JP2009270555A - Unbalanced rotary balance - Google Patents

Unbalanced rotary balance Download PDF

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JP2009270555A
JP2009270555A JP2008141638A JP2008141638A JP2009270555A JP 2009270555 A JP2009270555 A JP 2009270555A JP 2008141638 A JP2008141638 A JP 2008141638A JP 2008141638 A JP2008141638 A JP 2008141638A JP 2009270555 A JP2009270555 A JP 2009270555A
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weight
fuel
rotation
degrees
rotary balance
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Japanese (ja)
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Masahiro Ogata
正弘 尾形
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a rotary balance as improvement of a conventional technique using a power source appearing in two types, one based on a fuel which involves demerits in terms of consumption of the fuel resources and environmental pollution with the exhaust emission and the other based on the electricity which requires electricity distribution or cells/batteries, can solve the problems inherent therein such that both types require the supply of fuel/electricity at all times and the type using a natural energy depends upon the environmental or meteorological conditions to lead to difficulty in supplying a stable power source. <P>SOLUTION: The rotary balance works with a natural fall of a weight or a buoyancy of a float as the energy source which is stable anywhere, whereby it is possible to eliminate consumption of the resources and environmental pollution and to yield a stable output. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

地球引力又は、液体中での浮力を利用した動力源に関する。The present invention relates to a power source that uses earth attraction or buoyancy in a liquid.

本発明は、物理現象の思考実験用に作成したメモが発端となっている。  The present invention starts with a memo created for a physical phenomenon thinking experiment.

よって明確な背景技術としては無く、その後、同様な物が無いかをインターネットで調べた結果、本発明品に類似する発明品として1717年オルフィレウスの永久運動機械といわれるものがあったという文献をインターネット上で検索したが、機構、動作原理が公開されておらず、資料も無いため本発明品との相違点は不明。
「インターネットアドレス」http://x51.org/x/04/04/1302.php
Therefore, there is no clear background technology, and after that it was examined on the Internet whether there was a similar thing, and as a result, there was a literature called the 1717 Orfileus permanent motion machine as an invention similar to the present invention. Although it searched above, since a mechanism and an operation principle are not disclosed and there is no data, the difference with this invention product is unknown.
“Internet address” http: // x51. org / x / 04/04/1302. php

従来の動力源のほとんどは、電気、燃料などを消費し、燃料を使うものは資源の消費、環境汚染を引き起こす一因となっている。  Most conventional power sources consume electricity, fuel, etc., and those that use fuel contribute to resource consumption and environmental pollution.

また、資源の消費、環境破壊を起こさない動力として、水力、風力、太陽熱、太陽光、等を利用したものが従来使われてきたが、状況により動作が変化し安定した出力が得られない。  Further, as power that does not cause resource consumption and environmental destruction, those using hydropower, wind power, solar heat, sunlight, etc. have been used in the past, but the operation changes depending on the situation, and stable output cannot be obtained.

課題を解決する為の手段Means to solve the problem

不平衡状態のまま回転する天秤の構造体を作り、同じ重さの重りを付けることで地球引力による重力で回転を得られるようにした。  A balance structure that rotates in an unbalanced state was created, and weights of the same weight were attached to enable rotation by gravity due to the earth's attractive force.

これにより、重りを上げるときのエネルギーが回転軸を中心とした向かい合う重りの回転軸からの距離の比で割った重量で回転し、残ったエネルギーを外部に取り出す事が可能になる。  As a result, the energy when raising the weight is rotated by the weight divided by the ratio of the distance from the rotation axis of the opposite weight with the rotation axis as the center, and the remaining energy can be taken out.

また、重りを液体よりも比重の軽い浮子に変え液体中で同様の回転、動力として使うことができる。  Moreover, the weight can be changed to a float with a specific gravity lower than that of the liquid, and the same rotation and power can be used in the liquid.

発明の効果The invention's effect

重力を使い動力とすることで、電気、燃料の消費が無く資源の消費、環境破壊の無い動力源として使うことができる。  By using gravity as the power, it can be used as a power source without consumption of electricity and fuel, resource consumption and environmental destruction.

自然エネルギーとしても地球引力による重力又は、液体中では比重の差による浮力を利用できるため、常に安定した動力源として提供できる。  As natural energy, gravity due to the earth's attractive force or buoyancy due to the difference in specific gravity can be used in the liquid, so that it can always be provided as a stable power source.

発明の実施する為の最良の形態BEST MODE FOR CARRYING OUT THE INVENTION

以下、本発明の実施の形態を図1〜図基づいて説明する。  Hereinafter, embodiments of the present invention will be described with reference to FIGS.

図1は本発明の主要部品の一つ、重り軸3と重り4の関係を説明するために他の部品を取り去った状態の直線軌道板の図である。  FIG. 1 is a view of a linear raceway plate with one of the main parts of the present invention, the other parts removed, for explaining the relationship between the weight shaft 3 and the weight 4.

直線軌道板1には、回転軸2の中心から4分割した90度の線7に長穴6が明けてあり、ここに重り軸3と重り4を組とする重りブロックか各穴に一組づつ入り9,8,4,10、共に5の範囲を直線で移動できる。  The straight raceway plate 1 has a long hole 6 in a 90-degree line 7 divided into four from the center of the rotating shaft 2, and a weight block including a weight shaft 3 and a weight 4 or a pair in each hole. Each of 9, 8, 4, 10, and 5 can be moved in a straight line.

図2は、図1の状態に回転軸2に対して水平方向に12の距離、離れた位置11を中心とした同心円の円形軌道溝13があり重りブロック4、8、9,10は共に、この円形軌道溝13を通り、11を中心に円形に移動します。この円形の円形軌道溝13は、直線起動板1の回転に対して常に固定された位置にあります。  2 has a concentric circular raceway groove 13 centered on a position 11 that is a distance of 12 in the horizontal direction with respect to the rotation axis 2 in the state of FIG. 1, and the weight blocks 4, 8, 9, and 10 are both It passes through this circular track groove 13 and moves circularly around 11. This circular circular groove 13 is always in a fixed position with respect to the rotation of the linear starting plate 1.

これまでの構成により、重りブロック4、8、9、10は直線軌道板1の回転に対して、回転軸2を中心に回転するのではなく、回転軸2から12の距離ずれた点11を中心とした同心円を移動することになります。  According to the configuration so far, the weight blocks 4, 8, 9, 10 do not rotate around the rotation axis 2 with respect to the rotation of the linear raceway plate 1, but a point 11 shifted by a distance of 12 from the rotation axis 2. The concentric circle around the center will move.

図3〜図8は、この構成で図3の位置を0度として、15度毎に時計回りに回転させたときの直線軌道板1と円形軌道溝13と重りブロック4組の相対位置関係を示す。3 to 8 show the relative positional relationship between the linear track plate 1, the circular track groove 13 and the four weight blocks when the position of FIG. 3 is set to 0 degree in this configuration and rotated clockwise every 15 degrees. Show.

図3は0度の回転板1の回転角度のときの回転板と重りの相対位置の図で、図4は15度回転したとき、図5は30度、図6は45度、図7は60度、図8は75度、回転したときの図であり、以後90度回転したとき重りの相対位置は図3と同じになり、これを繰り返します。  FIG. 3 is a diagram of the relative positions of the rotating plate and the weight when the rotating plate 1 has a rotation angle of 0 degree. FIG. 4 shows a rotation of 15 degrees, FIG. 5 shows 30 degrees, FIG. 6 shows 45 degrees, and FIG. 60 degrees, Figure 8 is the figure when it is rotated 75 degrees, and when it is rotated 90 degrees thereafter, the relative position of the weight will be the same as in Figure 3, and this will be repeated.

回転方向は図3〜図8で示した通り、時計周りに回ります。この回転のときに、重要なのは、回転軸1からの各、重りブロックの距離で、重りブロックの上昇中は中心軸からずらした距離12の分、内側15を通り、下降中は距離12の分外側16を通ることです。この回転運動で、回転軸を天秤の支点として例えると、右側の重りは、左側の重りを、てこの原理で相対的に軽く上げる事ができるようになり、回転軸に対しての右側の距離と左側の重りの距離の差で360度、常に不平衡状態を保つ事になります。  The direction of rotation is clockwise as shown in Figs. In this rotation, what is important is the distance of each weight block from the rotating shaft 1. When the weight block is lifted, the distance is 12 corresponding to the distance shifted from the central axis. It ’s through the outside 16. In this rotary motion, if the rotation axis is compared with the balance fulcrum, the right weight can be lifted relatively lightly by the lever principle, and the right distance from the rotation axis. The difference between the weight on the left side and the weight on the left side will always keep an unbalanced state at 360 degrees.

以上が、回転したときの簡単な動作説明で、以降、動作時の力学的説明を進める上で各部分の寸法があると出力軸から取り出せる出力を簡略化し、説明を容易にかつ実際に取り出せる出力を計算できるとの判断で寸法を入れて、より詳しく説明します。  The above is a simple explanation of the operation when rotating. After that, when proceeding with the mechanical explanation at the time of operation, if there are dimensions of each part, the output that can be extracted from the output shaft is simplified, and the output that can be easily and actually explained We will explain in more detail by putting in the dimensions that we can calculate.

図9は、各部分の寸法取りを容易に説明できるように45度回転した図6の点線部分の拡大図である。  FIG. 9 is an enlarged view of the dotted line portion of FIG. 6 rotated 45 degrees so that the dimensioning of each portion can be easily explained.

設計の一例として、各部分の寸法は、回転軸中心2からの円形軌道溝13の中心11の距離を50mm、円形軌道溝13の半径14を150mm、とした場合、これを15度毎回転したときの回転軸1から各錘までの寸法を表1に示す。  As an example of the design, the dimensions of each part are set such that the distance of the center 11 of the circular raceway groove 13 from the rotation axis center 2 is 50 mm, and the radius 14 of the circular raceway groove 13 is 150 mm. Table 1 shows the dimensions from the rotary shaft 1 to each weight.

4組の重りは同じ重量の物を使うものを使い、対角にある重りの組は、天秤を形成するので、回転軸を始点として式1の公式になり、これに合わせ表1を表2のように計算すると、最終的な結果は、全角度で同じ値になります。  Since the four weights use the same weight, the diagonal weights form a balance. Therefore, the formula of Formula 1 starts from the rotation axis. The final result is the same for all angles.

最終的には、距離100mmとなり、図11のように回転軸2から水平に出した棒22の先に一組の重り10を付けた状態と同じとなり、この状態を全周において維持し回転を続けることになります。  Eventually, the distance becomes 100 mm, which is the same as the state in which a set of weights 10 is attached to the tip of the rod 22 that is horizontally extended from the rotary shaft 2 as shown in FIG. Will continue.

また、この回転を釣り合い、止った状態にするためには、式2の重量23が必要なので、この設計例の寸法で設計した場合は、回転軸の半径21が5mmで、一組の重り重量を1Kgとした場合、釣り合わせるためには、軸に20Kgの重り23を吊り下げる必要があります。よって、この重量よりも軽い負荷で重力が掛かる場所であれば、壊れるか、または消耗して負荷が大きくならない限り回転を続けることとなります、また始動するときに外部から力を掛ける必要もありません。  In addition, in order to balance and stop the rotation, the weight 23 of Formula 2 is necessary. Therefore, when designed with the dimensions of this design example, the radius 21 of the rotating shaft is 5 mm, and a set of weight weights. In order to balance 1kg, it is necessary to suspend a 20kg weight 23 on the shaft. Therefore, if it is a place where gravity is applied with a load lighter than this weight, it will continue to rotate as long as it does not break or wear out and the load increases, and there is no need to apply external force when starting.

この回転自体は、液体中でも液体の流体抵抗がかかるとして、重力がある限り同様に回転します。また重力だけではなく、重りの代わりに気体を封入した浮子又は、液体よりも比重の軽い物を同様に取り付けても回転をします。しかし力の方向が重力では下方向に力が掛かりますが、浮力では上方向に力が掛かるため回転方向は逆になります。  This rotation itself rotates in the same way as long as there is gravity, assuming that the fluid resistance of the liquid is applied even in the liquid. In addition to gravity, it rotates even if a float with gas sealed instead of weight or an object with a specific gravity lighter than liquid is installed in the same way. However, if the direction of force is gravity, force is applied downward, but if buoyancy is applied, force is applied upward, so the direction of rotation is reversed.

本発明品は、さらに固定としていた円形軌道溝13を回転軸方向に移動することで出力軸のトルクの可変も可能です。円形軌道中心11が回転軸中心2の位置と同じになると出力0、これを越え反対側になると回転軸、回転方向が逆回転するようになります。  The product of the present invention can also change the torque of the output shaft by moving the circular raceway groove 13, which has been fixed, in the direction of the rotation axis. When the circular orbit center 11 is the same as the position of the rotation axis center 2, the output is 0, and when it is beyond the rotation axis, the rotation axis and the rotation direction are reversed.

本発明の構成の一部、直線軌道板と一組の重り、重り軸Part of the configuration of the present invention, a linear track plate and a set of weights, weight shaft 本発明の全構成、図1に円形軌道溝と3組の重り、重り軸を追加した図The entire configuration of the present invention, a diagram in which a circular raceway groove, three sets of weights, and a weight shaft are added to FIG. 直線軌道板の回転角度0度のときの図The figure when the rotation angle of the straight track plate is 0 degree 同、回転角度15度のときの図The figure when the rotation angle is 15 degrees 同、回転角度30度のときの図The figure when the rotation angle is 30 degrees 同、回転角度45度のときの図The figure when the rotation angle is 45 degrees 同、回転角度60度のときの図The figure when the rotation angle is 60 degrees 同、回転角度75度のときの図The figure when the rotation angle is 75 degrees 図6点線部の拡大図Figure 6 Enlarged view of the dotted line 回転角度15度のときの全体拡大図Overall enlarged view when the rotation angle is 15 degrees 計算結果による等価図Equivalent diagram based on calculation results

表1Table 1

設計例による回転角度15度毎の回転軸から重りまでの距離の表Table of distance from rotation axis to weight for each rotation angle of 15 degrees according to design example

表2Table 2

表1の式1による計算結果Calculation result by equation 1 in Table 1

式1Formula 1

回転軸から重りまでの合算式Summation formula from rotating shaft to weight

式2Formula 2

回転軸出力に釣り合う重量の計算式Formula to calculate the weight that matches the rotary shaft output

Claims (2)

通常、重さを量るために使われる天秤を不平衡状態のまま回転可能な構造とした構造体。A structure in which a balance that is usually used for weighing can be rotated in an unbalanced state. 請求項1の不平衡状態で回転可能な構造体に、重り又は、浮子を取り付けることにより重力、浮力を利用して回転させ回転力を動力として取り出せるようにした動力源。A power source capable of extracting the rotational force as power by rotating the structure that can be rotated in an unbalanced state according to claim 1 by using a weight or a float and utilizing gravity and buoyancy.
JP2008141638A 2008-04-30 2008-04-30 Unbalanced rotary balance Pending JP2009270555A (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20110074163A1 (en) * 2009-09-29 2011-03-31 Mary Grace Soriano Timcang Cangrier-M87 machine or C-M87 a very powerful synchronized multi-lever perpetual motion machine designed for hydroelectric (hydraulic) power generation water recycling concept
US20110241355A1 (en) * 2008-12-13 2011-10-06 Egon Frommherz Assembly for the use of alternative energy

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20110241355A1 (en) * 2008-12-13 2011-10-06 Egon Frommherz Assembly for the use of alternative energy
US20110074163A1 (en) * 2009-09-29 2011-03-31 Mary Grace Soriano Timcang Cangrier-M87 machine or C-M87 a very powerful synchronized multi-lever perpetual motion machine designed for hydroelectric (hydraulic) power generation water recycling concept

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