JP5178487B2 - Permanent magnet rotating electric machine - Google Patents
Permanent magnet rotating electric machine Download PDFInfo
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- JP5178487B2 JP5178487B2 JP2008320138A JP2008320138A JP5178487B2 JP 5178487 B2 JP5178487 B2 JP 5178487B2 JP 2008320138 A JP2008320138 A JP 2008320138A JP 2008320138 A JP2008320138 A JP 2008320138A JP 5178487 B2 JP5178487 B2 JP 5178487B2
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Description
本発明は、回転子内部に導電板を内蔵した永久磁石式回転電機に関する。 The present invention relates to a permanent magnet type rotating electrical machine having a conductive plate built into a rotor.
回転子内に永久磁石を内蔵した永久磁石式回転電機では、永久磁石の鎖交磁束が常に一定の強さで発生しているので、永久磁石による誘導電圧は回転速度に比例して高くなる。そのため、低速から高速まで可変速運転する場合、高速回転では永久磁石による誘導電圧(逆起電圧)が極めて高くなる。永久磁石による誘導電圧がインバータの電子部品に印加されてその耐電圧以上になると、電子部品が絶縁破壊する。そのため、永久磁石の磁束量が耐電圧以下になるように削減された設計を行うことが考えられるが、その場合には永久磁石式回転電機の低速域での出力及び効率が低下する。 In a permanent magnet type rotating electrical machine in which a permanent magnet is built in a rotor, the interlinkage magnetic flux of the permanent magnet is always generated with a constant strength, so that the induced voltage by the permanent magnet increases in proportion to the rotational speed. Therefore, when variable speed operation is performed from low speed to high speed, the induced voltage (back electromotive voltage) by the permanent magnet becomes extremely high at high speed rotation. When the induced voltage by the permanent magnet is applied to the electronic component of the inverter and exceeds its withstand voltage, the electronic component breaks down. For this reason, it is conceivable to perform a design in which the amount of magnetic flux of the permanent magnet is reduced so as to be equal to or less than the withstand voltage.
そこで、回転子内に、固定子巻線のd軸電流で作る磁界により不可逆的に磁束密度が変化する程度の低保磁力の永久磁石(以下、可変磁力磁石という)と、可変磁力磁石の2倍以上の保磁力を有する高保磁力の永久磁石(以下、固定磁力磁石という)を配置し、電源電圧の最大電圧以上となる高速回転域では、可変磁力磁石と固定磁力磁石による全鎖交磁束が減じるように、全鎖交磁束量を調整する技術が提案されている。(特許文献1、特許文献2参照)
Therefore, a permanent magnet having a low coercive force (hereinafter referred to as a variable magnetic force magnet) in which the magnetic flux density is irreversibly changed by a magnetic field generated by the d-axis current of the stator winding, and a variable magnetic force magnet are included in the rotor. In a high-speed rotation range where a high coercivity permanent magnet (hereinafter referred to as a fixed magnet) having a coercive force more than double is placed and the maximum voltage of the power supply voltage is exceeded, the total flux linkage by the variable magnet and the fixed magnet is Techniques have been proposed for adjusting the total flux linkage so as to reduce. (See
なお、永久磁石の磁束量は、保磁力と磁化方向厚の積によって決定されるため、実際に回転子鉄心内に可変磁力磁石と固定磁力磁石とを組み込む場合には、可変磁力磁石としては保磁力と磁化方向厚の積が小の永久磁石を、固定磁力磁石としては保磁力と磁化方向厚の積が大の永久磁石を使用する。また、一般に、可変磁力磁石としては、アルニコ磁石やサマリウムコバルト磁石(サマコバ磁石)、フェライト磁石を使用し、固定磁力磁石としてはネオジム磁石(NdFeB磁石)を使用する。 Since the amount of magnetic flux of the permanent magnet is determined by the product of the coercive force and the magnetization direction thickness, when the variable magnetic magnet and the fixed magnetic magnet are actually incorporated in the rotor core, the permanent magnet is maintained as the variable magnetic magnet. A permanent magnet having a small product of magnetic force and magnetization direction thickness is used, and a permanent magnet having a large product of coercive force and magnetization direction thickness is used as the fixed magnet. In general, an alnico magnet, a samarium cobalt magnet (Samacoba magnet) or a ferrite magnet is used as the variable magnetic magnet, and a neodymium magnet (NdFeB magnet) is used as the fixed magnetic magnet.
ところで、この種の永久磁石式回転電機において、高速回転域でいったん減磁した可変磁力磁石を増磁する場合に、可変磁力磁石に近接配置した固定磁力磁石の磁界が、d軸電流が作る増磁用の磁界の妨げとなり、その分増磁のためのd軸電流(磁化電流)が増大する現象がある。 By the way, in this type of permanent magnet type rotating electrical machine, when the variable magnetic magnet once demagnetized in the high speed rotation range is increased, the magnetic field of the fixed magnetic magnet arranged close to the variable magnetic magnet is increased by the d-axis current. There is a phenomenon in which the magnetic field for magnetism is hindered and the d-axis current (magnetization current) for magnetizing is increased accordingly.
本発明は前記のような従来技術の問題点を解決するために提案されたものであって、その目的は、固定磁力磁石の近傍に導電板を配置し、この導電板を貫通するd軸電流による磁界によって導電板に誘導電流を発生させ、その誘導電流により前記固定磁力磁石に発生する磁界を打ち消すことにより、増磁時のd軸電流の増加を押さえた永久磁石式回転電機を提供することにある。 The present invention has been proposed in order to solve the problems of the prior art as described above, and its object is to arrange a conductive plate in the vicinity of a fixed magnetic magnet and to provide a d-axis current passing through the conductive plate. The present invention provides a permanent magnet type rotating electrical machine that suppresses an increase in d-axis current at the time of magnetizing by generating an induced current in a conductive plate by a magnetic field generated by and canceling out the magnetic field generated in the fixed magnetic magnet by the induced current. It is in.
本発明は、前記回転子鉄心とは別に、導電性を有するよう形成された導電板を不可逆的に変化させる永久磁石を除いた他の永久磁石の磁路部分、あるいは、他の永久磁石の磁化方向を中心軸として前記他の永久磁石の周囲に隣接するように設け、前記電機子巻線に磁化電流を通電させて、その磁束で前記導電板に短絡電流を発生させ、この短絡電流によって磁化電流による磁界と反対方向の磁力を有する磁界を発生させることを特徴とする。特に、本発明において、固定磁力磁石の上下、周囲、全表面、あるいは磁束が漏れる磁路部分であるブロック部導電板を設けることもできる。 In the present invention, apart from the rotor core, the magnetic path portion of other permanent magnets excluding the permanent magnet that irreversibly changes the conductive plate formed to have conductivity , or the magnetization of other permanent magnets It is provided so as to be adjacent to the periphery of the other permanent magnet with the direction as a central axis, and a magnetizing current is passed through the armature winding, and a short-circuit current is generated in the conductive plate by the magnetic flux. A magnetic field having a magnetic force in a direction opposite to a magnetic field generated by an electric current is generated. In particular, in the present invention, a block conductive plate which is a magnetic path portion where the magnetic flux leaks may be provided on the upper and lower sides, the periphery, the entire surface of the fixed magnetic force magnet.
以上のような構成を有する本発明によれば、導電板に誘導電流を発生させ、その誘導電流により前記固定磁力磁石に発生する磁界を打ち消すことにより、増磁時のd軸電流の増加を押さえることができるので、回転子の磁極の減磁時および増磁時の磁化電流の増加を抑止できるので、回転機の効率化を達成することができる。 According to the present invention having the above-described configuration, an increase in d-axis current at the time of magnetization is suppressed by generating an induced current in the conductive plate and canceling out the magnetic field generated in the fixed magnetic force magnet by the induced current. As a result, an increase in the magnetization current at the time of demagnetization and increase of the magnetic pole of the rotor can be suppressed, so that the efficiency of the rotating machine can be achieved.
以下、本発明に係る永久磁石式型回転電機の各実施形態について、図1〜18を参照して説明する。本実施形態の回転電機は12極の場合で説明しており、他の極数でも同様に適用できる。 Hereinafter, each embodiment of the permanent magnet type rotary electric machine according to the present invention will be described with reference to FIGS. The rotating electrical machine of the present embodiment has been described in the case of 12 poles, and can be similarly applied to other pole numbers.
(1.第1の実施形態)
(1−1.構成)
本発明の第1の実施形態について、図1〜図3を用いて説明する。図1は本実施形態の永久磁石式回転電機の回転軸と直交する方向の断面図で、減磁時の磁束の方向を示す図、図2は同じく増磁時の磁束の方向を示す図、図3は増磁時の磁束の方向を示す固定磁力磁石4と導電板8部分の斜視図である。
(1. First embodiment)
(1-1. Configuration)
A first embodiment of the present invention will be described with reference to FIGS. FIG. 1 is a cross-sectional view in a direction orthogonal to the rotation axis of the permanent magnet type rotating electrical machine of the present embodiment, showing the direction of magnetic flux at the time of demagnetization, FIG. 2 is a view showing the direction of magnetic flux at the time of demagnetization, FIG. 3 is a perspective view of the portion of the fixed magnetic magnet 4 and the conductive plate 8 showing the direction of the magnetic flux at the time of magnetization.
本発明の第1の実施形態の回転子1は、図1に示すように回転子鉄心2、保磁力と磁化方向厚みの積が小となる永久磁石3(以下、可変磁力磁石という)、保磁力と磁化方向厚の積が大となる永久磁石(以下、固定磁力磁石という)4,4から構成する。回転子鉄心2は珪素鋼板を積層して構成し、前記の可変磁力磁石3及び固定磁力磁石4,4は回転子鉄心2内に埋め込む。回転子鉄心2内を通過する磁束が可変磁力磁石3と固定磁力磁石4の厚さ方向に通過するように、可変磁力磁石3と固定磁力磁石4の端部に磁気障壁となる空洞5を設ける。
As shown in FIG. 1, the
本実施形態では、可変磁力磁石3はフェライト磁石またはアルニコ磁石とし、この実施形態ではフェライト磁石を使用した。固定磁力磁石4は、NdFeB磁石を使用した。この可変磁力磁石の保磁力は280kA/mとし、固定磁力磁石の保磁力は1000kA/mとする。可変磁力磁石3は磁極中央のd軸に沿って回転子鉄心2内に配置し、その磁化方向はほぼ周方向である。固定磁力磁石4は磁化方向がd軸方向に対して所定の角度を持つように、前記可変磁力磁石3の両側の回転子鉄心2内に配置する。 In this embodiment, the variable magnetic force magnet 3 is a ferrite magnet or an alnico magnet. In this embodiment, a ferrite magnet is used. The fixed magnetic magnet 4 was an NdFeB magnet. The coercive force of this variable magnetic magnet is 280 kA / m, and the coercive force of the fixed magnetic magnet is 1000 kA / m. The variable magnetic force magnet 3 is disposed in the rotor core 2 along the d-axis at the center of the magnetic pole, and the magnetization direction is substantially the circumferential direction. The fixed magnetic magnet 4 is disposed in the rotor core 2 on both sides of the variable magnetic magnet 3 so that the magnetization direction has a predetermined angle with respect to the d-axis direction.
前記回転子鉄心2内に埋め込まれた固定磁力磁石4の上側及び下側の全面を覆うように薄い板状の導電板8を配置する。この導電板8は、固定磁力磁石4と共に電機子巻線にd軸電流を通電させた場合に発生する磁束が貫通するもので、その際、平板状の導電板8の表面には渦巻き状に巡回する短絡電流が発生する。すなわち、導電板8は、可変磁力磁石3の磁化が変化する程度の短絡電流が1秒以内に流れ、その後1秒以内にその短絡電流を50%以上減衰させるものであることが好ましい。また、導電板8のインダクタンス値と抵抗値を、可変磁力磁石3の磁化が変化する程度の短絡電流が流れるような値とすると、効率が良い。 A thin plate-like conductive plate 8 is disposed so as to cover the entire upper and lower surfaces of the fixed magnetic magnet 4 embedded in the rotor core 2. This conductive plate 8 penetrates the magnetic flux generated when a d-axis current is passed through the armature winding together with the fixed magnetic magnet 4. At this time, the surface of the flat conductive plate 8 is spirally formed. A circulating short circuit current is generated. That is, it is preferable that the conductive plate 8 has a short-circuit current that can change the magnetization of the variable magnetic force magnet 3 within one second, and then attenuates the short-circuit current by 50% or more within one second. Further, when the inductance value and the resistance value of the conductive plate 8 are set to such values that a short-circuit current that changes the magnetization of the variable magnetic force magnet 3 flows, the efficiency is good.
前記回転子2の外周には、エアギャップ9を介して固定子10を設ける。この固定子10は、電機子鉄心11と電機子巻線12とを有する。この電機子巻線12に流れる磁化電流により、導電板8には誘導電流が誘起され、その誘導電流によって導電板8を貫通する磁束が形成される。
A stator 10 is provided on the outer periphery of the rotor 2 through an
また、この電機子巻線12に流れる磁化電流により、可変磁力磁石3の磁化方向が可逆的に変化する。すなわち、可変磁力磁石と固定磁力磁石に対しては、永久磁石式回転電機の運転時において、d軸電流による磁界で永久磁石3を磁化させて可変磁力磁石3の磁束量を不可逆的に変化させる。その場合、可変磁力磁石3を磁化するd軸電流を流すと同時にq軸電流により回転電機のトルクを制御する。 Further, the magnetization direction of the variable magnetic force magnet 3 reversibly changes due to the magnetization current flowing through the armature winding 12. That is, for the variable magnetic magnet and the fixed magnetic magnet, the permanent magnet 3 is magnetized by a magnetic field generated by the d-axis current during operation of the permanent magnet type rotating electric machine, and the amount of magnetic flux of the variable magnetic magnet 3 is irreversibly changed. . In this case, the d-axis current for magnetizing the variable magnetic force magnet 3 is supplied, and at the same time the torque of the rotating electrical machine is controlled by the q-axis current.
また、d軸電流で生じる磁束により、電流(q軸電流とd軸電流とを合成した全電流)と可変磁力磁石と固定磁力磁石とで生じる電機子巻線の鎖交磁束量(回転電機の全電流によって電機子巻線に生じる磁束と、回転子側の可変磁力磁石と固定磁力磁石とによって生じる磁束とから構成される電機子巻線全体の鎖交磁束量)をほぼ可逆的に変化させる。 In addition, the magnetic flux generated by the d-axis current causes the amount of interlinkage magnetic flux of the armature windings (of the rotating electric machine) The amount of interlinkage magnetic flux in the entire armature winding composed of the magnetic flux generated in the armature winding by the total current and the magnetic flux generated by the variable magnetic magnet and the fixed magnetic magnet on the rotor side is reversibly changed. .
特に、本実施形態では、瞬時の大きなd軸電流による磁界で可変磁力磁石3を不可逆変化させる。この状態で不可逆減磁がほとんど生じないか、僅かの不可逆減磁が生じる範囲のd軸電流を連続的に流して運転する。このときのd軸電流は電流位相を進めて端子電圧を調整するように作用する。すなわち、大きなd軸電流で可変用磁石3の極性を反転させ、電流位相を進める運転制御方法を行う。このようにd軸電流で可変用磁石3の極性を反転させているので、端子電圧を低下させるような負のd軸電流を流しても、可変用磁石3にとっては減磁界ではなく増磁界となる。すなわち、負のd軸電流で可変用磁石3は減磁することなく、端子電圧の大きさを調整することができる。 In particular, in the present embodiment, the variable magnetic force magnet 3 is irreversibly changed by a magnetic field generated by an instantaneous large d-axis current. In this state, operation is carried out by continuously supplying a d-axis current in a range where little or no irreversible demagnetization occurs. The d-axis current at this time acts to adjust the terminal voltage by advancing the current phase. That is, an operation control method is performed in which the polarity of the variable magnet 3 is reversed with a large d-axis current to advance the current phase. As described above, since the polarity of the variable magnet 3 is reversed by the d-axis current, even if a negative d-axis current that reduces the terminal voltage is supplied, the variable magnet 3 is not demagnetized but increased. Become. That is, the magnitude of the terminal voltage can be adjusted without demagnetizing the variable magnet 3 with a negative d-axis current.
(1−2.基本的な作用)
次に、前記のような構成を有する本実施形態の永久磁石式回転電機における増磁時と減磁時の作用について説明する。なお、各図中に、電機子巻線12や導電板8によって発生した磁力の方向を矢印により示す。
(1-2. Basic action)
Next, the operation at the time of magnetizing and demagnetizing in the permanent magnet type rotating electric machine of the present embodiment having the above-described configuration will be described. In each figure, the direction of the magnetic force generated by the armature winding 12 and the conductive plate 8 is indicated by an arrow.
本実施形態では、固定子10の電機子巻線12に通電時間が0.1ms〜100ms程度の極短時間となるパルス的な電流を流して磁界を形成し、可変磁力磁石3に磁界Aを作用させる(図1参照)。永久磁石を磁化するための磁界Aを形成するパルス電流は、固定子10の電機子巻線12のd軸電流成分とする。この時、可変磁力磁石3以外に作用する磁界A1も前記パルス電流によって作られる。 In the present embodiment, a magnetic field is formed by applying a pulsed current having an energization time of about 0.1 ms to 100 ms to the armature winding 12 of the stator 10, and the magnetic field A is applied to the variable magnetic force magnet 3. Act (see FIG. 1). The pulse current that forms the magnetic field A for magnetizing the permanent magnet is the d-axis current component of the armature winding 12 of the stator 10. At this time, the magnetic field A1 acting other than the variable magnetic force magnet 3 is also generated by the pulse current.
2種類の永久磁石の厚みはほぼ同等するとd軸電流による作用磁界による永久磁石の磁化状態変化は保磁力の大きさにより変る。永久磁石の磁化方向とは逆方向の磁界を発生する負のd軸電流を電機子巻線12にパルス的に通電する。負のd軸電流によって変化した磁石内の磁界Aが−280kA/mになったとすると、可変磁力磁石3の保磁力が280kA/mなので可変磁力磁石3の磁力は不可逆的に大幅に低下する。 If the thicknesses of the two types of permanent magnets are substantially equal, the change in the magnetization state of the permanent magnet due to the applied magnetic field due to the d-axis current varies depending on the magnitude of the coercive force. A negative d-axis current that generates a magnetic field in the direction opposite to the magnetization direction of the permanent magnet is pulsed through the armature winding 12. If the magnetic field A in the magnet changed by the negative d-axis current becomes −280 kA / m, the coercive force of the variable magnetic magnet 3 is 280 kA / m, so that the magnetic force of the variable magnetic magnet 3 significantly decreases irreversibly.
一方、固定磁力磁石4の保磁力が1000kA/mなので磁力は不可逆的に低下しない。その結果、パルス的なd軸電流が0になると可変磁力磁石3のみが減磁した状態となり、全体の磁石による鎖交磁束量を減少することができる。さらに−280kA/mよりも大きな逆磁界をかけると可変磁力磁石3は逆方向に磁化して極性は反転する。この場合、可変磁力磁石3の磁束と固定磁力磁石4の磁束は打ち消しあうので永久磁石の全鎖交磁束は最小になる。 On the other hand, since the coercive force of the fixed magnetic magnet 4 is 1000 kA / m, the magnetic force does not decrease irreversibly. As a result, when the pulsed d-axis current becomes zero, only the variable magnetic force magnet 3 is demagnetized, and the amount of interlinkage magnetic flux by the entire magnet can be reduced. Further, when a reverse magnetic field greater than -280 kA / m is applied, the variable magnetic force magnet 3 is magnetized in the reverse direction and the polarity is reversed. In this case, since the magnetic flux of the variable magnetic magnet 3 and the magnetic flux of the fixed magnetic magnet 4 cancel each other, the total interlinkage magnetic flux of the permanent magnet is minimized.
この場合、固定磁力磁石4によって生じる磁界の磁力の方向は、図1のBに示すように、固定磁力磁石4から可変磁力磁石3の方向となるので、前記電機子巻線12による磁界の磁力の方向と一致するため、可変磁力磁石3の減磁させる方向に強い磁力が作用する。同時に、導電板8には、電機子巻線12の磁界Aを打ち消すような誘導電流が発生し、その誘導電流によって図1矢印Cで示すような磁力の方向を有する磁界が発生する。この導電板8による磁力Cも、可変磁力磁石3の磁化方向を逆方向に向けるように作用する。これらより、可変磁力磁石3の減磁及び極性の反転が効率的に行われる。すなわち、導電板8に誘起された誘導電流により発生した磁界Cの磁力の方向は、可変磁力磁石3を貫通する部分においては、磁化電流による磁界Aの方向と一致するので、減磁方向の磁化も効果的に行われる In this case, the direction of the magnetic force of the magnetic field generated by the fixed magnetic force magnet 4 is from the fixed magnetic force magnet 4 to the variable magnetic force magnet 3 as shown in FIG. Therefore, a strong magnetic force acts in the demagnetizing direction of the variable magnetic force magnet 3. At the same time, an induced current that cancels the magnetic field A of the armature winding 12 is generated on the conductive plate 8, and a magnetic field having a magnetic force direction as indicated by an arrow C in FIG. 1 is generated by the induced current. The magnetic force C generated by the conductive plate 8 also acts to direct the magnetization direction of the variable magnetic force magnet 3 in the reverse direction. Thus, demagnetization and polarity inversion of the variable magnetic force magnet 3 are efficiently performed. That is, the direction of the magnetic force of the magnetic field C generated by the induced current induced in the conductive plate 8 coincides with the direction of the magnetic field A by the magnetizing current in the portion that penetrates the variable magnetic force magnet 3, so that the magnetization in the demagnetizing direction Is also done effectively
つぎに、永久磁石の全鎖交磁束を増加させて最大に復元させる過程(増磁過程)を説明する。減磁完了の状態では、図2に示すように、可変磁力磁石3の極性は反転しており、反転した磁化とは逆方向(図1に示す初期の磁化方向)の磁界を発生する正のd軸電流を電機子巻線12に通電する。反転した逆極性の可変磁力磁石3の磁力は前記磁界が増すに連れて減少し、0になる。さらに正のd軸電流による磁界を増加させると極性は反転して初期の極性の方向に磁化される。ほぼ完全な着磁に必要な磁界である350kA/mをかけると、可変磁力磁石3は着磁されてほぼ最大に磁力を発生する。 Next, a process of increasing the total interlinkage magnetic flux of the permanent magnet and restoring it to the maximum (magnetization process) will be described. In the demagnetization completed state, as shown in FIG. 2, the polarity of the variable magnetic force magnet 3 is reversed, and a positive magnetic field that generates a magnetic field in a direction opposite to the reversed magnetization (the initial magnetization direction shown in FIG. 1) is generated. A d-axis current is passed through the armature winding 12. The magnetic force of the reversed reversed polarity variable magnetic magnet 3 decreases as the magnetic field increases and becomes zero. When the magnetic field due to the positive d-axis current is further increased, the polarity is reversed and magnetized in the direction of the initial polarity. When 350 kA / m, which is a magnetic field necessary for almost complete magnetization, is applied, the variable magnetic force magnet 3 is magnetized and generates a magnetic force almost at its maximum.
この場合、減磁時と同様に、d軸電流は連続通電で増加させる必要はなく、目標の磁力にする電流を瞬間的なパルス電流を流せばよい。一方、固定磁力磁石4の保磁力が1000kA/mなので、d軸電流による磁界が作用しても固定磁力磁石4の磁力は不可逆的に変化しない。その結果、パルス的な正のd軸電流が0になると可変磁力磁石3のみが増磁した状態となり、全体の磁石による鎖交磁束量を増加することができる。これにより元の最大の鎖交磁束量に戻すことが可能となる。 In this case, as in the case of demagnetization, it is not necessary to increase the d-axis current by continuous energization, and an instantaneous pulse current may be used as the current to achieve the target magnetic force. On the other hand, since the coercive force of the fixed magnetic magnet 4 is 1000 kA / m, the magnetic force of the fixed magnetic magnet 4 does not change irreversibly even when a magnetic field due to the d-axis current acts. As a result, when the pulsed positive d-axis current becomes 0, only the variable magnetic force magnet 3 is magnetized, and the amount of flux linkage by the entire magnet can be increased. This makes it possible to return to the original maximum flux linkage.
以上のようにd軸電流による瞬時的な磁界を可変磁力磁石3と固定磁力磁石4に作用させることにより、可変磁力磁石3の磁力を不可逆的に変化させて、永久磁石の全鎖交磁束量を任意に変化させることが可能となる。 As described above, by applying an instantaneous magnetic field due to the d-axis current to the variable magnetic magnet 3 and the fixed magnetic magnet 4, the magnetic force of the variable magnetic magnet 3 is irreversibly changed, and the total interlinkage magnetic flux of the permanent magnet Can be arbitrarily changed.
この場合、永久磁石式回転電機の最大トルク時には磁極の永久磁石の磁束が加え合わせになるように可変磁力磁石3を磁化させ、トルクの小さな軽負荷時や、中速回転域と高速回転域では、前記可変磁力磁石3は、電流による磁界で磁化させて磁束を減少させる。また、磁極の磁石を不可逆変化させて鎖交磁束を最小にした状態で回転子が最高回転速度になったときに、永久磁石による誘導起電圧が、回転電機の電源であるインバータ電子部品の耐電圧以下とする。 In this case, the variable magnetic force magnet 3 is magnetized so that the magnetic flux of the permanent magnet of the magnetic pole is added at the time of the maximum torque of the permanent magnet type rotating electric machine. The variable magnetic force magnet 3 is magnetized by a magnetic field generated by an electric current to reduce the magnetic flux. In addition, when the rotor reaches the maximum rotational speed with the magnetic flux magnet minimized by irreversibly changing the magnetic pole magnet, the induced electromotive force generated by the permanent magnet is resistant to the inverter electronic components that are the power source of the rotating electrical machine. Below voltage.
(1−3.導電板8の作用)
つぎに、導電板8の作用について述べる。可変磁力磁石3と固定磁力磁石4は回転子鉄心2内に埋め込まれて磁気回路を構成しているので、前記d軸電流による磁界は可変磁力磁石3のみでなく、固定磁力磁石4にも作用する。本来、前記d軸電流による磁界は可変磁力磁石3の磁化を変化させるために行う。そこで、前記d軸電流による磁界が固定磁力磁石4に作用しないようにし、可変磁力磁石3に集中するようにすればよい。
(1-3. Action of conductive plate 8)
Next, the operation of the conductive plate 8 will be described. Since the variable magnetic magnet 3 and the fixed magnetic magnet 4 are embedded in the rotor core 2 to form a magnetic circuit, the magnetic field due to the d-axis current acts not only on the variable magnetic magnet 3 but also on the fixed magnetic magnet 4. To do. Originally, the magnetic field generated by the d-axis current is used to change the magnetization of the variable magnetic force magnet 3. Therefore, the magnetic field due to the d-axis current may be prevented from acting on the fixed magnetic magnet 4 and concentrated on the variable magnetic magnet 3.
本実施形態では、固定磁力磁石4の上下両面に導電板8を固定磁力磁石4の磁化方向を中心軸として配置する。そのため、図2に示す可変磁力磁石3の増磁方向の磁化を行う場合、前記d軸電流による磁界A1が固定磁力磁石4に作用すると、前記磁界A1を打ち消すような誘導電流が導電板8に流れる。そのため、固定磁力磁石4中には、前記d軸電流による磁界A1と短絡電流による磁界Cが作用し両者が打ち消し合うために、磁界の増減はほとんど生じない。したがって、少ないd軸電流で可変磁力磁石3を磁化できることになる。すなわち、少ない磁化電流により、可変磁力磁石3を効果的に増磁することができる。 In the present embodiment, the conductive plates 8 are arranged on the upper and lower surfaces of the fixed magnetic magnet 4 with the magnetization direction of the fixed magnetic magnet 4 as the central axis. Therefore, when the magnetization of the variable magnetic force magnet 3 shown in FIG. Flowing. Therefore, in the fixed magnetic force magnet 4, the magnetic field A1 due to the d-axis current and the magnetic field C due to the short-circuit current act and cancel each other, so that the magnetic field hardly increases or decreases. Therefore, the variable magnetic force magnet 3 can be magnetized with a small d-axis current. That is, the variable magnetic force magnet 3 can be effectively magnetized with a small magnetization current.
このとき、固定磁力磁石4は導電板8により前記d軸電流の影響を受けなく、磁束の増加はほとんど生じないので、d軸電流による電機子鉄心11の磁気飽和も緩和できる。すなわち、電機子鉄心11は、d軸電流によって発生する磁界A+磁界A1が電機子巻線12間に形成された磁路を通過することにより、その部分の磁気飽和が生じる可能性がある。しかし、本実施形態では、導電板8の磁界Cは磁界A1を打ち消し、磁界A1≒0とできるので、電機子鉄心11の磁路を通過する磁束の内、磁界A1による成分が減少するので、電機子鉄心11の磁路が磁気飽和することが緩和される。 At this time, the fixed magnetic magnet 4 is not affected by the d-axis current due to the conductive plate 8, and the magnetic flux hardly increases, so that the magnetic saturation of the armature core 11 due to the d-axis current can be reduced. That is, in the armature core 11, when the magnetic field A + the magnetic field A1 generated by the d-axis current passes through the magnetic path formed between the armature windings 12, there is a possibility that magnetic saturation of the portion occurs. However, in the present embodiment, the magnetic field C of the conductive plate 8 cancels the magnetic field A1, and the magnetic field A1≈0. Therefore, the component due to the magnetic field A1 in the magnetic flux passing through the magnetic path of the armature core 11 decreases. Magnetic saturation of the magnetic path of the armature core 11 is alleviated.
(2.第2の実施形態)
本発明の第2の実施形態について、図4〜図6を用いて説明する。図4は本実施形態の永久磁石式回転電機の回転軸と直交する方向の断面図で、減磁時の磁束の方向を示す図、図5は同じく増磁時の磁束の方向を示す図、図6は増磁時の磁束の方向を示す固定磁力磁石4と導電板8部分の斜視図である。
(2. Second Embodiment)
A second embodiment of the present invention will be described with reference to FIGS. FIG. 4 is a cross-sectional view in a direction orthogonal to the rotation axis of the permanent magnet type rotating electrical machine of the present embodiment, showing the direction of the magnetic flux at the time of demagnetization, and FIG. FIG. 6 is a perspective view of the portion of the fixed magnetic magnet 4 and the conductive plate 8 showing the direction of the magnetic flux at the time of magnetization.
この第2の実施形態において、導電板8は、固定磁力磁石4の上下両面に加えて、固定磁力磁石4の内部にも上下の導電板8と平行に配置されている。すなわち、d軸電流(磁化電流)によって生じる磁束の方向と直交するように各導電板8を設ける。 In the second embodiment, the conductive plate 8 is arranged in parallel to the upper and lower conductive plates 8 in the fixed magnetic magnet 4 in addition to the upper and lower surfaces of the fixed magnetic magnet 4. That is, each conductive plate 8 is provided so as to be orthogonal to the direction of the magnetic flux generated by the d-axis current (magnetization current).
このような構成を有する第2の実施の形態においては、前記第1の実施の形態の作用効果に加えて、次のような特徴を有する。すなわち、図4に示す、可変磁力磁石3の減磁方向の磁化を行う場合、固定磁力磁石4の側面からから上側に流れる磁界A’による短絡電流も固定磁力磁石4の内部に配置された導電板8に流れることになる。これとは逆の増磁を行う場合も、図5に示すように、固定磁力磁石4の上側から側面に流れる磁界A’による短絡電流も内部の導電板8に流れる。その結果、固定磁力磁石4に側方から進入する磁界A’の磁力を短絡電流に変化させることで減衰することができ、この磁界A’が固定磁力磁石4の磁力を増加させて、可変磁力磁石3の増磁の妨げになることを抑制できる。 The second embodiment having such a configuration has the following characteristics in addition to the operational effects of the first embodiment. That is, when the variable magnetic force magnet 3 is magnetized in the demagnetizing direction shown in FIG. 4, the short-circuit current due to the magnetic field A ′ flowing upward from the side surface of the fixed magnetic force magnet 4 is also conducted in the fixed magnetic force magnet 4. It will flow to the plate 8. Even when the magnetization is reversed, as shown in FIG. 5, a short circuit current due to the magnetic field A ′ flowing from the upper side to the side surface of the fixed magnetic magnet 4 also flows in the internal conductive plate 8. As a result, the magnetic force of the magnetic field A ′ entering the fixed magnetic magnet 4 from the side can be attenuated by changing it to a short-circuit current, and this magnetic field A ′ increases the magnetic force of the fixed magnetic magnet 4 so that the variable magnetic force. It can suppress that the magnet 3 is prevented from being magnetized.
更に、前記第1実施形態やこの第2実施形態では、導電板8を板状の部材とすることができるので、永久磁石式回転電機の製造時における導電板8の組み込み作業の簡略化が可能となる。特に、固定磁力磁石4と導電板8とを積層して一体化しておけば、通常の永久磁石を鉄心に組み込む場合と同様な作業で導電板8の組み込みを行うことができる。 Furthermore, in the first embodiment and the second embodiment, since the conductive plate 8 can be a plate-like member, it is possible to simplify the work of assembling the conductive plate 8 when manufacturing a permanent magnet type rotating electrical machine. It becomes. In particular, if the fixed magnetic magnet 4 and the conductive plate 8 are laminated and integrated, the conductive plate 8 can be assembled by the same operation as that for incorporating a normal permanent magnet into the iron core.
(3.第3の実施形態)
本発明の第3の実施形態について、図7〜図9を用いて説明する。図7は本実施形態の永久磁石式回転電機の回転軸と直交する方向の断面図で、減磁時の磁束の方向を示す図、図8は同じく増磁時の磁束の方向を示す図、図9は増磁時の磁束の方向を示す固定磁力磁石4と導電板8部分の斜視図である。
(3. Third embodiment)
A third embodiment of the present invention will be described with reference to FIGS. FIG. 7 is a cross-sectional view in a direction orthogonal to the rotation axis of the permanent magnet type rotating electrical machine of the present embodiment, showing the direction of the magnetic flux at the time of demagnetization, and FIG. FIG. 9 is a perspective view of the portion of the fixed magnetic magnet 4 and the conductive plate 8 showing the direction of the magnetic flux at the time of magnetization.
第3の実施形態では、導電板8は固定磁力磁石4の側面に密着した板状の部材であり、固定磁力磁石4をその磁路と平行に覆うように配置する。つまり、導電板8を、前記回転子鉄心2内に埋め込まれた固定磁力磁石4に対して、d軸電流の磁化方向と平行に設ける。 In the third embodiment, the conductive plate 8 is a plate-like member that is in close contact with the side surface of the fixed magnetic force magnet 4 and is disposed so as to cover the fixed magnetic force magnet 4 in parallel with its magnetic path. That is, the conductive plate 8 is provided in parallel with the magnetization direction of the d-axis current with respect to the fixed magnetic force magnet 4 embedded in the rotor core 2.
このように固定磁力磁石4の周囲に導電板8を巻き付けるように配置した第3実施形態では、d軸電流による磁界A1が固定磁力磁石4に作用すると、図7に示すように、磁界A1を打ち消すような誘導電流が導電板8に流れる。このとき、短絡電流による磁界Cは、固定磁力磁石4中に均一に作用する。これは、これとは逆の増磁を行う場合である図8でも同様である。そのため、第3の実施形態の効果としては、前記実施形態の効果に加えて、固定磁力磁石4の全域にわたり磁化電流によって発生する磁界の磁力を打ち消すことができるので、回転子の磁極の増磁時の磁化電流の増加を効率よく抑止できで、回転機の効率化を達成することができる。また、固定磁力磁石4の側面に導電板8が配置されていることから、側面から固定磁力磁石4内に磁化電流による磁界が進入することを防止できる利点もある。 In the third embodiment in which the conductive plate 8 is wound around the fixed magnetic magnet 4 as described above, when the magnetic field A1 caused by the d-axis current acts on the fixed magnetic magnet 4, the magnetic field A1 is changed as shown in FIG. An induced current that cancels out flows through the conductive plate 8. At this time, the magnetic field C due to the short-circuit current acts uniformly in the fixed magnetic magnet 4. The same applies to FIG. 8, which is a case where the magnetization is reversed. Therefore, as an effect of the third embodiment, in addition to the effect of the above-described embodiment, the magnetic force of the magnetic field generated by the magnetizing current can be canceled over the entire area of the fixed magnetic magnet 4, so that the magnetic pole of the rotor can be increased. The increase in the magnetizing current at the time can be efficiently suppressed, and the efficiency of the rotating machine can be achieved. In addition, since the conductive plate 8 is disposed on the side surface of the fixed magnetic force magnet 4, there is an advantage that it is possible to prevent a magnetic field due to a magnetizing current from entering the fixed magnetic force magnet 4 from the side surface.
(4.第4の実施形態)
本発明の第4の実施形態について、図10〜図12を用いて説明する。図10は本実施形態の永久磁石式回転電機の回転軸と直交する方向の断面図で、減磁時の磁束の方向を示す図、図11は同じく増磁時の磁束の方向を示す図、図12は増磁時の磁束の方向を示す固定磁力磁石4と導電板8部分の斜視図である。
(4. Fourth embodiment)
A fourth embodiment of the present invention will be described with reference to FIGS. FIG. 10 is a cross-sectional view in a direction orthogonal to the rotation axis of the permanent magnet type rotating electrical machine of the present embodiment, showing the direction of the magnetic flux at the time of demagnetization, and FIG. FIG. 12 is a perspective view of the portion of the fixed magnetic magnet 4 and the conductive plate 8 showing the direction of the magnetic flux at the time of magnetization.
第4の実施形態は、導電板8を固定磁力磁石4の上下及び側面、すなわち、固定磁力磁石4の全周囲に配置したもので、前記第1と第3の実施形態を組み合わせたものである。この場合、導電板8は板状の部材を溶接やろう付けで固定磁力磁石4の表面に接合しても良いし、メッキその他の手法で可変磁力磁石4の表面全体を導電性の材料で覆うことにより形成しても良い。 In the fourth embodiment, the conductive plate 8 is arranged on the upper and lower sides and the side surface of the fixed magnetic force magnet 4, that is, the entire periphery of the fixed magnetic force magnet 4, and the first and third embodiments are combined. . In this case, the conductive plate 8 may be a plate-shaped member joined to the surface of the fixed magnetic magnet 4 by welding or brazing, or the entire surface of the variable magnetic magnet 4 is covered with a conductive material by plating or other techniques. You may form by.
この第4実施形態においては、前記各実施形態の効果に加えて、固定磁力磁石4にいずれの方向から加わる磁化電流による磁界Aについても、そのエネルギーを誘導電流として消費する。 In the fourth embodiment, in addition to the effects of the respective embodiments, the energy of the magnetic field A generated by the magnetizing current applied to the fixed magnetic magnet 4 from any direction is consumed as an induced current.
(5.第5の実施形態)
本発明の第5の実施形態について、図13〜図15を用いて説明する。図13は本実施形態の永久磁石式回転電機の回転軸と直交する方向の断面図で、減磁時の磁束の方向を示す図、図14は同じく増磁時の磁束の方向を示す図、図15は増磁時の磁束の方向を示す固定磁力磁石4と導電板8部分の斜視図である。
(5. Fifth embodiment)
A fifth embodiment of the present invention will be described with reference to FIGS. FIG. 13 is a cross-sectional view in a direction orthogonal to the rotation axis of the permanent magnet type rotating electrical machine of the present embodiment, showing the direction of the magnetic flux at the time of demagnetization, and FIG. 14 is also a view showing the direction of the magnetic flux at the time of demagnetization, FIG. 15 is a perspective view of the portions of the fixed magnetic magnet 4 and the conductive plate 8 showing the direction of the magnetic flux at the time of magnetization.
この第5の実施形態において、導電板8は、その中央開口部をd軸電流による磁束が貫通するような無端状の部材であり、電機子巻線にd軸電流を通電させた場合に発生する磁束で、無端状の導電板8を巡回する短絡電流が発生する。この導電板8は、可変磁力磁石3を除いた固定磁力磁石4の磁路部分に設けるもので、固定磁力磁石4の磁化方向を中心軸として、固定磁力磁石4周囲に配置する。 In this fifth embodiment, the conductive plate 8 is an endless member through which the magnetic flux due to the d-axis current passes through the central opening, and is generated when the d-axis current is passed through the armature winding. A short-circuit current that circulates the endless conductive plate 8 is generated by the magnetic flux that is generated. The conductive plate 8 is provided in a magnetic path portion of the fixed magnetic magnet 4 excluding the variable magnetic magnet 3 and is arranged around the fixed magnetic magnet 4 with the magnetization direction of the fixed magnetic magnet 4 as a central axis.
このような構成を有する本実施形態では、図13に示す、可変磁力磁石3の減磁方向の磁化を行う場合、固定磁力磁石4の側面からから上側に流れる磁界A’による短絡電流も固定磁力磁石4の内部に配置された導電板8に流れることになる。これとは逆の増磁を行う場合も、図6に示すように、固定磁力磁石4の上側から側面に流れる磁界A’による短絡電流も導電板8に流れる。そのため、前記各実施形態の効果に加えて、導電板8によって固定磁力磁石4を被覆する部分が少なくて済み、鉄心内に磁気障壁となる導電性部材を配置する箇所が少なくて済み、永久磁石の磁気特性を損なうおそれがない。 In this embodiment having such a configuration, when performing magnetization in the demagnetization direction of the variable magnetic force magnet 3 shown in FIG. 13, the short-circuit current due to the magnetic field A ′ flowing upward from the side surface of the fixed magnetic force magnet 4 is also fixed magnetic force. It flows to the conductive plate 8 disposed inside the magnet 4. Even when the magnetization is reversed, as shown in FIG. 6, a short-circuit current due to the magnetic field A ′ flowing from the upper side to the side surface of the fixed magnetic magnet 4 also flows through the conductive plate 8. Therefore, in addition to the effects of the above-described embodiments, the portion that covers the fixed magnetic magnet 4 with the conductive plate 8 is small, and the number of places where the conductive member serving as a magnetic barrier is disposed in the iron core is small. There is no risk of damaging the magnetic properties of the.
(6.第6の実施形態)
本発明の第6の実施形態について、図16〜図18を用いて説明する。図16は本実施形態の永久磁石式回転電機の回転軸と直交する方向の断面図で、減磁時の磁束の方向を示す図、図17は同じく増磁時の磁束の方向を示す図、図18は増磁時の磁束の方向を示す鉄心のブリッジ部の斜視図である。
(6. Sixth embodiment)
A sixth embodiment of the present invention will be described with reference to FIGS. FIG. 16 is a cross-sectional view in a direction orthogonal to the rotation axis of the permanent magnet type rotating electrical machine of the present embodiment, showing the direction of the magnetic flux at the time of demagnetization, and FIG. FIG. 18 is a perspective view of the bridge portion of the iron core showing the direction of the magnetic flux when magnetizing.
第6の実施形態では、導電板8は固定磁力磁石4と可変磁力磁石3の間に設けられたブリッジ部6の周囲を覆う板状の部材であり、導電板8を前記回転子鉄心2内に埋め込まれた固定磁力磁石4を固定磁石のd軸の電流による磁路の境に設ける。 In the sixth embodiment, the conductive plate 8 is a plate-like member that covers the periphery of the bridge portion 6 provided between the fixed magnetic magnet 4 and the variable magnetic magnet 3, and the conductive plate 8 is disposed inside the rotor core 2. The fixed magnetic magnet 4 embedded in is attached to the boundary of the magnetic path by the d-axis current of the fixed magnet.
このような構成を有する第6実施形態では、図16及び図17に示すように、可変磁力磁石3の減磁あるいは増磁方向の磁化を行う場合、前記d軸電流による磁界A2がブリッジ部6に作用すると、磁界A2を打ち消すような誘導電流が導電板8に流れる。その結果、この誘導電流によって生じた磁界Cがd軸電流による磁界A2を打ち消すように作用するので、ブリッジ部6の部分に磁気障壁を作成することが可能になる。特に、ブリッジ部6には、鉄心の強度上の要請から空洞などを設けて磁気障壁を形成することが難しいが、本実施形態によれば、ブリッジ部6の機械的強度を確保したまま、磁気障壁を形成することができるので、前記実施形態と同様に、少ない磁化電流で効果的に増磁を行うことのできる効果もある。 In the sixth embodiment having such a configuration, as shown in FIGS. 16 and 17, when the variable magnetic force magnet 3 is demagnetized or magnetized in the direction of magnetization, the magnetic field A <b> 2 due to the d-axis current is changed to the bridge portion 6. , An induced current that cancels the magnetic field A2 flows through the conductive plate 8. As a result, the magnetic field C generated by the induced current acts so as to cancel the magnetic field A2 caused by the d-axis current, so that a magnetic barrier can be created at the bridge portion 6. In particular, it is difficult to form a magnetic barrier by providing a cavity or the like in the bridge portion 6 due to demands on the strength of the iron core. However, according to the present embodiment, the magnetic strength of the bridge portion 6 is ensured while ensuring the mechanical strength. Since the barrier can be formed, as in the above-described embodiment, there is an effect that the magnetization can be effectively performed with a small magnetization current.
(7.他の実施形態)
本発明は、前記の各実施形態に限定されるものではなく、つぎのような他の実施形態も包含する。
(7. Other embodiments)
The present invention is not limited to the above-described embodiments, and includes other embodiments as follows.
(1)前記各実施形態では4極の回転電機を示したが、8極等の多極の回転電機にも本発明を適用できるのは当然である。極数に応じて永久磁石の配置位置、形状が幾分変ることはもちろんであり、作用と効果は同様に得られる。特に、前記各実施形態は、中央に可変磁力磁石を、その両側に固定磁力磁石を配置したものであるが、可変磁力磁石と固定磁力磁石との他の配置にも適用できる。 (1) In each of the above embodiments, a four-pole rotating electric machine is shown, but the present invention is naturally applicable to a multi-pole rotating electric machine such as an eight-pole machine. Depending on the number of poles, the position and shape of the permanent magnets will of course change somewhat, and the action and effect can be obtained in the same way. In particular, each of the above embodiments has a variable magnetic magnet arranged in the center and fixed magnetic magnets arranged on both sides thereof, but can be applied to other arrangements of variable magnetic magnets and fixed magnetic magnets.
(2)前記回転子鉄心2において、固定磁力磁石の外周側に磁気障壁を構成するために設ける空洞の形状や位置、また、固定磁力磁石の内周側にその磁路断面積を決定するために設ける空洞の位置などは、使用する永久磁石の保磁力や磁化電流によって生じる磁界の強さなどに応じて、適宜変更できる。 (2) In the rotor core 2, in order to determine the shape and position of the cavity provided for forming the magnetic barrier on the outer peripheral side of the fixed magnetic magnet, and the magnetic path cross-sectional area on the inner peripheral side of the fixed magnetic magnet The position of the cavity provided in can be appropriately changed according to the coercive force of the permanent magnet used, the strength of the magnetic field generated by the magnetizing current, and the like.
(3)前記各実施形態を適宜組み合わせることも可能である。特に、ブリッジ部6と固定磁力磁石4の両方に導電板8を設けることで、より効果的に可変磁力磁石の減磁あるいは増磁を行うことができる。 (3) The above embodiments can be combined as appropriate. In particular, by providing the conductive plate 8 in both the bridge portion 6 and the fixed magnetic force magnet 4, the variable magnetic force magnet can be demagnetized or increased more effectively.
1…回転子
2…回転子鉄心
3…保磁力と磁化方向厚さの積が小さい永久磁石(可変磁力磁石)
4…保磁力と磁化方向厚さの積が大きい永久磁石(固定磁力磁石)
5…永久磁石端の空洞
6…ブリッジ部
8…導電板
9…エアギャップ
10…固定子
11…電機子鉄心
12…電機子巻線
DESCRIPTION OF
4. Permanent magnet with a large product of coercive force and magnetization direction thickness (fixed magnet)
5 ... Cavity 6 at the end of the permanent magnet 6 ... Bridge portion 8 ...
Claims (8)
前記回転子鉄心とは別に、導電性を有するよう形成された導電板を前記不可逆的に変化させる永久磁石を除いた他の永久磁石の磁路部分に、前記他の永久磁石と隣接するように設け、
前記電機子巻線に磁化電流を通電させて、その磁束で前記導電板に短絡電流を発生させ、
この短絡電流によって磁化電流による磁界と反対方向の磁力を有する磁界を発生させることを特徴とする永久磁石式回転電機。 A magnetic pole is formed by using two or more types of permanent magnets whose product of coercive force and magnetization direction thickness is different from other permanent magnets, and a plurality of the magnetic poles are arranged in the rotor core to constitute a rotor. A stator is arranged on the outer periphery of the child via an air gap, an armature core and an armature winding are provided on the stator, and a magnetic pole generated by the current of the armature winding constitutes the magnetic pole of the rotor. In a permanent magnet type rotating electrical machine that magnetizes at least one of the magnets and irreversibly changes the amount of magnetic flux of the permanent magnet,
Aside from the rotor core, a conductive plate formed to have conductivity is adjacent to the other permanent magnet in a magnetic path portion of another permanent magnet excluding the permanent magnet that irreversibly changes the conductive plate. Provided,
By passing a magnetizing current through the armature winding, a short-circuit current is generated in the conductive plate by the magnetic flux,
A permanent magnet type rotating electrical machine that generates a magnetic field having a magnetic force in a direction opposite to a magnetic field generated by a magnetizing current by the short-circuit current.
前記回転子鉄心とは別に、導電性を有するよう形成された導電板を前記不可逆的に変化させる永久磁石を除いた他の永久磁石の磁化方向を中心軸として前記他の永久磁石の周囲に、前記他の永久磁石と隣接するように設け、
前記電機子巻線に磁化電流を通電させて、その磁束で前記導電板に短絡電流を発生させ、
この短絡電流によって磁化電流による磁界と反対方向の磁力を有する磁界を発生させることを特徴とする永久磁石式回転電機。 A magnetic pole is formed by using two or more types of permanent magnets whose product of coercive force and magnetization direction thickness is different from other permanent magnets, and a plurality of the magnetic poles are arranged in the rotor core to constitute a rotor. A stator is arranged on the outer periphery of the child via an air gap, an armature core and an armature winding are provided on the stator, and a magnetic pole generated by the current of the armature winding constitutes the magnetic pole of the rotor. In a permanent magnet type rotating electrical machine that magnetizes at least one of the magnets and irreversibly changes the amount of magnetic flux of the permanent magnet,
Separately from the rotor core , around the other permanent magnet with the magnetization direction of another permanent magnet as a central axis except for the permanent magnet that irreversibly changes a conductive plate formed to have conductivity , Provided adjacent to the other permanent magnet ,
By passing a magnetizing current through the armature winding, a short-circuit current is generated in the conductive plate by the magnetic flux,
A permanent magnet type rotating electrical machine that generates a magnetic field having a magnetic force in a direction opposite to a magnetic field generated by a magnetizing current by the short-circuit current.
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| JP2008320138A JP5178487B2 (en) | 2008-12-16 | 2008-12-16 | Permanent magnet rotating electric machine |
| CN200980150361.1A CN102246399B (en) | 2008-12-15 | 2009-12-15 | Permanent magnet type rotary electrical machine |
| US13/139,889 US8796898B2 (en) | 2008-12-15 | 2009-12-15 | Permanent magnet electric motor |
| EP09833196.0A EP2372885B1 (en) | 2008-12-15 | 2009-12-15 | Permanent magnet type rotary electrical machine |
| PCT/JP2009/006899 WO2010070888A1 (en) | 2008-12-15 | 2009-12-15 | Permanent magnet type rotary electrical machine |
| US14/296,116 US9373992B2 (en) | 2008-12-15 | 2014-06-04 | Permanent magnet electric motor |
| US14/296,238 US9496774B2 (en) | 2008-12-15 | 2014-06-04 | Permanent magnet electric motor |
| US14/296,177 US9490684B2 (en) | 2008-12-15 | 2014-06-04 | Permanent magnet electric motor |
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