JPH0315262A - Magnetic rotary machine - Google Patents
Magnetic rotary machineInfo
- Publication number
- JPH0315262A JPH0315262A JP14756889A JP14756889A JPH0315262A JP H0315262 A JPH0315262 A JP H0315262A JP 14756889 A JP14756889 A JP 14756889A JP 14756889 A JP14756889 A JP 14756889A JP H0315262 A JPH0315262 A JP H0315262A
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnet
- rotor
- magnetic
- attached
- view
- 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
- 230000004907 flux Effects 0.000 claims description 19
- 239000000696 magnetic material Substances 0.000 claims description 8
- 239000000463 material Substances 0.000 claims description 8
- 239000000446 fuel Substances 0.000 abstract description 4
- 238000010586 diagram Methods 0.000 description 11
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 4
- 239000000853 adhesive Substances 0.000 description 4
- 230000001070 adhesive effect Effects 0.000 description 4
- 238000002485 combustion reaction Methods 0.000 description 4
- 230000004048 modification Effects 0.000 description 4
- 238000012986 modification Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 239000004575 stone Substances 0.000 description 3
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 2
- 241000723346 Cinnamomum camphora Species 0.000 description 2
- 241000190020 Zelkova serrata Species 0.000 description 2
- 229910052799 carbon Inorganic materials 0.000 description 2
- 239000004020 conductor Substances 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 235000003932 Betula Nutrition 0.000 description 1
- 241000219429 Betula Species 0.000 description 1
- 235000018185 Betula X alpestris Nutrition 0.000 description 1
- 235000018212 Betula X uliginosa Nutrition 0.000 description 1
- 238000006027 Birch reduction reaction Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 239000012530 fluid Substances 0.000 description 1
- 238000006722 reduction reaction Methods 0.000 description 1
Landscapes
- Reciprocating, Oscillating Or Vibrating Motors (AREA)
Abstract
Description
【発明の詳細な説明】
（イ）産業上の利用分野
本発明は、産業機械用、ＩＩＩ機用、自動車用、船舶用
の内燃機関、電動機、空気など各種流体を動力源とする
モータなどで代表される、回転動力機に関するものであ
る．
（ロ）従来の技術
従来の動力機関は、炭素系の燃料を爆発させる内燃機関
、電気をエネルギーとする電気モータなどいわば燃料消
耗型動力機である．燃料補給の必要があるばかりか、内
燃機関等は燃焼時の排気ガスや騒音を伴い、環境問題の
元凶となっている．（ハ）発明が解決しようとする問題
点
本発明は、従来の動力機関の前記のような問題点を取り
除くものであり、燃料の必要がなく、また排気ガスや騒
音も出ない磁力回転機を提供することを目的とする．
（二）問題点を解失するための手段
本発明の磁力回転機は、高透磁性材料からなるロータ、
または高透磁性材料からなるステータに、同極を対向す
るように取り付けられた、界磁を発生させる環状の主永
久磁石と、非磁性材料からなるロータまたは、非磁性材
料からなるステータに界磁と直角方向にｔ流を流した時
に発生する磁束と同欅の磁束を発生するように取り付け
られた、副永久磁石とを具備したことを要旨とする．（
ホ）作用
第１図のように、永久磁石の磁界中にある導体に紙面の
表から裏側へｔ流を流すと、フレミングの左手の法則よ
り、導体には左側へ運動力が発生する．また、ｔ流によ
って発生する磁界と、磁石によって発生する磁界は全く
同じものであることが、等価板磁石の理論式から証明さ
れている．このことより、永久磁石の磁界中に別の永久
磁石を挿入して、電直によって発生したのと同様の磁力
線を造れば、この磁界内において可動可能な状態の永久
磁石には、運動力が発生する．第２図は、磁石を空気中
に１いた場合の磁力線分布を表したものであり、第３図
は、この様子を電流に置き換えて示した図である．
第４図は、１個の主永久磁石２の界磁が副永久磁石１の
磁束の上側部分（主永久磁石側）とだけ作用丁る位置に
設置した場合の図である。ここで、■１ ：副永久磁石
の主永久磁石側の等ｆＩＩｔ ｆＬＩ．：副永久磁石の
主永久磁石と反対側の等価電流
Ｂ．：［．と作用する主永久磁石の磁束密度Ｂｚ：ｒオ
と作用する主永久磁石の磁束密度Ｌ ：磁石の長さ（こ
こでは単位長とし、Ｌ−１と仮定する．）
Ｆ＋ ： Ｉｔ ｘＢ，ｘＬで発生する電磁力Ｆ．：
ＩよＸＢ，ＸＬで発生する！磁力Ｆ ：Ｆ．−Ｆエで
表される、外部へ取り出される運動力．と定義すると第
４図の場合には、Ｂエ−０のため Ｆ．−０、よってＦ
，のｔ磁力だけで左側へ動作する．しかし、主永久磁石
からの距離が離れているため距離の２乗に反比例する磁
束密度Ｂ．が極めて小さく、従って＃ Ｆ ，も極めて
小さな力しか発生しない．
また逆に、副永久磁と主永久磁石を近ずけた場合？は、
第５図（イ）に示した襟に主永久磁石２の反発力により
、副永久磁石ｌの磁束分布がアンハランスになってしま
い、その結果１，＜Ｉ■となる．この場合、Ｆ−０とな
る条件はＦ．−Ｆ．であり、それ以外の時は、Ｆ＝Ｆ．
−Ｆ．の力が働く事になるが、この力も極めて小さな物
である．以上の問題点を解決するためには、第６図に示
した樟に、２個の界磁を発生させる主永久磁石２と３を
同極を対向するように設置し、この磁界中に可動可能な
副永久磁石１を設置すれば良い．この場合には、主永久
は石と副永久磁石の距離を離しても、または近すけでも
、第６図（イ）に示すように副永久磁石ｌの磁束分布は
、バランスを保てるためＩ．−１８となる．第６図（ロ
）は、この状態を電流に置き換えて示した図である．こ
こで、フレミングの左手の法則より、Ｆ１とＦ！は同一
方向でありＦ−Ｆ．＋Ｆ．の力が働くこととなり、主永
久磁石と副永久磁石の距離を近ずけると、強力な力が左
方向へ発生する．本発明は、この運動力を回転装置に応
用するものである．（へ）実施例
本発明の好適な実施例について、以下図面に従って説明
する．第７図は、主永久磁石を高透磁性材料からなるス
テータに取り付け、副永久磁石を非磁性材料からなるロ
ータに取り付けた、第１実施例の正面断面図である．
回転機の前面を覆うハウジングｌ１と、回転機の後面を
覆うハウジング１０とは、ボルト１２で結合されている
．シャフト４を支持するベヤリング８は、シャフト４に
圧入されたのち後面を覆うハウジング１０の中心にある
ベヤリングボックスに挿入され、他方のベヤリング７は
、前面を覆うハウジング１１の中心にあるベヤリングボ
ックスに挿入され、ベヤリングカバ−９とボルト１３で
、前面ハウジング１１に固定されている．シャフト４に
はロータ５が圧入されており、このロータ５の端面には
、第８図に平面図を示した様に着磁された副永久磁石１
が、接着剤等で結合され、ロータ５と一体となって回転
する．ステータ６は、前面ハウジング１１のインロ一部
でスライドできる構造になっており、後面ハウジング１
０に取付けられたスプリング１５によって前面ハウジン
グｌ１の方向へ押しつけられていてアジャストボルト１
６で出入りを！ＩＩ！ｆｆ出来る欅になっている．キー
１４により回転防止が図られている．またステータ６に
は、界磁を発生させる環状になった主永久磁石２と３が
、第８図に平面図を示した様に着磁され、同極を対向す
るように接着剤等で結合されている．
次に、本実施例の磁力回転機の作動について説明する．
第８図に平面図を示した欅に、ステータ６に取付けられ
た、環状になった主永久磁石２と３の間に、ロータ５に
取付けられた副永久磁石１を挿入すると、第６図の原理
図で説明した通り、フレミングの左手の法則により、ロ
ータ５は反時計方向へ回転する．
尚、ロータ５には、常に同じ方向の磁界が作用するため
、ヒステリシスによる鉄損は少ないが、ステータ６には
、交番磁界が作用するため、ヒステリシスによる鉄損を
軽減する必要がある，しかしこれは従来技術で解決出来
る．
第９図は、第７図の実施例の回転停止時の正面断面図を
示す．アジャストボルト１６を回して、主永久磁石２と
３の磁界より、副永久磁石１を離してやると運動力がな
くなるため停止する．尚、本実施例では主永久磁石２と
３及び副永久磁石１で構威したものを示したが、第１０
図に正面断面図を示した欅に、主永久磁石２′と２人及
び３と３Ａを軸方向に異極となる樺に設置すると、磁気
回路の溝戒がより効果的になる．この場合の主永久磁石
２と３及び２Ａと３Ａは同極を対向するように設置しな
ければならない．
第１１図は、第１０図のＡ−Ａ断面のローク５及び副永
久磁石１の配Ｉを示す平面図であり、又、第ｌ２図は、
第１０図のＢ−Ｂ断面のロータ５及び副永久磁石ＩＡの
配置を示す平面図である．この場合、ロータ５は時計方
向へ回転する．又、第１３図に正面断面図を示したよう
に、ロータ５に取付けられた、副永久磁石１を取り囲む
様に、ステータ６に環状をした主永久磁石２、３、３Ａ
，１７．１７Ａを同極を対向するように、取付けてもよ
い。副永久磁石１の配置は、第８図に示したものと同様
の配置にする．この場合、副永久磁石ｌの磁束の大部分
が有効にｆｌｌ用出来るため、発生トルクが大きく取れ
るという利点がある．更に、第１５図に正面断面図を、
第１４図に第ｌ５図のＡ−Ａ矢視図を示した陛に、主永
久磁石２と３及び副永久磁石ｌが、それぞれ、シャフト
４に対し直角方向に配置されても良い．この場合、回転
するロータ５に取付けられた副永久磁石１が遠心力で飛
ばされるのを、簡単に防止出来ると言う利点がある．こ
の場合、ロータ５は反時計方向へ回転する．
次に、副永久磁石を非磁性材料からなるステータに取り
付け、主永久磁石を高透磁性材料からなるロータに取り
付けた、第２実施例について説明する．第１７図は、第
２実施例の正面断面図を示す．副永久磁石１は、第１８
図に平面図を示した様に着磁され、ステータ６に接着剤
等で結合されている．シャフト４には、ロータ５が圧人
されており、このロータ５に１よ、第１８図に平面図モ
示した様に普磁された、界磁を発生させる環状の主永久
礎石２と３が同極を対向丁るように、それぞれ接着剤等
で結合され、ロータ５と一体となって回転する．本実施
例｛よ、第７図の実施例の王永久磁石と、副永久磁石の
取付け位置を同一にして、回転軸を変えただけであり、
作動についてｉよ第７図の実施例と同様、フレミングの
左手の法則により動作する．副永久磁石ｌを固定してい
るため、ロタ５は反作用により、時計方向へ回転する。Detailed Description of the Invention (a) Industrial Application Field The present invention is applicable to internal combustion engines, electric motors, motors powered by various fluids such as air, etc. for industrial machines, III machines, automobiles, and ships. This is related to rotary power machines, which are a typical example. (B) Conventional technology Conventional power engines are so-called fuel-consuming power machines, such as internal combustion engines that explode carbon-based fuel and electric motors that use electricity as energy. Not only do they require refueling, but internal combustion engines also produce exhaust gas and noise during combustion, making them a source of environmental problems. (c) Problems to be solved by the invention The present invention eliminates the above-mentioned problems of conventional power engines, and provides a magnetic rotating machine that does not require fuel and does not emit exhaust gas or noise. The purpose is to provide (2) Means for solving the problems The magnetic rotating machine of the present invention has a rotor made of a highly permeable material,
Alternatively, a stator made of a highly permeable material has an annular main permanent magnet that generates a field attached with the same poles facing each other, and a rotor made of a non-magnetic material, or a stator made of a non-magnetic material that generates a field. The main feature is that the magnet is equipped with an auxiliary permanent magnet that is attached so as to generate a magnetic flux that is the same as the magnetic flux that is generated when a t current is passed in a direction perpendicular to the magnetic flux. (
E) Effect As shown in Figure 1, when a t-current flows through a conductor in the magnetic field of a permanent magnet from the front to the back of the page, a kinetic force is generated in the conductor to the left according to Fleming's left-hand rule. Furthermore, it has been proven from the theoretical formula for an equivalent plate magnet that the magnetic field generated by the t-flow and the magnetic field generated by the magnet are exactly the same. From this, if we insert another permanent magnet into the magnetic field of a permanent magnet and create lines of magnetic force similar to those generated by a direct line, the permanent magnet that is movable within this magnetic field will have a kinetic force. Occur. Figure 2 shows the magnetic field line distribution when a magnet is placed in the air, and Figure 3 shows this situation in terms of electric current. FIG. 4 is a diagram showing the case where the magnetic field of one main permanent magnet 2 is installed at a position where it acts only on the upper part of the magnetic flux of the sub permanent magnet 1 (on the main permanent magnet side). Here, ■1: Equal fIIt fLI. of the sub permanent magnet on the main permanent magnet side. : Equivalent current of the sub permanent magnet on the opposite side of the main permanent magnet B. :[． Magnetic flux density of the main permanent magnet acting with r: Magnetic flux density of the main permanent magnet acting with r: Length of magnet (Here, it is assumed to be unit length and L-1.) F+: It xB, xL The electromagnetic force generated F. :
I, it occurs in XB, XL! Magnetic force F: F. −The kinetic force taken out to the outside, represented by F. In the case of FIG. 4, F. −0, so F
, moves to the left only by the t magnetic force of . However, since the distance from the main permanent magnet is large, the magnetic flux density B is inversely proportional to the square of the distance. is extremely small, so #F also generates only an extremely small force. Conversely, what if the secondary permanent magnet and the main permanent magnet are brought closer together? teeth,
Due to the repulsive force of the main permanent magnet 2 on the collar shown in FIG. 5(a), the magnetic flux distribution of the auxiliary permanent magnet l becomes unharmed, resulting in 1,<I■. In this case, the condition for F-0 is F. -F. At other times, F=F.
-F. A force will be exerted, but this force is also extremely small. In order to solve the above problems, two main permanent magnets 2 and 3 that generate a magnetic field are installed in the camphor tree shown in Fig. 6 so that the same poles face each other, and a movable magnet is placed in the camphor tree shown in Fig. 6. All you have to do is install a secondary permanent magnet 1 if possible. In this case, even if the distance between the main permanent magnet and the auxiliary permanent magnet is large or close, the magnetic flux distribution of the auxiliary permanent magnet l can be kept balanced as shown in FIG. -18. Figure 6 (b) is a diagram showing this state in terms of current. Here, from Fleming's left hand rule, F1 and F! are in the same direction and F-F. +F. When the distance between the main permanent magnet and the sub permanent magnet is brought closer, a strong force is generated to the left. The present invention applies this kinetic force to a rotating device. (F) Embodiments Preferred embodiments of the present invention will be described below with reference to the drawings. FIG. 7 is a front sectional view of the first embodiment, in which the main permanent magnet is attached to a stator made of a highly permeable material, and the auxiliary permanent magnet is attached to a rotor made of a non-magnetic material. A housing l1 that covers the front surface of the rotating machine and a housing 10 that covers the rear surface of the rotating machine are coupled with bolts 12. The bearing 8 supporting the shaft 4 is press-fitted into the shaft 4 and then inserted into the bearing box located at the center of the housing 10 covering the rear surface, and the other bearing 7 is inserted into the bearing box located at the center of the housing 11 covering the front surface. and is fixed to the front housing 11 with a bearing cover 9 and bolts 13. A rotor 5 is press-fitted into the shaft 4, and a sub-permanent magnet 1 is magnetized on the end face of the rotor 5 as shown in the plan view in FIG.
are connected with adhesive or the like and rotate together with the rotor 5. The stator 6 has a structure in which it can slide on a part of the spigot of the front housing 11.
The adjustment bolt 1 is pressed toward the front housing l1 by a spring 15 attached to the
Enter and exit at 6! II! It is a keyaki that can be ff. The key 14 is used to prevent rotation. In addition, in the stator 6, annular main permanent magnets 2 and 3 that generate a magnetic field are magnetized as shown in the plan view in Fig. 8, and are connected with adhesive or the like so that the same poles face each other. It has been done. Next, the operation of the magnetic rotating machine of this embodiment will be explained.
When the auxiliary permanent magnet 1 attached to the rotor 5 is inserted between the ring-shaped main permanent magnets 2 and 3 attached to the stator 6 in the keyaki whose plan view is shown in FIG. As explained in the principle diagram, the rotor 5 rotates counterclockwise due to Fleming's left hand rule. Note that since a magnetic field in the same direction always acts on the rotor 5, the iron loss due to hysteresis is small, but since an alternating magnetic field acts on the stator 6, it is necessary to reduce iron loss due to hysteresis. can be solved using conventional technology. FIG. 9 shows a front sectional view of the embodiment shown in FIG. 7 when rotation is stopped. When the adjustment bolt 16 is turned to separate the sub permanent magnet 1 from the magnetic field of the main permanent magnets 2 and 3, the motion force is lost and the motor stops. In addition, in this example, a configuration using main permanent magnets 2 and 3 and sub permanent magnet 1 was shown, but the 10th
If the main permanent magnets 2' and 2 and 3 and 3A are installed in birches with different poles in the axial direction, the groove control of the magnetic circuit will be more effective. In this case, main permanent magnets 2 and 3 and 2A and 3A must be installed so that the same poles face each other. FIG. 11 is a plan view showing the arrangement I of the rake 5 and the sub-permanent magnet 1 in the AA cross section of FIG. 10, and FIG.
10 is a plan view showing the arrangement of the rotor 5 and the auxiliary permanent magnets IA taken along the line BB in FIG. 10. FIG. In this case, the rotor 5 rotates clockwise. Further, as shown in the front sectional view in FIG. 13, annular main permanent magnets 2, 3, 3A are attached to the stator 6 so as to surround the sub permanent magnet 1 attached to the rotor 5.
, 17.17A may be installed with the same polarity facing each other. The arrangement of the sub-permanent magnets 1 is similar to that shown in Fig. 8. In this case, most of the magnetic flux of the auxiliary permanent magnet l can be effectively used for full use, so there is an advantage that a large amount of generated torque can be obtained. Furthermore, Fig. 15 shows a front sectional view,
As shown in FIG. 14, which is a view taken along the line A--A in FIG. In this case, there is an advantage that it is possible to easily prevent the auxiliary permanent magnet 1 attached to the rotating rotor 5 from being blown away by centrifugal force. In this case, the rotor 5 rotates counterclockwise. Next, a second embodiment will be described in which the auxiliary permanent magnets are attached to a stator made of a non-magnetic material, and the main permanent magnet is attached to a rotor made of a highly permeable material. FIG. 17 shows a front sectional view of the second embodiment. The sub permanent magnet 1 is the 18th
It is magnetized as shown in the plan view in the figure, and is bonded to the stator 6 with adhesive or the like. A rotor 5 is mounted on the shaft 4, and as shown in the plan view in FIG. are connected with adhesive or the like so that they have the same polarity facing each other, and rotate together with the rotor 5. In this embodiment, the mounting positions of the main permanent magnet and the auxiliary permanent magnet in the embodiment shown in FIG. 7 are the same, and the rotation axis is changed.
As for operation, like the embodiment shown in FIG. 7, it operates according to Fleming's left hand rule. Since the sub permanent magnet l is fixed, the rotor 5 rotates clockwise due to reaction.
又、第１９図に正面断面図を示したｆｌ造にしても良い
．これは、第１０図の実施例の主永久Ｌｉ石と副永久磁
石の取付け位置を同一にして、回転軸を変えたものであ
る．
以上述べた、第１実施例及び第２実施例では、主永久磁
石２と３は環状の一体もので示したが、第１６図（イ）
及び（口）に平面図を示した様に、３分割でも２分割で
も良い．即ち、主永久磁石は適宜に分割されていても良
い．
（ト）発明の効果
（イ）永久礎石を組み合わせる事により回転力を得るた
め、永久磁石の内部エネルギーが消滅するか、あるいは
、軸受部の寿命が来るまで一回転しつずける。Alternatively, it may be made into a fl structure, a front sectional view of which is shown in FIG. 19. In this example, the main permanent Li stone and the sub permanent magnet are installed in the same position as in the embodiment shown in Fig. 10, but the rotation axis is changed. In the first and second embodiments described above, the main permanent magnets 2 and 3 are shown as integral annular magnets, but as shown in FIG.
As shown in the plan view in and (mouth), it may be divided into three or two parts. That is, the main permanent magnet may be divided as appropriate. (g) Effects of the invention (a) Since rotational force is obtained by combining permanent foundation stones, the permanent magnet will continue to rotate once until the internal energy of the magnet disappears or the life of the bearing section ends.
（口）従来の動力機関の様に、炭素系の燃料を爆発させ
る必要がないため、燃料補給の必要がなく、又、騒音や
排気ガスが出ない．
（ハ）電気モータの樺に１４！線がなく、逆起電力が発
生しないため、原理的に超高速回転が可能であり、減速
比を適切にすれば、大トルクが取り出せる．
（二）構造が簡単であり、小型堅牢で、安価に製作出来
る．
以上述べた様な利点のある、磁力回転機を産業分野で利
用すれば、その効果は図り知れない程大きなものである
．(Example) Unlike conventional power engines, there is no need to explode carbon-based fuel, so there is no need for refueling, and there is no noise or exhaust gas. (c) 14 on the electric motor birch! Since there are no wires and no back electromotive force is generated, ultra-high speed rotation is possible in principle, and large torque can be obtained by adjusting the reduction ratio appropriately. (2) It has a simple structure, is small and robust, and can be manufactured at low cost. If magnetic rotating machines, which have the advantages mentioned above, are used in the industrial field, the effects will be immeasurably great.
第１図は、フレミングの左手の法則の説明図．第２図は
、副永久磁石の磁束分布図の平面図．第３図は、第２図
の磁束分布を電流に置き換えた説明図．
第４図（イ）は、界磁を発生させる１個の主永久礎石と
副永久磁石を離して設置した場合の磁束分布図の平面図
．
第４図（口）は、第４図（イ）の副永久磁石の磁束を電
流に置き換えた説明図．
第５図（イ）は、界磁を発生させる１個の主永久磁石と
、副永久磁石を接近させて設置した場合の磁束分布図の
平面図．
第５図（口）は、第５図（イ）の副永久磁石の磁束を電
流に置き換えた説明図．
第６図（イ）は、本発明の動作原理を説明するための磁
束分布図の平面図．
第６図（ロ）は、第６図（イ）の副永久磁石の磁束を電
流に置き換えた説明図．
第７図は、第１実施例の正面断面図．
第８図は、第７図のＡ−Ａ断面の平面図．第９図は、第
７図の実施例の回転停止時の正面断面図．
第ｌＯ図は、第７図の実施例の変形例の原理図の正面断
面図．
第１１図は、第１０図のＡ−Ａ断面のロータ部の平面図
．
第１２図は、第１０図のＢ−Ｂ断面のロータ部の平面図
．
第１３図は、第７図の実施例の変形例の原理図の正面断
面図．
第ｌ４図は、第１５図のＡ−Ａ矢視図．第１５図は、第
７図の実施例の変形例の原理図の正面断面図．
第１６図（イ）及び（口）は、主永久磁石の変形例の平
面図．
第１７図は、ロータに主永久磁石を取付け、ステータに
副永久磁石を取付けた、第２実施例の原理図の正面断面
図．
第１８図は、第１７図のＡ−Ａ断面の平面図．第１９図
は、第１７図の実施例の変形例の原理図の正面断面図．
ｌ：副永久磁石。 ２，３：主永久磁石．４：シャフ
ト．５：ロータ．６：ステータ．７、８：ベヤリング
９：ベヤリングカバｌＯ：後面ハウジング．１ｌ：前面
ノ＼ウジング。
１２．１３：ボルト． ｌ４：キー
１５：スプリング． １６：アジャストポルト１７
：主永久磁石．
Ｎ：磁石のＮ極，Ｓ：Ｆ６１石のＳ極．ｔ一：回転方向
あるいは、運動方向．
←一：主永久磁石の磁力線．
←一：副永久磁石の磁力線．
■二紙面の表から裏側へ流れるｔＩＲFigure 1 is an illustration of Fleming's left hand rule. Figure 2 is a plan view of the magnetic flux distribution diagram of the auxiliary permanent magnet. Figure 3 is an explanatory diagram in which the magnetic flux distribution in Figure 2 is replaced with current. Figure 4 (a) is a plan view of the magnetic flux distribution diagram when one main permanent cornerstone and a secondary permanent magnet that generate a magnetic field are installed apart from each other. Figure 4 (opening) is an explanatory diagram in which the magnetic flux of the auxiliary permanent magnet in Figure 4 (a) is replaced with a current. Figure 5 (a) is a plan view of the magnetic flux distribution diagram when one main permanent magnet that generates a magnetic field and a sub permanent magnet are installed close to each other. Figure 5 (opening) is an explanatory diagram in which the magnetic flux of the auxiliary permanent magnet in Figure 5 (a) is replaced with a current. FIG. 6(a) is a plan view of a magnetic flux distribution diagram for explaining the operating principle of the present invention. Figure 6 (B) is an explanatory diagram in which the magnetic flux of the sub permanent magnet in Figure 6 (A) is replaced with a current. FIG. 7 is a front sectional view of the first embodiment. FIG. 8 is a plan view of the AA cross section in FIG. 7. FIG. 9 is a front sectional view of the embodiment shown in FIG. 7 when rotation is stopped. Figure 10 is a front sectional view of the principle of a modification of the embodiment shown in Figure 7. FIG. 11 is a plan view of the rotor section taken along the line AA in FIG. 10. FIG. 12 is a plan view of the rotor section taken along the line B-B in FIG. 10. FIG. 13 is a front sectional view of the principle of a modification of the embodiment shown in FIG. Figure 14 is a view taken along the line A-A in Figure 15. FIG. 15 is a front sectional view of the principle of a modification of the embodiment shown in FIG. Figures 16(a) and 16(a) are plan views of modified examples of the main permanent magnet. FIG. 17 is a front sectional view of the principle of the second embodiment, in which the main permanent magnet is attached to the rotor and the auxiliary permanent magnet is attached to the stator. FIG. 18 is a plan view of the AA cross section in FIG. 17. FIG. 19 is a front sectional view of the principle of a modification of the embodiment shown in FIG. 17. l: Sub-permanent magnet. 2, 3: Main permanent magnet. 4: Shaft. 5: Rotor. 6: Stator. 7, 8: Bearing
9: Bearing cover lO: Rear housing. 1l: Front no\Using. 12.13: Bolt. l4: Key 15: Spring. 16: Adjust Porto 17
: Main permanent magnet. N: N pole of magnet, S: S pole of F61 stone. t1: Rotation direction or movement direction. ←1: Lines of magnetic force of the main permanent magnet. ←1: Lines of magnetic force of the sub-permanent magnet. ■tIR flowing from the front to the back of the second page
Claims (3)
料からなるステータに、同極を対向するように取り付け
られた、界磁を発生させる環状の主永久磁石と、非磁性
材料からなるロータまたは、非磁性材料からなるステー
タに、界磁と直角方向に電流を流した時に発生する磁束
と同様の磁束を発生するように取り付けられた、副永久
磁石とを具備したことを特徴とする磁力回転機。(1) A rotor made of a highly permeable material or a stator made of a highly permeable material, with an annular main permanent magnet that generates a field attached so that the same poles face each other, and a rotor made of a non-magnetic material. Alternatively, a magnetic force characterized by comprising a stator made of a non-magnetic material and a sub-permanent magnet attached so as to generate a magnetic flux similar to that generated when a current is passed in a direction perpendicular to the field. Rotating machine.
り付け、副永久磁石を非磁性材料からなるロータに取り
付けた、特許請求の範囲第１項に記載の磁力回転機。(2) The magnetic rotating machine according to claim 1, wherein the main permanent magnet is attached to a stator made of a highly permeable material, and the auxiliary permanent magnet is attached to a rotor made of a non-magnetic material.
付け、主永久磁石を高透磁性材料からなるロータに取り
付けた、特許請求の範囲第１項に記載の磁力回転機。(3) The magnetic rotating machine according to claim 1, wherein the auxiliary permanent magnet is attached to a stator made of a non-magnetic material, and the main permanent magnet is attached to a rotor made of a highly permeable material.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14756889A JPH0315262A (en) | 1989-06-10 | 1989-06-10 | Magnetic rotary machine |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14756889A JPH0315262A (en) | 1989-06-10 | 1989-06-10 | Magnetic rotary machine |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0315262A true JPH0315262A (en) | 1991-01-23 |
Family
ID=15433297
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14756889A Pending JPH0315262A (en) | 1989-06-10 | 1989-06-10 | Magnetic rotary machine |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0315262A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05236733A (en) * | 1991-03-01 | 1993-09-10 | Hiroyuki Hagiyama | Magnetic motor |
| WO2014077322A1 (en) * | 2012-11-15 | 2014-05-22 | Tochihira Hirotoshi | Magnet motor and drive mechanism |
| JP5727079B1 (en) * | 2014-09-09 | 2015-06-03 | 博敏 栃平 | Magnet drive mechanism |
-
1989
- 1989-06-10 JP JP14756889A patent/JPH0315262A/en active Pending
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH05236733A (en) * | 1991-03-01 | 1993-09-10 | Hiroyuki Hagiyama | Magnetic motor |
| WO2014077322A1 (en) * | 2012-11-15 | 2014-05-22 | Tochihira Hirotoshi | Magnet motor and drive mechanism |
| JP2014100027A (en) * | 2012-11-15 | 2014-05-29 | Hirotoshi Tochihira | Magnet motor and drive mechanism |
| JP5727079B1 (en) * | 2014-09-09 | 2015-06-03 | 博敏 栃平 | Magnet drive mechanism |
| WO2016039145A1 (en) * | 2014-09-09 | 2016-03-17 | 博敏 栃平 | Magnet driving mechanism |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP3879412B2 (en) | Power generation system | |
| EP1624555A2 (en) | Axial-gap dynamo-electric machine | |
| US6724115B2 (en) | High electrical and mechanical response structure of motor-generator | |
| JPS61180582U (en) | ||
| JP2000209825A (en) | Permanent magnet generator | |
| JPS6139839A (en) | Torque motor | |
| US5038064A (en) | Limited angle rotary actuator | |
| JPH01298948A (en) | Eddy current type decelerator | |
| JPH0315262A (en) | Magnetic rotary machine | |
| JP3613922B2 (en) | Crankshaft direct-coupled generator | |
| US4020370A (en) | Electric motor for general purposes | |
| JPH07107718A (en) | Permanent magnet generator | |
| JP3518922B2 (en) | Abduction type permanent magnet rotating electric machine and electric vehicle using abduction type permanent magnet rotating electric machine | |
| JPH03143258A (en) | Magnetic force rotating machine | |
| JP2021010211A (en) | Rotary electric machine and rotary electric machine manufacturing method | |
| US4206377A (en) | Single phase stepping motor | |
| JP3630377B2 (en) | Actuator | |
| EP0461490A1 (en) | Torque motor with rotor pole pieces | |
| JPH06141530A (en) | Rotating machine using permanent magnet in stator and rotor | |
| JPS61269664A (en) | Motor utilizing magnet | |
| KR20220017096A (en) | Double permanent magnet motor | |
| JP2002349411A (en) | Hydraulic driven generator | |
| KR910007216A (en) | Coil Rotational Power Generation Method and Generator | |
| JPH0515592B2 (en) | ||
| JPS6318976A (en) | Motor |