JP2013179724A - Rotation accelerating device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a rotation accelerating device that has a permanent magnet and a solenoid or electromagnet arranged, and electrically controls repulsive/attractive force of the magnet to have extremely small energy loss.SOLUTION: A rotation accelerating device causes disks 11, 11-1 to generate torque around their center axes by making S poles and N poles of a plurality of permanent magnets and a solenoid or electromagnet attract or repulse each other with magnetic fields generated in the plurality of permanent magnets and the solenoid or electromagnet supplied with a current. The attractive force and repulsive force that the permanent magnets have is utilized, and the permanent magnets which change applied inertial force into kinetic energy and the solenoid or electromagnet are arranged, and a sequence of an electronic integrated circuit for alternating and controlling the attractive force and repulsive force is used.

Description

  The present invention relates to a rotation acceleration device that uses the inertial force of a permanent magnet and a rotating body.

  Conventionally, the electromagnetic motor technology that generates power by generating a Lorentz force, known by Fleming's right-hand rule, by combining a permanent magnet and a copper wire coil and passing a current through the coil, and converting the force into a rotational force More widely known.

    A conventional electromagnetic motor is a device that uses a Lorentz force generated between a permanent magnet facing a coil as an electromagnet by passing an electric current through a coil. The Lorentz force is a force that attracts or repels the permanent magnet and the coil electromagnet relatively. If one is fixed and the other is attached to the rotating shaft, the one attached to the rotating shaft rotates. The structure of taking out as power is common. However, when generating the Lorentz force, there is a loss of force due to the resistance (cogging torque) generated by the magnetic field between the electromagnet and the permanent magnet of the coil, and the current energy is consumed by energy such as sound and heat, It is a well-known fact that hysteresis loss also occurs and not all is used as energy for rotational movement. For this reason, it has been impossible to create a closed power system in which, for example, power is generated by a generator, a motor is rotated by the electricity, and power is generated by the power.

  It is clear that a so-called permanent engine that circulates using the generated energy as power in a closed system does not hold according to the law of conservation of energy. On the other hand, solar power generation using solar energy that seems familiar and inexhaustible has actually been put into practical use, and can supply energy for an extremely long period of time without considering the consumption of equipment. However, although this energy is also “permanent”, it is a finite energy that will disappear after 10 billion years, which is said to be the life of the sun. Hydroelectric power generation is also a “semi-permanent” power generation system that generates electricity by changing the vaporization and liquefaction cycle of water into potential energy and kinetic energy. From this, it can be said that “a permanent engine does not exist but a semi-permanent engine exists” It can be said.

  In the first place, natural forces that exist on Earth and can be used semipermanently are attraction and magnetic force, and solar energy. The magnetic force (magnetic force) is a force in which the electron spin of a magnetic material such as iron is magnetized and stored by the magnetic field of the earth, and a semi-permanent engine using this has been considered for over 100 years. For example, in the model of Mr. Kitayoshi published in 2000, a rotating disk facing a fixed disk with a permanent magnet is rotated by an auxiliary motor to generate electricity, and a part of the generated power is used for the power source of the auxiliary motor. System. However, in this method, the magnetic field changeover switch is controlled mechanically, which is limited to several tens of times per second, which is sufficiently long considering the switch response speed and the life of the mechanical movement. It may be technically questionable, including structural problems, that the device will drive for a period of time.

Japanese Patent Application No. 2008-265972 Japanese Patent Application No. 2008-152111

  The problem to be solved by the present invention is not an electromagnetic motor using Lorentz force generated by a permanent magnet and a coil electromagnet with a large power loss, but a magnetic motor that obtains rotational force by a combination of permanent magnets and mechanical control and an auxiliary motor. In order to control the attractive force and repulsive force of the permanent magnet and apply the inertial force to convert the force into kinetic energy, based on the theory of the present invention, the permanent magnet and N poles at both ends when current is passed Rotation acceleration device that moves with extremely low power using a sequence of electronic integrated circuits that arranges and controls copper-wound solenoid coils (hereinafter referred to as “solenoids”) that create a magnetic field of the S and S poles. Is to provide.

   The rotational acceleration device of the present invention includes a plurality of permanent magnets arranged in a circumferential portion of a disk-shaped or cylindrical rotating solid (hereinafter referred to as “disk”) and a magnetic field generated in a solenoid through which electric current is applied. The disk is rotated by attracting or repelling the pole and the S pole, and the S and N poles of the solenoid, thereby generating a rotational moment force on the central axis of the disk.

  An even number of permanent magnets having the same size, weight, and magnetic force at the periphery of the disk having the central axis, and the center lines in the direction of the magnetic field connecting the north and south poles in a straight line are Arrange at equal intervals parallel to the central axis and equidistant from the center. If the center line in the direction of the magnetic field of a single permanent magnet is parallel to the central axis of the disk and the N and S poles are arranged in the east to west direction, the permanent magnets on both sides are N poles. And the direction of the pole of the permanent magnet is reversed so that the south pole is directed from the west to the east, and is alternately fixed to the peripheral edge portion at an equal distance from the center. All permanent magnets arranged in this way can rotate with a central axis integral with the disk. The above-mentioned disks are arranged in one or more sets, and the center axis common to each disk is supported at both ends by bearings, and can be smoothly rotated by bearings, etc., and the bearings that support the center axes are fixed to the gantry ing. Solenoids also have a center line in the direction of the magnetic field connecting the N and S poles that is generated when a current is passed through the coil, parallel to the center axis, and at equal distances from the center. Then, place and fix a small gap from the permanent magnet group on the support base fixed to the gantry. The support base is provided with a through hole so that the rotation of the central axis is not hindered, and the solenoid is wired from the power supply so that current can be passed.

  As shown in FIG. 4, when the center angle of the direction of the magnetic field connecting the north pole and the south pole of each of the two adjacent permanent magnets is alpha with the center angle formed across the center axis of the disk, The relationship with the total number M of permanent magnets to be arranged is as follows.

    Further, as shown in FIG. 5, angles beta and alpha formed by at least one pair of a plurality of solenoids and a point P on the central axis of the disk have the following relationship. (N is a natural number)

  Data on the opening / closing pattern of the electrical switch at a specific point on the disk and the data of a mechanical or optical sensor that senses the number of rotations of the disk are sent to a controller that supplies current to the solenoid, and the switch circuit is electronically controlled.

  According to the apparatus of the present invention, since the currents flowing through the solenoid to attract or repel the N and S poles of the permanent magnet and the N and S poles of the solenoid are mutually weak, the attractive force and the repulsive force The rotational moment obtained by the rotational force generated by the generator can be transmitted to the power of the connected generator, for example, and a part of the electric power obtained from the generator is used for driving the magnetic power unit of the present invention. Since the portion can be supplied as electric power for other uses, it can contribute to the industry as a power generation device that can be operated for a long time without requiring fuel.

It is a perspective view of the present invention. It is the figure which decomposed | disassembled this invention and showed the inside. It is a B arrow side view of FIG. FIG. 3 is a layout diagram of permanent magnets in a disk A and a disk B. It is a layout view of solenoids in the solenoid support base. It is a figure which shows the polarity of the permanent magnet in the disk A and the disk B. FIG. It is explanatory drawing seen from the E direction of FIG. FIG. 8 is a variation diagram of FIG. 7. 2 is an explanatory diagram of Embodiment 1. FIG. It is a current waveform diagram of a solenoid. It is a change figure of FIG. 10 is an explanatory diagram of Example 3. FIG. FIG. 10 is an explanatory diagram of Example 5.

  In FIG. 1, FIG. 2, FIG. 3 and FIG. 4, as a component in the first embodiment of the present invention, a disk A (11) and a disk B (11 fixed to the central axis (14) -1). The material of the disk is preferably a non-magnetic material such as aluminum die cast. An even number of permanent magnets having the same size, weight, and magnetic force at the peripheral portion of the disk A (11), and the center line in the direction of the magnetic field connecting the north and south poles in a straight line are Permanent magnets are arranged at equal intervals in parallel with the central axis. The permanent magnet 1 (12) is arranged such that the center line in the direction of the magnetic field is parallel to the central axis of the disk and is equidistant from the center, and the permanent magnets 2 on both sides of the permanent magnet 1 are The directions are reversed, and both ends are slightly outside the width of the disk and are alternately fitted to the peripheral portions. All permanent magnets can rotate with the disk and central axis. The disk B (11-1) has the same specifications as the disk A (11). A disk A and a disk B whose arrangement is the same as that of the disk A are connected by a central axis (14). Both ends of the central shaft are supported by bearings (16) and bearings (17) and can rotate smoothly. Both bearings are fixed to the gantry (15). Solenoid 1 (21), Solenoid 2 (22), Solenoid 3 (23) and Solenoid 4 (24) also have a central axis of the magnetic field connecting the N pole and S pole generated by passing a current through the coil in a straight line. And at a distance equidistant from the central axis at intervals spaced by the theory of the present invention described in paragraph (0012). Each solenoid is arranged by being fixed to the support base 1 (10) with a minute gap from the permanent magnet group, and is wired from the power supply unit (18) so that current can be passed. The support base 1 is fixed to the gantry (15) by passing the central axis (14) through the through hole (45) so as not to prevent rotation. Further, the sensor-equipped control unit (19) is incorporated in a circuit connecting the power source and the solenoid, detects information on a specific point (pattern range) of the disk B (11-1) and the rotation speed of the disk, and detects the solenoids 1 and 2. 3 and 4 to control the input pattern of the current.

    4 and FIG. 5, as calculated in (Equation 1), the permanent magnet is arranged on the disk with the central angle alpha consisting of the center of each of the two adjacent permanent magnets and the center of the disk being 30 degrees. The number is 12. When the solenoid is placed between 360 degrees counterclockwise with the center of the disk at the origin and the 3 o'clock position of the clock at 0 degrees, when the solenoid 1 (21) is placed at the 0 degree position, The angle beta formed by the solenoid 2 (22) and the center of the disk is 75 degrees according to (Equation 2).

  The interval between adjacent permanent magnets in FIG. 4 is smaller than the width of one magnet, but does not overlap, and twelve are arranged on the periphery of the disk at equal intervals. The gap between each solenoid and the permanent magnet on the disk is the same distance when the disk and the permanent magnet approach again when the disk rotates. The distance that can be met. The distance that can sufficiently influence the magnetic force depends on the strength of the permanent magnet, but may be about 5 mm in the case of 3000 Gauss, for example. An electromagnet can be used instead of the solenoid.

  In order to start the rotation of the disk, the disk A (11) is first placed so that the permanent magnet 1 (12) and the permanent magnet 2 (13) on the disk A (11) are in the state shown in FIG. That is, the permanent magnet 1 (12) is located in the range of 0 degrees to 30 degrees in the arrangement spanning 360 degrees counterclockwise with the center of the disk as the origin and the 3 o'clock position of the clock as 0 degrees. The disk A (11) is placed so that the permanent magnet 2 (13) is positioned from 360 degrees to 360 degrees. 6 shows the left side of the disk A (11) and the disk B (11-1) in FIG. The lines drawn on the radiation at intervals of 30 degrees from the center of the disk are explanatory lines indicating the gaps between the permanent magnets. In the right side surface of the disk A (11) and the disk B (11-1) in FIG. 3, the polarities at both ends of the permanent magnet fitted to the disk are opposite to those on the left side surface. The pole becomes the N pole. The disk B and the permanent magnet group overlap with the position where the arrangement of the disk A and the permanent magnet is translated. FIG. 7 is an enlarged view as seen from the direction of arrow B in FIG. When the position of the center line of the solenoid 1 (21) is in the middle of the pair of permanent magnets 1 (12) and 2 (13) adjacent to each other, current is passed through the solenoid 1 (21). When the disk A (11) side is the N pole of the solenoid 1 and the disk B (11-1) side is the S pole of the solenoid 1, the repulsive force f1 acts on the permanent magnet 1 (12) of the disk A (11), An attractive force f2 acts on the permanent magnet 2 (13). The resultant force F1 of the cosine components of f1 and f2 is a force for rotating the disk A (11). Similarly, repulsive force f3 acts on permanent magnet 1 (12) of disk B (11-1), and attractive force f4 acts on permanent magnet 2 (13). The resultant force F2 of the cosine components of f3 and f4 is a force for rotating the disk B (11-1). Since the disk A (11) and the disk B (11-1) are connected by the center axis, both the disks and the center axis rotate simultaneously with the vector of F1 plus F2.

  As shown in FIG. 8, the center line of the magnetic field of the solenoid 1 (21) overlaps the center line of the magnetic field of the permanent magnet 2 (13), and the N pole of the solenoid 1 (21) and the disk A (11 ), The S pole of solenoid 1 (21) and the N pole of disc B (11-1) are opposed to each other, and if current flows through solenoid 1, the vector of attraction becomes maximum and the disc rotates. The direction component is minimized. Further, the center line of the solenoid 1 (21) overlaps with the center line of the permanent magnet 1 (12), the N pole of the solenoid 1 (21), the N pole of the disk A (11), and the S pole of the solenoid 1 (21). When the south pole of the disk B (11-1) is opposed, the repulsive force vector is maximized, and the component in the direction in which the disk is rotated is minimized, which becomes a resistance that hinders the rotation of the disk. Therefore, in order to avoid this state in which resistance is generated in the rotation of the disk, when the pole of the disk surface of the solenoid 1 faces the permanent magnet 1 (12) or the permanent magnet 2 (13), the current to the solenoid 1 It is not necessary to generate a force that resists the rotation of the disk by blocking the magnetic field so as not to create a polarity and not to generate a magnetic field. That is, as shown in FIG. 7, the pole of the magnet on the disk side facing the pole of the solenoid has the same pole as the pole of the permanent magnet surface of the solenoid in front of the pole of the solenoid in the direction of rotation of the disk, and is different in the rear. Only when there is a pole, a rotating force acts on the disk. (Hereinafter, this force is referred to as “rotational force”) On the other hand, when the pole of the magnet on the disk side faces the pole of the solenoid as shown in FIG. (Hereafter, this force is called "braking force")

  In the first embodiment, the arrangement patterns of the permanent magnets that are formed when rotated every 15 degrees are only the four types of patterns shown in FIG. That is, in the disk A (11), No. 1 in FIG. SSNN pattern for one permanent magnet 2 (13) and one permanent magnet 1 (12) formed between arcs Z1Z2 in FIG. The NSSN pattern corresponding to half permanent magnet 1 (12), one permanent magnet 2 (13) and half permanent magnet 1 (12) formed between arcs Z1Z2 in FIG. NNSS pattern for one permanent magnet 1 (12) and one permanent magnet 2 (13) formed between arcs Z1Z2 in FIG. This is a SNNS pattern of half permanent magnet 2 (13), one permanent magnet 1 (12) and half permanent magnet 2 (13) formed between arcs Z1Z2 in FIG. (Hereinafter referred to as “rotational load pattern”) However, when the angle alpha formed by the center line of the poles of adjacent permanent magnets sandwiching the central axis is 30 degrees in this embodiment, for example, the SSNN pattern is the center Although the angle is in the range of 60 degrees, as long as the sensor can recognize the pattern and distinguish the four types, the pattern recognition range may be less than the central angle of 60 degrees. Even when set, the rotation load pattern can be set by calculating the angle.

  No. in FIG. 1 to No. In FIG. 4, the center of each disk is set as the origin, and the scale is set in increments of 15 degrees from 0 degrees to 360 degrees counterclockwise. In the pattern of FIG. 1, the same pole (N) is located in the 30 degree direction and the different pole (S) is located in the minus 30 degree direction with respect to the solenoid 1 (21) located at the 0 degree position. [0021] The counterclockwise rotational force in 0021). No. In the pattern of FIG. 2, since the same pole (N) is located in the rotational direction and the different pole (S) is located in the reverse rotational direction with respect to the solenoid 2 (22) located at 75 degrees, this is also a rotational force. Similarly, no. The positional relationship between the solenoid 3 (23) at 180 ° and the magnet on the disk in the pattern of FIG. It can be seen that the rotational force is also generated by the positional relationship between the solenoid 4 (24) at a position of 255 degrees and the magnet on the disk in the pattern of FIG.

  Therefore, when the permanent magnet passes through the solenoid, at the timing when the pole of the solenoid and the pole of the permanent magnet face each other and become a braking force, the current flowing through the solenoid is cut off so that no polarity is created and no magnetic field is generated. At the same time, if the current is sent only to the solenoid that generates the rotational force in any of the patterns described in paragraph (0022), the rotational force acting on the disk will not be interrupted. In order to detect this pattern and control the on / off of the current flowing to the solenoid, in FIG. 1 to No. As shown in FIG. 4, the position of 0 degree plus or minus 30 degrees on the disk A (11) or the disk B (11-1) is the pattern range (19-1), and the control unit with sensor (19) is the pattern. Recognize The position of the pattern range can be set at any position as long as it does not change relative to the solenoid arrangement.

  No. in FIG. 1 to No. In FIG. 4, an example of electrical input to each solenoid when the center of the disk is the origin, the 3 o'clock position of the watch is 0 degrees and the counterclockwise rotation is 360 degrees is shown in FIG. Each solenoid is intermittently loaded. For example, at the RP point (rotation angle around 220 degrees), the solenoid 2 is on and the other solenoids are off. This is the same relationship no matter how many times the disk rotates.

  While the disk is rotating at low speed, the current is repeatedly turned on and off according to the rotational load pattern in the order of solenoid 1, solenoid 2, solenoid 3, and solenoid 4, but when the disk rotates at high speed, it rotates with the inertial force of the disk itself. Therefore, by setting the electric signal input sequence in the control unit, the input to the solenoid can be skipped as shown in FIG. 11, and a pulse can be sent corresponding to the rotational load pattern to create a magnetic field. . The effect of skip is exhibited when the rotation of the disk is sufficiently high, and when the effect of the magnetic field is reversed and the brake is applied, the disk itself can be rotated by the inertial force. Also, reducing the number of pulses has a significant effect on reducing the input power.

  The advantage of the structure in which the solenoid is sandwiched between the two disks A and B is that the action of the magnetic field due to the polarity generated at both ends of the solenoid reaches the permanent magnets arranged on the disks A and B at the same time. Is to work efficiently for the rotation of both disks.

  The sensor-equipped control unit (19) senses the rotational load pattern and rotational speed of the disk and controls the current selector switch, so that the rotation can be accelerated in synchronization with the rotational speed. In order to decelerate or stop the rotating system, the current to the solenoid may be reduced.

    As shown in FIG. 12, a support base with a solenoid (10-1) and a disk C (11-2) are added to the disk and solenoid set of the first embodiment. Furthermore, it is possible to connect and connect one after another on a coaxial extension line such as a solenoid, a disk, a solenoid, and a disk.

  As shown in FIG. 12, it is an Example which connects a generator (25) to this invention and obtains electric power. In Example 2, it implements by connecting a generator directly or indirectly to the rotating shaft (14) of the present invention. If the radius of the disk is large, the inertial force increases and the rotational moment also increases. Therefore, a generator that can be rotated within the range of the rotational moment (torque) may be connected. In the present invention, the electric power input to the solenoid is for changing the polarity of the magnetic field and can be kept to the minimum necessary. In addition, power can be greatly reduced by the skip effect described in paragraph (0026). If a generator with an output larger than the power loaded on the device of the present invention is used, the generator can generate power without the need for an external power input. However, it is needless to say that this embodiment is a device that ends due to a natural decrease in the magnetic force of the permanent magnet, wear of the mechanical rotating portion, or the like, and is not a proposal of a “permanent engine”.

  In addition to the embodiment of connecting the generator (25) to the present invention, a starting battery and a current input / output controller are connected. In this embodiment, the generator is temporarily used as a starting motor. The current sent from the starting battery is controlled by the current input / output controller and sent to the generator. The generator temporarily becomes a motor and activates the connected rotation accelerator of the present invention. When the rotation accelerator is started, the device starts rotating with inertial force. If the load on the generator (temporarily motor) is stopped immediately by the current input / output controller, the generator is driven by the power of the rotation accelerator. Return to its original role and generate electricity.

  FIG. 13 shows an example in which the permanent magnet arrangement pattern described in paragraph (0022) of Example 1 is configured as a marker, and sensors are installed at four locations. In this embodiment, a total of 12 markers are arranged on the disk. Each marker is classified into four types and corresponds to the four types of patterns referred to by paragraph number (0022). That is, in FIG. 13, in P1, the current flows through the solenoid 21 when the sensor 31 senses the marker 41. In FIG. 2, when the sensor 32 senses the marker 42, the current flows through the solenoid 22, and in FIG. If the sensor 33 senses the marker 43, a current flows through the solenoid 23. In FIG. 4, a current flows through the solenoid 24 when the sensor 34 senses the marker 44. As a result, the arrangement pattern of the permanent magnets passes through the sensors, currents necessary for the rotational force flow to the solenoids, and the disk rotates.

  As an effect of the present invention, power can be obtained by rotating a motor without using external electricity, mechanical power, human power, or the like, and power can be generated by moving a generator with the power. Since the present invention is not a permanent engine, but a semi-permanent engine that uses the long-term life of a permanent magnet, it can be used for emergency use during disasters, power supply at sea such as small ships, Various drive devices and power generation devices can be configured by applying the present invention, such as power supply on a remote island.

10 Support stand 1
10-1 Support stand 2
11 Disc A
11-1 Disc B
11-2 Disc C
12 Permanent magnet 1
13 Permanent magnet 2
DESCRIPTION OF SYMBOLS 14 Rotating shaft 15 Mount 16 Bearing 17 Bearing 18 Power supply part 19 Control part with sensor 19-1 Pattern range 21 Solenoid 1
22 Solenoid 2
23 Solenoid 3
24 Solenoid 4
25 Generator 31 Sensor 1
32 Sensor 2
33 Sensor 3
34 Sensor 4
41 Marker 1
42 Marker 2
43 Marker 3
44 Marker 4
45 Through hole

Claims (5)

A disk-shaped or cylindrical rotating solid having a circular cross section, having a central axis, and a center line of magnetic polarity of the permanent magnet on each outer periphery intersecting a plane A perpendicular to the central axis of the rotating solid. A rotating solid in which a plurality of permanent magnets which are parallel to the central axis of the rotating body and are equidistant from the center are arranged at equal intervals by alternately inverting the polarities of adjacent permanent magnets, and a current flows In a device intended to obtain power by rotating a rotating solid by controlling the repulsive force and attractive force of a permanent magnet, the plurality of solenoids or electromagnets A pair of adjacent solenoids or electromagnets whose polar center lines are formed by sandwiching the central axis of the rotating solid on the outer periphery of the rotating solid as indicated by (Equation 2) Rotational acceleration having solenoids or electromagnets arranged to have an angle beta obtained by multiplying a natural number n plus 0.5 to an angle alpha formed by the center line of each polarity of the permanent magnet sandwiching the central axis of the rotating solid apparatus.
  The rotation acceleration device according to claim 1, wherein a single magnetic polarity center line of a permanent magnet is adjacent to a solenoid or electromagnet polarity center line with respect to a single or a plurality of solenoids or electromagnets. A rotational acceleration device that is electronically controlled so that the current flowing is cut off and no magnetic polarity is generated in the solenoid or electromagnet.   The rotation acceleration device according to claim 1, wherein a sensor-equipped control unit that detects an arrangement pattern of permanent magnets on a rotating solid and controls a solenoid or an electromagnet according to the data is arranged.   The rotational acceleration device according to claim 3, comprising a sensor-equipped control unit that measures and controls the rotational speed of a rotating solid, and corresponding to the rotational speed of the rotating solid with respect to a single or a plurality of solenoids or electromagnets, A rotation accelerator with a function to load and cut off current and a function to switch between plus and minus of current.   The rotation acceleration device according to claim 3, wherein a plurality of rotating solids and solenoids are alternately connected on the same central axis.