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JP5334303B2 - Permanent magnet motor, hermetic compressor, and refrigeration cycle apparatus - Google Patents
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JP5334303B2 - Permanent magnet motor, hermetic compressor, and refrigeration cycle apparatus - Google Patents

Permanent magnet motor, hermetic compressor, and refrigeration cycle apparatus Download PDF

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JP5334303B2
JP5334303B2 JP2009042515A JP2009042515A JP5334303B2 JP 5334303 B2 JP5334303 B2 JP 5334303B2 JP 2009042515 A JP2009042515 A JP 2009042515A JP 2009042515 A JP2009042515 A JP 2009042515A JP 5334303 B2 JP5334303 B2 JP 5334303B2
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permanent magnet
rotor
phase
core
excitation current
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JP2010200494A (en
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俊彦 二見
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Carrier Japan Corp
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Toshiba Carrier Corp
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a permanent magnet motor in which the amount of magnetic flux of a rotor can reliably be set appropriately, stable dynamic characteristics can be obtained, and excellent reliability is ensured, and to provide a sealed compressor and a refrigeration cycle device which ensure excellent reliability by employing the permanent magnet motor. <P>SOLUTION: The permanent magnet motor includes a rotor 12 formed by arraging a first core 12a and a second core 12b along the axial direction of a rotating shaft 13. A plurality of first permanent magnets 43 whose magnetic force changes by magnetization or demagnetization by an exciting current, are accommodated in the first core 12a of the rotor 12. A plurality of second permanent magnets 44 whose magnetic force does not change irrespective of supply of the exciting current, are accommodated in the second core 12b of the rotor 12. Then, the width of each first permanent magnet 43 is made narrower than that of each second permanent magnet 44. <P>COPYRIGHT: (C)2010,JPO&amp;INPIT

Description

この発明は、巻線を有する固定子および永久磁石を有する回転子からなる永久磁石電動機、この永久磁石電動機を収納した密閉型圧縮機、およびこの密閉型圧縮機を有する冷凍サイクル装置に関する。   The present invention relates to a permanent magnet motor including a stator having windings and a rotor having permanent magnets, a hermetic compressor housing the permanent magnet motor, and a refrigeration cycle apparatus having the hermetic compressor.

永久磁石電動機は、巻線を有する固定子および永久磁石を有する回転子からなる。回転子は、円形の多数枚の鋼板を積層してなるコアの中心部に回転軸の挿通孔を有し、この挿通孔を囲む位置に複数の直線状の磁石収容孔を有する。これら磁石収容孔は、回転軸の軸方向に沿ってコアを貫通する深さ形状を持ち、それぞれ永久磁石を収容している。これら永久磁石の磁界と固定子の巻線が発する磁界との相互作用により、回転子に回転力が生じる。   The permanent magnet motor includes a stator having windings and a rotor having permanent magnets. The rotor has an insertion hole for a rotating shaft at the center of a core formed by laminating a large number of circular steel plates, and has a plurality of linear magnet accommodation holes at positions surrounding the insertion hole. These magnet accommodation holes have a depth shape penetrating the core along the axial direction of the rotation shaft, and each accommodates a permanent magnet. Due to the interaction between the magnetic field of these permanent magnets and the magnetic field generated by the stator winding, a rotational force is generated in the rotor.

このような永久磁石電動機の例として、回転軸の軸方向に沿って配列された複数のコアからなる回転子を用い、この回転子の一方のコアに低保磁力の永久磁石を収容し、他方のコアに高保磁力の永久磁石を収容し、固定子の各相巻線に着磁用または減磁用の励磁電流を流すことで、低保磁力の永久磁石の磁力を変化させるものがある(例えば特許文献1)。   As an example of such a permanent magnet motor, a rotor composed of a plurality of cores arranged along the axial direction of the rotation shaft is used, and a low-coercivity permanent magnet is accommodated in one core of the rotor, while the other In which a high coercivity permanent magnet is housed and an excitation current for magnetization or demagnetization is applied to each phase winding of the stator to change the magnetic force of the low coercivity permanent magnet ( For example, Patent Document 1).

特開2005−304204号公報JP-A-2005-304204

上記特許文献1に記載の永久磁石電動機では、着磁用または減磁用の励磁電流を各相巻線に供給することで低保磁力の永久磁石の磁力を変化させることができるが、その磁化力が不安定で、回転子の磁束量を適正な状態に設定することが難しく、永久磁石電動機としての安定した動作特性が得られない。   In the permanent magnet motor described in Patent Document 1, the magnetic force of a low-coercivity permanent magnet can be changed by supplying an excitation current for magnetization or demagnetization to each phase winding. The force is unstable, it is difficult to set the amount of magnetic flux of the rotor to an appropriate state, and stable operating characteristics as a permanent magnet motor cannot be obtained.

この発明は、上記の事情を考慮したもので、その目的は、回転子の磁束量を適正な状態に確実に設定することができ、これにより安定した動作特性が得られる信頼性にすぐれた永久磁石電動機を提供することである。また、この永久磁石電動機を有する信頼性にすぐれた密閉型圧縮機および冷凍サイクル装置を提供することである。   The present invention takes the above-mentioned circumstances into consideration, and an object of the present invention is to set the magnetic flux amount of the rotor to an appropriate state with certainty, whereby a stable operating characteristic can be obtained. It is to provide a magnet motor. Another object of the present invention is to provide a hermetic compressor and a refrigeration cycle apparatus having the permanent magnet motor and excellent in reliability.

請求項1に係る発明の永久磁石電動機は、複数の相巻線が装着された固定子と、第1コアおよび第2コアを回転軸の軸方向に沿って配列してなる回転子と、前記第1コアにおける前記回転軸を囲む位置に形成されたV字形状の複数の第1磁石収容孔と、前記第2コアにおける前記回転軸を囲む位置に形成されたV字形状の複数の第2磁石収容孔と、前記各第1磁石収容孔にそのV字形状に合せて2分割状態で収容され、駆動装置から前記各相巻線に供給される励磁電流により着磁または減磁されて磁力が変化する複数の第1永久磁石と、前記各第2磁石収容孔にそのV字形状に合せて2分割状態で収容され、前記励磁電流の供給にかかわらず磁力変化がない複数の第2永久磁石とを備え、前記各第1永久磁石の幅を前記各第2永久磁石の幅よりも小さくするとともに、前記着磁または減磁に際しての前記固定子と前記回転子の位置関係に応じて、前記各第1磁石収容孔における2分割状態の第1永久磁石の端部同士を密接または離間させる。 Permanent magnet motor of the invention according to claim 1, and a stator having a plurality of phase windings is mounted, formed by arranging along the first core and the second core in the axial direction of the rotating shaft rotor, wherein A plurality of V-shaped first magnet housing holes formed at positions surrounding the rotation shaft in the first core, and a plurality of second V-shaped magnets formed at positions surrounding the rotation shaft in the second core. A magnet housing hole and each first magnet housing hole are housed in a two-divided state in accordance with the V shape, and are magnetized or demagnetized by an excitation current supplied from the driving device to each phase winding. And a plurality of second permanent magnets housed in the second magnet housing holes in a split state in accordance with the V-shape and having no change in magnetic force regardless of the supply of the excitation current. A width of each first permanent magnet is equal to a width of each second permanent magnet. With even smaller, according to the positional relationship of the said stator of when the magnetizing or demagnetizing the rotor, the end portions of the first permanent magnet of the two-divided state in each first magnet containing hole close or Separate.

請求項6に係る発明の密閉型圧縮機は、請求項1乃至5に係る発明の何れかの永久磁石電動機と、この永久磁石電動機により駆動される圧縮機構部とを、密閉容器に収納している。   According to a sixth aspect of the present invention, there is provided a hermetic compressor in which the permanent magnet motor according to any one of the first to fifth aspects of the present invention and a compression mechanism driven by the permanent magnet motor are housed in a hermetic container. Yes.

請求項7に係る発明の冷凍サイクル装置は。請求項6に係る発明の密閉型圧縮機と、凝縮器と、膨張装置と、蒸発器とからなる。   The refrigeration cycle apparatus of the invention according to claim 7. It consists of a hermetic compressor of the invention concerning Claim 6, a condenser, an expansion device, and an evaporator.

この発明の永久磁石電動機によれば、永久磁石電動機の回転子の磁束量を適正な状態に設定することができ、永久磁石電動機の安定した動作特性が得られる。また、この永久磁石電動機を有する信頼性にすぐれた密閉型圧縮機および冷凍サイクル装置が得られる。   According to the permanent magnet motor of the present invention, the amount of magnetic flux of the rotor of the permanent magnet motor can be set to an appropriate state, and stable operating characteristics of the permanent magnet motor can be obtained. In addition, a hermetic compressor and refrigeration cycle apparatus having the permanent magnet motor and excellent in reliability can be obtained.

各実施形態における冷凍サイクル装置の構成及びこの冷凍サイクル装置に搭載された密閉型圧縮機の内部の構成を示す図。The figure which shows the structure of the refrigerating-cycle apparatus in each embodiment, and the structure inside the hermetic compressor mounted in this refrigerating-cycle apparatus. 第1の実施形態における密閉型圧縮機の回転子および各永久磁石の構成を概略的に示す図。The figure which shows schematically the structure of the rotor of a hermetic compressor in 1st Embodiment, and each permanent magnet. 第1の実施形態における密閉型圧縮機の回転子の第1コアとその第1コアに収容された各永久磁石の構成を上方から見た図。The figure which looked at the structure of the 1st core of the rotor of the hermetic compressor in a 1st embodiment, and each permanent magnet stored in the 1st core from the upper part. 第1の実施形態における密閉型圧縮機の回転子の第2コアとその第2コアに収容された各永久磁石の構成を上方から見た図。The figure which looked at the structure of each 2nd core of the rotor of the hermetic compressor in 1st Embodiment, and each permanent magnet accommodated in the 2nd core from upper direction. 第1の実施形態における密閉型圧縮機の固定子、各相巻線、回転子、各永久磁石の構成を上方から見た図。The figure which looked at the structure of the stator, each phase winding, rotor, and each permanent magnet of the hermetic compressor in a 1st embodiment from the upper part. 各実施形態における駆動装置および相巻線の構成を示すブロック図。The block diagram which shows the structure of the drive device and phase winding in each embodiment. 図6における非通電状態の相巻線に誘起する電圧の波形図。FIG. 7 is a waveform diagram of a voltage induced in a non-energized phase winding in FIG. 6. 各実施形態における各永久磁石の着磁用または減磁用の3相励磁を説明するための図。The figure for demonstrating the three-phase excitation for magnetization or demagnetization of each permanent magnet in each embodiment. 第1の実施形態における各永久磁石の幅方向の位置と磁化力の関係を示す図。The figure which shows the position of the width direction of each permanent magnet in 1st Embodiment, and the relationship of a magnetizing force. 各実施形態における各永久磁石の磁束密度と磁化力の関係を示す図。The figure which shows the relationship between the magnetic flux density and magnetizing force of each permanent magnet in each embodiment. 第2の実施形態における回転子の第1コアを上方から見た図。The figure which looked at the 1st core of the rotor in a 2nd embodiment from the upper part. 第2の実施形態における回転子の第2コアを上方から見た図。The figure which looked at the 2nd core of the rotor in a 2nd embodiment from the upper part. 第2の実施形態における各永久磁石の幅方向の磁化力分布を示す図。The figure which shows the magnetic force distribution of the width direction of each permanent magnet in 2nd Embodiment. 第3の実施形態における回転子の第1コアとその第1コアに収容された各永久磁石の構成を上方から見た図。The figure which looked at the structure of the 1st core of the rotor in 3rd Embodiment, and each permanent magnet accommodated in the 1st core from the upper direction. 第3の実施形態における回転子の第2コアとその第2コアに収容された各永久磁石の構成を上方から見た図。The figure which looked at the structure of the 2nd core of the rotor in 3rd Embodiment, and each permanent magnet accommodated in the 2nd core from the upper direction. 各実施形態における各永久磁石の着磁用または減磁用の2相励磁を説明するための図。The figure for demonstrating the two-phase excitation for magnetization or demagnetization of each permanent magnet in each embodiment. 第3の実施形態における各永久磁石の幅が適切でない場合の構成を上方から見た図。The figure which looked at the structure when the width | variety of each permanent magnet in 3rd Embodiment is not appropriate from the upper direction. 図17における各永久磁石の幅方向の磁化力分布を示す図。The figure which shows the magnetic force distribution of the width direction of each permanent magnet in FIG. 第6の実施形態における固定子および回転子の磁束分布を示す図。The figure which shows magnetic flux distribution of the stator and rotor in 6th Embodiment. 第6の実施形態における永久磁石の幅方向の磁化力分布を示す図。The figure which shows the magnetic force distribution of the width direction of the permanent magnet in 6th Embodiment.

[1]以下、この発明の第1の実施形態について図面を参照して説明する。
空気調和機や冷蔵庫等の冷凍サイクル装置の構成、およびこの冷凍サイクル装置に搭載された密閉型圧縮機の内部の構成を、図1に示す。密閉型圧縮機1は、金属製の密閉容器1aで被われている。この密閉容器1aの下部に2つの吸込口2a,2bが取付けられ、上部に1本の吐出管3が取付けられている。この吐出管3に高圧側配管を介して凝縮器31の一端が接続され、その凝縮器31の他端に膨張装置たとえば膨張弁32を介して蒸発器33の一端が接続される。そして、蒸発器33の他端がアキュームレータ34および2本の吸込管35を介して上記吸込口2a,2bに接続される。
[1] A first embodiment of the present invention will be described below with reference to the drawings.
FIG. 1 shows a configuration of a refrigeration cycle apparatus such as an air conditioner or a refrigerator, and an internal configuration of a hermetic compressor mounted on the refrigeration cycle apparatus. The hermetic compressor 1 is covered with a metal hermetic container 1a. Two suction ports 2a and 2b are attached to the lower part of the sealed container 1a, and one discharge pipe 3 is attached to the upper part. One end of a condenser 31 is connected to the discharge pipe 3 via a high-pressure side pipe, and one end of an evaporator 33 is connected to the other end of the condenser 31 via an expansion device such as an expansion valve 32. The other end of the evaporator 33 is connected to the suction ports 2a and 2b via an accumulator 34 and two suction pipes 35.

密閉容器1aの内部には、永久磁石電動機10および圧縮機構部20が上下に分かれて収容されている。永久磁石電動機10は、密閉容器1aの内周面に接するように設けられた筒状の固定子11、この固定子11の内側に回転可能に設けられた回転子12を有する。この回転子12の中心部に回転軸(シャフトともいう)13が挿通され、その回転軸13が下方の圧縮機構部20に結合されている。   A permanent magnet electric motor 10 and a compression mechanism unit 20 are housed separately in the sealed container 1a. The permanent magnet motor 10 includes a cylindrical stator 11 provided so as to be in contact with the inner peripheral surface of the hermetic container 1a, and a rotor 12 provided rotatably inside the stator 11. A rotation shaft (also referred to as a shaft) 13 is inserted through the center of the rotor 12, and the rotation shaft 13 is coupled to the compression mechanism portion 20 below.

圧縮機構部20は、上記吸込口2a,2bにそれぞれ連通する2つの圧縮室21a,21b、およびこの圧縮室21a,21b内で上記回転軸13の回動を受けて偏心回転するローラ22a,22bを有し、ローラ22a,22bの偏心回転により圧縮室21a,21b内のガス冷媒を圧縮して密閉容器1a内に吐出する。吐出されたガス冷媒は、吐出管3を通って凝縮器31に流れる。   The compression mechanism unit 20 includes two compression chambers 21a and 21b communicating with the suction ports 2a and 2b, and rollers 22a and 22b that rotate eccentrically in response to the rotation of the rotary shaft 13 in the compression chambers 21a and 21b. The gas refrigerant in the compression chambers 21a, 21b is compressed by the eccentric rotation of the rollers 22a, 22b and discharged into the sealed container 1a. The discharged gas refrigerant flows to the condenser 31 through the discharge pipe 3.

永久磁石電動機10の回転子12は、図2に示すように、円形の多数枚の鋼板を積層してなる第1コア12a、および同じく円形の多数枚の鋼板を積層してなる第2コア12bを、回転軸13の軸方向に沿って配列してなる。   As shown in FIG. 2, the rotor 12 of the permanent magnet motor 10 includes a first core 12a formed by stacking a large number of circular steel plates and a second core 12b formed by stacking a plurality of circular steel plates. Are arranged along the axial direction of the rotary shaft 13.

第1コア12aおよび第2コア12bは、図3に示すように、中心部に回転軸挿通孔41aを有し、その回転軸挿通孔41aを囲む略正方形の四辺の位置にそれぞれ直線状の磁石収容孔42を有する。これら磁石収容孔42は、回転軸挿通孔41aに沿ってコア12a,12bを貫通する深さ形状を持つ。そして、第1コア12aの4つの磁石収容孔42に、板状で低保磁力の4極(=4個)の第1永久磁石43がそれぞれ収容される。これら第1永久磁石43は、磁石収容孔42の細長方向の幅よりも小さい幅W1を有し、幅W1の中央位置が磁石収容孔42の幅方向中央部と対応する状態に収容および固定される。また、図4に示すように、第2コア12bの4つの磁石収容孔42に、板状で高保磁力の4極の第2永久磁石44がそれぞれ収容される。これら第2永久磁石44は、磁石収容孔42の細長方向の幅とほぼ同じ幅Wを有している。したがって、第1永久磁石43の幅W1は、第2永久磁石44の幅Wより小さく形成されている。
また、図5に示すように、固定子11の内周面に複数の磁極歯が形成され、これら磁極歯に3つの相巻線Lu,Lv,Lwが集中巻き装着される。この相巻線Lu,Lv,Lwが発する磁界と上記各永久磁石43,44が発する磁界との相互作用により、回転子12が回転する。
As shown in FIG. 3, each of the first core 12a and the second core 12b has a rotation shaft insertion hole 41a at the center, and linear magnets are positioned at four substantially square sides surrounding the rotation shaft insertion hole 41a. A housing hole 42 is provided. These magnet accommodation holes 42 have a depth shape that penetrates the cores 12a and 12b along the rotation shaft insertion hole 41a. Then, the plate-shaped, four-pole (= 4) first permanent magnets 43 having low coercive force are accommodated in the four magnet accommodating holes 42 of the first core 12a. These first permanent magnets 43 have a width W1 that is smaller than the width of the magnet housing hole 42 in the elongated direction, and are housed and fixed in a state in which the center position of the width W1 corresponds to the widthwise center of the magnet housing hole 42. The Also, as shown in FIG. 4, plate-like, high coercivity, four-pole second permanent magnets 44 are accommodated in the four magnet accommodation holes 42 of the second core 12b, respectively. These second permanent magnets 44 have substantially the same width W as the width of the magnet housing hole 42 in the elongated direction. Therefore, the width W 1 of the first permanent magnet 43 is smaller than the width W of the second permanent magnet 44.
Further, as shown in FIG. 5, a plurality of magnetic pole teeth are formed on the inner peripheral surface of the stator 11, and three phase windings Lu, Lv, Lw are concentratedly mounted on these magnetic pole teeth. The rotor 12 rotates due to the interaction between the magnetic field generated by the phase windings Lu, Lv, and Lw and the magnetic field generated by the permanent magnets 43 and 44.

さらに、図6に示すように、相巻線Lu,Lv,Lwは中性点Cで星形結線されており、その相巻線Lu,Lv,Lwの非結線端に駆動装置が接続される。この駆動装置は、商用交流電源50の交流電圧を直流電圧に変換する順変換部51、この順変換部51の出力端に接続されたスイッチング回路52、このスイッチング回路52のスイッチングを制御する制御部53、スイッチング回路52と相巻線Lu,Lv,Lwとの間の各通電線に接続された2相通電位置検出部54、スイッチング回路52と相巻線Lu,Lv,Lwとの間の2つの通電線に設けられた電流センサ55,56、この電流センサ55,56に接続されたセンサレスベクトル制御部57などで構成される。   Further, as shown in FIG. 6, the phase windings Lu, Lv, Lw are star-connected at a neutral point C, and a driving device is connected to the non-connected ends of the phase windings Lu, Lv, Lw. . The drive device includes a forward conversion unit 51 that converts an AC voltage of a commercial AC power supply 50 into a DC voltage, a switching circuit 52 connected to an output terminal of the forward conversion unit 51, and a control unit that controls switching of the switching circuit 52. 53, a two-phase energization position detector 54 connected to each energization line between the switching circuit 52 and the phase windings Lu, Lv, Lw, and 2 between the switching circuit 52 and the phase windings Lu, Lv, Lw. It comprises current sensors 55 and 56 provided on one energization line, a sensorless vector control unit 57 connected to the current sensors 55 and 56, and the like.

上記スイッチング回路52は、一対のスイッチング素子の直列回路を3相分設けたもので、U相用としてスイッチング素子U+,U−の直列回路、V相用としてスイッチング素子V+,V−の直列回路、W相用としてスイッチング素子W+,W−の直列回路を有し、順変換部51の出力電圧(直流電圧)を三相交流電圧に変換する。このスイッチング回路52のスイッチング素子U+,U−の相互接続点に相巻線Luの非結線端が接続され、スイッチング素子V+,V−の相互接続点に相巻線Lvの非結線端が接続され、スイッチング素子W+,W−の相互接続点に相巻線Lwの非結線端が接続されるとともに、各スイッチング素子のベースに制御部53が接続される。   The switching circuit 52 is provided with a series circuit of a pair of switching elements for three phases, a series circuit of switching elements U + and U− for U phase, a series circuit of switching elements V + and V− for V phase, It has a series circuit of switching elements W + and W− for the W phase, and converts the output voltage (DC voltage) of the forward converter 51 into a three-phase AC voltage. The non-connection end of the phase winding Lu is connected to the interconnection point of the switching elements U + and U− of the switching circuit 52, and the non-connection end of the phase winding Lv is connected to the interconnection point of the switching elements V + and V−. The non-connection end of the phase winding Lw is connected to the interconnection point of the switching elements W + and W−, and the control unit 53 is connected to the base of each switching element.

上記2相通電位置検出部54は、3つの相巻線Lu,Lv,Lwのうち2つの相巻線に順に電流が流れる2相通電時、非通電状態の1つの相巻線に誘起する電圧から回転子12の回転位置を検出する。非通電状態の1つの相巻線に誘起する電圧の波形を図7に示す。すなわち、誘起電圧のレベルと基準電位(直流電圧の1/2または抵抗器で作られた仮想中性点電位)とが比較され、誘起電圧のレベルが基準電位を横切るときのタイミングから、回転子12の回転位置を検出することができる。   The two-phase energization position detecting unit 54 is a voltage induced in one phase winding in a non-energized state during two-phase energization in which current sequentially flows in two phase windings of the three phase windings Lu, Lv, and Lw. To detect the rotational position of the rotor 12. FIG. 7 shows a waveform of a voltage induced in one phase winding in a non-energized state. That is, the level of the induced voltage and the reference potential (1/2 of the DC voltage or a virtual neutral point potential created by a resistor) are compared, and from the timing when the level of the induced voltage crosses the reference potential, the rotor Twelve rotational positions can be detected.

上記センサレスベクトル制御部57は、電流センサ55,56の検知電流に基づくベクトル制御により回転子12の回転位置を推定する。   The sensorless vector control unit 57 estimates the rotational position of the rotor 12 by vector control based on currents detected by the current sensors 55 and 56.

上記制御部53は、2相通電駆動の場合にはスイッチング回路52における1つの相の一方のスイッチング素子をオンして他方のスイッチング素子をオフし、同時に別の1つの相の一方のスイッチング素子をオフして他方のスイッチング素子をオンする2相通電を順次に切換えることにより、相巻線Lu,Lv,Lwの2つの相巻線に順次に電流が流れる2相通電の駆動を制御するもので、2相通電位置検出部54で検出される回転位置、またはセンサレスベクトル制御部57で推定される回転位置に応じて、スイッチング回路52の各スイッチング素子に対するオン,オフタイミングを制御する。   In the case of two-phase energization driving, the control unit 53 turns on one switching element of one phase in the switching circuit 52 and turns off the other switching element, and simultaneously turns one switching element of another phase on. By sequentially switching the two-phase energization that turns off and turns on the other switching element, the two-phase energization drive in which current flows sequentially through the two phase windings Lu, Lv, and Lw is controlled. The on / off timing of each switching element of the switching circuit 52 is controlled in accordance with the rotational position detected by the two-phase energization position detection unit 54 or the rotational position estimated by the sensorless vector control unit 57.

また、上記制御部53はセンサレスベクトル制御の場合には、センサレスベクトル制御部57で推定される回転位置に応じて、スイッチング回路52の各スイッチング素子に対するオン,オフタイミングを制御し、正弦波PWMの3相波形を出力する。   Further, in the case of sensorless vector control, the control unit 53 controls the on / off timing for each switching element of the switching circuit 52 according to the rotational position estimated by the sensorless vector control unit 57, and the sine wave PWM is controlled. Outputs a three-phase waveform.

なお、回転位置検出用に2相通電位置検出部54とセンサレスベクトル制御部57の2つを用いているが、少なくも一方があればよく、それぞれの駆動方式に応じて制御部53はスイッチング回路52の各スイッチング素子のオン,オフタイミングを制御する。ただ、2相通電位置検出回路54を用いると、センサレスベクトル制御部57を用いる場合のように弱め界磁で回転数を高めるようなことができないこと、また運転電流が矩形波となるため電動機騒音が大きくなる等の問題があることから、通常運転はセンサレスベクトル制御部57を用いる方が望ましい。   The two-phase energized position detecting unit 54 and the sensorless vector control unit 57 are used for detecting the rotational position. However, at least one of them is sufficient, and the control unit 53 is a switching circuit according to each driving method. The on / off timing of each switching element 52 is controlled. However, if the two-phase energization position detection circuit 54 is used, it is not possible to increase the rotation speed with a field weakening as in the case of using the sensorless vector control unit 57, and the operating current becomes a rectangular wave, so that the motor noise Therefore, it is preferable to use the sensorless vector control unit 57 in normal operation.

このような構成の永久磁石電動機10において、回転子12の第1コア12aに収容されている低保磁力の各第1永久磁石43は、固定子11と回転子12が図5に示すような位置関係の時に、図8に示すように、相巻線Lu,Lv,Lwに励磁電圧Edを印加して相巻線Lu,Lv,Lwに励磁電流を供給することにより、着磁または減磁して磁力を変化させることができる。このとき、回転子12の第2コア12bに収容されている高保磁力の各第2永久磁石44は、保磁力が高いことから、相巻線Lu,Lv,Lwに励磁電流が供給されても、磁力が変化することはない。つまり、第1コア12aが磁束量可変となり、第2コア12bが磁束量非可変となる。   In the permanent magnet electric motor 10 having such a configuration, each of the first coercive magnets 43 having a low coercive force housed in the first core 12a of the rotor 12 includes the stator 11 and the rotor 12 as shown in FIG. In the positional relationship, as shown in FIG. 8, the excitation voltage Ed is applied to the phase windings Lu, Lv, Lw and the excitation current is supplied to the phase windings Lu, Lv, Lw, thereby magnetizing or demagnetizing. Thus, the magnetic force can be changed. At this time, each of the second permanent magnets 44 having a high coercive force housed in the second core 12b of the rotor 12 has a high coercive force, so even if an excitation current is supplied to the phase windings Lu, Lv, and Lw. The magnetic force does not change. That is, the first core 12a is variable in magnetic flux, and the second core 12b is non-variable in magnetic flux.

なお、第1コア12aの各第1永久磁石43に対する着磁に際しては、図5に示す相巻線Luに対向している2つの相対向する第1永久磁石43(A),43(A)と、相巻線Luに対向していない残りの2つの相対向する第1永久磁石43(B),43(B)との間で、図9に示すように磁化力が異なる。すなわち、回転子12の回転停止位置が図示の状態では第1永久磁石43(A),43(A)の磁力が大きくなり、第1永久磁石43(B),43(B)の磁力は小さくなる。そこで、1回目の着磁が終わった後、回転子12を90°回転し、相巻線Lu,Lv,Lwに極性が逆の励磁電流を再度供給する2回目の着磁を行うことにより、各第1永久磁石43の磁化力をほぼ同じ状態に設定することができる。   When magnetizing each first permanent magnet 43 of the first core 12a, two opposing first permanent magnets 43 (A) and 43 (A) facing the phase winding Lu shown in FIG. 9 and the remaining two first permanent magnets 43 (B) and 43 (B) facing each other not facing the phase winding Lu have different magnetizing forces as shown in FIG. That is, when the rotation stop position of the rotor 12 is in the illustrated state, the magnetic force of the first permanent magnets 43 (A) and 43 (A) is large, and the magnetic force of the first permanent magnets 43 (B) and 43 (B) is small. Become. Therefore, after the first magnetization is completed, the rotor 12 is rotated by 90 °, and the second magnetization is performed by supplying the excitation current having the opposite polarity to the phase windings Lu, Lv, Lw again. The magnetization force of each first permanent magnet 43 can be set to substantially the same state.

ただし、第1永久磁石43(A),43(A)においても磁化力は磁極中央部から端部に行くに従って小さくなり、磁極端部では電流・温度・永久磁石特性などに起因する着磁のバラツキが大きくなる。このため、磁束量の確実な可変が行えず、永久磁石電動機10の特性に悪影響を及ぼしてしまう。   However, also in the first permanent magnets 43 (A) and 43 (A), the magnetizing force decreases from the center of the magnetic pole to the end, and at the end of the magnetic pole, magnetization caused by current, temperature, permanent magnet characteristics, etc. Variations increase. For this reason, the amount of magnetic flux cannot be reliably changed, and the characteristics of the permanent magnet motor 10 are adversely affected.

そこで、第1コア12aの各第1永久磁石43の幅を、第2コア12bの各第2永久磁石44の幅よりも小さいW1としている。さらに、各第1永久磁石43の幅方向中央部を、各磁石収容孔42の幅方向中央部と対応させている。   Therefore, the width of each first permanent magnet 43 of the first core 12a is set to W1 smaller than the width of each second permanent magnet 44 of the second core 12b. Furthermore, the width direction center part of each first permanent magnet 43 is made to correspond to the width direction center part of each magnet accommodation hole 42.

このように、各第1永久磁石43の幅を大きな磁化力が得られるW1に制限することで、各第1永久磁石43の磁化力が安定化する。これにより、回転子12の磁束量を適正な状態に確実に設定することができ、永久磁石電動機10の安定した動作特性が得られる。また、各第1永久磁石43の幅がW1と小さくなるので、各第1永久磁石43の量を削減することができ、コストの低減が図れる。   In this way, by limiting the width of each first permanent magnet 43 to W1 at which a large magnetizing force is obtained, the magnetizing force of each first permanent magnet 43 is stabilized. Thereby, the magnetic flux amount of the rotor 12 can be reliably set to an appropriate state, and stable operating characteristics of the permanent magnet motor 10 can be obtained. Moreover, since the width | variety of each 1st permanent magnet 43 becomes small with W1, the quantity of each 1st permanent magnet 43 can be reduced and cost reduction can be aimed at.

なお、着磁または減磁のための励磁は、回転子が停止中で固定子と回転子の位置関係が図5に示す状態でも、あるいは回転中に固定子と回転子の位置関係が図5に示す状態になったときに行ってもよい。   The excitation for magnetization or demagnetization is performed even when the rotor is stopped and the positional relationship between the stator and the rotor is as shown in FIG. It may be performed when the state shown in FIG.

高保磁力の各第2永久磁石44については、予め大電流で着磁するので、幅が大きくても、端部まで十分な磁化力を与えることができる。   Since each second permanent magnet 44 having a high coercive force is previously magnetized with a large current, a sufficient magnetizing force can be applied to the end portion even if the width is large.

ここで、図10に示すB−H曲線を用いて、永久磁石の動作について説明しておく。
磁気回路中の永久磁石の動作は、永久磁石のB−H曲線と、磁気回路および永久磁石によって定まるパーミアンス係数Pcによって決まり、B−H曲線とパーミアンス線(Pc線)との交点pで動作する。永久磁石はこの動作点pにおける磁束密度B0で磁化される。このとき、固定子から発生する回転磁束のd軸成分を負方向に増加させると、永久磁石に負方向の磁化力がかかり、パーミアンス線が負方向(図示左方向)に平行移動して動作点がp1に移り、磁束密度はB1に低下する。一方、固定子から発生する回転磁束のd軸成分を正方向に増加させると、永久磁石に正方向の磁化力がかかり、パーミアンス線が正方向(図示右方向)に平行移動して動作点がp2に移り、磁束密度はB2に上昇する。
Here, the operation of the permanent magnet will be described using the BH curve shown in FIG.
The operation of the permanent magnet in the magnetic circuit is determined by the BH curve of the permanent magnet and the permeance coefficient Pc determined by the magnetic circuit and the permanent magnet, and operates at the intersection p between the BH curve and the permeance line (Pc line). . The permanent magnet is magnetized at the magnetic flux density B0 at this operating point p. At this time, if the d-axis component of the rotating magnetic flux generated from the stator is increased in the negative direction, a negative direction magnetizing force is applied to the permanent magnet, and the permeance line is translated in the negative direction (the left direction in the figure). Moves to p1, and the magnetic flux density decreases to B1. On the other hand, when the d-axis component of the rotating magnetic flux generated from the stator is increased in the positive direction, a permanent magnetizing force is applied to the permanent magnet, the permeance line is translated in the positive direction (right direction in the figure), and the operating point is Moving to p2, the magnetic flux density rises to B2.

このように、固定子から発生する回転磁束のd軸成分の増減によって永久磁石の磁束密度を変化させ、磁束量を増減できることに間違いはないが、この現象は低保磁力の永久磁石のみに起こるのではなく、高保磁力の永久磁石にも同様に起こる。   As described above, there is no doubt that the magnetic flux density of the permanent magnet can be changed by increasing or decreasing the d-axis component of the rotating magnetic flux generated from the stator, so that the amount of magnetic flux can be increased or decreased. However, this phenomenon occurs only in the low coercive force permanent magnet. Instead, it also occurs in high coercivity permanent magnets.

また、永久磁石の動作点はB−H曲線上を移動するが、B−H曲線の傾きはリコイル比透磁率μrecで表わされる。このリコイル比透磁率μrecは、希土類磁石では1に近く、真空中の透磁率4π×10−7にほぼ等しい。このため、磁束密度を大きく変えるためには、かなり大きな磁化力を加えなければならず、このためのd軸成分の磁束を発生するためには大きな励磁電流が必要となる。励磁電流を大きくするためには、駆動装置の電流容量を大きくしなければならず、駆動装置および電動機の効率が低下するという問題がある。 The operating point of the permanent magnet moves on the BH curve, and the slope of the BH curve is expressed by the recoil relative permeability μrec. The recoil relative permeability μrec is close to 1 in the rare earth magnet and is substantially equal to the permeability 4π × 10 −7 in vacuum. For this reason, in order to greatly change the magnetic flux density, it is necessary to apply a considerably large magnetizing force, and in order to generate a d-axis component magnetic flux for this purpose, a large excitation current is required. In order to increase the excitation current, it is necessary to increase the current capacity of the drive device, and there is a problem that the efficiency of the drive device and the electric motor is reduced.

なお、特許文献1に記載のものでは、高保磁力・低透磁率と低保磁力・高透磁率の二つの磁石を組み合わせているが、高透磁率の永久磁石ではB−H曲線の傾きが大きく、磁化力による動作点の磁束密度の変化が大きく、より少ない電流で磁束量を可変できることになる。しかし、この作用と保磁力は無関係であり、低保磁力と高保磁力を組み合わせることには意味がない。   In addition, in the thing of patent document 1, although two magnets of high coercive force / low magnetic permeability and low coercive force / high magnetic permeability are combined, the inclination of the BH curve is large in a high magnetic permeability permanent magnet. The change in the magnetic flux density at the operating point due to the magnetizing force is large, and the amount of magnetic flux can be varied with a smaller current. However, this action and the coercive force are irrelevant, and it is meaningless to combine the low coercive force and the high coercive force.

以上の通り、特許文献1に記載のものは、基本的に永久磁石のB−H曲線の直線部(リコイル線)における動作を利用したもので、動作は可逆的である。(可逆的な減磁および増磁)。   As described above, the one described in Patent Document 1 basically uses the operation in the straight line portion (recoil wire) of the BH curve of the permanent magnet, and the operation is reversible. (Reversible demagnetization and magnetization).

これに対して、永久磁石の磁化を非可逆的に変化させれば、大きな磁束量の変化が得られる。これは、永久磁石の非可逆減磁および再着磁を利用するものである。   On the other hand, if the magnetization of the permanent magnet is changed irreversibly, a large change in the amount of magnetic flux can be obtained. This utilizes irreversible demagnetization and remagnetization of a permanent magnet.

図10から分かるように、永久磁石に大きな負の磁化力を加えると、動作点はB−H曲線の屈曲点を越えて移動する。このようにすると、負の磁化力を取り去っても永久磁石は元のB−H曲線上を戻ることはできず(非可逆減磁が発生して)、動作点はp´点になり、磁束密度が大きく減少する。このとき、高保磁力の永久磁石では磁化力を加えても動作点が屈曲点を越えないので非可逆減磁は発生せず、元の磁束密度に戻る。   As can be seen from FIG. 10, when a large negative magnetizing force is applied to the permanent magnet, the operating point moves beyond the inflection point of the BH curve. In this way, even if the negative magnetizing force is removed, the permanent magnet cannot return to the original BH curve (irreversible demagnetization occurs), and the operating point becomes the p 'point, and the magnetic flux The density is greatly reduced. At this time, even if a magnetizing force is applied to the permanent magnet having a high coercive force, the operating point does not exceed the bending point, so irreversible demagnetization does not occur, and the original magnetic flux density is restored.

このような非可逆減磁を発生するためには、短時間だけ負の磁化力を加える励磁電流を流せばよい。この後、永久磁石の磁束密度を増大させたいときは短時間の正の磁化力を加えて再着磁を行えばよい。このとき、永久磁右の保磁力の違いを利用し、低保磁力永久磁石のみに非可逆減磁を発生させることで、一定の磁束量を確保した上で大きな磁束量の変化を得ることができる。   In order to generate such irreversible demagnetization, an excitation current for applying a negative magnetizing force only for a short time may be supplied. Thereafter, when it is desired to increase the magnetic flux density of the permanent magnet, re-magnetization may be performed by applying a short positive magnetic force. At this time, by utilizing the difference in coercivity on the right side of the permanent magnet and generating irreversible demagnetization only in the low coercivity permanent magnet, it is possible to obtain a large change in the amount of magnetic flux while ensuring a certain amount of magnetic flux. it can.

[2]第2の実施形態について説明する。
図11および図12に示すように、回転子12のコア12a,12bにおける各磁石収容孔42より外周側に、複数のスリット45が形成される。これらスリット45は、コア12a,12bの径方向に沿う細長形状を有するとともに、回転軸挿通孔41aに沿ってコア12a,12bを貫通する深さ形状を有する。
[2] A second embodiment will be described.
As shown in FIGS. 11 and 12, a plurality of slits 45 are formed on the outer peripheral side of the magnet housing holes 42 in the cores 12 a and 12 b of the rotor 12. These slits 45 have an elongated shape along the radial direction of the cores 12a and 12b, and a depth shape that penetrates the cores 12a and 12b along the rotation shaft insertion hole 41a.

また、各スリット45は、コア12a,12bの径方向における内周側端部と各磁石収容孔42との間隔が小さく設定されるとともに、コア12a,12bの径方向における外周側端部と回転子12の外周縁との間隔が小さく設定されている。これらの設定により、各スリット42の相互間部分が磁路として確保され、そこを各第1永久磁石43,44の磁束が効率よく通るようになる。   In addition, each slit 45 is set to have a small interval between the inner peripheral side end in the radial direction of the cores 12a and 12b and each magnet housing hole 42, and rotates with the outer peripheral side end in the radial direction of the cores 12a and 12b. The distance from the outer peripheral edge of the child 12 is set small. With these settings, the portion between the slits 42 is secured as a magnetic path, and the magnetic fluxes of the first permanent magnets 43 and 44 efficiently pass therethrough.

とくに、各スリット45の存在は、回転子12の周方向における磁束の流れを規制するものであって、図13に示すように、各第1永久磁石43での磁化力分布を各第1永久磁石43の中央部でより大きくする作用を生じる。この結果、各第1永久磁石43の磁化力がさらに安定化する。
他の構成および作用は第1の実施形態と同じである。よって、その説明は省略する。
In particular, the presence of each slit 45 regulates the flow of magnetic flux in the circumferential direction of the rotor 12, and as shown in FIG. 13, the distribution of the magnetizing force in each first permanent magnet 43 is changed to each first permanent magnet. The effect | action which enlarges in the center part of the magnet 43 is produced. As a result, the magnetization force of each first permanent magnet 43 is further stabilized.
Other configurations and operations are the same as those of the first embodiment. Therefore, the description is omitted.

[3]第3の実施形態について説明する。
図14に示すように、第1コア12aの各磁石収容孔42がV字形状を有し、これら磁石収容孔42に2分割状態の第1永久磁石43a,43bがそれぞれ収容される。同様に、図15に示すように、第2コア12bの各磁石収容孔42がV字形状を有し、これら磁石収容孔42に2分割状態の第2永久磁石44a,44bがそれぞれ収容される。
[3] A third embodiment will be described.
As shown in FIG. 14, each magnet accommodation hole 42 of the first core 12 a has a V shape, and the first permanent magnets 43 a and 43 b in a two-divided state are accommodated in these magnet accommodation holes 42, respectively. Similarly, as shown in FIG. 15, each magnet accommodation hole 42 of the second core 12 b has a V shape, and the second permanent magnets 44 a and 44 b that are divided into two are accommodated in these magnet accommodation holes 42, respectively. .

第1永久磁石43a,43bの2つを合わせた幅が第2永久磁石44a,44bの2つを合わせた幅より小さい幅を有する点は、第1の実施形態と同じである。すなわち、第1永久磁石43a,43bの2つを合わせた幅は第1の実施形態における第1永久磁石43の幅W1と同等であり、第2永久磁石44a,44bの2つを合わせた幅は第1の実施形態における第2永久磁石44の幅Wと同等である。第1永久磁石43a,43bは端部同士が略密接するように設けられている。   It is the same as the first embodiment in that the combined width of the two first permanent magnets 43a and 43b is smaller than the combined width of the second permanent magnets 44a and 44b. That is, the combined width of the first permanent magnets 43a and 43b is equal to the width W1 of the first permanent magnet 43 in the first embodiment, and the combined width of the second permanent magnets 44a and 44b. Is equivalent to the width W of the second permanent magnet 44 in the first embodiment. The first permanent magnets 43a and 43b are provided so that the ends are in close contact with each other.

このようなものにおいても、第1の実施形態と同様に、図8に示すように、相巻線Lu,Lv,Lwに励磁電圧Edを印加して相巻線Lu,Lv,Lwに励磁電流を供給することにより、着磁または減磁して磁力を変化させることができる。   Even in such a case, as in the first embodiment, as shown in FIG. 8, the excitation voltage Ed is applied to the phase windings Lu, Lv, Lw, and the excitation current is applied to the phase windings Lu, Lv, Lw. Can be magnetized or demagnetized to change the magnetic force.

他の構成および作用は第1の実施形態と同じである。よって、その説明は省略する。   Other configurations and operations are the same as those of the first embodiment. Therefore, the description is omitted.

また、固定子11と回転子12が図17に示すような位置関係のときに、図16に示すように、相巻線Lu,Lv,Lwのうち2つの相巻線に励磁電圧Edを印加して励磁電流を流す着磁または減磁を第1の実施形態と同様に回転子の位置と励磁電流の極性を変えて少なくとも2回行うことにより、各磁石収容孔42の第1永久磁石43a,43bをそれぞれ最適な状態に着磁または減磁することもできる。   When the stator 11 and the rotor 12 are in the positional relationship as shown in FIG. 17, the excitation voltage Ed is applied to two phase windings of the phase windings Lu, Lv, and Lw as shown in FIG. Then, the first permanent magnet 43a in each magnet housing hole 42 is obtained by performing magnetization or demagnetization for flowing an excitation current at least twice by changing the position of the rotor and the polarity of the excitation current in the same manner as in the first embodiment. 43b can be magnetized or demagnetized in an optimum state.

ただし、この場合には、図18に示すように、第1永久磁石43a,43bの境界部(各極の中央付近)の磁力化が小さくなってしまう。   However, in this case, as shown in FIG. 18, the magnetic force at the boundary between the first permanent magnets 43 a and 43 b (near the center of each pole) becomes small.

そこで、この場合には、図14に示す第1永久磁石43a,43bの端部同士が離間するように、すなわち、第1永久磁石43a,43bの端部間に空間ができるように配置することで上記と同様の効果が得られる。
なお、図16に示すように、相巻線Lu,Lv,Lwのうち2つの相巻線に励磁電圧Edを印加して励磁電流を流す着磁または減磁を、図3に示すような各極に1枚の永久磁石が配置された回転子に適用すると、各極の中央付近の磁化力が弱くなることになる。
Therefore, in this case, the end portions of the first permanent magnets 43a and 43b shown in FIG. 14 are arranged to be separated from each other, that is, so as to have a space between the end portions of the first permanent magnets 43a and 43b. Thus, the same effect as described above can be obtained.
As shown in FIG. 16, magnetization or demagnetization for applying an excitation voltage Ed to two phase windings of the phase windings Lu, Lv, and Lw to flow an excitation current is performed as shown in FIG. When applied to a rotor in which a single permanent magnet is disposed on each pole, the magnetizing force near the center of each pole is weakened.

そこで、この場合は図3に示す低保磁力の第1永久磁石43を幅方向に分割し、それぞれの幅を小さくして中央部に空間ができるように配置することで上記と同様の効果が得られる。
励磁電流を流すときの回転子は第1の実施形態と同様に停止中でも回転中でもよい。
Therefore, in this case, the same effect as described above can be obtained by dividing the first permanent magnets 43 having a low coercive force shown in FIG. 3 in the width direction and reducing the respective widths so that a space is formed in the central portion. can get.
The rotor for supplying the exciting current may be stopped or rotating as in the first embodiment.

[4]第4の実施形態について説明する。
第4の実施形態では、2相通電の駆動により回転子12を回転させながら、2相通電位置検出部54の検出位置に応じて各第1永久磁石43の着磁または減磁を行う。
[4] A fourth embodiment will be described.
In the fourth embodiment, each first permanent magnet 43 is magnetized or demagnetized according to the detection position of the two-phase energization position detection unit 54 while rotating the rotor 12 by driving the two-phase energization.

すなわち、相巻線Lu,Lv,Lwの2つずつの相巻線に電流が順に流れる2相通電を実行しながら、非通電状態の相巻線に誘起する電圧に基づいて2相通電位置検出部54が回転子12の回転位置を検出し、検出した回転位置に応じたタイミングで相巻線Lu,Lv,Lwに着磁用または減磁用の励磁電流を供給する。このときの励磁電流の供給は第1の実施形態または第3の実施形態に示されるように行うものである。
通常、センサレスベクトル制御部57による位置推定は誤差が大きく、上記のように2相通電位置検出部54の検出位置に応じて各第1永久磁石43の着磁または減磁を行うことにより、固定子と回転子のより正確な位置関係で着磁または減磁のための通電を行うことができ、磁束可変の確実性が高くなる。
That is, two-phase energization position detection is performed based on a voltage induced in a non-energized phase winding while performing two-phase energization in which current flows in sequence in each of the phase windings Lu, Lv, and Lw. The unit 54 detects the rotational position of the rotor 12 and supplies an excitation current for magnetization or demagnetization to the phase windings Lu, Lv, Lw at a timing according to the detected rotational position. In this case, the excitation current is supplied as shown in the first embodiment or the third embodiment.
Normally, the position estimation by the sensorless vector control unit 57 has a large error, and is fixed by magnetizing or demagnetizing each first permanent magnet 43 according to the detection position of the two-phase energization position detection unit 54 as described above. Energization for magnetization or demagnetization can be performed with a more accurate positional relationship between the rotor and the rotor, and the certainty of variable magnetic flux is increased.

なお、2相通電位置検出部54の検出位置に応じた2相通電の駆動では、センサレスベクトル制御のように弱め界磁で回転数を高めるような制御ができず、また運転電流が矩形波となるため、永久磁石電動機10の騒音が大きくなる等の問題があるため、通常運転時はセンサレスベクトル制御部57の推定位置に応じたベクトル制御による3相正弦波PWMの駆動を行うのが望ましい。
他の構成および作用は第1の実施形態と同じである。よって、その説明は省略する。
Incidentally, in the driving of the two-phase energization according to the detection position of the two-phase energization position detecting unit 54, it is not possible to control to increase the rotation speed with the weak field like the sensorless vector control, and the operation current is a rectangular wave. Therefore, since there is a problem that the noise of the permanent magnet motor 10 is increased, it is desirable to drive the three-phase sine wave PWM by vector control according to the estimated position of the sensorless vector control unit 57 during normal operation.
Other configurations and operations are the same as those of the first embodiment. Therefore, the description is omitted.

[5]第5の実施形態について説明する。
永久磁石電動機10の運転中、着磁または減磁のための励磁電流の供給に際し、2相通電位置検出部54の検出位置に従って適切なタイミングでセンサレスベクトル制御部57による運転に切り替え、相巻線Lu,Lv,Lwにd軸電流を供給する。
[5] A fifth embodiment will be described.
During operation of the permanent magnet motor 10, when supplying an excitation current for magnetization or demagnetization, the operation is switched to the operation by the sensorless vector control unit 57 at an appropriate timing according to the detection position of the two-phase energization position detection unit 54, and the phase winding A d-axis current is supplied to Lu, Lv, and Lw.

この場合のd軸電流は、運転トルクを発生させるためのq軸電流に重畳するように流す。   In this case, the d-axis current is supplied so as to be superimposed on the q-axis current for generating the operating torque.

なお、d軸およびq軸電流を供給するときは2相通電位置検出部54による位置検出はできないのでセンサレスベクトル制御部57による運転に切り替えるものである。 When the d-axis and q-axis currents are supplied, the position detection by the two-phase energization position detection unit 54 cannot be performed, so the operation is switched to the operation by the sensorless vector control unit 57.

第4の実施形態と同様に2相通電位置検出部54の検出位置に応じて着磁または減磁の通電を開始するので、固定子と回転子のより正確な位置関係で着磁または減磁のための通電を行うことができ、磁束可変の確実性が高くなる。   Since the energization of magnetization or demagnetization is started according to the detection position of the two-phase energization position detector 54 as in the fourth embodiment, the magnetization or demagnetization is performed with a more accurate positional relationship between the stator and the rotor. Can be energized, and the certainty of magnetic flux variation is increased.

この第5の実施形態のように、相巻線Lu,Lv,Lwにd軸電流を流すことは、センサレスベクトル制御のプ口グラムにおいて実行が可能であり、特別な制御ソフトウェアが不要であるという利点がある。
他の構成および作用は第1の実施形態と同じである。よって、その説明は省略する。
As in the fifth embodiment, it is possible to execute the d-axis current through the phase windings Lu, Lv, and Lw in the program of the sensorless vector control, and no special control software is required. There are advantages.
Other configurations and operations are the same as those of the first embodiment. Therefore, the description is omitted.

[6]第6の実施形態について説明する。
永久磁石電動機10の運転中、着磁または減磁のための励磁電流を供給する。具体的には、2相通電位置検出部54の検出位置に従って適切なタイミングでセンサレスベクトル制御部57による運転に切り替え、相巻線Lu,Lv,Lwに対し、励磁電流としてd軸電流を電気角で80°以上にわたり供給する。
[6] A sixth embodiment will be described.
During operation of the permanent magnet motor 10, an excitation current for magnetization or demagnetization is supplied. Specifically, the operation is switched to the operation by the sensorless vector control unit 57 at an appropriate timing according to the detection position of the two-phase energization position detection unit 54, and the d-axis current is converted into an electrical angle as an excitation current for the phase windings Lu, Lv, Lw. At 80 ° or more.

集中巻きの固定子11では、着磁用または減磁用のd軸電流を流した際に、各第1永久磁石43に加わる磁化力が各第1永久磁石43の位置によって大きなバラツキを持って分布し、固定子11と回転子12の位置関係により、分布が変化していく。これは、固定子11の相巻線Lu,Lv,Lwにd軸電流を流した場合に、固定子11および回転子12に生じる磁束が図19に示すように非対称となるためで、各第1永久磁石43に加わる磁化力の分布は図20のように回転子12の回転位置に応じて変化していく。   In the concentrated winding stator 11, the magnetization force applied to each first permanent magnet 43 varies greatly depending on the position of each first permanent magnet 43 when a magnetizing or demagnetizing d-axis current is passed. The distribution changes depending on the positional relationship between the stator 11 and the rotor 12. This is because when the d-axis current is passed through the phase windings Lu, Lv, Lw of the stator 11, the magnetic flux generated in the stator 11 and the rotor 12 becomes asymmetric as shown in FIG. The distribution of the magnetizing force applied to one permanent magnet 43 changes according to the rotational position of the rotor 12 as shown in FIG.

図20の角度は電気角を表し、0°〜120°の間で回転子12が60°回転し(4極なので)、その間に、各第1永久磁石43の磁化力分布が連続的に変化していく。   The angle in FIG. 20 represents an electrical angle, and the rotor 12 rotates 60 ° between 0 ° and 120 ° (because it has four poles), during which the magnetization force distribution of each first permanent magnet 43 changes continuously. I will do it.

従って、短い期間(例えば電気角で30°程度)の通電では、各第1永久磁石43の一部に着磁または減磁のための十分な磁化力が加わらない部分が生じる。   Therefore, when the energization is performed for a short period (for example, about 30 ° in electrical angle), a portion where a sufficient magnetizing force for magnetization or demagnetization is not applied to a part of each first permanent magnet 43 is generated.

固定子11と回転子12の位置関係による磁化力分布の変化は、電気角120°を一周期とするので、電気角で120°の期間だけ電流を流し続けることにより、ほぼ均一な着磁用磁界または減磁用磁界が与えられ、各第1永久磁石43の全体を確実に着磁・減磁することができる。   The change in the magnetizing force distribution due to the positional relationship between the stator 11 and the rotor 12 has an electrical angle of 120 ° as one cycle. A magnetic field or a demagnetizing magnetic field is applied, and the entire first permanent magnets 43 can be surely magnetized and demagnetized.

なお、電気角の適切な期間を選ぶことにより、実用的には電気角80°期間でも、ほぼ均一な着磁用磁界または減磁用磁界を得ることができる。   Note that, by selecting an appropriate period of electrical angle, practically a uniform magnetic field for demagnetization or demagnetization can be obtained even in an electrical angle period of 80 °.

[7]第7の実施形態について説明する。
第4の実施形態と同じく、2相通電の駆動により回転子12を回転させながら、2相通電位置検出部54の検出位置に応じて相巻線Lu,Lv,Lwに着磁用または減磁用の励磁電流を供給し、各第1永久磁石43を着磁または減磁する。
[7] A seventh embodiment will be described.
As in the fourth embodiment, the rotor 12 is rotated by the two-phase energization drive, and the phase windings Lu, Lv, Lw are magnetized or demagnetized according to the detection position of the two-phase energization position detection unit 54. For this reason, the first permanent magnets 43 are magnetized or demagnetized.

そして、この励磁電流の供給後、2相通電の駆動により回転子12を回転させながら、2相通電位置検出部54で検出される誘起電圧から回転子12の第1コア12aに生じる磁束量を求め、求めた磁束量が目標値に達していない場合に、再度、2相通電の駆動により回転子12を回転させながら、2相通電位置検出部54の検出位置に応じて相巻線Lu,Lv,Lwに着磁用または減磁用の励磁電流を供給し、各第1永久磁石43を着磁または減磁する。
こうして、再度の着磁または減磁を行うことで、所望の磁束を確実に得ることができる。
Then, after supplying the exciting current, the amount of magnetic flux generated in the first core 12a of the rotor 12 from the induced voltage detected by the two-phase energization position detecting unit 54 while rotating the rotor 12 by driving the two-phase energization. When the obtained magnetic flux amount does not reach the target value, the phase windings Lu and Lu according to the detection position of the two-phase energization position detection unit 54 while rotating the rotor 12 by driving the two-phase energization again. An excitation current for magnetization or demagnetization is supplied to Lv and Lw, and each first permanent magnet 43 is magnetized or demagnetized.
In this way, a desired magnetic flux can be reliably obtained by performing re-magnetization or demagnetization.

磁束量については、誘起電圧、極数(回転子12の1つのコアにおける永久磁石の個数に相当)、相巻線Lu,Lv,Lwの巻数、回転子12の回転数などを予め定められた所定の数式に代入することにより、算出することができる。   Regarding the amount of magnetic flux, the induced voltage, the number of poles (corresponding to the number of permanent magnets in one core of the rotor 12), the number of turns of the phase windings Lu, Lv, Lw, the number of rotations of the rotor 12, etc. are determined in advance. It can be calculated by substituting into a predetermined mathematical expression.

2相通電位置検出部54の検出位置に応じた2相通電の駆動では、センサレスベクトル制御のように弱め界磁で回転数を高めるような制御ができず、また運転電流が矩形波となるため、永久磁石電動機10の騒音が大きくなる等の問題があるため、通常運転時はセンサレスベクトル制御部57の推定位置に応じた2相通電の駆動を行うのが望ましい。
このセンサレスベクトル制御部57の推定位置に応じた2相通電駆動の通常運転への移行に際しては、上記算出した磁束量をセンサレスベクトル制御用のモータ定数として利用することができる。これにより、良好なセンサレスベクトル制御の2相通電駆動が可能となる。
In the driving of the two-phase energization according to the detection position of the two-phase energization position detection unit 54, it is not possible to control to increase the rotation speed by the weak field like the sensorless vector control, and the operation current becomes a rectangular wave. Since there is a problem that the noise of the permanent magnet motor 10 is increased, it is desirable to drive the two-phase energization according to the estimated position of the sensorless vector control unit 57 during normal operation.
When shifting to the normal operation of the two-phase energization drive according to the estimated position of the sensorless vector control unit 57, the calculated magnetic flux amount can be used as a motor constant for sensorless vector control. Thereby, two-phase energization driving with good sensorless vector control becomes possible.

[8]変形例
なお、上記各実施形態では、回転子12の1つのコアに設ける永久磁石の個数が4個であるいわゆる4極構成の永久磁石電動機10を例に説明したが、1つのコアに6個の永久磁石を設ける6極構成の永久磁石電動機10を用いる場合についても、同様に実施可能である。また、相巻線Lu,Lv,Lwが固定子11のスロットに集中巻き装着される場合を例に説明したが、分布巻き装着される場合についても、同様に実施可能である。
[8] Modification
In each of the above embodiments, the so-called four-pole permanent magnet motor 10 in which the number of permanent magnets provided in one core of the rotor 12 is four has been described as an example, but six permanent magnets are provided in one core. The same can be applied to the case of using a permanent magnet motor 10 having a six-pole configuration provided with magnets. Moreover, although the case where the phase windings Lu, Lv, and Lw are concentrated winding mounted on the slots of the stator 11 has been described as an example, the same can be applied to the case of distributed winding mounting.

その他、この発明は、上記各実施形態そのままに限定されるものではなく、実施段階ではその要旨を逸脱しない範囲で構成要素を変形して具体化できる。また、上記各実施形態に開示されている複数の構成要素の適宜な組み合わせにより種々の発明を形成できる。各実施形態に示される全構成要素から幾つかの構成要素を削除することも可能である。   In addition, the present invention is not limited to the above-described embodiments as they are, and can be embodied by modifying the constituent elements without departing from the scope of the invention in the implementation stage. In addition, various inventions can be formed by appropriately combining a plurality of constituent elements disclosed in the above embodiments. It is also possible to delete some components from all the components shown in each embodiment.

1…密閉型圧縮機、10…永久磁石電動機、11…固定子、12…回転子、12a…第1コア、12b…第2コア、31…凝縮器、32…膨張装置、33…蒸発器、41a…回転軸挿通孔、42…磁石収容孔、43…第1永久磁石、44…第2永久磁石、45…スリット、Lu,Lv,Lw…相巻線、50…商用交流電源、51…順変換部、52…スイッチング回路、53…制御部、54…2相通電位置検出部、57…センサベクトル制御部   DESCRIPTION OF SYMBOLS 1 ... Hermetic compressor, 10 ... Permanent magnet motor, 11 ... Stator, 12 ... Rotor, 12a ... 1st core, 12b ... 2nd core, 31 ... Condenser, 32 ... Expansion device, 33 ... Evaporator, 41a ... Rotating shaft insertion hole, 42 ... Magnet housing hole, 43 ... First permanent magnet, 44 ... Second permanent magnet, 45 ... Slit, Lu, Lv, Lw ... Phase winding, 50 ... Commercial AC power supply, 51 ... Forward Conversion unit, 52 ... switching circuit, 53 ... control unit, 54 ... two-phase energization position detection unit, 57 ... sensor vector control unit

Claims (7)

複数の相巻線が装着された固定子と、
第1コアおよび第2コアを回転軸の軸方向に沿って配列してなる回転子と、
前記第1コアにおける前記回転軸を囲む位置に形成されたV字形状の複数の第1磁石収容孔と、
前記第2コアにおける前記回転軸を囲む位置に形成されたV字形状の複数の第2磁石収容孔と、
前記各第1磁石収容孔にそのV字形状に合せて2分割状態で収容され、駆動装置から前記各相巻線に供給される励磁電流により着磁または減磁されて磁力が変化する複数の第1永久磁石と、
前記各第2磁石収容孔にそのV字形状に合せて2分割状態で収容され、前記励磁電流の供給にかかわらず磁力変化がない複数の第2永久磁石と、
を備え、
前記各第1永久磁石の幅を前記各第2永久磁石の幅よりも小さくし
前記着磁または減磁に際しての前記固定子と前記回転子の位置関係に応じて、前記各第1磁石収容孔における2分割状態の第1永久磁石の端部同士を密接または離間させる、
ことを特徴とする永久磁石電動機。
A stator equipped with a plurality of phase windings;
A rotor formed by arranging the first core and the second core along the axial direction of the rotation axis;
A plurality of V-shaped first magnet housing holes formed at positions surrounding the rotation shaft in the first core;
A plurality of V-shaped second magnet receiving holes formed at positions surrounding the rotating shaft in the second core;
Each of the first magnet accommodating holes is accommodated in a two-divided state in accordance with the V shape, and is magnetized or demagnetized by an excitation current supplied from the driving device to the phase windings to change the magnetic force. A first permanent magnet;
A plurality of second permanent magnets that are accommodated in the second magnet accommodation holes in a two-divided state in accordance with the V shape, and that do not change in magnetic force regardless of the supply of the excitation current,
With
The width of each first permanent magnet is made smaller than the width of each second permanent magnet ,
According to the positional relationship between the stator and the rotor at the time of magnetization or demagnetization, the ends of the first permanent magnets in the two-divided state in the first magnet housing holes are closely or separated from each other,
A permanent magnet motor characterized by that.
前記回転子における各永久磁石の収容部より外周側に形成された複数のスリット、をさらに備えることを特徴とする請求項1記載の永久磁石電動機。   2. The permanent magnet electric motor according to claim 1, further comprising a plurality of slits formed on an outer peripheral side of a housing portion of each permanent magnet in the rotor. 前記駆動装置は、
前記各相巻線の2つずつの相巻線に電流が順に流れる2相通電を実行しながら、非通電状態の相巻線に誘起する電圧に基づいて前記回転子の回転位置を検出し、検出した回転位置に応じたタイミングで前記各相巻線に着磁用または減磁用の励磁電流を供給する制御手段、
を備えることを特徴とする請求項1記載の永久磁石電動機。
The driving device includes:
Detecting the rotational position of the rotor based on the voltage induced in the non-energized phase winding while performing two-phase energization in which current sequentially flows through the two phase windings of each phase winding, Control means for supplying an excitation current for magnetization or demagnetization to each phase winding at a timing according to the detected rotational position;
The permanent magnet motor according to claim 1, further comprising:
前記励磁電流は、センサレスベクトル制御のd軸電流であることを特徴とする請求項3記載の駆動装置。   4. The driving apparatus according to claim 3, wherein the excitation current is a d-axis current of sensorless vector control. 前記駆動装置は、
前記各相巻線の2つずつの相巻線に順に電流が流れる2相通電を実行しながら、非通電状態の相巻線に誘起する電圧に基づいて前記回転子の回転位置を検出し、検出した回転位置に応じたタイミングで前記各相巻線に着磁用または減磁用の励磁電流を供給する第1制御手段と、
この第1制御手段による励磁電流の供給後、前記各相巻線の2つずつの相巻線に順に電流が流れる2相通電を実行しながら、非通電状態の相巻線に誘起する電圧から前記回転子の第1コアに生じる磁束量を求め、求めた磁束量が目標値に達していない場合に、前記第1制御手段による励磁電流の供給を再び実行する第2制御手段と、
を備えることを特徴とする請求項1記載の永久磁石電動機。
The driving device includes:
Detecting the rotational position of the rotor based on the voltage induced in the non-energized phase winding while performing two-phase energization in which current sequentially flows through the two phase windings of each phase winding, First control means for supplying an excitation current for magnetization or demagnetization to each phase winding at a timing according to the detected rotational position;
After the excitation current is supplied by the first control means, the two-phase energization in which the current sequentially flows through the two phase windings of each phase winding, while the voltage induced in the non-energized phase winding is Second control means for obtaining the amount of magnetic flux generated in the first core of the rotor, and executing the supply of excitation current by the first control means again when the obtained magnetic flux amount does not reach the target value;
The permanent magnet motor according to claim 1, further comprising:
請求項1乃至5の何れかに記載の永久磁石電動機と、この永久磁石電動機により駆動される圧縮機構部とを、密閉容器に収納したことを特徴とする密閉型圧縮機。   6. A hermetic compressor, wherein the permanent magnet motor according to claim 1 and a compression mechanism portion driven by the permanent magnet motor are housed in a hermetic container. 請求項6に記載の密閉型圧縮機と、凝縮器と、膨張装置と、蒸発器とからなることを特徴とする冷凍サイクル装置。   A refrigeration cycle apparatus comprising the hermetic compressor according to claim 6, a condenser, an expansion device, and an evaporator.
JP2009042515A 2009-02-25 2009-02-25 Permanent magnet motor, hermetic compressor, and refrigeration cycle apparatus Expired - Fee Related JP5334303B2 (en)

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