WO2018143207A1

WO2018143207A1 - Power generation device

Info

Publication number: WO2018143207A1
Application number: PCT/JP2018/002996
Authority: WO
Inventors: 日吉藤本; 豊池崎; 中村　英明; Fujiko FUJIMOTO (藤本富士子)
Original assignee: 日吉藤本; 水上彰澄; 豊池崎; 中村　英明
Priority date: 2017-02-01
Filing date: 2018-01-30
Publication date: 2018-08-09
Also published as: JP2020056311A

Abstract

Provided is a power generation device 10 in which it is possible to connect to a machine having rotation as a power source by converting gravitational force to rotational force. A power generation device 10 in which gravitational force is converted to rotational force and the converted force is used as a power source, wherein the power generation device 10 includes a mechanism for producing an imbalance by preventing gravitational equilibrium from being reached with respect to the natural law whereby gravitational equilibrium is sought, and generating rotational force that produces rotational energy due to the imbalance.

Description

Power generator

The present invention relates to a power generation device.

A typical example of equipment that converts gravity into rotational force is a water wheel.
However, since a water turbine uses water that flows down due to gravity as a power source, water must continue to flow into the water turbine. For this reason, the water as a power source was infinitely necessary.
In the present invention, the power source is only gravity, and the rotational force continues to be generated without replenishing the power source from other sources.
Moreover, it can become a more motive power source by connecting a rotary body.

The present invention is positioned as a power generation device that uses gravity as a power source, generates rotational force only by gravity, and supplies the rotational force to other devices.

Therefore, an object of the present invention is to provide a power generation device using gravity.

The present invention employs the following means.
The power generation device according to the present invention is a power generation device that converts gravity into a rotating force and uses the converted force as a power source, and is adapted to the natural law that attempts to balance gravity. And a mechanism for generating a rotational force for generating rotational energy in the imbalance.

The power generation device according to the present invention is characterized in that the power source is an imbalance caused by tilting the position of the mass point by 90 degrees with respect to the vertical direction according to the law of gravity.

The power generation device according to the present invention further includes a horizontal holding mechanism that holds the mass point in the horizontal direction according to the law of gravity, and a rotational force addition mechanism that adds an additional rotational force to the rotational force. Features.

The present invention uses the principle of a water wheel and a lever such as a seesaw as a classic method.
The present invention is characterized in that the two classical methods are used at the same time, and the rotational force generated by making the gravity applied to the mass point unbalanced is used.
In addition, regarding the portion that generates imbalance according to the present invention, since the “balance” of the natural law always occurs, the function to prevent the occurrence of the “balance” is also a feature.

According to the present invention, it can be used as a power source for equipment that requires rotation. Moreover, since the power generation device according to the present invention does not require another power source, it can be used as a power source considering the environment.

It is explanatory drawing of the generalized model of the mechanism which produces the rotational force in the case of an even-numbered mass point. It is explanatory drawing of the generalized model of the mechanism which produces the rotational force in the case of an odd-numbered mass point. It is explanatory drawing at the time of the mass point being located in the horizontal direction in the balance by gravity of the generalized model of the mechanism which produces a rotational force. In FIG. 3, it is explanatory drawing when a mass point is going to move to a perpendicular direction. It is explanatory drawing of the dynamic consideration of the generalized model of the mechanism which produces the rotational force shown in FIG.3 and FIG.4. It is a schematic diagram of a motive power generator provided with the mechanism which produces the rotational force using a stabilizer. It is explanatory drawing of the rotation direction of the transmission gear of a motive power generator. It is explanatory drawing of a stabilizer. FIG. 9 is an explanatory diagram of a state in which the stabilizer is in a natural balance in FIG. 8. It is explanatory drawing of the way of thinking of how to apply the force to a stabilizer, and the balance problem of a stabilizer. It is a front view explaining an example of the mechanism which produces a rotational force. It is sectional drawing which abbreviate | omitted a part of mechanism which produces the rotational force shown in FIG. It is explanatory drawing of the outline of the motive power generator provided with the rotational force addition mechanism. It is the front view which abbreviate | omitted a part of rotational force addition mechanism shown in FIG. It is sectional drawing which abbreviate | omitted a part of rotational force addition mechanism shown in FIG. It is an attenuation diagram in case there is no torque addition mechanism. It is an attenuation diagram in case there is a rotational force addition mechanism. It is the front view which abbreviate | omitted a part of another rotational force provision mechanism. It is explanatory drawing of connection operation.

Regarding the present invention, a generalized model of the mechanism 30 that generates the rotational force will be described, and then a specific power generation device 10 that realizes the generalized model of the mechanism 30 that generates the rotational force will be described.
FIG. 1 is an explanatory diagram of a generalized model of a mechanism 30 that generates a rotational force in the case of an even number of mass points. FIG. 2 is an explanatory diagram of a generalized model of a mechanism that generates a rotational force in the case of an odd number of mass points.

As shown in FIGS. 1 and 2, the generalized model having a plurality of mass points m has a direction perpendicular to the vertical direction Z (the direction in which gravity acts) (horizontal direction, the paper surface of FIGS. 1 and 2 spreads). A rotating body center axis O extending in a direction perpendicular to the direction) and a rotating body D having a rotation radius R that rotates about the rotating body center axis O.

Rotating body D rotates around a rotating body central axis O when viewed from a reference base (so-called absolute coordinate axis, pedestal B in FIGS. 1 and 2). In the rotator D, there are a plurality of rotation center positions P at positions separated from the rotator center axis O by the rotation radius R. The plurality of rotation center positions P are located at an equal angle with respect to the rotation body center axis O. The plurality of rotation center positions P rotate around the rotation body center axis O as the rotation body D rotates.

As shown in FIG. 1, when the number of rotation center positions P is two, the two rotation center positions P are positioned in opposite directions with respect to the rotation body center axis O. That is, the angle a is 180 degrees which is a half of 360 degrees.

As shown in FIG. 2, when the number of rotation center positions P is three, the three rotation center positions P are at a position opened 120 degrees with respect to the rotation body center axis O. That is, the angle a is 120 degrees, which is one third of 360 degrees.

As shown in FIGS. 1 and 2, the mass point m is located at a distance r from the rotation center position P, and when viewed from the base B, the mass point m is always positioned on the horizontal direction side of the rotation center position P. (In the example shown, it is located on the right side, but may be located on the left side). That is, in the generalized model of the mechanism 30 that generates the rotational force, the position of the mass point m is tilted by 90 degrees with respect to the vertical direction Z according to the law of gravity around the rotation center position P. Thereby, the mass point m is in an unbalanced state and tries to move in the vertical direction Z by gravity. The generalized model of the mechanism 30 that generates the rotational force uses the force to be moved at this time as a power source. Further, the generalized model of the mechanism 30 that generates the rotational force includes one that acts as a horizontal holding mechanism that holds the mass point m in the horizontal direction with respect to the rotation center position P, as will be described later.

The mass point m is rotatably supported by the rotating body D so as to rotate around the rotation center position P as viewed from the rotating body D. The mass m is supported by the rotating body D so as to rotate around the rotation center position P as the rotating body D rotates. When viewed from the pedestal B, the mass m is supported by the rotary body D such that when the rotary body D rotates once, the mass point m rotates once relative to the rotary body D. The rotation direction of the mass m with respect to the rotating body D is opposite to the rotating direction of the rotating body D with respect to the base B.

Therefore, when viewed from the pedestal B, when the rotating body D rotates around the rotating body central axis O, the mass point m is always located on the same side with respect to the rotating center position P, while the rotating body central axis O Seems to rotate around. That is, for example, when viewed from the pedestal B, when the mass point m is located on the right side in the horizontal direction of the rotation center position P, even if the rotating body D rotates with respect to the pedestal B, the mass point m always rotates. It is located to the right of the center position P in the horizontal direction.

As shown in FIG. 1, the number of mass points m to be rotated may be at least two, and may be an even number or an odd number. When the number of mass points m is two, as shown in FIG.

Further, as shown in FIG. 2, the number of mass points m may be three, and as the number of mass points m increases, the rotational force acting on the rotating body D increases as will be described later.

FIG. 3 is an explanatory diagram when the mass point is positioned in the horizontal direction in the balance of gravity of the generalized model of the mechanism that generates the rotational force. FIG. 4 is an explanatory diagram when the mass point is going to move in the vertical direction in the balance of gravity in the generalized model of the mechanism that generates the rotational force in FIG.

3 and 4, since the mass point m rotates around the rotation center position P, each mass point m tries to move to a position that can be balanced according to gravity g. That is, the mass point m tends to move downward in the vertical direction Z as shown in FIG. 4 from the position on the right side in the horizontal direction of the rotation center position P shown in FIG. At this time, since the mass point m is restricted to rotate about the rotation center position P, the mass point m is closer to the rotating body central axis O when viewed from the vertical direction Z as shown in FIG.

However, in the present invention, by preventing movement in the vertical direction Z, each mass point m is affected by gravity g in an unbalanced state.

FIG. 5 is an explanatory view of the dynamic consideration of the generalized model of the mechanism that generates the rotational force shown in FIGS. 3 and 4.
The rotational force (rotation, torque (N · m)) is the length (m, meter) of the line segment R2 in the direction from the rotating body central axis O to the mass point m1 and the force F1 of the tangential component perpendicular to the line segment R2. (N, Newton) and product.

The specific calculation is as follows.
For the mass m1, a moment (torque) M1 due to the mass is calculated.
First, a tangential component force F1 from the rotating body central axis O is obtained.

F1 = m × g × cos (θ2) = m × g × (R ₁ / R ₂ )
Here, R ₁ is the distance between the rotating body central axis O and the mass point m1 in the horizontal direction X, in other words, the Y axis (the axis in the vertical direction Z passing through the rotating body central axis O) and the mass point m1. Is the distance between.
R ₂ is the distance between the rotary body center axis O and the material point m1.
θ2 is an angle formed by a straight line connecting the rotating body central axis O and the mass point m1 and a straight line passing through the mass point m1 and orthogonal to the Y axis (in other words, a horizontal line passing through the mass point m11).

Therefore, when the moment (torque) M1 is obtained,
M1 = F1 × R ₂ = m × g × (R ₁ / R ₂ ) × R ₂ = m × g × R ₁
It becomes.

Also,
R ₁ = R × sin θ + r
Obviously.
Here, θ is an angle formed by a straight line extending on the upper side of the Y axis passing through the rotating body center axis O and the rotation center position P.

Then
M1 = m × g × (R × sin (θ) + r)
It becomes.

Similarly, the moment M2 of the mass point m2 is obtained.
Since the position of the mass point m2 is located on the opposite side of the mass point m1 with respect to the rotating body center axis O (180 degrees), a straight line extending through the rotating body center axis O and extending upward in the vertical direction Z and the rotation center position P Is represented by θ, θ + π, that is, θ + 180 degrees.

Therefore,
M2 = m × g × (R × sin (θ + π) + r) = m × g × (−R × sin θ + r)
It becomes.

Combining the moment forces of the two mass points m1 and m2,
M1 + M2 = m × g × (R × sin θ + r) + m × g × (−R × sin θ + r) = 2 mgr> 0
It becomes.

Therefore, since the moment representing the rotational force always takes a positive value, the rotational force is always generated regardless of the value of θ.

With reference to FIG. 6, the power generator 10 which is an example which implement | achieved the generalized model of the mechanism 30 which produces a rotational force is demonstrated. The power generation device 10 converts gravity into a rotating force, uses the converted force as a power source, and prevents the natural law that tries to balance gravity from being balanced. And a mechanism for generating a rotational force that creates an imbalance, and the generated imbalance generates rotational energy.
FIG. 6 is a schematic diagram of a power generation device including a mechanism that generates a rotational force using a stabilizing plate.

The power generation device 10 includes a rotating body central axis O, a plurality of transmission gears 16, a stabilizing plate 18 attached to the transmission gear 16 so as not to be relatively rotatable, and a weight attached to the stabilizing plate 18 so as not to be relatively movable. (Mass point m).
As an example, the rotating body D has an X-shape extending in all directions from the rotating body central axis O as shown in FIG. The rotating body D is rotatably supported by the base B around the rotating body central axis O.

Rotating body central axis O rotates with rotating body D. On the other hand, since the center gear 14 at the rotation center of the rotating body D is fixed to the base B, it does not rotate with respect to the base B.

Each of the plurality of transmission gears 16 is rotatably supported by the rotating body D via a plurality of rotation center shafts 20. The plurality of rotation center shafts 20 are attached to the rotating body D so as not to move relative to each other.
In the plurality of transmission gears 16, a transmission gear 16 that meshes with the central gear 14 and a plurality of transmission gears 16 that mesh with the transmission gear 16 in series are arranged in a row from the rotating body central axis O to the outside. In FIG. 5, four rows are formed.

Therefore, the plurality of transmission gears 16 rotate (revolve) around the rotating body central axis O together with the rotating body D, and rotate (rotate) around the rotation center axis 20 of each transmission gear 16. Become.

FIG. 7 is an explanatory diagram of the rotation direction of the transmission gear 16 of the power generation device 10. FIG. 8 is an explanatory diagram of the stabilizer. FIG. 9 is an explanatory diagram of a state in which the stabilizer is in a natural balance in FIG. FIG. 10 is an explanatory diagram of how to apply force to the stabilizer and how to solve the balance problem of the stabilizer. FIG. 7 shows four transmission gears 16 that mesh with the central gear 14, but these four transmission gears 16 are not meshed with each other.

The center gear 14 is fixed to the base B, and the transmission gear 16 can freely rotate (rotate) about the rotation center axis 20 of the transmission gear 16. Here, the number which counted the center gear 14 as the 1st gear in order is given to the some transmission gear 16 from the side close | similar to the center gear 14. FIG.
Even if the rotating body D rotates, the odd-numbered transmission gear 16 of 3 or more always moves in a certain direction, that is, moves so as not to rotate. The present invention is characterized in that this non-rotating movement is used for posture control.

More specifically, since the plurality of transmission gears 16 are the same gears as the central gear 14 (that is, the module and the pitch circle diameter are the same as each other), if the central gear 14 is the first gear, three or more The odd-numbered transmission gear 16 always faces in a certain direction.

That is, when the rotating body D is rotated in the clockwise direction CW with respect to the base B, the central gear 14 does not rotate, so that the transmission gear 16 (even-numbered transmission gear 16) meshed with the central gear 14 is the central gear 14. Rotate (revolve) in the clockwise direction CW1 with respect to the pedestal B, and rotate (rotate) in the clockwise direction CW2 with respect to the rotating body D around the rotation center axis 20.

On the other hand, the odd-numbered transmission gear 16 rotates in the counterclockwise direction CCW with respect to the rotating body D in response to the rotation of the even-numbered transmission gear 16 inside the odd-numbered one (rotation in the clockwise direction CW2). Since the rotating body D rotates in the clockwise direction CW with respect to the pedestal B, when viewed from the pedestal B, the odd-numbered transmission gears 16 are translated while being oriented in a certain direction.
That is, when the rotating body D is rotated about the rotating body central axis O with respect to the pedestal B by applying a rotational force to the rotating body D, the odd-numbered transmission gear 16 has a fixed direction with respect to the pedestal B. Around the center axis O of the rotating body. In addition, by applying a rotational force to the odd-numbered transmission gear 16, when the odd-numbered transmission gear 16 is rotated around the rotating body central axis O with the odd-numbered transmission gear 16 being directed in a certain direction with respect to the base B, the rotation is performed. The body D rotates around the rotating body central axis O.

As shown in FIG. 6, a stabilizing plate 18 is attached to the odd-numbered transmission gear 16 on the outermost side. The stabilizer 18 has a posture control function, that is, a horizontal holding mechanism that holds the mass point m in the horizontal direction in accordance with the law of gravity, and a role of a mechanism 30 that generates a rotational force.

Further, a weight (mass point m) for generating a rotational force is attached to the stabilizing plate 18.
Specifically, the stabilizing plate 18 is suspended so as to be swingable to the rotation center shaft 20 of the outermost odd-numbered transmission gear 16. The outermost odd-numbered transmission gear 16 meshes with another transmission gear 16 (even-numbered transmission gear 16). For this reason, the stabilizing plate 18 coincides with the movement of the transmission gear 16 from which the stabilizing plate 18 is suspended.

When the stabilizing plate 18 is balanced (maintains an equilibrium state), the rotational force around the rotating body central axis O does not act on the outermost transmission gear 16 and thus the rotating body D. That is, the outermost odd-numbered transmission gear 16 attached to the stabilization plate 18 does not rotate with respect to the rotating body D.
Therefore, it is important to maintain this balance in an unbalanced state.

In order to realize maintaining the unbalanced state, a suspension shaft for suspending the stabilizer 18 (the same shaft as the rotation center shaft 20 of the transmission gear 16 in FIGS. 8 and 9) and a suspension shaft other than the suspension shaft are provided. If the stabilizing plate 18 can be maintained in an unbalanced state by causing some action at least at one point, the force generated by the unbalance is transmitted to the rotation shaft (hanging shaft), and the rotation shaft (hanging shaft). ) Starts rotating (swinging) in an attempt to balance.

That is, as shown in FIG. 8, the weight (mass point) is such that the position of the center of gravity of the weight (mass point m) is away from the Y axis extending in the vertical direction Z through the suspension axis (rotation center axis 20). When m) is attached to the stabilizer 18, the stabilizer 18 rotates around the suspension shaft so that the stabilizer 18 is in a balanced position (right rotation Rr in the case of FIG. 9). By preventing this rotation using a "mechanism that generates rotational force", a balanced imbalance is created. In the unbalanced state, a force (rotational force) that always tries to shift to the balanced state works. A structure that uses this force to generate a rotational force is a feature of the present invention.

However, as shown in FIG. 10, when a weight (mass point m) is directly attached to the stabilizer 18, a force transmitted from the transmission gear 16 (left rotational force FL around the suspension shaft) and a weight (mass point m). ) (Right rotational force FR about the suspension axis) is offset and no rotational force is generated.

Therefore, by converting the force (right rotational force FR) received by the weight (mass point m) into the left rotational force FL and converting the canceled force relationship into the left rotational force FL in the rotating direction, Solve the offset problem.

The creation of this state of “left rotational force> right rotational force” is referred to as a mechanism 30 that generates rotational force in the present invention. As described above, the power generation device 10 converts gravity into a rotating force, uses the converted force as a power source, and balances the natural law that tries to balance gravity. In the absence of such a mechanism, a mechanism 30 is created that produces a rotational force that creates an imbalance and is imbalanced to produce rotational energy.

With reference to FIG. 11 and FIG. 12, an example of the mechanism 30 which produces this rotational force is demonstrated.
FIG. 11 is a front view illustrating an example of a mechanism that generates a rotational force. FIG. 12 is a cross-sectional view in which a part of the mechanism that generates the rotational force shown in FIG. 11 is omitted. FIG. 13 is a schematic explanatory diagram of a power generation device including a rotational force addition mechanism. FIG. 14 is a front view in which a part of the rotational force adding mechanism shown in FIG. 13 is omitted. FIG. 15 is a cross-sectional view in which a part of the rotational force adding mechanism shown in FIG. 14 is omitted.

As shown in FIGS. 11 and 12, the mechanism 30 that generates the rotational force includes the odd-numbered transmission gear 16, the stabilizing plate 18, the guide plate 19, the support plate 21, the lever bar na, and the lever bar na. And a weight (mass point) m provided at one end na1.

Since the rotation center shaft 20 is attached to the rotating body D so as not to move relatively, the transmission gear 16 rotates with respect to the rotation center shaft 20.

The stabilization plate 18 has the same center as that of the rotation center shaft 20 and has a disk shape larger than that of the transmission gear 16, and is attached to the transmission gear 16 by a plurality of screws 16a so as not to move relative thereto. For this reason, the stabilizer 18 rotates with respect to the rotation center shaft 20 together with the transmission gear 16.

The guide plate 19 includes a disk-shaped bottom portion 19a and a side surface portion 19b extending in a cylindrical shape in the axial direction of the rotation center shaft 20 from the periphery of the bottom portion 19a. Since the guide plate 19 is attached to the rotation center shaft 20 so as not to be relatively movable, the guide plate 19 rotates about the rotation center shaft 20 with respect to the transmission gear 16. The side surface portion 19b has a cylindrical inner peripheral surface 19c and an outer peripheral surface 19d with the rotation center axis 20 as a central axis.

The support plate 21 is a plate member. Three bearings B1, B2, B3 are provided on one surface side of the support plate 21 so that the bearings B1, B2 are kept in contact with the inner peripheral surface 19c and the bearing B3 is kept in contact with the outer peripheral surface 19d. Is attached. The support plate 21 rotates around the rotation center axis 20 while maintaining the state where the bearings B1 and B2 are in contact with the inner peripheral surface 19c and the state where the bearing B3 is in contact with the outer peripheral surface 19d. In other words, the support plate 21 relatively rotates along the guide of the guide plate 19.

The lever rod na has a rod shape, has a weight m at one end na1, and a retaining screw SW1 that rotatably supports the support plate 21 and a stabilizer 18 on the other end na2 side. A retaining screw SW2 to be supported is provided. That is, the lever rod na is supported by the stabilizing plate 18 so as to be swingable around the retaining screw SW2, and also supports the support plate 21 so as to be rotatable around the retaining screw SW1.

When the weight m is hung on one end na1 of the lever bar na, the gravity of the weight m acts on the one end na1 downward in the vertical direction Z. SW1 tries to rise (upward in the vertical direction Z).
However, since the support plate 21 sandwiches the side surface portion 19b of the guide plate 19 with the bearings B1, B2, and B3, the support plate 21 can be rotated about the rotation center axis 20, but the retaining screw SW2 is not attached. It cannot move upward in the vertical direction Z to the center. Further, the retaining screw SW1 fixes the other end na2 side of the lever bar na to the support plate 21. For this reason, the lever bar na is in the same state as the state where it is fixed to the guide plate 19. Further, in a state where the rotating body D does not rotate about the rotating body central axis O with respect to the base B, the rotating body D and the stabilizing plate 18 do not move relative to each other. Does not move relative to each other. That is, it can be said that the insulator rod na is the same as being fixed to the stabilizing plate 18.
Accordingly, the part that plays a role of releasing the force acting on the retaining screw SW1 is the retaining screw SW2, and the force acting on the retaining screw SW2 is downward in the vertical direction Z.

In FIG. 11, the retaining screw SW2 is fixed to the stabilization plate 18 slightly to the left of the position just below the rotation center shaft 20 (below the vertical direction Z). (Rotational force). However, even if this counterclockwise torque (rotational force) is present, this torque (rotational force) is insignificant, and a sufficient counterclockwise torque (rotational force) cannot be obtained.

The torque (rotational force) transmitted from the rotating body central axis O shown in FIG. 6 via the plurality of transmission gears 16 becomes the left rotational force FL as shown in FIG. The ratio between the rotational force FL and the right rotational force FR caused by the weight m being positioned on the right side from the rotation center axis 20 may be considered as 1: 1.

In the mechanism 30 that generates the rotational force shown in FIG. 6, the rotational force that promotes rotation is transmitted from the rotating body central axis O via the plurality of transmission gears 16. The rotational force is mechanical friction such as gear meshing. As a result, it attenuates slightly. Assuming that the damping coefficient indicating the slight attenuation rate is roughly 0.9, the ratio between the left rotational force FL acting on the stabilizer 18 and the right rotational force FR acting on the weight m is: 0.9: 1. In this state, the right rotational force FR is greater than the left rotational force FL, and the mechanism that generates the rotational force does not generate the rotational force.

Furthermore, even if a slight counterclockwise torque (rotational force) described in FIG. 11 is added to this state, sufficient rotational force cannot be obtained.

Therefore, as shown in FIG. 13, a mechanism having an auxiliary function for increasing the rotational force is introduced into the odd-numbered transmission gear 16 between the center gear 14 and the outermost odd-numbered transmission gear 16. To do. Since this is an auxiliary function for adding a rotational force, it will be referred to as a rotational force addition mechanism 40.
An example of the rotational force adding mechanism 40 will be described with reference to FIGS. 14 and 15.

The rotational force adding mechanism 40 is attached to the odd-numbered transmission gear 16 so as not to be relatively movable. The rotational force adding mechanism 40 includes a stabilizer 42, a support plate 44, a lever bar nb, a weight ma provided at one end nb1 of the lever bar nb, a support member 46, a lever bar nc, and a lever bar nc. And a weight mb provided at one end nc1.

The stabilizing plate 42 is a disk member having a radius larger than the radius of the odd-numbered transmission gear 16 to which the rotational force adding mechanism 40 is attached. The stabilizing plate 42 is attached with screws so as not to be relatively movable concentrically with the transmission gear 16. A retaining screw SW15 and a retaining screw SW13 are provided in the vicinity of the circumference of one side surface of the stabilizing plate 42. The retaining screw SW13 is provided below the retaining screw SW15 in the vertical direction Z. The retaining screw SW13 and the retaining screw SW15 are located on the left side of the vertical direction Z of the rotation center shaft 20, and the retaining screw SW15 is located on the left side of the retaining screw SW13.

The support plate 44 is a plate-like member and is attached to the rotation center shaft 20 so as to be rotatable about the rotation center shaft 20. The support plate 44 is provided with a retaining screw SW11 and a retaining screw SW14 on the side surface opposite to the stabilizing plate 42. The lower side surface portion of the support plate 44 in the vertical direction Z is in contact with the retaining screw SW15. For this reason, the support plate 44 is located on the left side of the rotation center shaft 20, and the retaining screws SW 15 support the support plate 44 so that the support plate 44 does not rotate counterclockwise.
The retaining screw SW11 and the retaining screw SW14 are generally located on the left side of the rotation center shaft 20 between the rotation center shaft 20 and the retaining screw SW15.

A weight mb is provided at one end nc1 of the insulator rod nc, and the other end nc2 is rotatably supported by the rotation center shaft 20. Further, a retaining screw SW14 is in contact with the lower side of the vertical direction Z between the one end nc1 and the other end nc2 of the lever rod nc. That is, the retaining screw SW14 supports the lever bar nc below the lever bar nc.

A weight ma is provided at one end nb1 of the insulator rod nb, and the other end nb2 is supported by a support plate 44 so as to be rotatable by a retaining screw SW11. A retaining screw SW11 is provided on the other end nb2 side between the one end nb1 and the other end nb2.

The support member 46 is a rod-shaped member having a bent portion, and both ends of the support member 46 are rotatably attached to the retaining screw SW12 and the retaining screw SW13, respectively. As a result, the support member 46 supports the lever bar nb from below the vertical direction Z, and can hold the force from the lever bar nb and transmit it to the screw SW13.

As described above, the rotational force adding mechanism 40 has a structure in which the weight ma and the weight mb can be placed on the left and right ends. Accordingly, the weight ma acts on the one end nb1 with the downward gravity Fa in the vertical direction Z, and the weight mb acts on the one end nc1 with the downward gravity Fb in the vertical direction Z.

Since gravity Fa in the vertical direction Z acting on the weight ma acts on one end nb1, one end nb1 functions as a power point, the retaining screw SW11 functions as a fulcrum, and the retaining screw SW12 functions as an operating point. For this reason, the gravity Fa acts on the retaining screw SW 13 as a downward force Fd in the vertical direction Z via the support member 46.

Since the gravity Fb in the vertical direction Z acting on the weight mb acts on one end nc1, one end nc1 functions as a power point, the rotation center shaft 20 serves as a fulcrum, and the retaining screw SW14 functions as an action point. For this reason, the gravity Fb acts on the retaining screw SW15 as a downward force Fc in the vertical direction Z via the support plate 44.
The positions of the force Fc and the force Fd that are finally applied are arranged so as to be in the direction FL that promotes rotation.

Let us explain these force relationships mathematically. As shown in FIG. 14, when the horizontal and vertical axes passing through the rotation center axis 20 are partitioned, a first quadrant I that is an upper right area of the rotation center axis 20 and a second quadrant that is an upper left area of the rotation center axis 20. II, the third quadrant III, which is the lower left area of the rotation center axis 20, and the fourth quadrant IV, which is the lower right area of the rotation center axis 20, are obtained. A rotating force FL can be generated by bringing a support point to the third quadrant III.
Therefore, the rotational force adding mechanism 40 is used to compensate for the rotational force that attenuates.

When the force F _(n) acting on the transmission gear 16 (n is the number of transmission gears 16 from the central gear 14) is expressed in a sequence, when the rotational force adding mechanism 40 is not used,
F _{(n + 1)} = (F _(n) * 0.9) = ((F _(n-1) * 0.9) * 0.9)
It becomes.
Here, when the attenuation ratio of the first term (when n = 1) is μ,
F _(n) = F ₍₁₎ × μ ⁽ⁿ⁻¹⁾
Can be thought of as a geometric sequence of
F _{(n) <} F ₍₁₎
An attenuation line can be drawn (see FIG. 16).

Here, when the rotational force addition mechanism 40 is used,
F _{(n + 1)} = (F _(n) × μ) = ((F _(n−1) × μ) × μ) + FL
Although it depends on the size of μ, if the gear attenuation is considered to be about 0.9,
F _(n) = F ₍₁₎ x μ ^(n-1) + FL
And
F _(n) > F ₍₁₎
Each parameter is determined so that
If F _(n) > F ₍₁₎ , the force FL that urges the rotation always remains without being canceled (see FIG. 17).

As shown in FIG. 17, the force in the final term of the step-like line is a force that promotes the rotation acting on the stabilizer, and the ratio between the force FL that promotes the revolution on the stabilizer and the force FR that prevents the rotation due to the weight. However, since the force FL that promotes the rotation of the stabilizer plate is greater than the force FR that prevents the rotation due to the weight, a force sufficient to maintain the rotation can be generated.

Thus, although it is necessary to adjust the respective sizes of the weight ma and the weight mb, by using this rotational force addition mechanism 40, it is possible to eliminate the force that prevents the rotation of the rotating body D. Thus, the rotating body D that has started rotating itself can continue to rotate using the inertial force of each mass point.

Rotational force according to the present invention can be a power source of equipment having a constant rotational force and mainly rotating.

When compared with the force relationship on the “generalized model”, the detailed position is slightly shifted, but since it is approximated on an actual device, a rotating force is always generated.

FIG. 18 is a front view in which a part of another rotational force applying mechanism 40a is omitted.
As shown in FIG. 18, another rotational force applying mechanism 40 a omits the weights ma and mb of the rotational force applying mechanism 40 and also has a bar-shaped link member nd, a bar-shaped link member ne, a slide guide bar nf, and a weight W. With.

One end of the link member nd is swingably attached to one end nb1 of the lever bar nb. For this reason, the rod-shaped link member nd extends in the vertical direction Z.
One end of the link member ne is swingably attached to one end nc1 of the lever bar nc. For this reason, the rod-shaped link member ne extends in the vertical direction Z.

Both ends of the slide guide rod nf are swingably attached to one end of the link member nd and the link member ne so as to extend in a substantially horizontal direction.
The weight W is attached so as to be movable in the extending direction (substantially horizontal direction) of the slide guide bar nf, and is attached to an arbitrary position on the slide guide bar nf so as not to be relatively movable by a locking means such as a retaining screw.

The downward gravity Fw1 and gravity Fw2 in the vertical direction Z vary depending on the position of the weight W. Therefore, by attaching an arbitrary weight W at an arbitrary position, the gravity Fw1 and the gravity Fw2 of the rotational force applying mechanism 40a can be made the same as the gravity Fa and the gravity Fb of the rotational force applying mechanism 40, respectively.

FIG. 19 is an explanatory diagram of the linked operation.
In operation, it is preferable to attach 16 stabilizers 18 before and after one rotating body D. In this case, about eight stabilizers 18 are attached to each surface of one rotating body D, which is ideal for operation. Further, by connecting the rotating bodies D in parallel, the rotational force increases by addition.

Therefore, in actual operation, a large power source can be obtained by using the plurality of stabilizing plates 18 and the plurality of rotating bodies D.

∙ When the rotational force is connected to the motor for power generation, power can be generated by gravity. The application range is wide because it can be used as a power source that is stable from the mathematical formula.

D Rotating body O Rotating body central axis P Rotating center position R Rotating radius 10 Power generator 14 Central gear 16 Transmission gear 18 Stabilizing plate 19 Guide plate 20 Rotating center shaft 21 Support plate 30

Mechanism

40, 40a for generating rotational force Addition of rotational force Mechanism 42 Stabilizing plate 44 Support plate 46 Support member

Claims

A power generation device that converts gravity into rotating force and uses the converted force as a power source,
Power generation including a mechanism that generates a rotational force that creates an energy of rotation in the imbalance by causing an imbalance by preventing the balance from occurring in a natural law that tries to balance gravity apparatus.
The power generation device according to claim 1, wherein the power source is an imbalance caused by tilting the position of the mass point by 90 degrees with respect to the vertical direction according to the law of gravity.
Furthermore, a horizontal holding mechanism that holds the mass point in the horizontal direction according to the law of gravity;
The power generation device according to claim 2, further comprising a rotational force addition mechanism that adds an additional rotational force to the rotational force.