JP2009118706A - Magnetism rotating apparatus and power conversion system using the same - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To reduce cogging torque and detent torque and realize high performance in a magnetism rotating apparatus, in which a rotor 2 made up of two or more permanent magnets 4 arranged at equal intervals along the hoop direction, and a stator 1 made up of two or more electromagnets 3 arranged at equal intervals along the hoop direction around the rotor 2 are provided, and the rotor 2 is rotated through an attractive force and a repulsive force generated between the permanent magnet and the electromagnet by feeding the electromagnet 3 with electricity intermittently. <P>SOLUTION: One or more magnetic bodies 7 are arranged between the electromagnet 3 and the electromagnet 3 in the stator 1. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

  The present invention includes a rotating body in which a permanent magnet is arranged in a circumferential region of a rotatable rotating shaft, and an electromagnet that generates a magnetic field that repels and attracts a magnetic field generated by the permanent magnet of the rotating body. The present invention relates to a magnetic rotating device and a power conversion system using the same.

  First, the principle of this type of magnetic rotating device will be described.

  As shown in FIG. 10, an electromagnet is disposed on the stator side and a permanent magnet is disposed on the rotor side. At this time, the electromagnet is arranged so that its magnetic pole is inward as viewed from the rotation axis direction, that is, toward the rotation center side, while the permanent magnet is a central straight line that divides each magnetic pole (hereinafter also referred to as a straight line between the magnetic poles). It arrange | positions so that L1 may become in parallel with the rotating surface of a rotor. In the figure, a straight line (hereinafter also referred to as a reference straight line) L2 connecting the center between the magnetic poles of the permanent magnet and the rotation center of the rotor intersects with the straight line L1 between the magnetic poles of the permanent magnet at an angle (crossing). (Angle φ).

  Under such a configuration, when a constant direct current is passed through the electromagnet, torque acts on the rotor due to the repulsive force or attractive force between the electromagnet and the permanent magnet. The characteristic of the torque Te at this time with respect to the rotation angle (mechanical angle) θ of the rotor is shown in the θ-Te characteristic diagram (FIG. 11). Note that the angle of the rotor when the reference line overlaps the straight line L3 connecting the rotation center of the rotor and the magnetic pole center of the electromagnet is 0, and the direction in which the rotor rotates counterclockwise is positive. Yes.

  As is clear from this θ-Te characteristic diagram, when the electromagnet is continuously energized with a constant DC current, the rotor moves in one direction in a narrow angle region (hereinafter also referred to as the first angle region) where θ is near 0 °. A relatively strong torque Ta (hereinafter also referred to as a large-value narrow-angle torque) that tends to rotate in the negative direction (here, referred to as a negative direction) is generated, and a wide angle region (hereinafter referred to as the second and third angle regions) on both sides of the region. In this case, relatively small torques Tb and Tc (hereinafter also referred to as small-value wide-angle torque) are generated to rotate the rotor in the reverse direction (here, the forward direction). By the way, the angles P1 and P2 at which the torque becomes 0 appear at the boundary between the first angle region and the second angle region and the boundary between the first angle region and the third angle region, respectively. Of these, the angle at which the torque that tries to return to the original position regardless of which direction is rotated from that angle acts as the stable equilibrium angle P1, and the torque that moves away from the original position acts when rotated in either direction. This angle is referred to as an unstable equilibrium angle P2.

  In this θ-Te characteristic diagram, when the torque is integrated over 0 ° to 360 °, it becomes zero. The sign of the torque is for convenience, and is reversed if the magnetic poles and the arrangement direction of the electromagnet or permanent magnet are exchanged.

  Thus, if the permanent magnet comes into one of the aforementioned first angle region or the second or third angle region, the electromagnet is energized and otherwise the energization is stopped. A torque for rotating the in one direction, either forward or reverse, is obtained. This is the operating principle of this magnetic rotating device.

The inventor has applied for a patent in this type of magnetic rotating device with the same number of electromagnets and permanent magnets arranged at equal intervals in the circumferential direction, and has already obtained the right. (Patent Document 1).
Japanese Patent No. 3897043

  However, in the configuration as in Patent Document 1, when considering the stop state, the permanent magnet is positioned at almost one point of the opposing position of each electromagnet having a ferromagnetic material in its own magnetic flux, and has a very strong force. Thus, the stopped state is maintained. That is, a stop maintaining torque having a narrow width and a high peak value acts near the stop position. For this reason, for example, when a power conversion system including this magnetic rotating device as a power generator is used, there is a tendency that a problem such as failure to start smoothly occurs depending on the configuration.

  Even in the rotating state, the permanent magnets approach and separate from each electromagnet at the same timing, so the timing of energizing and de-energizing each electromagnet is synchronized at the same time. The torque is digitally turned ON / OFF when no power is supplied, and a large torque pulsation occurs.

  The present invention has been made in view of such a problem, and is generated between a permanent magnet and an electromagnet ferromagnetic material when a force to move from outside is applied during non-energization (or non-excitation). In addition to reducing the steep stop maintenance torque (hereinafter also referred to as detent torque) with respect to the angle change, it also reduces the pulsation torque (hereinafter also referred to as cogging torque) generated during energization as described above. Providing a magnetic rotating device or the like is a main intended problem.

  In order to solve such a problem, the present invention adopts the following configuration.

  That is, the magnetic rotating device according to the present invention includes a rotor in which a plurality of permanent magnets are arranged at equal intervals in the circumferential direction, and a plurality of electromagnets around the rotor at equal intervals in the circumferential direction. The rotor is rotated by an attractive force and a repulsive force generated between the permanent magnet and the electromagnet by intermittently energizing the electromagnet. Then, one or a plurality of magnetic bodies are arranged between the electromagnets in the stator and the electromagnets.

  In such a case, since the attractive force generated between the permanent magnet and the magnetic material is also distributed to the magnetic material on both sides of the electromagnet, the peak value of the detent torque can be lowered. Such an effect becomes prominent when this magnetic rotating device is used as a generator to be described later. This is because the engine can be started with a small external force. Further, this torque dispersion action also works on the cogging torque, and the torque pulsation width can be reduced.

  In order to reduce energy loss due to eddy current, it is preferable that the cross-sectional area cut by a plane parallel to the rotation axis of the magnetic material is as small as possible. As a specific aspect for that purpose, for example, a magnetic body may be a columnar body using a laminated silicon steel plate or the like, and may be arranged parallel to the rotation axis direction of the rotor.

  In order to attenuate the detent torque as smoothly as the permanent magnet moves away from the electromagnet, a plurality of magnetic bodies are arranged on both sides of the electromagnet and the size of the magnetic body is made smaller than the iron core of the electromagnet. In addition, it is desirable to set the size of the magnetic material farther from the electromagnet to be smaller. The reason is that the detent torque due to each magnetic material is set to be smaller than the detent torque due to the iron core of the electromagnet, and smaller as the distance from the electromagnet is increased.

  As a specific arrangement position of the magnetic body, the distance between the magnetic body and the magnetic pole center of the electromagnet, or the distance between adjacent magnetic bodies is preferably set to about 10 ° to 20 ° or less. By the way, the timing of energizing the electromagnet is a large torque that rotates the permanent magnet in one direction when a constant direct current is energized to the electromagnet in the relationship between one permanent magnet and one electromagnet. Second and third angles for generating a small-value wide-angle torque that is formed on the first angle region for generating a narrow-angle torque or on both sides of the first-angle region and for rotating the permanent magnet in the reverse direction. In any of the regions, the electromagnet may be energized.

  In particular, it is preferable to energize all or part of the second and third angle regions in order to be able to cope with high-speed rotation. The first angle region is a narrow angle, and a pulse current with a short time width must be applied at high speed rotation. However, considering the rise time and decay time of the current to the electromagnet coil, high speed rotation is required. It is difficult to make it correspond. On the other hand, the second and third angle regions are wider than the first angle region, and it is easy to synchronize the energization timing even at high speed rotation.

  More preferably, a certain electromagnet may be configured such that the second angle region of one permanent magnet and the third angle region of the adjacent permanent magnet are adjacent or overlap each other. This eliminates the need to separate the energization timing into the second angle region and the third angle region, and makes it possible to reduce the switching frequency of the power switching element, thereby reducing the switching loss and improving the device efficiency. It becomes possible to improve.

  In order to further reduce the cogging torque and detent torque, the number of permanent magnets and the number of electromagnets are different from each other, and the number of permanent magnets does not become an integral multiple of the number of electromagnets, or the number of electromagnets is permanent magnets. What is necessary is just to comprise so that it may not become an integral multiple of the number of. In order to achieve maximum torque dispersion under this configuration, it is even better if the number of permanent magnets and the number of electromagnets are set so that there is no common divisor other than 1 between them.

  In such a case, the energization timings of the electromagnets are sequentially shifted, so that the total torque generated is not limited to the binary value of ON / OFF as in the prior art, but is distributed and the torque is correspondingly increased. Pulsation, that is, cogging torque can be reduced. In addition, as for the no-load state before starting, the permanent magnets are not closest to all the electromagnets and are not firmly held in the opposite positions as in the conventional case, so the detent torque is also reduced. it can.

  Such a magnetic rotating device can also be used as a generator. In addition, since these magnetic rotating devices and generators are close to the coreless structure and have very good efficiency, for example, the rotor of the magnetic rotating device and the rotor of the generator are connected by a coupling or the like and added to the magnetic rotating device. It is possible to configure a high-efficiency power conversion system that converts the direct-current power to be taken out from the generator as alternating-current power. Moreover, since it is close to the coreless structure, it can also contribute to lowering the price.

  According to the present invention configured as described above, since one or a plurality of magnetic bodies are arranged between the electromagnets in the stator, both the detent torque and the cogging torque can be reduced as compared with the conventional case. Thus, higher efficiency, lower noise, lower vibration, etc. can be promoted to obtain a higher-performance magnetic rotating device or the like.

  Hereinafter, a magnetic rotating device 100 according to an embodiment of the present invention will be described in detail with reference to the drawings as appropriate.

  As shown in FIGS. 1 to 3, the magnetic rotating device 100 according to the present embodiment includes an electromagnet 3, a stator 1 that also serves as a frame 11, and a permanent magnet 4 that can rotate to the stator 1. And the rotor 2 is configured to be rotated by an electromagnetic force between the electromagnet 3 and the permanent magnet 4.

  First, the rotor 2 will be described. The rotor 2 includes a shaft 21 that is a rotating shaft, a support disk 22 through which the shaft 21 penetrates the center, and an edge portion of the support disk 22 at an equal interval over the circumference (here, 4 at 90 ° intervals). And the plate-like permanent magnet 4 arranged in the above.

  The support disk 22 is fixed to the shaft 21. In this embodiment, as shown in FIGS. 1 and 2, two support disks 22 are provided in parallel, and the permanent magnets 4 are disposed at the same position in each. In a two-stage configuration.

  On the other hand, as shown in FIG. 3, the permanent magnet 4 has a plate shape and is formed with magnetic poles on the front surface side and the back surface side, and a straight line L1 between the magnetic poles (refer to the background art for this definition) The reference line L2 of the permanent magnet 4 (refer to the background art for the definition) is parallel to the disk surface (plane perpendicular to the rotation axis), and the line L1 between the magnetic poles of the permanent magnet 4 and the rotation axis direction. It is fixed to the support disk 22 so as to cross at an angle (crossing angle φ). Here, the intersection angle φ is set to about 30 ° or more and about 60 ° or less.

  As shown in FIGS. 1 and 2, the stator 1 has a frame 11 and an electromagnet 3 held by the frame 11.

  The frame 11 is composed of a pair of parallel side plates 12 provided on the outer side of the support disk 22 and a plurality of frames 13 that are spanned between the side plates 12 and fix the side plates 12 to each other. is there. Each end portion of the shaft 21 is supported by the two side plates 12.

  The electromagnets 3 are arranged further on the outer periphery of the permanent magnet 4. Here, as shown in FIG. 3, three electromagnets 3 are arranged at equal intervals at 120 ° in the circumferential direction. Here, the number of permanent magnets 4 is 4 and the number of electromagnets 3 is 3. The number of permanent magnets 4 and the number of electromagnets 3 are different from each other, and there is no common divisor other than 1 between them. It is for doing so.

  The configuration of the electromagnet 3 will be described in more detail. As shown in FIGS. 1 and 2, the electromagnet 3 has a configuration in which a coil 32 is wound around an iron core 31 having a substantially U shape, for example. Magnetic poles are formed at both ends of the iron core 31 by the flow of current. As shown in FIG. 3, the orientation direction of each magnetic pole, that is, the magnetic flux center axis is 0 ° with respect to a straight line (not shown) connecting the rotation center O of the rotor 2 and the center of the magnetic pole as seen from the rotation axis direction. It is set to make an angle of about 20 ° or less. Thereby, there is an advantage that the average electromagnetic torque is increased as compared with the case where the angle is set to 0 °. In addition, energy conversion efficiency is improved by making the permanent magnet 4 in a two-stage configuration and using the magnetic flux generated from both magnetic poles of the electromagnet 3 to rotate the rotor 2.

  As for the direction of the magnetic poles of the electromagnet 3 and the permanent magnet 4, the corresponding two-stage permanent magnets 4 face the same pole as the magnetic poles of the electromagnet 3, that is, correspond to the N pole of the electromagnet 3. The permanent magnet 4 is fixed to the disk 22 with the N pole facing outward, and the permanent magnet 4 corresponding to the S pole of the electromagnet 3 is fixed to the disk 22 with the S pole facing outward. A predetermined clearance (magnetic gap length) is set between the magnetic pole of the electromagnet 3 and the magnetic pole on the outer peripheral side of the permanent magnet 4.

  By arranging the electromagnet 3 and the permanent magnet 4 in this way, the relationship between one electromagnet 3 and one permanent magnet 4 is unidirectional in the narrow first angle region as described in the background art. Torque Ta (large-value narrow-angle torque) is generated in the (negative direction), and in the wide second and third angle regions on both sides thereof, torques Tb and Tc in the opposite direction (positive direction) Tb (small-value wide-angle torque) (See FIG. 11).

  Further, in this embodiment, a (strong) magnetic material such as iron (for example, a laminated silicon steel plate) is disposed between the electromagnets 3. Specifically, as shown in FIG. 3, a magnetic body 7 having a columnar shape, more precisely an equal cross-sectional columnar shape, is made parallel to the rotation shaft 21 at intervals of about 10 ° or less on both sides of the electromagnet 3 as a center. One or a plurality (two in this case) are arranged, and the one closer to the electromagnet 3 is enlarged, that is, the cross-sectional diameter is increased.

  In addition, in this embodiment, as shown in FIG. 2, based on the angle detector 5 for detecting the rotation angle of the support disk 22 and the angle information output from the angle detector 5, A control circuit 6 that performs energization control is provided.

  Here, as the angle detector 5, for example, a rotary encoder attached to the shaft 21 and rotating synchronously with the support disk 22 is used. However, any angle detector that outputs necessary angle information may be used. It goes without saying that it is not a thing.

  The control circuit 6 is an electric circuit including a switching element and an information processing circuit. The information processing circuit may be configured with discrete components, or a CPU or the like may be used. The control circuit 6 receives angle information from the angle detector 5, extracts the electromagnet 3 in which the permanent magnet 4 is present in the second and third angle regions based on the angle information, Only the electromagnet 3 is energized by driving the switching element.

  Next, the operation of the magnetic rotating device 100 configured as described above will be described.

  First, the control circuit 6 extracts the electromagnet 3 in which the permanent magnet 4 exists in the second and third angle regions based on the angle information from the angle detector 5. In this embodiment, the second and third angular region widths are about 66 ° (since they are about 35 ° and about 41 °, and their overlapping width is about 10 °), and the electromagnet 3 Since three are arranged at equal intervals, the total of the second and third angle regions covers about 198 °, while four permanent magnets 4 are arranged every 90 °. Therefore, regardless of the rotation angle of the rotor 2, any permanent magnet 4 is always present in the second and third angle regions of any electromagnet 3, and the electromagnet 3 cannot be extracted. It can be started without fail.

  Next, the control circuit 6 applies a constant DC current to the extracted electromagnet 3. As a result, electromagnetic torque is generated and the rotor 2 starts to rotate.

  When the permanent magnet 4 moves out of the second and third angle regions of the electromagnet 3 due to this rotation, the control circuit 6 stops energization of the electromagnet 3.

  Meanwhile, when one of the permanent magnets 4 enters the second and third angle regions of another electromagnet 3, the control circuit 6 is energized to that electromagnet 3.

  By repeating this, the electromagnetic torque is continuously applied without interruption, and the rotor 2 continues to rotate.

  More specifically, FIGS. 4A to 4C show energization timings of the electromagnets 3 when the above-described control is performed. As is clear from FIG. 4, the energization of the electromagnet 3 is performed with the timing sequentially shifted while overlapping. Particularly in this embodiment, the first angle region is about 24 °, the second and third angle regions are about 66 °, three electromagnets 3 are arranged every 120 °, and the permanent magnet 4 is 90 °. Since four are arranged per degree, as shown in FIG. 4D, at least any two electromagnets 3 are always excited, and all three electromagnets 3 are intermittently excited. . As can be seen from FIG. 4, when the first angle region is 30 ° or more and less than 60 °, a period in which any one of the electromagnets 3 is excited occurs. When the first angle region is 60 ° or more, a period in which all the electromagnets 3 are not excited occurs. This relationship varies depending on the number of electromagnets 3 and the number of permanent magnets 4.

  Next, the torque fluctuation of the magnetic rotating device 100 will be considered.

  As a comparison, a conventional apparatus, that is, one having the same number (four) of permanent magnets 4 and electromagnets 3 shown in FIG. In this conventional apparatus, since each permanent magnet 4 comes and leaves at each electromagnet 3 at the same timing, each electromagnet 3 is energized at the same timing (see FIG. 6). Then, when the torques of all the electromagnets 3 are superimposed and when no torque is generated, the torque ripple width, that is, the cogging torque becomes very large (FIG. 6 (e)). reference).

  On the other hand, according to the magnetic rotating device 100, as shown in FIG. 4D, any one of the electromagnets 3 is always energized, and the torque is dispersed without disappearing at any timing. It can be seen that the torque pulsation width, that is, the cogging torque is reduced accordingly.

  Considering the state of no load before starting, in this state, the electromagnet 3 can be regarded as a magnetic body having only the iron core 31. Therefore, the permanent magnet 4 is attracted to the electromagnet 3 by the magnetic flux to be attracted to the electromagnet 3. Try to move to the closest position. In this regard, in the case of the conventional device, as shown in FIG. 5, the permanent magnets 4 are close to all the electromagnets 3 and are firmly held at the facing positions. Therefore, if an attempt is made to move from this state by, for example, an external force, an external torque that can overcome a large detent torque is required.

  On the other hand, according to the magnetic rotating device 100, the permanent magnet 4 does not face all the electromagnets 3 regardless of the angle of the rotor 2, and can be moved with a small external force compared to the conventional device. be able to. In other words, it can be said that the detent torque is small.

  In addition, in this embodiment, since the magnetic body 7 is disposed between the electromagnet 3 and the electromagnet 3 in the stator 1, the attractive force of the permanent magnet 2 is applied to the magnetic bodies 3 on both sides of the electromagnet 3. Is also distributed, so that the peak value of the detent torque can be lowered. A qualitative diagram showing the relationship between the detent torque and the rotation angle θ of the permanent magnet 4 with respect to the electromagnet 3 is shown in FIG. In the case of the conventional one without the magnetic body 7, as shown by the dotted line in the figure, if it is far from the stable stop position, a steep torque is generated to return to the stop position, but according to this embodiment, It can be seen that the torque is dispersed and the peak value becomes small.

  Further, since the size of the magnetic body 7 is reduced as the distance from the electromagnet 3 is decreased, the torque gradually decreases as the distance from the electromagnet 3 is increased, and a smaller torque pulsation can be realized.

  Furthermore, since the magnetic body 7 has a columnar shape and is arranged parallel to the rotation shaft 21, the cross-sectional area of the magnetic body 7 cut along a plane parallel to the rotation shaft 21 is made as small as possible. Power loss due to current generation can be minimized.

  As described above, the magnetic body 7 can reduce the detent torque. Further, the cogging torque can be similarly subjected to the torque dispersion action by the magnetic body 7 to reduce the pulsation amplitude.

  The present invention is not limited to the above embodiment.

  For example, the shape of the magnetic body is conceivable elsewhere, and the number of magnetic bodies may be three or more or one.

  If the effect of only the magnetic material is to be obtained, the number of permanent magnets and electromagnets may be the same or different from the above-described embodiment if different. An example is shown in FIG. FIG. 8A shows an example in which there is no common multiple other than 1 between the number of electromagnets 3 and the number of permanent magnets 4 as in the above embodiment. Here, the number of electromagnets 3 is 5 and the number of permanent magnets 4 is 4, and the same operational effects as in the above embodiment can be obtained. In FIG. 8B, there is a common multiple other than 1 between the number of electromagnets 3 and the number of permanent magnets 4, but all the electromagnets 3 and the permanent magnets 4 are matched and come to the opposite positions. It can also contribute to the reduction of cogging torque and detent torque.

  Further, as shown in FIG. 9, two of these magnetic rotating devices 100 and 100 ′ are prepared, and the shafts 21 are connected to each other by a coupling CP or the like, and one of the magnetic rotating devices 100 is driven by applying electric power. You may make it do. As a result, the other magnetic rotating device 100 ′ acts as a generator, can take out AC power from the electromagnet 3, and the power conversion system 1000 can be constructed. Although the electric power from the electromagnet 3 is not shown in the drawing, since there are three electromagnets 3, special control is performed only by making the windings of the electromagnet 3 simple wiring such as so-called delta connection or Y-connection. It can be taken out without using a circuit. Thus, since the magnetic rotating device 100 and the generator 100 'are highly efficient, the power conversion system 1000 is also highly efficient, resistant to overload, and sufficiently practical.

  In addition, the present invention is not limited to the above-described embodiment and the like, and may be appropriately changed without departing from the gist of the present invention.

  According to the present invention configured as described above, since one or a plurality of magnetic bodies are arranged between the electromagnets in the stator, both the detent torque and the cogging torque can be reduced as compared with the conventional case. Therefore, it is possible to provide a higher-performance magnetic rotating device and the like by promoting high efficiency, low noise, and low vibration.

FIG. 1 is a partially broken perspective view showing the entire magnetic rotating device according to an embodiment of the present invention. FIG. 2 is a front view of the magnetic rotating device according to the embodiment. 3 is a cross-sectional view taken along line AA in FIG. FIG. 4 is a timing chart showing the energization timing of the magnetic rotating device according to the embodiment and a diagram showing qualitative torque pulsation. FIG. 5 is a configuration diagram of the conventional magnetic rotating device viewed from the direction of the rotation axis. FIG. 6 is a timing chart showing energization timing of a conventional magnetic rotating device and a diagram showing qualitative torque pulsation. FIG. 7 is a comparison diagram showing a qualitative variation with respect to the rotation angle of the detent torque of the magnetic rotating device according to the embodiment in comparison with that of the conventional device. FIG. 8 is a structural view of a magnetic rotating device according to another embodiment of the present invention viewed from the direction of the rotation axis. FIG. 9 is a front view showing a generator and a power conversion system according to still another embodiment of the present invention. FIG. 10 is a diagram for explaining the rotation principle of the magnetic rotating device. FIG. 11 is an example of a θ-Te characteristic diagram in the relationship between one electromagnet and one permanent magnet.

Explanation of symbols

DESCRIPTION OF SYMBOLS 100 ... Magnetic rotating apparatus 100 '... Generator 1 ... Stator 2 ... Rotor 3 ... Electromagnet 4 ... Permanent magnet L1 ... Center which divides | segments each magnetic pole of a permanent magnet Straight line L2: A straight line connecting the center between the magnetic poles of the permanent magnet and the rotation center of the rotor

Claims (8)

A rotor having a plurality of permanent magnets arranged at equal intervals along the circumferential direction, and a stator having a plurality of electromagnets arranged at equal intervals along the circumferential direction around the rotor, the electromagnet By intermittently energizing, the rotor is rotated by the attractive force and repulsive force generated between the permanent magnet and the electromagnet,
A magnetic rotating device in which one or a plurality of magnetic bodies are arranged between an electromagnet and an electromagnet in a stator.   2. The magnetic force rotating device according to claim 1, wherein the magnetic body has a columnar shape and is arranged in parallel with the rotation axis direction of the rotor.   The magnetic rotating apparatus according to claim 1, wherein a plurality of magnetic bodies are arranged on both sides of the electromagnet, and the size of the magnetic body closer to the electromagnet is set larger.   The magnetic rotating apparatus according to claim 1, wherein an interval between the magnetic body and the magnetic pole center of the electromagnet or an interval between adjacent magnetic bodies is set to about 10 ° or less. In the relationship between one permanent magnet and one electromagnet,
When the DC magnet is continuously energized with a constant DC current, it is formed on a first angle region that generates a large-value narrow-angle torque that is a torque that rotates the permanent magnet in one direction, or on both sides of the first angle region, 2. The magnetic force rotating device according to claim 1, wherein the electromagnet is energized in any one of second and third angle regions that generate a small-value wide-angle torque that is a torque for rotating the permanent magnet in the reverse direction.   2. The magnetic rotating apparatus according to claim 1, wherein the number of permanent magnets and the number of electromagnets are different from each other, and the number of permanent magnets and the number of electromagnets are not an integral multiple of the number of counterparts. A rotor having a plurality of permanent magnets arranged at equal intervals along the circumferential direction, and a stator having a plurality of electromagnets arranged at equal intervals along the circumferential direction around the rotor, A voltage is generated in the electromagnet by a change in the number of magnetic flux linkages of the permanent magnet magnetic flux to the electromagnet due to rotation of the magnet,
A generator in which one or more magnetic bodies are disposed between an electromagnet and an electromagnet in a stator.   The rotor of the magnetic rotating device according to claim 1 is connected to the rotor of the generator according to claim 7, and the direct current power applied to the magnetic rotating device is converted to take out alternating current power from the generator. Power conversion system.