WO1993009591A1 - Rotation amplifying device - Google Patents
Rotation amplifying device Download PDFInfo
- Publication number
- WO1993009591A1 WO1993009591A1 PCT/JP1991/001491 JP9101491W WO9309591A1 WO 1993009591 A1 WO1993009591 A1 WO 1993009591A1 JP 9101491 W JP9101491 W JP 9101491W WO 9309591 A1 WO9309591 A1 WO 9309591A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- disk
- rotation
- magnet
- circular
- disks
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Ceased
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Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K53/00—Alleged dynamo-electric perpetua mobilia
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K7/00—Arrangements for handling mechanical energy structurally associated with dynamo-electric machines, e.g. structural association with mechanical driving motors or auxiliary dynamo-electric machines
- H02K7/02—Additional mass for increasing inertia, e.g. flywheels
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
- Y02E60/16—Mechanical energy storage, e.g. flywheels or pressurised fluids
Definitions
- the second circular disk is rotated by the rotation of the first circular disk, and the outer circular disks are similarly sequentially rotated in the same manner, so that a large centrifugal force of the outermost circular disk is obtained.
- the inner disk is rotated further in the reverse direction, and the rotation of the inner disk is sequentially increased in the same manner, and so on.
- each of the disks has a higher speed than the rotation speed of the first disk given by the driving motor.
- the present invention relates to a rotation amplifying device that can obtain a rotation of the rotation.
- the present invention can obtain a higher rotational speed than the rotational speed given by the motor.
- the aim is to provide a new rotary amplification device.
- the rotation amplifying device includes a rotating shaft rotated by a motor
- a first outer circular body having a magnet exhibiting the polarity of a magnetic pole, and a (i-1) th (i is an integer from 2 to n-1) outer circumference of a circular body or a circular annular body And has an inner radius R i 1 (> R (i-1) 2) and an outer radius R i 2, and at the same predetermined angular position on the inner and outer circumferences as above,
- the magnet on the outer periphery of the (i-1) th outer circular body or the circular annular body is directed toward the outer peripheral side, and the inner magnet on the (i + 1) th circular annular body is directed toward the inner peripheral side.
- An i-th ⁇ -shaped body having a magnet whose polarity is shown toward the inner circumference side and whose polarity is shown toward the outer circumference side, respectively.
- n is an integer of 3 or more circular annular body and has an inner radius Rnl (> R (n-1) 2 ;; an outer radius Rn2).
- Rnl > R (n-1) 2 ;; an outer radius Rn2.
- the magnet on the outer circumference of the (n-1) -th ring has the polarity shown toward the outer IS side and the polarity of the repelling magnetic pole toward the inner circumference side.
- each disk in the stationary state, each disk is stationary in a state where the opposing magnets of the adjacent disks are located farthest apart from each other.
- the outer peripheral circular body is abbreviated as a circular disk) ′ is rotated by the motor, the rotation of the magnet of the first circular disk causes the rotation of the second circular circular body (hereinafter also referred to as the circular circular body).
- the disk is rotated in the same direction by the repulsion of the magnetic field between the magnets.
- the rotation is transmitted to the disk on the outer peripheral side, and the "rotation transmitting operation" toward the outer peripheral side causes each disk to rotate at almost the same speed. .
- the outermost disk is also rotated by its large centrifugal force so that its inner peripheral side is also rotated. It is faster than this and immediately tries to rotate (beyond the position of the corresponding magnets) by rolling over the inner disk, but this time the outer disk
- the (magnet of the disk) accelerates the rotation of the inner disk by applying a rotational urging force to the inner disk (magnet of the disk).
- the first disk fixed to the rotating shaft and the annular second or n-th disk sequentially and independently rotatably arranged outside the first disk are provided.
- the opposite ones are embedded at predetermined angular positions on the inner and outer circumferences of the above-mentioned disks with magnets indicating the repelling magnetic pole polarity, and the rotation of the first disk by motor drive is performed.
- the “rotation transmitting operation” is performed toward the outer peripheral side, which is sequentially transmitted to the outer peripheral disk, and the outermost circle
- the outermost disk accelerates its own rotation due to the large centrifugal force, and at that time,
- the magnet of the disk applies a rotational urging force to the magnet on the inner peripheral side of the disk and rotates it while shaking it off while increasing the speed.
- the rotation speed-up operation is sequentially performed toward the internal station, and the rotation transmission operation toward the outer circumference and the rotation speed-up operation toward the inner circumference are repeated.
- each disk rotates at a speed higher than the number of rotations given to the first disk by the motor, it can be large even with the input of small power. Thus, a very high-speed rotation of a circular disk can be obtained. At the time of this ultra-high speed rotation, a large centrifugal force causes a strong inertial force to stop at the absolute position, and a floating operation is performed using this state. This has the following effects.
- FIG. 1 is a perspective view of a rotary amplifying device according to one embodiment of the present invention
- FIG. 2 is a cross-sectional view of a rotary amplifying device according to one embodiment of the present invention
- FIG. 4 (a), 4 (b) and 4 (d) are views for explaining the operation of the above embodiment
- FIG. 5 shows a specific example of the structure of a bearing used in the above embodiment.
- Fig. 1 is a perspective view of a rotary amplifying apparatus O according to an embodiment of the present invention
- Fig. 2 is a cross-sectional view thereof
- Fig. 3 is a schematic plan view thereof
- Fig. 4 is an operation explanatory view thereof.
- 1 is a motor shaft
- 3 is a rotating shaft that is driven to rotate by the motor 1
- 3 a is a spline section integrally formed with the rotating shaft 3
- Numeral 4 is a device housing, and reference numerals 81 and 82 are provided between the rotating shaft 3 and the device housing 4 and are bearings which rotate between them.
- .100 is fixed to the rotating shaft 3 by being fitted to the spline portion 1a of the spline portion 1a or the spline portion 3a of the rotating shaft 3; , Aluminum plate, brass or other alloy, etc., and a first circle (circumferential circular body) having a circular shape with an outer radius R12 of an outer peripheral shape.
- a first circle circumferential circular body having a circular shape with an outer radius R12 of an outer peripheral shape.
- Permanent magnets 10a to 10 showing an N pole toward the side and an S pole toward the inside are embedded and formed.
- 200, 300, 400, and 500 are the first A second or fifth annular disk (circular annular body), which is sequentially and independently rotatably arranged on the outer periphery of the disk 100, and is the first or fifth annular disk.
- Bearings 12, 23, 34, and 45 are interposed between the disks so that the adjacent disks can rotate freely.
- disks 200, 300, and 400 are the inner radius R i 1 (> R (i-1) 2) and the outer radius R
- 20f, 30a to 30f to 40f to 40i to 40i are formed by embedding, and the outer periphery of the outer periphery is positioned at the same angular width of 60 ° as above on the outer periphery.
- Permanent magnets 50a to 50f indicating the polarity of the S pole are buried toward the inner peripheral side at a predetermined angular width at the same 60 ° interval, and no permanent magnet is provided on the outer periphery. .
- 101, I02 are fixedly provided on the upper and lower surfaces, respectively, at positions near the outer periphery of the first disk I00, and the second disk on the outer peripheral side thereof is provided.
- a bearing 61, 62 between the vertical movement restricting body 101, 102 and the second disc 200, and the vertical movement restricting body.
- Bearings 63, 64 are provided between 01, 102 and the device housing 4, respectively.
- a recess is formed in a semi-magnetic or non-magnetic disc made of an alloy such as a copper plate, an aluminum plate, or brass, and a permanent magnet is embedded in the recess.
- the magnetic field of the permanent magnet is not disturbed by the magnetization of the disc material, and the outside of the disc is not affected by the permanent magnet. The same magnetic field is formed.
- the outer radii R12 to R52 and the inner radii R21 to R51 of each of the above-mentioned disks are both increased by the same radius.
- the relationship between the circumferential length 1 of the magnet 30a and the like of each disk and the distance d between the magnets 30a and 30b is described later in the present invention.
- the distance d is set to be slightly longer than the length 1 in order to theoretically enable the following operation and, in addition, to allow the operation to have some play.
- Fig. 5 shows an example of the specific configuration of the bearings 12, 23, 34, and 45 provided between two disks used in this device.
- ball bearings 70 are The ball is composed of a ball holder 71 provided on the discs 100, 200, etc. on the peripheral side, and a ball 72 held by the ball holder 72. However, it is arranged so as to be rotatable between the inner surface of the holder 71 and the inner surface of the disk 200, 300 or the like on the outer peripheral side.
- the first disc 100, the second, third, fourth, and fifth annular discs 200, 300, 400, 500 are separate bodies. And are arranged so as to be rotatable independently of each other.
- the opposing magnets of the adjacent disks are assumed to have the same polarity, and each disk is affected by the magnetic field repulsion between these magnets.
- the magnets facing each other on adjacent disks come to the farthest position, that is, the magnet 21a comes in the middle between magnets 30a and 30b, and comes to rest. I do.
- the disks on the outer peripheral side are sequentially driven to rotate, and At the start, when each disk starts to supply Qc-voltage such that it rotates at almost the same speed9, the disk on the inner peripheral side by the G rotation driving force from 71- Will rotate steadily beyond the positional relationship that the magnet of Z- will be almost in the middle of the magnet on the outer circumferential disk, but the outer circumferential circle will soon be out of the way.
- the discs are gradually increased in speed, and eventually all the discs rotate at almost the same speed. In this way, when the "rotation transfer operation" to the outer circumference side using the magnetic field repulsion force between the magnets is performed and the rotation of each disk is reached; the rotation of the outer circumference side is almost completed.
- oArea area therefore large in weight, works during rotation 3 ⁇ , and is increased by force as if the straightness is increased.
- the inertia force is greater than the flywheel effect, so the disk on the outer periphery shakes the disk on the inner periphery.
- the outer peripheral G disk (magnet) is turned to the inner disk (rotating port for the magnet), while applying an urging force.
- the inner disk rotates at a higher speed while rotating at a higher speed, and thus rotating at a higher speed.
- Self-rotation due to the rotational inertia force 3 ⁇ 4 The “rotation amplification operation”, which increases the speed of the inner disk from a faster force, is sequentially performed on the inner magnet and the magnet. Between the magnet on the inner peripheral side and the innermost disk, and so on, but also between the magnet on the outermost disk and the magnet on the inner peripheral side.
- Figs. 4 (a) to 4 (d) show that the rotation of the first disk in the direction indicated by arrow X (clockwise rotation) is sequentially transmitted to the fifth disk, and then the fifth disk is rotated.
- the fourth disk is swung off by a large rotating centrifugal force and rotated, i.e., when rotating beyond the positional relationship between the magnets, and further accelerated at this time He is a physician showing how the fourth disk rotates while shaking off the third disk.
- the centrifugal force of the outer disk is almost equal to that of the outermost disk. Because of its large size, the fifth disk 500 has an increased rotational inertia force as if its weight was increased by its largest centrifugal force. If attention is paid to the disk magnet 50a, the rotational inertia overcomes the leftward biasing force from the magnet 41a and rotates beyond the magnet 41a. You are trying to do that. Then, by the rotation of the fifth disk, the magnet 50a is brought to a position covering most of the upper part of the magnet 41a as shown in FIG. 4 (b).
- the magnet 41a is rotating at a higher speed because the magnet 50a has passed most of the upper part of the magnet 41a.
- the magnet 50a is given a force F4 that urges the magnet 50a to rotate to the right in the figure, while the magnet 50a is rotating at a higher speed than the magnet 50a.
- Overpassed magnet 5 0 a exerts a force ⁇ 4 on the next magnet 4 l. b to urge it to rotate rightward in the figure ⁇ :.
- the positions of the third and fourth disks are almost the same as in FIG. 4 (a), and the forces F11, F11 ', F12 are almost the same. , F 1 'are working.
- the fourth disk is driven by the magnet 41b as shown in FIG. 4 (a) due to the fact that the magnet 41b is accelerated in this manner. 5
- the magnet 41b force is applied and the magnet 31c shown in Fig. 4 (d) is pushed into the covering position.
- the speed of the magnet on the inner horse side is increased in the same manner as above.
- the outer peripheral magnet rotates over the inner peripheral magnet while having a large rotational inertia force, which is increased by a large centrifugal force.
- the operation of increasing the speed of the plate proceeds toward the inner circumference o
- the outermost disk is increased by its large centrifugal force to increase the rotational inertia. Therefore, when rotating at a higher speed and rotating beyond the positional relationship of the inner disk with the magnet, the outermost disk accelerates one of the inner disks. While rotating, the accelerated inner disk is similarly rotated while its inner disk is accelerated while the inner disk is positioned with the magnet. It rotates beyond the relationship, and the same operation is performed thereafter, so that the innermost disk is sequentially accelerated. Then, the disk on which the innermost first disk 100 is rotated at the speed of kneading is sequentially moved toward the outer peripheral side in the same manner as in the above-described operation. The rotation is transmitted to the fourth disk, and the rotation amplifying operation similar to the above is performed again toward the inner circumference. A very high rotation speed higher than the rotation speed given to the disk 1 can be obtained.
- the first disk is accelerated to a speed equal to or higher than the rotation speed of the motor drive by the rotation increasing operation via the second disk and the fifth disk. At that time, the load is in emergency or unusual with respect to the motor, and the rotation of the motor itself is also becoming faster. It is.
- the rotation of the first disk is transmitted and amplified sequentially to the outside, the inside, the outside, the inside, and so on.
- the extremely high-speed rotation of each disk can be obtained. If such an ultra-high-speed rotation is obtained at the outermost circumference o circle or the like, it depends on the rotation at that time; the IS heart strength and the increase due to this
- the rotational inertia force is very large, and a state is maintained in which a large inertia force is maintained to stop at that absolute position, and a strong attempt is made to stop at this absolute position. It is possible to perform a levitation operation while maintaining a high inertia force.
- the number of magnets provided on one circumference of each disk, the length of the magnets in the circumferential direction is 1, and the magnets are provided immediately.
- the polarity of the magnet of each disk is opposite to that of the magnet on the inner circumference side and the magnet on the outer circumference side of the same disk, but this is the same disk.
- the inner and outer magnets may have the same polarity, and all magnets may have the same polarity outward, for example, the N pole.
- the means for restricting the vertical movement of each annular disk is constituted by providing a vertical movement restricting member on the disk on the inner peripheral side of the disk. It is also possible to provide a vertical movement restrictor for the outermost disk, and to provide a vertical movement restrictor for the inner disk below on the outer disk. Further, the above-mentioned vertical movement restricting body is not an annular one following the shape of the disk: it may be provided only at a few positions on the circumference.
- a lubricating oil may be sealed inside the device housing to prevent wear of the bearing.
- ball bearings are used for the bearings provided between the discs, between the housing and the regulating body, and between the regulating body and the discs, the ball bearings are always limited to these. Instead, a bearing that can rotatably hold between the rainers using a magnetic field repulsion force between magnets or the like may be configured.
- the output shaft of motor 1 is directly
- the motor is installed at a position distant from the rotating shaft 3 and the rotating shaft is controlled via a timing belt, pulley, etc. It may be configured to drive the motor.
- the device housing 4 is provided for supporting each disk at the time of stop, low-speed rotation, and the like, or in the present invention, the device housing 4 is always provided. There is no need to set up.
- a disc is used as the first outer circular body and an annular disc is used as the second or fifth circular annular body.
- the circular body is tO having a circular outer shape
- its cross-section is not limited to a flat plate, but may be any shape
- the circular annular body may also be a circular annular body.
- the cross section is not limited to a flat plate, but may be of any shape.
- a first outer circular body fixed to the rotating shaft having an outer peripheral radius R 12, and having a magnet having the same magnetic polarity toward the outer peripheral side at a predetermined angular position at an equal angular interval on the outer peripheral side;
- the (i ⁇ 1) (i is an integer from 2 to n—1) outer periphery of a circular body or a circular annular body, and an inner radius R i 1 (> R (i ⁇ I ) 2), having an outer radius R i 2, and at the same predetermined angular position on the inner circumference and the outer circumference, the outer circumference of the (i-11) outer circumference circular body or the circular annular body.
- the (i + 1) -th ring-shaped inner magnet has the polarity shown toward the inner circumference and the polarity of the repelling magnetic pole toward the inner circumference, respectively.
- An i-th circular annular body having magnets directed toward the outer periphery;
- a rotating amplifying device comprising: an n-th circular annular body having a magnet shown in FIG.
- a claim 1 characterized by further comprising a vertical movement restricting body for restricting the vertical movement of the second or n-th circular annular body. Or the rotary amplifying apparatus according to paragraph 2.
- the vertical movement restricting body for the i-th annular body (i is an integer from 2 to n-1) is the (i-1) -th peripheral circular body or the (i-i-1) -th circular body. 4.
- a claim characterized by further comprising a device housing for accommodating the rotating shaft, the first outer circular body, and the second or n-th circular annular body. Rotational amplification according to any of the first or fourth term
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Abstract
Description
明 細 書 Specification
発明の名称 Title of invention
回転増幅装置 Rotary amplification device
技術分野 Technical field
こ の発明は、 第 1 の円板の回転に よ り 第 2 の環状円板 を回転 さ せ、 同様に順次外側の環状円板を回転 さ せ、 最 外周の 円板の大 き な遠心力 に よ る 回転に よ り 今度は逆 に その内側の円板を さ ら に回転 さ せ、 同様に順次内側の 円 板の回転を順次増速 し、 以下同様に し て外周 側に 向 て の回転の伝達, 内周側に向 けて の回転の増幅を繰 り 返 し て、 '駆動用 モ ー タ に よ っ て与え られ る 第 1 の 円板の回転 数 よ り 高速の各円板の回転を得 る こ と ので き る 回転増幅 装置に関す る も のであ る 。 According to the present invention, the second circular disk is rotated by the rotation of the first circular disk, and the outer circular disks are similarly sequentially rotated in the same manner, so that a large centrifugal force of the outermost circular disk is obtained. Then, the inner disk is rotated further in the reverse direction, and the rotation of the inner disk is sequentially increased in the same manner, and so on. By repeating the transmission of the rotation and the amplification of the rotation toward the inner peripheral side, each of the disks has a higher speed than the rotation speed of the first disk given by the driving motor. The present invention relates to a rotation amplifying device that can obtain a rotation of the rotation.
背景技術 Background art
従来 こ の よ う な回転増幅装置はな か っ た。 Conventionally, there was no such a rotary amplification device.
発明の開示 Disclosure of the invention
上述の よ う に従来 こ の よ う な回転増幅装置は全 く な : 、 こ の発明 は、 モ 一 夕 に よ っ て与え ら れ る 回転数 よ り 高速 の回転を得 られ る 、 全 く 新規な回転増幅装置を提供す る こ と を 目 的 と して い る 。 As described above, there is no conventional rotary amplifying device such as this: the present invention can obtain a higher rotational speed than the rotational speed given by the motor. The aim is to provide a new rotary amplification device.
こ の発明 にかか る 回転増幅装置は、 モ ー タ に よ り 回転 さ れる 回転軸 と、 The rotation amplifying device according to the present invention includes a rotating shaft rotated by a motor,
上記回転軸に固定 さ れ、 外周半径 R 1 2 を有 し 、 そ の 外周 の等角度間隔の所定角度位置に外周側に 向 けて 同一 磁極の極.性を示す磁石を有する第 1 の外周円形体 と、 第 ( i 一 1 ) ( i は 2 以上 n — 1 ま での整数:) の外周 円形体ま たは円形環状体の外周に配置さ れ、 .内周半径 R i 1 ( > R ( i - 1 ) 2 ) , 外周半径 R i 2 を有 し、 そ の内周, 外周のそれぞれの上記 と同 じ所定角度位置に、 上記第 ( ί 一 1 ) の外周円形体ま たは円形環状体の外周 の磁石が外周側に向 けて, 第 ( i + 1 ) の円形環状体の 内周の磁石が内周側に向けてそれぞれ示す極性 と反発す る磁極の極性をそれぞれ内周側に向 けて, 外周側に向 け て示す磁石を有する第 i の Ρί形璟状体 と、 It is fixed to the rotating shaft and has an outer radius R 12, and is the same toward the outer periphery at a predetermined angular position at an equal angular interval of the outer periphery. A first outer circular body having a magnet exhibiting the polarity of a magnetic pole, and a (i-1) th (i is an integer from 2 to n-1) outer circumference of a circular body or a circular annular body And has an inner radius R i 1 (> R (i-1) 2) and an outer radius R i 2, and at the same predetermined angular position on the inner and outer circumferences as above, The magnet on the outer periphery of the (i-1) th outer circular body or the circular annular body is directed toward the outer peripheral side, and the inner magnet on the (i + 1) th circular annular body is directed toward the inner peripheral side. An i-th 璟 -shaped body having a magnet whose polarity is shown toward the inner circumference side and whose polarity is shown toward the outer circumference side, respectively.
第 ( n — 1 ) ( η は 3 以上の整数) の円形環状体の外 周に配置さ れ、 内周半径 R n l ( > R ( n - 1 ) 2 ; , 外周半径 R n 2 を有 し、 その内周の上記 と同 じ所定角度 位置に、 第 ( n — 1 ) の環状体の外周の磁石がその外 IS 側に向 けて示す極性と反発する磁極の極性を内周側に向 けて示す磁石を有する第 n の円形環状体 とを備えた こ と を特徴 とする。 It is arranged on the outer circumference of the (n-1) th (n is an integer of 3 or more) circular annular body and has an inner radius Rnl (> R (n-1) 2 ;; an outer radius Rn2). At the same predetermined angular position on the inner circumference as above, the magnet on the outer circumference of the (n-1) -th ring has the polarity shown toward the outer IS side and the polarity of the repelling magnetic pole toward the inner circumference side. And an n-th circular annular body having a magnet shown in FIG.
こ の発明においては、 静止状態では各円板は隣接する 円板の対向する磁石同士が最も離れた位置にあ る状態で 静止 してお り 、 こ の状態で第 1 の外周円形体 (以下外周 円形体を円板 と略称する) 'がモー タ に よ り 回転さ れ る と 、 該第 1 の円板の磁石の回転に よ り 第 2 の 円形環状体 (以 下円形環状体を も 円板 と略称する) の磁石が磁石間の磁 場反発力を受けて同方向に回転駆動 され、 同様に して順 3 In the present invention, in the stationary state, each disk is stationary in a state where the opposing magnets of the adjacent disks are located farthest apart from each other. When the outer peripheral circular body is abbreviated as a circular disk) ′ is rotated by the motor, the rotation of the magnet of the first circular disk causes the rotation of the second circular circular body (hereinafter also referred to as the circular circular body). The disk is rotated in the same direction by the repulsion of the magnetic field between the magnets. Three
次 よ り 外周側の 円板 に 回転が伝達 さ れ、 こ の外周 側へ向 けて の " 回転伝達動作 " に よ り 各 円板がほ ぼ同 一速度 て 回転す る よ う に な る 。 そ して、 各 円板がほ ぼ同 一速度で 回転す る よ う に な っ た状態で は、 最外周 の 円板 は そ の大 き い遠心力 に よ り そ の 内周 側の も の よ り よ り 速 く 、 即 ち 、 内側の 円板を振 り 切 っ て (対応す る 磁石の位置関係 を 越 えて ) 回転 し ょ う と す る が、 こ の と き 外側の 円板 ( 該 円 板の磁石) は 内側の 円板 (該 円 板の磁石) に対 し 回転付 勢力 を与え る こ と に よ っ て こ の 内側の 円板の 回転 を増速 . し な が ら こ れ よ り 速 く 回転す る こ と と な り 、 こ の よ う に 遠心力 に よ り 増大 さ れた慣性エ ネ ル ギ ー に よ り 自 己 の 回 転を速めな が ら 内側の 円板を も 増速す る " 回転増幅動作 " が順次最内周 の 円板 ま で行わ れ る こ と と な る 。 こ の よ う に して最内周 の 円板が増速 さ れ る と 、 こ れ は そ の増速 さ れた 回転を上記 と 同様の " 回転伝達動作 " に よ り 順次外 周 側 に 向 けて伝達す る と と も に 、 再 び外 周 側か ら 内 周 側 に 向 けて上記 と 同様の " 回転増幅動作 " が行な わ れ 、 こ の "回転伝達動作 " と " 回転増幅動作 " が何回 も 繰 り 返 さ れ る こ と に よ っ て、 モ ー タ に よ っ て第 1 の 円 板 に与え ら れ る 回転数 に比 し非常 に高速の 回転が各 円板 に 得 ら れ る こ と と な る 。 こ の よ う に し て 、 各 円板 に 非常 な 超高速 回転が得 ら れ る と 、 そ の大 き な 遠心力 に よ り 増大 さ れ る と こ ろ の回転慣性力 は き わ めて大 き な も の と な り 、 各 円 板が き わ めて大 き な慣性力 を持 っ て 回転 し て い る 状態 を 得る こ とができ る。 Next, the rotation is transmitted to the disk on the outer peripheral side, and the "rotation transmitting operation" toward the outer peripheral side causes each disk to rotate at almost the same speed. . Then, in a state where each disk rotates at almost the same speed, the outermost disk is also rotated by its large centrifugal force so that its inner peripheral side is also rotated. It is faster than this and immediately tries to rotate (beyond the position of the corresponding magnets) by rolling over the inner disk, but this time the outer disk The (magnet of the disk) accelerates the rotation of the inner disk by applying a rotational urging force to the inner disk (magnet of the disk). It rotates faster than this, and while its own rotation is accelerated by the inertial energy increased by the centrifugal force in this way, the inner side is rotated. The "rotational amplification operation" that also increases the speed of the disk is performed sequentially up to the innermost disk. In this way, when the innermost disk is accelerated, this accelerated rotation is sequentially transmitted to the outer peripheral side by the same "rotation transmitting operation" as described above. In addition to the above, the same "rotation amplification operation" is performed from the outer circumference to the inner circumference again, and the "rotation transmission operation" and "rotation transmission operation" are performed again. Since the "amplification operation" is repeated many times, the rotation at a very high speed compared with the rotation speed given to the first disk by the motor can be achieved. What you get on the board. In this way, when a very high speed rotation is obtained for each disk, the rotational inertia force at the time when it is increased by the large centrifugal force is extremely large. It becomes a big thing, and each disk is rotating with a very large inertia force. Obtainable.
こ の発明に よれば、 回転軸に固定 した第 1 の円板 と 、 こ の第 1 の円板の外側に順次独立に回転可能に配置 し た 環状の第 2 ない し第 n の円板 とを備え、 上記各円板の内 周, 外周の所定角度位置に相対向する も の同士は反発す る磁極の極性を示す磁石を埋め込み、 モー タ駆動に よ る 第 1 の円板の回転を隣接する 円板の対向する磁石間の磁 場反発力 に よ り 順次外周側の円板に伝達する外周側に向 けての "回転伝達動作 " が行なわれる と と も に、 最外周 の円板までがほぼ同一速度で回転する よ う にな つ た と き には、 該最外周の円板がその大き い遠心力 に よ り 自 己の 回転を増速する と と も にその際該円板の磁石でその内周 側の円板の磁石に回転付勢力 を与え こ れを増速 しなが ら こ れを振 り 切 っ て回転す る とい う "回転増速動作 " が順 次内局側に向けて行われ、 さ ら に上記外周側に向 けての 回転伝達動作 と上記内周側に向 けての回転増速動作が繰 り 返 し行われて、 .各円板がモー タ に よ り 第 1 の円板に与 え られる 回転数以上の高速の回転を行う よ う に したので、 小電力の投入で も つ て大き な円板の超高速回転が得 られ る こ と とな る。 そ して、 こ の超高速回転時には大きな遠 心力 に よ り その絶対位置に止ま ろ う とする 強大な慣性力 を保有する状態 とな り 、 こ の状態を利用 して浮上動作を 行わせる こ と もでき る効果があ る。 According to this invention, the first disk fixed to the rotating shaft and the annular second or n-th disk sequentially and independently rotatably arranged outside the first disk are provided. The opposite ones are embedded at predetermined angular positions on the inner and outer circumferences of the above-mentioned disks with magnets indicating the repelling magnetic pole polarity, and the rotation of the first disk by motor drive is performed. Due to the magnetic field repulsion between the opposing magnets of the adjacent disks, the “rotation transmitting operation” is performed toward the outer peripheral side, which is sequentially transmitted to the outer peripheral disk, and the outermost circle When the plates rotate at substantially the same speed, the outermost disk accelerates its own rotation due to the large centrifugal force, and at that time, The magnet of the disk applies a rotational urging force to the magnet on the inner peripheral side of the disk and rotates it while shaking it off while increasing the speed. The rotation speed-up operation is sequentially performed toward the internal station, and the rotation transmission operation toward the outer circumference and the rotation speed-up operation toward the inner circumference are repeated. Since each disk rotates at a speed higher than the number of rotations given to the first disk by the motor, it can be large even with the input of small power. Thus, a very high-speed rotation of a circular disk can be obtained. At the time of this ultra-high speed rotation, a large centrifugal force causes a strong inertial force to stop at the absolute position, and a floating operation is performed using this state. This has the following effects.
図面の簡単な説明 図 1 は こ の発明 の一実施例 に よ る 回転増幅装 置の斜視 図、 図 2 は こ の発明 の一実施例 に よ る 回転増幅装置 の断 面図、 図 3 は上記実施例 の要部平面図 、 図 4 ( a ), (b つ, ( d ) は上記実施例 の動作説明 図、 図 5 は上記実施例 に お いて用 い る ベ ア リ ン グの具体的構成例 を示す図で あ る 発明 を実施す る た め の最良の形態 BRIEF DESCRIPTION OF THE FIGURES FIG. 1 is a perspective view of a rotary amplifying device according to one embodiment of the present invention, FIG. 2 is a cross-sectional view of a rotary amplifying device according to one embodiment of the present invention, and FIG. 4 (a), 4 (b) and 4 (d) are views for explaining the operation of the above embodiment, and FIG. 5 shows a specific example of the structure of a bearing used in the above embodiment. BEST MODE FOR CARRYING OUT THE INVENTION
以下 こ の発明 の一実施例を図 に つ い て説明 す る c C describes the Figure an example of following this invention
. 図 1 は こ の発明 の一実施例 に よ る 回転増幅装置 O 科視 図、 図 2 は そ の横断面図、 図 3 は そ の概略平面図 、 図 4 はそ の動作説明 図であ る 。 図 に お いて 、 1 は モ ー 夕 、' 3 は上記モ ー タ 1 に よ り 回転駆動 さ れ る 回転軸、 3 a は 回 転軸 3 に一体 に形成 さ れた ス プ ラ イ ン 部、 4 は装置 匡体、 8 1 , 8 2 は回転軸 3 と 装置匡体 4 と の 間 に 設 け ら れ 、 両者間を回転 自 在 と す る ベ ア リ ン グで あ る 。 Fig. 1 is a perspective view of a rotary amplifying apparatus O according to an embodiment of the present invention, Fig. 2 is a cross-sectional view thereof, Fig. 3 is a schematic plan view thereof, and Fig. 4 is an operation explanatory view thereof. . In the figure, 1 is a motor shaft, 3 is a rotating shaft that is driven to rotate by the motor 1, and 3 a is a spline section integrally formed with the rotating shaft 3. Numeral 4 is a device housing, and reference numerals 81 and 82 are provided between the rotating shaft 3 and the device housing 4 and are bearings which rotate between them.
ま た、 .1 0 0 は そ の ス プ ラ イ ン 部 1 ひ 0 a か該 回転軸 3 の ス プ ラ イ ン 部 3 a に嵌合 し て 回転軸 3 に 固定 さ れ た '、 銅板、 ア ル ミ 板、 真鍮そ の 他の合金等か ら な り 、 外 周 半 径 R 1 2 の 円形形状を外周 形状 と し て有す る 第 1 の 円 柜 (外周 円形体) であ り 、 こ れ は 図 3 に 示す よ う に そ の外 周 の等角度間隔 の所定角 度位置、 例え ば 6 0 ° 間 隔 ご と の 6 個 の所定角 度幅の位置 に、 例 え ば外周 側 に 向 けて N 極, 内側 に 向 けて S 極を示す永久磁石 1 0 a 〜 1 0 ί 力、 埋め込み形成 さ れて い る 。 .100 is fixed to the rotating shaft 3 by being fitted to the spline portion 1a of the spline portion 1a or the spline portion 3a of the rotating shaft 3; , Aluminum plate, brass or other alloy, etc., and a first circle (circumferential circular body) having a circular shape with an outer radius R12 of an outer peripheral shape. This is, as shown in Fig. 3, at predetermined angular positions on the outer circumference at equal angular intervals, for example, at six predetermined angular widths at intervals of 60 °, for example, at the outer circumference. Permanent magnets 10a to 10 showing an N pole toward the side and an S pole toward the inside are embedded and formed.
ま た、 2 0 0 , 3 0 0 , 4 0 0 , 5 0 0 は上言己第 1 の 円板 1 0 0 の外周-に、 順次独'立に回転可能に配置さ れた 第 2 ない し第 5 の環状円板 (円.形環状体) であ り 、 第 1 ない し第 5 の円板間には隣接する 円板間を回転自在 とす るベア リ ン グ 1 2, 2 3 , 3 4 , 4 5 がそれぞれ介在さ れている。 Also, 200, 300, 400, and 500 are the first A second or fifth annular disk (circular annular body), which is sequentially and independently rotatably arranged on the outer periphery of the disk 100, and is the first or fifth annular disk. Bearings 12, 23, 34, and 45 are interposed between the disks so that the adjacent disks can rotate freely.
上記 4 つの環状円板の う ち 円板 2 0 0 , 3 0 0 , 4 0 0 は内周半径 R i 1 ( > R ( i - 1 ) 2 ) , 外周半径 R Of the above four circular disks, disks 200, 300, and 400 are the inner radius R i 1 (> R (i-1) 2) and the outer radius R
1 2 ( i = 2 , '3 , ' 4 ) を有 し、 その内周の上記第 1 の 円板と同 じ 6 0 ° 間隔の所定角度幅の位置に、 内周側に 向けて Ν極, S極, Ν極の極性を示す永久磁石 2 0 a 〜1 2 (i = 2, '3,' 4), and at its inner circumference, at the same angle of 60 ° as the first disk, at a predetermined angular width, the pole is directed toward the inner circumference. , S pole, and 永久 pole permanent magnets 20 a
2 0 f , 3 0 a〜 3 0 f , 4 0 a 〜 4 0 i を埋め込み形 成 し、 その外周の上記と同 じ 6 0 ° 間隔の所定角度幅の 位置に、 外周側に向 けて S極, N極, S極の極性を示す 永久磁石 2 1 a〜 2 1 f , 3 1 a 〜 3 1 f , 4 1 a 〜 420f, 30a to 30f to 40f to 40i to 40i are formed by embedding, and the outer periphery of the outer periphery is positioned at the same angular width of 60 ° as above on the outer periphery. Permanent magnets indicating the polarity of the S, N, and S poles 21 a to 21 f, 31 a to 31 f, 41 a to 4
1 f を埋め込み形成 してい る。 ま た、 第 5 の円板 5 0 0 は内周半径 R n i ( > R ( n - 1 ) 2 ) , 外周半径 R n 2 ( n = 5 ) を有 し、 'その内周の上記 と同 じ 6 0 ° 間隔 の所定角度幅の位置に 内周側に向 けて S極の極性を示 す永久磁石 5 0 a〜 5 0 f を埋め込み形成 し、 その外周 には永久磁石を設けていない。 1 f is buried. The fifth disk 500 has an inner radius R ni (> R (n-1) 2) and an outer radius R n 2 (n = 5). Permanent magnets 50a to 50f indicating the polarity of the S pole are buried toward the inner peripheral side at a predetermined angular width at the same 60 ° interval, and no permanent magnet is provided on the outer periphery. .
ま た、 1 0 1 , I 0 2 は上記第 1 の円板 I 0 0 の外周 に近い位置のそれぞれ上, 下面に固定 して設け られ、. そ の外周側にあ る第 2 の円板 2 0 0 の上下方向の移動を規 制する ための、 断面 L字状かつ平面環状の外周 円板上下 動規制体であ り 、 該上下動規制体 1 0 1 , 1 0 2 と 第 2 の 円板 2 0 0 と の間 に はベア リ ン グ 6 1 , 6 2 が、 該上 下動規制体 〗 0 1 , 1 0 2 と装置匡体 4 と の間 に はベア リ ン グ 6 3 , 6 4 が、 そ れぞれ設け られて い る 。 外周 円 板上下動規制体 2 0 1 , 2 0 2 , 3 0 1 , 3 0 2 , 4 0 1 , 4 0 2 について も 全 く 同様であ り 、 そ れ ぞれ第 2 , 第 3 , 第 · 4 の 円板に設 け ら れ, 第 3 , 第 4 , 第 5 の 円板 の上下動を規制す る ための も のであ る 。 Also, 101, I02 are fixedly provided on the upper and lower surfaces, respectively, at positions near the outer periphery of the first disk I00, and the second disk on the outer peripheral side thereof is provided. An upper and lower peripheral disk with an L-shaped cross section and a plane ring to regulate the vertical movement of 200 A bearing 61, 62 between the vertical movement restricting body 101, 102 and the second disc 200, and the vertical movement restricting body.ベ ア Bearings 63, 64 are provided between 01, 102 and the device housing 4, respectively. The same applies to the outer peripheral disk vertical movement restricting bodies 201, 202, 300, 300, 400, 402, respectively, and the second, third, and second respectively. · It is installed on the 4th disc to regulate the vertical movement of the 3rd, 4th and 5th discs.
こ こ で、 本構成では、 銅板、 ア ル ミ 板、 真鍮等の合金 か ら な る 半磁性体あ る いは非磁性体の 円板に 凹部を形成 して こ れに永久磁石を埋め込んでい る が、 該円板材料の 磁化に よ っ て永久磁石の磁界が乱 さ れ る と い う よ う な こ と はな く 、 該円板の外側に は該永久磁石に よ る そ の ま ま の磁場が形成 さ れ る も のであ る 。 In this configuration, a recess is formed in a semi-magnetic or non-magnetic disc made of an alloy such as a copper plate, an aluminum plate, or brass, and a permanent magnet is embedded in the recess. However, the magnetic field of the permanent magnet is not disturbed by the magnetization of the disc material, and the outside of the disc is not affected by the permanent magnet. The same magnetic field is formed.
こ こ で、 上記各 円板の外周半径 R 1 2 〜 R 5 2 , 内 周 半径 R 2 1 〜 R 5 1 は と も に 同一半径ずつ大 き く な る の が理想的であ る。 ま た、 各円板の磁石 3 0 a 等の 円周 方 向の長 さ 1 と 、 磁石 3 0 a , 3 0 b 等間の距離 d と の関 係 と して は、 本発明装置の後述す る動作を理論的 に可能 とす る ため と、 こ れに加えて該動作に多少遊びを も たせ め、 距離 d が長 さ 1 よ り 若干長い関係 と して い る 。 Here, it is ideal that the outer radii R12 to R52 and the inner radii R21 to R51 of each of the above-mentioned disks are both increased by the same radius. In addition, the relationship between the circumferential length 1 of the magnet 30a and the like of each disk and the distance d between the magnets 30a and 30b is described later in the present invention. The distance d is set to be slightly longer than the length 1 in order to theoretically enable the following operation and, in addition, to allow the operation to have some play.
次に、 図 5 は本装置において用 い る , 2 つの円板間 に 設け る ベア リ ン グ 1 2 , 2 3 , 3 4 , 4 5 の具体的構成 の一例を示す。 図 にお いて、 ボー ルベア リ ン グ 7 0 は内 周側の円板 1 0 0 , 2 0 0 等に設け られたボー ル保持具 7 1 と、 こ れに よ り 保持さ れたボール 7 2 とか ら な っ て お り 、 該ボール 7 2 は、 上記保持具 7 1 の内面 と外周側 の円板 2 0 0 , 3 0 0 等の内周面 との間で回転可能に惜 接する配置とな っ てい る。 Next, Fig. 5 shows an example of the specific configuration of the bearings 12, 23, 34, and 45 provided between two disks used in this device. In the figure, ball bearings 70 are The ball is composed of a ball holder 71 provided on the discs 100, 200, etc. on the peripheral side, and a ball 72 held by the ball holder 72. However, it is arranged so as to be rotatable between the inner surface of the holder 71 and the inner surface of the disk 200, 300 or the like on the outer peripheral side.
次に本装置の動作について図 1 ない し図 4 を用 いて説 明する。 Next, the operation of this device will be described with reference to FIGS.
本回転増幅装置においては、 第 1 の円板 1 0 0 、 第 2 , 第 3 , 第 4 , 第 5 の環状円板 2 0 0 , 3 0 0 , 4 0 0 , 5 0 0 は別体で構成されてお り 、 それぞれ独立に回転可 能な状態に配置さ れてい る。 モ一 夕 1 を駆動 していない 静止状態では、 隣接する 円板の対向する磁石は同一極性 を示す も の と している ので、 こ れ ら の磁石間の磁場反発 力 に よ り 各円板は図 3 に示すよ う に隣接する 円板の相対 向する磁石同士が最も離れた位置に来る状態, 即 ち磁石 3 0 a , 3 0 b 間の中間に磁石 2 1 a が来る状態で静止 してレ、 る。 In this rotary amplifying device, the first disc 100, the second, third, fourth, and fifth annular discs 200, 300, 400, 500 are separate bodies. And are arranged so as to be rotatable independently of each other. In the stationary state where the motor 1 is not driven, the opposing magnets of the adjacent disks are assumed to have the same polarity, and each disk is affected by the magnetic field repulsion between these magnets. As shown in Fig. 3, the magnets facing each other on adjacent disks come to the farthest position, that is, the magnet 21a comes in the middle between magnets 30a and 30b, and comes to rest. I do.
こ の状態において、 図示 しないバ ッ テ リ 等の電圧供給 手段よ り の電圧をモー 夕 1 に印加する と、 該モー タ 1 の 回転に よ り 回転軸 3 およ び'こ れ と一体の第 1 の円板 1 0 0 が回転する。 該第 1 の円板 1 0 0 が回転する と、 該第 1 の円板の磁石の回転に よ り 第 2 の円板の磁石が磁石間 の磁場反発力を受けて同方向に回転駆動さ れ、 同様に し て順次よ り 外周側の円板が回転駆動 さ れ る こ と とな り 、 各 円板がほ ぼ同一速度で回転 9 よ う に な Q c - 電圧の供給を始めて ま も な い始動 時 に は、 七 一 夕 よ り G 回転駆動力 に よ り 内周 側の 円板 は Z- の磁石が外 周 側 円 板の磁石の ほ ぼ中 間 に来 る と い う 位置関係 を越え て と 八 どん回転す る が、 し ば ら く す る う ち に外周 側 の 円 板か順 次増速 さ れて やがて すベて の 円板か ほ ぼ同一速度て 回転 す る よ う に 。 こ う し て、 磁石間 の磁場反発力 用 い た外周側への " 回転伝達動作 " が行わ れ て 各 円 板 ; z- 一疋速度の回転 に達す る と 、 外周 側の 円 板ほ ど そ o平面 積,· 従 つ て重量が大 き く 、 回転時 作 用 す 3≤ 'し、力 に よ つ て重直が増 し た かの如 く に 増大 さ れ る 慣性 ェ ネ ノ キ 一 即 ち フ ラ ィ ホ イ 一 ル効果 と も 言 え 慣性力 が よ り 大 き い 'の で、 こ の外周 側の 円 板 は 内 周 側 の 円板 を振 り 切 In this state, when a voltage from a voltage supply means such as a battery (not shown) is applied to the motor 1, the rotation of the motor 1 causes the rotation axis 3 and the integral part of the motor to rotate. The first disk 100 rotates. When the first disk 100 rotates, the rotation of the magnet of the first disk causes the magnet of the second disk to receive a magnetic field repulsive force between the magnets and rotate in the same direction. Similarly, the disks on the outer peripheral side are sequentially driven to rotate, and At the start, when each disk starts to supply Qc-voltage such that it rotates at almost the same speed9, the disk on the inner peripheral side by the G rotation driving force from 71- Will rotate steadily beyond the positional relationship that the magnet of Z- will be almost in the middle of the magnet on the outer circumferential disk, but the outer circumferential circle will soon be out of the way. The discs are gradually increased in speed, and eventually all the discs rotate at almost the same speed. In this way, when the "rotation transfer operation" to the outer circumference side using the magnetic field repulsion force between the magnets is performed and the rotation of each disk is reached; the rotation of the outer circumference side is almost completed. oArea area, therefore large in weight, works during rotation 3≤, and is increased by force as if the straightness is increased. In other words, the inertia force is greater than the flywheel effect, so the disk on the outer periphery shakes the disk on the inner periphery.
( こ れを越えて ) 回 ろ う と す る か こ の と き 外 周 側 G 円 板 (磁石 ) は 内 周 側の 円板 ( 磁石 に 対 し 回転方 Γ口」 、 付勢力 を与え つつ、 即 ち 、 内 側 の 円 板 の 回転 を増速 し が ら 、 こ れ よ り 速 く 回転す る こ と と な 。 こ の よ う に 回 転: IS 、力 に よ っ て増大せ ら れ る 回転慣性力 に よ つ て よ り 自 己の回転 ¾:速め な 力 ら 内側の 円 板を も 増速す る " 回転 増幅動作 " が順次そ の 内周 側の磁石 と さ ら に そ の 内 周 側 の磁石 と の 間 で も 行われて最内 周 の 円 板 ま で行わ れ る 二 と と な る が、 こ の 間 に も 上記最外 の 円 板 の磁石か上記 内 周 側の 円板の 1 つ の磁石を越え 回転 し て 内 周 側 の磁 石の ほ ぼ中 間位置 に来た と き に は つづ い て上記 と 同 様 の 動作を繰 り 返すこ と とな る か ら、 上記内周側に向 けて G "回転增幅動作 " は繰 り 返 し繰 り 返 し行われ る こ と と な る。 以下、 上述 した外周側に向けての回転伝達動作につ づ く 、 内周側に向けての回転増幅動作の詳細を、 図 4 を 参照して説明する。 When turning (beyond this), the outer peripheral G disk (magnet) is turned to the inner disk (rotating port for the magnet), while applying an urging force. Immediately, the inner disk rotates at a higher speed while rotating at a higher speed, and thus rotating at a higher speed. Self-rotation due to the rotational inertia force ¾: The “rotation amplification operation”, which increases the speed of the inner disk from a faster force, is sequentially performed on the inner magnet and the magnet. Between the magnet on the inner peripheral side and the innermost disk, and so on, but also between the magnet on the outermost disk and the magnet on the inner peripheral side. When the rotor rotates past one magnet of the disk and comes to a position almost in the middle of the magnet on the inner peripheral side, the same as above Since the operation is repeated, the G "rotational width operation" is repeatedly performed toward the above inner peripheral side. Hereinafter, the details of the rotation amplifying operation toward the inner peripheral side after the rotation transmitting operation toward the outer peripheral side described above will be described with reference to FIG.
図 4 ( a ) 〜(d ) は、 第 1 の円板の図示矢印 X方向 (右 回転方向) への回転が順次第 5 の円板まで伝達さ れた後、 第 5 の円板がその大き な回転遠心力 に よ り 第 4 の円板を 振 り 切 っ て回転する、 即ち、 磁石間の位置関係を越えて 回転する際の様子、 さ ら に こ の際に増速さ れた第 4 の円 板が第 3 の円板を振 り 切っ て回転する際の様子を示す医 であ る。 Figs. 4 (a) to 4 (d) show that the rotation of the first disk in the direction indicated by arrow X (clockwise rotation) is sequentially transmitted to the fifth disk, and then the fifth disk is rotated. The fourth disk is swung off by a large rotating centrifugal force and rotated, i.e., when rotating beyond the positional relationship between the magnets, and further accelerated at this time He is a physician showing how the fourth disk rotates while shaking off the third disk.
同図(a ) に示す第 5 の円板ま で回転が伝達さ れた状態 では、 第 3 の 円板 3 0 0 の外周 の磁石 3 1 a は、 図示 X 方向に 自 ら回転 しなが ら第 4 の 円板 4 0 0 の内周 G磁石 4 0 a に対 し図示右方向への回転付勢力 F 1 1 を与え、 他方、 第 3 の円板の磁石 3 1 b はやは り 回転 しなが ら上 記磁石 4 0 a に対 し図示左方向への回転付勢力 F 1 1 ' を与えてお り 、 磁石 3 l b , 3 1 c と磁石 4 O b 間に も 同様の力 F 1 2 , F 1 2 ' が作用 してい る。 ま た、 第 4 の円板の外周の磁石 4 1 f もやは り 回転 しなが ら第 5 の 円板の内.周の磁石 5 0 a に図示右方向への回転付勢力 F 2 を与え、 他方、 第 4 の円板の外周 の磁石 4 1 a も やは り 回転 しなが ら上記磁石 5 0 a に図示左方向への回転付 勢力 F 2 ' を与えて お り 、 こ の状態 に お い て 、 第 3 , 第 4 , 第 5 の 円板 は、 ほ ぼ こ の 図 4 ( a ) に 示す よ う な 磁石 間 の位置関係 を保 ち な が ら 、 かつ上記各回転付勢力 を相 互に加 え な が ら 図示 X 方向 に 同一速度で回転 し て い る も ので あ る 。 In the state where the rotation is transmitted to the fifth disk shown in FIG. 11A, the magnet 31a on the outer periphery of the third disk 300 rotates in the X direction in FIG. Gives a rotational urging force F 11 to the inner circumference G magnet 40 a of the fourth disk 400 in the right direction in the figure, while the magnet 31 b of the third disk 400 While rotating, a rotational urging force F11 'is applied to the above magnet 40a in the left direction in the figure, and the same force is applied between magnets 3lb, 31c and magnet 4Ob. F 1 2 and F 1 2 'are acting. In addition, while rotating the magnet 41 f at the outer periphery of the fourth disk, the inner circumferential surface of the fifth disk is subjected to a rotational urging force F2 to the right magnet 50a. On the other hand, while the magnet 41a on the outer periphery of the fourth disk is still rotating, the magnet 50a is rotated to the left in the drawing. In this state, the third, fourth, and fifth disks are almost in the positional relationship between the magnets as shown in FIG. 4 (a) under the influence of the power F 2 ′. While maintaining the above, and while applying the above-mentioned rotational biasing forces to each other, they are rotating at the same speed in the X direction shown in the figure.
そ して、 最内周 の 円板か ら こ の最外周 の 円 板 5 0 0 ま でがほ ぼ同一速度で回転す る 状態 に達す る と 、 外 周 側 の 円板ほ ど遠心力 が大 き い の で、 第 5 の 円 板 5 0 0 は そ の 最 も 大き い遠心力 に よ り そ の重みが増 し た か の 如 : に 回 . 転慣性力 が増大せ ら れ、 該 円板の磁石 5 0 a に着 目 す れ ば、 該回転慣性力 が上記磁石 4 1 a か ら の左方 向 へ の 回 転付勢力 に打ち 勝 っ て該磁石 4 1 a を越え て 回転 し ょ う と す る こ と と な る 。 そ して 、 こ の第 5 の 円 板の 回転 に よ り そ の磁石 5 0 a は 図 4 ( b ) に 示す よ う に磁石 4 1 a の 上部 の大半を お お う 位置 に つ っ こ む よ う な 感 じ と な る か、 こ の状態で は上記 F 2 , F 2 ' ( 磁力 に よ る 回 転方 向 へ ' の付勢力 ) は ほ と ん ど無い こ と と な り 、 上記第 5 の 円 板 は慣性力 に よ り さ ら に 図示右方向 に そ の ま ま 回 転 し て 、 図 4 ( c ) に示す よ う な 位置 に来 る こ と と な る 。 When the state from the innermost disk to the outermost disk 500 is rotated at almost the same speed, the centrifugal force of the outer disk is almost equal to that of the outermost disk. Because of its large size, the fifth disk 500 has an increased rotational inertia force as if its weight was increased by its largest centrifugal force. If attention is paid to the disk magnet 50a, the rotational inertia overcomes the leftward biasing force from the magnet 41a and rotates beyond the magnet 41a. You are trying to do that. Then, by the rotation of the fifth disk, the magnet 50a is brought to a position covering most of the upper part of the magnet 41a as shown in FIG. 4 (b). In this state, the above F 2 and F 2 ′ (the biasing force of ′ in the rotating direction by the magnetic force) are almost non-existent. The fifth disk is further rotated to the right in the drawing by inertia force, and comes to a position as shown in FIG. 4 (c).
こ の 図 4 ( c ) の位置で は、 磁石 5 0 a が磁石 4 1 a の 上部の大半を過 ぎ た こ と に よ っ て磁石 4 1 a が、 よ り 高 速で回転 し て い る 磁石 5 0 a に対 し こ れ を図示右方 向 へ 回転付勢す る 力 F 4 を与え る こ と と な り 、 一方 よ り 高速 回転 に な っ て お り 磁石 4 1 a の大半部 を過 ぎ た磁石 5 0 a は次の磁石 4 l . b に対 して-こ れを図示右方向 に回転付 勢する力 ί 4 を与える こ ^: とな .る。 こ の と き、 第 3 と第 4 の円板間は図 4 ( a ) の場合 とほぼ同 じ位置関係にあ り 、 両者間ほぼ同 じ力 F 1 1 , F 1 1 ' , F 1 2 , F 1 ' が働いている。 At the position shown in FIG. 4 (c), the magnet 41a is rotating at a higher speed because the magnet 50a has passed most of the upper part of the magnet 41a. The magnet 50a is given a force F4 that urges the magnet 50a to rotate to the right in the figure, while the magnet 50a is rotating at a higher speed than the magnet 50a. Overpassed magnet 5 0 a exerts a force ί 4 on the next magnet 4 l. b to urge it to rotate rightward in the figure ^:. At this time, the positions of the third and fourth disks are almost the same as in FIG. 4 (a), and the forces F11, F11 ', F12 are almost the same. , F 1 'are working.
従っ て、 第 4 の円板は、 その磁石 4 1 b が こ の よ う に して加速される こ と に よ っ て上述 した図 4 (a ) 力、 ら図 4 ( b ) への磁石 5 '0 a の動作 と同様に して、 磁石 4 1 b 力、 図 4 ( d ) に示す磁石 3 1 c をおお う 位置へつ つ 込むよ う な感 じ とな って こ れを越えて回転 し、 上記 と 同様に内馬 側の磁石を増速する こ と と な る。 こ の よ う に し て順次大 き な遠心力 に よ り 増大せ られて大き な回転慣性力を も つ 外周側の磁石が内周側の磁石を越えて回転 しつつ内周规' の円板を増速する動作が、 内周側に向か っ て進む こ と と る o Accordingly, the fourth disk is driven by the magnet 41b as shown in FIG. 4 (a) due to the fact that the magnet 41b is accelerated in this manner. 5 In the same manner as in the operation of '0a, the magnet 41b force is applied and the magnet 31c shown in Fig. 4 (d) is pushed into the covering position. And the speed of the magnet on the inner horse side is increased in the same manner as above. In this way, the outer peripheral magnet rotates over the inner peripheral magnet while having a large rotational inertia force, which is increased by a large centrifugal force. The operation of increasing the speed of the plate proceeds toward the inner circumference o
こ の よ う に、 .第 1 の円板の回転が順次最外周 の円扠ま で伝達さ れたのち、 最外周の円板がその大き な遠心力 に よ り 増大せ られる大きな回転慣性力で も っ て よ り 高速で 回転 し、 その内周側の円板の磁石との位置関係を越えて 回転する と き、 該最外周の円板はその 1 つ内周側の円板 を加速 しなが ら回転 し、 該加速さ れた内周側の 円板は同 様に してその内周側.の円板を加速 しなが らその内周側の 円板の磁石 との位置関係を越えて回転 し、 以下同様の動 作が行われて、 順次最内周の円板ま でが加速さ れ る こ と と な o そ し て、 最内 周 の第 1 の 円 板 1 0 0 がカ卩速 さ れ る と の 円板 は上述 の動作 と 同 様 に順次外周 側 に 向 て第 2 , 第 3 , 第 4 の 円板 に 回転 を伝達 さ れ 、 以下 再 び内周 向 か っ て上記 と 同様 の 回転増幅動作か行わ れ る こ と と な り 、 各 円板 に は モ ー 夕 に よ り 第 1 の 円 板 に 与え ら れ る 回転数以上の非常 に高速 な 回転速度が得 ら れ る こ と と な る In this way, after the rotation of the first disk is sequentially transmitted to the outermost circle, the outermost disk is increased by its large centrifugal force to increase the rotational inertia. Therefore, when rotating at a higher speed and rotating beyond the positional relationship of the inner disk with the magnet, the outermost disk accelerates one of the inner disks. While rotating, the accelerated inner disk is similarly rotated while its inner disk is accelerated while the inner disk is positioned with the magnet. It rotates beyond the relationship, and the same operation is performed thereafter, so that the innermost disk is sequentially accelerated. Then, the disk on which the innermost first disk 100 is rotated at the speed of kneading is sequentially moved toward the outer peripheral side in the same manner as in the above-described operation. The rotation is transmitted to the fourth disk, and the rotation amplifying operation similar to the above is performed again toward the inner circumference. A very high rotation speed higher than the rotation speed given to the disk 1 can be obtained.
な お こ こ で 、 第 1 の 円板が第 2 な し、 し 第 5 の 円 板 を 介 して の 回転増 ½動作 に よ り モ 一 夕 駆動 に よ る 回転数 以上 の速度 に加速 さ れ る と き に は モ 一 夕 に対 し て は負 荷か非 常 に な つ て い る も の で あ り 、 モ ー 夕 自 体 の 回転 も 同 栋 ^速 く な つ て い る も の で あ る 。 Here, the first disk is accelerated to a speed equal to or higher than the rotation speed of the motor drive by the rotation increasing operation via the second disk and the fifth disk. At that time, the load is in emergency or unusual with respect to the motor, and the rotation of the motor itself is also becoming faster. It is.
の よ う に、 本回転増幅装置で は最初 の 第 1 の 円 板 の 回転を、 外側 に、 内側 に、 外側 に 、 内側 に 、 と 順次 伝達 増幅 して い く こ と と な り 、 最終的 に は 各 円板 に あ る 極限 的 な超高速の 回転が得 ら れ る こ と と 7よ る 。 最外周 o 円 杞 等に こ の よ う な極限的な 超高速回転が得 ら れ る と 、 そ の と き の回転 に よ る ; IS心力 な ら び に こ れ に よ り 増大せ ら れ る 回転慣性力 は非常 に大 き く 、 そ の絶対位置 に止 ま ろ う と す る 強大な慣性力 を保有す る 状態 と な り 、 こ の絶対位 置に止 ま ろ う と す る 強大な慣性力 を保有 し た状態で は浮 上動作を行な う こ と も 可能 と な る も ので あ 0 As described above, in the present rotary amplification device, the rotation of the first disk is transmitted and amplified sequentially to the outside, the inside, the outside, the inside, and so on. According to Fig. 7, the extremely high-speed rotation of each disk can be obtained. If such an ultra-high-speed rotation is obtained at the outermost circumference o circle or the like, it depends on the rotation at that time; the IS heart strength and the increase due to this The rotational inertia force is very large, and a state is maintained in which a large inertia force is maintained to stop at that absolute position, and a strong attempt is made to stop at this absolute position. It is possible to perform a levitation operation while maintaining a high inertia force.
な お上記実施例 に お いて、 各 円板の一円 周 上 に設 け る 磁石の数、 磁石の 円 周 方向 の長 さ 1 , 即 ち 磁 設 け る I 4 In the above embodiment, the number of magnets provided on one circumference of each disk, the length of the magnets in the circumferential direction is 1, and the magnets are provided immediately. I 4
位置の角度幅、 およ び磁石閭の距離 d 、 各円板の内周, 外周半径、 およ びその質量、 隣接する 円扳間の距離、 お よ び磁石の磁力 については、 各要素相互間の相関関係を 考慮 して適宜設定する のがよい。 The angular width of the position, the distance d of the magnet, the inner and outer radii of each disk, and their mass, the distance between adjacent circles, and the magnetic force of the magnet, It is better to set appropriately in consideration of the correlation.
ま た上記実施例では、 各円板の磁石の極性を、 同 じ円 板の内周側の磁石 と外周側の磁石 とでは反対極性を示す も の と したが、 こ れは同 じ円板の内周側, 外周側の磁石 が と も に同 じ極性、 従っ てすベての磁石が外方に向か つ て同 じ極性、 例えば N極を示す も の と して も よ い。 In the above embodiment, the polarity of the magnet of each disk is opposite to that of the magnet on the inner circumference side and the magnet on the outer circumference side of the same disk, but this is the same disk. The inner and outer magnets may have the same polarity, and all magnets may have the same polarity outward, for example, the N pole.
ま た上記実施例では、 各環状円板の上下方向の移動を 規制する手段を、 該円板の内周側の円板に上下動規制体 を設けて構成 したが、 こ れは例えば匡体に最外周 の円板 用の上下動規制体を設け、 以下外周側の円板にその内周 側の円板用の上下動規制体を設けて も よ い。 ま た、 上記 上下動規制体は円板の形状に沿っ た環状の も のではな : 、 円周上の数ケ所の位置のみに設けて も よ い。 Further, in the above embodiment, the means for restricting the vertical movement of each annular disk is constituted by providing a vertical movement restricting member on the disk on the inner peripheral side of the disk. It is also possible to provide a vertical movement restrictor for the outermost disk, and to provide a vertical movement restrictor for the inner disk below on the outer disk. Further, the above-mentioned vertical movement restricting body is not an annular one following the shape of the disk: it may be provided only at a few positions on the circumference.
ま た上記実施例において、 ベア リ ン グの磨耗を防止す る ため装置匡体の内部に潤滑オイ ルを封入する よ う に し て も よい。 ま た、 各円板間, 匡体 と規制体間, 規制体 と 円板間に設ける ベア リ ン グ—にボ一ルベア リ ン グを用 いた が、 必ず し も こ れに限定ざれる も のではな く 、 磁石間の 磁場反発力等を用いて該雨者間を回転可能に保持で き る ベア リ ン グを構成 して も よい。 Further, in the above-described embodiment, a lubricating oil may be sealed inside the device housing to prevent wear of the bearing. In addition, although ball bearings are used for the bearings provided between the discs, between the housing and the regulating body, and between the regulating body and the discs, the ball bearings are always limited to these. Instead, a bearing that can rotatably hold between the rainers using a magnetic field repulsion force between magnets or the like may be configured.
ま た上記実施例では、 モー 夕 1 の出力軸を直接回転軸 3 と し たが、 こ れ は例 え ばモ ー タ を回転軸 3 と 離れ た 位 置 に設 け、 タ イ ミ ン グベ ル ト 、 プ ー リ 一 等 を介 し て 回転 軸をモ ー タ 駆動す る 等の構成 と し て も よ い。 In the above embodiment, the output shaft of motor 1 is directly For example, the motor is installed at a position distant from the rotating shaft 3 and the rotating shaft is controlled via a timing belt, pulley, etc. It may be configured to drive the motor.
さ ら に上記実施例で は、 停止時, 低速回転時等 に る 各円板の支持等の た め に装置匡体 4 を設 け た か、 本発 明では必ず し も こ の装置匡体 を設 け る 必要 は な い。 Further, in the above embodiment, the device housing 4 is provided for supporting each disk at the time of stop, low-speed rotation, and the like, or in the present invention, the device housing 4 is always provided. There is no need to set up.
ま た上記実施例で は、 隣接す る 円板間 を 回転可能 と す る た め両者間 に べァ リ ン グを 介在 さ せ た か 、 何 ら か の手 段 に よ り 、 あ る い は何 ら の手段が な '、 て も 静止 あ る い は . 回転状態て の 隣接す る 円板間 の 距離を一定 に 保持す る こ と がで き れ ば こ れは必ず し も 設 け る 必要 は な い。 Further, in the above-described embodiment, depending on whether or not a bearing is interposed between the adjacent disks so as to be rotatable between the two disks, some means may be used. If there is any means to keep the distance between adjacent disks in a stationary or rotating state, this must be provided if the distance between adjacent disks can be kept constant. There is no need to do this.
ま た上記実施例で は、 第 1 の外周 円形体 と し て 円 板 を 、 第 2 な い し第 5 の 円形環状体 と し て 環状 円板を 用 い た例 を示 し たが、 外周 円形体 は 円 形 の外周 形状 を有す る t O であ れ ばそ の断面 は平板 に 限 ら ず任意の形状 の ί J て ; く 、 ま た 円形環状体 も 円形形状の環状体で あ れ は そ の 断 面 は平板 に 限 ら ず任意の形状の も の で よ い。 Further, in the above embodiment, an example is described in which a disc is used as the first outer circular body and an annular disc is used as the second or fifth circular annular body. If the circular body is tO having a circular outer shape, its cross-section is not limited to a flat plate, but may be any shape, and the circular annular body may also be a circular annular body. The cross section is not limited to a flat plate, but may be of any shape.
産業上の利用可能性 Industrial applicability
こ の発明 を利用 して新た な 浮上原理 に基づ く 飛行体 を 構成す る こ と がで き る 。 請 求 の 範 囲 Using this invention, a flying object based on a new levitation principle can be constructed. The scope of the claims
1 . モー タ に よ り 回転さ れる 回転軸 と、 1. A rotating shaft that is rotated by the motor,
上記回転軸に固定さ れ、 外周半径 R 1 2 を有 し、 その 外周の等角度間隔の所定角度位置に外周側に向 けて同一 磁極の極性を示す磁石を有する第 1 の外周 円形体 と、 第 ( i 一 1 ) ( i は 2 以上 n — 1 ま での整数) の外周 円形体ま たは円形環状体の外周に配置さ れ、 内周半径 R i 1 ( > R ( i - I ) 2 ) , 外周半径 R i 2 を有 し、 そ の内周, 外周のそれぞれの上記 と同 じ所定角度位置に、 上記第 ( i 一 1 ) の外周 円形体ま たは円形環状体の外属 の磁石が外周側に向 けて, 第 ( i + 1 ) の 円形環状体の 内周の磁石が内周側に向けてそれぞれ示す極性 と反発す る磁極の極性をそれぞれ内周側に向 けて, 外周側に向 け て示す磁石を有する第 i の円形環状体 と、 A first outer circular body fixed to the rotating shaft, having an outer peripheral radius R 12, and having a magnet having the same magnetic polarity toward the outer peripheral side at a predetermined angular position at an equal angular interval on the outer peripheral side; , The (i−1) (i is an integer from 2 to n—1) outer periphery of a circular body or a circular annular body, and an inner radius R i 1 (> R (i−I ) 2), having an outer radius R i 2, and at the same predetermined angular position on the inner circumference and the outer circumference, the outer circumference of the (i-11) outer circumference circular body or the circular annular body. The (i + 1) -th ring-shaped inner magnet has the polarity shown toward the inner circumference and the polarity of the repelling magnetic pole toward the inner circumference, respectively. An i-th circular annular body having magnets directed toward the outer periphery;
第 ( n — 1 ) ( n は 3 以上の整数) の円形環状体の外 周 に配置さ れ、 内周半径 R n l ( > R ( n - 1 ) 2 .) , 外周半径 R n 2 を有 し、 その内周の上記 と 同 じ所定角度 位置に、 第 ( n — 1 ) の環状体の外周 の磁石がその外属 側に向けて示す極性と反発する磁極の極性を内周側に向 けて示す磁石を有する第 n の円形環状体 とを備えた こ と を特徵 とする回転.増幅装置。 It is arranged on the outer circumference of the (n-1) th (n is an integer of 3 or more) circular annular body and has an inner circumference radius Rnl (> R (n-1) 2.) And an outer circumference radius Rn2. At the same predetermined angular position on the inner circumference as above, the magnets on the outer circumference of the (n-1) -th annular body turn the polarity of the repelling magnetic pole toward the outer side toward the inner circumference. A rotating amplifying device, comprising: an n-th circular annular body having a magnet shown in FIG.
2 . 上記.第 1 の外周円形体 と第 2 の円形環状体 と の間, およ び第 i の円形環状体 と第 ( i 十 1 ) の円形環状体 と の間に各々 該両者間を回転可能とする ベア リ ン グが設け られてい る こ と を特徴 と す る 請求の範囲第 1 項に記載の 回転増幅装置。 2. Between the first peripheral circular body and the second circular annular body, and between the i-th circular annular body and the (i11) th circular annular body, the two are respectively connected to each other. A rotatable bearing is provided. The rotary amplifying device according to claim 1, wherein the rotary amplifying device is provided.
3 . 上記第 2 な い し第 n の円形環状体の上下方向 の移動 を規制す る ため の上下移動規制体を、 さ ら に備え た こ と を特徴 とす る 請求の範囲第 1 項 ま た は第 2 項に記載の回 転増幅装置。 3. A claim 1 characterized by further comprising a vertical movement restricting body for restricting the vertical movement of the second or n-th circular annular body. Or the rotary amplifying apparatus according to paragraph 2.
4 . 上記第 i ( i は 2 以上 n — 1 ま での整数) の環状体 用 の上下移動規制体は、 上記第 ( i - 1 ) の外周 円 形 体 ま た は第 ( i 一 1 ) 円形環状体に固定 し て設 け ら れ て い る こ と を特徵 と す る請求の範囲第 3 項に記載の回転増幅 4. The vertical movement restricting body for the i-th annular body (i is an integer from 2 to n-1) is the (i-1) -th peripheral circular body or the (i-i-1) -th circular body. 4. The rotational amplification according to claim 3, wherein the rotational amplification is fixed to the circular ring-shaped body.
5 . 上記回転軸 , 第 1 の外周 円形体, お よ び第 2 な い し 第 n の円形環状体を収容す る 装置匡体を、 さ ら に備え た こ と を特徵 とす る 請求の範囲第 1 項な い し第 4 項の いず れかに記載の回転増幅 5. A claim characterized by further comprising a device housing for accommodating the rotating shaft, the first outer circular body, and the second or n-th circular annular body. Rotational amplification according to any of the first or fourth term
6 . 上記第 1 の'外周 円形体, 第 2 な い し第 ( n — 1 ) の 円形環状体にそ れぞれ設けた第 2 な い し第 n の 円形環状 体用,の上下移動規制体 と上記装置匡体 と の間 に該両者間 を回転 自在 とす る ベア リ ン グを設け、 該第 2 な い し第 n の 円形環状体用 の上下移動規制体 と第 2 な い し第 n の 円 形環状体 と の間に該両者間を回転 自 在 と す る ベア リ ン グ を設けた こ と を特徴 とす る請求の範囲第 4 項 ま た は第 5 項に記載の回転増幅装 6. Restriction of vertical movement of the first 'outer circumference circular body and the second or nth circular annular body provided on the second or (n-1) th circular annular body, respectively. A bearing is provided between the body and the device housing so as to be rotatable therebetween, and a vertical movement restricting body for the second or n-th circular annular body is provided. The bearing according to claim 4 or 5, characterized in that a bearing is provided between the n-th circular annular body and the bearing so as to rotate between the two. Rotary amplification device
Priority Applications (7)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| PCT/JP1991/001491 WO1993009591A1 (en) | 1991-10-31 | 1991-10-31 | Rotation amplifying device |
| JP18321592A JP3632212B2 (en) | 1991-10-31 | 1992-06-17 | Flywheel |
| PCT/JP1992/001394 WO1993009589A1 (en) | 1991-10-31 | 1992-10-28 | Rotary apparatus |
| KR1019940701401A KR100282542B1 (en) | 1991-10-31 | 1992-10-28 | Rotator |
| DE69209516T DE69209516T2 (en) | 1991-10-31 | 1992-10-28 | TURNING DEVICE |
| CA002122452A CA2122452C (en) | 1991-10-31 | 1992-10-28 | Rotary apparatus |
| EP92922377A EP0610503B1 (en) | 1991-10-31 | 1992-10-28 | Rotary apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| PCT/JP1991/001491 WO1993009591A1 (en) | 1991-10-31 | 1991-10-31 | Rotation amplifying device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| WO1993009591A1 true WO1993009591A1 (en) | 1993-05-13 |
Family
ID=14014696
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/JP1991/001491 Ceased WO1993009591A1 (en) | 1991-10-31 | 1991-10-31 | Rotation amplifying device |
Country Status (1)
| Country | Link |
|---|---|
| WO (1) | WO1993009591A1 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102082482A (en) * | 2009-12-01 | 2011-06-01 | 天津荣亨集团股份有限公司 | Flywheel accumulator body structure |
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| JPS5076456A (en) * | 1973-08-17 | 1975-06-23 | ||
| JPS5239061A (en) * | 1975-09-18 | 1977-03-26 | Siemens Ag | Transmission coupling device |
| JPS5320061A (en) * | 1976-08-05 | 1978-02-23 | Kawasaki Heavy Ind Ltd | Structure of electromagnetic gear reducer |
| JPS55133670A (en) * | 1979-04-03 | 1980-10-17 | Shibaura Eng Works Co Ltd | Variable-speed motor |
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- 1991-10-31 WO PCT/JP1991/001491 patent/WO1993009591A1/en not_active Ceased
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5076456A (en) * | 1973-08-17 | 1975-06-23 | ||
| JPS5239061A (en) * | 1975-09-18 | 1977-03-26 | Siemens Ag | Transmission coupling device |
| JPS5320061A (en) * | 1976-08-05 | 1978-02-23 | Kawasaki Heavy Ind Ltd | Structure of electromagnetic gear reducer |
| JPS55133670A (en) * | 1979-04-03 | 1980-10-17 | Shibaura Eng Works Co Ltd | Variable-speed motor |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102082482A (en) * | 2009-12-01 | 2011-06-01 | 天津荣亨集团股份有限公司 | Flywheel accumulator body structure |
| CN102082482B (en) * | 2009-12-01 | 2013-12-25 | 天津荣亨集团股份有限公司 | Flywheel accumulator body structure |
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