JPH03105078A - Energy generating device - Google Patents

Energy generating device

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Publication number
JPH03105078A
JPH03105078A JP24296589A JP24296589A JPH03105078A JP H03105078 A JPH03105078 A JP H03105078A JP 24296589 A JP24296589 A JP 24296589A JP 24296589 A JP24296589 A JP 24296589A JP H03105078 A JPH03105078 A JP H03105078A
Authority
JP
Japan
Prior art keywords
centrifugal
energy
output
input
shaft
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
JP24296589A
Other languages
Japanese (ja)
Inventor
Saburo Kobayashi
三郎 小林
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 JP24296589A priority Critical patent/JPH03105078A/en
Publication of JPH03105078A publication Critical patent/JPH03105078A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To generate a large amount of energy by a simple structure by generating the energy in the ratio of input for output of 1:2, in the constitution in which the inertial force of a centrifugal weight, etc, which is revolved by an input is transmitted onto an output side rotary shaft, on the outer periphery of the output side rotary shaft. CONSTITUTION:A ring gear 4 is installed inside at the edge part of a gear holder 1 having an input shaft 3 fixed at the center of a disc part 2, and an inscribed gear 5 is meshed inside the gear holder 1. A cylinder 7 is fixed at one edge part of a driving shaft 6 the other edge of which is fixed onto the inscribed gear 5, and a piston 8 is slidingly installed in the cylinder 7. The basic edge of a rod 10 is slidingly fitted into a through hole 9 at the center of the piston 8, and a centrifugal weight 11 is fixed at the top edge of the rod 10. A roller 12 which rolls on a guide wall surface 17A of a guide wall 17 supported on the inside of an output body 15 which is installed on an input shaft in free revolution is installed on the centrifugal weight 11 by a shaft 13. The surface (a) of the guide surface 17A is formed from a part of the circle in nearly a half of the surface (b).

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はエネルギーを増幅するエネルギー生成装置に関
する. [従来の技術] 従来、この種のものとして、特公昭50一8134号公
報には入力軸及び出力軸間に介在し、入力軸に関連回転
しうるように出力軸周上に設けた回転軸中で往復運動す
るピストン端部に遠心重錘を設け、この遠心重錘を誘導
回転しうるように形成した内外接案内壁面に接して回転
させ遠心重錘の遠心力を効果的に回転力となしうるよう
構成された遠心式トルクコンバータが提供されている.
尚この特公昭50−8134号に係わる発明は米国特許
第3877252号rCENTRI FUGAL  T
ORQUF,  CONVERTERJとしても提案さ
れている. [発明が解決しようとする課題J 従来技術においては、主として自動車の動力伝達装置と
して用いることにとどまったものであるが、本発明にお
いては前記従来技術の特性を活かして組合わせによるエ
ネルギーの増幅を図ったエネルギー生成装置を提供する
ことを目的とする. [課題を解決するための手段] 本発明は、入力側回転軸と出力開回転軸間に介在し且つ
出力開回転軸外周にあって入力により回転する重錘の遠
心力を出力側回転軸の一方向にのみ作用させ出力軸を回
転させる遠心式トルクコンバータ型エネルギー生成装置
において、入力対出力が1=2となる遠心エネルギーを
生成し、これを出力圓回転軸に接続される受動体に伝達
するa能を持たせたものである. [作 用] 第5図は、半径r,速度Vで矢印方向に回転運動ずる遠
心m錘11Aの遠心力と、遠心垂錘が作用して垂直に吊
り下がる重錘8Aとの力関係を示しており、同図におい
て遠心垂錘11Aの質量をm,重錘8Aの質量をMとす
ると、遠心重錘11Aの速度Vにおける運動エネルギー
は−!−m v ′であり、又遠心力は1二二2r であって、図は遠心重錘11Aの遠心力によって重ii
8Aが両者の力の釣合い点まで引上げられた状態を示し
ている. このときに於ける遠心垂錘11Aの運動エネルギーは−
1 m v 2であるが、この状態からさ2 らに速度を早め、V+ΔVに増速したときの投入エネル
ギーは =1m(2vΔV+Δv2) 2 ・・・(1)投入エネルギー ここで遠心力F= mユニで計算されるが、r 運動速度VがV+ΔVとなった時の ところがF’>Fであるため、当然m,M間に於ける力
のバランスが崩れる.そこで遠心重錘11Aの回転半径
をr+Δrに.広げる事によって、遠心重錘11Aと垂
錘8Aの間に於いては新しい力の釣合い点が作られ、F
 = F’となる.よって、 したがって、前記(1)式に基づく投入工r +Δ r .’.( r十△r)v2=r (v+Δv)2これを
整埋すると △rv2=r (v+Δv)2−rv2以上からffi
u8Aに対ずる仕事(FΔr〉はr =m(2vΔV+Δv2 ) ・・・(2》仕事 =−Lm(2vΔv+Δv2)をいったん遠心2 エネルギーに変換しこれを前記《2)式の仕事m (2
vΔV十ΔV2 )に導くことによりて、出力エネルギ
ーを投入エネルギーの2倍にすることができる. 次に前記エネルギー増加を解析する. 即ち、力学的エネルギーである運動エネルギーと位置エ
ネルギーとは直接的な関係を有するが、この両エネルギ
ーの計算は、物体の運動或いは落下のスタート時点、即
ち0点から動き出し、t時間にどれだけ変位(s=12 at2)したかを梢成要素として見ており、これに対し
、遠心力の場合の中心に向かってのt時間に於ける変位
量等は、考え方に於いでは全く同じであるが、仕事をす
るfm力に関係ずる運動エネルギーと遠心エネルギーに
ついては、円運動そのものの性格から来るのでそこに違
いが出る.即ち物体の円運動の場合、常時中心に向かっ
て加速度をもつことに起因する. 要するに、本来円の接線の方向に直線運動している物体
が中心力によりその方向が間断なく曲げさせられる場合
、当然円の中心に向っての慣性力が働くが、これと物体
の運動速度等が混じり合って遠心力の大小等変化が生ず
る.換言すれば、運動の軌道上の各点において、中心力
により無断にその接線の方向から離れさせられる運動物
体が、その慣性力によって抵抗する、その力が遠心力で
ある.そしてこの場合、投入エネルギーが、仕事に対し
て2分の1となる理由は、遠心重錘11Aを増速くΔV
)するため投入されるエネルギー以外、重錘8Aの引上
げに対してはエネルギーの投入が行われないからである
.即ち、遠心重鍾11Aに働く半径方向の力は、エネル
ギーに深くかかわりのある作用、反作用とは無関係な慣
性力によるものであり、したがって、この力により引上
げられる重錘8Aには特にエネルギーの投入が行われな
いからである. [実施例] 次に本発明の一実施例を添付図面の第1図ないし第4図
を参照して説明する. 1は、円板部2の中心に入力軸3を固設したギアホルダ
ーであって、その縁部にはリングギア4が内側に形成さ
れている.またこのリングギア4にはギアホルダー1の
内開に設けた内接ギア5が噛合している.この内接ギア
5に一端を固設した駆動軸6の他端部にはシリンダ7が
固設されており、このシリンダ7内にはピストン8が摺
動自在に設けられている.そして、このピストン8には
、該ピストン8の中心に形成した貫通孔9にロツド10
の基端を活動自在に嵌挿するとともに、このロッド10
の先端には遠心重錘11が固着されており、この遠心重
錘11には後述する案内壁面17Aを摺動するローラ1
2が軸13によって設けられている.尚、14はロツド
10がピストン8より抜け出すことを防止する抜け止め
用ストッパーであり、これとピストン8の両端部との間
には遊かんが作られている. 15は前記入力軸3に逆転自在に設けられた出力体であ
り、この出力体15は円筒箱状であって、その内側には
第4図に示すような複数個の内接案内壁面17Aが案内
壁17によって形成されており、案内壁17の一測には
、前記駆動軸16との距離を大きく形成した径大部が形
威されている.そして、この案内壁17の内周面17A
に沿って前記ローラ12が転動するようになっている. さらに、第3図に於いて前記内接案内壁面17Aは、第
4図に示されているようにAB,BC間は駆動軸6を中
心とした円状に形成され、CD間を徐々に径小に形成し
、DEfftlはOB間の略2分の1の円となし、EF
間は略榎直線状とし、さらにFA間は円を描きつつ広げ
てAに接続するというものである.尚、18は前記入力
軸3と同軸に前記出力体154こ固設した出力軸であり
、19は遠心重錘11に形戒された突起であり、この突
起19は前記両開面16に形成された外接案内壁面17
Bに摺動するようになっている. 次に前記構成につきその作用を説明する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an energy generation device that amplifies energy. [Prior Art] Conventionally, as a device of this kind, Japanese Patent Publication No. 50-18134 discloses a rotating shaft interposed between an input shaft and an output shaft and provided on the circumference of the output shaft so as to be able to rotate relative to the input shaft. A centrifugal weight is provided at the end of the piston that reciprocates inside the centrifugal weight, and the centrifugal weight is rotated in contact with an inner and outer guide wall surface formed to allow guided rotation, thereby effectively converting the centrifugal force of the centrifugal weight into rotational force. A centrifugal torque converter is provided that is configured to do so.
The invention related to this Japanese Patent Publication No. 50-8134 is U.S. Patent No. 3877252 rCENTRI FUGAL T
It has also been proposed as ORQUF and CONVERTERJ. [Problem to be solved by the invention J] In the prior art, the use was mainly limited to a power transmission device for an automobile, but in the present invention, the characteristics of the above-mentioned prior art are utilized to amplify energy by combination. The purpose of this project is to provide an energy generation device that achieves this goal. [Means for Solving the Problems] The present invention utilizes the centrifugal force of a weight that is interposed between the input-side rotating shaft and the output-opening rotating shaft and is located on the outer periphery of the output-opening rotating shaft and rotates due to the input to the output-side rotating shaft. In a centrifugal torque converter type energy generation device that acts only in one direction and rotates the output shaft, it generates centrifugal energy with an input to output ratio of 1 = 2, and transmits this to a passive body connected to the output circle rotation shaft. It has the ability to [Function] Figure 5 shows the force relationship between the centrifugal force of the centrifugal weight 11A rotating in the direction of the arrow with radius r and speed V, and the force between the centrifugal weight 8A, which hangs vertically due to the action of the centrifugal plumb. In the figure, if the mass of the centrifugal weight 11A is m and the mass of the weight 8A is M, then the kinetic energy at the speed V of the centrifugal weight 11A is -! -m v ', and the centrifugal force is 1222r, and the figure shows that the centrifugal force of the centrifugal weight 11A causes the weight ii
8A shows the state where it has been pulled up to the point where the two forces are balanced. The kinetic energy of the centrifugal plumb 11A at this time is -
1 m v 2, but when the speed is further increased from this state to V + ΔV, the input energy is = 1 m (2v ΔV + Δv2) 2 ... (1) Input energy Here, centrifugal force F = m It is calculated by Uni, but since F'>F when the r motion speed V becomes V + ΔV, the balance of forces between m and M naturally collapses. Therefore, the radius of rotation of the centrifugal weight 11A is set to r+Δr. By widening, a new force balance point is created between centrifugal weight 11A and plumbum 8A, and F
= F'. Therefore, the input work r + Δ r . based on the above formula (1). '. (r×△r)v2=r (v+Δv)2 If we fill this out, we get △rv2=r (v+Δv)2−rv2 or more, so ffi
The work (FΔr〉) for u8A is r = m (2vΔV+Δv2) ... (2) Work = -Lm (2vΔv+Δv2) is once converted into centrifugal energy, and this is the work m (2) of the above formula (2).
vΔV+ΔV2), the output energy can be made twice the input energy. Next, let's analyze the energy increase. In other words, there is a direct relationship between kinetic energy and potential energy, which are mechanical energies, but the calculation of both energies is based on the amount of displacement in time t when an object starts moving or falling from the 0 point. (s = 12 at2) is seen as a top component, whereas in the case of centrifugal force, the amount of displacement toward the center at time t, etc. is exactly the same in terms of the concept. However, there is a difference between kinetic energy and centrifugal energy, which are related to the fm force that does work, because they come from the nature of circular motion itself. In other words, this is due to the fact that when an object moves in a circular motion, there is always acceleration toward the center. In short, if an object that is originally moving linearly in the direction of the tangent to a circle is forced to bend its direction continuously due to a central force, an inertial force will naturally act toward the center of the circle, but this and the speed of the object's motion, etc. The centrifugal force changes in magnitude as a result of mixing. In other words, at each point on a trajectory of motion, a moving object that is forced away from its tangential direction by a central force is resisted by its inertial force; that force is centrifugal force. In this case, the reason why the input energy is 1/2 of the work is that the centrifugal weight 11A is accelerated by ΔV.
This is because, other than the energy input for lifting the weight 8A, no energy is input for lifting the weight 8A. In other words, the radial force acting on the centrifugal weight 11A is due to an inertial force that has nothing to do with action or reaction, which is deeply related to energy. Therefore, it is especially important to input energy to the weight 8A, which is pulled up by this force. This is because it is not done. [Embodiment] Next, an embodiment of the present invention will be described with reference to FIGS. 1 to 4 of the accompanying drawings. 1 is a gear holder in which an input shaft 3 is fixed at the center of a disc part 2, and a ring gear 4 is formed inside the edge of the gear holder. Further, an internal gear 5 provided at the inner opening of the gear holder 1 meshes with the ring gear 4. A cylinder 7 is fixed to the other end of the drive shaft 6, one end of which is fixed to the internal gear 5, and a piston 8 is slidably provided within the cylinder 7. This piston 8 has a rod 10 inserted into a through hole 9 formed in the center of the piston 8.
The proximal end of the rod 10 is freely inserted and
A centrifugal weight 11 is fixed to the tip of the centrifugal weight 11, and a roller 1 that slides on a guide wall surface 17A, which will be described later, is attached to the centrifugal weight 11.
2 is provided by the shaft 13. Incidentally, reference numeral 14 is a stopper for preventing the rod 10 from coming off from the piston 8, and play holes are provided between this stopper and both ends of the piston 8. Reference numeral 15 denotes an output body which is reversibly provided on the input shaft 3, and this output body 15 has a cylindrical box shape, and inside thereof there are a plurality of inscribed guide wall surfaces 17A as shown in FIG. It is formed by a guide wall 17, and the guide wall 17 has a large diameter portion formed at a large distance from the drive shaft 16. Inner peripheral surface 17A of this guide wall 17
The roller 12 is adapted to roll along. Further, in FIG. 3, the inscribed guide wall surface 17A is formed in a circular shape between AB and BC with the drive shaft 6 as the center, as shown in FIG. DEfftl is approximately 1/2 circle between OB, EF
The space between the two is approximately a straight line, and the space between the FA is drawn in a circle and widened to connect to A. In addition, 18 is an output shaft fixed to the output body 154 coaxially with the input shaft 3, and 19 is a projection shaped like the centrifugal weight 11, and this projection 19 is formed on the double opening surface 16. Circumscribed guide wall surface 17
It is designed to slide towards B. Next, the operation of the above structure will be explained.

入力軸3を回転駆動すると、該回転力はギアホルダー1
から両ギア4.5を介して駆動軸6に伝達され、シリン
ダー7を回転駆動する.このシリンダー7の回転に伴っ
てピストン8が回転するとともに遠心重錘11のローラ
12が内接案内壁面17Aに沿って回動し、したがって
遠心重錘11も回転する. この際第4図AC間は出力軸18からの半径方向に対し
略直角の向に指向しており、したがって、この区間では
遠心重錘11の遠心力が案内壁17の半径方向に働き、
その回転力を出力軸18に伝えてこれを回転駆動し、第
5図の解析で言う所の仕事をすることになる.一方CE
間では、遠心重錘11が案内壁17によって軸心に誘導
圧入され、従って、これとほぼ一体のピストン8は駆動
軸6を中心とするバランサーとしての働きをなし、遠心
力の左右相殺が行われ、DE間では完全なバランスが取
られる様になる.又、EF間は緩曲線であるため、遠心
力の働きが押えられる一方、遠心重錘11に付せられた
突起19と外接案内壁面17Bとが作用しあって、遠心
重錘11及びピストン8の両者を同時且つ急速に引出す
ときに起こる慣性力を外接案内壁面17Bの外面に作用
させ、その力を第1図矢印C方向の回転力同様に活用す
ることができる. FA間及びCD間に於いては、円形のため遠心力が生ず
るが出力部材の軸18に対しては半径方向であるため回
転力には影響がない.この様にして遠心重錘11が内接
案内壁面17Aを押圧しつつその遠心力として出力軸1
8に作用することができる. 要するにピストン8は遠心重錘11のAC間回転中は、
駆動軸6の軸点に位置しており十分に遠心重錘の遠心力
を案内壁17に作用させ、回転力として出力部材に鋤か
せる一方、非出力fil (DE間)では遠心重錘11
とのバランサーとしての働きをなすものである. 尚、ピストン8は中心に形成した貫通孔9内にあるロッ
ド10の2組のストッパー14間で自由に動き得る状態
にあるため、内接案内壁面17Aに作用する遠心重錘1
1の遠心力はピストン8の制約なしに働くことになる. 以上により遠心重錘11が回転中は、AC間に於いては
内接案内壁面17A,EF間に於いては外接案内壁面1
7Bを介して出力軸18に回転力を与えるため、第5図
の解析によりAC間では、エネルギーの消耗は回転のた
めの投入エネルギーのみであり、したがって、仕事に対
しては2分の1で済み、その他のCE間では出力体15
の回転に繋がる仕事がなされないためエネルギーと仕事
の関連からエネルギーの消耗は摩擦等による場合を除い
てはあり得ない. この遠心式トルクコンバータは出力側の回転数に対して
入力測の回転数が大きい場合、即ち相対的な回転差が生
じた時にのみ、それによって生ずる遠心力を回転力とし
て利用し得るものであるから、この理論を利用して、人
,出力軸3.18間に常時一定の回転差を設けるよう負
荷側との間に調整を行えば、有効な仕事をさせ、省エネ
ルギーに役立たせることができる. 例えば投入エネルギーより大きな仕事がなされることか
ら、その余分なものをエネルギーとして還元し、再利用
することができる.但し、このトルクコンバータを自動
車の駆動用に用いた場合、その走行速度が増すにしたが
って人,出力軸3.18間の回転数差が減ぜられること
になり、最終的には遠心重錘11がその有する大きな遠
心力により、出力軸18の軸心を中心とする半径方向に
位置しようとし、人,出力軸3.18間に完全な直結状
態を作ることとなる. このように前記実施例では、遠心重錘11が内接案内壁
面17A及び外接案内壁面17Bに案内され、継目なく
遠心重錘11を内接案内壁面17Aに当接させたことに
よって、スムーズな動力の伝達を行うことができる. 尚、又、第5図とこの機構の関連であるが、第5図の遠
心重錘11Aの遠心力が重力に逆らって重錘8Aを引上
げようとする働きが、第1図の遠心重錘11が内接案内
壁面17Aに作用する働きと同じ理論形をなすものであ
る.本発明は前記実施例に限定されるものではなく、例
えば1箇所の案内壁に複数の遠心重錘を設けるなど種々
の変形が可能である. [発明の効果] 本発明は入力側回転軸と出力測回転軸間に介在し且つ出
力側回転軸の外周にあって入力により回転する重錘の遠
心力を出力開回転軸の一方向にのみ作用させ出力軸を回
転させる遠心式トルクコンバータ型エネルギー生成装置
であって、入力対出力が1:2となる遠心エネルギーを
生威し、これを出力側回転軸に接続する受動体例えば発
電機等に伝達する機能を持たせたものでありこれにより
入力エネルギーに対して出力エネルギーを2倍にするこ
とができる.この場合、入力と負荷の間で人為的な調整
を行い入出力軸間に一定の回転差を設けた場合、入力以
上出力が得られることを利用して、より大きなエネルギ
ーを得ることが考えられる.なお、これは解析により明
らかなようにエネルギー保存の法則には反しない. 11・・・遠心重錘 18・・・出力軸 特  許  出  願 同 人 小   林 小  林  と
When the input shaft 3 is driven to rotate, the rotational force is transferred to the gear holder 1.
is transmitted to the drive shaft 6 via both gears 4.5, and rotationally drives the cylinder 7. As the cylinder 7 rotates, the piston 8 rotates, and the roller 12 of the centrifugal weight 11 rotates along the internal guide wall surface 17A, so that the centrifugal weight 11 also rotates. At this time, the section AC in FIG.
The rotational force is transmitted to the output shaft 18 to rotate it and perform the work described in the analysis in Figure 5. On the other hand, CE
In between, the centrifugal weight 11 is guided and press-fitted into the shaft center by the guide wall 17, and therefore, the piston 8, which is almost integral with the centrifugal weight 11, acts as a balancer around the drive shaft 6, and the left and right centrifugal forces are offset. A perfect balance will be achieved between us and DE. Furthermore, since the section EF is a gentle curve, the action of centrifugal force is suppressed, while the protrusion 19 attached to the centrifugal weight 11 and the circumscribed guide wall surface 17B act on each other, so that the centrifugal weight 11 and the piston 8 The inertial force that occurs when both of the two are simultaneously and rapidly pulled out can be applied to the outer surface of the circumscribed guide wall surface 17B, and this force can be utilized in the same way as the rotational force in the direction of arrow C in FIG. Centrifugal force is generated between FA and CD because they are circular, but since they are in the radial direction with respect to the shaft 18 of the output member, there is no effect on rotational force. In this way, the centrifugal weight 11 presses the internal guide wall surface 17A, and the centrifugal force is applied to the output shaft 1.
8. In short, while the centrifugal weight 11 is rotating between AC, the piston 8 is
Located at the axis point of the drive shaft 6, the centrifugal force of the centrifugal weight sufficiently acts on the guide wall 17 and is applied to the output member as rotational force, while at the non-output fil (between DE) the centrifugal weight 11
It acts as a balancer between Incidentally, since the piston 8 is in a state where it can freely move between the two sets of stoppers 14 of the rod 10 located in the through hole 9 formed at the center, the centrifugal weight 1 acting on the inscribed guide wall surface 17A
The centrifugal force of 1 acts without the restriction of piston 8. As described above, while the centrifugal weight 11 is rotating, the inscribed guide wall surface 17A is between AC and the circumscribed guide wall surface 1 is between EF.
Since the rotational force is applied to the output shaft 18 via 7B, the analysis in Figure 5 shows that between AC, the only energy consumed is the input energy for rotation, and therefore the work is halved. completed, output 15 between other CEs
Because the work that leads to the rotation of is not done, due to the relationship between energy and work, energy consumption is impossible except in cases such as friction. This centrifugal torque converter can use the centrifugal force generated by this as rotational force only when the input rotation speed is larger than the output rotation speed, that is, when there is a relative rotation difference. Therefore, by using this theory and adjusting the load side so that there is always a constant rotational difference between the person and the output shaft, effective work can be done and energy can be saved. .. For example, since more work is done than the input energy, that excess can be returned as energy and reused. However, when this torque converter is used to drive a car, as the running speed increases, the difference in rotational speed between the person and the output shaft 3.18 will decrease, and eventually the centrifugal weight 11 Due to its large centrifugal force, the shaft tends to be positioned in the radial direction around the axis of the output shaft 18, creating a complete direct connection between the person and the output shaft 3.18. In this manner, in the above embodiment, the centrifugal weight 11 is guided by the internal guide wall surface 17A and the external guide wall surface 17B, and by seamlessly abutting the centrifugal weight 11 against the internal guide wall surface 17A, smooth power is generated. can be transmitted. Furthermore, regarding the relationship between Fig. 5 and this mechanism, the centrifugal force of the centrifugal weight 11A in Fig. 5 that tries to pull up the weight 8A against gravity is the same as that of the centrifugal weight 11A in Fig. 1. 11 has the same theoretical form as the function acting on the inscribed guide wall surface 17A. The present invention is not limited to the embodiments described above, and various modifications are possible, such as providing a plurality of centrifugal weights on one guide wall, for example. [Effects of the Invention] The present invention applies the centrifugal force of a weight that is interposed between the input rotation shaft and the output measurement rotation shaft and rotates due to the input to the output rotation shaft only in one direction. This is a centrifugal torque converter type energy generation device that rotates the output shaft by generating centrifugal energy with an input to output ratio of 1:2, and connects this to the output rotating shaft with a passive body such as a generator. It has the function of transmitting energy to the user, thereby making it possible to double the output energy relative to the input energy. In this case, if an artificial adjustment is made between the input and the load and a certain rotation difference is established between the input and output shafts, it is possible to obtain greater energy by taking advantage of the fact that the output is greater than the input. .. Note that this does not violate the law of conservation of energy, as is clear from analysis. 11...Centrifugal weight 18...Output shaft patent filed with Doujin Kobayashi Kobayashi

Claims (1)

【特許請求の範囲】[Claims] 入力側回転軸と出力側回転軸間に介在し且つ出力側回転
軸の外周にあって入力により回転する重錘の遠心力を出
力側回転軸の一方向にのみ作用させ出力軸を回転させる
遠心式トルクコンバータ型エネルギー生成装置において
、入力対出力が1:2となる遠心エネルギーを生成し、
これを出力側回転軸に接続される受動体に伝達する機能
を持たせたことを特徴とするエネルギー生成装置。
A centrifugal system that rotates the output shaft by applying the centrifugal force of a weight that is interposed between the input-side rotation shaft and the output-side rotation shaft, and rotates due to input from the output-side rotation shaft in one direction. In the formula torque converter type energy generation device, centrifugal energy with an input to output ratio of 1:2 is generated,
An energy generation device characterized by having a function of transmitting this energy to a passive body connected to an output rotating shaft.
JP24296589A 1989-09-19 1989-09-19 Energy generating device Pending JPH03105078A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24296589A JPH03105078A (en) 1989-09-19 1989-09-19 Energy generating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24296589A JPH03105078A (en) 1989-09-19 1989-09-19 Energy generating device

Publications (1)

Publication Number Publication Date
JPH03105078A true JPH03105078A (en) 1991-05-01

Family

ID=17096866

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24296589A Pending JPH03105078A (en) 1989-09-19 1989-09-19 Energy generating device

Country Status (1)

Country Link
JP (1) JPH03105078A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8022149B2 (en) * 2003-05-02 2011-09-20 Kaneka Corporation Organic polymer containing reactive silicon group

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8022149B2 (en) * 2003-05-02 2011-09-20 Kaneka Corporation Organic polymer containing reactive silicon group

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