JPS62281756A - Application of permanent-magnet rotation method - Google Patents

Application of permanent-magnet rotation method

Info

Publication number
JPS62281756A
JPS62281756A JP12144886A JP12144886A JPS62281756A JP S62281756 A JPS62281756 A JP S62281756A JP 12144886 A JP12144886 A JP 12144886A JP 12144886 A JP12144886 A JP 12144886A JP S62281756 A JPS62281756 A JP S62281756A
Authority
JP
Japan
Prior art keywords
circle
stator
rotor
line
center
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
Application number
JP12144886A
Other languages
Japanese (ja)
Inventor
Satoshi Uchida
聡 内田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Priority to JP12144886A priority Critical patent/JPS62281756A/en
Publication of JPS62281756A publication Critical patent/JPS62281756A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain a continuous turning force by using attraction and repulsion of a stator provided with an irregular cavity and a rotor with its center deviating from a rotating shaft. CONSTITUTION:A rotating shaft is positioned at a place deviating from the center of a stator X to an N pole side. The center of a rotor Z is set at a place deviating further from the former place to an N pole side. The rotor Z is divided into the N and S poles by a line P. A circle Y making intersections of a line M and a circle R and a line L and the circle R its tangent points, respectively, decreases in the diameter of the circle R by the deviation of the rotating shaft from the center of the circle R. The stator X is provided with an irregular cavity to strengthen its attraction and repulsion.

Description

【発明の詳細な説明】 3、発明の詳細な説明 本発明は、永久磁石回転運動法における応用に、関する
ものである0本発明の特長は、磁力をさえぎらずに回転
運動を持続させる点で、絶磁装置がなく、構造も簡単に
なり余分な磁力の抵抗が無くなった事である。
Detailed Description of the Invention 3. Detailed Description of the Invention The present invention relates to application in the permanent magnet rotational motion method.The feature of the present invention is that the rotational motion is sustained without blocking the magnetic force. , there is no magnetism-absorbing device, the structure is simple, and there is no extra magnetic resistance.

以下、図示に基づき本発明を説明する。Hereinafter, the present invention will be explained based on illustrations.

図1は、基本になる装置の横断面図で、まず、固定子(
X)のための円(R)e書き、その中心(L、にの接点
)よりNBi側(し線上)にずらせた所に、回転軸(L
、Mの接点)を位置し、そこからさらにNi側〈L線上
)にずらせた所を回転子(Z)の中心(L、Pの交点)
とし、pHにより回転子(Z)のN、3%を分ける0M
線と円(R)の交点及び、し線と円(R)の交点を接点
とした円(Y)は1円(R)の中心(L、にの接点)か
ら回転軸(L、Mの接点)のずらせた分はど、円(R)
より直径で小さく、これは図2のGで回転子(Z)が固
定子(X)と、接触しないことが基準となる。にノ+線
と円(Y)の接点及び、Pliと円(Y)の交点で固定
子(X)のN、Sliを分けている。P線と円の交点、
N極間は円(R)、S極側は円(Yンとなる。
Figure 1 is a cross-sectional view of the basic device. First, the stator (
Draw a circle (R) e for
, M contact point), and the point further shifted toward the Ni side (on the L line) is the center of the rotor (Z) (the intersection of L and P)
and divide the N of the rotor (Z) by 3% according to the pH into 0M
A circle (Y) whose tangent points are the intersection of the line and the circle (R) and the intersection of the line and the circle (R) is connected from the center of the circle (R) (the point of contact with L) to the axis of rotation (L, M). The shifted part of the contact point) is a circle (R)
This is based on the fact that the rotor (Z) does not come into contact with the stator (X) at G in FIG. 2. N and Sli of the stator (X) are separated at the point of contact between the + line and the circle (Y) and the point of intersection between Pli and the circle (Y). The intersection of the P line and the circle,
The area between the N poles is a circle (R), and the S pole side is a circle (Y).

図2は、図1の装置で順次回転が8分の1づつ(A−H
)進んだところを示しており、固定子(X)と回転子(
Z)の形状や位11!2!系の図である。A〜Hを個々
に見ると、Aは1回転方向が決っておらず、Bで反発力
がみき、Cになると吸引力が歯くようになり、Dで回転
子(Z)と固定子(X)の間が最も[#lく、Eで吸引
力が働き、Fでは、吸引力が更に強くなる。このように
、Aの状態で回転方向が決まらず、G、Hの状態は、逆
回軟状1となる。そこでA〜Hそれぞれの状りの装置を
同じ軸で固定し1回転させ互いに停止状態を回転状層で
助力し、回転を持続させる。
Figure 2 shows that the device in Figure 1 is rotated sequentially in 1/8 increments (A-H).
) shows the advanced state, and the stator (X) and rotor (
Z) shape and place 11!2! This is a diagram of the system. Looking at A to H individually, in A the direction of one rotation is not determined, in B there is a repulsive force, in C the suction force increases, and in D the rotor (Z) and stator ( The area between X) is the strongest, the suction force works at E, and the suction force becomes even stronger at F. In this way, the direction of rotation is not determined in the A state, and the G and H states are reverse rotation soft 1. Therefore, each of the devices A to H is fixed on the same shaft and rotated once, and the rotating layers help each other to stop each other so that the rotation continues.

図3は、より分かりやすくするため、A〜Hを同軸に固
定した状態の装置が、回転する様子と表にしたものであ
る1表は、1〜8で、8分の1づつ回転の経過を表して
おり、例えば1(A〜H)のG、Hで、逆回転状1だが
、残りのB、C,DE、Fで回転を助力し、わずかに動
くとAの回転力が加わり、更に強い力が働き、持続出力
する。
To make it easier to understand, Figure 3 is a table showing how the device rotates with A to H fixed coaxially. For example, G and H of 1 (A to H) are in reverse rotation, but the remaining B, C, DE, and F assist the rotation, and when it moves slightly, the rotational force of A is added, Stronger force works to provide continuous output.

4、追加の関係 原発明く昭和59年願26561号)においては、磁力
をさえぎり尚かつ、停止状態を回転状態て′助力し回転
持続出力したものであった。
4. In an additional related invention (Application No. 26561 of 1982), the magnetic force is blocked, and the stopped state is assisted by the rotating state to provide continuous rotational output.

本発明は、磁力をさえぎる事なく回転子(X)が偏心し
た位置にある事で、同じ効果を持たせて停止状態を回転
状態で助力した。又58分の1回転づつによるA−Hの
状態を同軸に固定する方法ら原発明を応用発展させたし
のである。
In the present invention, the rotor (X) is located at an eccentric position without blocking the magnetic force, thereby providing the same effect and assisting the stopped state in the rotating state. Furthermore, the original invention has been applied and developed by a method of coaxially fixing the state of A-H by each 1/58th rotation.

【図面の簡単な説明】[Brief explanation of the drawing]

図1は基本装置のヨコ断面図、図2は図1が回転した様
子の図、図3は図1を図2の状態でA〜Hそれぞれを同
軸で固定したときの回転状層を示した表である。 N、S・・・磁極  X・・固定子  Z・回転子A〜
H・・・8分の1の回転状層 1〜8・・・・・回転の経過 R,Y・・・・固定子を書くための円 り線とKilの接点・・・・・・円(R)の中心し線と
Mliの接点・・・・・回転軸 り線とP線の交点・・−・回転子の中心円(Y)とK 
II線の接点・・・・固定子の磁極の春日(Y、R)と
Pliの交点・・・・固定子の磁極の界円転子の中のP
線・・・・・回転子の磁極の界マキ許出 願人    
 内   1)    聡P に HA 巳             C 図2 手続補正書 く自発) 昭和61年11月20コ差出 昭和61年11月15日
Figure 1 is a horizontal sectional view of the basic device, Figure 2 is a diagram of Figure 1 rotated, and Figure 3 shows the rotating layer when Figure 1 is in the state of Figure 2 and A to H are fixed coaxially. It is a table. N, S...Magnetic pole X...Stator Z/Rotor A~
H... 1/8 rotational layer 1 to 8... Progress of rotation R, Y... Point of contact between the circular line to draw the stator and Kil... Circle The point of contact between the center line of (R) and Mli...The intersection of the rotation axis line and the P line...The center circle of the rotor (Y) and K
Contact point of the II line...Intersection of Kasuga (Y, R) of the stator magnetic pole and Pli...P in the field trochanter of the stator magnetic pole
Wire: Field deviation of the rotor's magnetic poles Applicant
1) Satoshi P to HA Mi C Fig. 2 Procedural amendment voluntarily submitted) November 20, 1985 Submitted November 15, 1986

Claims (1)

【特許請求の範囲】[Claims] 図で示したように、変則的な円の空洞を設けた固定子と
、回転軸から中心をずらせた回転子の吸引反発により回
転する、永久磁石回転運動法における応用。
As shown in the figure, this is an application of the permanent magnet rotational motion method, in which a stator with an irregular circular cavity rotates due to the attraction and repulsion of a rotor whose center is offset from the rotation axis.
JP12144886A 1986-05-27 1986-05-27 Application of permanent-magnet rotation method Pending JPS62281756A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12144886A JPS62281756A (en) 1986-05-27 1986-05-27 Application of permanent-magnet rotation method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12144886A JPS62281756A (en) 1986-05-27 1986-05-27 Application of permanent-magnet rotation method

Publications (1)

Publication Number Publication Date
JPS62281756A true JPS62281756A (en) 1987-12-07

Family

ID=14811386

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12144886A Pending JPS62281756A (en) 1986-05-27 1986-05-27 Application of permanent-magnet rotation method

Country Status (1)

Country Link
JP (1) JPS62281756A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008029190A (en) * 2006-06-19 2008-02-07 Kozo Matsuki Arrangement method of magnet in magnetic driving, and magnetic driving device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008029190A (en) * 2006-06-19 2008-02-07 Kozo Matsuki Arrangement method of magnet in magnetic driving, and magnetic driving device

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