JPH10262359A - Permanent magnet dynamo-electric machine - Google Patents
Permanent magnet dynamo-electric machineInfo
- Publication number
- JPH10262359A JPH10262359A JP9062708A JP6270897A JPH10262359A JP H10262359 A JPH10262359 A JP H10262359A JP 9062708 A JP9062708 A JP 9062708A JP 6270897 A JP6270897 A JP 6270897A JP H10262359 A JPH10262359 A JP H10262359A
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnet
- electric machine
- rotating electric
- magnet rotating
- induced voltage
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02T—CLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO TRANSPORTATION
- Y02T10/00—Road transport of goods or passengers
- Y02T10/60—Other road transportation technologies with climate change mitigation effect
- Y02T10/64—Electric machine technologies in electromobility
Landscapes
- Brushless Motors (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
- Permanent Magnet Type Synchronous Machine (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は永久磁石回転電機装
置に係り、小形軽量,高トルクの永久磁石回転電機、及
び電流容量の小さなスイッチング素子ですむインバータ
とを備えた永久磁石回転電機装置を提供するものであ
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a permanent magnet rotating electric machine, and more particularly, to a permanent magnet rotating electric machine having a small, lightweight, high-torque permanent magnet rotating electric machine, and an inverter having a switching element having a small current capacity. Is what you do.
【0002】[0002]
【従来の技術】電動車両、特に電気自動車において使用
される駆動電動機は電気自動車として積載されるバッテ
リの量が限定され、かつそれで十分一充電走行距離を確
保することが必要なために小型軽量,高効率であること
が望まれる。一方、車両としての加速性能,最高速の確
保等のために高トルクであること、弱め界磁に適した永
久磁石回転電機であることが要求される。2. Description of the Related Art Driving motors used in electric vehicles, particularly electric vehicles, are limited in the amount of batteries loaded as electric vehicles, and it is necessary to secure a sufficient mileage for one charge. High efficiency is desired. On the other hand, a high torque is required for the acceleration performance of the vehicle, the highest speed, and the like, and a permanent magnet rotating electric machine suitable for the field weakening is required.
【0003】以上の条件に適した電動機として永久磁石
回転電機が有効であり、特に永久磁石によるトルクと突
極性を利用したリラクタンストルクを有効に発生する方
式の永久磁石回転電機が効果的であることが、特開平2
−324232 号で開示されている。[0003] A permanent magnet rotating electric machine is effective as a motor suitable for the above conditions, and in particular, a permanent magnet rotating electric machine of a system that effectively generates reluctance torque utilizing the torque by the permanent magnet and saliency is effective. However, JP 2
-324232.
【0004】[0004]
【発明が解決しようとする課題】上記従来技術によれ
ば、永久磁石を永久磁石よりも高い透磁率を有する回転
子鉄心の中に配置し、かつ周方向に永久磁石と回転子鉄
心とで構成される補助磁極とを並置した構成を示してい
る。一方、固定子は分布巻の固定子で永久磁石回転子の
回転に同期して滑らかな回転磁界を作り出す構成であ
る。According to the above prior art, a permanent magnet is arranged in a rotor core having a higher permeability than a permanent magnet, and is constituted by a permanent magnet and a rotor core in a circumferential direction. A configuration in which auxiliary magnetic poles are arranged side by side. On the other hand, the stator is a distributed winding stator and is configured to generate a smooth rotating magnetic field in synchronization with the rotation of the permanent magnet rotor.
【0005】このように永久磁石を永久磁石よりも高い
透磁率を有する磁性材からなる回転子鉄心の中に配置す
るすなわち内部磁石回転子構成とすることによって弱め
界磁が可能となり、高効率でかつ高速領域までの運転が
可能となる。[0005] By arranging the permanent magnet in the rotor core made of a magnetic material having a higher magnetic permeability than the permanent magnet, that is, by employing an internal magnet rotor configuration, a field weakening is possible, and high efficiency is achieved. In addition, operation up to the high-speed range is possible.
【0006】しかし、永久磁石を弱め界磁する回転電機
において、高速運転時にインバータが故障すると弱め界
磁制御が不能となり、永久磁石回転電機の線間には高電
圧が発生し、バッテリに大きなパワーを戻すことにな
る。これは、第1には、急ブレーキが生じ、走行車両姿
勢の不安定を招く。第2にはバッテリ,平滑コンデン
サ,インバータ等を損傷せしめる可能性がある点で問題
がある。However, in a rotating electric machine that weakens a permanent magnet, if the inverter fails during high-speed operation, field weakening control becomes impossible, a high voltage is generated between the lines of the permanent magnet rotating electric machine, and large power is returned to the battery. Will be. This firstly causes sudden braking and instability of the posture of the traveling vehicle. Second, there is a problem in that the battery, the smoothing capacitor, the inverter and the like may be damaged.
【0007】また、上記従来技術では一般にトルク発生
に寄与する永久磁石の磁束の割合が少ないためにその発
生する誘起電圧は比較的小さく押さえられるが、それで
も最高速での発生誘起電圧は非常に大きなものとなる。Further, in the above prior art, since the ratio of the magnetic flux of the permanent magnet which contributes to the generation of torque is generally small, the induced voltage generated is suppressed to a relatively small value. However, the generated induced voltage at the highest speed is still very large. It will be.
【0008】さらに、分布巻固定子の永久磁石電動機等
の場合はスロットリプルによる誘起電圧の跳ね上がりに
よって一層深刻になる場合もある。Further, in the case of a permanent magnet motor of a distributed winding stator or the like, there is a case where the induced voltage jumps due to the slot ripple and becomes more serious.
【0009】実際には以上を避けるためには第1にはイ
ンバータと回転電機の間にコンタクタを挿入し、故障時
に永久磁石回転電機をインバータより切り離す方法、第
2には誘起電圧を低く設定する方法があるが、第1の方
法では、コンタクタのスペース,重量等がネックで、他
の電動機例えば誘導電動機に対する優位点が損なわれ
る。また、第2の点ではリラクタンストルク成分に期待
する比率が大きく、電動機の体格を大きくすること、及
びトルクを発生するのに必要な電流が増加し、インバー
タの電流容量をいたずらに増加させる結果を生ぜしめる
欠点がある。In practice, in order to avoid the above, first, a method of inserting a contactor between the inverter and the rotating electric machine to disconnect the permanent magnet rotating electric machine from the inverter when a failure occurs, and secondly, setting the induced voltage low. There is a method, but in the first method, the space and weight of the contactor are a bottleneck, and the advantage over other electric motors, for example, induction motors, is lost. In the second point, the expected ratio of the reluctance torque component is large, and the result is that the physical size of the motor is increased, the current required to generate the torque is increased, and the current capacity of the inverter is unnecessarily increased. There are drawbacks that can occur.
【0010】本発明は故障時の誘起電圧のピーク値を低
減し、これによって小形軽量,高トルクの永久磁石回転
電機、及び電流容量の小さなスイッチング素子ですむイ
ンバータとを備えた永久磁石回転電機装置を提供するこ
とを目的とするものである。The present invention reduces the peak value of the induced voltage at the time of a failure, thereby reducing the size and weight of the permanent magnet rotating electric machine with a high torque, and a permanent magnet rotating electric machine equipped with an inverter that requires only a switching element having a small current capacity. The purpose is to provide.
【0011】[0011]
【課題を解決するための手段】本発明は、直流電源と、
それに接続されるインバータにより回転速度が制御され
る永久磁石回転電機と、該永久磁石回転電機を弱め界磁
制御する手段とを備えてなる永久磁石回転電機装置にお
いて、前記永久磁石回転電機の端子間の発生誘起電圧の
ピーク値をVpとし、その基本波電圧のピーク値をVp
1としたとき、Vp<Vp1の誘起電圧値となさしめる
ことによって達成される。SUMMARY OF THE INVENTION The present invention comprises a DC power supply,
In a permanent magnet rotating electric machine comprising: a permanent magnet rotating electric machine whose rotation speed is controlled by an inverter connected to the permanent magnet rotating machine; The peak value of the induced voltage is defined as Vp, and the peak value of the fundamental wave voltage is defined as Vp.
When it is set to 1, it is achieved by setting an induced voltage value of Vp <Vp1.
【0012】本発明の好ましくは、永久磁石回転電機の
端子間の発生誘起電圧の中心の電圧値をVmとし、その
発生誘起電圧のピーク値をVpとしたとき、Vm<Vp
の誘起電圧値となさしめたことによって達成される。Preferably, Vm <Vp, where Vm is a voltage value at the center of the induced voltage between terminals of the permanent magnet rotating electric machine, and Vp is a peak value of the induced voltage.
Is achieved by setting the induced voltage value of
【0013】本発明の好ましくは、永久磁石回転電機の
コイル幅を永久磁石回転子の磁極の幅にほぼ等しくした
ことによって達成される。Preferably, the present invention is attained by making the coil width of the permanent magnet rotating electric machine substantially equal to the width of the magnetic pole of the permanent magnet rotor.
【0014】本発明の好ましくは、永久磁石回転子の磁
極中心の空隙長を磁極端の空隙長より大ならしめること
によって達成される。Preferably, the present invention is achieved by making the gap length at the center of the magnetic pole of the permanent magnet rotor larger than the gap length at the pole tip.
【0015】本発明の好ましくは、同じ相に属する固定
子巻線を巻回した複数の固定子突極が電気的にすべて同
相の位置に配置することによって達成される。Preferably, the present invention is attained by arranging a plurality of stator salient poles on which stator windings belonging to the same phase are wound at electrically in-phase positions.
【0016】本発明の好ましくは、低回転数での定トル
ク範囲と高速時の定出力運転範囲とを有し、かつ定トル
ク範囲の最高回転数をN1,定出力範囲の最高回転数を
N2としたとき、N2/N1が2以上であることによっ
て達成される。Preferably, the present invention has a constant torque range at a low rotation speed and a constant output operation range at a high speed, and the maximum rotation speed in the constant torque range is N1, and the maximum rotation speed in the constant output range is N2. Is achieved by N2 / N1 being 2 or more.
【0017】[0017]
【発明の実施の形態】以下、本発明の実施例について説
明する。Embodiments of the present invention will be described below.
【0018】図1は本発明にかかわる永久磁石回転電機
装置の一実施例を、図2に本発明の永久磁石回転電機の
構造を、図3に本発明の永久磁石回転電機の断面構造を
示す。FIG. 1 shows an embodiment of a permanent magnet rotating electric machine according to the present invention, FIG. 2 shows a structure of the permanent magnet rotating electric machine of the present invention, and FIG. 3 shows a sectional structure of the permanent magnet rotating electric machine of the present invention. .
【0019】図2,図3において永久磁石回転電機は固
定子1と回転子2とからなり、該固定子1は積層された
鉄心からなりスロット部11に絶縁材を介して固定子巻
線3を巻装している。ここで、固定子構造は一般に広く
使用されている分布巻固定子構造であって、例えば、固
定子鉄心は歯部12とで磁気回路を形成するヨーク部1
3とからなり、固定子巻線3は固定子鉄心の空隙面に近
い部分のスリット部14からスロット部11に収納され
る。2 and 3, the permanent magnet rotating electric machine comprises a stator 1 and a rotor 2. The stator 1 is composed of a laminated iron core and a stator winding 3 having a slot portion 11 interposed with an insulating material. Is wound. Here, the stator structure is a generally used distributed winding stator structure. For example, the stator core includes a yoke portion 1 that forms a magnetic circuit with the tooth portion 12.
The stator winding 3 is housed in the slot 11 from the slit 14 near the gap surface of the stator core.
【0020】回転子2は高透磁率磁性材料である、例え
ば珪素鋼板よりなる積層鉄心と、その積層鉄心に設けら
れた永久磁石挿入孔21に挿入された永久磁石22とシ
ャフト4とからなる。この高透磁率磁性材料からなる積
層鉄心は隣り合う永久磁石22間に設けられた補助磁極
部23と永久磁石22の外周に設けられた磁極片部24
とヨーク部13とを備え、このヨーク部には前記した永
久磁石挿入孔21とシャフト4を通す孔が打ち抜かれ
る。この永久磁石回転子2の回転方向は反時計方向に回
転し、電動機として運転するものとする。ここで、使用
する永久磁石22は直方体にしてあるため、弧状の磁石
に比較して寸法精度が確保しやすく、回転子のバランス
作業なしに高速回転に供することができる。また永久磁
石22には高性能磁石であるネオジウム磁石等が使用さ
れるものとする。The rotor 2 comprises a laminated core made of a magnetic material having high magnetic permeability, for example, a silicon steel plate, a permanent magnet 22 inserted into a permanent magnet insertion hole 21 provided in the laminated core, and the shaft 4. The laminated core made of the high magnetic permeability magnetic material includes an auxiliary magnetic pole portion 23 provided between the adjacent permanent magnets 22 and a magnetic pole piece portion 24 provided on the outer periphery of the permanent magnet 22.
And a yoke portion 13, in which a hole for passing the permanent magnet insertion hole 21 and the shaft 4 is punched. The rotation direction of the permanent magnet rotor 2 rotates counterclockwise and operates as an electric motor. Here, since the permanent magnet 22 to be used is a rectangular parallelepiped, dimensional accuracy is easily ensured as compared with an arc-shaped magnet, and the rotor can be used for high-speed rotation without a balancing operation of the rotor. Further, a neodymium magnet or the like, which is a high-performance magnet, is used as the permanent magnet 22.
【0021】図3に本発明の永久磁石回転電機の断面構
造図を示す。回転電機の固定子1は一対のハウジング1
0,101の内周面に固定されている。ここで、固定子
鉄心のスロット部11は24個で永久磁石回転子の極数
8に対して毎極毎相あたりのスロット数が1の例で示し
てある。これが2,3と増加しても同様である。FIG. 3 is a sectional structural view of a permanent magnet rotating electric machine according to the present invention. The stator 1 of the rotating electric machine includes a pair of housings 1.
0, 101 are fixed to the inner peripheral surface. Here, an example is shown in which the number of slots 11 of the stator core is 24, and the number of slots per phase is 1 for 8 poles of the permanent magnet rotor. The same applies even if this increases to a few.
【0022】シャフト4はベアリング10a,10bを
介してハウジング10,101に回転自在に保持されて
いる。ここで、PSは回転子2の永久磁石22の位置を
検出する磁極位置検出器であり、Eは回転子2の位置を
検出するエンコーダである。回転電機はこの磁極位置検
出器PSの信号と、エンコーダEの出力信号により、制
御装置を介して運転制御される構成である。Eは速度制
御用の位置センサである。The shaft 4 is rotatably held by the housings 10 and 101 via bearings 10a and 10b. Here, PS is a magnetic pole position detector for detecting the position of the permanent magnet 22 of the rotor 2, and E is an encoder for detecting the position of the rotor 2. The operation of the rotating electric machine is controlled via a control device by a signal from the magnetic pole position detector PS and an output signal from the encoder E. E is a position sensor for speed control.
【0023】図1に本発明の永久磁石回転電機装置の制
御回路を示す。FIG. 1 shows a control circuit of the permanent magnet rotating electric machine according to the present invention.
【0024】図において、直流電源30よりインバータ
31を介して多相の固定子巻線3に電力を供給する。In the figure, a DC power supply 30 supplies power to a multi-phase stator winding 3 via an inverter 31.
【0025】速度制御回路(ASR)32では、速度指
令ωsと、エンコーダEよりの位置情報θからF/V変
換器33を介して得られる実際の速度ωfとから速度差
ωeを算出し、これにPI制御(P:比例項,I:積分
項)等によってトルク指令すなわち電流指令Isと回転
子2の回転角θ1を出力する。The speed control circuit (ASR) 32 calculates a speed difference ωe from the speed command ωs and the actual speed ωf obtained from the position information θ from the encoder E via the F / V converter 33, A torque command, that is, a current command Is and a rotation angle θ1 of the rotor 2 are output by PI control (P: proportional term, I: integral term) and the like.
【0026】一方、正弦波,余弦波発生器34では、回
転子2の永久磁石磁極の位置を検出する位置検出器PS
とエンコーダEよりのパルスすなわち回転子の位置情報
θから、固定子巻線3の各巻線(ここでは3相)の誘起
電圧と同相の正弦波出力、あるいは必要に応じて位相シ
フトした正弦波出力を発生する。On the other hand, the sine wave / cosine wave generator 34 has a position detector PS for detecting the position of the permanent magnet magnetic pole of the rotor 2.
And a pulse from the encoder E, that is, the rotor position information θ, a sine wave output in phase with the induced voltage of each winding (here, three phases) of the stator winding 3 or a sine wave output phase-shifted as necessary Occurs.
【0027】2相−3相変換回路35においては、電流
指令Isと正弦波,余弦波発生器34の出力に応じて各
相に電流指令Isa,Isb,Iscを出力する。各相
はそれぞれ個別に電流制御系(ACR)36を持ち、電
流指令Isa,Isb,Iscと電流検出器CTからの
電流検出信号Ifa,Ifb,Ifcに応じた信号をイ
ンバータ31に送って各相電流を制御する。この場合、
各相合成の電流は界磁磁束に直角、あるいは位相シフト
した位置(各相電流の合成の起磁力を永久磁石より90
度以上進ませる制御を弱め界磁制御という)電流を常に
形成し、これによって無整流子で、かつ直流機と同等の
特性を得ることができる。The two-phase to three-phase conversion circuit 35 outputs current commands Isa, Isb, Isc to each phase according to the current command Is and the output of the sine and cosine wave generators 34. Each phase has a current control system (ACR) 36 individually, and sends a signal corresponding to the current commands Isa, Isb, Isc and the current detection signals Ifa, Ifb, Ifc from the current detector CT to the inverter 31, Control the current. in this case,
The combined current of each phase is perpendicular to the field magnetic flux or at a position shifted in phase (the combined magnetomotive force of each phase current is 90
A current is always formed by weakening the control to advance by more than one degree, thereby obtaining a commutator-free characteristic equivalent to that of a DC machine.
【0028】以上の構成で、制御装置によって固定子巻
線3に流す電流のつくる電機子起磁力の合成ベクトルを
補助磁極部23の中心位置より回転方向側に向くように
制御することによって、回転電機は、永久磁石22によ
るトルクの他に補助磁極部23によるリラクタンストル
クを発生することができ、高トルクの電動機として運転
することができる。With the above configuration, the control device controls the combined vector of the armature magnetomotive force generated by the current flowing through the stator winding 3 so as to be directed to the rotation direction side from the center position of the auxiliary magnetic pole portion 23, thereby rotating the motor. The electric machine can generate a reluctance torque by the auxiliary magnetic pole part 23 in addition to the torque by the permanent magnet 22, and can operate as a high-torque motor.
【0029】以上の構成において、本発明では図1に示
すように直流電源30と、それに接続されたインバータ
31と、インバータ31の出力端に直接接続された永久
磁石回転電機とを備え、かつ永久磁石回転電機を位相シ
フト回路37によって弱め界磁制御する方式の永久磁石
回転電機装置において、永久磁石回転電機の端子間の発
生誘起電圧のピーク電圧をVpとし、その基本波電圧の
ピーク値をVp1としたとき、Vp<Vp1の誘起電圧
形状となさしめたことを特徴とするものである。According to the present invention, as shown in FIG. 1, the present invention comprises a DC power supply 30, an inverter 31 connected thereto, and a permanent magnet rotating electric machine directly connected to the output terminal of the inverter 31. In the permanent magnet rotating electric machine of the system in which the magnet rotating electric machine controls the field weakening by the phase shift circuit 37, the peak voltage of the induced voltage between the terminals of the permanent magnet rotating electric machine is Vp, and the peak value of the fundamental wave voltage is Vp1. In this case, the shape of the induced voltage is Vp <Vp1.
【0030】電気自動車等の電動車両に使用する駆動電
動機に求められるトルク特性は、低速(ある回転数まで
の範囲)では大トルクの発生が可能であり、かつそれを
越える高速領域ではインバータ31の容量がなるべく大
きくならない範囲で定出力の運転が可能であることが望
まれている。このため、低速ではインバータ31のスイ
ッチング素子の許容電流の範囲内での定トルク運転範囲
と高速での定出力範囲での運転とを一般に行っている。The torque characteristics required of a drive motor used for an electric vehicle such as an electric vehicle are such that a large torque can be generated at a low speed (a range up to a certain number of rotations), and in a high-speed region exceeding the range, the inverter 31 needs to operate at a high speed. It is desired that a constant output operation be possible within a range in which the capacity does not increase as much as possible. Therefore, at a low speed, a constant torque operation range within a range of the allowable current of the switching element of the inverter 31 and an operation at a high speed constant output range are generally performed.
【0031】永久磁石モータのトルクTは一般に T=(E0・Iq+(Xq−Xd)・Id・Iq)/ω …(1) ここで、E0:誘起電圧 ω:回転角速度 Id,Iq:d,q軸の電流 Xq,Xd:d,q軸のリアクタンス (1)式で第1項は永久磁石22によるトルク成分で、
第2項は補助磁極部23によるリラクタンストルク成分
である。The torque T of the permanent magnet motor is generally T = (E00Iq + (Xq-Xd) ・ Id ・ Iq) / ω (1) where, E0: induced voltage ω: rotational angular velocity Id, Iq: d, q-axis current Xq, Xd: d, q-axis reactance In equation (1), the first term is a torque component by the permanent magnet 22,
The second term is a reluctance torque component by the auxiliary magnetic pole part 23.
【0032】トルクを大きくするためにはリラクタンス
によるトルクと永久磁石によるトルクを最大に利用する
必要がある。従って永久磁石の誘起電圧を増加させた法
がインバータ31のスイッチング素子の電流容量を小さ
くすることができる。In order to increase the torque, it is necessary to maximize the torque by the reluctance and the torque by the permanent magnet. Therefore, the method of increasing the induced voltage of the permanent magnet can reduce the current capacity of the switching element of the inverter 31.
【0033】一方、高速回転数の領域では定出力のた
め、必要トルクは小さくなり、リラクタンスによるトル
クも永久磁石によるトルクも同一の電流に対する最大の
トルクを出せる位相とはしない。ここでは、永久磁石2
2の磁束を弱めて永久磁石による誘起電圧を低める、い
わゆる弱め界磁制御で運転する。これによって永久磁石
による誘起電圧を下げ、従って永久磁石回転電機に加え
る端子電圧以下にして直流電源より電力が供給されるよ
うになって高速まで回転可能とすることができるのであ
る。On the other hand, since the output is constant in the high-speed range, the required torque is small, and neither the torque by reluctance nor the torque by the permanent magnet is in a phase in which the maximum torque can be generated for the same current. Here, the permanent magnet 2
The operation is performed by so-called field weakening control, which weakens the magnetic flux of No. 2 to lower the induced voltage by the permanent magnet. As a result, the voltage induced by the permanent magnet is reduced, so that the power is supplied from the DC power supply to a terminal voltage lower than the terminal voltage applied to the permanent magnet rotating electric machine, and the motor can be rotated up to a high speed.
【0034】この条件で低速のトルクを優先させて誘起
電圧を上昇させると、高速で弱め界磁を大きくする必要
がある。If the induced voltage is increased by giving priority to low-speed torque under these conditions, it is necessary to increase the field weakening at high speed.
【0035】ここで、制御装置が正常動作中であれば永
久磁石の誘起電圧は弱め界磁制御によってインバータ3
1の素子耐圧、及びインバータの入力端子間に設けられ
たコンデンサ等の耐圧の範囲を超えることはないが、高
速運転まで正常に運行し、その後、インバータが故障し
た場合には弱め界磁が不能となり、大きな誘起電圧が直
接インバータ31及びコンデンサにかかり、破損のおそ
れと、大きな電力を直流電源に戻すことにより大きなブ
レーキ力を引き起こすおそれもある。If the control device is operating normally, the induced voltage of the permanent magnet is reduced by the field weakening control.
1, but it does not exceed the range of the withstand voltage of the capacitor and the like provided between the input terminals of the inverter. However, it operates normally up to high-speed operation, and if the inverter breaks down, field weakening cannot be performed. Thus, a large induced voltage is directly applied to the inverter 31 and the capacitor, which may cause damage and return large power to the DC power source to cause a large braking force.
【0036】従って、インバータの素子容量を小さくす
るためには大きなトルクの発生と誘起電圧の最大値を低
減せしめるという合い矛盾する課題を達成する必要があ
る。一方、永久磁石回転電機の固定子鉄心には前述のよ
うに固定子巻線3をスロット部11に収納するスリット
14が一般に設けられている。このスリットの影響は、
図2で示したようなリラクタンストルクを積極的に利用
する補助磁極部23を有する型の永久磁石回転電機では
永久磁石の角度τ1の選定によっては図4(a)のよう
にな波形になる。つまり中心部の誘起電圧波形Vm=V
pが大きくなってしまう。Therefore, in order to reduce the element capacity of the inverter, it is necessary to achieve the contradictory problems of generating a large torque and reducing the maximum value of the induced voltage. On the other hand, a slit 14 for accommodating the stator winding 3 in the slot portion 11 is generally provided in the stator core of the permanent magnet rotating electric machine as described above. The effect of this slit is
In the permanent magnet rotating electric machine having the auxiliary magnetic pole portion 23 that actively uses the reluctance torque as shown in FIG. 2, the waveform becomes as shown in FIG. 4A depending on the selection of the permanent magnet angle τ1. That is, the induced voltage waveform Vm = V at the center
p becomes large.
【0037】このような波形で高速領域でのインバータ
31の故障を考えるとインバータ31の素子及びコンデ
ンサの電圧耐量は誘起電圧の最大値Vpで決まってしま
うため、結果としてトルクに影響する誘起電圧の実行値
は小さくせざるを得ず、従って、同一トルクを得るため
にはインバータ素子の電流容量を増加させなければなら
ない欠点がある。Considering the failure of the inverter 31 in the high-speed region with such a waveform, the withstand voltage of the elements and the capacitor of the inverter 31 is determined by the maximum value Vp of the induced voltage. There is a drawback that the effective value must be reduced, and therefore the current capacity of the inverter element must be increased in order to obtain the same torque.
【0038】本発明では、図2で示した永久磁石τ1の
角度をパラメータに検証した結果、角度によって誘起電
圧波形に図4(a),(b),(c)のように変化すること
を見いだした。According to the present invention, as a result of verifying the angle of the permanent magnet τ1 shown in FIG. 2 as a parameter, the induced voltage waveform changes as shown in FIGS. 4 (a), (b) and (c) depending on the angle. I found it.
【0039】図4は8極,スロット48個での図示例
で、実線は線間誘起電圧、波線はその基本波分を示すも
のである。FIG. 4 shows an example in which there are eight poles and 48 slots. The solid line indicates the induced voltage between lines, and the dashed line indicates the fundamental wave component.
【0040】図4(a)は永久磁石τ1の角度と極節τ
pの比を0.63 にした場合で、この場合、回転電機の
誘起電圧の最大値Vpは誘起電圧の中心部の値Vmに等
しく、その値は誘起電圧の基本波分Vp1よりも大きく
なる。FIG. 4A shows the angle of the permanent magnet τ1 and the pole node τ.
In the case where the ratio of p is 0.63, in this case, the maximum value Vp of the induced voltage of the rotating electric machine is equal to the value Vm at the center of the induced voltage, and the value is larger than the fundamental wave component Vp1 of the induced voltage. .
【0041】図4(b)は永久磁石τ1の角度と極節τ
pの比を0.58 にした場合で、この場合、回転電機の
誘起電圧の最大値Vpは誘起電圧の中心部の値Vmより
高く、誘起電圧の基本波分Vp1よりも小さくなる。FIG. 4B shows the angle of the permanent magnet τ1 and the pole node τ.
In the case where the ratio of p is 0.58, the maximum value Vp of the induced voltage of the rotating electric machine is higher than the value Vm at the center of the induced voltage and smaller than the fundamental wave component Vp1 of the induced voltage.
【0042】図4(c)は永久磁石τ1の角度と極節τ
pの比を0.53 にした場合で、この場合、回転電機の
誘起電圧の最大値Vpは誘起電圧の中心部の値Vmより
大きく、誘起電圧の基本波分Vp1よりも小さくなる。FIG. 4C shows the angle of the permanent magnet τ1 and the pole node τ.
In the case where the ratio of p is 0.53, in this case, the maximum value Vp of the induced voltage of the rotating electric machine is larger than the value Vm at the center of the induced voltage and smaller than the fundamental wave component Vp1 of the induced voltage.
【0043】図4(d)には永久磁石τ1の角度と極節
τpの比に対するVp/Vp1,Vm/Vpを示す。FIG. 4D shows Vp / Vp1 and Vm / Vp with respect to the ratio between the angle of the permanent magnet τ1 and the pole node τp.
【0044】ここで、誘起電圧の基本波分Vp1はトル
クに直接関係するもので大きい方が望ましい。一方、誘
起電圧の最大値Vpは高速時まで運転させるにはできる
限り小さいことが望ましい。従って、Vp/Vp1の比
を小さくすることが求められる。図4(d)では永久磁
石τ1の角度と極節τpの比が0.6 以下、つまりVp
/Vp1が1.0 以下(Vp<Vp1)がよい。一方、
誘起電圧の中心部の値Vmは直接は意味を持たないが図
4(d)で示すようにVm/Vp<1となる範囲と上記
の範囲はよく対応している。つまりVp<Vp1はVm
<Vpで顕彰できる。Here, the fundamental wave component Vp1 of the induced voltage is directly related to the torque and is preferably large. On the other hand, it is desirable that the maximum value Vp of the induced voltage be as small as possible in order to operate until high speed. Therefore, it is required to reduce the ratio of Vp / Vp1. In FIG. 4D, the ratio between the angle of the permanent magnet τ1 and the pole node τp is 0.6 or less, that is, Vp
/ Vp1 is preferably 1.0 or less (Vp <Vp1). on the other hand,
Although the value Vm at the center of the induced voltage has no direct meaning, the above range and the range where Vm / Vp <1 correspond well as shown in FIG. 4D. That is, Vp <Vp1 is Vm
<Vp can be honored.
【0045】以上、図4(b),(c)のようにすること
によってインバータ素子の電流容量を小さくすることが
できる。As described above, the current capacities of the inverter elements can be reduced by the arrangements shown in FIGS. 4B and 4C.
【0046】以上の効果は、低回転数での定トルク範囲
と高速時の定出力運転範囲とを有し、かつ定トルク範囲
の最高回転数をN1,定出力範囲の最高回転数をN2と
したとき、N2/N1の値が大きいほど効果がある。つ
まり、高速域で永久磁石の磁束を弱める必要が大きくな
るためである。ここではこの値が2以上で上記の効果を
発揮できる。The above-described effect is obtained by having a constant torque range at a low rotation speed and a constant output operation range at a high speed, and setting the maximum rotation speed of the constant torque range to N1 and the maximum rotation speed of the constant output range to N2. Then, the larger the value of N2 / N1, the more effective. In other words, it is necessary to weaken the magnetic flux of the permanent magnet in a high speed range. Here, when the value is 2 or more, the above effect can be exhibited.
【0047】図5に本発明の永久磁石回転電機装置の回
転電機の他の実施例を示す。FIG. 5 shows another embodiment of the rotating electric machine of the permanent magnet rotating electric machine device of the present invention.
【0048】図2と同一記号は同一構成部品を示す。こ
こでも、同相に属する固定子巻線(例えばU1,U2,
U3,U4)が電気的にすべて同相の位置に配置された
構成で示す。同じ位相とすることによって誘起電圧の高
調波がすべての固定子巻線で発生するため減衰せず、台
形状の誘起電圧を発生しやすくなる。The same symbols as those in FIG. 2 indicate the same components. Here, too, the stator windings belonging to the same phase (eg U1, U2,
U3, U4) are electrically arranged in the same phase. With the same phase, harmonics of the induced voltage are generated in all the stator windings, so that they are not attenuated, and a trapezoidal induced voltage is easily generated.
【0049】ここでは永久磁石回転子の中心の外周部の
磁極片部24の空隙部を大きくする構成とした。以上の
形状によって図5(b)に示すように永久磁石回転電機
の誘起電圧は階段状となってVp<Vp1とすることが
でき、図4での説明と同様の効果を得ることができる。In this embodiment, the gap of the pole piece 24 at the center of the permanent magnet rotor is increased. With the above shape, as shown in FIG. 5B, the induced voltage of the permanent magnet rotating electric machine becomes stair-like, and Vp <Vp1, and the same effect as that described in FIG. 4 can be obtained.
【0050】図6に本発明の永久磁石回転電機装置の回
転電機の他の実施例を示す。図2と同一記号は同一構成
部品を示す。ここでは永久磁石回転電機の固定子を集中
巻としたことを特徴とする。ここでも、固定子巻線を集
中的に巻回し、かつ同相に属する固定子巻線が電気的に
すべて同じ位相の位置に配置された構成である。FIG. 6 shows another embodiment of the rotating electric machine of the permanent magnet rotating electric machine device of the present invention. The same symbols as those in FIG. 2 indicate the same components. Here, the stator of the permanent magnet rotating electric machine is characterized by being concentratedly wound. Also in this case, the stator winding is intensively wound, and the stator windings belonging to the same phase are all electrically arranged at the same phase position.
【0051】以上の構成とすることによって回転子はほ
ぼ全周にわたって永久磁石を配置した構成であっても図
5(b)に示すように永久磁石回転電機の誘起電圧は階
段状とすることができる。これによってVp<Vp1と
することができ、図4での説明と同様の効果を得ること
ができる。With the above configuration, even if the rotor has a configuration in which permanent magnets are arranged over almost the entire circumference, the induced voltage of the permanent magnet rotating electric machine can be stepped as shown in FIG. 5B. it can. Accordingly, Vp <Vp1 can be satisfied, and the same effect as that described with reference to FIG. 4 can be obtained.
【0052】なお、以上の永久磁石回転電機を電動車
両、特に電気自動車に適用すれば、小型軽量高効率の永
久磁石回転電機駆動装置を搭載でき、一充電走行距離の
長い電気自動車を提供することができる。また、安全性
の高い電動車両を提供できる。また、以上は制御装置と
して速度制御機能(ASR)を有する永久磁石回転電機
装置について述べたが、トルク制御機能を有する永久磁
石回転電機装置についても適用可能である。また、回転
電機としては軸方向の空隙を有する回転電機及び発電
機,電動機及び内転型,外転型,リニア型を問わず適用
可能である。When the above-described permanent magnet rotating electric machine is applied to an electric vehicle, particularly an electric vehicle, it is possible to mount a small, light and high-efficiency permanent magnet rotating electric machine driving device, and to provide an electric vehicle having a long charge traveling distance. Can be. In addition, a highly safe electric vehicle can be provided. In the above, a permanent magnet rotating electric machine having a speed control function (ASR) has been described as a control device, but the present invention is also applicable to a permanent magnet rotating electric machine having a torque control function. Further, as the rotating electric machine, any of a rotating electric machine having a gap in the axial direction, a generator, a motor, and an internal rotation type, an external rotation type, and a linear type can be applied.
【0053】[0053]
【発明の効果】以上の構成によれば、小形軽量,高トル
クの永久磁石回転電機、及び電流容量の小さなスイッチ
ング素子ですむインバータとを備えた永久磁石回転電機
装置を提供できる。According to the above configuration, it is possible to provide a permanent magnet rotating electric machine including a small, lightweight, high-torque permanent magnet rotating electric machine and an inverter that requires only a switching element having a small current capacity.
【図1】本発明の永久磁石回転電機装置を示す。FIG. 1 shows a permanent magnet rotating electric machine device of the present invention.
【図2】本発明の永久磁石回転電機を示す。FIG. 2 shows a permanent magnet rotating electric machine of the present invention.
【図3】本発明の永久磁石回転電機の断面を示す。FIG. 3 shows a cross section of the permanent magnet rotating electric machine of the present invention.
【図4】本発明の誘起電圧波形の動作説明図を示す。FIG. 4 is a diagram illustrating the operation of an induced voltage waveform according to the present invention.
【図5】本発明の永久磁石回転電機の他の実施例を示
す。FIG. 5 shows another embodiment of the permanent magnet rotating electric machine of the present invention.
【図6】本発明の永久磁石回転電機の他の実施例を示
す。FIG. 6 shows another embodiment of the permanent magnet rotating electric machine of the present invention.
1…固定子、2…回転子、3…固定子巻線、11…スロ
ット部、12…固定子歯部(突極部)、13…固定子ヨ
ーク部、21…永久磁石挿入孔、22…永久磁石、23
…補助磁極部、24…磁極片部、31…インバータ、3
2…速度制御回路(ASR)、33…F/V変換器、3
4…正弦波,余弦波発生器、36…電流制御系(AC
R)、35…2相−3相変換回路、37…位相シフト回
路。DESCRIPTION OF SYMBOLS 1 ... Stator, 2 ... Rotor, 3 ... Stator winding, 11 ... Slot part, 12 ... Stator tooth part (salient pole part), 13 ... Stator yoke part, 21 ... Permanent magnet insertion hole, 22 ... Permanent magnet, 23
... Auxiliary magnetic pole part, 24 ... Magnetic pole piece part, 31 ... Inverter, 3
2: Speed control circuit (ASR), 33: F / V converter, 3
4: Sine wave and cosine wave generators 36: Current control system (AC
R), 35: a two-phase to three-phase conversion circuit, 37: a phase shift circuit.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 渋川 末太郎 茨城県ひたちなか市大字高場2520番地 株 式会社日立製作所自動車機器事業部内 (72)発明者 小泉 修 茨城県ひたちなか市大字高場2520番地 株 式会社日立製作所自動車機器事業部内 ──────────────────────────────────────────────────の Continuing on the front page (72) Inventor Suetaro Shibukawa 2520 Oji Takaba, Hitachinaka-shi, Ibaraki Co., Ltd.Automotive Equipment Division, Hitachi, Ltd. Hitachi, Ltd. Automotive Equipment Division
Claims (6)
により回転速度が制御される永久磁石回転電機と、該永
久磁石回転電機を弱め界磁制御する手段とを備えてなる
永久磁石回転電機装置において、 前記永久磁石回転電機の端子間の発生誘起電圧のピーク
値をVpとし、その基本波電圧のピーク値をVp1とし
たとき、Vp<Vp1の誘起電圧値となるようにしたこ
とを特徴とする永久磁石回転電機装置。1. A permanent magnet rotating electric machine comprising: a DC power supply; a permanent magnet rotating electric machine whose rotation speed is controlled by an inverter connected to the DC power supply; and means for performing field weakening control on the permanent magnet rotating electric machine. A permanent magnet characterized in that, when a peak value of an induced induced voltage between terminals of a permanent magnet rotating electric machine is Vp and a peak value of a fundamental wave voltage thereof is Vp1, an induced voltage value of Vp <Vp1 is satisfied. Rotary electric machine.
により回転速度が制御される永久磁石回転電機と、該永
久磁石回転電機を弱め界磁制御する手段とを備えてなる
永久磁石回転電機装置において、 永久磁石回転電機の端子間の発生誘起電圧の中心の電圧
値をVmとし、その発生誘起電圧のピーク値をVpとし
たとき、Vm<Vpの誘起電圧値となるようにしたこと
を特徴とする永久磁石回転電機装置。2. A permanent magnet rotating electric machine comprising: a DC power supply; a permanent magnet rotating electric machine whose rotation speed is controlled by an inverter connected thereto; and means for weakening and controlling the field of the permanent magnet rotating electric machine. When the voltage value at the center of the induced electromotive force between the terminals of the magnet rotating electric machine is Vm, and the peak value of the induced electromotive voltage is Vp, the induced voltage value is such that Vm <Vp. Magnet rotating electric machine.
のコイル幅を永久磁石回転子の磁極の幅にほぼ等しくし
たことを特徴とする永久磁石回転電機装置。3. The permanent magnet rotary electric machine according to claim 2, wherein the coil width of the permanent magnet rotary electric machine is substantially equal to the width of the magnetic pole of the permanent magnet rotor.
石回転子の磁極中心の空隙長を磁極端の空隙長より大き
くしたことを特徴とする永久磁石回転電機装置。4. The permanent magnet rotating electrical machine according to claim 1, wherein the gap length at the center of the magnetic pole of the permanent magnet rotor is larger than the gap length at the pole tip.
に属する固定子巻線を巻回した複数の固定子突極が電気
的にすべて同相の位置になるようにしたことを特徴とす
る永久磁石回転電機装置。5. The permanent magnet according to claim 1, wherein a plurality of stator salient poles wound with stator windings belonging to the same phase are all electrically in-phase. Magnet rotating electric machine.
定トルク範囲と高速時の定出力運転範囲とを有し、かつ
定トルク範囲の最高回転数をN1,定出力範囲の最高回
転数をN2としたとき、N2/N1が2以上であること
を特徴とする永久磁石回転電機装置。6. A constant torque range having a constant torque range at a low rotation speed and a constant output operation range at a high speed, wherein the maximum rotation speed in the constant torque range is N1 and the maximum rotation speed in the constant output range. A permanent magnet rotating electrical machine, wherein N2 / N1 is 2 or more, where N2 is the number of revolutions.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP06270897A JP3289635B2 (en) | 1997-03-17 | 1997-03-17 | Permanent magnet rotating electric machine |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP06270897A JP3289635B2 (en) | 1997-03-17 | 1997-03-17 | Permanent magnet rotating electric machine |
Publications (2)
Publication Number | Publication Date |
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JPH10262359A true JPH10262359A (en) | 1998-09-29 |
JP3289635B2 JP3289635B2 (en) | 2002-06-10 |
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Application Number | Title | Priority Date | Filing Date |
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JP06270897A Expired - Lifetime JP3289635B2 (en) | 1997-03-17 | 1997-03-17 | Permanent magnet rotating electric machine |
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Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2000134891A (en) * | 1998-10-28 | 2000-05-12 | Okuma Corp | Synchronous motor and controller therefor |
WO2001095464A1 (en) * | 2000-06-02 | 2001-12-13 | Mitsubishi Heavy Industries, Ltd. | Brushless motor |
WO2003053734A1 (en) * | 2001-12-21 | 2003-07-03 | Aisin Aw Co., Ltd. | Electrically-driven vehicle drive controller |
US7482724B2 (en) | 2004-02-05 | 2009-01-27 | Mitsubishi Heavy Industries, Ltd. | Ipm electric rotating machine |
US7521832B2 (en) | 2004-03-10 | 2009-04-21 | Hitachi, Ltd. | Rotating electric machine having rotor embedded-permanent-magnets with inner-end magnetic gaps and outer-end magnetic gaps, and electric car using the same electric machine |
US7635039B2 (en) | 2004-01-13 | 2009-12-22 | Mitsubishi Heavy Industries, Ltd. | Series hybrid electric vehicle |
JP2021005934A (en) * | 2019-06-26 | 2021-01-14 | 株式会社Subaru | Motor device |
-
1997
- 1997-03-17 JP JP06270897A patent/JP3289635B2/en not_active Expired - Lifetime
Cited By (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2000134891A (en) * | 1998-10-28 | 2000-05-12 | Okuma Corp | Synchronous motor and controller therefor |
WO2001095464A1 (en) * | 2000-06-02 | 2001-12-13 | Mitsubishi Heavy Industries, Ltd. | Brushless motor |
US6853106B2 (en) | 2000-06-02 | 2005-02-08 | Mitsubishi Heavy Industries, Ltd. | Brushless motor |
WO2003053734A1 (en) * | 2001-12-21 | 2003-07-03 | Aisin Aw Co., Ltd. | Electrically-driven vehicle drive controller |
US7163072B2 (en) | 2001-12-21 | 2007-01-16 | Aisin Aw Co., Ltd. | Motor-driven vehicle drive control apparatus and method thereof |
US7635039B2 (en) | 2004-01-13 | 2009-12-22 | Mitsubishi Heavy Industries, Ltd. | Series hybrid electric vehicle |
US7482724B2 (en) | 2004-02-05 | 2009-01-27 | Mitsubishi Heavy Industries, Ltd. | Ipm electric rotating machine |
US7521832B2 (en) | 2004-03-10 | 2009-04-21 | Hitachi, Ltd. | Rotating electric machine having rotor embedded-permanent-magnets with inner-end magnetic gaps and outer-end magnetic gaps, and electric car using the same electric machine |
US8067871B2 (en) | 2004-03-10 | 2011-11-29 | Hitachi, Ltd. | Permanent magnet rotating electric machine and electric car using the same |
USRE44037E1 (en) | 2004-03-10 | 2013-03-05 | Hitachi, Ltd. | Rotating electric machine having rotor embedded-permanent-magnets with inner-end magnetic gaps and outer-end magnetic gaps, and electric car using the same electric machine |
JP2021005934A (en) * | 2019-06-26 | 2021-01-14 | 株式会社Subaru | Motor device |
Also Published As
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