JPH0888988A - Magnetic power plant - Google Patents

Magnetic power plant

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Publication number
JPH0888988A
JPH0888988A JP10868893A JP10868893A JPH0888988A JP H0888988 A JPH0888988 A JP H0888988A JP 10868893 A JP10868893 A JP 10868893A JP 10868893 A JP10868893 A JP 10868893A JP H0888988 A JPH0888988 A JP H0888988A
Authority
JP
Japan
Prior art keywords
force
magnetic force
magnetic
magnet
strong
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
JP10868893A
Other languages
Japanese (ja)
Inventor
Kozo Matsuki
剛三 松木
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 JP10868893A priority Critical patent/JPH0888988A/en
Publication of JPH0888988A publication Critical patent/JPH0888988A/en
Pending legal-status Critical Current

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Abstract

PURPOSE: To provide a magnetic power plant, wherein magnetic force is made to be the power source. CONSTITUTION: A yoke is brought into contact with a magnet 1, and a side surface 3 having weak magnetic force and a side surface 4 having strong magnetic force are formed. A plurality of these magnets are regularly arranged on a fixed stage 5 and a rotary disk 6, and the line of the magnetic field, wherein the strong and weak magnetic forces are present, is formed. The magnetic force in the advancing direction toward the rotating direction of the rotary disk 6 is arranged so that the side surfaces 4 with the strong magnetic force of the magnet 1 on the fixed stage 5 and of the magnet 1 on the rotary disk 6 face to each other. For the magnetic force in the blocking direction of the rotating direction, the arrangement is performed so that the side surfaces 3 with the weak magnetic force of the magnet 1 on the fixed stage 5 and the magnet 1 on the rotary disk face to each other. Thus, the constitution is formed so that the total force of the repulsion of the magnetic force pushing the advance cannot exceed the total force of the repulsion force of the magnetic force blocking the advance in progress in the advancing direction even if the rotary disk 6 is located at any position.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は磁石に磁力の弱い側面と
別の側面に強い磁力を持たせ,これらの磁石を規則的に
並べ強い磁力同志の反発力で弱い磁力同志の反発力を越
えさせるようにした磁気動力装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention provides a magnet with a strong magnetic force on the side having a weak magnetic force and a strong magnetic force on another side, and these magnets are regularly arranged to overcome the repulsive force of the weak magnetic force by the repulsive force of the strong magnetic force. The present invention relates to a magnetic power unit configured to do so.

【002】[002]

【従来の技術】従来の動力装置には電磁誘動によるもの
はあるが,磁力のみで構成される動力装置は存在してい
ない。
2. Description of the Related Art Some conventional power plants are based on electromagnetic induction, but none of them are composed of magnetic force.

【0003】[0003]

【発明が解決しようとする課題】従来のモーターなどの
動力装置は電気による動力装置であり電気エネルギーを
必要とするため様々な費用や公害をもたらす問題が有っ
た。本発明は磁力のみを利用した磁気動力装置を提供す
ることを目的とする。
The conventional power unit such as a motor is an electric power unit and requires electric energy, and thus has a problem of causing various costs and pollution. An object of the present invention is to provide a magnetic power unit that uses only magnetic force.

【0004】[0004]

【課題を解決するための手段】上記目的を達成するため
に,本発明の磁気動力装置は,磁石(1)にヨーク
(2)を当て弱い磁力を持った側面(3)と強い磁力を
持った側面(4)を作り,これらを複数個固定台座
(5)の上に規則的にならべて固定し,磁力の強弱のあ
る磁界の列を作る。又,回転盤(6)上に上記ヨーク
(2)を当てた磁石(1)を複数個規則的に並べて固定
し,磁力の強弱のある磁界の列を作る。磁力の反発力を
利用して,回転盤(6)の進行方向に向かって推進され
る方向に当たる磁力は,固定台座(5)上の磁石(1)
と回転盤(6)上の磁石(1)のそれぞれの強い磁力を
持った側面(4)同志が向かい合う様に配置し,かつ,
回転盤(6)の進行方向を阻害する方向の磁力に対して
は,固定台座(5)上の磁石(1)と回転盤(6)上の
磁石(1)のそれぞれの弱い磁力を持った側面(3)同
志が向かい合う様に配置することによって,進行方向を
推進する磁力の反発力の総計の力が進行方向の推進を阻
害する磁力の反発力の総計の力を越えることができるよ
うに構成した磁気動力装置を提供するものである。
In order to achieve the above object, the magnetic power unit of the present invention has a side surface (3) having a weak magnetic force and a strong magnetic force by applying a yoke (2) to a magnet (1). A plurality of side surfaces (4) are formed, and a plurality of these are regularly arranged and fixed on the fixed pedestal (5) to form a row of magnetic fields having strong and weak magnetic forces. Further, a plurality of magnets (1) to which the yoke (2) is applied are regularly arranged and fixed on a rotating disk (6) to form a magnetic field array having strong and weak magnetic forces. Using the repulsive force of the magnetic force, the magnetic force that strikes in the direction in which the rotary disc (6) is propelled toward the traveling direction is the magnet (1) on the fixed pedestal (5).
And the side (4) with strong magnetic force of the magnet (1) on the turntable (6) are arranged to face each other, and
The magnets (1) on the fixed pedestal (5) and the magnet (1) on the turntable (6) have weak magnetic forces against the magnetic force in the direction that impedes the traveling direction of the turntable (6). Side surface (3) By arranging them so that they face each other, the total force of the magnetic repulsive forces that propel the traveling direction can exceed the total force of the magnetic repulsive forces that inhibit the traveling direction. The magnetic power unit configured is provided.

【0005】[0005]

【作用】磁力の強い磁石同志の反発力は,磁力の弱い磁
石同志の反発力を越えることができるので,磁石(1)
にヨーク(2)を当て弱い磁力を持った側面(3)と強
い磁力を持った側面(4)を作り,これらを複数個固定
台座(5)の上に規則的にならべて固定し,磁力の強弱
のある磁界の列を作る。又,回転盤(6)上に上記ヨー
ク(2)を当てた磁石(1)を複数個規則的に並べて固
定し,磁力の強弱のある磁界の列を作る。磁力の反発力
を利用して,回転盤(6)の進行方向に向かって推進さ
れる方向に当たる磁力は,固定台座(5)上の磁石
(1)と回転盤(6)上の磁石(1)のそれぞれの強い
磁力を持った側面(4)同志が向かい合う様に配置し,
かつ,回転盤(6)の進行方向を阻害する方向の磁力に
対しては,固定台座(5)上の磁石(1)と回転盤
(6)上の磁石(1)のそれぞれの弱い磁力を持った側
面(3)同志が向かい合う様に配置することによって,
進行方向を推進する磁力の反発力の総計の力が進行方向
の推進を阻害する磁力の反発力の総計の力を越えること
ができるように構成することによって,回転する円運動
の場合,連続した運動をする動力装置として活用でき
る。
[Operation] Since the repulsive force of the magnets with strong magnetic force can exceed the repulsive force of the magnets with weak magnetic force, the magnet (1)
Apply a yoke (2) to the side surface to make a side surface (3) having a weak magnetic force and a side surface (4) having a strong magnetic force, and regularly arrange a plurality of these on a fixed pedestal (5) to fix the magnetic force. Make a sequence of magnetic fields with different strengths. Further, a plurality of magnets (1) to which the yoke (2) is applied are regularly arranged and fixed on a rotating disk (6) to form a magnetic field array having strong and weak magnetic forces. Utilizing the repulsive force of the magnetic force, the magnetic force that strikes in the direction propelled in the traveling direction of the rotating disk (6) is the magnet (1) on the fixed pedestal (5) and the magnet (1) on the rotating disk (6). ) Each side with strong magnetic force (4) Arranged so that comrades face each other,
Moreover, with respect to the magnetic force in the direction that obstructs the traveling direction of the turntable (6), the weak magnetic forces of the magnet (1) on the fixed pedestal (5) and the magnet (1) on the turntable (6) are Sides held (3) By arranging each other so that they face each other,
In the case of rotating circular motion, it is continuous by constructing so that the total force of the magnetic repulsive force that propels the traveling direction can exceed the total force of the magnetic repulsive force that inhibits the traveling direction. It can be used as a power unit for exercise.

【0006】[0006]

【実施例】以下本発明の実施例について説明する。 (イ)使用する磁石(1)は上面がN極,下面がS極の
四角形のもので固定台座上に9個,回転盤上に10個使
用する。(図1参照) (ロ)図3のように,使用する磁石(1)のN極の面と
S極の面に磁性体の板を当ててヨーク(2)の働きをさ
せて,磁石(1)の側面の磁力を強める。四方の側面の
内少なくとも一方の側面に磁性体の板を当ててヨーク
(2)の働きをさせて弱い磁力を持った側面(3)を作
り,他方を強い磁力を持った側面(4)とする。 (ハ)一般にヨークを当てた磁石は磁束が集中する面で
は,元の磁石の単体の磁力の5〜10倍の磁力になるこ
とが知られているが,本発明も弱い磁力を持った側面
(3)と強い磁力を持った側面(4)の磁力の差は大き
い方が効果が有るが,少なくとも3倍以上の磁力の差が
有れば実施できる。 (ニ)中を円形にくり抜いた非磁体の固定台座(5)の
上に,くり抜いた円周にそって9個の磁石(1)を規則
正しく等間隔に配列する。 (ホ)固定台座(5)の上に配列する磁石(1)はくり
抜いた円の中心線上に磁石(1)の対角線が重なるよう
にし,各々の磁石(1)の弱い磁力を持った側面(3)
が同一方向になるように配列する。(図4参照) 図1,図2,図4,図5,では上方から見た平面上円の
中心に向かって左方の方向に各々の磁石(1)の弱い磁
力を持った側面(3)が来る様に配列してある。(図4
参照) (ヘ)固定台座(5)のくり抜いた円よりも2〜3mm
短い半径の非磁性体の回転盤(6)を作り,この回転盤
(6)の中心に支持軸(7)を設けて外枠(9)でおさ
えて回転盤(6)が固定台座(5)のくり抜いた円の中
で回転できるようにする。(図2参照) (ト)回転盤(6)の円周にそって磁石(5)を10個
規則正しく等開隔に配列する。 (チ)回転盤(6)の上に配列する磁石(1)は回転盤
(6)の円の中心線上に磁石(1)の対角線か重なるよ
うにし,各々の磁石(1)全ての弱い磁力を持った側面
(3)が同一方向になるように配列する,図1,図2,
図4,図5,では上方から見た平面上円の中心に向かっ
て右方の方向各々の磁石(1)の弱い磁力を持った側面
(3)が来るように配列してある。(図4参照) (リ)固定台座(5)と回転盤(6)上の磁石(1)は
反発力を利用するため,図1,図2,図4,図5,では
固定台座(5)と回転盤(6)上の磁石(1)とも上方
がN極となっている。 (ヌ)磁気に関するクーロンの法則によると『2つの点
磁極間に作用する力は相対する点磁極の強さの相乗積に
比例し,これらの点磁極間の距離の2乗に反比例す
る。』となっているのでこれを元に磁力の状態を試算し
てみる。尚,固定台座(5)上の磁石(1)が回転盤
(6)上の磁石(1)に影響をおよぼす磁石の側面同志
の最も近い距離にある点を2つの点磁極とみなして,上
記クーロンの法則を適用する。 (ル)図4の回転盤の位置による回転方向を推進する磁
力の反発力の総計と,回転方向の推進を阻害する磁力の
反発力の総計の差は次のようになる。 (a)弱い磁力を持った側面(3)と強い磁力を持つた
側面(4)の磁力の差が3倍の場合。 弱い磁力と弱い磁力の間に作用する力は 1×1=1 弱い磁力と強い磁力の間に作用する力は 1×3=3 強い磁力と強い磁力の間に作用する力は 3×3=9 となるので,それぞれの磁石(1)の位置による力の関
係は次のようになる。 推進する方向の力と推進を阻害する方向の力の差は1.
3463−1.0199=0.3264 となり,これ
は弱い磁力の32%の推進する方向の力となる。 (b)弱い磁力を持った側面(3)と強い磁力を持った
側面(4)の磁力の差が4倍の場合。 弱い磁力と弱い磁力の間に作用する力は 1×1=1 弱い磁力と強い磁力の間に作用する力は 1×4=4 強い磁力と強い磁力の間に作用する力は 4×4=16 となるので,それぞれの磁石(1)の位置による力の関
係は次のようになる。 推進する方向の力と推進を阻害する方向の力の差は2.
3946−1.3525=1.0421 となり,これ
は弱い磁力の100%の推進する方向の力となる。 (オ)図5の回転盤の位置による回転方向を推進する磁
力の反発力の総計と,回転方向の推進を阻害する磁力の
反発力の総計の差は次のようになる。 (c)弱い磁力を持った側面(3)と強い磁力を持った
側面(4)の磁力の差が3倍の場合。 弱い磁力と弱い磁力の間に作用する力は 1×1=1 弱い磁力と強い磁力の間に作用する力は 1×3=3 強い磁力と強い磁力の間に作用する力は 3×3=9 となるので,それぞれの磁石(1)の位置による力の関
係は次のようになる。 推進する方向の力と推進を阻害する方向の力の差は1.
2991−0.6439=0.6552 となり,これ
は弱い磁力の65%の推進する方向の力となる。 (d)弱い磁力を持った側面(3)と強い磁力を持った
側面(4)の磁力の差が4倍の場合。 弱い磁力と弱い磁力の間に作用する力は 1×1=1 弱い磁力と強い磁力の間に作用する力は 1×4=4 強い磁力と強い磁力の間に作用する力は 4×4=16 となるので,それぞれの磁石(1)の位置による力の関
係は次のようになる。 推進する方向の力と推進を阻害する方向の力の差は2.
1616−0.8228=1.3388 となり,これ
は弱い磁力の133%の推進する方向の力となる。以上
のことから,弱い磁力を持った側面(3)と強い磁力を
持った側面(4)の磁力の差が 3倍の場合は弱い磁力の約 32%〜 65% 4倍の場合は弱い磁力の約100%〜133%の推進す
る方向の力となる。 (ワ)以上のように,回転盤(6)は磁力の反発力によ
って連続運動をすることになる。 (カ)上記実施例における固定台座(5)上の磁石
(1)の数や回転盤(6)上の磁石(1)の数は,回転
盤(6)の大きさや,弱い磁力を持った側面(3)と強
い磁力を持った側面(4)の磁力の差の倍率や,又,固
定台座(5)上の磁石(1)と回転盤(6)上の磁石
(1)の接近点における距離などによって異なってくる
ため,回転盤(6)が連続運動するためには,これらを
調整することが大切となる。 (ヨ)よりスムーズな連続運動を得るためには,進行方
向の推進を阻害する磁力の反発力の強い点においては,
回転盤(6)上の他の磁石(1)の進行方向を推進する
磁力のより強い点が当たる様な配置が固定台座(5)上
の磁石(1)と,回転盤(6)上の磁石(1)の間に求
められる。
EXAMPLES Examples of the present invention will be described below. (A) The magnet (1) to be used is a square magnet having an N pole on the upper surface and an S pole on the lower surface, and 9 magnets are used on the fixed base and 10 magnets are used on the turntable. (See FIG. 1) (b) As shown in FIG. 3, a plate of magnetic material is applied to the N-pole surface and the S-pole surface of the magnet (1) to be used, so that the yoke (2) is caused to function and the magnet ( Increase the magnetic force on the side of 1). At least one of the four side surfaces is contacted with a magnetic plate to act as a yoke (2) to form a side surface (3) having a weak magnetic force, and the other side as a side surface (4) having a strong magnetic force. To do. (C) Generally, it is known that a magnet with a yoke applied thereto has a magnetic force of 5 to 10 times the magnetic force of the original magnet alone in terms of magnetic flux concentration, but the present invention also has a weak magnetic force. The larger the difference in magnetic force between (3) and the side surface (4) having a strong magnetic force, the greater the effect. However, it can be carried out if there is a difference in magnetic force of at least 3 times or more. (D) Nine magnets (1) are regularly arranged at regular intervals along the hollowed out circumference on a fixed base (5) of a non-magnetic body which is hollowed out in a circular shape. (E) The magnets (1) arranged on the fixed pedestal (5) are arranged such that the diagonal lines of the magnets (1) overlap with the center line of the hollowed circle, and the side surface of each magnet (1) having a weak magnetic force ( 3)
Arrange so that they are in the same direction. (See FIG. 4) In FIG. 1, FIG. 2, FIG. 4, and FIG. 5, the side surface (3) having a weak magnetic force of each magnet (1) in the leftward direction toward the center of the plane circle viewed from above. ) Are arranged so that they will come. (Fig. 4
(F) 2-3 mm more than the circle cut out from the fixed pedestal (5)
A non-magnetic rotating disk (6) having a short radius is made, a supporting shaft (7) is provided at the center of the rotating disk (6), and the rotating disk (6) is held by an outer frame (9) to fix the stationary base (5 ) Be able to rotate in a hollow circle. (Refer to FIG. 2) (g) Ten magnets (5) are regularly arranged at equal intervals along the circumference of the rotary disk (6). (H) The magnets (1) arranged on the turntable (6) should be such that the diagonal line of the magnet (1) overlaps the center line of the circle of the turntable (6), and the weak magnetic force of each magnet (1) is weak. 1 and 2 are arranged so that the side surfaces (3) having the edges have the same direction.
In FIGS. 4 and 5, the side surfaces (3) having a weak magnetic force of the magnets (1) in the right direction are arranged so as to come toward the center of the circle on the plane viewed from above. (See FIG. 4.) (i) Since the fixed pedestal (5) and the magnet (1) on the turntable (6) utilize repulsive force, the fixed pedestal (5) is used in FIGS. 1, 2, 4, and 5. ) And the magnet (1) on the turntable (6) have N poles on the upper side. (E) According to Coulomb's law on magnetism, "The force acting between two point magnetic poles is proportional to the product of the strengths of the opposing point magnetic poles, and inversely proportional to the square of the distance between these point magnetic poles. ", So try to calculate the state of magnetic force based on this. The point where the magnet (1) on the fixed pedestal (5) affects the magnet (1) on the turntable (6) at the closest distance between the side surfaces of the magnet is regarded as two point magnetic poles. Apply Coulomb's law. (L) The difference between the total repulsive force of the magnetic force that propels the rotational direction and the total repulsive force of the magnetic force that inhibits the propulsion in the rotational direction is as follows, depending on the position of the rotating disk in FIG. (A) When the difference in magnetic force between the side surface (3) having a weak magnetic force and the side surface (4) having a strong magnetic force is three times. The force acting between weak and weak magnetic forces is 1 × 1 = 1 The force acting between weak and strong magnetic forces is 1 × 3 = 3 The force acting between strong and strong magnetic forces is 3 × 3 = Therefore, the relation of the force depending on the position of each magnet (1) is as follows. The difference between the force in the direction of propulsion and the force in the direction of impeding propulsion is 1.
3463-1.0199 = 0.3264, which is 32% of the weak magnetic force in the propelling direction. (B) When the difference in magnetic force between the side surface (3) having a weak magnetic force and the side surface (4) having a strong magnetic force is four times. The force acting between weak and weak magnetic forces is 1 × 1 = 1 The force acting between weak and strong magnetic forces is 1 × 4 = 4 The force acting between strong and strong magnetic forces is 4 × 4 = Therefore, the relation of the force depending on the position of each magnet (1) is as follows. The difference between the force in the direction of propulsion and the force in the direction of impeding propulsion is 2.
3946-1.3525 = 1.0421, which is 100% of the weak magnetic force in the propelling direction. (E) The difference between the total repulsive force of the magnetic force for propelling the rotating direction and the total repulsive force of the magnetic force for inhibiting the propulsion in the rotating direction is as follows depending on the position of the rotating disk in FIG. (C) When the difference in magnetic force between the side surface (3) having a weak magnetic force and the side surface (4) having a strong magnetic force is three times. The force acting between weak and weak magnetic forces is 1 × 1 = 1 The force acting between weak and strong magnetic forces is 1 × 3 = 3 The force acting between strong and strong magnetic forces is 3 × 3 = Therefore, the relation of the force depending on the position of each magnet (1) is as follows. The difference between the force in the direction of propulsion and the force in the direction of impeding propulsion is 1.
2991-0.6439 = 0.6552, which is 65% of the weak magnetic force in the propelling direction. (D) When the difference in magnetic force between the side surface (3) having a weak magnetic force and the side surface (4) having a strong magnetic force is four times. The force acting between weak and weak magnetic forces is 1 × 1 = 1 The force acting between weak and strong magnetic forces is 1 × 4 = 4 The force acting between strong and strong magnetic forces is 4 × 4 = Therefore, the relation of the force depending on the position of each magnet (1) is as follows. The difference between the force in the direction of propulsion and the force in the direction of impeding propulsion is 2.
1616−0.8228 = 1.3388, which is 133% of the weak magnetic force in the propelling direction. From the above, when the difference in magnetic force between the side surface (3) having a weak magnetic force and the side surface (4) having a strong magnetic force is 3 times, the weak magnetic force is about 32% to 65%. It becomes the force in the direction of propulsion of about 100% to 133% of. (W) As described above, the rotating disk (6) moves continuously due to the repulsive force of the magnetic force. (F) The number of the magnets (1) on the fixed pedestal (5) and the number of the magnets (1) on the turntable (6) in the above-mentioned embodiment have the size of the turntable (6) and a weak magnetic force. Magnification of the difference in magnetic force between the side surface (3) and the side surface (4) having a strong magnetic force, and the approach point between the magnet (1) on the fixed pedestal (5) and the magnet (1) on the turntable (6). Since it depends on the distance and so on, it is important to adjust these in order for the turntable (6) to move continuously. (Y) In order to obtain a smoother continuous motion, at the point where the repulsive force of the magnetic force that hinders the thrust in the traveling direction is strong,
The magnet (1) on the fixed pedestal (5) and the magnet (1) on the turntable (6) are arranged so that the stronger magnetic point that propels the traveling direction of the other magnet (1) on the turntable (6) hits. Required between the magnets (1).

【0007】[0007]

【発明の効果】本発明は以上のような構成で,動力源に
永久磁石を利用できるため,公害のない安価な動力装置
となる,又この磁気動力装置によって,発電をすること
も容易であり,既存の電気器具等にエネルギーを供給で
きる。
Since the present invention has the above-mentioned structure and can use a permanent magnet as a power source, it becomes an inexpensive power unit without pollution, and it is easy to generate electricity by this magnetic power unit. , Energy can be supplied to existing electric appliances.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の斜視図である。FIG. 1 is a perspective view of the present invention.

【図2】本発明の断面図である。FIG. 2 is a sectional view of the present invention.

【図3】本発明の磁石にヨークを当てた斜視図である。FIG. 3 is a perspective view in which a yoke is applied to the magnet of the present invention.

【図4】本発明の磁石間の距離を示す平面図である。FIG. 4 is a plan view showing a distance between magnets of the present invention.

【図5】本発明の磁石間の距離を示す別の状態の平面図
である。
FIG. 5 is a plan view of another state showing the distance between the magnets of the present invention.

【符号の説明】[Explanation of symbols]

1 磁石 2 ヨーク 3 弱い磁力を持った側面 4 強い磁力を持った側面 5 固定台座 6 回転盤 7 支持軸 8 外枠 A,B,C,D,E,F,G,H,I,J 回転盤上の
磁石
1 Magnet 2 Yoke 3 Side with weak magnetic force 4 Side with strong magnetic force 5 Fixed pedestal 6 Rotating plate 7 Support shaft 8 Outer frame A, B, C, D, E, F, G, H, I, J Rotation Magnet on board

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 磁石(1)にヨーク(2)を当て弱い磁
力を持った側面(3)と強い磁力を持った側面(4)を
作り,これらを複数個固定台座(5)の上に規則的にな
らべて固定し,磁力の強弱のある磁界の列を作る。又,
回転盤(6)上に上記ヨーク(2)を当てた磁石(1)
を複数個規則的に並べて固定し,磁力の強弱のある磁界
の列を作る。磁力の反発力を利用して,回転盤(6)の
進行方向に向かって推進される方向に当たる磁力は,固
定台座(5)上の磁石(1)と回転盤(6)上の磁石
(1)のそれぞれの強い磁力を持った側面(4)同志が
向かい合う様に配置し,かつ,回転盤(6)の進行方向
を阻害する方向の磁力に対しては,固定台座(5)上の
磁石(1)と回転盤(6)上の磁石(1)のそれぞれの
弱い磁力を持った側面(3)同志が向かい合う様に配置
することによって,進行方向を推進する磁力の反発力の
総計の力が進行方向の推進を阻害する磁力の反発力の総
計の力を越えることができるように構成した磁気動力装
置。
1. A yoke (2) is applied to a magnet (1) to form a side surface (3) having a weak magnetic force and a side surface (4) having a strong magnetic force, and a plurality of these are mounted on a fixed pedestal (5). They are regularly arranged and fixed to form a row of magnetic fields with strong and weak magnetic forces. or,
A magnet (1) in which the above-mentioned yoke (2) is applied to a rotating disk (6).
A number of magnetic fields are regularly arranged and fixed to form a row of magnetic fields with strong and weak magnetic forces. Utilizing the repulsive force of the magnetic force, the magnetic force that strikes in the direction propelled in the traveling direction of the rotating disk (6) is the magnet (1) on the fixed pedestal (5) and the magnet (1) on the rotating disk (6). ) The magnets on the fixed pedestal (5) are arranged so that the side surfaces (4) with strong magnetic forces of (4) face each other and that obstruct the traveling direction of the turntable (6). By arranging (1) and the side of the magnet (1) on the turntable (6) with weak magnetic force (3) facing each other, the total repulsive force of the magnetic force that propels the traveling direction. Is a magnetic power unit configured to exceed the total repulsive force of magnetic force that hinders the propulsion in the traveling direction.
JP10868893A 1993-03-31 1993-03-31 Magnetic power plant Pending JPH0888988A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10868893A JPH0888988A (en) 1993-03-31 1993-03-31 Magnetic power plant

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10868893A JPH0888988A (en) 1993-03-31 1993-03-31 Magnetic power plant

Publications (1)

Publication Number Publication Date
JPH0888988A true JPH0888988A (en) 1996-04-02

Family

ID=14491141

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10868893A Pending JPH0888988A (en) 1993-03-31 1993-03-31 Magnetic power plant

Country Status (1)

Country Link
JP (1) JPH0888988A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2007007411A1 (en) * 2005-07-14 2007-01-18 Crystalbay Co., Ltd. Permanent magnet unit, rotation assist device, and motor with rotation assist
JP2008029190A (en) * 2006-06-19 2008-02-07 Kozo Matsuki Arrangement method of magnet in magnetic driving, and magnetic driving device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2007007411A1 (en) * 2005-07-14 2007-01-18 Crystalbay Co., Ltd. Permanent magnet unit, rotation assist device, and motor with rotation assist
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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