WO2004011803A1

WO2004011803A1 - Permanent magnet rotational energy amplifier

Info

Publication number: WO2004011803A1
Application number: PCT/JP2002/007718
Authority: WO
Inventors: Shunichi Matsuya
Original assignee: Shunichi Matsuya
Priority date: 2002-07-30
Filing date: 2002-07-30
Publication date: 2004-02-05
Also published as: AU2002368119A1

Abstract

With notches (5, 6) at the opposite end parts in the axial direction of an input rotor magnet (3) at an N pole facing an outer circumferential surface, an inner arcuate face causes N pole output slider magnets (21) to face it. The notches (5, 6) face the output slider magnet (21) alternately as the input rotor magnet (3) rotates. The output slider magnet (21) reciprocates by a repulsive force acting between the output slider magnet (21) and the input rotor magnet (3). A load is applied to a motor (14) by an attraction acting between the notches (5, 6) and the output slider magnet (21). Since efficiency is determined by the ratio between the dimension of the notches (5, 6) and the axial dimension of the input rotor magnet (3), output energy larger than input energy is obtained apparently. Energy can be outputted without causing any environmental pollution by returning a part of output energy back to input energy.

Description

Akinaga Hisashi Magnet-type rotating energy amplification device technology field

The present invention relates to a permanent magnet rotating energy amplification device equipped with an input rotating magnet and an output magnet.

Itoda

— 冃 Landscape technology

Conventionally, there are motives that use fossil fuels, or motives that use electric energy from hydro, thermal, nuclear power, and so on.

However, in the prime mover using the fossil fuel described above, the discharge gas from the combustion of fossil fuel and the like accumulates over a long period of time. In addition, natural pollution on the earth, which is caused by air pollution, marine pollution, deforestation, acid rain, and global warming, is progressing.

In addition, in areas where energy resources are relatively low, forests are cut down to obtain thermal, hydro, or other energy resources. Deforestation is progressing due to the deforestation of forests, which may be used as power or building dams.

In addition, electric energy generated by nuclear power generation has a problem in that it is not easy to dispose of used nuclear fuel and the like, and disposal of power generation facilities is a problem. As mentioned above, the prime mover using fossil fuels causes natural environmental destruction on the earth such as air pollution, marine pollution, deforestation, acid rain, and global warming. Motors that use electric energy from hydro, thermal, nuclear power, etc., cause problems such as desertification due to deforestation of forests, or treatment of spent nuclear fuel. However, there is a problem that the emission of energy causes pollution.

The present invention has been made in view of the above points, and has a permanent magnet type rotating energy that can output energy without causing pollution. It aims to provide a gear amplifier. Disclosure of the invention

The permanent magnet type rotary energy amplifying device of the present invention comprises a rotatable, substantially cylindrical input rotary magnet having a monopolar outer peripheral surface, and a rotary input rotary magnet. A rotating drive means for rotating and having a longitudinal dimension substantially equal to the axial dimension of the input rotating magnet, and a predetermined distance from the outer circumferential surface of the input rotating magnet via an air gap; And an output magnet having an arc-shaped cross section, which is disposed so as to be able to reciprocate in the axial direction of the input rotary magnet, and which is connected to the output magnet. A conversion unit for converting a reciprocating motion of the magnet into a rotating motion, wherein the input rotating magnet is configured such that both ends in the axial direction that are symmetric with respect to a central axis are connected to the input rotating magnet. of A plurality of cutouts are formed in the circumferential direction at a predetermined angle and in the axial direction at a predetermined size.The output magnet faces the outer peripheral surface of the input rotary magnet. The inner circular arc surface is formed as a single pole, and is disposed corresponding to each of the notches of the input rotating magnet, and is not more than the notch dimension of the notch of the input rotating magnet. It is provided so as to be able to reciprocate in the axial direction of the input rotary magnet by the dimension. When the input rotary magnet whose outer peripheral surface is formed as a single pole is rotated by the rotary drive means, notches are formed at both ends in the axial direction of the input rotary magnet. The notch alternately faces the output magnet, which is provided opposite to the outer peripheral surface of the input rotary magnet via a gap of a predetermined distance, so that the outer circumference of the input rotary magnet is The magnetism between the entire surface and the entire inner arc surface of the output magnet causes the output magnet to reciprocate in the axial direction of the input rotating magnet, and the notch in the input rotating magnet. The magnetism between the magnetism of the section and the inner arc surface of the output magnet is a load for rotating the input rotating magnet by the rotating drive means. As a result, the energy required for input is approximately proportional to the magnetism between the inner and outer peripheral surfaces of the notch of the input rotating magnet and the inner arc surface of the output magnet, and The energy to be applied is almost proportional to the magnetism between the entire outer peripheral surface of the input rotary magnet and the entire inner arc surface of the output magnet, so the energy required for input and the output The ratio of the energy to the input energy is approximately the ratio of the notch dimension of the notch of the input rotating magnet to the axial dimension of the input rotating magnet. The input rotary magnet is larger in the axial direction than the notch in the notch, so the input power is also larger. Since energy can be obtained, a part of the output energy is returned to the input energy, which does not cause any pollution. You can output lugi.

Further, in the permanent magnet type rotary energy amplifying device of the present invention, the conversion unit is provided with a crank guide device connected to the output magnet. . By providing a crank guide device in the conversion section, the reciprocating motion of the output magnet can be converted to output more efficiently.

Further, in the permanent magnet type rotary energy amplifying device of the present invention, the conversion unit is connected to one end of the output magnet in the longitudinal direction, and the conversion unit is connected to the output magnet. An output conversion magnet formed in a longitudinal shape along the longitudinal direction and having a longitudinal dimension corresponding to the reciprocating force of the output magnet, having an arc-shaped cross section, and a longitudinal dimension of the output conversion magnet. Has a dimension in the axial direction that is smaller than the reciprocating dimension of the output magnet, is coaxial with the input rotating magnet, and has an outer peripheral surface that is spaced from the inner arc surface of the output converting magnet by a predetermined distance. And a substantially cylindrical rotatable output rotating magnet opposed thereto, wherein the output converting magnet has a longitudinal direction in the width direction of the output converting magnet, and has an arcuate surface. The output conversion magnet is an arc-shaped conversion magnet formed into a single pole. A predetermined number of inner arc surfaces are provided adjacent to each other so that the inner arc surfaces alternately have different polarities in the longitudinal direction of the output rotary magnet. Is an arc-shaped rotating magnet having a longitudinal direction in the circumferential direction of the output rotating magnet, having a width dimension equal to the arc-shaped converting magnet described above, and having a single pole arc-shaped surface. A predetermined number of adjacent ring-shaped annular magnets are alternately arranged in the circumferential direction of the output rotating magnet so as to have different polarities alternately in the circumferential direction. They are provided adjacent to each other by a predetermined number in the axial direction. The output conversion magnet is formed in a longitudinal shape along the longitudinal direction of the output magnet and has an arc-shaped cross section having a longitudinal dimension corresponding to the reciprocating force of the output magnet. A substantially cylindrical output rotating magnet connected to one end in the longitudinal direction and having an axial dimension smaller than the longitudinal dimension of the output conversion magnet by the reciprocating dimension of the output magnet. The outer peripheral surface is coaxial with the input rotating magnet, and faces the inner arc surface of the output converting magnet via a gap at a predetermined distance. For this reason, when the output magnet reciprocates in the axial direction of the input rotating magnet, the output converting magnet reciprocates in the axial direction of the output rotating magnet in conjunction with the output magnet. The output rotating magnet is rotated by the magnetic force between the inner arc surface of each conversion magnet of the output rotating magnet and the outer arc surface of each rotating magnet of the output rotating magnet. . As a result, the reciprocating motion of the output magnet is brought into contact with the output rotating magnet in a non-contact manner by the magnetic force between the inner arc surface of the output converting magnet and the outer peripheral surface of the output rotating magnet. It can be converted to motion and converted to output energy.

In addition, the permanent magnet type rotary energy amplifying device of the present invention is provided on the center axis side of the input rotary magnet, the outer side of the output magnet, It is provided with a ferromagnetic material provided at least at one of the outside of the output conversion magnet and the central axis side of the output rotary magnet. Then, at least one of the central axis side of the input rotary magnet, the outside of the output magnet, the external side of the output conversion magnet, and at least one of the central axis side of the output rotary magnet. By providing a ferromagnetic material in the system, for example, when the device is enlarged, the input rotating magnet, the output magnet, the output converting magnet, and the output rotating magnet can be replaced by a small magnet. If it is necessary to manufacture by combining them, the magnetic force of the input rotary magnet, output magnet, output conversion magnet, and output rotary magnet should be converted to ferromagnetic material. Induction, the mutual magnetic force of the small magnets affects each other, and the magnetic force of the input rotating magnet, output magnet, output converting magnet, and output rotating magnet decreases. And can be prevented

In addition, the permanent magnet type rotary energy amplifier of the present invention has at least at least an input rotary magnet, an output magnet, an output conversion magnet, and an output rotary magnet. One of them is formed by doubly combining magnets with opposite poles. Then, at least one of the input rotating magnet, the output magnet, the output converting magnet and the output rotating magnet, and the magnet having the opposite pole opposite to the other magnet are doubled. The magnets that work at the part where the dowels are combined are the input rotating magnets, the output magnets, the output converting magnets and the output magnets. By stabilizing at least one of the magnets of the entire rotating magnet, the amount of demagnetization is reduced. As a result, long-term use becomes possible.

Further, the permanent magnet type rotary energy amplifying device of the present invention is provided in the axial direction of the input rotary magnet, and reciprocates the output magnet in the axial direction of the input rotary magnet. It has a guide part that can be devised in the direction. By providing a guide part for reciprocating the output magnet in the axial direction of the input rotary magnet in the axial direction of the input rotary magnet, the input rotary mechanism is provided. The magnetic force between the outer peripheral surface of the magnet and the inner arc surface of the output magnet can be converted to a force that causes the output magnet to reciprocate more efficiently.

Further, the permanent magnet type rotary energy amplifying device of the present invention is provided with a generator connected to the conversion unit and capable of obtaining an output by the rotary motion of the conversion unit. It is a thing. By connecting a generator that obtains output by the rotational motion of the converter to the converter, the outer peripheral surface of the input rotary magnet and the inner arc surface of the output magnet are connected. The magnetic energy between them can be output as power. Brief explanation of drawings

FIG. 1 is a longitudinal sectional view showing an embodiment of a permanent magnet type rotating energy amplifying device of the present invention, and FIG. 2 is a permanent magnet type rotating energy boosting device according to the present invention. FIG. 2 is a cross-sectional plan view showing the energy amplifying device. Best form to carry out the invention Hereinafter, the configuration of an embodiment of the permanent magnet type rotary energy amplifying device of the present invention will be described with reference to the drawings.

In FIG. 1, reference numeral 1 denotes a permanent magnet type rotary energy amplifier, and the permanent magnet type rotary energy amplifier 1 has a hollow, substantially cylindrical shape. It has a casing 2 as an enclosure of the horn.

In addition, an input rotor magnet 3 as an input rotary magnet is mounted in the casing 2. The input magnet 3 is formed in a substantially cylindrical shape having an axial dimension L and an outer diameter smaller than the inner diameter of the casing 2. The center axis is fitted to the center axis of the casing 2 so that it can rotate in the circumferential direction.o

In addition, the magnet 3 at the input port has a rotor magnet 3a whose outer peripheral surface is a single pole, for example, an N pole, and whose inner peripheral surface is a substantially cylindrical magnet having an S pole. The outer diameter of the rotor magnet 3a is substantially equal to the inner diameter of the rotor magnet 3a, and the outer circumference is an N pole, and the inner circumference is an S pole. By mounting the magnet 3b, the inner surface of the lower magnet 3a, which has a different polarity from the outer magnet, is connected to the outer surface of the magnet 3b. It is formed so as to be doubled facing. As a result, the outer peripheral surface is formed as a single pole, for example, an N pole, and the inner peripheral surface is formed as an S pole, and the inner peripheral surface of the mouth magnet 3a and the rotor magnet 3a are formed. The attractive force acting between the outer peripheral surface of b and the input rotor magnet 3 stabilizes the entire magnet and demagnetizes it. The amount is reduced so that it can be used for a long time. In addition, the inner peripheral surface of the rotor magnet 3a of the input magnet 3 at the input port, that is, the center axis side of the input rotor magnet 3 is made of a strong cylindrical material such as iron. The ferromagnetic material 4 to which the magnetic material 4 is attached induces the magnetic force of the input low-magnet 3 by the so-called magnetic shadow effect, so that the input low-magnet 3 Strengthen the magnetic force of Notch portions 5 and 6 are formed at both ends of the input rotor magnet 3 in the axial direction at two positions, respectively.

These notches 5 and 6 have a predetermined angle in the circumferential direction of the input port magnet 3, for example, 90 °, and a predetermined dimension 1 in the axial direction of the input port magnet 3. For example, cutouts are formed over the size of about 1/8 to 1/7 of the axial dimension L of the input rotor magnet 3, and the cutouts 5 and 6 are formed. In addition, the input rotor magnet 3 is formed symmetrically with respect to the central axis. The notch 5 and the notch 6 are formed at mutually symmetrical positions with respect to the center axis of the magnet 3 of the input port.

For this reason, the input magnet 3 has a shape in which both ends in the axial direction are two different places in the axial direction and are displaced differently in the axial direction, a so-called set-noc shape. It is formed.

Further, a rotating shaft 11 is connected to the center axis of the magnet 3 at the input port. The distal end of the rotating shaft 11 is connected to the outside of the casing 2 through a through hole (not shown) formed at one end of the casing 2 in the axial direction. And protrude, It is passed through the bearing 12 attached to the casing 2. The portion of the rotating shaft 11 protruding outside the casing 2 is inserted into the bevel gear 13.

On the same side as the projecting direction of the rotating shaft 11 of the casing 2, a motor 14 as a rotating drive means is mounted. The motor 14 is mounted vertically to the axial direction of the casing 2 and is driven by an external input (not shown).

Further, a bevel gear 15 is attached to the rotating shaft of the motor 14. The bevel gear 15 is connected to the bevel gear 13 of the rotating shaft 11, and when the motor 14 is driven, the bevel gear 15 rotates. Through the bevel gear 13 connected to the bevel gear 15, the input port magnet 3 is rotationally driven via the bevel gear 13.

The output slider magnet 21 as an output magnet is arranged around the input port magnet 3 in the casing 2 around the magnet 3 for example. It is set up. These output slider magnets 21 are formed so that the thickness dimension is slightly smaller than the difference between the inner diameter dimension of the casing 2 and the outer diameter dimension of the input rotor magnet 3. The center axis of the casing 2 has an angle of, for example, 75 ° and a cross section along the outer peripheral surface of the input rotor magnet 3. It is formed in an arc shape.

That is, as shown in FIG. 2, each output slider magnet 21 is a horizontal line and a vertical line passing through the center of the input low magnet 3 when viewed from the side. 7 and 5 respectively from the lines. Off each The output slider magnet 21 adjacent to the input rotor magnet 3 in the circumferential direction is, for example, relative to the center axis of the input rotor magnet 3. 15 ° apart. As a result, the output slider magnets 21 adjacent to the input port magnet 3 in the circumferential direction of the magnet 3 are hardly affected by the mutual magnetic force.

Each of the output slider magnets 21 is, for example, a magnet having an arcuate cross section in which the inner arc surface is formed on the N pole and the outer arc surface is formed on the S pole. The slider magnets 21a and 21b are formed so that the inner and outer peripheral surfaces having opposite polarities are opposed to each other so as to be doubled. For this reason, the output slider magnet 21, like the input rotor magnet 3, has an inner peripheral surface of the slider magnet 21 a and an outer peripheral surface of the slider magnet 21 b. By the attraction force acting between the magnets, the magnetism of the output slider magnet 21 as a whole can be stabilized and the amount of demagnetization can be reduced so that the magnet can be used for a long time It has become .

In addition, the output slider magnet 21 is provided at a predetermined distance, for example, a gap of about 5 m in between the outer peripheral surface of the input rotor magnet 3, that is, through an air gap. The notches 5 and 6 are attached to the corresponding number and position of the notches 5 and 6, respectively.

Here, the air gap between the outer peripheral surface of the input rotor magnet 3 and the inner arc surface of the output slider magnet 21 is determined by the input rotor magnet 3 and the input rotor magnet 3. Minimize the magnetic force between the output slider magnets 21 as much as possible to make them work more strongly The output slider magnet 21 has a surface facing the input rotor magnet 3, that is, the inner arc surface has a single pole, for example, an N pole, that is, an N pole. The input port is formed in the same polarity as the outer peripheral surface of the magnet 3. The output slider magnet 21 is formed to have a long dimension substantially equal to the axial dimension L of the magnet 3 at the input port.

Further, each output slider magnet 21 is housed in a case 22. This case 22 is formed in a box shape having a shape substantially similar to the outer shape of the output slider magnet 21, and each of the output slider magnets 21 Is that only the inner arc surface is exposed from the case 22 in the state of being housed in the case 22 and faces the outer peripheral surface of the magnet 3 at the input port. For this reason, the center position of each output slider magnet 21 in the longitudinal direction is set with respect to the input center position of the input rotor magnet 3 in the axial direction. Position the magnet 3 so that it is displaced in the axial direction.

A slider device 23 is attached to the outside of the case 22, that is, on the surface opposite to the magnet 3 at the input port. The slider device 23 is formed so as to protrude to the outer periphery of the casing 2, and is arranged corresponding to the number of output slider magnets 21. It has been done. Further, a plurality of the slider devices 23 are linearly arranged in the longitudinal direction of the case 22.

The outer peripheral surface of the casing 2 has a substantially rectangular shape at the axial position of the casing 2 of the slider device 23. 3 The holding members 24 are attached. Further, in each slider device 23, a through hole 25 is provided so as to penetrate in the thickness direction. In addition, a bearing 26 is provided around the entire inner periphery of the negative breamer 25 at a substantially equiangular angle in the circumferential direction of the through-hole 25. O Installed o

In addition, a linear slide shaft 27 serving as a holding shaft is passed through the tool through hole 25. The slide shaft 27 is provided over substantially the entire area in the axial direction of the casing 2, and the size of the slide shaft 27 depends on the diameter of the through hole 25. Also, it has a slightly smaller diameter dimension, and its outer peripheral surface is held in contact with the bearing 26. Further, the slide shaft 27 is also passed through a not-shown through-hole formed in the holding member 24 so that the slide shaft 27 can pass through the holding member 24. Is held.

The sliders 23, the bearings 26, and the slide shafts 27 are provided as guides 28 as guide parts. Is configured.

As a result, the slider device 23 takes the magnetic force between the outer peripheral surface of the magnet 3 at the input port and the inner arc surface of the output slider magnet 21. Since the attached case 22 moves along the slide shaft 27, the guide 28 is the output slider magnet 21. In the longitudinal direction, and in the axial direction of the input rotor magnet 3, that is, in the longer direction of the output slider magnet 21, for example, the input low magnet. Notches 1 and 2 have the same notch dimension 1 as the notch dimension 1 of the notches 5 and 6 It is possible to reciprocate slightly smaller dimensions. That is, the output slider magnet 21 has a slide stroke 1 _s which is a reciprocating dimension not more than the notch dimension 1 of the notch portions 5 and 6. Let's do.

In addition, on the opposite side of the input port magnet 3 in the longitudinal direction of the casing 2, a substantially cylindrical output port output magnet 3 serving as an output rotating magnet is provided. 1 is rotatably mounted on the same axis as the input rotor magnet 3. The output magnet 31 has an outer diameter approximately equal to that of the input magnet 3, for example, and the axial dimension is equal to the output slider. magnet 2 1 of the scan La Yi pass to collected by filtration chromatography click l _s is formed in a size corresponding to LesゝRu.

Further, the output rotor magnet 31 is configured by adjoining, for example, fifteen annular annular magnets 32 in the axial direction of the output rotor magnet 31. ing . In addition, these annular magnets 32 are constituted by rotating segment magnets 33 as rotating magnets whose outer peripheral surface is formed as a single pole of N pole or S pole. ing .

These rotating segment magnets 33 have a longitudinal direction along the circumference of the output port magnet 31, and the output port magnet 31. It is formed at a predetermined angle with respect to the central axis in plan view, for example, 90 °. The width dimension of these rotating segment magnets 33 is a width dimension corresponding to the slide stroke 1 _s of the output slider magnet 21, for example, Output slider magnet 21 Slide stroke of 1 half the size of 1 _s The center angle of the rotating segment magnet 33 is an angle obtained by dividing 360 ° which is the entire circumference by the number of the output slider magnets 21. These rotating segment magnets 33 are segment magnets 33a that are arc-shaped magnets whose outer and inner peripheral surfaces are monopolar. , .33b are formed by doubly joining the inner peripheral surface of the segment magnet 33a and the outer peripheral surface of the segment magnet 33b, which have mutually different polarities, facing each other. The annular magnet 32 is provided with four rotating segment magnets 33 in the circumferential direction, so that the magnetic poles on the outer peripheral surface are alternately different in polarity. As a result, the attraction force acting between the inner peripheral surface of the segment magnet 33a and the outer peripheral surface of the segment magnet 33b causes the ring magnet to move. 32 Stabilizes the overall magnetism and reduces the amount of demagnetization, so that the output port magnet 31 can be used for a long time. We have that.

Further, the annular magnet 32 is alternately rotated in a circumferential direction of the output port 31 by a predetermined angle, for example, 45 ° every time, so as to rotate the output port. An output rotor magnet 31 is configured such that a predetermined number, for example, 15 magnets are adjacent to each other in the axial direction of the magnet 31. That is, the output magnets 31 of the output port are arranged such that the odd-numbered rows in the axial direction are in the same state as each other, and the even-numbered rows in the axial direction are the same. The rows are 45 ° out of alignment with the odd-numbered rows so that they are in the same state.

The inner peripheral surface of the ring magnet 32, which is the inner peripheral surface of the output rotor magnet 31, that is, the center axis of the output port magnet 31 On the side, a cylindrical ferromagnetic body 34 such as iron is attached. The ferromagnetic material 34 induces the magnetic force of the output rotor magnet 31 by the so-called magnetic shading effect of iron or the like, thereby strengthening the magnetic force of the output port magnet 31. .

The other end of the input magnet in the output slider magnet 21, which is opposite to the rotating shaft 11 of the magnet 3, has an arcuate cross section through the connecting device 35. A case 36 is mounted. An output conversion slider magnet 37 serving as an output conversion magnet is housed in the case 36. Yes.

Here, the output conversion slider magnet 37 is, like the output slider magnet 21, stored in the case 36 on the inner arc surface. The light is exposed to the outside of the case 36, and the output is at a fixed distance on the outer peripheral surface of the evening magnet 31, for example, through a gap of about 5 mm through the gap. I'm crazy.

The output conversion slider magnet 37 is formed by a conversion segment magnet 38 as a conversion magnet. These conversion segment magnets 38 have the same width dimensions as the rotation segment magnets 33, and are flat with respect to the center axis of the output rotor magnet 31. It is formed at a predetermined angle in a plan view, for example, at an angle of 75 °, and has a longitudinal direction along the width direction of the output conversion slider magnet 37. .

Further, the conversion segment magnet 38 is a segment magnet 38a having a cross-section arc-shaped magnet in which the outer peripheral surface and the inner peripheral surface are monopolar. The inner surface of the segment magnet 38a and the outer surface of the segment magnet 38b, As a result, the conversion segment magnet 38 is formed so that the inner arc surface is a single pole of the N pole or the S pole. It is formed.

In addition, the output conversion slider magnet 37 is configured such that the conversion segment magnet 38 is formed such that the inner arc surface is alternately poled alternately in the longitudinal direction of the output conversion slider magnet 37. Are formed adjacent to each other by a predetermined number, for example, 17 pieces, that is, two pieces more than the rotating segment magnet 33. Attraction force acting between the inner peripheral surface of the segment magnet 38a and the outer peripheral surface of the segment magnet 38b stabilizes the magnetism of the entire conversion segment magnet 38 by the attraction force. Then, the amount of demagnetization is reduced, and the output conversion slider magnet 37 can be used for a long period of time.

Here, the conversion segment magnet 38 that is adjacent to the output conversion slider magnet 37 in the longitudinal direction is connected to the slide storage opening 1 _s by the conversion segment magnet 1. The number of output magnets divided by the width of the magnets 38 is greater than the number of rotating segment magnets 33 adjacent to the output low magnet 31 in the axial direction. You

Therefore, the output conversion slider magnet 37 is formed in a longitudinal shape along the longitudinal direction of the output slider magnet 21, and the output conversion slider magnet 37 is formed. Output slider, which is the force applied in the reciprocating direction of the magnet 21, the longitudinal dimension corresponding to the reciprocating force of the magnet 21, ie, the input port Magnet 3 and the output slider It is formed with a longitudinal dimension that is correlated with the magnetism and magnetic force between the iron magnet 21. A result of this, axial direction toward the size of the output ports one evening magnet 31, the output conversion scan La Lee Da also Ri by the longitudinal dimension of the magnet 37 rather Is the scan La Yi pass to collected by filtration chromatography click l _s worth Small form It has been.

When the reciprocating force of the output slider magnet 21 is large, the longitudinal dimension of the output conversion slider magnet 37 or the outer dimension of the output rotor magnet 31 is reduced. The reciprocating force of the output slider magnet 21 is increased by increasing the diameter, etc., in accordance with the reciprocating force of the output slider magnet 21. You can get out.

On the other hand, a slider device 41 is attached to the outer peripheral surface of the case 36 in the same manner as the case 22. The slider device 41 has a configuration similar to that of the slider device 23. That is, the bearings 42 are mounted above and below the through holes (not shown), and the slides are provided between the bearings 42. The shaft 27 is passed through, and the output conversion slider magnet 37 is linked to the output slider magnet 21 via the case 36 to be able to reciprocate. ing .

The conversion section 43 is composed of the output port overnight magnet 31, the output conversion slider magnet 37, and the slider device 41.

In addition, the input rotor magnet 3, the output slider magnet 21, the output rotor magnet 31, and the output conversion slider magnet 37 are made of neodymium-iron— The largest energy products, such as boron (Nd—Fe—B) magnets, are formed by relatively large magnets. Also, at one end of the casing 2 opposite to the motor 14 in the axial direction, there is an output port magnet 31 that is passed through a through hole (not shown). The rotating shaft 44 protrudes, and is inserted into the bearing 45 attached to the casing 2.

Then, the distal end side of the rotating shaft 44 is attached to a generator 46 as an output part. The generator 46 rotates to generate power when the magnet 31 rotates.

Next, the operation of the above embodiment will be described.

First, when the motor 14 is driven to rotate, the bevel gear 15 connected to the motor 14 rotates, and the input gear is rotated by the rotation of the bevel gear 15. The bevel gear 13 attached to the rotation shaft 11 of the rotor magnet 3 rotates, and the input rotor magnet 3 rotates.

As a result, the outer peripheral surface of the input rotor magnet 3 and the inner arc surface of the output slider magnet 21 of the same polarity face each other. Between the outer peripheral surface of the output slider magnet 21 and the inner arc surface of the output slider magnet 21, that is, the inner arc surface of the output slider magnet 21. A repulsive force F i acts in a direction perpendicular to the direction.

At this time, this repulsive force is output by the slider device 23 of the guide 28 and is output along the slide shaft 27 in the longitudinal direction of the slider magnet 21. As a result, the output slider magnet 21 is subjected to the repulsive force F toward the cutouts 5 and 6 in the longitudinal direction of the output slider magnet 21. It moves more and more. That is, the output slider magnet 21 facing the center axis of the magnet 3 at the input port moves in the same direction, and the pair of output sliders moves. The magnet 21 moves to the notch 5 side, and the other pair of output slider magnets 21 moves to the notch 6 side.

If the input rotor magnet 3 continues to be rotated in a fixed direction, the outer peripheral surface of the input rotor magnet 3 will be cut off by the cutouts 5 and 6 of the output slider magnet 21. The output slider magnet 21 reciprocates in the longitudinal direction of the output slider magnet 21 because it repeatedly faces the inner surface and the outer peripheral surface.

Therefore, ignoring the friction caused by the movement of the output slider magnet 21, the output energy due to the reciprocation of the output slider magnet 21 is ignored. The gear E 0 is approximately proportional to the repulsive force F.

Here, the magnetic distribution between the input rotor magnet 3 and the output slider magnet 21, and the outer peripheral surface of the input rotor magnet 3 and the output slider magnet 21. Since the air gap between the inner arc surface and the inner arc surface is considered to be substantially constant, the repulsion between the input port magnet 3 and the output slider magnet 21 is considered. If the forces F i are approximately equally distributed, the repulsive force is equal to the area S of the inner arc surface of the output slider magnet 21 facing the outer peripheral surface of the input port magnet 3. Is proportional to.

In addition, since the inner peripheral surfaces of the notches 5 and 6 of the magnet 3 at the input port are S poles, the inner peripheral surfaces of the notches 5 and 6 of the magnet 3 at the input port are used. Attraction and repulsion between the outer peripheral surface and the inner arc surface of the output slider magnet 21 Force (hereinafter Aspirate shall be the repulsive force) F ₂ is for work, Aspirate repulsion force F ₂ of this input B over evening Chi match for you load Ru magnet 3 is rotating mode one evening 14 Will be a load that causes the robot to rotate. On the other hand, since the repulsive force is applied to the central axis of the magnet 3 at the input port, the repulsive force does not become a load when the magnet 3 is rotated at the input port.

Therefore, ignoring the weight of the input rotor magnet 3 and the rotational friction, the input energy for rotating the motor rotor 14 is not absorbed. in here substantially Proportional to pull repulsive force F _2, the area of the inner circle arc surface of the notch 5, ejection you face the 6 scan la Lee da magnet 21 of the input b over data magnet 3 and S ₂ Then, the suction repulsion F ₂ is proportional to this area S ₂ o

Therefore, the efficiency 77 of the permanent magnet type rotary energy amplifier 1 is apparently "^ Eo / Er ^ Fi / FsSi / Ss". Since the width dimension W of the output slider magnet 21 is constant, the area S i and the area S ₂ are respectively set in the axial direction L of the input port magnet 3 in the axial direction. The efficiency of the permanent magnet type rotary energy amplifier 1 is apparently approximately 7 ^ because it is proportional to the notch size 1 of the notches 5 and 6. L / 1

That is, the notch dimension 1 of the cutouts 5 and 6 with respect to the axial dimension of the magnet 3 and the longitudinal dimension of the output slider magnet 21 is determined. As a result, the efficiency of the permanent magnet type rotary energy amplifier 1? ? Can be set In addition, due to the shape of the input rotor magnet 3, the axial dimension L of the input port magnet 3 was always larger than the notch dimension 1 of the notches 5 and 6. Therefore, the efficiency 77 of the permanent magnet type rotary energy amplifier 1 is 77 = L / 1> 1/1 / 1, which is apparently larger than the input energy. Output energy E. Get.

Further, in conjunction with the reciprocating motion of the output slider magnet 21, the output conversion slider magnet 37 reciprocates in the longitudinal direction of the output conversion slider magnet 37. Accordingly, the inner arc surface of each conversion segment magnet 38 of the output conversion slider magnet 37 is connected to the outer peripheral surface of each rotation segment magnet 33 of the output rotor magnet 31. opposite .

At this time, the inner circumferential arc surface of each conversion segment magnet 38 is placed in the same state as one in the longitudinal direction of the output conversion slider magnet 37 so that each rotation segment is in the same state. The magnet faces the outer peripheral surface of the magnet 33.

That is, the odd-numbered rows in the axial direction of the output port magnet 31 in the axial direction are in the same state, respectively, and the inner arcuate surface of the conversion segment magnet 38 is in the same state. The outer peripheral surfaces of the output rotor magnets 31 are opposed to each other, and the even-numbered rows in the axial direction of the output rotor magnets 31 are the rotating segment magnets 33 and 4 of the odd-numbered rows. In a state shifted by 5 °, the outer circumferential surfaces are opposed to each other between the inner circumferential arc surfaces of the two conversion segment magnets 38 whose inner arc surfaces are opposite in polarity to each other. .

For this reason, for example, the input port of the rotating segment magnet 33 Overnight, the odd-numbered rows from the magnet side provide repulsive force, and the even-numbered rows provide repulsive force and suction force to apply a constant rotational force to the output rotor magnet 31. This output port overnight The magnet 31 rotates in the circumferential direction. These repulsive forces are caused by the movement of the output conversion slider magnet 37 due to the movement of the output slider magnet 21, and the repulsive force becomes the attraction force and the attraction force becomes the attraction force. Each time the repulsive force is switched, the magnet 31 continues to apply a constant rotating force to the output port.

In addition, electric power is output by rotating the generator 46 by the rotation of the output rotor magnet 31.

As described above, according to the above-described embodiment, the input magnet between the input magnet 3 and the output slider magnet 21 whose input energy is approximately proportional. The difference between the magnetic energy due to the repulsive force F i and the magnetic energy due to the suction repulsive force F _{2, in} which the output energy E 0 is approximately proportional, is apparent. The output energy E is larger than the input energy. Because that was the that Ki out and give Ru this, the output error, channel formic Ε ₀ of some of the input error, channel formic: Ε Ri by the and this you return to _Σ, etc. I匕石fuel Because it does not generate any combustion gas or spent nuclear fuel, it can output energy without causing pollution.

In addition, the outer peripheral surface of the magnet 3 at the input port and the inner arc surface of the output slider magnet 21 are both formed into a pole, and the longitudinal direction of the output slider magnet 21 is formed. Enter the center position of the input magnet and the center of the input low magnet 3. The input rotor magnets 3 and the output slider magnets 21 are axially shifted from each other due to the nature of the magnets. Since the center position and the center position in the longitudinal direction are different from each other, that is, it is easy to move in the longitudinal direction of the output slider magnet 21, the input is performed. The output slider magnet 21 reciprocates due to the repulsive force Fi between the outer peripheral surface of the magnet 3 and the inner circular surface of the output slider magnet 21, The repulsive force F i between the outer peripheral surface of the input rotor magnet 3 and the inner arc surface of the output slider magnet 21 is more efficiently applied to the reciprocating motion of the output slider magnet 21. Conversion.

In addition, the reciprocating movement of the output slider magnet 21 is set to the input port — a guide 28 is provided in the axial direction of the input magnet 3 in the axial direction of the input magnet. As a result, the repulsive force between the outer peripheral surface of the input rotor magnet 3 and the inner arc surface of the output slider magnet 21 can be reduced more efficiently. This can be converted into a force that causes the magnet 21 to reciprocate.

Then, the output conversion slider magnet 37 is connected to the output slider magnet 21 via the connecting device 35, so that the output slider magnet 41 is connected via the slider device 41. The output conversion slider magnet 37 reciprocates in conjunction with the reciprocating motion of the output slider magnet 21, and the output segment of the rotating segment magnet 33 of the magnet 31 and the output magnet 33 are output. Because the output rotor magnet 31 rotates due to the attraction and repulsion between the conversion slider magnet 37 and the inner arc surface of each conversion segment magnet 38, Output mouth Isuzu Magnet 31 The reciprocating force between the outer peripheral surface and the inner arc surface of the output conversion slider magnet 37 or the attraction force allows the reciprocating motion of the output slider magnet 21 to be output in a non-contact manner. Russia over data Ru can a ₀ force energy-saving Ε out to reduce the loss of Ru good to etc. friction error, channel formate in the Ru can be converted to rotational movement of the magnet 31 at the output.

Also, by connecting the generator 46 to the output port of the converter 43 and the rotating shaft 44 of the magnet 31, the outer peripheral surface of the input port magnet 3 and the output slider magnet 21 are connected. The magnetic energy between the inner arc surface and the magnetic energy can be output as electric power.

Further, an input rotor magnet 3, an output slider magnet 21, an output rotor magnet 31 and an output conversion slider magnet 37 are respectively provided for the rotor magnets 3a, 3b, Slider magnets 21a, 21b Segment magnets 33a, 33b and segment magnets 38a, 38b are formed by doubly joining them with their opposite poles facing each other. As a result, the magnetism of each magnet as a whole is reduced by stabilizing the magnetism of each magnet as a whole with the attractive force acting between the different poles, reducing the amount of demagnetization and reducing the amount of demagnetization. The energy amplifier 1 can be used for a long period of time.

And, by receiving the rotating shafts 11 and 44 by the bearings 12 and 45, respectively, the energy generated by the friction caused by the rotation of the rotating shafts 11 and 44 is obtained. Loss can be reduced.

In addition, the output energy E is relatively large with only the permanent magnet type rotary energy amplifier 1 alone. Since a large input energy EI is not required, it is possible to reduce the energy cost. In addition, the permanent magnet type rotary energy amplifying device 1 is approximately efficient only in the axial dimension L of the input magnet 3 and the notch dimension 1 of the notches 5 and 6. Since 7? Can be determined, the permanent magnet rotary energy amplifier 1 can be reduced in size without having to make it larger than necessary.

The input low magnet 3, the output slider magnet 21, the output low magnet 31, and the output conversion slider magnet 37 use magnetic energy. When the magnetic force decreases due to consumption, these magnets can be demagnetized and then re-magnetized, so these input rotor magnets 3, output slider magnets 21, and output rotor magnets can be used. The motor magnet 31 and the output conversion slider magnet 37 can be easily recycled.

Also, the ferromagnetic materials 4 and 3 4 are attached to the input rotor magnet 3 and the output rotor magnet 31 respectively, for example, a permanent magnet type. Increase the size of the rotary energy amplifier 1 to increase the size of the input port magnet 3 or the output rotor magnet 31 to increase the size of these input ports. Even if the magnet 3 and the output port of the magnet 3 are formed by combining small magnets, the magnetic circuit of the magnet located on the inner side is adjacent to this magnet. To prevent the magnetic force due to the so-called neutron transfer, which is affected by and hindered by the magnets, from lowering, so that the input magnet 3 and the output port The magnetic force of the magnet 31 is induced to enhance the magnetic force of the input rotor magnet 3 and the output slider magnet 21. it can .

In the above embodiment, the output slider When converting the reciprocating motion of the magnet 21 into the rotating motion more easily, a crank guide device may be provided in the conversion section 43. In other words, a crank shaft (not shown) is converted into a rotational motion of each output slider magnet 21 by rotating the reciprocating motion of the output slider magnet 21 into each output slider magnet 21. And connect each small shaft, for example, a small bevel gear, and rotate each of these bevel gears. It is also possible to rotate a relatively large bevel gear with these bevel gears.

In addition, the input port magnet 3, the output slider magnet 21, the output port magnet 31, and the output conversion slider magnet 37 can simplify the configuration. However, at least one of them may be formed by double doping, or all may be formed by a single magnet.

In addition, in order to stabilize the output rotational motion, a not-shown flywheel or the like as a rotation maintaining means is used as an output rotor magnet 31. No matter where you install it.

Then, for example, a ferromagnetic material such as iron is attached to the outside of the output slider magnet 21 or the output conversion slider magnet 37, and this is attached. The magnetic force of the output slider magnet 21 or the output conversion slider magnet 37 is induced by the so-called magnetic shading effect of the ferromagnetic material, and these inputs are used. By strengthening the magnetic force of the rotor magnet 3 and the output slider magnet 21, the input port overnight magnet 3 and the center of the output rotor magnet 31 are strengthened. When ferromagnetic materials 4 and 34 are mounted on the shaft side The same operation and effect can be obtained.

The notches 5 and 6 of the magnet 3 at the input port are

D-Increase or decrease the number according to the number of rotations of evening magnet 3. For example, when increasing the number of rotations of the input rotor magnet 3, the number of notches 5 and 6 should be reduced and the number of rotations of the input magnet 1 should be reduced. When the size is reduced, more notches 5 and 6 are provided to enable the setting of the number of rotations.

Furthermore, the axial dimension L of the magnet 3 at the input port is determined by the efficiency required of the permanent magnet type rotating energy amplification device 1.

According to V, determine the size of the notch portions 5 and 6 with respect to the notch size 1.

The conversion unit 43 converts the reciprocating motion of the output slider magnet 21 into not only the electric power generated by the generator 46 but also the mechanical driving force and outputs the converted output. You can do it ο

If it is difficult to obtain external power when starting the motor 14 for the first time, for example, manually attach the rotating shaft 11 to a handle, etc. Then, the magnet 3 may be rotated for the first time.

In addition, the bearings 12, 45, etc. may be made to hold the rotating shafts 11, 44, for example, without magnetic contact. the, that can enter the load that by the friction, Oh Ru have a force out of the output load eyes ∎ You can at a reduced Ri by the, out rather than by good Ri efficiency force et ne le formic e ₀ .

Then, the motor 14 rotates the input low evening magnet 3 to rotate. If possible, the input rotor may be connected to the input magnet 3 in other ways, such as connecting directly to the rotating shaft 11, or the output rotor. In the case where the diameter of the magnet 31 can be formed larger than the diameter of the input rotor magnet 3, in this case, for example, a lever is used. The reciprocating motion of the output slider magnet 21 can be converted into the reciprocating motion of the output conversion slider magnet 37.

The guide 28 and the slider device 41 reciprocate the output slider magnet 21 and the output conversion slider magnet 37. If it is possible to do so, for example, it may be a non-contact type using magnetism or the like, and it is not limited to the above configuration.

As another embodiment, the outer peripheral surface of the input rotor magnet 3 and the outer peripheral surface of the output slider magnet 21 may have different polarities. In this case, the suction force between the outer peripheral surface of the input rotor magnet 3 and the inner arc surface of the output slider magnet 21 is reduced by the repulsive force F in the above-described embodiment. By causing the output slider magnet 21 to reciprocate instead of i, the same operation and effect as in the above-described embodiment can be obtained. .

(Example )

Hereinafter, examples of input and output of the permanent magnet type rotary energy amplifying device of the above-described embodiment will be described with reference to Table 1 or Table 5.

First, the input rotor magnet 3 and the output Anisotropy of the strobing magnet is provided for each of the magnet 21 for the slider, the magnet 31 for the output port, and the magnet 37 for the output conversion. I used a magnet. Table 1 shows the characteristics of this anisotropic storage magnet — ferrite magnet. (table 1 )

The input rotor magnet 3 has a substantially cylindrical shape with a length of 200 mm, a diameter of 220 mm and a notch of 30 mm, and the output slider magnet 21 has a width of not less than 30 mm. It has a cross-sectional shape of 135 mm in length and 100 x 2 mm in length.

In addition, the output conversion slider magnet 37 has an arc-shaped conversion segment magnet 38 having a length of 150 mm and a width of 30 mm, and the inner arc surface has an output conversion surface. The slider magnet 37 is formed so as to alternately become N-S in the longitudinal direction of the slider magnet 37. The output magnet 31 is an arc-shaped rotating segment having a width of 30 mm. Four magnets 33 and an annular magnet 32 of 240 mm diameter formed alternately in the circumferential direction of the output rotor magnet 31 so as to become N-S are provided at the output port overnight magnet. The output port was formed so as to be adjacent to the magnet 31 in the axial direction while rotating alternately by 45 ° in the circumferential direction of the magnet 31.

Also, the motor 14 has a voltage of 200 V, 0.75 kW. Using a phase induction motor, a generator 46 used was a 12 V, 55 A automotive generator.

Then, the motor 14 is rotated, and the number of rotations, voltage, and current of the input low magnet 3 and the generator 46 are changed to the commuter, voltmeter, and current, respectively. The input energy and the output energy were calculated. Table 2 shows the measurement results.

(Table 2) ―

As shown in Table 2, when the rotation speed of the magnet 3 is less than 500 rpm, the efficiency is not enough. ? Was less than 1, but when the rotation speed of the input rotor magnet 3 was set to 75 rpm or more, the efficiency became larger than 1 and the input magnet 3 When the number of revolutions was set to 124 O rpm, 7? = 0.23 / 0.066 = 3.48.

• As a result, the permanent magnet type rotation mechanism of the above-described embodiment is used. By using the energy amplifier 1, the outer peripheral surface and the output slur of the input low rocker 3 whose input and output power are proportional to each other The magnetic force between the inner arc surface of the inductor 21 and the output energy E 0 is proportional to the inner and outer peripheries of the cutouts 5 and 6 of the input row evening magnet 3 where the output energy E 0 is proportional. Due to the difference between the magnetic force between the inner circular surface of the surface and the output conversion slider magnet 37, the input power apparently larger than the input energy Ε _τ Energy E. You can see that is obtained.

In addition, the input port magnet 3, the output slider magnet 21, the output port magnet 31, and the output conversion slider magnet 37 are connected to the anisotropic strong magnet. Instead of a titanium-ferrite magnet, a neodymium-iron-boron magnet is used. First, the properties of the used neodymium-iron-polygon magnets are shown.

(Table 3)

In addition, an air gap between the input port magnet 3 and the output slider magnet 21, and the output port magnet 31 and the output conversion slider magnet Reduce the gap between 37 and 7.5 mm from 5 mm to 5 mm. At this time, the magnetic force between the input rotor magnet 3 and the output slider magnet 21 and the output port overnight magnet 31 and the output conversion slider magnet 37 When The magnetic force during this time is (7.55) ² = 2.25 times that of Coulomb's shellfish (J).

In addition, the axial dimension of the input rotor magnet 3 and the output rotor magnet 31 and the longitudinal dimension of the output slider magnet 21 and the output conversion slider magnet 37 are determined. The outer diameter of the magnet 3 for the input port and the magnet 31 for the output port is halved in each case. As a result, the output energy E is obtained from the equation of efficiency 7 ?. Only 4 x 0.5 = 2 times.

Table 4 below shows the improvements.

(Table 4)

As a result, according to the improvements shown in Table 4, the load on the input side is 20.25 times, while the load on the output side is 40.50 times. It can be seen that each improvement improves efficiency 7 7 twice. Input port Overnight When the rotation speed of the magnet 3 is set to 1,240,111, the input energy is £ ₁ , and the output energy E is. And efficiency? ? Table 5 shows the changes in the values. (Table 5)

Possibility of industrial use

As described above, the permanent magnet type rotary energy amplifier of the present invention is used as a prime mover for, for example, power generation, automobiles, various transportation small aircraft, ships, etc. It is done.

Claims

The scope of the claims

1. A rotatable, substantially cylindrical input rotary magnet having a single-pole outer peripheral surface;

A rotating drive means for rotating the input rotating magnet; and

The input rotary magnet has a longitudinal dimension substantially equal to the axial dimension of the input rotary magnet, and is provided on the outer peripheral surface of the input rotary magnet so as to face the input rotary magnet via a gap of a predetermined distance, and An output magnet having an arc-shaped cross section which is arranged to be able to reciprocate in the axial direction of the magnet;

A converter connected to the output magnet and converting a reciprocating motion of the output magnet into a rotary motion;

The input rotary magnet has opposite axially symmetrical ends with respect to a central axis at a predetermined angle in the circumferential direction of the input rotary magnet and in a predetermined dimension in the axial direction. It has a plurality of notches formed,

The output magnet has a monopolar inner arc surface facing the outer peripheral surface of the input rotating magnet, and is provided corresponding to each cutout of the input rotating magnet. A permanent magnet type rotation characterized by being provided so as to be able to reciprocate in the axial direction of the input rotation magnet by a dimension not more than the notch dimension of the notch of the input rotation magnet. Energy amplification device.

2. The conversion unit is a crank guide connected to the output magnet. Equipment

The permanent magnet rotary energy amplifying device according to claim 1, characterized by this.

3. The conversion part is connected to one end of the output magnet in the longitudinal direction, and is formed in a longitudinal shape along the longitudinal direction of the output magnet, and corresponds to the reciprocating force of the output magnet. An output conversion magnet having an arc-shaped cross section having a longitudinal dimension.

It has an axial dimension that is smaller than the longitudinal dimension of the output conversion magnet by the forward and backward dimensions of the output magnet, is coaxial with the input rotary magnet, and has an outer circumferential surface that is the inner circle of the output converter magnet. A substantially cylindrical rotatable output rotating magnet opposed to the arc surface via a gap at a predetermined distance;

The output conversion magnet is an arc-shaped conversion magnet having a longitudinal direction in the width direction of the output conversion magnet and having an arc surface formed as a single pole, and a longitudinal direction of the output conversion magnet. A predetermined number of inner circular arc surfaces are placed adjacent to each other so that they have different polarities alternately.

The output rotating magnet has a longitudinal direction in the circumferential direction of the output rotating magnet, has a width dimension equal to that of the arc-shaped converting magnet, and has a single-pole arc surface. A predetermined number of arc-shaped rotating magnets are alternately arranged in the circumferential direction of the output rotating magnet so as to have different polarities, and a ring-shaped annular magnet is alternately arranged in the circumferential direction at a predetermined angle. A predetermined number of them are placed adjacent to each other in the axial direction.

Claims 1 or 2 characterized by this The permanent magnet type rotary energy amplifying device described in (1).

4. At least one of the central axis side of the input rotary magnet, the outside of the output magnet, the external side of the output conversion magnet, and at least one of the central axis side of the output rotary magnet. Equipped with a ferromagnetic material

The permanent magnet type rotary energy amplifying device according to claim 3, characterized by this.

5. At least one of the input rotating magnet, the output magnet, the output converting magnet and the output rotating magnet is a double magnet with opposite poles. Was formed according to

The permanent magnet rotary energy amplifying device according to claim 3 or 4, characterized by this.

6. A guide portion is provided in the axial direction of the input rotating magnet and guides the reciprocating motion of the output magnet in the axial direction of the input rotating magnet.

The permanent magnet type rotary energy amplifying device according to any one of claims 3 to 5, which is characterized by the claims.

7. Equipped with a generator that is connected to the conversion unit and obtains output by the rotation of the conversion unit

The permanent magnet type rotary energy amplifier according to any one of claims 1 to 6, which is characterized by the claims.