JP2009113778A - Angle changing and moving method by rotating body, and moving body - Google Patents

Angle changing and moving method by rotating body, and moving body Download PDF

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JP2009113778A
JP2009113778A JP2007311574A JP2007311574A JP2009113778A JP 2009113778 A JP2009113778 A JP 2009113778A JP 2007311574 A JP2007311574 A JP 2007311574A JP 2007311574 A JP2007311574 A JP 2007311574A JP 2009113778 A JP2009113778 A JP 2009113778A
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Toshimaro Sada
俊麿 佐田
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Abstract

<P>PROBLEM TO BE SOLVED: To solve the problems in an angle changing and moving method by a rotating body, and a moving body such that the moving body is moved by kicking an object such as the ground backwardly; however, the moving body is moved depending on the object, and the movement of the body caused by the linear action/reaction slips according to the state of the object, and causes troubles such as an accident due to insufficient braking or the like. <P>SOLUTION: A moving body is moved by kicking an object 4 backwardly by a rotary shaft 6 at a center of a long hole 10 formed in the center of a rotating body 9. When a trouble occurs by the slip of the object 4, the rotary shaft 6 is shifted to a rotary shaft 6' to generate the lateral movement component at a right angle thereto. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

棒高跳びの、棒先のように、棒先を跳躍者が次々と長く繰り出して、長さが変化して、地面等の対象を蹴らずに移動する、回転体による角度変換移動方法および移動体に関する。  The present invention relates to an angle conversion moving method using a rotating body and a moving body, in which a jumper extends a bar tip one after another like a rod tip of a pole vault, and the length changes to move without kicking an object such as the ground. .

棒高跳びにおいて、跳躍者は前方に棒先をついて、棒先を支点として、高さを競うが、これを観ると、跳躍者は跳躍により、高さと同時に棒先へと、横方向に進む。
すなわち、跳躍者は、上方向と横方向に、棒先を支点として回転している。
この状態は、跳躍者(回転体)の半径の円周を越えて、すなわち半径の外(そと)に、回転の支点を設置して、回転体全体が回転(公転)している、回転体の動きと等しい。
In a pole vault, a jumper puts a rod tip forward and competes for height using the rod tip as a fulcrum. When this is seen, the leap jumper proceeds to the rod tip at the same time as the height by jumping.
That is, the jumper rotates in the upward direction and the horizontal direction with the rod tip as a fulcrum.
In this state, the rotation body is rotated (revolved) by setting a fulcrum of rotation beyond the circumference of the radius of the jumper (rotary body), that is, outside the radius. Equal to body movement.

言い換えると、回転軸(跳躍者の回転)方向以外への、主として逆回転方向に加力(棒先をついて)して発生する加力方向(上方向)と、直角方向(横方向)の合力のうちの、高さ方向(上方向)で高さを競い、本願では、直角方向(横方向)の移動成分により移動する、回転体による角度変換移動である。  In other words, the resultant force in the direction of the force (upward) generated by applying force (with the tip of the rod) mainly in the reverse direction to the direction other than the direction of the rotation axis (the jumper's rotation) and the right angle (lateral direction) Among them, in the present application, it is an angle conversion movement by a rotating body that competes for height in the height direction (upward direction) and moves by a moving component in a right angle direction (lateral direction).

この際、棒先は対象である地面を、頂上に達するまで、後方に蹴ることはできない。
すなわち、自転している回転体が公転するに際して、0度から90度までの移動間は、反作用は下方向となり、回転体は後方に、反作用を及ぼさないもので、結果として後方に蹴ることはなく、棒先を支点として、上方向と横方向の合力により、公転する回転体は、加力(棒先をつく)により、発生した加力方向の成分と直角方向の成分の合力の成分の内の直角(横)方向の移動成分により、移動するため、作用(加力)と直角移動成分とは、作用と反作用が、直線の作用反作用ではなく、直角の作用反作用となる。
At this time, the stick tip cannot kick the target ground until it reaches the top.
That is, when the rotating body that rotates is revolving, the reaction is in the downward direction during the movement from 0 to 90 degrees, and the rotating body does not exert the reaction backwards. Instead, the rotating body that revolves with the resultant force in the upward and lateral directions using the tip of the rod as a fulcrum, the component of the resultant force of the component in the direction perpendicular to the component in the direction perpendicular to the force applied by the force (attaching the rod tip) The movement (force) and the right-angle movement component are not a linear action and reaction, but a right-angle action and reaction.

上記現象は、棒高跳びに止まらず、ステッキ、松葉杖、人間の歩行の際の差し足等、対象を押さえ付けて移動する、すべての動作に当てはまり、また、地面(対象)を蹴って移動する、とする、車両等のタイヤ等も、重力により生じる摩擦により、横方向(後方)への加力により発生した、逆横方向と下方向の合力の移動成分の内の横移動成分により、移動するものであり、直進しておらず、横、下方向の成分で移動して、軌跡は円弧の連続で、対象(地面)に対して滑っては進めないのは、その証左となる現象であり、銃の弾丸、ロケット、素粒子等、直接爆発等から力を重心に受けて移動する、直線の作用反作用(以下直線法と称す)による移動体以外の、すべての、水、空気、地面等の対象に依拠して、重心以外に加力して移動する、、微生物から飛行機等の果てまで、対象が必要であって、対象に依拠して、移動するものは、すべて回転により移動する。と言える。  The above phenomenon does not stop at the pole vault, but applies to all movements that hold down the object, such as walking sticks, crutches, limbs when walking, etc., and also moves by kicking the ground (object) Tires of vehicles, etc., also move due to the lateral movement component of the reverse lateral and downward resultant force generated by the force applied in the lateral direction (rear) due to the friction caused by gravity It is a phenomenon that proves that it is not going straight, it moves in the horizontal and downward components, the locus is a continuous arc, and it does not slide forward against the object (ground), All of water, air, ground, etc., except for moving objects such as gun bullets, rockets, elementary particles, etc., which move directly under the force of a direct explosion, etc. Depending on the object, move with force other than the center of gravity, From microorganisms to the ends of such an airplane, a required subject, it relies on the subject, those that move, all moved by the rotation. It can be said.

2005−112718  2005-127718 大原出版社−高校教科書−新物理  Ohara publisher-high school textbook-new physics

従来古来、物体の移動は、すべて、直線の作用反作用で成り立つものとされてきたため、すべての力の取り出し方は、直線の作用反作用でなされると決められ、開発創造も、その方向に決められたため、移動においても、一方向のみの力の取り出し方を必要として、ひいては、直面する、温暖化等、多くの生物の生存上の危機と直面している。
本願は、その解決、あるいは先延ばしの端緒となるものである。
Traditionally, the movement of an object has always been realized by the action and reaction of a straight line. Therefore, it is determined that all methods of taking out force are made by the action and reaction of a straight line, and development and creation are also decided in that direction. Therefore, even in movement, it is necessary to take out a force in only one direction, and as a result, we are faced with the survival crisis of many organisms such as global warming.
This application is the beginning of the solution or procrastination.

直線の作用反作用となる物体の移動の他に、回転体には、各々独立して、かつ相関する自転と公転があり、本願は、自転が公転に移行する際の原理に基づくもので、回転体の移動においては、前記棒高跳びの例のように、回転要素、あるいは回転体の移動においては、直角に作用反作用が表れる現象が存在して、上記回転体全体が回転して公転となる、自転と公転は各々が独立した動きである、自転が公転に変化する際の現象により、作用と反作用が直角となる現象により、直線の作用反作用の直線法ではなく、直角の作用反作用(以下直角法と称す)による、回転体の移動を得るものである。  In addition to the movement of the object that acts as a reaction of the straight line, the rotating body has independent and correlated rotations and revolutions, and this application is based on the principle when the rotation shifts to revolutions. In the movement of the body, as in the example of the pole vault, in the movement of the rotating element or the rotating body, there is a phenomenon in which an action and reaction appears at a right angle, and the entire rotating body rotates and revolves. And revolutions are independent movements, and due to the phenomenon when the rotation changes to revolution, the action and the reaction become a right angle. To obtain the movement of the rotating body.

すなわち、回転体の一部に加力して、加力により発生する合力の、加力方向成分と、直角方向成分との内の、直角方向成分と加力は、作用と反作用が直角となる、即ち、角度ガ直角に変換して移動する状態であり、以下角度変換移動、または直角法と称す。
角度変換する公転の範囲は、主として回転体の回転方向と逆方向に、加力方向と回転軸を結ぶ線と平行に、即ち重心に向けて加力するのではなく、主として回転体の時計回りの3〜6時の扇状の加力領域への、重心方向以外への、即ち平行方向への加力、即ち、重力下の地上では、上方向への加力で、回転体の逆行する成分のない、上方向(加力方向)移動成分と横(直角方向)移動成分の合力が発生して、加力点を仮の支点として公転する。
In other words, the action and reaction of a right-angle component and a force of the resultant force generated by the force applied to a part of the rotating body are perpendicular to each other. That is, it is a state in which the angle is converted into a right angle and moved, and hereinafter referred to as an angle conversion movement or a right angle method.
The range of revolution to convert the angle is mainly in the direction opposite to the rotation direction of the rotating body, parallel to the line connecting the force direction and the rotation axis, that is, not in the direction of the center of gravity, but mainly in the clockwise direction of the rotating body. The force applied to the fan-shaped force area at 3-6 o'clock in a direction other than the direction of the center of gravity, that is, in the parallel direction, that is, on the ground under gravity, the component reverses by the upward force. The resultant force of the upward (force direction) movement component and the lateral (right angle direction) movement component is generated and revolves with the force point as a temporary fulcrum.

公転する範囲は、回転軸と水平位置に、上方向に加力すれば、0〜90度の間を公転して、最大の公転範囲となる。すなわち、自転する回転体へ、上記の扇状領域に、重力下では、上方向に加力すれば、回転体は加力点を仮の支点として、全体が回転(公転)して角度変換移動して、発生した合力の内の逆行しない横移動成分により横移動する。  The revolving range is the maximum revolving range by revolving between 0 and 90 degrees if an upward force is applied to the rotation axis and the horizontal position. In other words, if an upward force is applied to the above-mentioned rotating area in the fan-shaped region under gravity, the rotating body rotates (revolves) as a temporary fulcrum as a temporary supporting point, and undergoes an angle conversion movement. The horizontal movement is caused by the non-reverse horizontal movement component of the generated resultant force.

したがって、回転体の内径、外径を問わず、回転体の主として上記扇状領域へ上方向に加力することにより、自転する回転体の上記領域に加力した、加力点を公転軸として公転して、上記領域であれば、加力により発生する合力の、加力方向成分と、直角方向成分との比率は変わるが、公転が発生して、回転体全体が回転することを意味する。  Therefore, regardless of the inner diameter and outer diameter of the rotating body, by applying an upward force mainly to the fan-shaped area of the rotating body, the revolving axis is revolved with the applied point applied to the above-mentioned area of the rotating body rotating. In the above region, the ratio of the applied force component and the perpendicular component of the resultant force generated by the applied force changes, but it means that revolution occurs and the entire rotating body rotates.

すなわち、自転する回転体は、回転軸と加力方向とを結ぶ線と平行に、即ち、回転軸方向以外の方向に、上記領域に加力することにより、公転して、重力下では90度まで公転して重力で元の位置に落下し、無重力下では90度で落下することなく、次の自転、あるいは公転の始点となる。  That is, the rotating body that rotates is revolved by applying a force to the region in parallel to the line connecting the rotation axis and the direction of the force, that is, in a direction other than the direction of the rotation axis, and is 90 degrees under gravity. It revolves until it falls to its original position under gravity and becomes the starting point of the next rotation or revolution without falling at 90 degrees under zero gravity.

また、回転軸と加力点間の距離を次々と長くして、加力棒を形成すれば、公転円も次々と発生して、0〜90度の範囲内で公転円が次々と連続状態となって角度変換して移動できて、横移動が可能となり、課題を解決できる。  Also, if the distance between the rotating shaft and the applied point is increased one after another to form an applied rod, revolving circles are generated one after another, and the revolving circles are continuously in a range of 0 to 90 degrees. Thus, the angle can be changed and moved, and the lateral movement becomes possible and the problem can be solved.

重力下の地面等の対象上を移動し、あるいは無重力下の加力で移動する回転体による角度変換移動において、上記領域内に、上方向または回転軸以外の平行方向(以下上方向または回転軸以外の平行方向を、上方向と称す)に加力した結果、発生する公転円で、加力位置により、上、横方向の移動成分の比率は変わるが、回転体の回転方向の3〜6時の間の扇状領域に上方向に加力することにより、直接対象に接して、あるいは直接接せず公転して、あるいは無重力下では加力して、加力点を形成することにより、加力点が次々と表れることにより、公転は0〜90度の制限内で公転が次々と発生することにより、その制限を受けず、  In angle conversion movement by a rotating body that moves on an object such as the ground under gravity, or moves under the force of weightlessness, in the above area, the upper direction or a parallel direction other than the rotation axis (hereinafter referred to as the upper direction or the rotation axis) As a result of applying an additional force to the other parallel direction, the revolving circle is generated. As a result, the ratio of the upward and lateral movement components varies depending on the applied position, but the rotational direction of the rotating body is 3-6. By applying an upward force to the fan-shaped area during the time, the force points are formed one after the other by forming a force point by touching the object directly or revolving without touching directly or by applying force under zero gravity. By appearing, the revolution is not subject to the limitation by the occurrence of one revolution after another within the limit of 0-90 degrees,

また無重力下における、加力、あるいは互いの反作用を相殺して移動する、対の回転体の移動で、最大の角度変換を求めるための、加力点を円周または外径に設けることにより、回転軸と水平な受け部の形成が不要となり、無回転部分の受け部が不要となる等、構造の簡素化が可能となり、 回転体の公転範囲は0〜90度の範囲であるが、棒高跳びの棒を次々と長さを変えて繰り出すに等しい、公転軸と加力点間を次々と長く変化することにより、そのたびごとに新たな公転の始点となって公転が行われて、0〜90度の公転範囲の範囲内で公転円を次第に大きくして、公転移動して、真円の180度の半円の公転範囲、あるいはアンモナイト貝殻状(渦巻き状)等では、それ以上の領域の利用が可能となって公転移動に資する。  In addition, rotation is performed by providing a force point on the circumference or outer diameter to obtain the maximum angle conversion in the movement of a pair of rotating bodies that move by canceling the applied force or mutual reaction under zero gravity. It is not necessary to form a receiving part that is parallel to the shaft, and the receiving part of the non-rotating part is not required, which makes it possible to simplify the structure, and the revolution range of the rotating body is in the range of 0 to 90 degrees. By changing the length between the revolution axis and the applied point one after another, it is equivalent to paying out the rod one after another by changing the length one after another. If the revolution circle is gradually enlarged within the range of revolution, and the revolution moves, the revolution range of a 180 degree semicircle or the shape of an ammonite shell (swirl) can be used beyond that. It becomes possible and contributes to revolving movement.

、真円、即ち半径が各方向に等しくても、公転軸である回転軸をずらせば、即ち偏心すれば、角度変換して合力による移動が発生することを意味する。
したがって、発生する公転円は、回転軸がずれた、円周までの円の半径が、回転軸が回転方向により変化する、公転軸(以下回転軸と称す)となり、たとえ、真円においても、回転軸(公転軸)から円周の各点までの距離は、例えば地面等の対象に接した回転体の円周に仮の支点となる加力点と、回転軸を設けた状態で回転が始まり、最初は回転軸も加力点も同一の始点にあるが、即ち、対象(地面)との接点にあったものが、回転軸は公転と同時に、対象との接点となる円周の加力点から回転軸は公転軸となった回転軸までの、両点間に距離が発生して変化して、即ち始点位置から公転につれて、回転軸と加力点間の距離は順次長くなって、加力点の頂上の半円まで順次長くなって、角度変換移動する。
This means that even if the true circle, that is, the radius is equal in each direction, if the rotation axis that is the revolution axis is shifted, that is, decentered, the angle is converted and the movement due to the resultant force occurs.
Accordingly, the generated revolution circle is a revolution axis (hereinafter referred to as a rotation axis) in which the rotation axis is shifted and the radius of the circle to the circumference changes depending on the rotation direction, even in a perfect circle, The distance from the rotation axis (revolution axis) to each point on the circumference starts to rotate with a force point that becomes a temporary fulcrum around the circumference of the rotating body in contact with the object such as the ground and the rotation axis. First, the rotation axis and the force point are at the same starting point, that is, the one that was at the point of contact with the object (ground), but at the same time as the rotation axis revolves, The rotation axis changes with the distance between the two points to the rotation axis that became the revolution axis, that is, the distance between the rotation axis and the force point gradually increases with the revolution from the starting point position. The length gradually increases to the semicircle at the top, and the angle is changed.

例えると、棒高跳びの棒の長さを、跳びながら次々と競技者が、棒の長さを伸ばして跳び上がって、移動する状態に例えられる。
自転している回転体が、対象に落下して、対象と接すれば、回転体は重力方向の直下で対象と接する。
回転軸が中心にあれば、 摩擦による加力方向は後方となって、地上の直線法で対象上を移動する。
いま、移動する回転体に棒等で、前方に加力点を形成して、棒先が対象と接すれば、回転体は、棒先の加力点の直上に達するまで、上方向と進行方向(横方向)に移動して、落下して、自転に戻る。
For example, the length of a pole vaulting rod can be compared to a state in which a competitor jumps and jumps while extending the length of the rod.
When the rotating rotator falls on the object and comes into contact with the object, the rotator comes into contact with the object immediately below the direction of gravity.
If the axis of rotation is at the center, the direction of force applied by friction is backward, and the object moves on the ground using the straight line method on the ground.
Now, if a moving point is formed on the moving rotating body with a stick or the like, and the tip of the stick touches the target, the rotating body will move upward and forward (sideways) until it reaches directly above the point of application of the stick. Direction), fall and return to rotation.

公転する回転体が棒先の直上に達するまで、回転体は棒先を後方に蹴ることは、条件が変わらない限り、できない。
その結果、加力方向が後方でなく、上下であり、時計回りに3〜6時の扇状領域で、回転軸方向と平行に、即ち回転軸方向以外に加力すれば、回転体の公転範囲は0〜90度を最大とする、公転範囲となる。
Until the revolving rotator reaches directly above the rod tip, the rotator cannot kick the rod tip backward unless the conditions change.
As a result, the revolving range of the rotating body is obtained when the force is applied not in the rear but up and down, and in the fan-shaped region in the clockwise direction at 3 to 6 o'clock in parallel with the rotation axis direction, that is, in the direction other than the rotation axis direction Is the revolution range where 0 to 90 degrees is the maximum.

例えると、ステッキ、棒高跳びの棒の長さが、次々と変化する公転円に等しく、アンモナイトの貝殻のように、あるいはロールパンのように、渦巻き状であれば、回転軸に対して、順次半径が大きくなる等の形状であれば、原状(加力点の始点)に復帰して繰り返すまで、真円のように公転円の2分の1等の制限は解消する。、  For example, if the length of a stick or pole vaulting rod is the same as the revolving circle that changes one after another, and if it is spiral like an ammonite shell or a roll, the radius will increase sequentially relative to the axis of rotation. In the case of a shape such as a larger shape, the limit of half of the revolution circle, such as a perfect circle, is removed until it returns to the original state (starting point of the applied point) and repeats. ,

すなわち、見かけ上各方向の半径が等しい円であっても、回転軸をずらすことにより、対象に対して、荷重点は直下でも、駆動する回転軸(以下駆動軸を回転軸と称す)は異なり、回転につれて半径が異なる、回転軸を兼ねた駆動軸が公転軸となって公転円を描いて、回転して、移動する回転軸(駆動軸又は公転軸)が半円の頂上が対象に接するまでは後方に加力(蹴って)して移動する事なく、上方向に加力して、水平の受け部を必要としないで角度変換(公転)して移動することにより、直線法に起因する課題の一部である、地面等の対象を蹴って移動することによる、対象が滑る、動く等、対象に依拠するために生じる、不具合を防いで、求める行動がとれて、事故等を予防して、課題の一部を解決するものである。  In other words, even if the radii seem to have equal radii in each direction, the rotational axis to be driven (hereinafter referred to as the rotational axis) differs even when the load point is directly below the target by shifting the rotational axis. The drive shaft that doubles as the rotation axis becomes a revolution axis, draws a revolution circle, rotates, and the moving rotation axis (drive shaft or revolution axis) touches the top of the semicircle Due to the straight line method, it does not move by applying force (kicking) backward until it is applied, but it is applied upward, and the angle is changed (revolved) without requiring a horizontal receiving part. Preventing accidents by preventing the malfunctions caused by relying on the target, such as sliding or moving the target by kicking and moving the target such as the ground, which is part of the task to be performed Thus, a part of the problem is solved.

実施のための最良の形態Best mode for implementation

回転軸の内径、外径を問わず、真円の場合は、加力点を中心軸よりずらすことにより、初期には中心線の直下、あるいは重複する公転のための回転軸(公転軸)と加力点が、回転と同時に、支点となる、接する主として円周と、回転軸(公転軸)までの距離が変わって、回転軸は公転軸となり、加力点の頂上までの半円まで順次長くなって、0〜90度の公転の領域で、後方に蹴ることなく、公転して、、棒高跳びの棒先を次々と繰り出す形状と等しい、あるいは渦巻き状に棒先の長さの異なる棒先の棒を束ねた形状とすれば、公転する距離は、半円であれば始点への復帰の限界の、180度までの半円まで続き、渦巻き状であれば公転距離は180度を越えて延長できる。  Regardless of the inner and outer diameters of the rotating shaft, in the case of a perfect circle, the applied point is shifted from the central axis at the initial stage, so that the rotating shaft (revolving shaft) for rotation that overlaps directly below the center line or overlaps is initially added. At the same time as the rotation, the distance between the contact point, which is the fulcrum, which is the fulcrum, and the rotation axis (revolution axis) changes, the rotation axis becomes the revolution axis, and gradually increases to the semicircle up to the top of the force point. In the region of revolution of 0 to 90 degrees, revolve without kicking backward, and the rod tip of the rod tip with the same length as the shape of paying out the rod tip of the rod high jump one after another, or in a spiral shape In the case of a bundled shape, the revolving distance continues to a semicircle up to 180 degrees, which is the limit of return to the starting point if it is a semicircle, and the revolution distance can be extended beyond 180 degrees if it is spiral.

図1において、競技者1は、棒2の棒先3を、地面等の対象4について、回転方向を示す矢印5のように、点線で表す棒2′へと進み、競技者1に回転力があれば、棒2の長さを長くして、次々と前方について、頂点を次の始点として、上方向と横方向の合力となって、進む。  In FIG. 1, the athlete 1 moves the stick tip 3 of the stick 2 toward the stick 2 ′ indicated by a dotted line as indicated by the arrow 5 indicating the rotation direction with respect to the object 4 such as the ground, and the player 1 turns the turning force. If there is, the length of the rod 2 is lengthened, and the forward and forward directions are made with the apex as the next starting point and the resultant force in the upward and lateral directions.

このことは、図2に表すように、競技者を回転軸6とすれば、棒は半径7となり、棒先にあたる加力点8が連続して、加力点である前の円周を越えて、渦巻き状に円周に加力点を形成して、重力下では加力点8は対象4と上下に当接して、無重力下では下方向からの加力により、当接(以下重力下、無重力下を通じて加力と称す)と等しく加力して、接する対象4と加力点8との接点を支点として、回転体9全体が回転して、自転が公転となり、後方に支点を蹴ることなく、回転軸6と加力点8の長さの変化により、連続して角度変換して移動するもので、  As shown in FIG. 2, this means that if the competitor is the rotation axis 6, the rod has a radius of 7, and the force point 8 corresponding to the tip of the rod continues and exceeds the previous circumference that is the force point. A force point is formed in a spiral shape on the circumference, and the force point 8 abuts the object 4 in the vertical direction under gravity, and a force (from below under gravity and under zero gravity) due to the force from below in weightlessness. The rotation body 9 rotates as a whole with the contact point between the contact point 4 and the force point 8 as a fulcrum, and the rotation is revolved without causing the fulcrum to be kicked backward. By changing the length of 6 and the force point 8, the angle is continuously converted and moved.

即ち、回転体の、回転方向の時計回りに回転体の3時から6時までの間の扇状領域に、加力する方向が、回転軸方向ではなく、回転軸方向と平行に加力すべく、内径、外形、円周を問わず、扇状領域内の適宜位置に加力点を形成して、回転軸の回転により、対象と接する加力点が仮の支点となって、上方向に、または無重力下では回転軸方向と平行に加力して発生する、上方向、または加力方向の移動成分と直角方向の移動成分の合力の内の、横(直角方向)移動成分により移動して、回転軸と加力点間の距離を、回転体の回転軸と加力点間の距離の限界まで、加力点を移動して、発生する横(直角方向)移動成分で移動して、回転軸および加力点が元の始点に復帰して、同じ動作を繰り返して移動するもので、公転の0〜90度の任意の範囲の繰り返しが得られる。  That is, the direction in which the force is applied to the fan-shaped region between 3 o'clock and 6 o'clock of the rotating body in the clockwise direction of the rotating body is not parallel to the rotating shaft direction but to be applied parallel to the rotating shaft direction. Regardless of the inner diameter, outer shape, or circumference, a force point is formed at an appropriate position in the fan-shaped region, and the force point in contact with the object becomes a temporary fulcrum by the rotation of the rotating shaft, or upward, or weightless Below, generated by applying a force parallel to the rotation axis direction, and rotating by a lateral (right-angled) moving component of the upward direction or the resultant force of the moving component in the applied direction and the moving component in the perpendicular direction. Move the force point between the axis and the force point to the limit of the distance between the rotating shaft and the force point of the rotator, move with the generated lateral (perpendicular direction) moving component, and rotate the shaft and force point. Will return to the original starting point and repeat the same movement to move to any range of 0 to 90 degrees of revolution. Repetition is obtained.

すなわち、棒高跳びのように、一点の加力点の場合は、一点を支点として公転し、図2の場合のように連続して加力点が形成された場合は、その最長の限界まで、連続して公転して、角度変換して移動するものである。
まとめると、回転体の、回転方向の時計回りに3時から6時までの間の、扇状領域内の適宜位置に加力点を形成して、回転軸と加力点間の距離を、加力点を移動して変化して、回転軸の回転により、対象と接する加力点が、回転軸方向と平行な加力となって、加力点を仮の支点として公転して、発生する合力の内の、直角方向の移動成分、又は合力成分により移動する構造および方法の回転体による角度変換移動方法および移動体である。
That is, in the case of a single point, such as a pole vault, it revolves around one point as a fulcrum, and when the point is continuously formed as in the case of FIG. 2, it continues until the longest limit. It revolves and moves with angle conversion.
In summary, a force point is formed at an appropriate position in the fan-shaped region between 3 o'clock and 6 o'clock in the rotation direction of the rotating body, and the distance between the rotation axis and the force point is determined as the force point. Due to the rotation and rotation of the rotating shaft, the applied point that contacts the target becomes an applied force parallel to the direction of the rotating shaft, and the applied point is revolved as a temporary fulcrum. An angle conversion moving method and a moving body by a rotating body having a structure and a method of moving by a moving component in a perpendicular direction or a resultant force component.

この際、加力方向は、時計回りに3〜6時の間の扇状領域の上方向または、重心方向と平行方向であるから、対象が滑る、動いている等の状態であっても、上下に作用反作用が成り立てば、公転ができて、角度変換して移動ができる。  At this time, since the direction of the force is the upward direction of the fan-shaped region between 3 and 6 o'clock in the clockwise direction or the direction parallel to the direction of the center of gravity, even if the target slides or moves, it acts up and down. If the reaction is established, it can revolve and move with angle conversion.

図3において、円形の回転体9は、中央に穿設した長穴状の回転軸6の移動部10の中央で回転軸6により、対象4を後方へ蹴って回転して移動しているが、対象4が、滑る等の不具合により、移動に支障を来す場合等、必要に応じて移動部10内を、回転軸6を回転軸6′にずらすことにより、直下で接する加力点8は回転軸6の前方となって、ずれた回転軸6′が加力点の後方となって、相対的に上下方向の加力が表れ、その分が合力を発生して、直角の横移動成分が生じる。  In FIG. 3, the circular rotating body 9 is moved by kicking the object 4 backward by the rotating shaft 6 at the center of the moving portion 10 of the long hole-shaped rotating shaft 6 drilled in the center. When the object 4 is hindered to move due to a problem such as slipping, the force point 8 which is in direct contact with the moving part 10 is shifted to the rotating shaft 6 'within the moving unit 10 as necessary. In front of the rotation shaft 6, the displaced rotation shaft 6 ′ is behind the force application point, and a relatively vertical force appears, and a resultant force is generated, resulting in a perpendicular lateral movement component. Arise.

この移動成分が発生する位置は、回転体9の矢印5方向の回転として、ずれた回転軸6が、回転して上端に来る、左半分の間で、回転軸6′の上昇とともに、加力点8との間は順次伸びて、回転軸6は公転して、角度変換して移動して、実施例1では、回転軸と加力点の距離を加力点を移動して、公転を得ており、本実施例2では、回転軸を移動して、両者間の距離を変化して、公転を得て移動するものである。
まとめると、地面等の対象により移動する回転体の、中央に回転軸の移動部を設置して、中央の回転軸により、対象を後方へ蹴って回転して移動する回転体において、回転体の中央に設置した移動部の、中央の回転軸を移動部によりずらすことにより、直下にあった加力点は、回転軸の前方となって、ずれた回転軸が、加力点の後方となって、上下方向の加力となり、公転して合力が発生して、横移動成分が生じ、ずれた回転軸が、公転して上限に来る、半円の間で、回転軸の上昇とともに、加力点との間の距離は順次変化して、加力点が地面等の対象と、直接接して公転して、角度変換して移動する構造および方法の回転体による角度変換移動方法および移動体である。
The position where this moving component is generated is that the rotational axis 6 is rotated as the rotation of the rotating body 9 in the direction of the arrow 5 and between the left half where the rotational axis 6 rotates and comes to the upper end. In the first embodiment, the rotation axis 6 is revolved and moved by changing the angle. In the first embodiment, the distance between the rotation axis and the force point is moved between the force points to obtain the revolution. In the second embodiment, the rotation axis is moved, the distance between the two is changed, and the revolution is obtained to move.
In summary, in the rotating body that moves by rotating the rotating shaft at the center of the rotating body that moves according to the object such as the ground, and that moves by kicking the object backward by the rotating shaft at the center, By shifting the central rotation axis of the moving unit installed in the center by the moving unit, the force point that was directly below becomes the front of the rotation axis, the shifted rotation axis becomes the rear of the force point, The force is applied in the vertical direction, revolves to generate a resultant force, a lateral movement component is generated, and the displaced rotation axis revolves and reaches the upper limit. The angle conversion moving method and the moving body by the rotating body of the structure and method in which the distance between is changed sequentially and the applied point revolves directly in contact with the object such as the ground and moves by converting the angle.

回転軸6は上端に達して、下降する際の加力点8は、回転軸8の後方となり、地面等の対象4を、90度ずれて、後方に蹴って移動して、加力方向が移動方向と同方向となり、いわゆる地上の直線法となる。
上記のいずれの実施例においても、回転体の公転による直角の作用反作用となる位置は、対象に対して、回転体の回転方向の、回転軸の前方、即ち回転方向の回転軸の前方に加力点が存在する間であり、棒高跳びの棒先と等しく、回転体の時計回りの3〜6時の間への、上方向への加力を次々と支点を変化して、あるいは回転軸を変化して、公転して、角度変換して、直角の移動成分で移動するものである。
The rotating shaft 6 reaches the upper end, and the applied force point 8 when descending is behind the rotating shaft 8, and the target 4 such as the ground is shifted 90 degrees and kicked backward to move, and the direction of the applied force moves. It becomes the same direction as the direction, which is a so-called straight line method on the ground.
In any of the above-described embodiments, the position at which a right-angled action and reaction is caused by the revolution of the rotating body is applied to the object in front of the rotating shaft in the rotating direction of the rotating body, that is, in front of the rotating shaft in the rotating direction. While the force point is present, it is the same as the tip of the pole vault, and the upward force applied between 3 to 6 o'clock in the clockwise direction of the rotating body is changed one after another, or the rotating shaft is changed. , Revolve, change angle, and move with right-angle moving component.

したがって、地上では利用可能な右半円の位置エネルギーは、無重力下では、利用できない。
回転体の回転軸をずらすことにより、中央で回転軸を回転すれば、対象に対して、従来の横方向の後方に蹴る、移動方向となり、回転軸をずらすことにより、相対的に、直下の荷重点に対して、駆動の回転軸()がずれて、回転体全体が回転して、後方への加力ではなく、上下方向への加力成分が発生して、角度変換して移動するもので、加力方向が変わることにより、摩擦による移動とならず、上下方向の加力となって、対象への依存方向が、横方向から上方向に変化して移動する、構造および方法の回転体による角度変換移動方法および移動体である。
Therefore, the potential energy of the right semicircle available on the ground cannot be used under zero gravity.
If the rotating shaft is rotated at the center by shifting the rotating shaft of the rotating body, the moving direction is kicked rearward in the conventional lateral direction with respect to the object, and by moving the rotating shaft, it is relatively directly below. The rotational axis () of the drive is shifted with respect to the load point, and the entire rotator rotates to generate a force component in the vertical direction instead of the force applied to the rear, and move by converting the angle. In the structure and method, since the direction of the force is changed, the movement is not caused by friction but the force is applied in the vertical direction and the direction of dependence on the object is changed from the lateral direction to the upward direction. An angle conversion moving method using a rotating body and a moving body.

図4、5、は、実施例2の、移動する駆動軸である公転軸を、回転体9の半円毎に回転体9の中心を対称に設置したもので、いま下端の公転軸の回転軸6を回転すると、全体が公転して、接地する直下が、回転体にかかる荷重点であるとともに、公転のための回転軸6の加力点8となって公転するもので、回転軸6は回転方向の左半分の上端の直上に達するまで、回転方向に対して、加力点8の後方となって公転するもので、直上を越えると、回転体9の左半円は上下方向の加力成分がなく、後方へ蹴る加力方向が90度ずれた前後の横下の公転となって、対象を蹴る移動となる。
図6は上述本願原理による人力による角度変換移動を例示すもので、二つの回転体9、9間を、中心軸14により連結されており、中間に支持部11を回動可能に設置して、上部にサドル12を形成している。
サドル12に、人が腰掛けると荷重は、中心軸14により対象4との直下の接点にかかる。
FIGS. 4 and 5 show the revolution shaft, which is a moving drive shaft, according to the second embodiment, in which the center of the rotation body 9 is symmetrically arranged for each semicircle of the rotation body 9, and the rotation of the revolution shaft at the lower end now. When the shaft 6 is rotated, the whole revolves, and immediately below the ground is a load point applied to the rotating body and revolves as a force point 8 of the rotating shaft 6 for revolution. Until it reaches just above the upper end of the left half of the rotation direction, it revolves behind the force point 8 with respect to the rotation direction, and beyond that, the left half circle of the rotating body 9 is applied in the vertical direction There is no component, and the direction of the force applied to kick backwards is 90 degrees forward and backward revolving, resulting in a kicking movement.
FIG. 6 shows an example of the angle conversion movement by human power according to the principle of the present application described above. Two rotating bodies 9 and 9 are connected by a central shaft 14 and a support portion 11 is rotatably installed in the middle. The saddle 12 is formed on the top.
When a person sits on the saddle 12, the load is applied to a contact point directly below the object 4 by the central shaft 14.

片側の回転体9の適宜位置に駆動軸13を設けて、中心軸14を対称に、他方の回転体9に駆動軸13を設置して、両側の回転体9にペダル15を連結棒15′で、公転の駆動軸13に連結する。
いま、サドル12に人が腰掛けて、ペダル15を、回転体の上から下に回動すると、荷重点の後方にある回転軸6は、直下の荷重点と上下に又は重なって在る加力点と、回動につれて両者間の距離は、駆動軸13が、相対的に後になるため、伸びる。
A drive shaft 13 is provided at an appropriate position of the rotary body 9 on one side, the central shaft 14 is symmetrical, the drive shaft 13 is installed on the other rotary body 9, and a pedal 15 is connected to the rotary body 9 on both sides. Then, it is connected to the revolving drive shaft 13.
Now, when a person sits on the saddle 12 and the pedal 15 is rotated from the top to the bottom of the rotating body, the rotating shaft 6 behind the load point is applied to the load point directly below or overlapping the load point directly below. And the distance between the two increases as the drive shaft 13 is relatively behind as it rotates.

すなわち、荷重点は直下で対象4と接しているが、駆動軸13の移動により、駆動軸13が半円の頂上に達するまで、即ち、ペダルが下となるまで、回転体9は上下方向の加力を受けて、対象を後方に蹴ることなく、押さえ付けて、対象に加えられる反作用で、上昇移動するもので、加力方向が横方向でなく、対象の反作用で上方向となって、移動するものである。
すなわち、回転体は円形でも、回転軸が円周の中心にないため、円周までの半径が、半円で異なり、そのために、半円の頂上までは、実施例1の棒高跳びの状態となり、残りの半円は下端の始点となって位相が90度ずれた、地上の直線法となり、両側の各々の加力によって、回転体全体が半円ごとに公転する。
これをまとめると、円形の回転体の回転軸以外の任意の位置に、駆動軸を設置して、対象と接する直下の荷重点を重複する駆動軸の加力点として、駆動軸を回転することにより、回転方向に対して駆動軸は、荷重点と回転軸を結ぶ線の後方となる位置に達して、駆動軸は公転して、即ち公転が始まり、回転体の最大の半径に達するまで、駆動軸と加力点間の距離が変化することにより公転が、連続して、結果として、半円毎の公転が連続して角度変換して、発生する合力の内の、直角方向の移動成分により、移動する構造および方法の回転体による角度変換移動方法および移動体である。
That is, the load point is in direct contact with the object 4, but the rotary body 9 is moved in the vertical direction until the drive shaft 13 reaches the top of the semicircle by the movement of the drive shaft 13, that is, until the pedal is lowered. In response to the applied force, pressing the object backward without pressing it, it is a reaction that is applied to the object and moves up, the force direction is not lateral, but the object's reaction is upward, It is something that moves.
That is, even if the rotating body is circular, since the rotation axis is not at the center of the circumference, the radius to the circumference is different in the semicircle, and therefore, the top of the semicircle is in the state of the pole vault of Example 1, The remaining semicircle becomes the starting point of the lower end and becomes a linear method on the ground with a phase shift of 90 degrees, and the entire rotating body revolves for each semicircle by the applied forces on both sides.
To summarize, by installing the drive shaft at an arbitrary position other than the rotation shaft of the circular rotating body and rotating the drive shaft with the load point directly below the target as the force point of the overlapping drive shaft, The drive shaft with respect to the rotation direction reaches the position behind the line connecting the load point and the rotation shaft, and the drive shaft revolves, that is, until the revolution starts and reaches the maximum radius of the rotating body. As the distance between the axis and the applied point changes, the revolution continues, and as a result, the revolution of each semicircle continuously undergoes an angle conversion, and due to the moving component in the perpendicular direction of the resultant force, An angle conversion moving method and moving body by a rotating body of a moving structure and method.

従来の移動方法においては、後方に蹴って移動を得るため、対象に対して、重力による荷重点と、後方に蹴る加力点、駆動点は、回転軸に対して重複して、あるいは重力で直下となっていたが、本願では、荷重は直下の荷重点となり、加力点は、荷重点に重なって在り、回転軸と駆動軸は重複して、あるいは別個に存在している形状となる。  In the conventional movement method, in order to obtain movement by kicking backward, the load point due to gravity, the force point kicking backward, and the driving point overlap with the rotation axis or directly under gravity. However, in the present application, the load is a load point immediately below, the applied point is overlapped with the load point, and the rotary shaft and the drive shaft are overlapped or separately exist.

回転体の移動に対して、後方に蹴ることなく、下方向に押さえる移動成分を含むため、対象が滑る、動いている等、対象の状態により、移動が左右されない。
また、本実施例では加力点を半円ごとの2点として、固定しているが、実施例2のように、回転軸を可動として、対象の状態に対応して、公転による移動量を増減し、あるいは3点以上の複数の駆動軸の公転位置を変えることにより、公転の移動量成分の比率を変化できる。。
Since the moving body includes a moving component that is pressed downward without kicking backward with respect to the movement of the rotating body, the movement is not affected by the state of the object such as the object slipping or moving.
In this embodiment, the force point is fixed as two points for each semicircle. However, as in the second embodiment, the rotation axis is movable, and the amount of movement due to revolution is increased or decreased according to the target state. Alternatively, by changing the revolution positions of a plurality of drive shafts at three or more points, the ratio of the revolution movement amount component can be changed. .

いずれの実施例においても、回転体は地面等の対象に接して、本願の上方向への加力、あるいは、従来の加力方法と等しい横方向の加力により、移動するものであり、
実施例2、3においては、中心軸をずらすことにより、位置エネルギーとして、右半分を、地上の重力で、従来の後方へ蹴る成分が利用できる。
また、実施例2、3のいずれにおいても、時計回りに3〜6時の加力領域ではなく、公転を得るための加力領域は、6〜9時〜12時の、回転体の左半分に対して、上方向への加力となっている。
In any of the embodiments, the rotating body is in contact with an object such as the ground, and is moved by an upward force of the present application, or a lateral force equal to the conventional force method,
In the second and third embodiments, by shifting the central axis, a conventional component of kicking the right half backward with gravity on the ground can be used as potential energy.
Moreover, in any of Examples 2 and 3, the force region for obtaining revolution is not the force region at 3 to 6 o'clock clockwise, but the left half of the rotating body at 6 to 9 o'clock to 12 o'clock On the other hand, it is an upward force.

このことは、回転体の直下の地面等対象と接する位置が、3〜6時の領域の加力点となっって、駆動軸に加えられる上方向への力は、自転力と公転力とを同時に加える状態となることを意味している。
また、地上においては、無重力下では、通用しない、重力により発生する、摩擦による横方向の加力により発生する、合力の横、下方向成分の内の横移動成分による、地上の直線法、あるいは上方向の加力による上、横方向の移動成分による横移動の直角法による回転体の移動であり、実施例2、3では、その両方法を利用しての、重力下でのみ、有効な、地上の直線法の両方法を交互に、あるいは同時に利用して、また自転と公転に対する回転体への加力方向が、回転方向の3〜6時間の領域への公転と同時に、回転軸方向への加力を除く、6〜9時間への自転への加力とが、実施例3では、同時に発生する、状態を利用した移動方法の構造および方法の回転体による角度変換移動方法および移動体を表している。
This means that the position in contact with the object, such as the ground directly below the rotating body, is the applied point in the region of 3 to 6 o'clock, and the upward force applied to the drive shaft is the rotation force and the revolution force. It means that it is in a state to be added at the same time.
Also, on the ground, it does not work under zero gravity, it is generated by gravity, it is generated by lateral force due to friction, the lateral force of the resultant force, the lateral movement method of the downward component, or the ground linear method, or It is the movement of the rotating body by the right angle method of the lateral movement by the upward moving force and the lateral movement component. In the second and third embodiments, it is effective only under gravity using both methods. The ground linear method is used alternately or simultaneously, and the direction of force applied to the rotating body for rotation and revolution is in the direction of the rotation axis simultaneously with the revolution in the region of 3 to 6 hours of the rotation direction. In Example 3, the force applied to the rotation for 6 to 9 hours, excluding the force applied to the motor, is generated at the same time. The structure of the moving method using the state and the angle conversion moving method and the moving by the rotating body of the method Represents the body.

また実施例3において、駆動軸は加力点となる、直下の接点の後方となる。
このことは、円周等に加力して、自転を得る、時計回りに6時の位置を越えて、9時の方向の自転に加力することと等しく、加力点の存在により、加力点による公転と同時に自転を得ている状態の、同じ上方向の加力による、角度変換移動の構造および方法の回転体による角度変換移動方法および移動体であり、円周速度を越えて、回転軸方向と平行に、あるいは円周の接線方向に加力して、自転を得るとともに公転を得て移動するものである。
In the third embodiment, the drive shaft is behind the contact point immediately below, which is the applied point.
This is equivalent to applying force to the circumference, etc., to obtain rotation, exceeding the 6 o'clock position in the clockwise direction, and applying force to 9 o'clock direction rotation. The angle conversion movement method and moving body by the rotating body of the angle conversion moving structure and method by the same upward force, with the rotation at the same time as the revolution by Applying force parallel to the direction or in the tangential direction of the circumference, it acquires rotation and revolves and moves.

また、前述のように、重力下において重力に抗して、上方向の移動成分により、発生する位置エネルギーも、落下することによる力として、自転エネルギー、あるいは公転が90度ずれた、地上の直線法として利用できて、損失とならない。
上記各実施例を要約すると、自転する回転体の、回転方向の、時計回りに3時から6時の間の扇状領域に、回転軸方向を除く、回転軸と加力方向を結ぶ線と平行に、即ち接線方向に加力すべく、回転体の内径、外径、円周を問わず、加力点を対象に直接接して、又は受け部を介する等して間接的に形成して、加力点を支点として、回転体全体が回転することにより、すなわち公転して、発生した加力方向の移動成分と、直角方向の移動成分の内の、主として重力下の地上では直角方向の、すなわち横方向の移動成分により、移動して、無重力下では二方向成分により、又は直角方向成分により移動する構造および方法の回転体による角度変換移動方法および移動体である。
In addition, as described above, the potential energy generated by the upward moving component against gravity under gravity is also a straight line on the ground where the rotation energy or revolution is shifted by 90 degrees as a force caused by falling. It can be used as a law and does not cause a loss.
To summarize each of the above embodiments, the rotating body of the rotating body, in the direction of rotation in the clockwise direction from 3 o'clock to 6 o'clock, in parallel to the line connecting the rotation axis and the force direction, excluding the rotation axis direction, In other words, in order to apply force in the tangential direction, regardless of the inner diameter, outer diameter, and circumference of the rotating body, the applied point is formed in direct contact with the object or indirectly through the receiving portion, etc. As a fulcrum, when the entire rotating body rotates, that is, revolves, the generated force component in the direction of force and the component in the right-angle direction, which are mainly perpendicular to the ground under gravity, that is, in the lateral direction. An angular conversion moving method and moving body by a rotating body of a structure and method that moves by a moving component, moves by a two-way component under zero gravity, or moves by a right-angle component.

すなわち、地上等重力下においては、重力のために主として対象と直接、あるいは間接に接して加力点を形成して、上下に当接して加力して、あるいは対象に反作用をおよぼし、無重力下では、点あるいは複数点に加力して、同様に機能せしめて公転をえるもので、自転する回転体の回転軸以外の内径円周外径の任意の位置に、回転軸方向と平行に加力して、回転方向の加力であれば、自転力として用いて、逆回転方向であれば、加力点を仮の支点として公転して、公転により発生する合力の内の直角方向の移動成分により、直角方向に移動して、あるいは無重力下では発生した二方向の合力の移動成分で移動して、あるいは加力が複数の場合、自転と公転を同時に発生して、発生した公転による合力の内の直角方向の移動成分により、あるいは無重力下では二方向成分により移動する回転体による角度変換移動方法および移動体である。  In other words, under gravity such as the ground, a force point is formed mainly by direct or indirect contact with the object due to gravity, and is applied by contacting the top and bottom or exerting a reaction on the object. Applying force to a point or multiple points and causing them to revolve in the same way, applying force parallel to the rotation axis direction at any position of the inner diameter circumference outside the rotation axis of the rotating body that rotates If the force is applied in the rotational direction, it is used as the rotational force, and if it is in the reverse rotational direction, it revolves around the applied point as a temporary fulcrum, and the vertical component of the resultant force generated by the revolution In the case of moving in a right-angle direction or under zero gravity, it is moved by the moving component of the resultant force in two directions, or when there are multiple applied forces, rotation and revolution occur simultaneously, Due to the right-angle moving component of Is under zero gravity is the angle convert moving method and mobile by rotation body that moves by a two directional component.

前願の2005−112718号においては、回転軸と水平な位置での加力を主体として、本願原理の説明を例示しているが、本願では、重力により直下となる、荷重点であっても、回転軸が回転方向の後方に公転軸あるいは駆動軸がずれることにより、水平な受け部の必要がなく、アンモナイト状、あるいは円形でも上下方向の加力を形成できることを証明し、回転体の荷重に、無回転部分の荷重を利用して、前願の直接対象に接しないための、公転する回転体のみの重量(質量)による移動ではなく、回転体にかかる重量(質量)が回転要素として利用可能となり、また、対象の状態に即して、後方に蹴る成分の多い直線法を併用して移動して、また、扇状の公転領域全体を対象とした、公転による角度変換移動を可能とした例示である。  In the prior application No. 2005-112718, the principle of the present application is illustrated mainly with the force applied at a position parallel to the rotation axis. However, in the present application, even if the load point is directly below due to gravity. It is proved that the rotating shaft can be formed in the vertical direction even in an ammonite or circular shape by eliminating the need for a horizontal receiving portion by shifting the revolving shaft or drive shaft to the rear in the rotational direction, and the load on the rotating body In addition, using the load of the non-rotating part, it is not the movement by the weight (mass) of only the rotating body that revolves so that it does not contact the direct object of the previous application. It can be used, and it can move along with the linear method with many components kicking backwards according to the state of the target, and it can also perform angle conversion movement by revolution for the whole fan-shaped revolution area Is an example

本願は、従来、物体の移動は、すべてが直線の作用反作用でなされるものと、決められてきたが、回転体の移動には、その他に、直角の作用反作用となる移動方法が存在することを、発見して、吾人の日常に深く関わり、爆発等より、直接力を受けて移動するロケット等の物体移動以外の、地面等の対象に依拠して移動するものは、生物、無生物を含む、すべてが回転により移動する現象事実に基づく、回転体による移動部分の発明出願である。  In the present application, it has been determined that all the movement of an object is performed by a linear reaction and reaction. However, there is another movement method that causes a perpendicular reaction and reaction in the movement of a rotating body. The thing which moves depending on the object such as the ground other than the movement of the object such as the rocket that moves by receiving direct force from the explosion etc. , An invention application of a moving part by a rotating body based on the fact that everything moves by rotation.

物体の移動による、事故、危険性等は、すべて対象に依拠して、主として後方に蹴ることにより、移動することに起因している。
本願は、作用と反作用が直角となる移動方法のために、依拠する対象に対して、摩擦を必要としない移動方法となり、重力下、無重力下を問わず、安全な移動方法となり、車両の脱線事故等も、未然に防ぐことが可能となり、また力の取り出し方も、直線の作用反作用とならないために、発生する力のすべてを利用することが可能で、温暖化等の根本原因の一つである力の取り出し方も変わり、解決あるいは先延ばしが可能となる本願は、その実用化の端緒である。
Accidents, dangers, and the like due to the movement of the object all depend on the object and move mainly by kicking backward.
This application is a moving method that does not require friction for the object to be relied upon because of the moving method in which the action and the reaction are at right angles, and it becomes a safe moving method regardless of gravity or weightlessness, and derailment of the vehicle. Accidents can be prevented in advance, and since the force extraction method does not become a linear action reaction, it is possible to use all of the generated force, which is one of the root causes of global warming etc. The method of taking out the force is also changed, and the present application, which can be solved or postponed, is the beginning of its practical application.

棒高跳びの状態による横移動の模式図。The schematic diagram of the horizontal movement by the state of pole vault. 渦巻き状の加力点の伸長状態を表す模式図。The schematic diagram showing the expansion | extension state of a spiral shaped force point. 回転軸がずれることにより、加力点との距離が変化する状態を表す模式図。The schematic diagram showing the state from which a distance with an applied point changes, when a rotating shaft shifts | deviates. 半円を合わせた円形の回転体で、2点の回転軸を設けて、連続して公転する模式図。The schematic diagram which revolves continuously by providing the rotating shaft of 2 points | pieces with the circular rotary body which match | combined the semicircle. 図4の側面図。The side view of FIG. 人力による実用に供する実証装置の見取り図。A sketch of a demonstration device for practical use by human power.

符号の説明Explanation of symbols

1. 競技者。
2.2′棒。
3. 棒先。
4. 対象。
5. 回転方向の矢印。
5′ 中心線
6.6′回転軸。
7. 半径。
8 加力点。
9. 回転体。
10 長穴。
11. 支持部。
12. サドル。
13 駆動軸。
14. 中心軸。
15. ペダル。
15′ 連結棒。
1. Athlete.
2.2 'bar.
3. Stick tip.
4). Subject.
5). Rotation direction arrow.
5 'Centerline 6.6' axis of rotation.
7). radius.
8 Force point.
9. Rotating body.
10 Slotted hole.
11. Support part.
12 saddle.
13 Drive shaft.
14 Central axis.
15. pedal.
15 'connecting rod.

Claims (5)

回転体の、回転方向の時計回りに3時から6時までの間の、扇状領域内の適宜位置に加力点を形成して、回転軸と加力点間の距離を、加力点を移動して変化して、回転軸の回転により、対象と接する加力点が、回転軸方向と平行な加力となって、加力点を仮の支点として公転して、発生する合力の内の、直角方向の移動成分又は合力成分により移動する構造および方法の請求項1の回転体による角度変換移動方法および移動体。  Form a force point at an appropriate position in the fan-shaped region between 3 o'clock and 6 o'clock in the rotation direction of the rotating body, and move the force point between the rotation axis and the force point As a result of the rotation of the rotating shaft, the applied point in contact with the object becomes an applied force parallel to the direction of the rotating shaft, and the applied point is revolved as a temporary fulcrum. The angle conversion movement method and moving body by the rotating body of Claim 1 of the structure and method of moving by a moving component or a resultant force component. 地面等の対象により移動する回転体の、中央に回転軸の移動部を設置して、中央の回転軸により、対象を後方へ蹴って回転して移動する回転体において、回転体の中央に設置した移動部の、中央の回転軸を移動部によりずらすことにより、直下にあった加力点は、回転軸の前方となって、ずれた回転軸が、加力点の後方となって、上下方向の加力となり、公転して合力が発生して、横移動成分が生じ、ずれた回転軸が、公転して上限に来る、半円の間で、回転軸の上昇とともに、加力点との間の距離は順次変化して、加力点が地面等の対象と、直接接して公転して、角度変換して移動する構造および方法の請求項2の回転体による角度変換移動方法および移動体。  Install a moving part of the rotating shaft in the center of the rotating body that moves according to the object such as the ground, and install it at the center of the rotating body in the rotating body that moves by kicking the object backward using the central rotating shaft. By shifting the central rotation axis of the moving part by the moving part, the force point that was directly below becomes the front of the rotation axis, and the shifted rotation axis becomes the rear of the force point, so that It becomes an applied force, revolves to generate a resultant force, a lateral movement component is generated, and the displaced rotation axis revolves and reaches the upper limit. 3. The angle conversion moving method and the moving body by the rotating body according to claim 2, wherein the distance is changed sequentially, and the applied point revolves in direct contact with an object such as the ground and moves by converting the angle. 円形の回転体の回転軸以外の任意の位置に、駆動軸を設置して、対象と接する荷重点を重複する駆動軸の加力点として、駆動軸を回転することにより、回転方向に対して駆動軸は、荷重点と回転軸を結ぶ線の後方となる位置に達して駆動軸は公転して、回転体の最大の半径に達するまで、駆動軸と加力点間の距離が変化することにより、半円毎の公転が連続して、角度変換して、発生する合力の内の、直角方向の移動成分により、移動する構造および方法の請求項2または請求項3の回転体による角度変換移動方法および移動体。  Drive in the rotational direction by installing the drive shaft at an arbitrary position other than the rotary shaft of the circular rotating body and rotating the drive shaft with the load point in contact with the target as the force point of the overlapping drive shaft The shaft reaches the position behind the line connecting the load point and the rotation axis, the drive shaft revolves, and the distance between the drive shaft and the force point changes until the maximum radius of the rotating body is reached. 4. A method and an angle conversion movement method using a rotating body according to claim 2 or 3, wherein the rotation of each semicircle is continuously converted by an angle conversion, and the resultant force is moved by a movement component in a perpendicular direction. And moving body. 自転する回転体の、回転方向の、時計回りに3時から6時の間の扇状領域に、回転軸方向を除く、回転軸と加力方向を結ぶ線と平行に、加力すべく、加力点を対象に直接接して、又は間接的に形成して、加力点を支点として、回転体全体が回転することにより公転して、角度変換して発生した加力方向の移動成分と、直角方向の移動成分の内の、主として重力下の地上では、横方向の移動成分により移動して、無重力下では二方向成分により、又は直角方向成分により移動する構造および方法の請求項1または請求項2または請求項3または請求項4の回転体による角度変換移動方法および移動体。  In order to apply force to the rotating area of the rotating body in the direction of rotation in the clockwise direction between 3 and 6 o'clock, excluding the direction of the rotation axis, parallel to the line connecting the rotation axis and the force direction, Directly in contact with the object or indirectly formed, revolving by rotating the entire rotating body with the applied point as a fulcrum, and the moving component in the applied direction generated by angle conversion and the movement in the perpendicular direction Claim 1 or claim 2 or claim 2 of the structure and method wherein the component moves on a ground surface, mainly under gravity, with a laterally moving component, and moves under zero gravity with a two-way component or with a perpendicular component. An angle conversion moving method and a moving body by the rotating body according to claim 3 or 4. 自転する回転体の回転軸以外の内径円周外径の任意の位置に、回転軸方向と平行に加力して、回転方向の加力であれば、自転力として用いて、逆回転方向であれば、加力点を仮の支点として公転して、公転により発生する合力の内の直角方向の移動成分により、直角方向に移動して、あるいは発生した二方向の移動成分で移動して、あるいは加力が複数の場合、自転と公転を同時に発生して、発生した公転による合力の内の直角方向の移動成分により、あるいは二方向成分により移動する構造および方法の請求項4または請求項5の回転体による角度変換移動方法および移動体。  Applying a force in parallel to the direction of the rotation axis to any position of the outer circumference of the rotating body other than the rotation axis of the rotating body. If the force is applied in the rotation direction, it can be used as the rotation force in the reverse rotation direction. If there is, it revolves around the applied point as a temporary fulcrum and moves in the right-angle direction due to the right-angled movement component of the resultant force generated by the revolution, or moves in the generated two-way movement component, or 6. The structure and method according to claim 4 or 5, wherein when there are a plurality of applied forces, rotation and revolution occur simultaneously, and the structure and method move by a perpendicular moving component or a two-way component of the resultant force of the generated revolution. Angle conversion moving method and moving body by rotating body.
JP2007311574A 2007-11-02 2007-11-02 Angle changing and moving method by rotating body, and moving body Pending JP2009113778A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN116176721A (en) * 2023-04-25 2023-05-30 哈尔滨工业大学(深圳)(哈尔滨工业大学深圳科技创新研究院) Continuous jumping robot with adjustable jumping track

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN116176721A (en) * 2023-04-25 2023-05-30 哈尔滨工业大学(深圳)(哈尔滨工业大学深圳科技创新研究院) Continuous jumping robot with adjustable jumping track
CN116176721B (en) * 2023-04-25 2023-07-18 哈尔滨工业大学(深圳)(哈尔滨工业大学深圳科技创新研究院) Continuous jumping robot with adjustable jumping track

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