JPH05180227A - Superconductive bearing device - Google Patents
Superconductive bearing deviceInfo
- Publication number
- JPH05180227A JPH05180227A JP34609991A JP34609991A JPH05180227A JP H05180227 A JPH05180227 A JP H05180227A JP 34609991 A JP34609991 A JP 34609991A JP 34609991 A JP34609991 A JP 34609991A JP H05180227 A JPH05180227 A JP H05180227A
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnets
- rotating body
- bearing device
- superconductor
- permanent magnet
- 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.)
- Granted
Links
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F16—ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
- F16C—SHAFTS; FLEXIBLE SHAFTS; ELEMENTS OR CRANKSHAFT MECHANISMS; ROTARY BODIES OTHER THAN GEARING ELEMENTS; BEARINGS
- F16C32/00—Bearings not otherwise provided for
- F16C32/04—Bearings not otherwise provided for using magnetic or electric supporting means
- F16C32/0406—Magnetic bearings
- F16C32/0408—Passive magnetic bearings
- F16C32/0436—Passive magnetic bearings with a conductor on one part movable with respect to a magnetic field, e.g. a body of copper on one part and a permanent magnet on the other part
- F16C32/0438—Passive magnetic bearings with a conductor on one part movable with respect to a magnetic field, e.g. a body of copper on one part and a permanent magnet on the other part with a superconducting body, e.g. a body made of high temperature superconducting material such as YBaCuO
Landscapes
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Magnetic Bearings And Hydrostatic Bearings (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は、たとえば高速回転を
必要とする流体機械や工作機械、余剰電力をフライホイ
ールの運動エネルギに変換して貯蔵する電力貯蔵装置、
またはジャイロスコープなどに適用される超電導軸受装
置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to, for example, a fluid machine or a machine tool which requires high speed rotation, an electric power storage device for converting surplus electric power into kinetic energy of a flywheel and storing it.
Also, the present invention relates to a superconducting bearing device applied to a gyroscope or the like.
【0002】[0002]
【従来の技術と発明の課題】近年、回転体の高速回転と
高剛性を可能にした軸受装置として、非接触状態で回転
体を支持しうる超電導軸受装置が開発されている。2. Description of the Related Art In recent years, a superconducting bearing device capable of supporting a rotating body in a non-contact state has been developed as a bearing device capable of high-speed rotation and high rigidity of the rotating body.
【0003】この種超電導軸受装置としては、たとえば
回転体に同心状に設けられ、かつ回転軸心方向両端部が
互いに逆の極性の磁気を帯びた1つの環状永久磁石と、
この永久磁石の端面に対して回転体の回転軸心方向に間
隔をおいて対向するように配置された環状超電導体とを
備えているものが考えられる。An example of this type of superconducting bearing device is one annular permanent magnet that is concentrically provided on a rotating body and that has both ends in the direction of the axis of rotation bearing magnets of opposite polarities.
It is conceivable that the permanent magnet is provided with an annular superconductor arranged so as to oppose the end surface of the permanent magnet in the direction of the rotation axis of the rotating body.
【0004】ところが、上記のような超電導軸受装置で
は、負荷容量および剛性が不足するという問題がある。
しかも、剛性が不足するため回転体の軸ぶれが生じ、回
転体を非接触状態で安定的に支持することができないと
いう問題がある。However, the superconducting bearing device as described above has a problem that the load capacity and the rigidity are insufficient.
In addition, there is a problem in that the rigidity of the rotating body causes axial deviation of the rotating body, which makes it impossible to stably support the rotating body in a non-contact state.
【0005】この発明の目的は、上記の問題を解決した
超電導軸受装置を提供することにある。An object of the present invention is to provide a superconducting bearing device which solves the above problems.
【0006】[0006]
【課題を解決するための手段】この発明による超電導軸
受装置は、回転体を固定部に対して非接触状態で支持す
る超電導軸受装置であって、回転体と同心状になり、か
つ互いに対向するように設けられた2つの環状永久磁石
と、回転体と同心状になり、かつ両環状永久磁石間に位
置するように設けられた超電導体とを備えており、両永
久磁石の対向する面が、互いに同一の極性の磁気を帯び
ているとともに、両永久磁石どうしの間隔が、互いに反
発し合うような距離となされているものである。A superconducting bearing device according to the present invention is a superconducting bearing device which supports a rotating body in a non-contact state with a fixed portion, and is concentric with the rotating body and faces each other. Two annular permanent magnets provided in such a manner, and a superconductor provided concentrically with the rotating body and located between both annular permanent magnets. The magnets have the same polarity as each other, and the distance between the permanent magnets is such that they repel each other.
【0007】[0007]
【作用】回転体と同心状になり、かつ互いに対向するよ
うに設けられた2つの環状永久磁石と、回転体と同心状
になり、かつ両環状永久磁石間に位置するように設けら
れた超電導体とを備えていると、両永久磁石と超電導体
とが所定の間隔をあけて対向した状態に保持され、回転
体が非接触状態で支持される。Operation: Two annular permanent magnets which are concentric with the rotating body and are provided so as to face each other, and a superconducting device which is provided concentrically with the rotating body and is located between the two annular permanent magnets. If the body is provided, both permanent magnets and the superconductor are held in a state of facing each other with a predetermined gap, and the rotating body is supported in a non-contact state.
【0008】また、両永久磁石の対向する面が、互いに
同一の極性の磁気を帯びているとともに、両永久磁石ど
うしの間隔が、互いに反発し合うような距離となされて
いると、両永久磁石により形成される磁束が、圧縮され
る。このため、超電導体を貫通する磁束が多くなり、超
電導体が多くの磁束をトラップすることになる。If the opposing surfaces of the two permanent magnets are magnetized with the same polarity, and the distance between the two permanent magnets is such that they repel each other, the two permanent magnets will become repulsive. The magnetic flux formed by is compressed. Therefore, a large amount of magnetic flux penetrates the superconductor, and the superconductor traps a large amount of magnetic flux.
【0009】[0009]
【実施例】以下、この発明の実施例を、図面を参照して
説明する。Embodiments of the present invention will be described below with reference to the drawings.
【0010】図1は、超電導軸受装置の主要部を概略的
に示す。FIG. 1 schematically shows a main part of a superconducting bearing device.
【0011】超電導軸受装置は、垂直な軸状の回転体
(1) を備えている。回転体(1) には、上下2つの水平円
板状の永久磁石部(2a)(2b)が、その回転軸心方向に間隔
をおいて回転体(1) と同心状に設けられ、両永久磁石部
(2a)(2b)の対向面に対して回転体(1) の回転軸心方向に
間隔をおいて対向するように、両永久磁石部(2a)(2b)
間、および両永久磁石部(2a)(2b)の回転軸心方向の外側
に、それぞれ環状超電導体部(3a)(3b)(3c)が配置されて
いる。The superconducting bearing device is a vertical shaft-shaped rotating body.
It has (1). The rotating body (1) is provided with two upper and lower horizontal disk-shaped permanent magnet parts (2a) (2b) concentrically with the rotating body (1) at intervals in the direction of the rotation axis. Permanent magnet part
Both permanent magnet parts (2a) and (2b) so that they face the facing surfaces of (2a) and (2b) with a gap in the direction of the rotation axis of the rotating body (1).
The ring-shaped superconductor portions (3a) (3b) (3c) are respectively arranged between the permanent magnet portions (2a) (2b) and between the permanent magnet portions (2a) (2b).
【0012】永久磁石部(2a)(2b)は、回転体(1) に固定
状に設けられ、かつ回転軸心方向に間隔をおいて対向す
る、たとえば銅からなる上下2つの水平円板(4a)(4b)を
備えている。上側の円板(4a)の上面、および下側の円板
(4b)の下面に、それぞれ回転体(1) と同心の同一円周状
に位置する環状凹みぞ(5a)(5b)が形成されており、これ
らの凹みぞ(5a)(5b)内にそれぞれ環状永久磁石(6a)(6b)
が嵌められて固定されている。各永久磁石(6a)(6b)は上
下両端部が互いに逆の極性の磁気を帯び、かつ両永久磁
石(6a)(6b)の対向する面が、互いに同一の極性の磁気を
帯びている。たとえば、上側の永久磁石(6a)の上端部は
N極、下端部はS極の磁気を帯びており、下側の永久磁
石(6b)の上端部はS極、下端部はN極の磁気を帯びてい
る。また、両永久磁石(6a)(6b)どうしの間隔は、互いに
反発し合うような距離となされている。そして、回転軸
心の周囲の磁束分布が回転によって変化しないようにな
っている。The permanent magnet portions (2a), (2b) are fixedly provided on the rotating body (1), and are opposed to each other at intervals in the direction of the axis of rotation, and are composed of, for example, two upper and lower horizontal discs made of copper ( It has 4a) and 4b). The upper surface of the upper disc (4a) and the lower disc
On the lower surface of (4b), annular grooves (5a) (5b) concentric with the rotating body (1) are formed respectively, and these are formed in these grooves (5a) (5b). Ring permanent magnets (6a) (6b)
Is fitted and fixed. The upper and lower ends of each of the permanent magnets (6a) (6b) are magnetized with opposite polarities, and the opposing surfaces of both permanent magnets (6a) (6b) are magnetized with the same polarity. For example, the upper end of the upper permanent magnet (6a) has an N-pole magnetism and the lower end has an S-pole magnetism. The upper end of the lower permanent magnet (6b) has an S-pole magnetism and the lower end has an N-pole magnetism. Bears. The distance between the permanent magnets (6a) and (6b) is such that they repel each other. The magnetic flux distribution around the rotation axis does not change due to rotation.
【0013】超電導体部(3a)(3b)(3c)は、それぞれハウ
ジング(7) に固定状に設けられた、たとえば銅からなる
穴あき水平円板(8a)(8b)(8c)と、穴あき円板(8a)(8b)(8
c)の穴(9a)(9b)(9c)の周囲における回転体(1) と同心状
の環状部分に、両永久磁石(6a)(6b)と対向して埋設され
ている複数の超電導体(10)とよりなる。全ての超電導体
(10)の体積は等しくなっている。The superconductor portions (3a) (3b) (3c) are fixedly provided in the housing (7), respectively, and have perforated horizontal discs (8a) (8b) (8c) made of copper, for example. Perforated disk (8a) (8b) (8
c) A plurality of superconductors embedded in the annular part concentric with the rotating body (1) around the holes (9a) (9b) (9c) facing both permanent magnets (6a) (6b). It consists of (10). All superconductors
The volumes of (10) are equal.
【0014】超電導体(10)は、たとえばイットリウム系
高温超電導体であるYBa2Cu3Oxからなる基板の
内部に常電導粒子(Y2Ba1Cu1)を均一に混在さ
せたものからなり、永久磁石(7a)(7b)から発せられる磁
束侵入を拘束する性質を持つものである。そして、超電
導体(10)は、永久磁石(7a)(7b)の磁束が所定量侵入する
離間位置であってかつ上記回転体の回転によって侵入磁
束の分布が変化しない位置に配置されている。The superconductor (10) is made of, for example, a yttrium-based high-temperature superconductor, YBa 2 Cu 3 O x, in which normal conductive particles (Y 2 Ba 1 Cu 1 ) are uniformly mixed in a substrate. , Has the property of restraining the penetration of magnetic flux emitted from the permanent magnets (7a) and (7b). The superconductor (10) is arranged at a separated position where the magnetic flux of the permanent magnets (7a) (7b) penetrates by a predetermined amount, and at a position where the distribution of the magnetic flux penetrating does not change due to the rotation of the rotating body.
【0015】超電導軸受装置の水平円板(8a)(8b)(8c)に
冷却ケース(図示略)が設けられ、冷却ケースに冷却装
置(11)が接続されている。A cooling case (not shown) is provided on the horizontal disks (8a) (8b) (8c) of the superconducting bearing device, and the cooling device (11) is connected to the cooling case.
【0016】超電導軸受装置を作動させる場合、超電導
体(10)は冷却装置(11)により円板(8a)(8b)(8c)の冷却ケ
ース内に循環させられる適当な冷媒によって冷却され、
超電導状態に保持される。このため、回転体(1) の永久
磁石(6a)(6b)から発せられる磁束の多くが超電導体(10)
の内部に侵入して拘束されることになる(ピンニング現
象)。ここで、超電導体(10)はその内部に常電導体粒子
が均一に混在されているため、超電導体(10)内部への侵
入磁束の分布が一定となり、そのため、あたかも超電導
体(10)に立設した仮想ピンに回転体(1) の永久磁石(6a)
(6b)が貫かれたようになり、超電導体(10)に対して永久
磁石部(2a)(2b)とともに回転体(1) が拘束される。その
ため、回転体(1) は、きわめて安定的に浮上した状態
で、アキシアル方向およびラジアル方向に支持されるこ
とになる。When operating the superconducting bearing device, the superconductor (10) is cooled by a cooling medium (11) with a suitable refrigerant circulated in the cooling cases of the disks (8a) (8b) (8c),
It is kept superconducting. For this reason, most of the magnetic flux generated from the permanent magnets (6a) (6b) of the rotating body (1) is the superconductor (10).
Will be invaded and restrained (pinning phenomenon). Here, since the superconductor (10) has the normal conductor particles uniformly mixed therein, the distribution of the magnetic flux penetrating into the superconductor (10) is constant, and therefore, as if the superconductor (10) Permanent magnet (6a) of the rotating body (1) on the erected virtual pin
The (6b) appears to be penetrated, and the rotating body (1) is constrained to the superconductor (10) together with the permanent magnet parts (2a) and (2b). Therefore, the rotating body (1) is supported in the axial direction and the radial direction while floating very stably.
【0017】永久磁石部(2a)(2b)の永久磁石(6a)(6b)
は、互いに反発し合うので、両永久磁石(6a)(6b)により
形成される磁束は、回転軸心方向に圧縮される。このた
め、超電導体(10)を貫通する磁束が多くなり、超電導体
(10)が多くの磁束をトラップすることにより、負荷容量
および剛性が向上する。Permanent magnets (2a), (2b) permanent magnets (6a) (6b)
Repel each other, so that the magnetic flux formed by both permanent magnets (6a) and (6b) is compressed in the direction of the rotation axis. As a result, more magnetic flux penetrates the superconductor (10),
Since (10) traps a large amount of magnetic flux, load capacity and rigidity are improved.
【0018】上記実施例においては、回転体に永久磁石
が設けられ、固定部であるハウジングに超電導体が設け
られているが、これとは逆に、回転体に超電導体が設け
られ、固定部であるハウジングに永久磁石が設けられて
いてもよい。また、上記実施例においては、両永久磁石
部間だけではなく、両永久磁石部の回転軸心方向の外側
に、それぞれ環状超電導体部が配置されているが、回転
軸心方向の外側の永久磁石部は必ずしも必要としない。In the above-described embodiment, the rotating body is provided with the permanent magnet and the housing, which is the fixed portion, is provided with the superconductor. On the contrary, the rotating body is provided with the superconductor and the fixed portion is provided. The housing may be provided with a permanent magnet. Further, in the above embodiment, the annular superconductor portions are arranged not only between the permanent magnet portions but also on the outer sides of the permanent magnet portions in the rotational axis direction, respectively. The magnet part is not always necessary.
【0019】[0019]
【発明の効果】この発明の超電導軸受装置によれば、上
述のように、回転体を安定的に非接触状態で回転支持す
ることができる。また、超電導体を貫通する磁束が多く
なり、超電導体が多くの磁束をトラップすることになる
ので、負荷容量および剛性が向上する。According to the superconducting bearing device of the present invention, as described above, the rotating body can be stably rotatably supported in a non-contact state. Further, since the magnetic flux penetrating the superconductor increases and the superconductor traps a large amount of magnetic flux, load capacity and rigidity are improved.
【図1】この発明の実施例を示す超電導軸受装置主要部
の概略縦断面図である。FIG. 1 is a schematic vertical sectional view of a main part of a superconducting bearing device showing an embodiment of the present invention.
1 回転体 6a、6b 永久磁石 10 超電導体 1 Rotating body 6a, 6b Permanent magnet 10 Superconductor
Claims (1)
持する超電導軸受装置であって、 回転体と同心状になり、かつ互いに対向するように設け
られた2つの環状永久磁石と、回転体と同心状になり、
かつ両環状永久磁石間に位置するように設けられた超電
導体とを備えており、両永久磁石の対向する面が、互い
に同一の極性の磁気を帯びているとともに、両永久磁石
どうしの間隔が、互いに反発し合うような距離となされ
ている超電導軸受装置。1. A superconducting bearing device for supporting a rotating body in a non-contact state with a fixed portion, comprising: two annular permanent magnets concentric with the rotating body and provided so as to face each other; It becomes concentric with the rotating body,
And a superconductor provided so as to be located between both annular permanent magnets, the facing surfaces of both permanent magnets are magnetized with the same polarity, and the distance between the two permanent magnets is , A superconducting bearing device having a distance such that they repel each other.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP34609991A JP3232463B2 (en) | 1991-12-27 | 1991-12-27 | Superconducting bearing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP34609991A JP3232463B2 (en) | 1991-12-27 | 1991-12-27 | Superconducting bearing device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH05180227A true JPH05180227A (en) | 1993-07-20 |
JP3232463B2 JP3232463B2 (en) | 2001-11-26 |
Family
ID=18381129
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP34609991A Expired - Fee Related JP3232463B2 (en) | 1991-12-27 | 1991-12-27 | Superconducting bearing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3232463B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1767798A1 (en) * | 2005-09-23 | 2007-03-28 | Nexans | Superconducting magnetic bearing |
-
1991
- 1991-12-27 JP JP34609991A patent/JP3232463B2/en not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1767798A1 (en) * | 2005-09-23 | 2007-03-28 | Nexans | Superconducting magnetic bearing |
Also Published As
Publication number | Publication date |
---|---|
JP3232463B2 (en) | 2001-11-26 |
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