JPH10299637A - Magnetic rotary engine having planet gear unit - Google Patents

Abstract

PROBLEM TO BE SOLVED: To take out rotational energy continuously by generating a rotational force by rotating bodies provided with a plurality of magnets arranged and fixed on the same axis as the sun gear and the planet gear of a planet gear unit. SOLUTION: When the planet gear 10B is engaged with the internal gear in a planetary gear unit, the force of the planet gear 10B acted by the magnetic force of a magnetic rotary body 1B is distributed uniformly to two contact points 16AB, 16BC. Therefore, the force of the planet gear 10B acting to a sun gear 10A is reduced in half and the acting force of the sun gear 10A is larger than the acting force of the planet gear 10B at the contact point 16AB and the acting force by the magnetic force of a magnetic rotating body 1A is transmitted to the magnetic rotary body 1B via the sun gear 10A and the planet gear 10B, and when the magnetic rotary body 1A is rotated, the magnetic rotary body 1B is rotated on an arm 14 and around the magnetic rotary body 1A along the inner periphery of the internal gear 10C with a fulcrum of the contact point 16BC of the planet gear 10B and with an acting point of the contact point 16AB.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION When accommodating a plurality of rotating bodies in a rotating device as shown in a magnetic rotating engine of Japanese Patent Application No. 9-81782 filed on Feb. 25, 1997, BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic rotating engine that aims to provide rotational energy by acquiring rotational ability generated from an interaction force due to magnetic force of potential energy of each rotating body by using a planetary gear device as kinetic energy.

[0002]

2. Description of the Related Art A magnetic rotating engine of a patent application filed on Feb. 25, 1997 and having a patent application number (Japanese Patent Application No. 9-81782) has a structure in which a rotating body having magnets arranged and fixed is accommodated in a rotating device. The rotating body was rotated by the difference in the input force in the transmission of the force resulting from the difference between the radius of the rotating body and the gear radius and the acting force of the gear caused by the difference in the output. The rotating bodies and the rotating shafts of the gears were supported by an underframe.

[0003]

The patent application filed in the prior application uses a plurality of magnet rotating bodies and equips the rotating body with a resultant force of attractive force, repulsive force and sliding force generated by the interaction of magnets. The working force transmitted to the contact point of each gear was changed by using the gears.

When a plurality of rotators 1B are arranged around the rotator 1A, each of the rotators has a rotational ability to rotate in the same direction. At that time, by giving a difference between the distance from the resultant point of the magnetic force of the rotating body to the center of the rotating shaft of the rotating body and the distance from the center of the rotating shaft to the contact point of the gear on which the force acts, the contact point of the gear A rotary engine that can give a difference to the mutual acting force transmitted to the rotary engine and converts it into rotary motion.

According to the present invention, the distance from the resultant point of the magnetic force of each rotating body to the center of the rotating shaft of the rotating body is determined as described above.
Regardless of the difference in the distance from the center of the rotating shaft to the contact point of the gear on which the force acts, the acting force transmitted to the contact point of each gear by the attractive force, repulsion, and sliding force of the magnet of the rotating body Equally, when the rotating body is unstablely balanced,
This is a magnetic rotating engine that gives a reducing effect to any of the acting forces of a plurality of rotating bodies, breaks the balance of acting forces at the contact points of the gears, acquires kinetic energy, and converts it into rotational motion.

[0006]

In order to achieve the above object, the present invention uses a planetary gear device as a rotating device, and uses a rotating shaft of the rotating body 1A and a rotating body 1 disposed around the rotating body 1A.
The underframe of the rotating shaft of B is separated, and the group of rotating bodies B can move around the rotating body 1A while rotating on the rotating arm of the planetary gear device.

[0007] The sun gear of the rotating body 1A meshes with the planetary gear of the rotating body 1B, and the planetary gear and the internal gear are meshed using the internal gear of the large gear internal meshing. The rotating shaft of the rotating body 1A is supported by the underframe, and the rotating shaft of the rotating body 1B is supported by the arm of the planetary gear device. Further, the internal gear is fixed.

[0008] At this time, the kinetic energy of each rotating body generated by the attractive force of the magnetic force, the repulsive force, and the resultant force of the slip, which is the potential energy, becomes a force acting on the contact point of each gear, and this force becomes an interaction force. Affects all rotating bodies.

[0009]

BEST MODE FOR CARRYING OUT THE INVENTION The magnets arranged and fixed on a plurality of rotating bodies conform to the example of the magnet arrangement shown in the patent application filed on Feb. 25, 1997, application number (Japanese Patent Application No. 9-81782). To create. As an example, the rotating body 1A is provided with a plurality of magnets in FIG.
The magnets are arranged and fixed to the rotating body B as shown in FIG. In addition, sun gear,
A sun gear is used for the rotating body 1A, and a rotating body 1B is used for the rotating body 1A using a planetary gear device having a planetary gear and an internal gear that meshes with a large gear.
Is equipped with a planetary gear and housed.

For the above reasons, the rotating shaft of the rotating body 1A and the sun gear is supported by the underframe, and the rotating body 1B and the shaft of the planetary gear are supported by the arm of the planetary gear device. And
The internal gear that meshes with the planetary gears is fixed, and the meshing of the planetary gears and the internal gear is made removable with a leverage device.

[0011]

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment will be described below with reference to the accompanying drawings. In each figure, reference numerals 1A and 1B denote rotating bodies on which magnets are arranged and fixed. 2A and 2B are axes of the rotating body. 10A
Is a sun gear mounted on the rotating body 1A. 10B is a planetary gear mounted on the rotating body 1B. 10C is a fixed internal gear of a large gear internal gear, and a planetary gear 10B.
The engagement between the internal gear 10 </ b> C and the internal gear 10 </ b> C is made detachable by the shifting lever device 17. 12A, 12B, and 12C are forces acting on the contact points of the gears. 13A and 13B are bearings. 14 is an arm of the planetary gear set. 15 is a rotating body A
Bearing frame. 16AB is a sun gear 10A mounted on the rotating body A and a planetary gear 10B mounted on the rotating body 1B.
Are the contact points at which they mesh. 16BC is planetary gear 10B
And the contact point where the internal gear 10C meshes.

FIG. 1 is a configuration diagram according to an embodiment of the present invention. 2 and 3 show the arrangement of magnets shown in the previously filed patent application and application number (Japanese Patent Application No. 9-81782).
It is a rotating body in which magnets are arranged and fixed in three stages.

FIG. 4 is a diagram showing the direction of the kinetic energy of the magnetic force of the two rotating bodies acting on the gears A and B mounted on the rotating bodies. And the size is equal,
When the oppositely acting forces 12A and 12B act on the contact point 16AB, the rotating body is in an unstable state and is in balance.

FIG. 5 shows a sun gear 10A, a planetary gear 10B,
It is a figure showing the direction of the force which acts on internal gear 10C. 12
A is the acting force by the magnetic force of the rotating body 1A, and 12B is the acting force by the magnetic force of the rotating body 1B. Then, as shown in the figure, when the planetary gear and the internal gear are brought into the meshing state by the shifting lever 17, the acting force by the magnetic force of the rotating body 1B becomes:
The acting force is divided into two points of contact points 16AB and 16BC of the planetary gear. Also, 12C is a divided acting force 12C.
The reaction force against B.

FIG. 6 shows the internal gear 10C of the large gear internal meshing.
It is a figure which shows the Example of the positional relationship of the arm 14 of a planetary gear apparatus, and the bearing frame 15 of the rotating body 1A.

FIG. 7 shows a sun gear 10A, a planetary gear 10B,
It is a figure which shows the Example of the positional relationship with the internal gear 10C, the arm 14 of a planetary gear device, and the bearing frame 15 of the rotating body 1A.

FIG. 8 shows a sun gear 10A, a planetary gear 10 in a combination of the rotating body 1A, the rotating body 1B and the planetary gear device.
FIG. 9 is a diagram showing a force relationship acting on B. 12A is the rotating body 1
A is the acting force by the magnetic force of A, and is the acting force divided into four contact points of the sun gear. 12B is the acting force by the magnetic force of the rotating body 1B. The engagement between the planetary gear and the internal gear is in a disengaged state.

FIG. 9 shows that the planetary gear 10 is
It is a figure which shows the force which acts on sun gear 1A, planetary gear 10B, and internal gear 10C at the time of making B and internal gear 10C mesh. Reference numeral 12A denotes an acting force by the magnetic force of the rotating body 1A, which is divided into four contact points of the sun gear. Numeral 12B is the acting force by the magnetic force of the rotating body 1B, which is divided into two contact points of the planetary gear and the internal gear. Further, 12C is a divided acting force 12B.
Is the reaction force.

FIG. 10 is a diagram showing an embodiment of the relationship between the combination positions of the rotating bodies 1A and 1B.

[0020]

Since the present invention is constructed as described above, it has the following effects. FIG.
As shown by the energy conservation law, the acting force of the planetary gear due to the magnetic force of the rotating body 1B is equal to the contact points 16AB and 16
It is divided into two points of BC. Contact point 1 between planetary gear and internal gear
The force 12C at 6BC is a reaction force of the internal gear with respect to the acting force of the planetary gear. The planetary gear is fixed to the internal gear, the rotating body 1B cannot rotate, and the acting force at the contact point 16BC between the planetary gear and the internal gear. Are cancelled, and the work performed by the planetary gear at the contact point 16BC becomes zero. The rotator 1B has the ability to do work, but is not working, and the rotator 1B applied to the contacting sun gear
However, the acting force of the planetary gear due to the magnetic force decreases.

At the contact point 16AB, the acting force of the sun gear exceeds the acting force of the planetary gear, and the acting force due to the magnetic force of the rotating body 1A is reduced by the acting force of the planetary gear and the internal gear. The rotating body 1B, which is transmitted to the rotating body 1B via a gear and rotates the rotating body 1A, is supported by the arm of the planetary gear set at the contact point 1 of the planetary gear.
With the 6BC as a fulcrum and the contact point 16AB as a power point, the rotating body 1A rotates around the rotating body 1A like a planet along an internal gear of the internal gear.

As an example, the resultant force by the magnetic force of the rotating body is represented by (f), and (a) of the rotating body A and (b) of the rotating body B are
The distance from the resultant point of the magnetic force to the center of the rotating body,
(R) is the radius of the gear, (x) is the force acting on the sun gear,
(Y1) and (y2) are the forces acting on the planetary gears, and
Assuming that (z) is the reaction force of the internal gear, as shown in FIG.
When the engagement between the planetary gear and the internal gear is released, when the rotating direction of the rotating body 1A acts clockwise, the rotating body 1B also has a clockwise acting force, and the rotating direction and the ease of rotation. Are compared, the force moment (N
1A) is (N1A) = a × f (clockwise), and the force moment (N1B) of the rotating body 1B is (N1B) = b × f (clockwise). The force acting at the contact point between two rotating bodies having the same rotation direction is an interaction force, and the directions are opposite.

As shown in FIG. 5, the sun gear 10A, the planetary gear 10B, and the internal gear 10C are
, As shown in the figure, the force relationship acting on the contact point 16AB between the sun gear 10A and the planetary gear 10B and the contact point 16BC between the planetary gear 10B and the internal gear 10C is as follows. Sun gear 10 at contact point 16AB
The acting force (x) of A is x × r = a × f∴x = a × f / r.

According to the law of conservation of energy, at the two contact points of the planetary gear, the acting force is divided into two, and (y1) of the planetary gear 10B having the contact point 16AB and (y2) having the contact point 16BC. The acting force is y1 = y2, and y1 × r = b × f / 2 y1 (y2) = b × f / 2r.

The acting force of the internal gear 10C at the contact point 16BC is the reaction force 12 against the acting force of the planetary gear 10B.
C. When the acting force (y2) acts on the planetary gear 10B, a reaction force (z) is generated on the internal gear 10C,
From the law of action and reaction, z = −y2∴z = − (b × f / 2r), and the interaction forces acting on the planetary gear and the internal gear are equal in magnitude and opposite in direction.

The sun gear 1 at the contact point 16AB
0A acting force (x) formula, planetary gear 10B acting force (y
The difference between the forces in equation (1) is x-y1 = (a * f / r)-(b * f / 2r) = 1 / 2r * (2af-bf).

As an example, when the planetary gears and the internal gear are engaged with each other, the shapes of the rotating bodies 1A and 1B and the gears are (a = b =
r> 0), the acting force x, y1, y of each gear
2, z are: x = a × f / r = fy 1 = b × f / 2r = f / 2 y2 = b × f / 2r = f / 2 (10) z = f / 2 (11) The acting force (y2) of the planetary gear is offset by the reaction force (z) of the internal gear.

The difference between the acting force (x) of the sun gear and the acting force (y1) of the planetary gear is given by the following equation: x−y1 = (a × f / r) − (b × f / 2r) = ff / 2/2 = f / 2 (12). Therefore, at the contact point 16AB, the acting force of the sun gear 10A is added to the acting force of the planetary gear 10B by f
/ 2 power is better.

This is because when the rotating body 1A rotates clockwise, the force of f / 2 is simultaneously transmitted from the sun gear 10A to the planetary gear 1A.
0B, a counterclockwise force is applied to the planetary gear 10B fixed to the internal gear, with the contact point 16BC as a fulcrum and the contact point 16AB as a power point, and counterclockwise along the inner gear of the internal gear 10C. To rotate.

When the rotating direction of the rotating body 1A due to the magnetic force f acts clockwise, the rotating body 1B also has a clockwise acting force. The comparison of the individual force moments of the rotating body and the gear is a comparison of the direction of rotation and the ease of rotation. The clockwise moment (N1A) of the rotating body 1A is (N1A) = a × f = rf (clockwise) (13).

The sun gear 1 having the contact point 16AB as a power point
Since the force of the counterclockwise moment of 0A (N10A) is the acting force (y1) from the planetary gear 10B, (N10A) = a × y1 = a × (b × f / 2r) = abf / 2r = rf / 2 (counterclockwise) (14), ∴ (N1A) = rf> (N10A) = rf / 2 (15), and the clockwise force moment of the rotating body A due to the magnetic force f is the planetary gear. It is larger than the counterclockwise force moment of the sun gear whose force is the acting force y1 received from 10B.

The clockwise force moment (N1B) due to the magnetic force f of the rotating body B with the rotating shaft fixed is given by the following equation: (N1B) = b × f (clockwise). Of the rotating body B riding on the arm of (a), the acting force (y
2) is offset by the reaction force (z), and
From (▼) and (11), (N1B) = b × (y1 + y2-z) (N1B) = b × f / 2 = r × f / 2 (clockwise) (16), and the planetary gear and the internal gear are In the case of meshing, the contact point (1) due to the magnetic force f of the rotating body B supported on the arm of the planetary gear device.
6AB) is equivalent to a reduction to (y1 = f / 2).

Further, the planetary gear 1 having the rotation shaft 2B as a fulcrum
Since the force of the counterclockwise force moment (N10B) of 0B is the acting force (x) formula received from the sun gear 10A, (N10B) = r × x = rf (counterclockwise) (17). From equations (16) and (17), (N10B) = rf> (N1B) = rf / 2 (18), and the clockwise force moment due to the magnetic force f of the rotating body B is the acting force received from the sun gear 10A. It is smaller than the counterclockwise moment of the planetary gear 10B whose force is x.

Also, the diameter of the planetary gear is set as a line segment, the contact point 16AB is set as a power point, and the contact point 16BC is set as a fulcrum.
The moment of the counterclockwise force of the planetary gear 10B (left N10A
Since the forces B to BC are the acting forces (x) received from the sun gear 10A, (left N10AB to BC) = 2rxx = 2rxaf / r = 2af = 2rf (counterclockwise) (19) is there.

Similarly, the rightward moment of the planetary gear 10B (right N10AB to BC) is the acting force (y1) received from the magnetic force of the rotating body B (right N10AB to BC) = 2r × (Y1 + y2-z) = 2r × bf / 2r = bf = rf (clockwise) (20) (left N10AB to BC)> (right N10AB to BC), and the rotating body B having the contact point 16BC as a fulcrum Similarly, the clockwise force moment of the planetary gear 10B due to the magnetic force f is smaller than the counterclockwise force moment whose force is the acting force x received from the sun gear 10A.

In order to apply the force (f) to the rotating body and rotate it, it is natural that the greater the force (f), the faster the rotation occurs. If the point where the force is applied is r from the rotation axis, The larger the force moment (N = r × f), the easier it is to rotate. From the expressions (13) and (17), (N1A) = rf> (N1B) = rf / 2, that is, the rotating body A is easier to rotate than the rotating body B.

As described above, the planetary gear 10B and the internal gear 1
When 0C is engaged, the rotating force of the rotating body 1B is halved by the effect of reducing the acting force by the planetary gear and the internal gear, and at the contact point 16AB, the acting force 12A generated from the magnetic force of the rotating body 1A and the rotating force 1A A difference is generated in the acting force 12B generated from the magnetic force, and the rotating body B group can be rotated by the rotation ability of the rotating body 1A, and further, can be provided as rotational energy.

[Brief description of the drawings]

FIG. 1 is a configuration diagram illustrating a magnetic rotary engine according to an embodiment of the present invention.

FIG. 2 is a diagram showing an example of a fixed arrangement of magnets of a rotating body 1A.

FIG. 3 is a diagram showing an embodiment of the arrangement of magnets fixed on a rotating body 1B.

FIG. 4 is a diagram showing a force relationship acting on gears 1A and 1B of two rotating bodies.

FIG. 5 shows a sun gear, a planetary gear,
FIG. 4 is a diagram showing a force relationship acting on an internal gear;

FIG. 6 is a diagram showing an embodiment of the positional relationship between the internal gear, the arm of the planetary gear device, and the bearing installation frame of the rotating body 1A.

FIG. 7 is a diagram showing an example of a positional relationship among a sun gear, a planetary gear, an internal gear, an arm of a planetary gear device, and a bearing installation frame of a rotating body 1A.

FIG. 8 is a diagram showing a force relationship acting on a sun gear and a planetary gear in a combination of the rotating bodies 1A and 1B and the planetary gear device.

FIG. 9 is a diagram illustrating a force relationship acting on a sun gear, a planetary gear, and an internal gear when a planetary gear and an internal gear are combined by the leverage device;

FIG. 10 is a diagram showing an embodiment of a combination arrangement of rotating bodies 1A and 1B.

FIG. 11 is a diagram showing an embodiment in which the combination arrangement of the rotating bodies 1A and 1B is exchanged.

[Explanation of symbols]

Reference Signs List 1A Rotating body A with magnets fixedly arranged 1B Rotating body B with magnets fixedly arranged 2 Shaft of rotating body 9 Rotating body and rotating direction of gears 10A Sun gear 10B Planetary gear 10C Internal gear meshing with large gear 11 Gear teeth 12A Force of sun gear acting on contact point between sun gear and planet gear 12B Force of planet gear acting on contact point of sun gear and planet gear 12C Acting force of planet gear at contact point of planet gear and internal gear 13 Bearing 14 Arm of planetary gear device 15 Bearing frame of rotator A 16AB Contact point between sun gear of rotator A and planetary gear of rotator B 16BC Planetary gear of rotator B and internal gear Contact point 17 of C

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[Procedure amendment]

[Submission date] May 13, 1997

[Procedure amendment 1]

[Document name to be amended] Statement

[Correction target item name] Full text

[Correction method] Change

[Correction contents]

[Document Name] Statement

[Title of the Invention] A magnetic rotating engine having a planetary gear device

[Claims]

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION When accommodating a plurality of rotating bodies in a rotating device as shown in a magnetic rotating engine of a patent application filed on Feb. 25, 1997, application number (Japanese Patent Application No. 9-81782), BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic rotating engine that aims to provide rotational energy by acquiring rotational ability generated from an interaction force due to magnetic force of potential energy of each rotating body by using a planetary gear device as kinetic energy.

[0002]

2. Description of the Related Art A magnetic rotating engine of a patent application and application number (Japanese Patent Application No. 9-81782) filed on Feb. 25, 1997 has a structure in which a rotating body having magnets arranged and fixed is accommodated in a rotating device. The rotating body was rotated by the difference in the input force in the transmission of the force resulting from the difference between the radius of the rotating body and the gear radius and the acting force of the gear caused by the difference in the output. The rotating bodies and the rotating shafts of the gears were supported by an underframe.

[0003]

[Problem to be solved by the invention]
Using a plurality of rotating magnets, the resultant force of attractive, repulsive and sliding forces generated by the interaction of the magnets is transmitted to the contact points of each gear using the gears mounted on the rotating body. Changed the working force.

When a plurality of rotators 1B are arranged around the rotator 1A, each of the rotators has a rotational ability to rotate in the same direction. At that time, the distance from the resultant point of the magnetic force of the rotating body to the center of the rotating shaft of the rotating body,
By giving a difference in the distance from the center of the rotating shaft to the contact point of the gear on which the force acts, it is possible to give a difference also to the mutual acting force transmitted to the contact point of the gear, and convert it to rotary motion Met.

The present invention provides a distance between the above-described resultant point of the magnetic force of each rotating body to the center of the rotating shaft of the rotating body and a distance from the center of the rotating shaft to the contact point of the gear on which the force acts. Irrespective of the difference, the acting force transmitted to the contact point of each gear is equal due to the attractive force, repulsive force and sliding force of the magnet of the rotating body, and the rotating body is unstablely balanced to give a reduction effect to any of the acting force of the plurality of rotating bodies, breaking the balance of the acting force at the contact point of the gear, or the magnetic force
Kinetic energy, convert it to rotational motion, and rotate
This is a magnetic rotating engine for the purpose of providing energy.

[0006]

Means for Solving the Problems In order to achieve the above object, the present invention uses a planetary gear device as a rotating device, and uses a rotating shaft of a rotating body 1A and a rotating body 1B disposed around the rotating body 1A. The frame of the rotating shaft is separated, and the group of rotating bodies 1B can make a round around the rotating body 1A while rotating on the rotating arm of the planetary gear device.

[0007] The sun gear of the rotating body 1A meshes with the planetary gear of the rotating body 1B, and the planetary gear and the internal gear are meshed using the internal gear of the large gear internal meshing. Also,
The rotating shaft of the rotating body 1A is supported by the underframe, and the rotating shaft of the rotating body 1B is supported by the arm of the planetary gear device. Further, the internal gear is fixed.

At this time, the kinetic energy of each rotating body, which is generated by the attractive force, repulsive force, and sliding force of the magnetic force, which is potential energy, becomes a force acting on the contact point of each gear, and this force becomes an interaction force. Affects all rotating bodies.

[0009]

BEST MODE FOR CARRYING OUT THE INVENTION The magnets arranged and fixed to a plurality of rotating bodies are based on the example of the magnet arrangement shown in the patent application filed on Feb. 25, 1997, application number (Japanese Patent Application No. 9-81782). To create. As an example, a plurality of magnets are arranged and fixed to the rotating body 1A as shown in FIG. 2, and magnets are arranged and fixed to the rotating body 1B as shown in FIG. Also, a planetary gear device having a sun gear, a planetary gear, and an internal gear meshing with a large gear is used as the rotating device, and the rotating body 1A is equipped with a sun gear, and the rotating body 1B is equipped with a planetary gear. I do.

For the above reason, the rotating body 1A and the rotating shaft of the sun gear are supported by the underframe, and the rotating body 1B and
The shaft of the planetary gear is supported on the arm of the planetary gear set. And, the internal gear meshing with the planetary gear is fixed,
Further, the engagement between the planetary gear and the internal gear is made detachable by a shift lever device.

[0011]

An embodiment will be described below with reference to the accompanying drawings. In each figure, reference numerals 1A and 1B denote rotating bodies on which magnets are arranged and fixed. 2A and 2B are axes of the rotating body. 10A
Is a sun gear mounted on the rotating body 1A. 10B is a planetary gear mounted on the rotating body 1B. 10C is a fixed internal gear of a large gear internal gear, and a planetary gear 10B.
The engagement between the internal gear 10 </ b> C and the internal gear 10 </ b> C is made detachable by the shifting lever device 17. 12A, 12B, and 12C are forces acting on the contact points of the gears. 13A and 13B are bearings. 14 is an arm of the planetary gear set. 15 is a rotating body A
Bearing frame. 16AB is a sun gear 10A mounted on the rotating body 1A, and a planetary gear 10 mounted on the rotating body 1B.
This is the contact point where B engages. 16BC is planetary gear 10B
And the contact point where the internal gear 10C meshes.

FIG. 1 is a configuration diagram according to an embodiment of the present invention. 2 and 3 show a rotating body in which magnets are arranged and fixed in three stages in accordance with the arrangement and fixing of magnets shown in the previously filed patent application and application number (Japanese Patent Application No. 9-81782).

FIG. 4 shows the resultant magnetic force of two rotating bodies.
Direction and kinetic energy by magnetic force , equip the rotating body
The direction of the force acting on the sun gear 10A and the planetary gear 10B
It is a figure which shows a direction. And the same size, opposite
When the acting force 12A, 12B of the above acts on the contact point 16AB, the rotating body is in an unstable state and keeps a balance.

FIG. 5 shows a sun gear 10A and a planetary gear 10
B is a diagram showing the direction and direction of the force acting on the internal gear 10C. 12A is the acting force by the magnetic force of the rotating body 1A,
12B is the acting force by the magnetic force of the rotating body 1B. Then, as shown in the figure, when the planetary gear and the internal gear are brought into the meshing state by the shift lever 17, the acting force by the magnetic force of the rotating body 1B is divided into two points of contact points 16AB and 16BC of the planetary gear. Help. 12C is a reaction force to the divided force 12B.

FIG. 6 shows the internal gear 10 meshed with the large gear.
C, arm 14 of planetary gear set, bearing frame 1 of rotating body 1A
It is a figure which shows the Example of the positional relationship of No. 5.

FIG. 7 shows a sun gear 10 A and a planetary gear 10.
B, internal gear 10C, arm 14 of planetary gear set, rotating body 1A
FIG. 6 is a view showing an embodiment of a positional relationship with the bearing frame 15 of FIG.

FIG. 8 shows the sun gear 10 A and the planetary gear 1 in the combination of the rotating body 1 A, the rotating body 1 B, and the planetary gear device.
It is a figure which shows the force relationship which acts on 0B. 12A is the acting force by the magnetic force of the rotating body 1A, and is the acting force divided into four contact points of the sun gear. 12B is the acting force by the magnetic force of the rotating body 1B. The engagement between the planetary gear and the internal gear is in a disengaged state.

FIG. 9 shows that the planetary gear 1 is
In the case of the state meshing with 0B and internal gear 10C, thick
It is a figure which shows the force relationship which acts on the positive gear 10A , the planetary gear 10B, and the internal gear 10C. 12A is the acting force by the magnetic force of the rotating body 1A, and the sun gear and four planetary gears are in contact
A working force, which is divided into the contact point of the four-point to. 12B are each in the acting force by the magnetic force of the rotating body 1B, the planetary gear and the sun
The acting force is divided into two contact points of the gear and the planetary gear and the internal gear. Also, 12C is at contact point 16BC
It is a reaction force for the definitive split of action force 12B.

FIG. 10 is a view showing an embodiment of a combination position of the rotating body 1A and the rotating body 1B.

[0020]

The present invention is configured as described above, and has the following effects. As shown in Figure 5, from the energy saving laws, the planetary gear instrumentation
When the planetary gear and the internal gear are meshed with each other, the acting force of the planetary gear due to the magnetic force of the rotating body 1B is equal to the contact point 16.
It is divided into two points of AB and 16BC. The force 12C at the contact point 16BC between the planetary gear and the internal gear is a reaction force of the internal gear with respect to the acting force of the planetary gear, and the planetary gear is fixed to the internal gear, so that the rotating body 1B cannot rotate. The acting force at the contact point 16BC of the internal gear and the internal gear is canceled, and the work performed by the planetary gear at the contact point 16BC becomes zero. The rotating body 1B has the ability to do work, but does not work, and the magnetic force of the rotating body 1B
And the planetary gear and sun gear, and the planetary gear
By being transmitted to the two contact points of the internal gear, the sun gear
The acting force of the planetary gear to be given is halved.

The sun gear and the planet of the planetary gear device
The contact point 16
In AB, the acting force of the sun gear exceeds the acting force of the planetary gear, and the acting force due to the magnetic force of the rotating body 1A is transmitted to the rotating body 1B via the sun gear and the planetary gear, and at the same time as the rotating body 1A rotates, The rotating body 1B supported by the arm of the planetary gear unit rotates while rotating on the arm, and contacts the contact point 16 of the planetary gear.
With BC as a fulcrum and the contact point 16AB as a power point, it rotates around the rotating body 1A like a planet along the internal gear of the internal gear like a planet.

As an example, the operation is performed at the resultant point of the magnetic force of the rotating body.
The force to be used is (f), (a) of the rotating body 1A and the rotating body
1B is the distance from the resultant point of the magnetic force to the center of the rotating body, (r) is the radius of the gear, and (x) is the sun tooth.
The acting force of the sun gear acting on the point of contact between the car and the planetary gear,
(Y1) is planetary gear and sun gear, and (y2) is
Creation of planetary gears acting on two contact points of a star gear and an internal gear
The utility and create a (z) to the contact points of the planetary gear and the internal gear
Assuming that the reaction force of the internal gear to be used is as shown in FIG. 4, when the engagement between the planetary gear and the internal gear is released,
When the rotation direction of the rotating body 1A acts clockwise due to the magnetic force (f), the relation between the action and the reaction by the magnetic force (f) is similarly determined.
The rotation direction of the rotating body 1B in the engagement is also a clockwise acting force.
You. Comparing the rotation direction and the ease of rotation, the force moment (N1A) of the rotating body 1A is (N1A) = a × f (clockwise), and the force moment (N1B) of the rotating body 1B is N1B) = b × f (clockwise). The force acting at the contact point between two rotating bodies having the same rotation direction is an interaction force, and the directions are opposite.

As shown in FIG. 5, the sun gear 10 A, the planetary gear 10 B, and the internal gear 10 C
, As shown in the figure, the force relationship acting on the contact point 16AB between the sun gear 10A and the planetary gear 10B and the contact point 16BC between the planetary gear 10B and the internal gear 10C is as follows. Magnet of rotating body A at contact point 16AB
The acting force (x ) of the sun gear 10A due to the force (f) is x × r = a × f∴x = a × f / r.

Further, according to the law of conservation of energy, at the two contact points of the planetary gear, the operation by the magnetic force (f) of the rotating body B is performed.
The utility is divided into two parts. (Y1) is the contact point 16AB and (y2) is the acting force of the planetary gear at the contact point 16BC.
Then, the force moment of the rotating body 1B and the planetary gear 10B
The relation of (y1 + y2) × r = b × f holds for the acting force (y1, y2), and since y1 = y2, 2 × y1 × r = b × f , and the action of the planetary gear at the contact point 16AB Force (y
1) is y1 = b × f / 2r .

The acting force of the internal gear 10C at the contact point 16BC is a reaction force to the acting force of the planetary gear 10B.
is there. Then, the acting force (y2) of the planetary gear 10B acts.
Then, reaction force (z) is generated in the internal gear 10C, action
From the law of reaction , z = y2 y2 + (− z) = 0 , and the interaction forces acting on the planetary gear and the internal gear are equal in magnitude and opposite in direction.

The acting force (x) of the sun gear 10A at the contact point 16AB is given by the following equation.
Since the acting force (y1) is given by the equation, the sun gear and the planet
The difference between the gear forces is x-y1 = (a * f / r)-(b * f / 2r) = 1 / 2r * (2af-bf).

As an example, in a state where the planetary gear and the internal gear are meshed, the shapes of the rotating bodies 1A and 1B and the gear are (a = b
= R> 0), the acting force (x), (y) of each gear
1), (y2) and (z) are as follows: x = a × f / r = fy y1 = b × f / 2r = f / 2 y2 = b × f / 2r = f / 2 (10) z = f / 2 <11>, and the acting force (y2) of the planetary gear is canceled by the reaction force (z) of the internal gear.

The difference between the acting force (x) of the sun gear and the acting force (y1) of the planetary gear is expressed by the following equation: x−y1 = (a × f / r) − (b × f / 2r) = ff / 2/2 = f / 2 (12). Therefore, at the contact point 16AB, the acting force of the sun gear 10A is changed to the acting force of the planetary gear 10B.
(F / 2) power is superior.

This is because, at the same time when the rotating body 1A rotates clockwise, the force of (f / 2) is transmitted from the sun gear 10A to the planetary teeth.
Planetary gear 10 transmitted to the wheel 10B and fixed to the internal gear
To of B, as a fulcrum contact points 16bc, the contact point 16AB and force point, the counterclockwise force acts, the planetary gear is an internal gear 1
Planetary gear while rotating counterclockwise along the inner radius of 0C
The rotating body 1B supported by the arm of the device is also provided around the rotating body 1A.
Tour around.

The magnetic force (f) causes the rotating body 1 A to rotate.
When the rotation direction acts clockwise, the rotating body 1B also rotates clockwise.
The comparison of the individual force moments of the rotating body and the gear is a comparison of the direction of rotation and the ease of rotation.
The clockwise force moment (N1A) of the rotating body 1A is (N1A) = a × f = rf (clockwise) (13).

[0031] a force point contact points 16AB, the force of counterclockwise force moment of the sun gear 10A (N10A) is a work for force from the planetary gear 10B (y1), or formula
Et al, (N10A) = a × y1 = a × (b × f / 2r) = abf / 2r = rf / 2 ( counterclockwise) ▲ 14 is ▼, ∴ (N1A) = rf > (N10A) = rf / 2 ▲ 15 are ▼, clockwise force moment of the rotary body 1A by the magnetic force (f) is acting force Ru received from the planetary gears 10B to (y1)
It is larger than the counterclockwise force moment of the sun gear as the force.

Further, when the rotation bearing is in a fixed state,
Clockwise force moment (N1 ) due to the magnetic force (f) of the body 1B
B) is (N1B) = b × f = rf (clockwise) from the equation, and (N1A) = rf (clockwise) from equation ( 13 ) , and the two rotating bodies are unstable. Balanced in state
You. However, the rotating body 1B supported by the arm of the planetary gear device
The force moment of the sun gear, planetary gear and internal gear
Due to the effect of reducing the acting force, the planetary teeth at the contact point 16BC
The acting force (y2) of the vehicle is determined by the reaction force (z) of the internal gear.
From the formulas (10) and (11) , (N1B) = b × (y1 + y2-z) = b × f / 2 = rf / 2 (clockwise) . When the gears are meshed with each other, the force generated by the magnetic force (f) of the rotating body 1B supported by the arm of the planetary gear set.
(R × f) decreased to (r × f / 2)
New

Further, since the force of the counterclockwise force moment (N10B) of the planetary gear 10B about the rotation shaft 2B as a fulcrum is the acting force (x) received from the sun gear 10A ,
More, (N10B) = r × x = rf ( counterclockwise) ▲ 17 is ▼, and moment of force of the rotary body 1B, the planetary gear 10
Is the comparison of the moment of the force of B a formula (16) or (17)?
Et al, (N10B) = rf> ( N1B) = rf / 2 ▲ 18 are ▼, clockwise force motor of the rotating body 1B by a magnetic force (f)
The force exerts the acting force (x) received from the sun gear 10A.
Is smaller than the counterclockwise force moment of the planetary gear 10B.

In addition, a moment of the counterclockwise force of the planetary gear 10B (left N10), where the diameter of the planetary gear is a line segment, the contact point 16AB is a power point, and the contact point 16BC is a fulcrum.
AB to BC) is counterclockwise received from sun gear 10A
Because it is the action force (x), (left N10AB~BC) = 2r × x = 2r × af / r = 2af = 2rf ( counterclockwise) ▲ 19 is ▼.

Similarly, the moment of the clockwise force of the planetary gear 10B (the right N10AB to BC) is equal to the force of the rotating body 1B.
Since a clockwise acting force received from the magnetic force (f) (y1), (right N10AB~BC) = 2r × (y1 + y2-z) = 2r × bf / 2r = bf = rf ( clockwise) ▲ 20 ▼ ( Left N10AB to BC) = 2rf> (Right N10AB to BC) = rf , and the magnetic field of the rotating body 1B with the contact point 16BC as a fulcrum
Similarly, the clockwise force moment of the planetary gear 10B due to the force (f) is equal to the acting force (x) received from the sun gear 10A.
Force is smaller than the counterclockwise force moment.

[0036] to rotate by applying a force (f) to the rotating body, the greater the force (f) is a fast rotating happen naturally, the point of application of force from the rotation axis (r)
Then, the larger the force moment (N = r × f), the easier it is to rotate. From the expressions ( 13 ) and ( 16 ) , (N1A) = rf> (N1B) = rf / 2, that is, the rotating body 1A is easier to rotate than the rotating body 1B .

As described above, when the planetary gear 10B and the internal gear 10C are engaged with each other, the sun gear, the planetary gear,
The rotating body 1B
Of the rotating body 1A at the contact point 16AB and the acting force 12A generated by the magnetic force of the rotating body 1A,
A difference occurs in the acting force 12B generated from the magnetic force of B, and the rotating body 1A can rotate the group of rotating bodies 1B due to the rotation ability of the rotating body 1A, and can further provide rotation energy.

[Brief description of the drawings]

FIG. 1 is a configuration diagram illustrating a magnetic rotary engine according to an embodiment of the present invention.

FIG. 2 shows an embodiment in which the magnets of the rotating body 1A are fixedly arranged and gears.
, A left side view, and a right side view.

FIG. 3 shows an embodiment of a magnet arrangement and a gear of a rotating body 1B and gears.
, A left side view, and a right side view.

FIG. 4 shows two rotating gears 1A and 1B and a gear 10.
It is a figure which shows the force relationship which acts on A and 10B .

FIG. 5 is a diagram showing a force relationship acting on a sun gear, a planetary gear, and an internal gear in the planetary gear device.

FIG. 6 is a front view showing an embodiment of the positional relationship between the internal gear, the arm of the planetary gear device, and the bearing installation frame of the rotating body 1A , and
It is a side view.

FIGS . 7A and 7B are a front view and a side view showing an example of a positional relationship between a sun gear, a planetary gear, an internal gear, an arm of a planetary gear device, and a bearing installation frame of a rotating body 1A .

FIG. 8 is a diagram showing a force relationship acting on a sun gear and a planetary gear in a combination of the rotating bodies 1A and 1B and the planetary gear device.

FIG. 9 is a diagram showing a force relationship acting on a sun gear, a planetary gear, and an internal gear when a planetary gear and an internal gear are combined by a leverage device.

FIG. 10 is a view showing an embodiment of a combination arrangement of rotating bodies 1A and 1B.

[Description of Signs] 1A Rotating body A with magnets fixed and fixed 1B Rotating body B with magnets fixed and fixed 2 Shaft of rotating body 9 Rotating body and gear rotation direction 10A Sun gear 10B Planetary gear 10C gear 11 acting on the contact points of the teeth 12A sun gear and planet gears of the gear, the action force 12B contact point of the sun gear and the planetary gears of the sun gear, the parallel beauty, planet
The acting force of the planetary gear acting on the contact point between the gear and the internal gear 12C The reaction force of the internal gear against the acting force of the planetary gear at the contact point between the planetary gear and the internal gear 13 Bearing 14 Arm of planetary gear device 15 Rotating body Bearing frame of A 16AB Contact point between sun gear of rotating body A and planetary gear of rotating body B 16BC Contact point between planetary gear of rotating body B and internal gear C 17 Pulling device ────────── ───────────────────────────────────────────

[Procedure amendment]

[Submission date] July 28, 1997

[Procedure amendment 1]

[Document name to be amended] Statement

[Correction target item name] FIG.

[Correction method] Deleted ───────────────────────────────────────────── ────────

[Procedure amendment]

[Submission date] July 28, 1997

[Procedure amendment 1]

[Document name to be amended] Drawing

[Correction target item name] Fig. 4

[Correction method] Change

[Correction contents]

FIG. 4

[Procedure amendment 2]

[Document name to be amended] Drawing

[Correction target item name] Fig. 5

[Correction method] Change

[Correction contents]

FIG. 5

[Procedure amendment 3]

[Document name to be amended] Drawing

[Correction target item name] Fig. 8

[Correction method] Change

[Correction contents]

FIG. 8

[Procedure amendment 4]

[Document name to be amended] Drawing

[Correction target item name] Fig. 9

[Correction method] Change

[Correction contents]

FIG. 9 ────────────────────────────────────────────────── ───

[Procedure amendment]

[Submission date] September 11, 1997

[Procedure amendment 1]

[Document name to be amended] Statement

[Correction target item name] 0014

[Correction method] Change

[Correction contents]

FIG. 5 shows a sun gear 10A and a planetary gear 10
B is a diagram showing the direction and direction of the force acting on the internal gear 10C. 12A is the acting force by the magnetic force of the rotating body 1A,
12B is the acting force by the magnetic force of the rotating body 1B. Then, as shown in the drawing, when the planetary gear and the internal gear are brought into the meshing state by the shifting lever 17, the acting force by the magnetic force of the rotating body 1B is reduced to the two contact points 16AB and 16BC of the planetary gear.
The acting force is equally distributed to the points. Also, 12C is equally distributed
This is a reaction force to the applied force 12B .

[Procedure amendment 2]

[Document name to be amended] Statement

[Correction target item name] 0017

[Correction method] Change

[Correction contents]

FIG. 8 shows the sun gear 10 A and the planetary gear 1 in the combination of the rotating body 1 A, the rotating body 1 B, and the planetary gear device.
It is a figure which shows the force relationship which acts on 0B. 12A is the acting force due to the magnetic force of the rotating body 1A, and the four points of contact of the sun gear
The acting force is equally distributed to the points. 12B is the acting force by the magnetic force of the rotating body 1B. The engagement between the planetary gear and the internal gear is in a disengaged state.

[Procedure amendment 3]

[Document name to be amended] Statement

[Correction target item name] 0018

[Correction method] Change

[Correction contents]

FIG. 9 shows that the planetary gear 1 is
It is a figure which shows the force relationship which acts on sun gear 10A, planetary gear 10B, and internal gear 10C at the time of making 0B and internal gear 10C mesh. 12A is the acting force by the magnetic force of the rotating body 1A, which is equally distributed to the four contact points where the sun gear and the four planetary gears come into contact. 12B
Are the acting forces of the magnetic force of the rotating body 1B, and are equal to the contact points of the planetary gear and the sun gear, and the two contact points of the planetary gear and the internal gear.
It is the distributed acting force. 12C is the contact point 16B
It is a reaction force to the equally distributed acting force 12B in C.

[Procedure amendment 4]

[Document name to be amended] Statement

[Correction target item name] 0020

[Correction method] Change

[Correction contents]

[0020]

The present invention is configured as described above, and has the following effects. As shown in FIG. 5, according to the law of conservation of mechanical energy, when the planetary gear and the internal gear of the planetary gear device are engaged with each other, the acting force of the planetary gear due to the magnetic force of the rotating body 1B is in contact.
The points are equally distributed to two points 16AB and 16BC. The force 12C at the contact point 16BC between the planetary gear and the internal gear is:
This is the reaction force of the internal gear with respect to the operation force of the planetary gear. The planetary gear is fixed to the internal gear, so that the rotating body 1B cannot rotate. The work performed by the planetary gear at 16BC is zero. The rotator 1B has the ability to do work, but is not working, and the rotator 1B
Is transmitted to the two contact points of the planetary gear and the sun gear, and the planetary gear and the internal gear, whereby the acting force of the planetary gear applied to the sun gear is reduced by half.

[Procedure amendment 5]

[Document name to be amended] Statement

[Correction target item name] 0022

[Correction method] Change

[Correction contents]

As an example, the force acting on the resultant point of the magnetic force of the rotating body is represented by (f), and (a) of the rotating body 1A and (b) of the rotating body 1B are respectively separated from the resultant point of the magnetic force by the rotating body. (R) is the radius of the gear, (x) is the acting force of the sun gear acting on the contact point between the sun gear and the planetary gear,
(Y1) is the planetary gear and the sun gear, (y2) is the acting force of the planetary gear acting on the two contact points of the planetary gear and the internal gear, and (z) is the contact point of the planetary gear and the internal gear. When the reaction force of the internal gear acting on the planetary gear and the internal gear is disengaged as shown in FIG.
When the rotation direction of the rotating body 1A acts clockwise due to the magnetic force (f), similarly, the rotating direction of the rotating body 1B that has the action and reaction of the magnetic force (f) also becomes clockwise acting force. When comparing the direction of rotation and the ease of rotation , the rotating body
The moment (N1A) of the force of 1A is (N1A) = a × f (clockwise), and the moment (N1B) of the force of the rotating body 1B is also (N1B) = b × f (clockwise). Gear connection of two rotating bodies with the same rotation direction
The force acting on the touch point becomes the interaction force, and the direction is reversed.

[Procedure amendment 6]

[Document name to be amended] Statement

[Correction target item name] 0024

[Correction method] Change

[Correction contents]

According to the law of conservation of mechanical energy, at the two contact points of the planetary gear, the acting force due to the magnetic force (f) of the rotating body 1B is equally distributed, and the force (y1) is reduced to the contact point 16A.
Assuming that B and the force (y2) are the acting force of the planetary gear at the contact point 16BC, the moment of the force of the rotating body 1B and the acting force (y1, y2) of the planetary gear 10B are (y1 + y2) × r = Since the relationship of b × f is established and y1 = y2, 2 × y1 × r = b × f, and the acting force of the planetary gear at the contact point 16AB (y
1) is y1 = b × f / 2r.

[Procedure amendment 7]

[Document name to be amended] Statement

[Correction target item name] 0030

[Correction method] Change

[Correction contents]

When the rotating direction of the rotating body 1A acts clockwise due to the magnetic force (f), the rotating body 1B also becomes clockwise acting force, and the moments of the individual forces of the rotating body and the gear.
Is a comparison between the direction of rotation and the ease of rotation.
Then, the moment of the clockwise force is (+), and the counterclockwise force
When the moment of (−) is defined as (−) , rotation by magnetic force f
The moment of the clockwise force (+ N1A) of the body 1A is (+ N1A) = a × f = rf (clockwise) (13).

[Procedure amendment 8]

[Document name to be amended] Statement

[Correction target item name] 0031

[Correction method] Change

[Correction contents]

The force of the moment of the counterclockwise force of the sun gear 10A (−N10A) with the contact point 16AB as the power point
Is the force received from the rotating body 1B, that is , the acting force (y1) received from the planetary gear 10B. From the formula, (−N10A) = a × y1 = a × (b × f / 2r) = abf / 2r = rf / 2 (counterclockwise) １４14 ▼, ∴ (+ N1A) = rf> (− N10A) = rf / 2 １５15 ▼ , and the rightward force of the rotating body 1A due to the magnetic force (f)
The moment is the acting force (y) received from the planetary gear 10B.
It is the moment of the counterclockwise force of the sun gear whose force is 1)
Bigger.

[Procedure amendment 9]

[Document name to be amended] Statement

[Correction target item name] 0032

[Correction method] Change

[Correction contents]

Further , the rotation of the rotating bodies A and B relative to each other.
When the bearing is fixed to the underframe,

FIG. 4 shows the magnetic force (f) of the rotating body 1A.
The moment of the clockwise force (+ N1A) is
Et al, (+ N1A) = a × f = a rf (clockwise), the counterclockwise force of the rotating body 1A moment (-N1
The force of A) is obtained by rotating the gear of the rotating body 1A from the gear of the rotating body 1B.
Acting force (y), and (−N1A) = r × y = rf (counterclockwise) . In addition, the clockwise rotation due to the magnetic force (f) of the rotating body 1B
From the equation, the moment of force (+ N1B) is (+ N1B) = b × f = rf (clockwise) , and the force of the counterclockwise moment of the rotating body 1B is
This is the force (x) received from the gear of the rotating body A, and (−N1B) = rx = rf (counterclockwise) , and the individual rotating bodies are pressed by the gears of each other.
While acting as energy, they balance in an unstable state. However, as shown in FIG. 5, the mode of the clockwise force of the rotating body 1B supported by the arm of the planetary gear set is shown.
The action force (y2) of the planetary gear at the contact point 16BC is offset by the reaction force (z) of the internal gear due to the effect of reducing the action force of the sun gear, the planetary gear, and the internal gear. From (10 ) and ( 11 ) , (+ N1B) = b × (y1 + y2-z) = b × f / 2 = rf / 2 (clockwise) (16), and when the planetary gear meshes with the internal gear, the planetary gear The force due to the magnetic force (f) of the rotating body 1B supported by the arm of the device
The moment (r × f) is equal to reduced to (r × f / 2).

[Procedure amendment 10]

[Document name to be amended] Statement

[Correction target item name] 0033

[Correction method] Change

[Correction contents]

The counterclockwise moment (−N10B) of the planetary gear 10B with the rotation shaft 2B as a fulcrum .
Since the force is the acting force (x) received from the sun gear 10A, from the formula, (−N10B) = r × x = rf (counterclockwise) (17) , the moment of the clockwise force of the rotating body 1B And the planet
The comparison of the moment of the counterclockwise force of the gear 10B is given by the following equation:
From (6 ) and ( 17 ) , (+ N1B) = rf / 2 <(-N10B) = rf ( 18 ) , and the model of the clockwise force of the rotating body 1B due to the magnetic force (f).
Is smaller than the counterclockwise moment of the planetary gear 10B whose force is the acting force (x) received from the sun gear 10A.

[Procedure amendment 11]

[Document name to be amended] Statement

[Correction target item name] 0034

[Correction method] Change

[Correction contents]

The moment of the counterclockwise force of the planetary gear 10 B (−N 1 ), with the diameter of the planetary gear as a line segment, the contact point 16 AB as a power point, and the contact point 16 BC as a fulcrum.
Since the force of 0AB to BC) is the counterclockwise acting force (x) received from the sun gear 10A, (−N10AB to BC) = 2rxx = 2rxaf / r = 2af = 2rf (counterclockwise) 19 ▼.

[Procedure amendment 12]

[Document name to be amended] Statement

[Correction target item name] 0035

[Correction method] Change

[Correction contents]

Similarly, the contact point 16 between the planetary gear and the internal gear
The mode of the clockwise force of the planetary gear 10B with the BC as a fulcrum.
Since the force of the instrument (+ N10AB~BC) is the clockwise acting force received from the magnetic force (f) of the rotating body 1B (y1, y2), ( + N10AB~BC) = 2r × (y1 + y2-z) = 2r × bf / 2r = bf = rf (clockwise) is (20) , and from (19) and ( 20 ) , (+ N10AB to BC) = rf <(-N10AB to BC) = 2rf , and the contact point 16BC is a fulcrum. Moment of the clockwise force of the planetary gear 10B due to the magnetic force (f) of the rotating body 1B
G is the acting force (x) received from the sun gear 10A.
Smaller than the moment of the left-handed power to the force.

[Procedure amendment 13]

[Document name to be amended] Statement

[Correction target item name] 0036

[Correction method] Change

[Correction contents]

In order to apply the force (f) to the rotating body and rotate it, it is natural that the greater the force (f), the faster the rotation occurs. Then, the larger the moment of force (N = r × f), the easier it is to rotate. Then, the shapes of the rotating body and the gear are (a = b =
In the case of r), the rotating body 1A and the rotating body received from the magnetic force (f)
The comparison of the moment of the 1B force is given by the formulas (13) and (16).
Therefore , (+ N1A) = rf> (+ N1B) = rf / 2 , and therefore, the rotating body 1A is easier to rotate than the rotating body 1B. That is, the rotating body 1A rotates clockwise by itself, and
Sometimes, the rotating body 1B supported by the arm of the planetary gear unit and the planet
While rotating the gear counterclockwise, around the rotating body 1A
Circling clockwise along the internal law of the internal gear
I can . ────────────────────────────────────────────────── ───

[Procedure amendment]

[Submission date] October 15, 1997

[Procedure amendment 1]

[Document name to be amended] Statement

[Correction target item name] 0007

[Correction method] Change

[Correction contents]

As an example, the sun gear of the rotating body 1A meshes with the planetary gear of the rotating body 1B, and the planetary gear and the internal gear are meshed using the internal gear of the large gear internal meshing. The rotating shaft of the rotating body 1A is supported by the underframe, and the rotating shaft of the rotating body 1B is supported by the arm of the planetary gear device. Further, the internal gear is fixed. In addition,
The fixed internal gear meshes with the fixed external gear.
Possible as meshing gear. ────────────────────────────────────────────────── ───

[Procedure amendment]

[Submission date] February 25, 1998

[Procedure amendment 1]

[Document name to be amended] Statement

[Correction target item name] Full text

[Correction method] Change

[Correction contents]

[Document Name] Statement

[Title of the Invention] A magnetic rotating engine having a planetary gear device

[Claims]

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION A plurality of rotating bodies for arranging and fixing magnets, which are shown in a magnetic rotating engine of Japanese Patent Application No. 9-81782 filed on Feb. 25, 1997, are disclosed. When housed in the rotation device , each of the individual
Generated from the interaction force of magnetic force, which is the potential energy of the rotating body
The combined force of the twisting, attractive, repulsive , and sliding forces
The present invention relates to a magnetic rotary engine for obtaining kinetic energy, and at the same time, providing rotational energy.

[0002]

2. Description of the Related Art A magnetic rotating engine of a patent application and application number (Japanese Patent Application No. 9-81782) filed on Feb. 25, 1997 is used to accommodate a plurality of rotating bodies having magnets arranged and fixed in a rotating device. The rotation axis of each magnet rotating body is supported by the underframe
I have. Then, a plurality of magnets are rotated around the magnet rotor 1A.
When the rolling element 1B is arranged, each magnet rotating body has an individual
Attraction, repulsion, and slip generated from the interaction of magnets
Rotation in the same direction due to the combined force of
Rolling ability occurs. And equip it with the magnet rotating body and the rotating shaft.
When the gears are used to transmit to the contact points of each gear,
At the point of contact of the car, the gears interact with each other. That
The distance from the resultant point of the magnetic force of the rotating magnet to the center of the rotating shaft.
Separation from the center of the rotating shaft to the contact point of the gear where the force acts.
When a difference is given to the distance, the resultant force of the input magnetic force and the output
A difference can be given to the acting force of the gear. And
At the same time, the difference in input and output
Rotation of the magnet rotor by the difference in the mutual acting force of the gears
It is a rotary engine that converts to motion.

[0003]

As described above, the magnetic rotary engine shown in the previously filed patent application has a structure in which the magnetic force generated from the interaction between the magnets of the magnet rotating body and the resultant point of the magnetic force to the center of the rotating shaft. and distance tooth wheel acting force from hearts of the rotary shaft
To the contact point of each gear,
Breaking the balance of the mutual acting force of the transmitted gears, the rotation ability
To bring out.

However, attraction and repulsion of magnetic force as input
The resultant force of the force and the sliding force is
Contact when the gears are equally transmitted
The working force of the rotating gears is balanced, and the rotating magnet
You will not be able to turn.

[0005] Then, the above-mentioned acting force keeps the balance,
Input when the magnet rotor cannot rotate
The kinetic energy is obtained from the sum of the magnetic forces of the rotating magnets.
And convert it to rotational energy that becomes rotational motion
In order for any output to be transmitted to the contact point of the gear
To reduce the acting force of the gears and balance the mutual acting force of the gears.
There was a problem that it had to be broken.

[0006]

To achieve the above object of the Invention The present invention uses a planetary gear unit to the rotation device, the rotation
It is arranged around the rotation axis of the body 1A (FIG. 1) and the rotation body 1A.
Of the rotating body 1B (FIG. 2) supporting the rotating shaft
Then, the group of rotating bodies 1B is allowed to travel around the rotating body 1A while rotating on the rotating arm of the planetary gear device.

Then, as shown in FIG. 4, the sun gear of the rotating body 1A meshes with the planetary gear of the rotating body 1B,
The planetary gear and the internal gear are meshed using the internal gear of the large gear internal mesh. Also, as shown in FIG.
The rotation shaft of A is supported by the underframe, and the rotation shaft of the rotating body 1B is supported by the arm of the planetary gear device. Further, the internal gear is fixed. It should be noted that the fixed internal gear of the large gear can be used as a fixed external gear.

At this time, the combined force of the attractive force, the repulsive force, and the sliding force as the potential energy shown in FIG.
The kinetic energy of each rotating body generated as shown in FIG.
In addition, as shown in FIG. 11, the force acts on the contact point of each gear, and this force acts as an interaction force and affects all rotating bodies.

[0009]

BEST MODE FOR CARRYING OUT THE INVENTION A plurality of times for arranging and fixing magnets
The rolling body is created according to the example of the magnet arrangement shown in the patent application filed on Feb. 25, 1997, and the application number (Japanese Patent Application No. 9-81782). As an example, as shown in FIG.
Magnets are arranged and fixed to A, and shown in FIG.
The magnets are arranged and fixed as described above. FIG. 3 and FIG.
As shown in the above, using a planetary gear device equipped with a sun gear, a planetary gear, and a large gear internal gear,
The rotating body 1A is equipped with a sun gear, and the rotating body 1B is equipped with a planetary gear, and housed in a rotating device as shown in FIG.

For the above reason, the rotating body 1A and the rotating shaft of the sun gear are supported by the underframe, and the rotating body 1B and
The rotation shaft of the planetary gear is supported by the arm of the planetary gear device. So
Then, the internal gear is fixed, and the engagement between the planetary gear and the internal gear is made detachable by a shift lever device.

[0011]

An embodiment will be described below with reference to the accompanying drawings. In each figure, (1A, 1B) is a rotating body having magnets arranged and fixed. (2A, 2B) is the axis of the rotating body.
10A is a sun gear mounted on the rotating body 1A. 10B
Is a planetary gear mounted on the rotating body 1B. Also, 10C
Is a fixed large gear internal meshing internal gear, and the meshing of the planetary gear 10B and the internal gear 10C is performed by the shifting lever device 17.
Detachable with. (12A, 12B, 12C) are the forces acting on the contact points of the respective gears. (13A, 13
B) is a bearing. 14 is an arm of the planetary gear set.
Reference numeral 15 denotes a bearing frame of the rotating body 1A . 16AB is a contact point where the sun gear 10A mounted on the rotating body 1A meshes with the planetary gear 10B mounted on the rotating body 1B. 16BC
Is a contact point where the planetary gear 10B and the internal gear 10C mesh.

(FIGS. 1 and 2) show a rotation in which magnets are triple-connected and fixedly arranged in accordance with the arrangement and fixing of magnets shown in the previously filed patent application and application number (Japanese Patent Application No. 9-81782). Body.

FIG . 3 is a longitudinal section taken along section line α-α in FIG.
FIG. 3 is a plan view showing an arm 14 of the planetary gear device and a shaft of the rotating body 1A.
FIG. 4 is a diagram showing a positional relationship of a receiving frame 15 ; FIG.
Is a longitudinal sectional view taken along a cutting line β-β in FIG.
Car 10A, planetary gear 10B, internal gear 10C, planetary gear
FIG. 6 is a diagram showing a positional relationship between the mounting arm 14 and the bearing frame 15.
Thus, the planetary gear and the internal gear are in mesh with each other.

FIG . 5 is a block diagram according to an embodiment of the present invention.
It is. FIG. 6 is a longitudinal sectional view taken along a cutting line α-α in FIG.
Configuration diagram showing positioning of rotating body 1A and rotating body 1B
It is.

FIG . 7 shows the magnetic properties of the magnet rotating bodies (1A, 1B).
Indicates the direction and direction of the resultant force, and indicates the kinetic energy
Is the force acting on the sun gear 10A and the planetary gear 10B.
It is a figure which shows the direction and direction of. And the action of the sun gear
The force 12A and the acting force 12B of the planetary gear are
When opposite forces of equal magnitude act on each other,
The body is balanced in an unstable state.

FIG . 8 shows a sun gear 10A, a planetary gear 10
B is a diagram showing the direction and direction of the force acting on the internal gear 10C.
is there. 12A is the action of the sun gear by the magnetic force of the rotating body 1A
12B is the force of the planetary gear due to the magnetic force of the rotating body 1B.
Acting force. And the planetary gear and the internal gear meshed
In the state, the action of the planetary gear by the magnetic force of the rotating body 1B
The force is the two contact points of the planetary gear (16AB, 16BC)
The acting force is equally distributed to And again, contact point 16
The BC has an equal distribution of the acting force 12B of the planetary gears.
A reaction force 12C of the internal gear is generated.

FIG . 9 is a longitudinal section taken along section line α-α in FIG.
A plane view, the direction of the resultant force of the magnetic force of the magnet rotator of individual and countercurrent
Are indicated by arrows. At this time, the magnet rotating body 1A
, The combined force of the individual magnetic forces around the axis acts as a corner force
I do .

FIG . 10 shows a planetary gear 10B and an internal gear 10
Sun gear 1 for disengaging C
0A and the force relationship acting on the planetary gear 10B are indicated by arrows.
FIG. 12A is the sun due to the combined magnetic force of the rotating body 1A
This is the force acting on the gear, which is the contact force between the sun gear and the planet gear.
The acting force is equally distributed to the point of contact. Also, 12B
Is the acting force of the planetary gear due to the resultant force of the magnetic force of the rotating body 1B.
You . At this time, the rotating body keeps balance in an unstable state
You.

FIG. 11 shows the planetary gear 10 B and the internal gear 10.
It is a figure which shows the force relationship which acts on sun gear 10A, planetary gear 10B, and internal gear 10C at the time of making C into an engagement state with an arrow. 12A is the acting force of the sun gear by the resultant force of the magnetic force of the rotating body 1A, and is the acting force equally distributed to four contact points where the sun gear and the planet gear contact. 12B
Are the acting forces of the planetary gears due to the magnetic force of the rotating body 1B, and are the two points of the planetary gear and the sun gear, and the planetary gear and the internal gear.
This is the acting force equally distributed to the contact points. And 12C is
The acting force 12B of the planetary gear equally distributed to the contact point 16BC
Of the internal gear. FIG.
The direction and direction of the force transmitted to each gear of the star
In addition, the direction of rotation is indicated by arrows.

[0020]

The present invention is configured as described above, and has the following effects. Figure
As shown in FIG. 8, when the planetary gear and the internal gear of the planetary gear device are engaged with each other from the law of conservation of mechanical energy, the acting force of the planetary gear due to the magnetic force of the rotating body 1B is two points.
Are equally distributed to the contact points (16AB, 16BC) . Soshi
In addition, at the contact point 16BC between the planetary gear and the internal gear, a reaction force of the internal gear with respect to the action force of the planetary gear is generated.
The gear is fixed to the internal gear. The rotating body 1B is
It becomes impossible to rotate with these rotation capabilities, and the planetary gear
The acting force is offset by the internal gear, and at the contact point 16BC, the internal gear
The work performed by the planetary gear for the car is zero. Rotating body 1B
Has the ability to do work, but does not work, and the acting force of the magnetic force of the rotating body 1B is transmitted to the two contact points of the planetary gear and the sun gear, and the planetary gear and the internal gear. As a result, the acting force of the planetary gear applied to the sun gear is reduced by half.

The contact point 16 is reduced by the effect of reducing the acting force by the sun gear, the planetary gear, and the internal gear of the planetary gear device.
In AB, the acting force of the sun gear exceeds the acting force of the planetary gear, and the acting force due to the magnetic force of the rotating body 1A is transmitted to the rotating body 1B via the sun gear and the planetary gear, and at the same time as the rotating body 1A rotates, The rotating body 1B supported by the arm of the planetary gear unit rotates while rotating on the arm, and contacts the contact point 16 of the planetary gear.
With BC as a fulcrum and the contact point 16AB as a power point, it rotates around the rotating body 1A like a planet along the internal gear of the internal gear like a planet.

As an example, as shown in FIG. 7 and FIG.
In addition, the force acting on the resultant point of the magnetic force of the rotating body is represented by (f),
(A) of the rotating body 1A and (b) of the rotating body 1B are respectively distances from the resultant point of the magnetic force to the center of the rotating shaft , and (r)
Is the radius of the gear, (x) is the acting force of the sun gear acting on the contact point between the sun gear and the planetary gear, (y1) is the planetary gear and the sun gear, and (y2) is the two points of the planetary gear and the internal gear. Assuming that the acting force of the planetary gear acting on the contact point of the internal gear and the (z) is the reaction force of the internal gear acting on the contact point of the planetary gear and the internal gear, as shown in FIG. In the case where the engagement is released, when the rotating direction of the rotating body 1A acts clockwise due to the magnetic force (f), the rotating direction of the rotating body 1B, which is in the relation of the action and reaction by the magnetic force (f), is also changed. , Clockwise acting force. Comparing the rotation direction with the ease of rotation, the moment of force (N1A) of the rotating body 1A is (N1A) = a × f (clockwise), and the moment of force (N1B) of the rotating body 1B is also , (N1B) = b × f (clockwise). The forces acting on the contact points of the gears of the two rotating bodies having the same rotation direction are interaction forces, and the directions are opposite.

Also, as shown in FIG.
The sun gear, planetary gears, and internal gear
The contact point 16AB between the sun gear and the planetary gear, and
Force relation acting on contact point 16BC between planetary gear and internal gear
Is as follows. The acting force (x ) of the sun gear due to the magnetic force (f) of the rotating body 1A at the contact point 16AB is: x × r = a × fｆx = a × f / r.

According to the law of conservation of mechanical energy, at the two contact points of the planetary gear, the acting force due to the magnetic force (f) of the rotating body 1B is equally distributed, and the force (y1) is reduced to the contact point 16A.
B, and assuming that the force (y2) is the acting force of the planetary gear at the contact point 16BC, the moment of the force of the rotating body 1B and the planet
The relation (y1 + y2) × r = b × f is established for the acting force (y1, y2) of the gear, and since y1 = y2, 2 × y1 × r = b × f, and the planetary gear at the contact point 16AB Acting force (y
1) is y1 = b × f / 2r.

The acting force of the internal gear at the contact point 16BC is a reaction force against the acting force of the planetary gear . Then, when the acting force (y2) of the planetary gear acts, the internal gear
, A reaction force (z) is generated, and from the law of action and reaction, y2 = zy2 + (− z) = 0, and the interaction forces acting on the planetary gear and the internal gear are equal in magnitude and opposite in direction. It is.

The sun gear at the contact point 16 AB
The acting force (x) of the planetary gear is given by the following equation.
Since 1) is an equation, the difference between the forces of the sun gear and the planetary gear is as follows: xy1 = (a × f / r) − (b × f / 2r) = 1 / 2r × (2af−bf) is there.

As an example, when the planetary gear and the internal gear are engaged with each other, the rotating body 1A and the rotating body 1B, and the
When the shape is ( a = b = r> 0), the acting force (x), (y1), (y2), (z) of each gear is: x = a × f / r = fy1 = b × f / 2r = f / 2 y2 = b × f / 2r = f / 2 (10) z = f / 2 (11), and the acting force (y2) of the planetary gear is the reaction force (z) of the internal gear. Is offset by

Further, the difference between the acting force (x) of the sun gear and the acting force (y1) of the planetary gear is expressed by the following equation: ( x−y1 ) = (a × f / r) − (b × f / 2r) = f−f / 2∴ = f / 2 (12) Therefore, at the contact point 16AB, the sun
The acting force of the gear is superior to the acting force of the planetary gear by a force of (f / 2).

This is because, at the same time as the rotating body 1A rotates clockwise, the force (f / 2) is transmitted from the sun gear to the planetary gear.
Reached and fixed to the internal gear, the contact point 16
Counterclockwise with BC as fulcrum and contact point 16AB as power point
Of force acts.

When the rotating direction of the rotating body 1A acts clockwise due to the magnetic force (f), the rotating body 1B also acts clockwise, and the moment of the individual forces of the rotating body and the gear is compared. This is a comparison between the rotation direction and the ease of rotation.
Therefore, when the moment of the clockwise force is (+) and the moment of the counterclockwise force is (−), the rotating body 1 by the magnetic force f
The moment of the clockwise force of A (+ N1A) is (+ N1A) = a × f = rf (clockwise) (13)

A sun gear having the contact point 16AB as a power point
The force counterclockwise force moment (-N10A), the force received from the rotating body 1B, i.e., a working force from the planetary gear (y1), from the formula, (-N10A) = r × y1 = r × (B × f / 2r) = rbf / 2r = rf / 2 (counterclockwise) (14), and the clockwise moment of the rotating body 1A and the sun
A comparison of the moment of the counterclockwise force of the gear is given by the formula (▲ 13
▼, ▲ 14 ▼), ∴ (+ N1A) = rf> (− N1
0A) = rf / 2 ( 15 ) , and the magnetic force (f)
The clockwise moment of the rotating body 1A due to
Counterclockwise rotation of sun gear using force (y1) received from car
Greater than the moment of force.

Further, the rotating body 1A and the rotating body 1B
A state in which the rotating shaft is supported by an underframe, or shown in FIG.
When the planetary gear and the internal gear are in the disengaged state ,
From the formula, the moment (+ N 1A) of the clockwise force due to the magnetic force (f) of the rotating body 1A is (+ N1A) = a × f = rf (clockwise). Moment (-N1
The force of A) is that the sun gear of the rotating body 1A is the planet of the rotating body 1B.
The acting force (y) received from the gear , and (−N1A) = r × y = rf (counterclockwise). From the formula, the moment (+ N1B) of the clockwise force due to the magnetic force (f) of the rotating body 1B is (+ N1B) = b × f = rf (clockwise). The moment force is
Acting force on planet gears from sun gear of rotor 1A
( −N1B) = r × x = rf (counterclockwise), and the individual rotating bodies press the mutual gears equally.
While acting as kinetic energy, they balance in an unstable state. However, as shown in FIG.
When the planetary gear and the internal gear are engaged, the contact point 1
The acting force (y2) of the planetary gear at 6BC is
Canceled by the reaction force (z) and supported by the arm of the planetary gear unit.
The clockwise force moment of the rotating body 1B is expressed by the following equation.
From (, (10), ( 11)), (+ N1B) = b × (y1 + y2-z) = b × f / 2 = rf / 2 (clockwise) (16), the sun gear and the planetary gear, and , With internal gear
Due to the power reduction effect, the moment of force (r × f) due to the magnetic force (f) of the rotating body 1B supported by the arm of the planetary gear device.
Is reduced to (r × f / 2).

Further , a planetary gear having the rotating shaft 2 B as a fulcrum
Of, the power of the moment (-N10B) of the left-handed force, thick
Since it is the acting force (x) received from the positive gear , from the formula, (−N10B) = r × x = rf (counterclockwise) (17), and the moment of the clockwise force of the rotating body 1B and the contact point The comparison of the moment of the counterclockwise force of the planetary gear at 16AB is as follows from the equations (16) and ( 17): (+ N1B) = rf / 2 <(-N10B) = rf (18), and the magnetic force (f ) moment clockwise force of the rotating body 1B by the Yu star counterclockwise force moment is smaller than the gear acting force received from the sun gear (x) is the force.

The contact point 16 AB is set as a power point, and 16
With the BC as a fulcrum, the planetary gear
Since the force of the counterclockwise moment (−N10AB to BC) is the counterclockwise acting force (x) received from the sun gear , (−N10AB to BC) = 2r × x = 2r × af / r = 2af = 2rf (counterclockwise) (19).

Similarly, the contact point 16 between the planetary gear and the internal gear
The force of the clockwise moment of the planetary gear (+ N10AB to BC) with BC as the fulcrum is the clockwise acting force (y1, y2) received from the magnetic force (f) of the rotating body 1B, so that (+ N10AB) .About.BC) = 2r.times. (Y1 + y2-z) = 2r.times.bf / 2r = bf = rf (clockwise) (20). From the equations (19) and ( 20), (+ N10AB to BC) = rf <(− N10AB to BC) = 2rf, and the moment of the clockwise force of the planetary gear due to the magnetic force (f) of the rotating body 1B with the contact point 16BC as a fulcrum is
Similarly, the moment is smaller than a counterclockwise moment whose force is the acting force (x) received from the sun gear .

In order to apply the force (f) to the rotating body and rotate it, it is natural that the larger the force (f), the faster the rotation occurs. Then, the larger the moment of force (N = r × f), the easier it is to rotate. Then, the shapes of the rotating body and the gear are (a = b =
r), the comparison of the moments of the forces of the rotating body 1A and the rotating body 1B received from the magnetic force (f) is expressed by the following equations (13) and (16).
From ( ▼), (+ N1A) = rf> (+ N1B) = rf / 2, so that the rotating body 1A is easier to rotate than the rotating body 1B. That is, as shown in FIG. 12, the rotating body 1A rotates clockwise by itself, and at the same time, rotates the rotating body 1B and the planetary gears supported by the arms of the planetary gear device counterclockwise while rotating the rotating body 1A. The circumference can be circulated clockwise along the internal gear internal law.

As described above , the planetary gear device of the present invention
Magnetic rotating engine with mesh planetary gear and internal gear
When the sun gear of the planetary gear, the planetary gear, the action force reducing effect due to the internal gear, the rotational capability of the rotary body 1B by half, in the contact point 16AB, constantly magnetized rotary body 1A
Working force 12A (x) generated from force (f) and rotation
Acting force 12B generated from magnetic force (f) of body 1B
(Y), and the difference in the acting force causes the rotation
A can rotate the rotator 1B group, and at the same time,
Difference between the rotation ability of the rotating body 1A and the rotating ability of the rotating body 1B group.
And a rotational energy can be provided.

[Brief description of the drawings]

FIG. 1 shows an embodiment in which a magnet arrangement of a magnet rotating body 1A is fixed.
FIG.

FIG. 2 shows an embodiment in which an arrangement of magnets of a magnet rotor 1B is fixed.
FIG.

FIG. 3 shows an arm of the planetary gear set of FIG. 5 and a bearing of a rotating body.
A diagram showing the positional relationship of the installation frame and the vertical line of the cutting line (α-α).
It is sectional drawing .

4 is a sun gear, a planetary gear, an internal gear, and a planetary gear of FIG.
Shows the positional relationship between the arm of the car device and the bearing installation base frame of the rotating body
It is a figure and a longitudinal cross-sectional view of a cutting line (β-β).

FIG. 5 illustrates a magnetic rotary engine according to an embodiment of the present invention.
FIG.

FIG. 6 shows a positional relationship between the rotating bodies (1A and 1B) in FIG.
FIG. 3 is a vertical sectional view taken along a cutting line (α-α).

FIG. 7 shows a magnet rotating body (1A, 1B) and a gear (10A,
10B) and the transmission of the force by the rotating shaft
It is a figure which shows by an arrow.

FIG. 8 shows a sun gear and a planetary gear in a planetary gear device.
It is a figure which shows the force relationship which acts on a vehicle and an internal gear with an arrow.

FIG. 9 is a longitudinal sectional view taken along a cutting line α-α in FIG.
It is a figure which shows the direction and direction of the resultant force of the magnetic force of a rotating body with an arrow.
You.

FIG. 10 shows a state where the engagement between the planetary gear and the internal gear is released.
The force gear acting on the sun gear and the planetary gear
FIG .

FIG. 11 shows a state where the planetary gear and the internal gear are meshed.
Shows the relationship between the forces acting on the sun, planet, and internal gears.
FIG .

FIG. 12 shows the force transmitted to each gear of the planetary gear set and the teeth.
It is a figure which shows the rotation direction of a vehicle with an arrow.

[Description of Signs] 1A Rotating body A with magnets arranged and fixed 1B Rotating body B with magnets fixedly arranged 2 Rotating shaft 9 Rotating body and gear rotation direction 10A Sun gear 10B Planetary gear 10C Internal gear meshing with large gear 12A The acting force of the sun gear acting on the contact point of the sun gear and the planet gear 12B The acting force of the planet gear acting on the contact point of the sun gear and the planet gear and the contact point of the planet gear and the internal gear 12C Reaction force of the internal gear with respect to the acting force of the planetary gear at the contact point of the internal gear 13 Bearing 14 Arm of the planetary gear device 15 Bearing frame of the rotating body A 16AB Contact between the sun gear of the rotating body A and the planetary gear of the rotating body B Point 16BC Contact point between the planetary gear of the rotating body B and the internal gear C 17

[Procedure amendment 2]

[Document name to be amended] Drawing

[Correction target item name] All figures

[Correction method] Change

[Correction contents]

FIG.

FIG. 2

FIG. 3

FIG. 7

FIG. 4

FIG. 5

FIG. 6

FIG. 8

FIG. 9

FIG. 10

FIG. 11

FIG.

Claims (1)

[Claims] Patent application and application number (Fe. 9
The present invention relates to a magnetic rotating engine in which a plurality of magnets and a plurality of rotating bodies are accommodated in a rotating device of an arbitrary shape in a predetermined state. According to the present invention, a plurality of magnets and a plurality of rotating bodies are provided.
A magnetic rotating engine housed in a rotating device of any shape having a planetary gear set as a predetermined state.