JPS62131754A - Apparatus for converting rotary kinetic force to unidirectional propulsive force - Google Patents
Apparatus for converting rotary kinetic force to unidirectional propulsive forceInfo
- Publication number
- JPS62131754A JPS62131754A JP27004185A JP27004185A JPS62131754A JP S62131754 A JPS62131754 A JP S62131754A JP 27004185 A JP27004185 A JP 27004185A JP 27004185 A JP27004185 A JP 27004185A JP S62131754 A JPS62131754 A JP S62131754A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic force
- force
- rotor
- generator
- magnet
- 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
- Reciprocating, Oscillating Or Vibrating Motors (AREA)
- Linear 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、自動車、船舶、航空機、宇宙船等の推進装置
に関する。DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to propulsion devices for automobiles, ships, aircraft, spacecraft, etc.
(ロ) 従来の技術
従来の自ttth*、船舶、航空機等の推進装置の構造
及びその原理は各種乗り物に依って著しく異なるもので
あり、又装置も極めて複雑な構造をしている。(b) Prior Art The structures and principles of conventional propulsion devices for ships, aircraft, etc. differ significantly depending on the type of vehicle, and the devices also have extremely complex structures.
(B) 発明が解決しようとする問題点従って、従来の
乗り動用推進装置に於ては、必然的に大型1量物化して
しまい、且つ、故障の原因となりつる個所も極めて多い
。これに対し、本発明は極めて簡単な構造である為、小
型軽量化出来ると共に故障の原因を減らす事が出来、且
つ同一メカニズムで自動車、船舶、航空機等の共通の推
進装置と成りつる。(B) Problems to be Solved by the Invention Therefore, conventional propulsion devices for vehicles are inevitably large and monolithic, and have an extremely large number of parts that can cause failures. On the other hand, since the present invention has an extremely simple structure, it can be made smaller and lighter, and the causes of failure can be reduced, and the same mechanism can be used as a common propulsion device for automobiles, ships, aircraft, etc.
に)問題を解決する為の手段
本発明の実施の一例を図面に基づき説明すると、第1図
に於て回転子2に磁力発生装置3を取付け、角度αを自
在にする為のベアリング7を経て連結器6を用いて回転
軸1に連結する。そしてこの磁力発生装@6の回転円周
上に磁力発生装@4(この例でfl ’Jング状の電磁
石)を設置し本体5に固着している。(b) Means for Solving the Problems An example of the implementation of the present invention will be explained based on the drawings. In FIG. Then, it is connected to the rotating shaft 1 using a coupler 6. A magnetic force generating device @4 (in this example, a fl'J ring-shaped electromagnet) is installed on the rotating circumference of this magnetic force generating device @6 and is fixed to the main body 5.
又この例でii磁力発生装置6が永久磁石、他方が電磁
石としであるが反対にしても良いし、又は両方共電磁石
としても良い。要Via力の反発作用を一時的に発生さ
せる事が出来れば良いのである。その為にマイクロスイ
ッチ13を連結器6醜付けている。Further, in this example, the magnetic force generating device ii is a permanent magnet and the other is an electromagnet, but the arrangement may be reversed, or both may be electromagnets. It is sufficient if the repulsive action of the required Via force can be generated temporarily. For this purpose, the microswitch 13 is attached to the coupler 6.
図では省略しであるがこのマイクロスイッチ13は磁力
発生装置4の電磁石コイルと接続されコイルは電源に接
続される。Although not shown in the figure, this microswitch 13 is connected to an electromagnetic coil of the magnetic force generator 4, and the coil is connected to a power source.
(ホ)作 用
このような装置に於て回転軸1をモーター12で回転さ
せると、本装置の如く回転子が回転軸に対して角度自在
構造をもつ場合、遠心力作用の一面として回転子と回転
軸との間には角度αを直角に保とうとする作用が生じる
。(e) Effect When the rotary shaft 1 is rotated by the motor 12 in such a device, if the rotor has a structure that can freely angle with respect to the rotary shaft as in this device, one aspect of the centrifugal force is that the rotor There is an effect that attempts to keep the angle α perpendicular between the axis of rotation and the axis of rotation.
つまり伺らかの方法により一時的に回転子が回転軸に対
して直角方向からずれた場合には、回転子を回転軸に対
して直角に戻そうとする力が働くのである。さて、図で
は角度αが直角に近い角度の詩画磁力発生装置間の間隔
が接近した状態となるようにしである。この時点でマイ
クロスイッチ15がONの状態に入り磁力発生装置61
4にt九が流れ両磁力発生fc置間に磁力の反発作用を
生じさせる。その結果磁力発生装置4に入方向のインパ
クト力を与え、反対に磁力発生装置5は回転子が連結器
の中のベアリングのセンタービンを中心に回転してB方
向へ移動する。この作用は角度αを直角に保とうとする
遠心力作用に抗してB方向へ移動するものである。従っ
てこの磁力の反発作用は遠心力の角枇αを直角に保とう
とする力よりも太きけれは良いのである。その結果第2
図の如き状態になる。この時に大事な事は磁力発生装#
3がB方向へ移動する際の作用力の一部が本体5には伝
わりにくい機構でもあるという点である。モしてB方向
への作用力と遠心力作用により角度αを直角にしようと
する力とが釣り合った時点でB方向への磁力発生装置3
の移動は止まり今匿は遠心力作用により磁力発生装f3
が磁力発生装置4に加速をつけながら接近していく。つ
まり第2図の状態から再び第1図の状態へと復帰する。In other words, if the rotor is temporarily displaced from the direction perpendicular to the rotation axis using the method described above, a force acts to return the rotor to the direction perpendicular to the rotation axis. In the figure, the angle α is close to a right angle so that the distance between the poetry magnetic force generating devices is close to each other. At this point, the microswitch 15 enters the ON state and the magnetic force generator 61
At 4, t9 flows, causing repulsion of magnetic force between both magnetic force generation fc positions. As a result, an impact force is applied to the magnetic force generating device 4 in the incoming direction, and conversely, the rotor of the magnetic force generating device 5 rotates around the center pin of the bearing in the coupler and moves in the B direction. This action causes movement in the direction B against the action of centrifugal force which attempts to keep the angle α perpendicular. Therefore, the repulsion of this magnetic force is better if it is greater than the force of centrifugal force that tries to keep the angle α at right angles. As a result, the second
The state will be as shown in the figure. The important thing at this time is the magnetic force generator #
It is also a mechanism in which a part of the acting force when 3 moves in direction B is difficult to be transmitted to main body 5. When the force acting in the direction B and the force trying to make the angle α perpendicular due to the centrifugal force are balanced, the magnetic force generating device 3 in the direction B
stopped moving, and now the magnetic force generator f3 was activated by centrifugal force.
approaches the magnetic force generator 4 while accelerating. That is, the state shown in FIG. 2 returns to the state shown in FIG. 1 again.
この時に大事な事は磁力発生装置3のこの移動が遠心力
作用の角度αを直角に保とうとする言わば自然の力の一
部を利用している為にこの磁力発生装置6の移動に際し
又もや本体5には殆ど反作用が掛らないという点である
。それ故に上述したこのシステムの1サイクルに於て本
体をF方向に推進させる力とその反作用との間に力の差
が生じる為に本装置自体がF方向へ推進する事が可能で
あり、本装置はこれら一連の作用を規則的且つ連続的釦
発生させて本装置自体を単一方へ推進させる発明である
。What is important at this time is that this movement of the magnetic force generator 3 utilizes a part of the natural force that tries to keep the angle α of centrifugal force at right angles, so when moving the magnetic force generator 6, the main body 5 has almost no reaction. Therefore, in one cycle of this system described above, there is a difference in force between the force that propels the main body in the F direction and its reaction, so the device itself can be propelled in the F direction. The device is an invention that generates a series of these actions regularly and continuously using buttons to propel the device itself in a single direction.
向 (へ)発明の効果
本発明は、以上説明した如(、極めて簡単な構造ながら
、本装置自身が自ら単一方向へと推進するという、正に
画期的な推進装置であり、今後の産業上に多大なメリッ
トを与える事が出来つるものでおる。Effects of the Invention As explained above, the present invention is a truly revolutionary propulsion device in which the device itself propels itself in a single direction, although it has an extremely simple structure. It is a vine that can bring great benefits to industry.
第1図、第2図共に本装置の側面図であり、第1図は磁
力発生値[3が磁力発生装置4に最接近した瞬間を示し
、第2図は磁力の反発作用によって磁力発生値[3が磁
力発生値[4から離れた状態を示す。Both Figures 1 and 2 are side views of this device. Figure 1 shows the moment when the magnetic force generation value [3 approaches the magnetic force generator 4], and Figure 2 shows the magnetic force generation value due to the repulsion of the magnetic force. [3 indicates a state away from the magnetic force generation value [4].
Claims (1)
徴とする回転子に磁力発生装置(3)を取付け、この磁
力発生装置の回転円周上の対面する位置に磁力発生装置
(4)を設置し、回転軸をモーター等により回転させる
。 そして両磁力発生装置間の間隔接近時に両磁力発生装置
に磁力の反発作用を一時的に発生させ、磁力発生装置(
4)に(A)方向のインパクト力を与え本体(5)を(
F)方向へ推進させ、反対に磁力発生装置(5)を(B
)方向に移動させる。この際角度自在構造をもつ回転子
故、磁力発生装置(3)の(B)方向への作用力の一部
が本体(5)には伝わりにくいという性質を利用し、反
対に両磁力発生装置間の間隔を最大から最小へと変化さ
せるには、遠心力作用の一面として生ずる回転軸と回転
子とのなす角度(α)を直角に保とうとする性質を利用
して略一方的な作用により磁力発生装置(3)を磁力発
生装置(4)方向に移動させ、再度磁力の反発工程へと
至らせる事を特徴とする、回転運動力を単一方向推進力
に変換する装置[Claims] A magnetic force generating device (3) is attached to a rotor characterized by being able to freely change the angle (α) with respect to the rotation axis, and the magnetic force generating device (3) is placed at facing positions on the rotational circumference of the rotor. A magnetic force generator (4) is installed, and the rotating shaft is rotated by a motor or the like. Then, when the distance between the two magnetic force generators approaches, a repulsive effect of magnetic force is temporarily generated in both the magnetic force generators, and the magnetic force generator (
Apply an impact force in the direction (A) to 4) and move the main body (5) to (
Propel the magnetic force generator (5) in the direction (B).
) direction. In this case, since the rotor has a freely angular structure, a part of the acting force of the magnetic force generator (3) in the (B) direction is difficult to be transmitted to the main body (5), and by using this property, both magnetic force generators In order to change the distance between the two from the maximum to the minimum, the angle (α) between the rotation axis and the rotor, which occurs as one aspect of the centrifugal force, is maintained at right angles by a substantially unilateral action. A device for converting rotational kinetic force into unidirectional propulsive force, characterized by moving the magnetic force generator (3) in the direction of the magnetic force generator (4) and causing the magnetic force to repel the process again.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27004185A JPS62131754A (en) | 1985-12-01 | 1985-12-01 | Apparatus for converting rotary kinetic force to unidirectional propulsive force |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27004185A JPS62131754A (en) | 1985-12-01 | 1985-12-01 | Apparatus for converting rotary kinetic force to unidirectional propulsive force |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62131754A true JPS62131754A (en) | 1987-06-15 |
Family
ID=17480705
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP27004185A Pending JPS62131754A (en) | 1985-12-01 | 1985-12-01 | Apparatus for converting rotary kinetic force to unidirectional propulsive force |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62131754A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1993008635A1 (en) * | 1991-10-14 | 1993-04-29 | Muneaki Takara | Rotary electric machine |
WO1993008634A1 (en) * | 1991-10-14 | 1993-04-29 | Muneaki Takara | Rotary electric machine |
GB2337304A (en) * | 1998-04-23 | 1999-11-17 | David Hellier | Thrust producing device |
GB2481604A (en) * | 2010-06-29 | 2012-01-04 | Roger William Hall | Device that converts rotary motion into unidirectional motion |
-
1985
- 1985-12-01 JP JP27004185A patent/JPS62131754A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1993008635A1 (en) * | 1991-10-14 | 1993-04-29 | Muneaki Takara | Rotary electric machine |
WO1993008634A1 (en) * | 1991-10-14 | 1993-04-29 | Muneaki Takara | Rotary electric machine |
GB2337304A (en) * | 1998-04-23 | 1999-11-17 | David Hellier | Thrust producing device |
GB2481604A (en) * | 2010-06-29 | 2012-01-04 | Roger William Hall | Device that converts rotary motion into unidirectional motion |
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