Device for increasing the force of mechanical movement in a stator-rotor system by the interaction of permanent magnet magnetic fields

Abstract

The invention relates to mechanical engineering and is intended for increasing the force of mechanical movement of a rotor in a stator-rotor system. The invention can be used for domestic, industrial and public needs. The claimed device comprises a source of external force, a stator, a rotor, a group of permanent magnets, and a resilient fastening mechanism. The sources of an increase in the force of mechanical movement of the rotor are: 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 rotor magnets with the magnetic fields of stator magnets prevents the device from assuming a state of equilibrium, therefore increasing the force of mechanical movement of the rotor.

Description

[0001] A device for increasing the force of mechanical movement in a stator-rotor system through the interaction of magnetic fields of permanent magnets

[0002] AREA OF TECHNOLOGY

[0003] The invention relates to mechanical engineering and is used to increase the force of mechanical movement in the stator-rotor system, which occurs during the interaction of magnetic fields of permanent magnets. The invention makes it possible to increase the force of mechanical movement of the rotor for obtaining energy, including electrical energy, for household, industrial and public needs.

[0004] A device known as a “Permanent Magnet Motor” (RU Patent No. 2177201) consists of a non-magnetic housing, two permanent spherical magnets, a cubic permanent slider magnet, 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 electrical energy.

[0006] The device “Magnetic engine” is known, patent of the Russian Federation No. K” 34826, consisting 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, interrupting the interaction of magnetic fields of 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 screen 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 increasing the force of mechanical movement as a result of the cyclic interaction of the magnetic fields of the permanent magnets of the rotor with the magnetic fields of the 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 increase the force of mechanical movement of the rotor when obtaining energy, including electrical energy, for household, industrial and public needs.

[0010] The technical result of the invention consists in increasing the force of mechanical movement, which occurs as a result of adding an external force applied to the rotor generator, 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. Cyclicity of the interaction of the magnetic fields of the rotor and stator.is achieved due to 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 ceased. The description presents a variant of increasing the force of 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 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 arranging the stator magnet at an angle relative to the plane of rotation of the rotor magnets.

[0011] The technical result of the invention is achieved due to the fact that the device for increasing the force of mechanical movement in the stator-rotor system, by means of 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 field of the stator magnet, attached to the base by means of an elastic fastening. To increase the force of mechanical movement stator-rotor, the force formed during the interaction of magnetic fields of 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, force, 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 obtaining a force in the direction of the rotor movement and a 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 restoring the symmetry of the interaction of parts of their magnetic fields, which, due to the rigid attachment of the rotor magnets to its cylindrical generatrix, is the source of the centrifugal force of the rotor movement on the one hand, and the force increasing the resistance of the elastic attachment of the stator magnet, on the other hand.During 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 a state of balancing of the forces of the interacting magnets. Thus, the rotation force of the rotor increases. In a device for increasing the force of mechanical movement in the stator-rotor system, through the interaction of the magnetic fields of permanent magnets, the sources of increasing the force of rotor movement are: the force of connecting 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 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.

[0012] During the patent research, no technical solution was identified from the state of the art that has features identical to all the features of the proposed invention, and therefore, the proposed invention meets the patentability condition of the invention ~ “novelty”.

[0013] The proposed invention does not clearly follow from the state of the art, and, therefore, the proposed invention meets the patentability requirement of “inventive step”.

[0014] The information set out in the application materials is sufficient for the implementation of the invention, therefore, the proposed invention meets the patentability requirement - “industrial applicability”.

[0015] DESCRIPTION OF FIGURES AND DRAWINGS

[0016] (Figs. 1-9) show a diagram of a device for increasing the force of mechanical movement of the stator-rotor by means of the interaction of the magnetic fields of permanent magnets, where: the base of the device (1), the axis of rotation of the rotor attached to the base of the device (2), the cylindrical generatrix of the rotor (3), the permanent magnets of the rotor (4.1, 4.2, 4.3), the permanent magnets of the stator (5; 5.1; 5.2; 5.3), the rigid fastening of the rotor magnets to the cylindrical generatrix of the rotor (6), the fastening of the stator magnets, having resistance, 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 (I), the projection trajectories of the rotor magnates (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 F1, the force, .directed in the direction opposite to the rotor rotation F2, the force aimed 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 magnet-stator F3, the force of gravity 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 rotor magnets 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.

[0017] In (Fig. 1a and 1b) a variant of the placement of a group of rotor and stator magnets symmetrically to the axis of rotation 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 magnets (4), the stator magnets (5), the center of gravity of the rotor (16). The fastening of the stator magnets in (Fig. 1a and 1b) is not shown.

[0018] In (Fig. 2) a variant of the device is shown, in which the force of gravity arising as a result of the displacement of the center of gravity of the rotor is used, 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), the permanent magnet of the stator (5), the rigid fastening of the rotor magnets to the cylindrical generatrix of the rotor (6), the fastening of the stator magnets creating resistance (7), the neutral line of the rotor magnets forming its neutral zone (10), the 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 lower point of rotation of the center of gravity of the rotor (19).centrifugal force of the rotor F, force directed in the direction of rotation of the rotor P1, force directed in the direction opposite to the rotation of the rotor F2, force directed at restoring the symmetrical interaction of magnetic fields arising during the movement of the rotor magnet along the neutral line of the stator magnet F3, gravitational force F4, external force applied to the cylindrical generatrix of the rotor F5.

[0019] 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 field of the stator magnet (9.2).

[0020] In (Fig. 4) the magnetic fields of the stator and rotor are shown 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 F1.

[0021] On (Fig. 5 - 5a) are shown: the force directed at restoring the symmetrical interaction of the parts of the magnetic fields and the resistance force of the stator magnet fastening, creating an asymmetrical interaction with the rotor magnets, where: the cylindrical generatrix of the rotor (3), the rotor magnet (4.1), the stator magnet (5), the rigid fastening of the rotor magnet to the cylindrical generatrix of the rotor (6), the fastening of the stator magnet, creating resistance (7), the magnetic field of the rotor magnet (9.1), the magnetic field of the stator magnet (9.2), the combined magnetic field of the rotor and stator magnets. (9.3), 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 force directed at restoring the symmetrical interaction of the parts of the magnetic fields F3, the resistance force of the stator magnet fastening F6.

[0022] (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).

[0023] 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 magnets of the rotor F6, the force applied to the fastening of the stator magnet F7.

[0024] (Fig. 7a and 7b) show variants of fastening the stator magnet 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 force, the resistance of the fastening. of the stator magnet, creating an asymmetric interaction with the magnets of the rotor F6, the force applied to the fastening of the stator magnet F7.

[0025] In (Fig. 3) 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. (5), 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.

[0026] (Fig. 9) shows the location of the stator magnet relative to the projection of the trajectories of the rotor magnet motion 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 mount (7), the neutral line of the rotor magnet (10), the neutral line of the stator magnet (11), the projection of the trajectory of the motion of the rotor magnet boundaries (12), the projection of the trajectory 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 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,

[0027] DESCRIPTION OF THE OPERATING PRINCIPLE OF THE INVENTION

[0028] The device for increasing the mechanical motion force in the 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, removing wind, water, etc., is applied to the cylindrical generatrix of the rotor (3). Movement occurs in the D direction. 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 movement 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 towards the rotor rotation as a result of the connection of the magnetic fields of the rotor and stator magnets. (Fig. 3) shows the magnetic fields of the rotor magnet (9.1) and 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 F1. The source of force F1 is the process of connection of 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 magnets, 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 magnate (4.1), which has a rigid fastening (6) to the cylindrical generatrix of the rotor (3) and the stator (5), fastened 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 FL is generated directed in the direction of rotation of the rotor and a force F2, between the magnetic field of the stator magnet (5) and the magnetic zero 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 rotor magnet moves along the neutral line of the stator magnet, a force F3 acts on the rotor magnet. The length of the stator magnet coincides with the length of its neutral line L2 (Fig.8) the distance between the rigid fastenings of the rotor magnets L1 is greater, 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 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 fastening of the stator (7) experiences the action of doubled force РЗ, 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 base of rotation of the rotor.Thus, during the rotation of the cylindrical generator of the rotor (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 occurrence of a state of equilibrium of the device and increases the force of movement of the rotor.

[0029] 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 (Fig. 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 field 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).

[0030] In order to increase the asymmetric interaction of the magnetic fields of the rotor magnets with the magnetic fields of the stator magnets and 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 an applied force and form a lever of the 1st, 2nd or 3rd kind, respectively.

[0031] The stator magnet (5) (Fig. 9) is located within the boundaries of the projection of the trajectory of motion of the rotor magnets (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 < L4. 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 a centrifugal force of the rotor, which increases the external force applied to the rotor.

[0032] (Fig. 1a and 1b) shows a version of the device with the placement of the rotor magnets (4) and the stator magnets (5) symmetrically to the axis of rotation of the rotor (2).

[0033] In (Fig. 2) one of the embodiments of the device for increasing the force of mechanical movement in the stator-rotor system is shown, by means of cyclic interaction of magnetic fields of permanent magnets using the force of gravity F4. 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 force of gravity 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 rotor magnet (4.1) (Fig.4) the magnetic field of the stator magnet (5) acts. Further interaction of the magnetic fields of the stator and rotor magnets occurs similarly to the above-described option. The centrifugal force of the rotor F is calculated by the formula: F≃3(F1 + F2 + F3) + F4 + F5.

[0034] The base of the device (1), the cylindrical rotor generatrix (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.

[0035] 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.

[0036] The energy generated as a result of the increase in the force of mechanical movement of the rotor is transmitted by any known method, including through a soft or rigid connection with a gearbox or generator. Also, magnetic fields of rotor magnets can be used to obtain induced electric current. For this purpose, windings of an 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.

[0037] The increase in the mechanical motion force in the stator-rotor system by means of the interaction of the magnetic fields of permanent magnets has been confirmed by a practical experiment. The experimental device is manufactured in accordance with (Fig. 2). The base of the device (1) is made in the form of a frame made of AISI 304 stainless steel, the axis of rotation of the rotor (2) is a freely rotating sleeve attached to the base of the device. The cylindrical generatrix of the rotor (3) is made of aluminum and has a diameter of 420 mm. The permanent magnets of the rotor are neodymium magnets, rod 20x40 mm, weight 90 g. - 3 pcs. The permanent magnet of the stator is a neodymium magnet rectangle 75x20x5 mm. Additional load - lead plates with a total weight of 160 g. To obtain an external force of the same magnitude, necessary for the purity of the experiment, in the area of ​​​​the rigid attachment of the rotor magnet (4.2), which coincides with the center of gravity of the rotor (16), a device is located that fixes an additional load on the cylindrical generatrix of the rotor during movement from the highest point of rotation of the rotor (18) to the lower point (1.9). At the lower point of rotation of the rotor (19), the additional load, under its own weight, is disconnected from the cylindrical generatrix of the rotor. In the experiments, the cylindrical generatrix of the rotor was located at an angle of 20 degrees to the surface of the Earth. Three permanent neodymium magnets are installed on it, the south poles of which are directed toward the axis of rotation of the rotor. The distance from the neutral line of the rotor magnets to the axis of rotation is 235 mm. The distance between the rigid fastenings of the rotor magnets is 60 mm. The center of gravity of the rotor (16) is located at the place of the rigid fastening of the rotor magnet (4.2). The stator magnet is located at the highest point of rotation (18). The fastening of the stator magnet is made using an elastic material made of fiberglass.The north pole of the stator magnet is directed toward the rotor rotation axis. The distance from the neutral line of the stator magnet to the rotation axis is 245 mm.

[0038] The experiment consisted of 2 parts. In the first part, the stator magnet was missing. An additional load was placed on the cylindrical generatrix of the rotor, at the location of its center of gravity (16). The center of gravity of the rotor was shifted in the direction of rotation by 45 degrees from the highest point of rotation (18). In this position, the rotor began to move. At the lowest point of rotation of the rotor (19), the additional load was disconnected. The rotor received an external force sufficient to overcome the highest point of rotation (18) and made one complete revolution around its axis. On the second revolution of rotation, due to the law of conservation of energy, the center of gravity of the rotor could not reach the highest point of rotation of the rotor (18), as a result of which the rotor moved in the opposite direction. Thus, the rotor made one complete revolution around its axis.

[0039] In the second part of the experiment, the stator magnet was placed along the movement of the rotor magnets at the highest point of rotation (18), as described above. Similar to the first part of the experiment, an additional load was placed on the cylindrical generatrix of the rotor at the location of its center of gravity (16). The center of gravity of the rotor was shifted in the direction of rotation by 45 degrees from the highest point of rotation (18). In this position, the rotor began to move. At the lower point of rotation of the rotor (19), the additional load was disconnected. The rotor received an external force sufficient to overcome the highest point of rotation (18) and made three full revolutions around its axis. On the fourth revolution of rotation, due to the law of conservation of energy, the center of gravity of the rotor could not reach the highest point of rotation (18), as a result of which the rotor moved in the opposite direction. Thus, the rotor made three full revolutions around its axis.Comparison of the obtained results indicates an increase in the external force applied to the rotor by at least 3 times.

[0040] The experiment was conducted 75 times and in all cases the same results were obtained, which is a practical confirmation of the declared technical result, namely: an increase in the mechanical force of the rotor in the stator-rotor system, through the interaction of the magnetic fields of permanent magnets.

Claims

CLAUSE OF INVENTION 1. A device for increasing the force of 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 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 distance between the rotor magnets installed on its cylindrical generatrix is less than the length of the stator magnet.

2. The device according to item 1 is distinguished by the fact that the stator has an elastic mount with an applied force.

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

4. The device according to item 1 is characterized in that the stator has a fuse that prevents mechanical contact of the stator magnets with the rotor magnets.

5. The device according to item 1 is characterized in that the neutral line forming the neutral zone of the stator magnet has an angle of inclination relative to the plane of movement of the rotor magnets.

6. The device according to item 1 is distinguished 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.

7. Device no. 1 is distinguished by the fact 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.

8. The device according to item 1 is characterized in that the groups of interacting rotor and stator magnets are located at different distances from the rotor rotation axis, with the possibility of simultaneous or sequential interaction.

9. The device according to item 1 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.

Images