltage command v v (broken line), and a W-phase voltage command v w (one-dot chain line) as shown in FIG. An operation example of six gate signals of Sz is shown. In the above three phases, the V0 period in which the lower arm switching elements (Sx, Sy, Sz) are conductive (ON) and the upper arm switching element (Su, Sv, Sw) are conductive (ON) V7. The period is specifically shown in this figure. Since the voltage command is small at low speeds, the three-phase voltage commands are also concentrated almost at the center level with respect to the amplitude of the triangular carrier waveform. Therefore, it can be read that both the V0 period and the V7 period are longer than the other voltage vector periods.

このような三角波キャリア比較法によるPWM制御を利用して電流制御系を構成するためには、図7の時刻tm、tm+1、tm+2、tm+3のようにキャリア信号の上下限の頂点に同期して電流検出する方法が使用されている。In order to construct a current control system using PWM control based on such a triangular wave carrier comparison method, carrier signals at times t m , t m + 1 , t m + 2 and t m + 3 in FIG. A method is used in which current is detected in synchronization with the top and bottom vertices.

図8は図7に示したPWM波形発生時において、本実施形態で提案する電流微分を検出するための電流検出時刻と、PWMリプルを除去した電流成分と等価な同期電流の検出結果との関係を示したものである。図8において、時刻tm、tm+1、tm+2、tm+3は、前述のように従来の電流制御に利用していた検出時刻であり、iumなどの電流を検出している。これに対して、各頂点に対称な検出時刻を追加する。例えば、時刻tm+1に対してはt2とt3、時刻tm+2に対してはt4とt5などであり、このときの電流iu2やiu3などを検出する。各t2とt3、t4とt5の検出時刻の時間差をΔTpとする。この時間幅は電圧振幅の最大量を考慮して決定する。FIG. 8 shows the relationship between the current detection time for detecting the current differentiation proposed in the present embodiment and the detection result of the synchronous current equivalent to the current component from which the PWM ripple is removed when the PWM waveform shown in FIG. 7 is generated. Is shown. In FIG. 8, times t m , t m + 1 , t m + 2 , t m + 3 are detection times used for conventional current control as described above, and detect currents such as i um. ing. In contrast, a symmetrical detection time is added to each vertex. For example, t 2 and t 3 for time t m + 1 , t 4 and t 5 for time t m + 2 , and currents i u2 and i u3 at this time are detected. Let ΔTp be the time difference between the detection times of t 2 and t 3 and t 4 and t 5 . This time width is determined in consideration of the maximum amount of voltage amplitude.

なお、図7では後述の実施形態3や実施形態4のために必要なV0期間とV7期間の中間に設定した例で示しているが、本実施形態1や後述の実施形態2においては電流微分が検出できればよく、中間ではなくて多少のズレが生じても問題はない。   FIG. 7 shows an example in which the V0 period and the V7 period necessary for the third and fourth embodiments described later are set, but in the first embodiment and the second embodiment described later, current differentiation is performed. Can be detected, and there is no problem even if some deviation occurs rather than in the middle.

このときの三相電流の波形と電流の検出点を図8の下段に○印や□印で示している。同図は定常時でデッドタイムの影響を受けていない場合のチャート例であるが、各零電圧ベクトル期間中の電流変化量は一定であり、2点間の電流検出値の差分は電流の時間微分と比例することが分かる。   The waveform of the three-phase current and the current detection point at this time are indicated by circles and squares in the lower part of FIG. This figure is an example of a chart when it is steady and not affected by the dead time. However, the amount of current change during each zero voltage vector period is constant, and the difference between the two current detection values is the current time. It can be seen that it is proportional to the differentiation.

以上の内容をふまえて、図1における電流引込法の基本構成について説明する。電流制御部1は、電流値Iγ *=|I1 *|とIδ *=0および角周波数ω*からなる電流指令と、基本波電流検出部8の電流サンプラ8Aで検出した電流iu,iv,iwを3相/2相変換部8Bで2相に変換し、これを固定/回転座標変換部8Cで座標変換し、さらに電流サンプラ8Dで同期検出した基本波検出電流iγ、iδから電流制御を行なう。電流制御部1は、制御基準である回転座標上の2軸電圧成分vγ *とvδ *を出力するので、これを回転座標変換部(e-jθ)2により固定座標系の電圧値va *とvb *に変換した後、2相/3相変換部3による2相/3相変換や零相変調などを適用して三相の電圧指令(vu *、vv *、vw *)に変換し、最後にPWM制御部4でPWM波形に変換してインバータ6の主回路のスイッチング素子を制御するゲー卜信号を生成する。電流誤差の大きな要因であるデッドタイムはこのPWM制御部4で付加されている。そして、インバータ6にてゲート信号に応じてPWM電圧指令と等価なPWM電圧パターンを出力してPMモータ7に給電する。Based on the above description, the basic configuration of the current drawing method in FIG. 1 will be described. The current control unit 1 includes a current command including a current value I γ * = | I 1 * |, I δ * = 0 and an angular frequency ω * , and a current i u detected by the current sampler 8A of the fundamental wave current detection unit 8. , I v , i w are converted into two phases by the three-phase / two-phase conversion unit 8B, the coordinates are converted by the fixed / rotation coordinate conversion unit 8C, and further, the fundamental wave detection current i γ detected synchronously by the current sampler 8D. , I δ is used for current control. Since the current control unit 1 outputs the biaxial voltage components v γ * and v δ * on the rotational coordinates, which are control references, the rotational coordinate conversion unit (e −jθ ) 2 outputs the voltage values v of the fixed coordinate system. After conversion to a * and v b * , two-phase / three-phase conversion by the two-phase / three-phase conversion unit 3 or zero-phase modulation is applied to apply three-phase voltage commands (v u * , v v * , v w * ), and finally, the PWM controller 4 converts it into a PWM waveform to generate a gate signal for controlling the switching elements of the main circuit of the inverter 6. The dead time, which is a major factor of current error, is added by the PWM control unit 4. Then, the inverter 6 outputs a PWM voltage pattern equivalent to the PWM voltage command in accordance with the gate signal and supplies power to the PM motor 7.

PMモータ7の三相電流は電流検出器(HCT)で信号に変換して検出する。電流サンプラ8は、マイクロコンピュータ構成など、ディジタル制御で構成する場合には、アナログの電流検出信号をサンプルホールドしてからA/D変換し、その後、3相/2相変換や回転座標変換e(exp(jθ))を介してγ−δ座標成分の検出電流iγとiδを得る。この検出電流は前述の電流制御に利用される。The three-phase current of the PM motor 7 is detected by converting it into a signal with a current detector (HCT). When the current sampler 8 is configured by digital control, such as a microcomputer configuration, the analog current detection signal is sampled and held, and then A / D converted, and then three-phase / two-phase conversion or rotational coordinate conversion e jθ. The detected currents i γ and i δ of the γ-δ coordinate component are obtained via (exp (jθ)). This detected current is used for the above-described current control.

PWM生成のために必要な三角波発振部5とそれに同期したトリガ信号発生部9が、PWM制御に必要な三角波と電流検出時刻tmやt2n、t(2n+1)を生成している。また、回転座標変換に入力される位相情報θは、補正を加えていない角周波数指令ω*を積分部10が時間積分して推定位相θ^(図面中では^マークをθの頂部に付けて記載)得る。A triangular wave oscillating unit 5 necessary for PWM generation and a trigger signal generating unit 9 synchronized therewith generate a triangular wave necessary for PWM control and current detection times t m , t 2n , t (2n + 1) . Further, the phase information θ input to the rotation coordinate transformation is obtained by integrating the angular frequency command ω * without correction by the integration unit 10 by time integration and adding an estimated phase θ ^ (in the drawing, a ^ mark is attached to the top of θ. Description) get.

以上が従来の電流引込法の構成であるが、本実施形態ではこれに新たに下記の機能を追加する。   The above is the configuration of the conventional current drawing method. In the present embodiment, the following functions are newly added thereto.

時刻t(2n)とt(2n+1)の時間差ΔTpの電流検出のためのトリガ信号の発生には、電流差分を検出する最初の時刻をt(2n)とするトリガ信号と、次の時刻をt(2n+1)とするトリガ信号をトリガ信号発生部9が発生している。γ軸電流差分検出部11は、トリガ信号の発生に基づく時刻t2nの電流検出値iγ(t2n)と検出時刻t(2n+1)の電流検出値iγ(t2n+1)から電流差分iγ(t2n+1)−iγ(t2n)を求める。これは、(14)式の微分電流成分と時間の積であるΔTp(p・iγ)に相当している。To generate a trigger signal for detecting a current having a time difference ΔT p between time t (2n) and t (2n + 1) , a trigger signal having t (2n) as the first time to detect the current difference, The trigger signal generation unit 9 generates a trigger signal whose time is t (2n + 1) . gamma-axis current difference detector 11, the current detection value at time t 2n based on the generation of the trigger signal i γ (t 2n) and the detection time t (2n + 1) current detection value i gamma of (t 2n + 1) The current difference i γ (t 2n + 1 ) −i γ (t 2n ) is obtained. This corresponds to ΔTp (p · i γ ), which is the product of the differential current component of equation (14) and time.

抵抗と速度起電力による電流差分成分演算部12は、前記(14)式の(ΔTp/L)(R・iγ−ω*・L・iδ)成分を演算する部分であり、電流制御用の電流検出値iγとiδからモータ抵抗Rによる電圧降下分とインダクタンスLおよび周波数指令ω*より速度起電力を演算し、インダクタンスLと電流差分の時間差ΔTpを利用して、電圧成分による生じる電流差分成分に変換し、電圧差分成分演算部12の出力をγ軸電流差分検出部11から出力される電流差分iγ(t2n+1)−iγ(t2n)と加算する。11の出力である電流検出差分は、端子電圧ベクトルと逆極性方向に発生するので、ここではこれを考慮して極性の反転と減算をまとめて加算演算に簡略化している。The current difference component calculation unit 12 based on the resistance and speed electromotive force is a part that calculates the (ΔT p / L) (R · i γ −ω * · L · i δ ) component of the equation (14). The speed electromotive force is calculated from the voltage drop due to the motor resistance R, the inductance L, and the frequency command ω * from the detected current values i γ and i δ , and the time difference ΔTp between the inductance L and the current difference is used. The generated current difference component is converted, and the output of the voltage difference component calculation unit 12 is added to the current difference i γ (t 2n + 1 ) −i γ (t 2n ) output from the γ-axis current difference detection unit 11. 11 is generated in the opposite polarity direction to the terminal voltage vector, and here, in consideration of this, polarity inversion and subtraction are combined into a simplified addition operation.

バンドパスフィルタ13は電流差分成分演算部12の出力から高周波帯域と低周波帯域を抑制し、このフィルタ出力に補正ゲイン乗算部14で補正ゲインKpとを乗じたものに、周波数重み関数乗算部15で角周波数指令ω*の除算の代わりに設定した角周波数重み関数Kωを乗じた値を乗算することにより補正角周波数Δωp *を演算し、これを角周波数指令ω*に加算して、(14)式に従った新しい角周波数指令ωp *を演算する。これら13〜15は、補正角周波数指令演算部を構成する。What the band pass filter 13 which suppresses the high frequency band and low frequency band from the output of the current difference component calculation unit 12, by multiplying the correction gain K p to the filter output by the correction gain multiplication unit 14, a frequency weighting function multiplier 15 is multiplied by the angular frequency weighting function K ω set in place of the division of the angular frequency command ω * to calculate the corrected angular frequency Δω p * , and this is added to the angular frequency command ω *. , A new angular frequency command ω p * according to the equation (14) is calculated. These 13-15 comprise the correction | amendment angular frequency command calculating part.

上記では従来の電流制御のタイミングと、電流微分による補償演算のタイミングとの相関を明記していないが、この安定化方式では電流制御などに比べて低い周波数成分しか補償しない。そのため、安定化補償のフィードバックにPWM周期程度の遅れ時間か存在しても大きな影響は無い。そのため、電流制御との関係までは限定する必要は無い。   In the above, the correlation between the current control timing and the compensation calculation timing by current differentiation is not clearly described, but this stabilization method compensates only a low frequency component as compared with current control. Therefore, even if there is a delay time of about the PWM period in the feedback of the stabilization compensation, there is no significant influence. Therefore, there is no need to limit the relationship with current control.

(4)実施形態2
本実施形態は、図2に示す装置構成とする。同図は、図1の構成に対して、電流差分成分演算部12を省いた点が異なる。すなわち、前記(14)式の(R・iγ−ω*・L・iδ)成分の変化量が小さい場合には、後段のバンドパスフィルタ13で抑制されてしまうことを考慮して、この電流差分成分演算部12を省略した構成とする。
(4) Embodiment 2
This embodiment has the apparatus configuration shown in FIG. This figure differs from the configuration of FIG. 1 in that the current difference component calculation unit 12 is omitted. That is, in consideration of the fact that the amount of change in the (R · i γ −ω * · L · i δ ) component of the equation (14) is small, this is suppressed by the subsequent band-pass filter 13. The current difference component calculation unit 12 is omitted.

(5)実施形態3
本実施形態は、図3に示す装置構成とする。同図は、図1の構成に対して、電流差分成分演算部12の演算機能を変更した点にある。
(5) Embodiment 3
This embodiment has the apparatus configuration shown in FIG. This figure is that the calculation function of the current difference component calculation unit 12 is changed from the configuration of FIG.

図1の構成では(14)式中の(R・iγ−ω*・L・iδ)の演算に使用する電流成分iγとiδを、三角波キャリアの頂点である同期電流の検出値を利用していたが、時刻tmに対して検出時刻t2nとt(2n+1)を前後に均等な時間差に設定すれば、電流差分用に検出した2点の電流成分iγとiδの平均を利用しても時刻tmの電流検出と等価な値が得られる。In the configuration of FIG. 1, the current components i γ and i δ used for the calculation of (R · i γ −ω * · L · i δ ) in the equation (14) are detected values of the synchronous current that is the apex of the triangular wave carrier. However, if the detection times t 2n and t (2n + 1) are set to equal time differences before and after the time t m , the two current components i γ and i detected for the current difference are used. Even if the average of δ is used, a value equivalent to the current detection at time t m can be obtained.

そこで、電流差分成分の平均値演算部12Aは、電流差分用に検出した電流成分iγとiδの平均値{iγ(t2n+1)+iγ(t2n)}/2と{iδ(t2n+1)+iδ(t2n)}/2で時刻tmの電流成分iγとiδと等価な電流検出値として置き換え、この平均値{iγ(t2n+1)+iγ(t2n)}/2と{iδ(t2n+1)+iδ(t2n)}/2と、上アームと下アームそれぞれの電流差分を検出する時刻のモータ抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ω*より速度起電力を演算し、インダクタンスLと電流差分の時間差ΔTpを利用してその電圧成分により生じる電流差分成分に変換する。この電流差分成分の平均演算部12Aの出力を電流差分の平均値の出力と加算部12Cで加算する。Therefore, the current difference component average value calculator 12A calculates the average value {i γ (t 2n + 1 ) + i γ (t 2n )} / 2 of the current components i γ and i δ detected for the current difference and {i δ (t 2n + 1 ) + i δ (t 2n )} / 2 is replaced with a current detection value equivalent to the current components i γ and i δ at time t m , and this average value {i γ (t 2n + 1 ) + i γ (t 2n )} / 2, {i δ (t 2n + 1 ) + i δ (t 2n )} / 2, and the voltage drop due to the motor resistance R at the time when the current difference between the upper arm and the lower arm is detected Then, the speed electromotive force is calculated from the inductance L and the angular frequency command ω *, and converted into a current difference component generated by the voltage component using the time difference ΔTp between the inductance L and the current difference. The output of the average calculation unit 12A for the current difference component is added to the output of the average value of the current difference by the addition unit 12C.

(6)実施形態4
本実施形態は、図4に示す装置構成とする。図3の演算は、(R・iγ−ω*・L・iδ)や{iγ(t2n+1)−iγ(t2n)}成分について常に最新の値を利用していたが、実際には零電圧ベクトル期間は、V0とV7という異なる条件が交互に生じている。そのため、インバータの主回路などの電圧降下が異なったり、デッドタイムなどの影響によって基本波成分の電流値も変動する可能性がある。
(6) Embodiment 4
This embodiment has the apparatus configuration shown in FIG. The calculation in FIG. 3 always uses the latest values for the components (R · i γ −ω * · L · i δ ) and {i γ (t 2n + 1 ) −i γ (t 2n )}. Actually, different conditions of V0 and V7 are alternately generated in the zero voltage vector period. Therefore, there is a possibility that the voltage drop of the main circuit of the inverter is different, or the current value of the fundamental wave component is fluctuated due to the influence of dead time or the like.

そこで、本実施形態の電流差分成分の移動平均値演算部12Bでは、図3に示す移動平均値演算部12Aに、最新検出電流微分値と前回の電流微分値との2点の移動平均を取る機能を加えたもので、統計的な処理により外乱成分を抑制する。   Therefore, in the moving average value calculation unit 12B of the current difference component of this embodiment, the moving average value calculation unit 12A shown in FIG. 3 takes a moving average of two points of the latest detected current differential value and the previous current differential value. A function is added, and disturbance components are suppressed by statistical processing.

なお、図4は図3に示す実施形態3の演算部12Aを12Bに変更した場合を示すが、図1に示す実施形態1の構成に対しても、または図2の実施形態2の構成に対しても同様な改善を適用することは可能である。   4 shows a case where the arithmetic unit 12A of the third embodiment shown in FIG. 3 is changed to 12B, but the configuration of the first embodiment shown in FIG. 1 or the configuration of the second embodiment shown in FIG. It is possible to apply similar improvements to this.

また、以上までの装置構成は、前記の(14)式に基づいた演算部構成の例を示したが、原理的には(11)式に準拠していれば、サンプラの位置を座標変換の前に移動したり、演算の順序を入れ替えたり、係数にインダクタンス成分を含ませて演算形式を変更するなど、上記実施形態1乃至4以外の異なる形態でも同様な効果が得られることは明白である。   In addition, the above-described apparatus configuration has shown an example of the calculation unit configuration based on the above-mentioned equation (14). However, in principle, if it conforms to the equation (11), the position of the sampler can be converted into coordinates. It is clear that the same effect can be obtained in different forms other than the first to fourth embodiments, such as moving forward, changing the order of calculations, and changing the calculation format by including an inductance component in the coefficient. .

これら実施形態1乃至4より、磁気的に突極性のないPMモータの磁極位相θを電流位相に追従させて始動する電流引込法を適用した場合の振動抑制をするようにしたため、電流引込法による速度振動(軸振動)の抑制および脱調を防止できる。   According to the first to fourth embodiments, vibration suppression is applied when the current pulling method of starting the magnetic pole phase θ of a PM motor having no magnetic saliency following the current phase is applied. Suppression of speed vibration (shaft vibration) and step-out can be prevented.

(7)シミュレーション
上記の実施形態4の装置構成と従来の電流引込法による装置を例にしてシミュレーションを行い、本発明の効果を確認した。
(7) Simulation A simulation was performed by using the apparatus configuration of the fourth embodiment and a conventional current drawing method as an example, and the effect of the present invention was confirmed.

図10は従来の基本的な電流引込法のシミュレーション波形図である。この場合の可変速周波数指令は、時刻0.05Sの時点までに指令した電流値になるように電流制御により直流電流を確立させ、時刻0.05S〜0.25Sの期間で0%から10%の速度まで周波数を連続的に増加させた。そして、時刻0.4Sから0.65Sの間に今度は10%から0%速度に連続的に周波数を減少させ、そのまま引き続いて時刻0.65S〜0.85Sにかけて0%から−10%速度まで逆転方向に周波数を増加させている。   FIG. 10 is a simulation waveform diagram of the conventional basic current drawing method. In this case, the variable speed frequency command establishes a direct current by current control so that the current value is commanded up to the time of 0.05S, and 0% to 10% in the period of 0.05S to 0.25S. The frequency was continuously increased to the speed of. Then, between time 0.4S and 0.65S, the frequency is continuously reduced from 10% to 0% speed, and then from 0% to -10% speed from time 0.65S to 0.85S. The frequency is increased in the reverse direction.

図10のチャートの第1段は2軸電流成分を示したものである。ここには制御軸γ−δ軸の電流指令と、実際の磁極軸d軸とq軸の実電流成分を示している。制御基準であるγ−δ座標成分に換算した実電流は、ほぼ指令値と等しい電流が流れているので省略している。制御軸の電流が安定していても、実際の磁極軸d軸とγ軸との位相差ψが存在するため、実際のd軸電流とq軸電流はこの位相差ψに応じて変動する。このd軸とq軸電流の脈動状態からも軸位相が振動的であることが推定できる。   The first stage of the chart of FIG. 10 shows the biaxial current component. Here, the current command of the control axis γ-δ axis and the actual current components of the actual magnetic pole axis d-axis and q-axis are shown. The actual current converted to the control reference γ-δ coordinate component is omitted because a current substantially equal to the command value flows. Even if the current of the control axis is stable, there is a phase difference ψ between the actual magnetic pole axis d-axis and the γ-axis, so the actual d-axis current and the q-axis current vary according to this phase difference ψ. From the pulsation state of the d-axis and q-axis currents, it can be estimated that the axis phase is oscillatory.

第2段は、三相の交流電流波形であり、電流指令どおりの一定振幅でかつ周波数指令どおりに電流が流れていることが確認できる。   The second stage is a three-phase alternating current waveform, and it can be confirmed that a current flows with a constant amplitude according to the current command and according to the frequency command.

第3段は、モータの回転子に発生するトルクを示している。このトルクにはモータの出力軸成分ではなくモータの回転子の慣性モーメントを加減速するためのトルク成分も含まれている。トルク波形からも振動的であることが分かる。   The third stage shows the torque generated in the rotor of the motor. This torque includes not only the output shaft component of the motor but also a torque component for accelerating / decelerating the inertia moment of the rotor of the motor. From the torque waveform, it can be seen that it is vibrational.

第4段目は、周波数指令とモータ回転子の実速度を比較したものである。台形波形の周波数指令に対して、回転子速度には振動的な正負の偏差が生じている。   The fourth stage compares the frequency command and the actual speed of the motor rotor. In contrast to the trapezoidal waveform frequency command, a positive and negative deviation occurs in the rotor speed.

第5段目は電流差分成分とそれにバンドパスフィルタをかけた成分、そしてこれに周波数重みを乗算したものである。電流差分成分に対して、直流分か抑制されていること、速度が零付近では補償量が強制的に零に抑制されていること、そして、周波数の極性が反転すると補償量の正負の極性が反転していることが確認できる。   The fifth level is a current difference component, a component obtained by applying a band pass filter to the current difference component, and a frequency weight multiplied by this. For the current difference component, the direct current component is suppressed, the compensation amount is forcibly suppressed to zero when the speed is near zero, and the polarity of the compensation amount becomes positive or negative when the polarity of the frequency is reversed. It can be confirmed that it is reversed.

しかし、この補償演算量はまだ周波数に対して加算していないので、発生した振動は減衰せず持続しやすい。   However, since the compensation calculation amount has not yet been added to the frequency, the generated vibration is not attenuated and tends to be sustained.

図11は、本発明の実施形態4の振動抑制を適用した例であり、上記の周波数補正量を指令周波数に加算補正した。   FIG. 11 is an example in which the vibration suppression of the fourth embodiment of the present invention is applied, and the above frequency correction amount is added and corrected to the command frequency.

第4段目の速度を見れば振動成分が抑制されていることがよく分かる。その結果γ軸とd軸間との位相角ψの変動が緩やかになり、その結果第2段目のトルク波形のように振動し始めても緩やかに減衰する特性を実現できている。   It can be clearly seen that the vibration component is suppressed by looking at the speed of the fourth stage. As a result, the fluctuation of the phase angle ψ between the γ-axis and the d-axis becomes gradual, and as a result, even if it starts to oscillate like the torque waveform in the second stage, a characteristic that gently attenuates can be realized.

また、この振動抑制効果は逆転周波数でも有効である。また、零速度領域では補償が停止しているが、周波数指令が零速度領域を短時間で通過する場合には、振動が大きくなる前に零速度域を通過できている。   This vibration suppression effect is also effective at the reverse frequency. Further, although the compensation is stopped in the zero speed region, when the frequency command passes through the zero speed region in a short time, it can pass through the zero speed region before the vibration becomes large.

【0005】
速度起電力を利用した磁極位相推定方法だけでは正確な磁極位相を推定できない。また、(b)の方法は磁気的な突極性を利用するため、磁気的に突極性のない非突極機にはそのまま適用することができない。また、電流引込法を適用した場合には軸ねじれ振動を招く問題が残る。また、(c)の方法は、大容量の電力変換器を必要とするなどの問題がある。
[0022]
本発明の目的は、磁気的に突極性のないPMモータの磁極位相を定格速度の10%以下などの低い速度まで精度良く推定でき、この磁極位相の推定を基にした電流引込法による速度振動(軸振動)の抑制および脱調を防止できる永久磁石同期電動機の位置センサレス制御装置を提供することにある。
[0023]
本発明に用いる前記の零電圧ベクトル期間の電流微分情報は、デッドタイムの影響を受けないため、従来のPWM制御に入力する電圧指令などを利用する磁極位相推定方法よりも、より低い速度から速度起電力情報が得られる可能性があることに着目し、零電圧ベクトル期間の電流微分情報を検出して速度起電力情報を取得し、この速度起電力を利用した磁極位相推定方法で磁極位相を推定し、この推定した磁極位相を基に磁気的に突極性のないPMモータに電流引込法を適用した場合の速度振動(軸振動)の抑制をするようにしたもので、以下の構成を特徴とする。
[0024]
(1)非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θの振動情報を推定して角周波数指令を補正する手段を有する永久磁石同期電動機の制御装置であって、
前記角周波数指令を補正する手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、各前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記2点以上の時刻t2n、t(2n+1)の電流検出値から電流差分を演算する電流
[0005]
An accurate magnetic pole phase cannot be estimated only by the magnetic pole phase estimation method using velocity electromotive force. Further, since the method (b) uses magnetic saliency, it cannot be applied as it is to a non-salient pole machine having no magnetic saliency. Further, when the current drawing method is applied, there remains a problem that causes shaft torsional vibration. Further, the method (c) has a problem that a large capacity power converter is required.
[0022]
It is an object of the present invention to accurately estimate the magnetic pole phase of a PM motor having no magnetic saliency up to a low speed such as 10% or less of the rated speed, and to perform velocity oscillation by a current drawing method based on the estimation of the magnetic pole phase. An object of the present invention is to provide a position sensorless control device for a permanent magnet synchronous motor that can suppress (shaft vibration) and prevent step-out.
[0023]
Since the current differential information of the zero voltage vector period used in the present invention is not affected by the dead time, the speed is reduced from a lower speed than the magnetic pole phase estimation method using a voltage command or the like input to the conventional PWM control. Focusing on the possibility that electromotive force information can be obtained, current differential information during zero voltage vector period is detected to obtain speed electromotive force information, and the magnetic pole phase is estimated by the magnetic pole phase estimation method using this speed electromotive force. Based on this estimated magnetic pole phase, velocity vibration (shaft vibration) is suppressed when the current drawing method is applied to a PM motor with no magnetic saliency. And
[0024]
(1) A synchronous motor using a permanent magnet that is a non-salient pole machine and has no damper winding as a field source is started by following the current phase of the magnetic pole phase θ, and the vibration information of the magnetic pole phase θ is estimated. A control device for a permanent magnet synchronous motor having means for correcting an angular frequency command,
The means for correcting the angular frequency command is:
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental wave current detection unit (8) for detecting current at times t 2n and t (2n + 1) at least two points during each of the zero voltage vector periods;
A current for calculating a current difference from current detection values at times t 2n and t (2n + 1) at two or more points.

【0006】
差分検出部(11)と、
前記時刻t2n,t2n+1の時間差ΔTpと前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ωより速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した値と前記速度起電力との乗算値となる電流差分成分を出力する電流差分成分演算部(12)と、
前記電流差分検出部の出力と前記電流差分成分演算部の出力は正値と負値であるので、加算によりこの2種類の電流差分の誤差分を求め、この加算値をフィルタで直流分を除去して補正ゲインKを乗算し、さらに前記補正ゲインKを乗算した出力に周波数が零付近では補償量の大きさを零に抑圧する角周波数重み関数Kωを乗じることにより補正角周波数Δω を演算し、これを前記角周波数指令ωに加算して新しい角周波数指令ω を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする。
[0025]
(2)非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θの振動情報を推定して角周波数指令を補正する手段を有する永久磁石同期電動機の制御装置であって、
前記角周波数指令を補正する手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記2点以上の時刻t2n、t(2n+1)の電流検出値から電流差分を演算する電流差分検出部(11)と、
前記電流差分をフィルタにより直流分を除去して補正ゲインを乗算し、さらに前記補正ゲインKを乗算した出力に周波数が零付近では補償量の大きさを零に抑圧する角周波数重み関数Kωを乗じることにより補正角周波数Δω を演算し、これを角周波数指令ωに加算して新しい角周波数指令ω を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする。
[0006]
A difference detector (11);
The speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L, and the angular frequency command ω * , and the value obtained by dividing the time difference ΔTp by the inductance L A current difference component calculation unit (12) that outputs a current difference component that is a multiplication value of the speed electromotive force;
Since the output of the current difference detection unit and the output of the current difference component calculation unit are a positive value and a negative value, the difference between the two types of current difference is obtained by addition, and the direct current component is removed by a filter. to the correction gain K p multiplies, further the correction gain K p corrected angular frequency Δω by frequency output obtained by multiplying the in multiplying the angular frequency weighting function K omega to suppress the zero magnitude of the compensation amount in the vicinity of zero calculating a p *, which was added to the angular frequency command omega * calculates a new angular frequency command omega p * corrected angular frequency command calculation section (13 to 15),
It is provided with.
[0025]
(2) The magnetic pole phase θ of a synchronous motor that uses a permanent magnet that is a non-salient pole machine and has no damper winding as a field source is started by following the current phase, and vibration information of the magnetic pole phase θ is estimated. A control device for a permanent magnet synchronous motor having means for correcting an angular frequency command,
The means for correcting the angular frequency command is:
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental current detection unit (8) that detects current at times t 2n and t (2n + 1) at least two points during the zero voltage vector period;
A current difference detector (11) that calculates a current difference from current detection values at times t 2n and t (2n + 1) at two or more points;
The current differences by removing the DC component is multiplied by the correction gain by the filter, further the correction gain K p in the vicinity of the frequency is zero in the output obtained by multiplying the compensation amount of the angular frequency weighting function to suppress the magnitude to zero K omega A corrected angular frequency command calculation unit (13 to 15) that calculates a corrected angular frequency Δω p * by multiplying by and adds this to the angular frequency command ω * to calculate a new angular frequency command ω p * ;
It is provided with.

【0007】
[0026]
(3)非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θの振動情報を推定して各周波数指令を補正する手段を有する永久磁石同期電動機の制御装置であって、
前記角周波数指令を補正する手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、前記零電圧ベクトル期間中に三角波キャリア信号の上下限の頂点に対して対称な少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記上アームと下アーム2種類の零電圧ベクトル期間(V7,V0)の頂点に対して対称な2点以上の時刻t2n、t(2n+1)の電流検出値の電流成分の平均値を求め、前記時刻t2n,t2n+1の時間差ΔTpと、前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ωより速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した値と前記速度起電力との乗算値となる電流差分成分について、V7とV0の2種類の検出期間の成分を平均して出力する平均値演算部(12A)と、
前記基本波電流検出部(8)が出力する零電圧ベクトル期間の頂点に対して対称な2点以上の時刻t2n,t(2n+1)における電流検出値の電流差分の平均値出力と前記電流差分成分の平均値演算部(12A)の出力は、それぞれ正値と負値であるので、加算(12C)によりこの2種類の電流差分の誤差分を求め、この加算値をフィルタで直流分を除去して補正ゲインKを乗算し、さらに前記補正ゲインK乗算した出力に周波数が零付近では補償量の大きさを零に抑圧する角周波数重み関数Kωを乗じることにより補正角周波数Δω を演算し、これを前記角周波数指令ωに加算して新しい角周波数指令ω を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする。
[0027]
(4)非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θの振動情報を推定して各周波数指令を補正する手段を有する永久磁石同期電動機の制御装置で
[0007]
[0026]
(3) A synchronous motor using a permanent magnet which is a non-salient pole machine and has no damper winding as a field source is started by following the current phase of the magnetic pole phase θ, and the vibration information of the magnetic pole phase θ is estimated. A control device for a permanent magnet synchronous motor having means for correcting each frequency command,
The means for correcting the angular frequency command is:
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental wave current detection unit (8) for detecting currents at times t 2n and t (2n + 1) at least two points symmetrical with respect to the upper and lower vertices of the triangular wave carrier signal during the zero voltage vector period;
An average value of current components of current detection values at two or more times t 2n and t (2n + 1) symmetrical with respect to the vertices of the zero voltage vector period (V7, V0) of the upper arm and the lower arm is obtained. A speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L, and the angular frequency command ω * , and the value obtained by dividing the time difference ΔTp by the inductance L An average value calculation unit (12A) that averages and outputs components of two types of detection periods of V7 and V0 for a current difference component that is a product of the speed electromotive force,
An average value output of current differences of current detection values at two or more times t 2n and t (2n + 1) symmetrical with respect to the vertex of a zero voltage vector period output from the fundamental wave current detection unit (8) and the current difference Since the output of the component average value calculation unit (12A) is a positive value and a negative value, respectively, an error amount of these two kinds of current differences is obtained by addition (12C), and the direct current component is removed by using this added value with a filter. Then, the correction gain K p is multiplied, and when the frequency multiplied by the correction gain K p is multiplied by an angular frequency weighting function K ω that suppresses the amount of compensation to zero when the frequency is near zero, the correction angular frequency Δω p * the calculated corrected angular frequency command calculating unit for calculating the said angular frequency command omega * new angular frequency command omega is added to the p * At the (13-15),
It is provided with.
[0027]
(4) Start a synchronous motor having a non-salient pole machine having a permanent magnet without a damper winding as a field source by making the magnetic pole phase θ follow the current phase, and estimate the vibration information of the magnetic pole phase θ. A control device for a permanent magnet synchronous motor having means for correcting each frequency command.

【0008】
あって、
前記角周波数指令を補正する手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間において、前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記上アームの零電圧ベクトル期間(V7)と下アームの零電圧ベクトル期間(V0)の2種類の検出期間における前記2点以上の時刻t2n、t(2n+1)の電流成分を移動平均し、前記時刻t2n、t2n+1の時間差ΔTpと、前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ωより速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した値と前記速度起電力との乗算値となる電流差分成分を出力する移動平均値演算部(12B)と、
前記基本波電流検出部(8)が出力する零電圧ベクトル期間の頂点に対して対称な2点以上の時刻t2n,t(2n+1)における電流検出値の電流差分の平均値出力と移動平均値演算部(12B)のそれぞれの出力は正値と負値であるので、加算によりこの2種類の電流差分の誤差分を求め(12C)、この加算値をフィルタで直流分を除去して補正ゲインKを乗算し、さらに前記補正ゲインKp乗算した出力に周波数が零付近では補償量の大きさを零に抑圧する角周波数重み関数Kωを乗じることにより補正角周波数Δω を演算し、これを前記角周波数指令ωに加算して新しい角周波数指令ω を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする。
[0028]
以上のとおり、本発明によれば、零電圧ベクトル期間の電流微分情報を利用して速度起電力情報を取得し、この速度起電力を利用した磁極位相推定方法で磁極位相を推定し、この推定した磁極位相を基に磁気的に突極性のないPMモータの磁極位相θを電流位相に追従させて始動する電流引込法を適用した場合の制御方法に対して、の振動抑制を追加したことにより、磁気的に突極性のないPMモータの磁極位相の推定を基に
[0008]
There,
The means for correcting the angular frequency command is:
During the zero voltage vector period in the output voltage period by PWM control, the zero voltage vector period in which the switching element of the upper arm is conducted in all three phases or the zero voltage vector period in which the switching element of the lower arm is conducted in all three phases A fundamental wave current detector (8) for detecting currents at times t 2n and t (2n + 1) at least two points at
A moving average of current components at times t 2n and t (2n + 1) at two or more points in two types of detection periods of the upper arm zero voltage vector period (V7) and the lower arm zero voltage vector period (V0), A speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L, and the angular frequency command ω * , and the value obtained by dividing the time difference ΔTp by the inductance L A moving average value calculation unit (12B) that outputs a current difference component that is a multiplication value of the speed electromotive force;
The average value output and moving average value of the current difference of the current detection values at two or more times t 2n , t (2n + 1) symmetrical with respect to the vertex of the zero voltage vector period output by the fundamental wave current detection unit (8). Since each output of the calculation unit (12B) is a positive value and a negative value, an error amount between these two types of current difference is obtained by addition (12C), and the DC value is removed from the addition value by a filter to obtain a correction gain. A corrected angular frequency Δω p * is calculated by multiplying the output multiplied by K p and further multiplied by the correction gain Kp by an angular frequency weighting function K ω that suppresses the amount of compensation to zero when the frequency is near zero, A corrected angular frequency command calculation unit (13 to 15) for calculating a new angular frequency command ω p * by adding this to the angular frequency command ω * ,
It is provided with.
[0028]
As described above, according to the present invention, the speed electromotive force information is obtained using the current differential information in the zero voltage vector period, and the magnetic pole phase is estimated by the magnetic pole phase estimation method using the speed electromotive force. By adding vibration suppression to the control method in the case of applying the current pulling method that starts the magnetic pole phase θ of a PM motor with no magnetic saliency following the current phase based on the magnetic pole phase Based on the estimation of magnetic pole phase of PM motor without magnetic saliency

Claims (4)

非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θを推定する位相推定手段を有する永久磁石同期電動機の位置センサレス制御装置であって、
前記位相推定手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、各前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記2点以上の時刻t2n、t(2n+1)の電流検出値から電流差分を演算する電流差分検出部(11)と、
前記時刻t2n,t2n+1の時間差ΔTpと前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ω*より速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した除算値と前記速度起電力との乗算値となる電流差分成分に変換する電流差分成分演算部(12)と、
前記電流差分検出部の出力と前記電流差分成分演算部の出力を加算し、この加算値をフィルタで直流分を除去して補正ゲインKpを乗算し、さらに前記補正ゲインKpを乗算した出力に角周波数重み関数Kωを乗じることにより補正角周波数Δωp *を演算し、これを前記角周波数指令ω*に加算して新しい角周波数指令ωp *を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする永久磁石同期電動機の位置センサレス制御装置。
A permanent magnet having a phase estimation means for starting the magnetic pole phase θ of a synchronous motor having a field source as a permanent magnet which is a non-salient pole machine and does not have a damper winding, follows the current phase and estimates the magnetic pole phase θ. A position sensorless control device for a synchronous motor,
The phase estimation means includes
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental wave current detector (8) for detecting currents at times t 2n and t (2n + 1) at least two points during each of the zero voltage vector periods;
A current difference detector (11) that calculates a current difference from current detection values at times t 2n and t (2n + 1) at two or more points;
A speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L, and the angular frequency command ω * , and the time difference ΔTp is divided by the inductance L. A current difference component calculation unit (12) that converts a current difference component that is a product of the value and the speed electromotive force;
An output obtained by adding the output of the current difference detection unit and the output of the current difference component calculation unit, removing the DC component by a filter, multiplying the sum by a correction gain K p , and further multiplying the correction gain K p angular frequency weight multiplied by the function K omega calculates the correction angle frequency [Delta] [omega p *, the correction angular frequency command calculator for calculating the angular frequency command omega * to a new angular frequency command omega p * by adding this to the ( 13-15)
A position sensorless control device for a permanent magnet synchronous motor, comprising:
非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θを推定する位相推定手段を有する永久磁石同期電動機の位置センサレス制御装置であって、
前記位相推定手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記2点以上の時刻t2n、t(2n+1)の電流検出値から電流差分を演算する電流差分検出部(11)と、
前記電流差分をフィルタにより直流分を除去して補正ゲインを乗算し、さらに前記補正ゲインKpを乗算した出力に角周波数重み関数Kωを乗じることにより補正角周波数Δωp *を演算し、これを前記角周波数指令ω*に加算して新しい角周波数指令ωp *を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする永久磁石同期電動機の位置センサレス制御装置。
A permanent magnet having a phase estimation means for starting the magnetic pole phase θ of a synchronous motor having a field source as a permanent magnet which is a non-salient pole machine and does not have a damper winding, follows the current phase and estimates the magnetic pole phase θ. A position sensorless control device for a synchronous motor,
The phase estimation means includes
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental current detector (8) for detecting currents at times t 2n and t (2n + 1) at least two points during the zero voltage vector period;
A current difference detector (11) that calculates a current difference from current detection values at times t 2n and t (2n + 1) at two or more points;
A correction angular frequency Δω p * is calculated by multiplying an output obtained by removing the DC component from the current difference by a filter and multiplying the correction gain by the filter, and multiplying the output multiplied by the correction gain K p by an angular frequency weighting function K ω. the was added to the angular frequency command omega * calculates a new angular frequency command omega p * corrected angular frequency command calculation section (13 to 15),
A position sensorless control device for a permanent magnet synchronous motor, comprising:
非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θを推定する位相推定手段を有する永久磁石同期電動機の位置センサレス制御装置であって、
前記位相推定手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間(V7)、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間(V0)において、前記零電圧ベクトル期間中に三角波キャリア信号の上下限の頂点に対して対称な少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記上アームと下アーム2種類の零電圧ベクトル期間(V7,V0)の頂点に対して対称な2点以上の時刻t2n、t(2n+1)の電流検出値の電流差分の平均値を求め、前記時刻t2n,t2n+1の時間差ΔTpと、前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ω*より速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した除算値と前記速度起電力との乗算値となる電流差分成分に変換する電流差分成分の平均値演算部(12A)と、
前記電流検出部の電流差分の平均値出力と電流差分成分演算部の出力を加算(12C)し、この加算値をフィルタで直流分を除去して補正ゲインKpを乗算し、さらに前記補正ゲインKp乗算した出力に角周波数重み関数Kωを乗じることにより補正角周波数Δωp *を演算し、これを前記角周波数指令ω*に加算して新しい角周波数指令ωp *を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする永久磁石同期電動機の位置センサレス制御装置。
A permanent magnet having a phase estimation means for starting the magnetic pole phase θ of a synchronous motor having a field source as a permanent magnet which is a non-salient pole machine and does not have a damper winding, follows the current phase and estimates the magnetic pole phase θ. A position sensorless control device for a synchronous motor,
The phase estimation means includes
In the output voltage period by PWM control, in the zero voltage vector period (V7) in which the switching element of the upper arm is conducted in all three phases, or in the zero voltage vector period (V0) in which the switching element of the lower arm is conducted in all three phases, A fundamental wave current detector (8) for detecting currents at times t 2n and t (2n + 1) at least two points symmetrical with respect to the upper and lower vertices of the triangular wave carrier signal during the zero voltage vector period;
The average value of the current difference of the current detection values at time t 2n and t (2n + 1) at two or more points symmetrical with respect to the vertices of the zero voltage vector period (V7, V0) of the upper arm and the lower arm. The speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L, and the angular frequency command ω * , and the time difference ΔTp is calculated by the inductance L. An average value calculation unit (12A) of a current difference component that is converted into a current difference component that is a multiplication value of the divided value divided by the speed electromotive force;
The average value output of the current difference of the current detection unit and the output of the current difference component calculation unit are added (12C), the DC value is removed by a filter, and the correction gain Kp is multiplied. K p and calculates the correction angle frequency [Delta] [omega p * by multiplying the angular frequency weighting function K omega output multiplication, it calculates the angular frequency command omega * to a new angular frequency command omega p * by adding this correction angle A frequency command calculation unit (13 to 15);
A position sensorless control device for a permanent magnet synchronous motor, comprising:
非突極機でかつダンパ巻線を有しない永久磁石を界磁源とする同期電動機の磁極位相θを電流位相に追従させて始動し、前記磁極位相θを推定する位相推定手段を有する永久磁石同期電動機の位置センサレス制御装置であって、
前記位相推定手段は、
PWM制御による出力電圧期間のうち、三相とも上アームのスイッチング素子が導通する零電圧ベクトル期間、または、三相とも下アームのスイッチング素子が導通する零電圧ベクトル期間において、前記零電圧ベクトル期間中に少なくとも2点以上の時刻t2n、t(2n+1)の電流を検出する基本波電流検出部(8)と、
前記2点以上の時刻t2n、t(2n+1)の電流検出値から電流差分を演算する電流差分検出部(11)と、
前記上アームの零電圧ベクトル期間(V7)と下アームの零電圧ベクトル期間(V0)の2種類の検出期間における前記2点以上の時刻t2n、t(2n+1)の電流差分を移動平均し、前記時刻t2n、t2n+1の時間差ΔTpと、前記同期電動機の抵抗Rによる電圧降下分とインダクタンスLおよび角周波数指令ω*より速度起電力を演算し、前記時間差ΔTpをインダクタンスLで除した除算値と前記速度起電力との乗算値となる電流差分成分に変換する電流差分成分の平均値演算部(12B)と、
前記電流検出部の電流差分と電流差分成分演算部の出力を加算(12C)し、この加算値をフィルタで直流分を除去して補正ゲインKpを乗算し、さらに前記補正ゲインKp乗算した出力に角周波数重み関数Kωを乗じることにより補正角周波数Δωp *を演算し、これを前記角周波数指令ω*に加算して新しい角周波数指令ωp *を演算する補正角周波数指令演算部(13〜15)と、
を備えたことを特徴とする永久磁石同期電動機の位置センサレス制御装置。
A permanent magnet having a phase estimation means for starting the magnetic pole phase θ of a synchronous motor having a field source as a permanent magnet which is a non-salient pole machine and does not have a damper winding, follows the current phase and estimates the magnetic pole phase θ. A position sensorless control device for a synchronous motor,
The phase estimation means includes
During the zero voltage vector period in the output voltage period by PWM control, the zero voltage vector period in which the switching element of the upper arm is conducted in all three phases or the zero voltage vector period in which the switching element of the lower arm is conducted in all three phases A fundamental wave current detector (8) that detects currents at times t 2n and t (2n + 1) at least at two points;
A current difference detector (11) that calculates a current difference from current detection values at times t 2n and t (2n + 1) at two or more points;
A moving average of current differences at times t 2n and t (2n + 1) at two or more points in two types of detection periods of the upper arm zero voltage vector period (V7) and the lower arm zero voltage vector period (V0). Then, the speed electromotive force is calculated from the time difference ΔTp between the times t 2n and t 2n + 1 , the voltage drop due to the resistance R of the synchronous motor, the inductance L and the angular frequency command ω * , and the time difference ΔTp is calculated by the inductance L. An average value calculation unit (12B) of current difference components to be converted into a current difference component that is a multiplication value of the divided value divided by the speed electromotive force;
Wherein adding the output of the current difference and the current difference component calculation unit of the current detecting portion (12C), the added value by removing the DC component in the filter multiplied by the correction gain K p, multiplied further the correction gain Kp Output angular frequency weight multiplied by the function K omega calculates the correction angle frequency [Delta] [omega p *, the correction angular frequency command calculator for calculating the angular frequency command omega * to a new angular frequency command omega p * by adding this to the ( 13-15)
A position sensorless control device for a permanent magnet synchronous motor, comprising:
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