Method for producing mechanical movement in a stator-rotor system by the interaction of permanent magnet magnetic fields and device for carrying out same

Abstract

The invention relates to mechanical engineering and is intended for producing mechanical movement in a stator-rotor system by the interaction of the magnetic fields of permanent magnets for conversion into energy, inter alia electrical energy, for domestic, industrial and public needs. The claimed device comprises a source of external force, a rotor, a stator, a group of permanent magnets, and a resilient fastening mechanism. The source of mechanical movement of the rotor is centrifugal force. The source of centrifugal force is the force of connection between the magnetic fields of the permanent magnets, a force that restores the symmetrical interaction of parts of the magnetic fields of the permanent magnets, and the capacity of permanent magnets to restore the shape, strength and direction of their magnetic field when interaction with the magnetic field of another magnet ceases. Asymmetrical interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnets prevents the device from assuming a state of equilibrium, therefore resulting in mechanical movement of the rotor.

Description

[0001] Method for obtaining mechanical motion in a stator-rotor system through the interaction of magnetic fields of permanent magnets and a device for its implementation

[0002] AREA OF TECHNOLOGY

[0003] The invention relates to mechanical engineering and is used to transform the force generated by the interaction of magnetic fields of permanent magnets into mechanical movement in a stator-rotor system. The invention will make it possible to obtain energy of various types, including electrical energy, which can be used for domestic, industrial and public needs.

[0004] The device “Engine on permanent magnets” is known, patent of the Russian Federation No. 2177201, consisting of a non-magnetic housing, two permanent spherical magnets, a cubic permanent magnet-slider, solenoids and an independent source of electric current.

[0005] The disadvantage of the known device is the complexity of the design and low efficiency. A significant number of rotating and rubbing surfaces complicate the design, and the presence of 4 cyclically operating solenoids requires significant consumption of...electric energy.

[0006] A device known as a “Magnetic engine” (RU patent No. 34826) consists of a non-magnetic housing, two magnets directed towards each other with the same poles, a connecting rod, a crankshaft and a movable ferromagnetic screen that interrupts the interaction of the magnetic fields of the permanent magnets as a result of the return movement.

[0007] The disadvantage of the known device is the physical absence of a material capable of shielding or transforming the magnetic fields of permanent magnets properly, as a result of which the action of the attractive force between the ferromagnetic shield and the permanent magnets of the rotor will bring the device to a state of equilibrium and stop the mechanical movement.

[0008] DISCLOSURE OF INVENTION

[0009] The present invention is aimed at obtaining mechanical movement as a result of cyclic interaction of magnetic fields of permanent magnets of the rotor with magnetic fields of permanent magnets of the stator, which have the properties of connection, disconnection, restoration of force, shape, direction and symmetry of their magnetic fields. The invention relates to mechanical engineering and is used to obtain energy, including electrical energy, for domestic, industrial and public needs.

[0010] The technical result of the invention consists in obtaining mechanical movement, in particular rotation of the rotor, arising as a result of the addition of the centrifugal force of the rotor, the source of which is the force aimed at restoring the symmetrical interaction of parts of the magnetic fields of the permanent magnets of the stator and rotor, and the force arising in the direction of rotation of the rotor, the source of which is the force formed when connecting the magnetic fields of the permanent magnets. The cyclic interaction of the magnetic fields, rotor and stator is achieved due to the property of magnetic. iodines of permanent magnets to restore the shape, strength and direction of their magnetic field after the interaction with the magnetic field of another magnet has ceased.The description presents a variant of obtaining mechanical movement of the rotor using the force of gravity, which occurs as a result of the displacement of the center of gravity of the rotor relative to the axis of its rotation and the location of the plane of rotation of the rotor at an angle relative to the surface of the Earth. To increase the volume of interaction of the magnetic fields of the stator and rotor, the description presents a variant of the location of the magnet, the stator at an angle relative to the plane of movement of the rotor magnets.

[0011] The technical result is achieved due to the fact that in the method for obtaining mechanical movement in the stator-rotor system, by means of the interaction of magnetic fields of permanent magnets, a centrifugal force of the rotor arises as a result of the action of the attractive force, at. interaction of magnetic fields of opposite direction and the force restoring the symmetry of the interaction of parts of the magnetic fields, arising at the displacement of the neutral line of the interacting magnets relative to each other. At the interaction of magnetic fields with poles of opposite polarity, their connection and, accordingly, displacement occur. After the end of the interaction of the magnets, the magnetic fields are separated and restore their shape, strength and direction. Thus, the sources of the force of mechanical movement of the stator-rotor are: the force of the connection of magnetic .fields of permanent magnets, the force restoring 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 ceased. The technical result is achieved due to the fact that the device for obtaining mechanical movement of the stator-rotor, through the interaction of magnetic fields of permanent magnets, consists of a rotor rotating around its axis, on the cylindrical generatrix of which permanent magnets are fixed, interacting with their magnetic fields with the magnetic fields of the stator magnets attached to the base using elastic fasteners. To obtain mechanical movement of the stator-rotor, the force formed 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 property of magnetic fields to connect, disconnect, restore the direction, strength, symmetry and shape of parts of their magnetic field before, at the moment and after interaction with another magnet, respectively, create cyclic operation of the device. The specified properties of permanent magnets allow to obtain a force in the direction of the rotor movement and the centrifugal force of the rotor. When the rotor magnets approach the stator magnet, an attractive force arises between the magnets directed along the rotation of the rotor, rotating the cylindrical generatrix of the rotor.When the rotor magnet moves along the neutral line of the stator magnet, due to the displacement of the trajectory of the neutral line of the rotor magnet relative to the neutral line of the stator magnet, a force arises between the magnetic fields of the rotor and stator magnets that restores the symmetry of the interaction of parts of their magnetic fields, which, due to the rigid attachment of the rotor magnet to its cylindrical generatrix, is the source of the centrifugal force of the rotor movement on the one hand, and the force that increases the resistance of the elastic fastening of the stator magnet, on the other hand. During the rotation of the cylindrical generatrix of the rotor, the stator magnets alternately interact with one or two rotor magnets, increasing and decreasing the force acting on the elastic fastening of the stator magnet, which creates an asymmetric interaction with the magnetic fields of the rotor magnets and prevents the occurrence of the equilibrium state of the device. Thus, the rotor moves.In a device for obtaining mechanical movement of a stator-rotor, through the interaction of magnetic fields of permanent magnets, the sources of movement are: the force of the connection of the magnetic fields of the magnets, the force restoring the symmetrical interaction of parts of the magnetic fields of the magnets and the property of permanent magnets to restore the shape, strength and direction of their magnetic field after the interaction with the magnetic field of another magnet has ceased.

[0012] The proposed invention meets the conditions of patentability of an invention: “novelty”, “inventive step” and “industrial applicability”.

[0013] DESCRIPTION OF FIGURES AND DRAWINGS

[0014] (Fig. 1-9) shows a diagram of a device for obtaining mechanical motion in a stator-rotor system by means of the interaction of magnetic fields of permanent magnets, where: the base of the device (G), the axis of rotation of the rotor attached to the base of the device (2), the cylindrical generatrix of the rotor (3), permanent magnets of the rotor (4.1, 4.2, 4.3), permanent magnets of the stator (5; 5.1; 5.2; 5.3), rigid fastening of the rotor magnets to the cylindrical generatrix of the rotor (b), fastening of the stator magnets to the base of the device (7), an additional support point for fastening the stator, forming a lever (8), the magnetic field of the rotor magnet (9.1), the magnetic field of the stator magnet (9.2), the connected magnetic field of the rotor and stator magnets (9.3), the neutral line of the rotor magnets, forming its neutral zone (10), the neutral line of the stator magnet, forming its neutral zone (11), projection of the trajectory of movement of the rotor magnets (12) and their neutral lines (12.1), the plane of rotation of the rotor magnets (13), the angle of the stator magnet relative to the trajectory of the neutral line of the rotor magnet (14), the angle of inclination of the neutral line of the stator magnet, forming its neutral zone, to the plane of rotation of the rotor magnets (15), the center of gravity of the rotor (16), the load for balancing the rotor (17), the highest point of rotation of the center of gravity of the rotor (18), the lower point of rotation of the center of gravity of the rotor (19), the direction of movement of the rotor D, the centrifugal force of the rotor. F, the force directed in the direction of rotation of the rotor F.1, the force directed in the direction opposite to the rotor rotation F2, the force directed at restoring the symmetrical interaction of parts of the magnetic fields, arising during the movement of the rotor magnet along the neutral line of the stator magnet F3, the gravitational force F4, the external force applied to the cylindrical generatrix of the rotor F5, the resistance force of the stator magnet mount, creating an asymmetrical interaction with the magnets of the rotor F6, the force applied to the stator magnet mount F7, the distance between the rigid mount of the rotor magnets L1, the length of the stator magnet coinciding with the length of its neutral line L2, the distance between the boundaries of the neutral line of the stator magnet and the axis of rotation of the rotor L3 and L4.

[0015] (Fig. 1a and 1b) shows a variant of the placement of a group of rotor and stator magnets symmetrically to the axis of rotation, where the base of the device (1), the axis of rotation of the rotor (2), the cylindrical generatrix of the rotor (3), the rotor magnets (4), the stator magnets (5), the center of gravity of the rotor (16). The fastening of the stator magnets on. (Fig. 1a and 1b) is not shown.

[0016] (Fig. 2) shows a variant of the device that uses the force of gravity that occurs as a result of the displacement of the rotor's center of gravity, where: the base of the device (1), the axis of rotation of the rotor (2), the cylindrical generatrix of the rotor (3), the permanent magnets of the rotor (4.1, 4.2, 4.3), a permanent magnet of the stator (5), a rigid fastening of the rotor magnets to the cylindrical generatrix of the rotor (6), fastening of the stator magnets creating resistance (7), a neutral line of the rotor magnets forming its neutral zone (10), a neutral line of the stator magnet forming its neutral zone (11), the center of gravity of the rotor (16), the highest point of rotation of the center of gravity of the rotor (18), the lowest point of rotation of the center of gravity of the rotor (19), the centrifugal force of the rotor F, the force directed in the direction of rotation of the rotor F1, the force directed in the direction opposite to the rotation of the rotor F2, the force aimed at restoring the symmetrical interaction of the magnetic fields arising during the movement of the rotor magnet along the neutral line of the stator magnet F3, the force of gravity F4, the external force applied to the cylindrical generatrix of the rotor F5.

[0017] In (Fig. 3) the magnetic fields of the stator and rotor are shown that do not interact with each other, where: rotor magnet (4.1), magnetic field of the rotor magnet (9.1), stator magnet (5), magnetic belt of the stator magnet (9.2).

[0018] (Fig. 4) shows the magnetic fields of the stator and rotor interacting with each other, where: rotor magnet (4.1), magnetic field of the rotor magnet (9.1), stator magnet (5), magnetic field of the stator magnet (9 / 2), magnetic field formed as a result of the interaction of magnets (9.3), force directed in the direction of rotation of the rotor FL

[0019] In (Fig. 5 - 5a) are shown: a force aimed at restoring the symmetrical interaction of parts of the magnetic fields and a resistance force of the stator magnet fastening, creating an asymmetrical interaction with the rotor magnets, where: a cylindrical generatrix of the rotor (3), a rotor magnet (4.1), a stator magnet (5), a rigid fastening of the rotor magnet to the cylindrical generatrix of the rotor (6), a fastening of the stator magnet, creating resistance (7), a magnetic field of the rotor magnet (9.1), a magnetic field of the stator magnet (9.2), a connected magnetic field of the rotor and stator magnets (9.3), a neutral line of the rotor magnet, forming its neutral zone (10), a neutral line of the stator magnet, forming its neutral zone (11), a force aimed at restoring the symmetrical interaction of parts of the magnetic fields F3, a resistance force of the stator magnet fastening F6.

[0020] (Fig. 6) shows the angle of inclination of the neutral line of the stator magnet, forming its neutral zone, relative to the plane of rotation of the rotor magnets, where: the base of the device (1), the axis of rotation of the rotor (2), the cylindrical generatrix of the rotor (3), the rotor magnet (4.1), the stator magnet (5), the elastic fastening of the stator magnet (7), the neutral line of the rotor magnet, forming its neutral zone (10), the neutral line of the stator magnet, forming its neutral zone (11), the plane of rotation of the rotor magnets (13), the angle of inclination of the neutral line of the stator magnet, forming its neutral zone, relative to the plane of rotation of the rotor magnets (15).

[0021] In (Fig. 7) a variant of fastening a stator magnet with an applied force is shown, where: the base of the device (1), the axis of rotation of the rotor (2), the cylindrical generatrix of the rotor (3), the rotor magnet (4, 1, 4.2 and 4.3), the stator magnet (5), the fastening of the stator magnet (7), the resistance force of the fastening of the stator magnet, creating an asymmetric interaction with the rotor magnets F6, the force applied to the fastening of the stator magnet F7.

[0022] In (Fig. 7a and 7b) variants of fastening the stator magnet are shown using additional support points and applied force, where: the base of the device (1), the axis of rotation of the rotor (2), the cylindrical generatrix of the rotor (3), the rotor magnet (4.1, 4.2 and 4.3), the stator magnet (5), the fastening of the stator magnet (7), additional support points of the stator fastening, forming a lever (8), the resistance force of the fastening, the stator magnet, creating an asymmetric interaction with the rotor magnets F6, the force applied to the fastening of the stator magnet F7.

[0023] In (Fig. 8) the distance between the rotor magnets mounted on the cylindrical generatrix of the rotor and the length of the stator magnet, coinciding with the length of its neutral line, are shown, where: the base of the device (1), the axis of rotation of the rotor (2), the cylindrical generatrix of the rotor (3), the rotor magnet (4.1, 4.2 and 4.3), the stator magnet (S'), the rigid fastening of the rotor magnets (6), the fastening of the stator magnet (7), the distance between the rigid fastening of the rotor magnets. L1, the length of the stator magnet, coinciding with the length of its neutral line L2.

[0024] (Fig. 9) shows the location of the stator magnet relative to the projection of the trajectories of the rotor magnet movement and the angle formed by the neutral line of the stator magnet relative to the projection of the trajectory of the neutral line of the rotor magnet, where: the base of the device (1), the axis of rotation of the rotor (2), the cylindrical generatrix of the rotor (3), the rotor magnet (4.1), the stator magnet (5), the stator magnet fastening (7), the neutral line of the rotor magnet (10), the neutral line of the stator magnet (1.1), the projection of the trajectory of the movement of the rotor magnet boundaries (12), the projection of the trajectory of the movement of the neutral line of the rotor magnet (12.1), the angle of the neutral line of the stator magnet relative to the trajectory of the movement of the neutral line of the rotor magnet (14), the distances between the boundaries of the neutral line of the stator magnet and the axis of rotation of the rotor L3 and L4.

[0025] DESCRIPTION OF THE OPERATING PRINCIPLE OF THE INVENTION

[0026] A device for producing mechanical motion in a stator-rotor system by means of interaction of magnetic fields of permanent magnets operates as follows (Fig. 1). An external force F5, for example, the physical force of a person, the force of wind, water, etc., is applied to the cylindrical generatrix of the rotor (3). Movement occurs in the direction D. The rotor is balanced using a load (17), the center of gravity of the rotor. (16) coincides with the axis of rotation of the rotor (2), and the stator has a group of magnets (5, 5.1, 5.2, 5.3) located along the trajectory of motion of the rotor magnets. When the rotor magnet (4.1), (Fig. 4) approaches the stator magnet (5), the rotor magnet is acted upon by force F1, directed in the direction of rotation of the rotor as a result of the connection of the magnetic fields of the rotor magnets to the stator. (Fig. 3) shows the magnetic fields of the rotor magnet (9.1) and the stator (9.2) before interacting with each other. (Fig. 4) shows the interaction of the magnetic field of the rotor magnet (9.1) with the magnetic field of the stator magnet (9.2), the result of which is the connection of the magnetic fields of the magnets (9.3) and the emergence of force FL. The source of force F1 is the process of connecting the magnetic fields of the rotor and stator magnets. When the rotor magnet moves along the neutral line of the stator magnet (Fig. 5), as a result of the displacement of the neutral lines of the permanent magnets of the rotor (10) and stator (11) relative to each other, between the magnetic fields of the magnates, force F3 arises, aimed at restoring the symmetrical interaction of parts of their magnetic fields and combining their neutral lines, and force F6, affecting the resistance of the fastening (7), as a result of which the position of the stator magnet (5) changes relative to the axis of rotation of the rotor (2). Force F3, directed from the rotor magnet (4.1) to the stator magnet (5), is the source of the centrifugal force of the rotor F.The source of force F3 is the force tending to restore the symmetrical interaction of parts of the magnetic fields of the rotor magnet (4.1), which has a rigid fastening (6) to the cylindrical generatrix of the rotor. (3) and the stator (5), attached to the base of the device (1) by an elastic fastening (7), with an applied force F7. Further rotation of the cylindrical generatrix of the rotor (3) leads to the fact that the magnetic field of the stator magnet (5) begins to interact with the magnetic field of the rotor magnet (4.2), a force F1 arises, directed towards the rotation of the rotor and a force F2, 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 rotor (4.2 and 4.3) interact with their magnetic fields with the magnetic field of the stator magnet. (5) in a similar way. When the magnet, rotor moves along the neutral line of the stator magnet, the force F3 acts on the rotor magnet.The length of the stator magnet, coinciding with the length of its neutral line L2 (Fig. 8) is greater than the distance between the rigid fastenings of the rotor magnets L1, as a result of which the action of the force F2 of the magnet (4.1) is compensated by the force F1 of the magnet (4.2), and the force F2 of the magnet (4.2), respectively, by the force F1 of the magnate (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 fastening of the stator (7) experiences the action of a doubled force F3, and at the moment of interaction of the magnetic field of the stator magnet (5) with the magnetic field of one rotor magnet, for example (4.2), the action of the force F3 decreases, which leads to a change in the force acting on the elastic fastening of the stator (F6) and, accordingly, changes the position of the stator magnet relative to the axis of rotation of the rotor.Thus, during the rotation of the rotor dilindrical generator (3), an asymmetric interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnets is created, which prevents the emergence of a state of equilibrium of the device.

[0027] In order to increase the volume of interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnet, the neutral line of the stator magnet, forming its neutral zone, can be located at an angle relative to the plane of rotation of the rotor magnets (fit. 6). Due to the three-dimensional nature of the magnetic fields of permanent magnets, the angle of inclination of the neutral line forming the neutral zone of the stator magnet (15) relative to the plane of rotation of the rotor magnets (13), increases the volume of interaction of the magnetic floor of the rotor magnet (4.1) with the magnetic field of the stator magnet (5), in comparison with the perpendicular arrangement of the neutral line / zone of the stator magnet (5) relative to the plane of rotation of the rotor magnets (13).

[0028] In order to increase the asymmetric interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnets and to prevent the occurrence of a state of equilibrium of the device (Fig. 7, 7a and 7b), a force F7 is applied to the stator mount (7), and additional support points of the stator mount (8) are made with the applied force and form a lever of the 1st, 2nd or 3rd kind, respectively.

[0029] The stator magnet (5) (Fig. 9) is located within the boundaries of the projection of the trajectory of motion of the magnets, the rotor (12). The boundaries of the neutral lines of the stator magnet (Fig. 9) can be at different distances relative to the rotor rotation axis L3 < 14. In this case, the neutral line of the stator magnet forms an angle (14) relative to the projection of the trajectory of motion of the neutral line of the rotor magnets (4.1, 4.2 and 4.3), which increases the asymmetry of the interaction of the magnetic fields of the rotor and stator magnets, since the magnetic field strength increases in the direction of the ends of the magnet poles and decreases in the direction of its neutral line. The centrifugal force of the rotor F is calculated using the formula: F≃3(F1 + F2 + F3) + F5. The interaction of the rotor magnets (4.1, 4.2 and 4.3) with other stator magnets (5.1, 5.2 and 5.3) occurs in a similar way. Thus,.a cyclic interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnets occurs, resulting in mechanical movement in the stator-rotor system, taking into account the conditional use of external force.

[0030] (Fig. 1a and 1b) shows a version of the device with the placement of rotor magnets (4) and stator magnets (5) symmetrically to the axis of rotation of the rotor (2).

[0031] In (Fig. 2) one of the embodiments of the device for obtaining mechanical motion in the stator-rotor system, by means of the interaction of magnetic fields of permanent magnets using the gravitational force F4, is shown. In the presented embodiment, the center of gravity of the rotor (16) does not coincide with the axis of rotation (2). When the center of gravity of the rotor (16) moves, from the highest point of rotation of the center of gravity of the rotor (18) to the lowest point of rotation (19), the gravitational force F4 acts on the cylindrical generatrix of the rotor. The rotor receives acceleration, as a result of which, after the center of gravity (16) passes the lowest point of rotation of the rotor (19), an inertial movement of the center of gravity of the rotor (16) from the lowest point of rotation (19) to the highest point of rotation (18) occurs. 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 stator magnet (5) acts on the magnetic field of the rotor magnet (4.1) (Fig. 4).Further interaction of the magnetic fields of the stator and rotor magnets occurs similarly to the above-described variant. The centrifugal force of the rotor F is calculated by the formula: F≃. : 3(F1 + F2 + F3) + F4 + F5

[0032] The base of the device (1), the cylindrical generatrix of the rotor (3), the stator magnet mount (7), and the rotor balancing weight (17) are made of a material that does not interact with the magnetic fields of permanent magnets, or interacts only slightly.

[0033] It is possible to design a device where the interacting groups of magnets are located at different distances relative to the rotor rotation axis. The number of interacting groups of rotor and stator magnets can be different, and the magnets can interact with their magnetic fields simultaneously or alternately.

[0034] The energy generated as a result of the mechanical movement of the rotor is transmitted by any known method, including through a soft or hard connection with a gearbox or generator. Also, magnetic fields of the rotor magnets can be used to obtain induced electric current. For this purpose, windings of the electric generator are placed along the trajectory of the rotor magnets to obtain induced electric current when they are crossed by the magnetic fields of the rotor magnets.

Claims

AMENDED CLAUSE received by the International Bureau on May 11, 2025 (11.05.2025) CLAUSE OF INVENTION 1. A method for obtaining mechanical movement in a stator-rotor system by means of the interaction of magnetic fields of permanent magnets consists in connecting an external force applied to the rotor with the force of interaction of the magnetic fields of permanent magnets rigidly attached to the cylindrical generatrix of the rotor with permanent magnets placed on the generatrix of the stator, characterized in that the permanent magnets of the stator are placed within the boundaries of the projection of the trajectory of movement of the rotor magnets between the poles of their opposite polarity with the possibility of connecting their magnetic fields, wherein the permanent magnets of the stator and rotor are placed relative to each other so that their neutral lines are at different distances from the axis of rotation of the rotor, and the stator magnets have elastic fastenings.

2. The method according to paragraph 1 is characterized in that a force is applied to the elastic fastening of the stator magnet.

3. The method according to paragraph 2 is characterized in that the elastic fastening of the stator magnets has at least one additional support point forming a lever.

4. The method according to paragraph 1 is characterized in that the neutral line of the stator magnets, forming its neutral zone, has an angle of inclination relative to the plane of movement of the rotor magnets.

5. The method according to I.1 differs in that the boundaries of the neutral line of the stator magnet are located at different distances relative to the axis of rotation of the rotor.

6. The method according to paragraph 1 is characterized in that the length of the stator magnets is greater than the distance between the magnets installed on the cylindrical generatrix of the rotor.

7. The method according to paragraph 1 is characterized in that the rotor is at an angle relative to the Earth’s surface and has a center of gravity and / or additional load different from the axis of rotation.

8. The method according to I.1 is distinguished in that the groups of interacting magnets of the rotor and stator are placed at different distances from the axis of rotation of the rotor, with the possibility of simultaneous or sequential interaction.

9. A device for producing mechanical movement in a stator-rotor system by means of the interaction of magnetic fields of permanent magnets, consisting of a source of external force applied to the rotor, a rotor containing a set of permanent magnets rigidly attached to a cylindrical generatrix of the rotor, and permanent magnets placed on the generatrix of the stator, characterized in that the permanent magnets of the stator are placed within the boundaries of the projection of the trajectory of the rotor magnets between the poles of their opposite polarity with the possibility of connecting their magnetic fields, wherein the permanent magnets of the stator and rotor are placed relative to each other so that their neutral The lines are located at different distances from the rotor axis of rotation, and the stator magnets have elastic fastenings.

10. The device according to item 9 is characterized in that a force is applied to the elastic fastening of the stator magnet.

11. The device according to item 10 is characterized in that the elastic fastening of the stator magnets has at least one additional support point forming a lever.

12. The device according to item 9 is characterized in that the stator has a fuse that prevents mechanical contact of the stator magnets with the rotor magnets.

13. The device according to item 9 is characterized in that the neutral line of the stator magnets, forming its neutral zone, has an angle of inclination relative to the plane of movement of the rotor magnets.

14. The device according to item 9 is characterized in that the boundaries of the neutral line of the stator magnets are located at different distances relative to the axis of rotation of the rotor.

15. The device according to item 9 is characterized in that the length of the stator magnets is greater than the distance between the magnets installed on the cylindrical generatrix of the rotor.

16. The device according to item 9 is characterized in that the rotor is at an angle relative to the Earth’s surface and has a center of gravity and / or additional load that is different from the axis of rotation.

17. The device according to item 9 is characterized in that the groups of interacting magnets of the rotor and stator are located at different distances from the axis of rotation of the rotor, with the possibility of simultaneous or sequential interaction.

18. The device according to item 9 is characterized in that the device is connected to a gearbox or generator and / or the generator windings are located along the trajectory of the rotor magnets. Explanation under Art. 19(1) Please make punctuation changes to the invention formula related to the correction of the numbering of dependent claims of the invention formula. In the submitted application materials, the numbers of dependent claims after claim 14 are incorrectly indicated in the invention formula. Attached is a new version of the invention formula with the correct numbering of dependent claims.

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