JPS62114465A - Magnet motor - Google Patents
Magnet motorInfo
- Publication number
- JPS62114465A JPS62114465A JP25166085A JP25166085A JPS62114465A JP S62114465 A JPS62114465 A JP S62114465A JP 25166085 A JP25166085 A JP 25166085A JP 25166085 A JP25166085 A JP 25166085A JP S62114465 A JPS62114465 A JP S62114465A
- Authority
- JP
- Japan
- Prior art keywords
- rotor
- diamagnetic
- stator
- force
- motor
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Landscapes
- Iron Core Of Rotating Electric Machines (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は、電気エネルギー等の外部エネルギーの消費を
仔なうことなく、回転子軸から所定の回転トルクを引き
出すことか可能な画期的な磁石モーターに関する。[Detailed Description of the Invention] <Industrial Application Field> The present invention is an epoch-making method that makes it possible to extract a predetermined rotational torque from the rotor shaft without consuming external energy such as electrical energy. Regarding magnetic motors.
〈従来例および間通点〉
一般に、従来の反磁性体材料は外部磁界内に置かれると
6ii棒に近い(!―Iか同名の極に、また遠い側か異
名の棒に磁化されるが、磁化の程度は極めて小さいため
、その反発力を殆ど運動エネルギーとして利用すること
のできないものである。<Conventional Examples and Points of Interchange> In general, when conventional diamagnetic materials are placed in an external magnetic field, they are magnetized to the pole close to the 6ii bar (!-I or the same name, and to the far side or the pole of the different name). Since the degree of magnetization is extremely small, the repulsive force can hardly be used as kinetic energy.
従って、従来より磁力を利用するモー
ターにおいては、強磁性体軟質材料たる鉄、コバルト、
ニッケル、等の昨金属または合金を固定手用および又は
回転子用の鉄心として用いてこれを電気的に@i極交番
させ、その強力な磁気吸引力・反発力を利用することか
回転運動に変換するための唯一・の現実的な方法とされ
ている。このようなモーターとして誘導電動機、同期電
動機、直流7に動機等が知られている。Therefore, motors that use magnetic force have conventionally used soft ferromagnetic materials such as iron, cobalt,
It is possible to use metals or alloys such as nickel as the iron core for the stationary hand and/or the rotor, electrically alternating the poles, and use its strong magnetic attraction and repulsion to achieve rotational movement. It is considered the only practical way to convert. As such motors, induction motors, synchronous motors, DC motors, etc. are known.
しかるに、上記の強磁性体材料の鉄心に交番!ffpj
Aを生じさせるためには、モーター出力に比例した電力
の消費を前提とするものである。しかも鉄心材料の保磁
力によるヒシテリシス損すなわち鉄損が避けらす、その
材質改善にも限度があるので、電力を100%存効に回
転運動に変換することもできない。However, the above-mentioned ferromagnetic material core has alternating! ffpj
In order to generate A, it is assumed that power consumption is proportional to the motor output. Moreover, there is a limit to the improvement of the material to avoid hysteresis loss, that is, iron loss due to the coercive force of the iron core material, and therefore it is not possible to convert electric power into rotational motion 100% effectively.
く問題点を解決するための手段〉
本発明は、強磁性体の磁化力を利用する従来のモーター
の欠点を除去するために提案されたものであり、
本発明の目的は、電力の消費を必要としないモーターを
提供することにある。Means for Solving the Problems The present invention was proposed to eliminate the drawbacks of conventional motors that utilize the magnetizing force of ferromagnetic materials, and an object of the present invention is to reduce power consumption. Our goal is to provide motors that are not required.
本発明の他の目的は、当初に外部から回転子を起動回転
させるだけで、その後は外部からのエネルギー供給を必
要とせずに回転出力を保持することのできるモーターを
提供することにある。Another object of the present invention is to provide a motor that can initially start and rotate the rotor from the outside and then maintain its rotational output without requiring any external energy supply.
而して、上記本発明の目的は、「永久磁石を素材とする
固定−rと、高透磁率・極小保磁力のアモルファス合金
製反磁性体を素材とする回転子とからなる磁石モーター
」によって達成される。Therefore, the object of the present invention is to provide a magnetic motor consisting of a stationary member made of a permanent magnet and a rotor made of a diamagnetic material made of an amorphous alloy with high magnetic permeability and minimal coercive force. achieved.
〈実施例〉
次に、本発明を図面に示された実施例に従って更に詳し
く説明することとする。<Example> Next, the present invention will be explained in more detail according to an example shown in the drawings.
TS1図には、本発明に係るモーター(1)の構成模式
図が示されており、(2)は馬蹄形の永久磁石よりなる
固定子、(3)は該磁石モーター(1)の両磁極間に配
設された回転子、(4)は回転子軸である。該回転子(
3)はコバルト(Go)を基材とし・、鉄(Fe)、ニ
ッケル(Ni)、モリブデン(MO)、ホロン(Ilo
ron) 、シリコン(Si)を副材としたアモルファ
ス合金を素材としており、高飽和・高速&fiyである
とともに小保磁力の特性を有する軟質の反磁性材料であ
る。その標準的組成および磁気特性等を表−1に示す。Figure TS1 shows a schematic configuration diagram of the motor (1) according to the present invention, in which (2) is a stator made of a horseshoe-shaped permanent magnet, and (3) is a structure between the two magnetic poles of the magnet motor (1). (4) is the rotor shaft. The rotor (
3) is based on cobalt (Go), iron (Fe), nickel (Ni), molybdenum (MO), and holon (Ilo).
ron), is made of an amorphous alloy with silicon (Si) as a secondary material, and is a soft diamagnetic material that is highly saturated, high speed, and has the characteristics of a small coercive force. Its standard composition, magnetic properties, etc. are shown in Table 1.
(表−1)
一組一一込一
コバルト(CO67) 45重量%鉄(Fe)
26−<(i量%ニッケル(N i
) l 9徂)廿%モリブデン(Mo)4
重量%
ボロン(Boron) 4重量%けい素(S
i) 2重量%−愁」[理」辷件−
同(Oe)の磁場、不活性ガス(N2十八r =99
、9996)の雰囲気で、5分間325℃の加熱をした
のち、lO℃/min以トの速度で冷却。(Table-1) Cobalt (CO67) 45% by weight Iron (Fe)
26-<(i amount% nickel (N i
) l 9 徂) 廿%Molybdenum (Mo)4
Weight% Boron 4% by weight Silicon (S
i) 2% by weight - Magnetic field of Oe, inert gas (N28r = 99
, 9996) for 5 minutes at 325°C, and then cooled at a rate of less than 10°C/min.
一33配砥」い主が50KIIz ; 0.I
T飽和挺東密度 (IIs) 0.7007残留磁
束密度 (Br) 0.[i21 T保磁力
(llc) 0.21 0c最大透Wt率 (μ
max) l x IQ6鵠が・ が性
キュリ一温度 (’rc) 365 ℃結晶化温
度 (Tx) 536 ℃@十(λ) 0
密 度 (ρ) 7.9 g
/cm’鉄 損 5.2
9 W/Kg上記の特性を有する反ifi性材料は
、元来結晶質・強磁性体であるところのコバルト(GO
)、鉄(Fe)、ニッケル(Ni)、モリブデン(MO
)、ボロン(Boron) 、シリコン(Si)をアモ
ルファス化すなわち非晶質化することにより、磁化特性
を反磁性体に変化させたものであり、しかもその高透磁
率・小保磁力を維持するものである。The owner of 133 points is 50KIIz; 0. I
T saturation density (IIs) 0.7007 Residual magnetic flux density (Br) 0. [i21 T coercive force
(llc) 0.21 0c maximum transmittance Wt rate (μ
Max) l
/cm' Iron loss 5.2
9 W/Kg The anti-ifi material with the above characteristics is cobalt (GO), which is originally a crystalline and ferromagnetic material.
), iron (Fe), nickel (Ni), molybdenum (MO
), boron, and silicon (Si) are made amorphous, that is, non-crystalline, to change the magnetization characteristics to a diamagnetic material, while maintaining high magnetic permeability and low coercive force. It is.
いま、初めて回転子(3)が7gZ a図の状態すなわ
ち長袖の両端(P)、(Q)が固定子(2)による磁界
の中央付近に位置するときは、磁気的にニュートラルで
あり、両端(P)、(Q)は磁化されていない。Now, for the first time, when the rotor (3) is in the state shown in Figure 7gZa, that is, when both ends (P) and (Q) of the long sleeve are located near the center of the magnetic field by the stator (2), it is magnetically neutral and both ends are (P) and (Q) are not magnetized.
次いで、固定子(2)を矢印(f)方向に回転起動力を
加えると、端部(P)は固定子(2)の固定磁極Sに接
近するので反磁性体の特性として次第にS極に磁化され
、一方の端部(0)は周定1.fiiNに接近するので
反磁性体の特性として次第にN極に磁化され、第2b図
における固定子(2)の磁軸線(X)上に至って最大の
磁化力を受けるが、外部起動力による慣性回転力でなお
も回転し、両端(P)、(Q)か該!fi軸線IX)を
越えると回転子(3)の&fi極に対して同極で対面し
ている固定子(2)は強い反発力を受けて同図の矢印方
向へ回転付勢される。Next, when a rotation starting force is applied to the stator (2) in the direction of the arrow (f), the end (P) approaches the fixed magnetic pole S of the stator (2), so as a characteristic of diamagnetic material, it gradually becomes the S pole. magnetized, one end (0) is circumferential 1. fiiN, it is gradually magnetized to the north pole as a characteristic of diamagnetic material, and reaches the magnetic axis (X) of the stator (2) in Fig. 2b, where it receives the maximum magnetizing force, but due to inertial rotation due to external motive force. It still rotates due to the force, and both ends (P) and (Q) correspond! When the stator (2), which faces the &fi poles of the rotor (3) with the same polarity, receives a strong repulsive force, it is urged to rotate in the direction of the arrow in the figure.
次いで、固定子(2)が残留磁束を有して第2c図の位
置まで回転すると、S極の端部(P)は回転子(3)の
N極からの吸引力を受け、またN極の端部(Q)は回転
子(3)のS極からの吸引力を受けるので、さらに回転
付勢されて増速する。その後、両端(P)、(Q)がそ
れぞれ回転子(3)の磁極に近fすくと素早く極性が入
れ替わり、第1図のように回転子(3)と同極で対面す
ることとなるが、それまでの回転付勢力による慣性力で
回転子(3)の@軸を越え、館述と同様に反発回転力が
付与される。Next, when the stator (2) rotates with residual magnetic flux to the position shown in Figure 2c, the end (P) of the S pole receives an attractive force from the N pole of the rotor (3), and the N pole end (P) receives an attractive force from the N pole of the rotor (3). Since the end (Q) of the rotor (3) receives an attractive force from the S pole of the rotor (3), it is further urged to rotate and speed up. After that, when both ends (P) and (Q) come close to the magnetic poles of the rotor (3), their polarities quickly switch, and they end up facing the rotor (3) with the same polarity as shown in Figure 1. , the inertia force caused by the rotational biasing force up to that point crosses the @ axis of the rotor (3), and a repulsive rotational force is applied as described above.
上記の回転サイクルにおいて、固定子
(2〕はその素材が高飽和・高速Mi率かっ小保磁力で
あるので、強力な反発力・吸引力を生じて回転子軸(4
)に強力なトルクを得るとともに、固定子(2)からの
僅かな逆磁化力によって迅速な極性変換か可能となって
いる。従って、回転子(3)は若干の脈動回転を呈する
ものの、固定子(2)の磁束密度すなわち磁化力に応じ
た回転数および回転トルクを維持して連続回転するもの
である。In the above rotation cycle, the stator (2) is made of a material with high saturation, high speed Mi, and small coercive force, so strong repulsive and attractive forces are generated and the rotor shaft (4) is
), and a quick polarity change is possible due to the slight demagnetizing force from the stator (2). Therefore, although the rotor (3) exhibits some pulsating rotation, it continuously rotates while maintaining the rotational speed and rotational torque according to the magnetic flux density, that is, the magnetizing force, of the stator (2).
なお、図面の実施例では固定子(2)を24JUとした
ものを示したが、これを複数とすること、および/又は
回転子(3)を2以上の複数突極型回転子とすること、
さらに回転子I噛(4)に弾み東を取り付けて回転を滑
らかにすること等は本発明に含まれる実施例である。In the embodiment of the drawings, the stator (2) is shown as having 24 JU, but the stator (2) may have a plurality of 24 JU, and/or the rotor (3) may have two or more salient pole rotors. ,
Further, it is an embodiment included in the present invention to attach a springboard to the rotor I catch (4) to smoothen the rotation.
く効 果〉
本発明に係る磁石モーターによれば、回転子の素材とし
て、高い飽和磁束密度、高透磁率、小保磁力の特性を持
つ反磁性軟質材料を用いているので、当初に外部から回
転子を起動回転させるだけで、その後は電力等の外部エ
ネルギーの供給を必要とせすに連続回転し、所定の回転
トルクを出力することができるものである。Effect> According to the magnet motor of the present invention, since a diamagnetic soft material having the characteristics of high saturation magnetic flux density, high magnetic permeability, and small coercive force is used as the material of the rotor, it is possible to Simply by starting the rotor and rotating it, the rotor can rotate continuously and output a predetermined rotational torque without requiring the supply of external energy such as electric power.
図面は本発明に係る磁石モーターの一実施例を示すもの
であり、第1図は概略構成図、第2図(a)、(b)、
(C)はその作動を示す説明図、である。
(1) ・・・・・・ 磁石モーター、(2)・・・・
・・ 固疋子、
(3)・・・・・・ 回転子、
(4)・・・・・・ 回転子軸。The drawings show one embodiment of the magnet motor according to the present invention, and FIG. 1 is a schematic configuration diagram, and FIGS. 2(a), (b),
(C) is an explanatory diagram showing the operation. (1) ... Magnet motor, (2) ...
・ ・ Jarbiki, (3) ・ ・ ・ ・ Transled, (4) ・ ・ ・ ・ ・ ・ The rotation axis.
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP25166085A JPS62114465A (en) | 1985-11-08 | 1985-11-08 | Magnet motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP25166085A JPS62114465A (en) | 1985-11-08 | 1985-11-08 | Magnet motor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62114465A true JPS62114465A (en) | 1987-05-26 |
Family
ID=17226121
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP25166085A Pending JPS62114465A (en) | 1985-11-08 | 1985-11-08 | Magnet motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62114465A (en) |
-
1985
- 1985-11-08 JP JP25166085A patent/JPS62114465A/en active Pending
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