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JPS6327577B2 - - Google Patents
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JPS6327577B2 - - Google Patents

Info

Publication number
JPS6327577B2
JPS6327577B2 JP54135492A JP13549279A JPS6327577B2 JP S6327577 B2 JPS6327577 B2 JP S6327577B2 JP 54135492 A JP54135492 A JP 54135492A JP 13549279 A JP13549279 A JP 13549279A JP S6327577 B2 JPS6327577 B2 JP S6327577B2
Authority
JP
Japan
Prior art keywords
magnet
magnetic bearing
rotating body
fixed
bearing
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.)
Expired
Application number
JP54135492A
Other languages
Japanese (ja)
Other versions
JPS5659027A (en
Inventor
Masaharu Miki
Tadao Ishizawa
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Seiko Instruments Inc
Original Assignee
Seiko Instruments Inc
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Seiko Instruments Inc filed Critical Seiko Instruments Inc
Priority to JP13549279A priority Critical patent/JPS5659027A/en
Publication of JPS5659027A publication Critical patent/JPS5659027A/en
Publication of JPS6327577B2 publication Critical patent/JPS6327577B2/ja
Granted legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16CSHAFTS; FLEXIBLE SHAFTS; ELEMENTS OR CRANKSHAFT MECHANISMS; ROTARY BODIES OTHER THAN GEARING ELEMENTS; BEARINGS
    • F16C32/00Bearings not otherwise provided for
    • F16C32/04Bearings not otherwise provided for using magnetic or electric supporting means
    • F16C32/0406Magnetic bearings
    • F16C32/044Active magnetic bearings
    • F16C32/0474Active magnetic bearings for rotary movement
    • F16C32/0476Active magnetic bearings for rotary movement with active support of one degree of freedom, e.g. axial magnetic bearings
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16CSHAFTS; FLEXIBLE SHAFTS; ELEMENTS OR CRANKSHAFT MECHANISMS; ROTARY BODIES OTHER THAN GEARING ELEMENTS; BEARINGS
    • F16C32/00Bearings not otherwise provided for
    • F16C32/04Bearings not otherwise provided for using magnetic or electric supporting means
    • F16C32/0406Magnetic bearings
    • F16C32/0408Passive magnetic bearings
    • F16C32/0423Passive magnetic bearings with permanent magnets on both parts repelling each other
    • F16C32/0425Passive magnetic bearings with permanent magnets on both parts repelling each other for radial load mainly
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16CSHAFTS; FLEXIBLE SHAFTS; ELEMENTS OR CRANKSHAFT MECHANISMS; ROTARY BODIES OTHER THAN GEARING ELEMENTS; BEARINGS
    • F16C32/00Bearings not otherwise provided for
    • F16C32/04Bearings not otherwise provided for using magnetic or electric supporting means
    • F16C32/0406Magnetic bearings
    • F16C32/044Active magnetic bearings
    • F16C32/0459Details of the magnetic circuit
    • F16C32/0461Details of the magnetic circuit of stationary parts of the magnetic circuit
    • F16C32/0465Details of the magnetic circuit of stationary parts of the magnetic circuit with permanent magnets provided in the magnetic circuit of the electromagnets

Landscapes

  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Magnetic Bearings And Hydrostatic Bearings (AREA)

Description

【発明の詳細な説明】 本発明はラジアル方向の減衰機能を有した磁気
軸受に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic bearing having a radial damping function.

スラスト方向は制御型磁気軸受で支持され、ラ
ジアル方向は反発型磁気軸受(無制御)で支持さ
れている回転装置は、そのままではスラスト方向
は制御型であるので減衰効果を持たせる事は可能
であるが、ラジアル方向は、まつたく減衰機能を
有しない。
A rotating device that is supported in the thrust direction by a controlled magnetic bearing and in the radial direction by a repulsion magnetic bearing (uncontrolled) can have a damping effect because the thrust direction is controlled as it is. However, it does not have a damping function in the radial direction.

そのため、共振作用や外乱の影響でラジアル方
向に振動が生じた場合、振動の振幅が非常に大き
くなり、回転体の破損の原因になつている。
Therefore, when vibration occurs in the radial direction due to resonance or disturbance, the amplitude of the vibration becomes extremely large, causing damage to the rotating body.

第1図は従来の磁気軸受である。 FIG. 1 shows a conventional magnetic bearing.

11が反発型ラジアル磁気軸受(無制御)、2
1がスラスト方向制御型磁気軸受、31が回転軸
である。
11 is a repulsion type radial magnetic bearing (uncontrolled), 2
1 is a thrust direction control type magnetic bearing, and 31 is a rotating shaft.

従来ラジアル方向の減衰効果を持たせるために
イのような導体を付し、うず電流式減衰機構を設
けていたが、このうず電流式減衰機構は、その減
衰力が磁束の変化量に比例するため、磁気軸受の
ような、特に低い共振点を持つ場合、その効果は
不満足なものである。
Conventionally, in order to have a damping effect in the radial direction, a conductor like A was attached and an eddy current damping mechanism was installed, but with this eddy current damping mechanism, the damping force is proportional to the amount of change in magnetic flux. Therefore, the effect is unsatisfactory especially when the bearing has a low resonance point, such as a magnetic bearing.

本発明は、上記した従来の欠点を改善しようと
するもので、その目的の一つは、低周波数におい
ても有効な減衰効果を持ち、また機構的にも比較
的簡単で、小型の磁気軸受を得る事である。
The present invention aims to improve the above-mentioned conventional drawbacks, and one of its objectives is to have an effective damping effect even at low frequencies, to have a relatively simple mechanism, and to use a compact magnetic bearing. It's about getting.

以下本発明の一実施例を第2図に従つて説明す
る。スラスト軸受部は従来通りで、1が永久磁
石、2が制御コイル、3が回転子側のヨーク、4
が固定子側のヨークである。3,4は磁性体であ
る。5は反発型ラジアル磁気軸受(無制御)の回
転軸8に固定された永久磁石である。固定子側の
3つの永久磁石6の中で中央の磁石6′を回転軸
8に対して直角ラジアル方向に可動可能にして置
く。残りの2つの永久磁石6″は固定金具7に固
定される。この固定金具7は非磁性体である。そ
れぞれの永久磁石6′,6″の配列は第2図のよう
に互いに反発するようにし、また回転軸8側の磁
石5と固定子側の磁石6も当然互いに反発する配
置とする。可動磁石6′の半径は、固定磁石6″の
半径よりも大にして置く。それは、磁石6′が安
定に存在し得るためである。磁石6′と6″との半
径の差は、振動論の教える所により、回転軸全体
の共鳴振動数と磁石6′の共鳴振動数が一致する
ように決める。8は回転軸で非磁性体である。固
定金具7と固定磁石6″の間の部分には、油等の
粘性物9を封入して減衰力を調節する。しかしこ
の粘性物9は無くとも空気が粘性体として働いて
磁石6′が支持されるので同等の効果が得られる。
An embodiment of the present invention will be described below with reference to FIG. The thrust bearing part is the same as before, 1 is a permanent magnet, 2 is a control coil, 3 is a yoke on the rotor side, 4
is the yoke on the stator side. 3 and 4 are magnetic materials. 5 is a permanent magnet fixed to the rotating shaft 8 of a repulsion type radial magnetic bearing (uncontrolled). Among the three permanent magnets 6 on the stator side, the central magnet 6' is movable in a radial direction perpendicular to the rotating shaft 8. The remaining two permanent magnets 6'' are fixed to a fixture 7. This fixture 7 is a non-magnetic material.The arrangement of the respective permanent magnets 6' and 6'' is such that they repel each other as shown in Figure 2. Furthermore, the magnet 5 on the rotating shaft 8 side and the magnet 6 on the stator side are also arranged to naturally repel each other. The radius of the movable magnet 6' is set larger than the radius of the fixed magnet 6''. This is so that the magnet 6' can exist stably. The difference in radius between the magnets 6' and 6'' is According to theory, the resonant frequency of the entire rotating shaft is determined to match the resonant frequency of the magnet 6'. 8 is a rotating shaft made of a non-magnetic material. A viscous substance 9 such as oil is sealed between the fixing fitting 7 and the fixed magnet 6'' to adjust the damping force. However, even without this viscous substance 9, air acts as a viscous substance and the magnet 6' Since it is supported, the same effect can be obtained.

本発明によれば、回転体の共振振動数と一致し
た固有振動数をもつ可動磁石が、粘性体を介在さ
せて固定磁石間に反発支持されているので、可動
磁石が回転体の共振点でスムーズに動き、回転体
の回転軸の振動エネルギーが可動磁石6′の振動
エネルギーに移り、固定金具7と可動磁石6′間
の摩擦、およびその間の粘性体9の粘性にエネル
ギーが消費され、ダンピング減衰力が生じ、特に
回転体の共振振動に対し減衰し、振動を小さく抑
えることができる効果が得られ、従来のうず電流
式減衰機構による欠点である減衰力が弱い事(特
に低周波数において)を改善できる。また機構も
簡単なので小型の軸受にする事も可能である。
According to the present invention, the movable magnet, which has a natural frequency that matches the resonance frequency of the rotating body, is repulsively supported between the fixed magnets with the viscous body interposed, so that the movable magnet is at the resonance point of the rotating body. It moves smoothly, and the vibration energy of the rotating shaft of the rotating body is transferred to the vibration energy of the movable magnet 6', and the energy is consumed by the friction between the fixed bracket 7 and the movable magnet 6' and the viscosity of the viscous body 9 between them, resulting in damping. A damping force is generated, which dampens the resonance vibration of the rotating body in particular, and has the effect of suppressing the vibration to a small level.The damping force, which is a drawback of conventional eddy current damping mechanisms, is weak (especially at low frequencies). can be improved. Also, since the mechanism is simple, it is possible to use a small bearing.

尚、公知技術ではあるが、固定金具にダンピン
グ向上用のシキリ等を設ければ効果は更に向上す
ることはいうまでもない。
Although it is a known technique, it goes without saying that the effect can be further improved by providing a damping improver on the fixing fitting.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は従来の磁気軸受の縦断面図、第2図は
本発明からなる減衰機構をラジアル軸受け有する
磁気軸受の縦断面図である。 1……永久磁石、2……コイル、3……ヨー
ク、4……ヨーク、5……永久磁石、6,6′,
6″……永久磁石、7……固定金具、8……回転
軸、9……粘弾性体。
FIG. 1 is a longitudinal sectional view of a conventional magnetic bearing, and FIG. 2 is a longitudinal sectional view of a magnetic bearing having a radial bearing and a damping mechanism according to the present invention. 1... Permanent magnet, 2... Coil, 3... Yoke, 4... Yoke, 5... Permanent magnet, 6, 6',
6″...Permanent magnet, 7...Fixing metal fitting, 8...Rotating shaft, 9...Viscoelastic body.

Claims (1)

【特許請求の範囲】 1 スラスト方向に制御型磁気軸受を有し、ラジ
アル方向に無制御反発型磁気軸受を持つ回転体軸
受において、 ラジアル軸受の静止側磁石が 固定部材により静止側に固定された固定磁石
と、 回転体の共振振動数と一致する固有振動数をも
つ可動磁石を有し、かつ この可動磁石と固定部材との間に粘性体を介在
させるとともに、可動磁石を固定磁石で回転体の
回転軸方向に反発挟持し回転体の回転軸直角方向
に移動可能に構成され、 ラジアル方向の減衰効果を高める構成としたこ
とを特徴とする磁気軸受。
[Claims] 1. In a rotating body bearing having a controlled magnetic bearing in the thrust direction and an uncontrolled repulsion magnetic bearing in the radial direction, the stationary side magnet of the radial bearing is fixed to the stationary side by a fixing member. It has a fixed magnet and a movable magnet having a natural frequency that matches the resonance frequency of the rotating body, and a viscous body is interposed between the movable magnet and the fixed member, and the movable magnet is connected to the rotating body using the fixed magnet. What is claimed is: 1. A magnetic bearing characterized in that it is configured to be movable in a direction perpendicular to the rotation axis of a rotating body, and to enhance a damping effect in the radial direction.
JP13549279A 1979-10-19 1979-10-19 Magnetic bearing Granted JPS5659027A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13549279A JPS5659027A (en) 1979-10-19 1979-10-19 Magnetic bearing

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13549279A JPS5659027A (en) 1979-10-19 1979-10-19 Magnetic bearing

Publications (2)

Publication Number Publication Date
JPS5659027A JPS5659027A (en) 1981-05-22
JPS6327577B2 true JPS6327577B2 (en) 1988-06-03

Family

ID=15152992

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13549279A Granted JPS5659027A (en) 1979-10-19 1979-10-19 Magnetic bearing

Country Status (1)

Country Link
JP (1) JPS5659027A (en)

Families Citing this family (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6231720A (en) * 1985-07-31 1987-02-10 Copal Electron Co Ltd Damper device of magnetic bearing
JPS62177314A (en) * 1986-01-30 1987-08-04 Shimadzu Corp Magnetic floating type rotary machine
JPS63190928A (en) * 1987-02-03 1988-08-08 Koyo Seiko Co Ltd Dynamic pressure bearing
US5514924A (en) * 1992-04-30 1996-05-07 AVCON--Advanced Control Technology, Inc. Magnetic bearing providing radial and axial load support for a shaft
US5521448A (en) * 1994-08-01 1996-05-28 Mechanical Technology Incorporated Damping for passive magnetic bearings
FR2732734B1 (en) * 1995-04-07 1997-06-27 Aerospatiale MINIATURE MAGNETIC BEARING HAS AT LEAST ONE ACTIVE AXIS
JP4504734B2 (en) * 2004-05-11 2010-07-14 日特エンジニアリング株式会社 Center pressing device and method for winding machine
EP3081997A1 (en) * 2015-04-16 2016-10-19 Montres Breguet S.A. Magnetic shock-absorber for timepiece arbour
CN104832538B (en) * 2015-05-25 2017-03-22 哈尔滨工业大学 Magnetic circuit decoupled permanent magnet biased active and passive hybrid axial and radial magnetic suspension bearing

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54121143U (en) * 1978-02-13 1979-08-24

Also Published As

Publication number Publication date
JPS5659027A (en) 1981-05-22

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