Device for increasing the efficiency of mechanical motion in a stator-rotor system through the interaction of the magnetic fields of permanent magnets

Abstract

Device for increasing the efficiency of mechanical motion in the stator-rotor system by the interaction of magnetic fields of permanent magnets, comprising a rotor containing a set of permanent magnets rigidly attached to the cylindrical rotor surface and permanent magnets arranged on the stator surface within the limits of the projection of the path of motion of the rotor magnets, characterized in that the permanent magnets of the stator and the rotor are arranged relative to each other such that the zero lines of the magnets of the rotor and the stator are at different distances from the rotor axis of rotation.

Description

[0001] The invention relates to mechanical engineering and serves to increase the efficiency of mechanical motion in the stator-rotor system. The mechanical motion is generated by the interaction of the magnetic fields of permanent magnets. The invention makes it possible to increase the efficiency of energy generation, including electrical energy, for private, industrial, and public use.

[0002] A well-known device, the “permanent magnet motor”, RF patent Nº 2177201, consists of a non-magnetic housing, two spherical permanent magnets, a cubic permanent magnet slider, magnetic coils and an independent electrical power source.

[0003] The disadvantages of this known device are its complex design and low efficiency. The large number of rotating and rubbing surfaces increases the complexity of the design, and the four cyclically operating solenoids require considerable power consumption.

[0004] Another well-known device, the "magnetic motor," RF Patent No. 34826, consists of a non-magnetic housing, two magnets directed toward each other by like-poles, a connecting rod, a crankshaft, and a movable ferromagnetic shield. The ferromagnetic shield interrupts the interaction of the magnetic fields of the permanent magnets due to the reciprocating motion.

[0005] The disadvantage of the known device is the lack of a material capable of shielding or transforming the magnetic fields of the permanent magnets, so that the effect of the attractive force between the ferromagnetic shield and the permanent magnets of the rotor brings the device into a state of equilibrium and stops the mechanical movement.

[0006] The present invention aims to increase the efficiency of mechanical motion as a result of the cyclic interaction of the magnetic fields of the rotor's permanent magnets with the magnetic fields of the stator's permanent magnets. These have the properties of connecting, separating, restoring the strength, shape, direction, and symmetry of their magnetic fields. The invention relates to mechanical engineering and serves to increase the efficiency of energy generation, including electrical energy, for private, industrial, and public use.

[0007] The cyclic interaction of the rotor and stator magnetic fields is achieved by the property of the magnetic fields of magnets to constantly restore the shape, strength, and direction of their magnetic field after the interaction with the magnetic field of another magnet has ended. The description presents an embodiment in which the efficiency of the rotor's mechanical movement is increased by gravity. This results from the shift of the rotor's center of gravity and the position of the rotor plane at an angle to the Earth's surface. To increase the interaction of the stator and rotor magnetic fields, a variant of the arrangement of the stator magnet at an angle to the rotation plane of the rotor magnets is described.

[0008] The technical result is achieved by the fact that the useful model for increasing the efficiency of mechanical motion in the stator-rotor system through the interaction of the magnetic fields of permanent magnets consists of a rotor rotating around its axis. Permanent magnets are attached to the cylindrical surface of the rotor. These permanent magnets interact with the magnetic field of the stator magnet with their magnetic fields. The stator magnet is attached to the base with an elastic fastener. To increase the efficiency of the mechanical stator-rotor motion, the force generated by the interaction of the magnetic fields of the permanent magnets of the stator and rotor is converted into the centrifugal force of the rotor.The ability of magnetic fields to combine, separate, and restore the direction, strength, symmetry, and shape of parts of their magnetic field before, during, and after interaction with another magnet enables the cyclic operation of the device. These properties of permanent magnets allow the force to be maintained in the direction of the rotor's movement and the rotor's centrifugal force. When the rotor magnets approach the stator magnet, an attractive force arises between the magnets directed along the rotor's rotation, rotating the cylindrical generatrix. When the rotor magnet moves along the stator magnet's zero line, a force arises between the magnetic fields of the rotor and stator magnets due to the displacement of the trajectory of the rotor magnet's zero line relative to the stator magnet's zero line. This force restores the symmetry of the interaction of parts of their magnetic fields.Given the rigid attachment of the rotor magnet to its cylindrical surface, this is, on the one hand, the source of the centrifugal force of the rotor's motion and, on the other hand, the force that increases the resistance of the stator magnet's elastic attachment. During rotation of the cylindrical surface, the stator magnets alternately interact with one or two rotor magnets. This increases and decreases the force acting on the stator magnet's elastic attachment. This, in turn, leads to asymmetric interaction with the magnetic fields of the rotor magnets, preventing the occurrence of an equilibrium state of the forces of the interacting magnets. This increases the rotor's rotational efficiency.

[0009] In the device for increasing the efficiency of mechanical movement in the stator-rotor system by means of the interaction of the magnetic fields of permanent magnets, the sources for increasing the efficiency of the rotor movement are: - the force of the connection of the magnetic fields of magnets, - the force that restores the symmetrical interaction of parts of the magnetic fields of magnets and - the property of magnets to constantly restore the shape, strength and direction of their magnetic field after the interaction with the magnetic field of another magnet has ended.

[0010] The patent search did not find any technical solution from the prior art that is identical to all features of the proposed invention. Therefore, the proposed invention meets the requirement for patentability as a utility model—"novelty."

[0011] The information contained in the application documents is sufficient to realize the invention, so that the proposed utility model meets the requirement for patentability - "industrial applicability".

[0012] InFig. 1 - 9 is a schematic representation of a device for increasing the efficiency of the mechanical stator-rotor movement through the interaction of the magnetic fields of permanent magnets.

[0013] These include: 1 fixture base, 2 Rotor rotation axis, which is attached to the device base, 3 cylindrical surface line, 4.1, 4.2, 4.3 rotor permanent magnets 5, 5.1, 5.2, 5.3 stator permanent magnets 6 rigid attachment of the rotor magnets to the cylindrical surface line 7 resistance-generating attachment of the stator magnets to the device base 8 additional support point of the stator holder as a lever 9.1 Magnetic field of the rotor magnet 9.2 Magnetic field of the stator magnet 9.3 coupled magnetic field of rotor and stator magnets 10 Zero line of the rotor magnets 11 Zero line of the stator magnet 12 Projection of the trajectory of the rotor magnets 12.1 their zero lines 13 Rotation plane of the rotor magnets 14 Angle of the stator magnet position relative to the path of the rotor magnet neutral line 15 Inclination angle of the stator magnet neutral line to the rotation plane of the rotor magnets 16 Rotor center of gravity 17 Rotor balance weight 18 highest pivot point of the rotor center of gravity 19 lowest pivot point of the rotor center of gravity D Direction of movement of the rotor F Centrifugal force of the rotor F1 is the force directed towards the rotor rotation F2 is the force directed on the opposite side of the rotor rotation F3 is the force directed to restore the symmetrical interaction of the parts of the magnetic fields arising during the movement of the rotor magnet along the neutral line of the stator magnet F4 gravity F5 is the external force of the required size acting on the cylindrical rotor surface line F6 the resistance force of the stator magnet attachment, which creates an asymmetric interaction with the rotor magnets F7 the force that generates the overload of the stator magnet attachment L1 is the distance between the rotor magnets of the rigid mounting L2 is the length of the neutral line of the stator magnet L3 and L4 the distance between the boundaries of the neutral line of the stator magnet and the rotor rotation axis.

[0014] The Fig. 1a and Fig. Figure 1b shows a variant of the arrangement of the rotor and stator magnets symmetrical to the rotation axis. It shows the base of the device 1, the rotor rotation axis 2, the cylindrical generatrix 3, the rotor magnets 4, the stator magnets 5, and the rotor center of gravity 16. The fastening of the stator magnets in ( Fig. 1a and Fig. 1b) is not shown.

[0015] In Fig. Figure 2 shows a variant of the device that utilizes the force of gravity resulting from the displacement of the rotor's center of gravity. It includes the base of the device 1, the rotor rotation axis 2, the cylindrical rotor shape 3, and the permanent magnets of the rotor 4.1, 4.2, and 4.3, the stator permanent magnet 5, the rigid attachment of the rotor magnets to the cylindrical rotor centerline 6, the resistance-generating attachment of the stator magnets 7, the rotor magnet neutral line 10, the stator magnet neutral line 11, the rotor center of gravity 16, the highest pivot point of the rotor center of gravity 18, the lowest pivot point of the rotor center of gravity 19, the rotor centrifugal force F, force directed towards the rotor rotation F1, force directed towards the opposite side of the rotor rotation F2, force directed towards restoring the symmetrical interaction of the magnetic fields created during the movement of the rotor magnet along the neutral line of the stator magnet F3, gravity F4, external force of the required magnitude acting on the cylindrical rotor surface line F5.

[0016] The Fig. Figure 3 shows the stator and rotor magnetic fields, which do not interact with each other. 4.1 is the rotor magnet, 9.1 is the rotor magnetic field, 5 is the stator magnet, and 9.2 is the stator magnetic field.

[0017] In Fig. Figure 4 shows the magnetic fields of the stator and rotor interacting with each other. 4.1 is the rotor magnet, 9.1 is the magnetic field of the rotor magnet, 5 is the stator magnet, 9.2 is the magnetic field of the stator magnet, and 9.3 is the magnetic field created by the interaction of the magnets, which is the force F1 directed in the direction of rotation of the rotor.

[0018] In Fig. Figures 5 - 5a show the force restoring the symmetrical interaction of the magnetic field components and the resistance force of the stator magnet support, which creates an asymmetrical interaction with the rotor magnets. Where 3 is the cylindrical rotor surface line, 4.1 is the rotor magnet, 5 is the stator magnet, 6 is the rigid support of the rotor magnet to the cylindrical rotor surface line, 7 is the stator magnet support, which creates a resistance, 9.1 is the magnetic field of the rotor magnet, 9.2 is the magnetic field of the stator magnet, 9.3 is the coupled magnetic field of the rotor and stator magnets, 10 is the zero line of the rotor magnet, 11 is the zero line of the stator magnet, F3 is the force restoring the symmetrical interaction of the magnetic field components, and F6 is the resistance force of the stator magnet support, which creates an asymmetrical interaction with the rotor magnets.

[0019] The Fig. Figure 6 shows the angle of inclination of the stator magnet's zero line relative to the rotation plane of the rotor magnets. Here, 1 is the base of the device, 2 is the rotor rotation axis, 3 is the cylindrical rotor surface line, 4.1 is the rotor magnet, 5 is the stator magnet, 7 is the elastic mounting of the stator magnet, 13 is the rotation plane of the rotor magnets, and 15 is the angle of inclination of the stator magnet's zero line relative to the rotation plane of the rotor magnets.

[0020] In Fig. Figure 7 shows a variant of the stator magnet mounting using an additional support point. Here, 1 is the device base, 2 is the rotor rotation axis, 3 is the cylindrical rotor surface line, 4.1, 4.2, 4.3 is the rotor magnet, 5 is the stator magnet, 7 is the stator magnet holder, 8 is the additional support points of the stator holder that form a lever, F6 is the resistance force of the stator magnet holder, which creates an asymmetric interaction with the rotor magnets, and F7 is the overload force of the stator magnet holder.

[0021] In Fig. Figure 8 shows the relationship between the distances between the rotor magnets mounted on the cylindrical rotor surface lines and the length of the stator magnet's neutral line. Here, 1 is the device base, 2 is the rotor rotation axis, 3 is the cylindrical rotor surface line, 4.1, 4.2, and 4.3 are the rotor magnet, 5 is the stator magnet, 6 is the rigid support for the rotor magnet, 7 is the support for the stator magnet, L1 is the distance of the rigid support for the rotor magnet, and L2 is the length of the stator magnet's neutral line.

[0022] In Fig. Figure 9 shows the position of the stator magnet relative to the projection of the rotor magnet's trajectories and the angle formed by the stator magnet's neutral line relative to the projection of the rotor magnet's neutral line. Here, 3 is the cylindrical rotor surface line, 4.1 is the rotor magnet, 5 is the stator magnet, 7 is the stator magnet mount, 10 is the rotor magnet neutral line, 11 is the stator magnet neutral line, 12 is the projection of the rotor magnet boundary trajectory, 12.1 is the projection of the rotor magnet neutral line trajectory, 14 is the angle of the stator magnet neutral line relative to the rotor magnet neutral line trajectory, and L3 and L4 are the distances between the stator magnet neutral line boundaries and the rotor rotation axis.

[0023] The device for increasing the efficiency of mechanical movement in the stator-rotor system by interaction of the magnetic fields of permanent magnets works as follows ( Fig. 1). The external force F5 is applied to the cylindrical rotor surface line 3. A movement in the direction D occurs. The rotor is balanced with a weight 17. The center of gravity of the rotor 16 coincides with the axis of rotation of the rotor 2. The stator has a plurality of magnets 5, 5.1, 5.2, 5.3, which are arranged along the path of the rotor magnets. When the rotor magnet 4.1 ( Fig. 4) The force F1 acts on the rotor magnet 5, which, due to the connection of the magnetic fields of the rotor and stator magnets, is directed in the direction of rotation of the rotor. Figure 3 shows the magnetic fields of the rotor magnet 9.1 and the stator magnet 9.2 before the interaction between them. Figure 4 shows the interaction of the magnetic field of the rotor magnet 9.1 with the magnetic field of the stator magnet 9.2, which leads to the connection of the magnetic fields of the magnets 9.3 and the generation of force F1. The source of force F1 is the process of coupling the magnetic fields of the rotor and stator magnet. When the rotor magnet moves along the zero line of the stator magnet ( Fig. 5), as a result of the displacement of the zero lines of the permanent magnets of rotor 10 and stator 11 relative to each other, a force F3 arises between the magnetic fields of the magnets. This force aims to restore the symmetrical interaction of parts of their magnetic fields and the alignment of their zero lines, as well as a force F6 that changes the resistance of the stator magnet holder 7. The force F3 directed from the rotor magnet 4.1 to the stator magnet 5 is the source of the rotor centrifugal force F. The source of force F3 is the force that tends to restore the symmetrical interaction of parts of the magnetic fields of the rotor magnet (4.1) and the stator, which has a rigid attachment (6) to the cylindrical rotor surface line (3), and the stator (5), which is attached to the base of the device (1) by an elastic attachment that creates a resistance (7).

[0024] The further rotation of the cylindrical rotor surface line 3 causes the magnetic field of the stator magnet 5 to begin to interact with the magnetic field of the rotor magnet 4.2. This creates a force F1 that is directed in the direction of the rotor's rotation. The force F2 that also occurs is between the magnetic field of the stator magnet 5 and the magnetic field of the rotor magnet 4.1, directed against the rotation of the rotor. The permanent magnets of the rotors 4.2 and 4.3 interact with their magnetic fields in the same way with the magnetic field of the stator magnet 5. When the rotor magnet moves along the neutral line of the stator magnet, the force F3 acts on the rotor magnet. The length of the zero line of the stator magnet L2 ( Fig. 8) is greater than the distance between the rigid supports of the rotor magnets L1. As a result, the effect of the force F2 of magnet 4.1 is compensated by the force F1 of magnet 4.2, or the force F2 of magnet 4.2 is compensated by the force F1 of magnet 4.3. At the moments of interaction of the magnetic fields of the rotor magnets 4.1 and 4.2 and 4.2 and 4.3 ( Fig. 7) with the magnetic field of the stator magnet 5, the elastic bearing of the stator 7 experiences the effect of a doubled force F3. At the moment of interaction of the magnetic field of the stator magnet 5 with the magnetic field of a rotor magnet, for example 4.2, the effect of the force F3 is reduced. This leads to a change in the force of the elastic bearing of the stator F6. Thus, during the rotation of the cylindrical rotor surface line 3, an asymmetric interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnets occurs. This prevents the occurrence of an equilibrium state of interaction between the magnets of the device, and the efficiency of the rotor movement is increased. To increase the interaction between the magnetic fields of the rotor magnets and the magnetic fields of the stator magnet, the zero line of the stator magnet can be arranged at an angle to the rotation plane of the rotor magnets ( Fig. 6). Due to the three-dimensional nature of the magnetic fields of permanent magnets, the angle of inclination of the zero line of the stator magnet 15 relative to the rotation plane of the rotor magnets 13 increases the extent of the interaction between the magnetic field of the rotor magnet 4.1 and the magnetic field of the stator magnet 5 compared to the perpendicular position of the zero line of the stator magnet (5) relative to the rotation plane of the rotor magnets (13). In order to enhance the asymmetric interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnets and prevent the device from reaching an equilibrium state Fig. 7), the stator support 7 is designed with an excessive force load F7. Additional support points of the stator support 8 can have a resistance and a lever of the 1st, 2nd, or 3rd type. The stator magnet 5 ( Fig. 9) is located within the boundaries of the projection of the projection path of the rotor magnets 12. The boundaries of the neutral line of the stator magnet ( Fig. 9) can be located at different distances from the rotor rotation axis L3 < L4. In this case, the zero line of the stator magnet forms an angle 14 with the projection of the zero line path of the rotor magnets 4.1, 4.2, and 4.3. This increases the asymmetry of the interaction of the magnetic fields of the rotor and stator magnets, since the magnetic field strength increases towards the ends of the magnetic poles and decreases towards their zero line. The centrifugal force of the rotor F is calculated using the following formula: F=3(F1 + F2 + F3) + F5. Similarly, the rotor magnets 4.1, 4.2, and 4.3 interact with other stator magnets 5.1, 5.2, and 5.3. This results in a cyclic interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnets. This results in a centrifugal force of the rotor, which increases the efficiency of the mechanical movement in the stator-rotor system.

[0025] In Fig. 1a and Fig. Figure 1b shows a variant of the device in which the rotor magnets 4 and the stator magnets 5 are arranged symmetrically to the axis of rotation of the rotor 2.

[0026] In Fig. Figure 2 shows an embodiment for increasing the efficiency of mechanical movement in the stator-rotor system through cyclic interaction of the magnetic fields of permanent magnets using the gravitational force F4. In the embodiment shown, the center of gravity of the rotor 16 does not coincide with the axis of rotation 2. During the movement of the rotor center of gravity 16 from the highest rotation point of the rotor center of gravity 18 to the lowest rotation point 19, a gravitational force F4 acts on the cylindrical rotor surface line. The rotor receives an acceleration, which leads to an inertial movement of the center of gravity of the rotor 16 from the lowest rotation point 19 to the highest rotation point 18 after the center of gravity 16 has passed the lowest rotation point of the rotor 19. Due to the law of conservation of energy, the center of gravity of the rotor 16 cannot reach the highest point of rotation 18. In this position, the magnetic field of the rotor magnet 4.1 ( Fig. 4) is influenced by the magnetic field of the stator magnet 5. The further interaction of the magnetic fields of the stator and rotor magnets is similar to the variant described above. The centrifugal force of the rotor F is calculated using the following formula: F = 3(F1 + F2 + F3) + F4 + F5.

[0027] The base of the device 1, the cylindrical rotor surface line 3, the magnet holder of the stator 7 and the counterweight of the rotor 17 are made of a material that does not interact or only slightly interacts with the magnetic fields of the permanent magnets.

[0028] It is possible to construct a device in which the interacting magnet groups are arranged at different distances from the rotor's rotational axis. The number of interacting rotor and stator magnet groups can vary. The magnets can interact with their magnetic fields simultaneously or alternately.

[0029] The energy generated by the increased efficiency of the rotor's mechanical movement is transferred by any known means, including a soft or hard coupling to a gearbox or generator. Furthermore, the magnetic fields of the rotor magnets can be used to generate an induced electric current. For this purpose, the windings of the electric generator are arranged along the path of the rotor magnets to generate an induced electric current when traversed by the magnetic fields of the rotor magnets.

[0030] The increase in the efficiency of mechanical motion in the stator-rotor system through the interaction of the magnetic fields of permanent magnets is confirmed by practical experiments. The experimental device is designed according to Fig. 2. The base of the device 1 is made in the form of a frame made of stainless steel AISI 304.

[0031] The rotational axis of the rotor 2 is a freely rotating sleeve. This is attached to the base of the device. The cylindrical rotor surface line 3 is made of aluminum and has a diameter of 420 mm. The rotor permanent magnets are neodymium magnets, 20x40 mm rods, weighing 90 g. Stator magnets are 3 neodymium magnets, rectangular, measuring 75x20x5 mm. The additional load is lead plates with a total weight of 160 g. To obtain an external force of the same magnitude as required for the purity of the experiment, a device is located in the area of ​​the rigid attachment of the rotor magnet 4.2, which coincides with the center of gravity of the rotor 16. This device attaches an additional weight to the cylindrical rotor surface line during the movement from the highest point of the rotor rotation 18 to the lowest point 19. At the lowest pivot point of the rotor 19, the additional weight detaches from the cylindrical rotor surface line under its own weight.During the experiments, the cylindrical rotor surface line was positioned at an angle of 20 degrees to the Earth's surface. It is equipped with three neodymium permanent magnets, whose south poles point in the direction of the rotor's rotational axis. The distance from the zero line of the rotor magnets to the rotational axis is 235 mm. The distance between the rigid rotor magnet mounts is 60 mm. The center of gravity of the rotor 16 is located at the rigid attachment point of the rotor magnet 4.2. The stator magnet is located at the highest point of rotation 18. The stator magnet is secured with an elastic fiberglass material. The north pole of the stator magnet points in the direction of the rotor's rotational axis. The distance between the zero line of the stator magnet and the rotational axis is 245 mm.

[0032] The experiment consisted of two parts. In the first part, the stator magnet was missing. The additional weight was attached to the cylindrical rotor surface line at the location of its center of gravity 16. The center of gravity of the rotor was shifted 45 degrees from the highest pivot point 18 in the direction of rotation. The rotor began to move at this position. At the lowest pivot point of the rotor 19, the additional weight was released. The rotor received a force sufficient to overcome the highest pivot point 18. The rotor completed one complete rotation around its axis. During the second rotation, the center of gravity of the rotor could not reach the highest point of rotation of the rotor 18 due to the law of conservation of energy. This caused the rotor to move in the opposite direction. The rotor therefore completed one complete rotation around its axis.

[0033] In the second part of the experiment, the stator magnet was positioned along the movement of the rotor magnets at the highest pivot point 18 in the manner described above. Similar to the first part of the experiment, an additional weight was placed on the cylindrical rotor surface line at the location of its center of gravity 16. The center of gravity of the rotor was shifted 45 degrees from the highest pivot point 18 in the direction of rotation. The rotor began to move at this position. At the lowest pivot point of the rotor 19, the additional weight was released. The rotor received a certain force sufficient to overcome the highest pivot point 18. The rotor made three complete revolutions around its axis. During the fourth revolution, the center of gravity of the rotor could not reach the highest point of rotation 18 due to the law of conservation of energy. As a result, the rotor moved in the opposite direction.The rotor has therefore made three complete revolutions around its axis.

[0034] The comparison of the results obtained shows that the efficiency of the stator-rotor system, in this case gravity, can be increased by at least three times.

[0035] The experiment was carried out 75 times. The same results were obtained in all cases. This is a practical confirmation of the claimed technical result: increased efficiency in the stator-rotor system through the interaction of the magnetic fields of permanent magnets.

Claims

[1] Device for increasing the efficiency of mechanical movement in the stator-rotor system by the interaction of magnetic fields of permanent magnets, consisting of a rotor containing a set of permanent magnets rigidly attached to the cylindrical rotor surface line, and permanent magnets arranged on the stator surface line within the limits of the projection of the trajectory of the rotor magnets, characterized by that the permanent magnets of the stator and the rotor are arranged relative to each other in such a way that the zero lines of the magnets of the rotor and the stator are at different distances from the rotor axis of rotation. [2] Device according to claim 1, characterized by that an external force of the required magnitude is applied to the cylindrical rotor surface line. [3] Device according to claim 1, characterized bythat the elastic fastening of the stator magnet has a resistance directed both parallel and perpendicular to the plane of movement of the rotor magnets, even in the event of overload. [4] Device according to claim 1, characterized by that the elastic fastening of the stator magnets has an additional support point(s) including an overloaded support point forming a lever. [5] Device according to claim 1, characterized by that the stator has a fuse that prevents mechanical contact between the stator magnets and the rotor magnets. [6] Device according to claim 1, characterized by that the zero line of the stator magnets has an inclination angle relative to the plane of movement of the rotor magnets. [7] Device according to claim 1, characterized by that the boundaries of the neutral line of the stator magnet are at different distances from the rotor axis of rotation. [8] Device according to claim 1, characterized by that the length of the neutral line of the stator magnets is greater than the distance between the magnets mounted on the cylindrical rotor surface line. [9] Device according to claim 1, characterized by that the rotor is at an angle to the earth's surface and has a different center of gravity than the axis of rotation and / or additional weight. [10] Device according to claim 1, characterized by that the groups of interacting rotor and stator magnets are arranged at different distances from the rotor axis of rotation, with the possibility of simultaneous or sequential interaction. [11] Device according to claim 1, characterized by that the device is connected to a gearbox or a generator and / or the generator windings are arranged along the path of movement of the rotor magnets.

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