JPS5884221A - Five-axle control type magnetic bearing - Google Patents
Five-axle control type magnetic bearingInfo
- Publication number
- JPS5884221A JPS5884221A JP56182088A JP18208881A JPS5884221A JP S5884221 A JPS5884221 A JP S5884221A JP 56182088 A JP56182088 A JP 56182088A JP 18208881 A JP18208881 A JP 18208881A JP S5884221 A JPS5884221 A JP S5884221A
- Authority
- JP
- Japan
- Prior art keywords
- rotor
- stator
- magnetic
- air gap
- magnetic path
- 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
- 230000004907 flux Effects 0.000 claims abstract description 29
- 238000006073 displacement reaction Methods 0.000 abstract description 5
- 230000007935 neutral effect Effects 0.000 abstract description 5
- 239000011800 void material Substances 0.000 abstract 5
- 238000010276 construction Methods 0.000 abstract 2
- 239000000696 magnetic material Substances 0.000 description 2
- 229910000831 Steel Inorganic materials 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000005012 migration Effects 0.000 description 1
- 238000013508 migration Methods 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 230000003313 weakening effect Effects 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
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
- F16C32/044—Active magnetic bearings
- F16C32/0459—Details of the magnetic circuit
- F16C32/0461—Details of the magnetic circuit of stationary parts of the magnetic circuit
- F16C32/0465—Details of the magnetic circuit of stationary parts of the magnetic circuit with permanent magnets provided in the magnetic circuit of the electromagnets
-
- 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
- F16C32/044—Active magnetic bearings
- F16C32/0474—Active magnetic bearings for rotary movement
- F16C32/0489—Active magnetic bearings for rotary movement with active support of five degrees of freedom, e.g. two radial magnetic bearings combined with an axial bearing
-
- 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
- F16C2300/00—Application independent of particular apparatuses
- F16C2300/40—Application independent of particular apparatuses related to environment, i.e. operating conditions
- F16C2300/62—Application independent of particular apparatuses related to environment, i.e. operating conditions low pressure, e.g. elements operating under vacuum conditions
-
- 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
- F16C2370/00—Apparatus relating to physics, e.g. instruments
Landscapes
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Magnetic Bearings And Hydrostatic Bearings (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は、永久磁石の吸引力と電磁コイルの制御吸引力
との相互作用により、ステータ部に対しロータ部を非接
触で支持すると共に、特に全方向に対しロータ部の微少
表姿勢制御を可能とする1軸制御型磁気軸受に関する本
のである。Detailed Description of the Invention The present invention supports the rotor part in a non-contact manner with respect to the stator part through the interaction of the attractive force of the permanent magnets and the controlled attractive force of the electromagnetic coil, and in particular supports the rotor part in all directions. This book is about a single-axis control type magnetic bearing that enables minute surface posture control.
磁気軸受とは回転している物体を支持する力として、磁
気力を利用する軸受けである。この磁気軸受は、摩擦・
疲労による寿命の制限がないこと、摩擦トルクが極めて
小さいこと、真空・高温・低温等の特殊な環境に対する
適合性が優れている等の著しい特色があるために近年盛
んに研究され或いは水平二方向の姿勢制御する所謂−軸
又は二軸制御であり、残りの自由度は受動安定なので振
動や振れ廻りが生じ易く軸受の剛性が小さい。又、所謂
玉軸制御型の回転軸方向、それと直交する2軸方向、及
びその2軸まわりの傾き2方向の五方向を制御する磁気
軸受も知られてはいるが、永久磁石を使用しない電磁石
制御なので電力損失が大きい欠点がある。更には従来の
磁気軸受は各制御軸ごとに永久磁石を使う場合が多く4
.その構造が極めて複雑となる欠点がある。A magnetic bearing is a bearing that uses magnetic force to support a rotating object. This magnetic bearing is designed for friction and
It has been actively researched in recent years due to its remarkable features such as no life limit due to fatigue, extremely low friction torque, and excellent suitability for special environments such as vacuum, high temperature, and low temperature. This is so-called -axis or two-axis control to control the posture of the bearing, and the remaining degrees of freedom are passively stable, so vibration and wobbling are likely to occur, and the rigidity of the bearing is low. In addition, so-called ball-axis control type magnetic bearings that control five directions: the direction of the rotational axis, two axes perpendicular to it, and two directions of inclination around the two axes are also known, but electromagnets that do not use permanent magnets Since it is controlled, it has the disadvantage of large power loss. Furthermore, conventional magnetic bearings often use a permanent magnet for each control axis4.
.. The disadvantage is that the structure is extremely complicated.
ここに於いて本発明の目的は、上述の欠点を解消すると
共に、2個の永久磁石を使用して所謂五軸制御を行ない
、制御し易い磁界変調型の玉軸制御型磁気軸受を提供す
ることにあり、その内容は非接触で相対的に回転し得る
ロータ部とステータ部とから成り、ロータ部又はステー
タ部又は両者に軸方向に着磁した2個の円筒形と等価の
第1、第2の永久磁石を設け、ロータ部とステータ部の
ヨーク間K、前記第1及び第2の永久磁石の磁束が分岐
して軸方向に相互に逆方向に通過する第1及び第2の空
隙磁路を形成し、ステータ部に設けた第1の電磁コイル
により発生する磁束が、前記第1、第2の空隙磁路を直
列に通過するようにし、ロータ部とステータ部の軸方向
両端部((は、ステータヨークをロータヨークがそれぞ
れ円周状に囲み、これらの間に前記第1の永久磁石、第
2の永久磁石の磁束がそれぞれ半径方向に通過する第3
、第4の空隙磁路を形成し、ステータ部の軸方向両端部
のステータヨークは放射状に少なくとも3個にほぼ分割
し、それぞれ少なくとも2組ずつの電磁コイ□ルを巻回
し、これらの電磁コイルにより発する磁束がそれぞれ第
3、第4の空隙磁路を通過させるようにすると共に、軸
方向、ロータ部軸方向両端部のそれぞれの軸方向と直交
する対称2方向の計5方向の位置を検出するためにロー
タ部周囲に少なくとも5個の位置検出器を配置し、各位
置検出器の出力を基に対応する電磁コイルに供給する電
流を制御するようにしたことを特徴とするものである。SUMMARY OF THE INVENTION An object of the present invention is to eliminate the above-mentioned drawbacks, and to provide a magnetic field modulation type ball axis control magnetic bearing that performs so-called five-axis control using two permanent magnets and is easy to control. In particular, it consists of a rotor part and a stator part that can rotate relative to each other without contact, and the rotor part, the stator part, or both are magnetized in the axial direction. A second permanent magnet is provided between the yokes K of the rotor section and the stator section, and first and second gaps through which the magnetic fluxes of the first and second permanent magnets are branched and pass through in mutually opposite directions in the axial direction. A magnetic path is formed so that the magnetic flux generated by the first electromagnetic coil provided in the stator section passes through the first and second air gap magnetic paths in series, and both axial ends of the rotor section and the stator section (The stator yoke is circumferentially surrounded by rotor yokes, and the magnetic fluxes of the first and second permanent magnets pass in the radial direction between them.
, a fourth air gap magnetic path is formed, and the stator yokes at both axial ends of the stator section are roughly divided radially into at least three parts, each of which is wound with at least two sets of electromagnetic coils. The magnetic flux generated by the rotor is caused to pass through the third and fourth air gap magnetic paths, respectively, and the position is detected in a total of five directions: the axial direction and two symmetrical directions perpendicular to the axial direction at both ends of the rotor part in the axial direction. In order to achieve this, at least five position detectors are arranged around the rotor section, and the current supplied to the corresponding electromagnetic coil is controlled based on the output of each position detector.
本発明を図示の実施例に基づいて詳細に説明する。陶、
説明の便宜上、軸方向両端部、この2軸に直交する2方
向をY軸、Y軸として説明する。The present invention will be explained in detail based on illustrated embodiments. Pottery,
For convenience of explanation, both ends in the axial direction and two directions orthogonal to these two axes will be described as the Y-axis and the Y-axis.
第1図は本発明に係る磁気軸受の縦断面図であり、第2
図は第1図のπ−■線に沿った断面図である。この磁気
軸受はロータ部1とステータ部2とから成り、ロータ部
1dステータ部2の周囲をステータ部2の回転軸3を中
心に回転するようになっている。ロータ部1の上下対称
の中心部には、磁性体から成る円環状の第1のロータヨ
ーク4が設けられ、その周囲は上下に端部5.6を有す
る短円筒状となっている。この第1のロータヨーク4の
周縁部の上下には、軸方向に着磁された円筒状の第1、
第2の永久磁石1.8が接続されており、各々の上端部
及び下端部には円環状の磁性体から成る第2、第3のロ
ータヨーク9.1oが配置されている。第1、第2の永
久磁石7.8の極性は、第1のロータヨーク4に接する
端部同士を例えば南極Sの同極性とし、第2、第3のロ
ータヨーク9.10に接する端部同士を北極Nとしてい
る。一方、ステータ部2には回転軸3を中心に第1のス
テータヨーク15が設けられ、その中央部には前述の第
1のロータヨーク4の端部5.6との間に第1、第2の
空隙磁路16.17を形成する端部18,19を有する
開口部が設けられている。又、この第1のステータヨー
ク15、第1、第2の空隙磁路16,17.第1のロー
タヨーク4から成る磁気回路に磁束を通過させるための
第1の電磁フィル20が第1のステータヨーク16に巻
回されている。この第1のステータヨーク16の上下端
には、ステータヨーク15と磁気的に接続する第2、第
3のステータヨーク21.22が設けられており、これ
らのステータヨーク21.22は、前述の第2、第・3
の1−タヨーク9.10の内周部との間に円環状の第3
、第4の空隙磁路23.24が形成されている。第2、
第3のステータヨーク21,22には 第2図に示すよ
うにその中心部に向う4個の切込み25 、 26.2
7゜28が等間隔に設けられており、ステータヨーク2
1 、 22は4個に分割されている一℃ただし、第3
のステータヨークの切込み、分割部にっやては図示を省
略)。又、これらの分割部29.30 。FIG. 1 is a longitudinal sectional view of the magnetic bearing according to the present invention, and FIG.
The figure is a sectional view taken along the line π-■ in FIG. 1. This magnetic bearing consists of a rotor part 1 and a stator part 2, and is adapted to rotate around a rotor part 1d and a stator part 2 around a rotation axis 3 of the stator part 2. An annular first rotor yoke 4 made of a magnetic material is provided at the vertically symmetrical center of the rotor portion 1, and the circumference thereof has a short cylindrical shape having upper and lower end portions 5.6. Above and below the peripheral edge of the first rotor yoke 4, there are first cylindrical magnets magnetized in the axial direction.
A second permanent magnet 1.8 is connected, and second and third rotor yokes 9.1o made of an annular magnetic material are arranged at the upper and lower ends of each rotor yoke. The polarity of the first and second permanent magnets 7.8 is such that the ends in contact with the first rotor yoke 4 have the same polarity as the south pole S, and the ends in contact with the second and third rotor yokes 9.10 have the same polarity. It is called North Pole N. On the other hand, the stator portion 2 is provided with a first stator yoke 15 centered around the rotating shaft 3, and a first stator yoke 15, a first stator yoke 15, a first stator yoke 15, a second stator yoke 15, etc. An opening is provided with ends 18, 19 forming an air gap magnetic path 16,17. Moreover, this first stator yoke 15, first and second air gap magnetic paths 16, 17 . A first electromagnetic filter 20 is wound around the first stator yoke 16 to allow magnetic flux to pass through the magnetic circuit made up of the first rotor yoke 4 . Second and third stator yokes 21.22 are provided at the upper and lower ends of the first stator yoke 16, and are magnetically connected to the stator yoke 15. 2nd, 3rd
An annular third yoke 9 and the inner periphery of the yoke 9 and
, a fourth air gap magnetic path 23,24 is formed. Second,
As shown in FIG. 2, the third stator yokes 21 and 22 have four notches 25 and 26.2 toward the center thereof.
7°28 are provided at equal intervals, and the stator yoke 2
1 and 22 are divided into four parts. However, the third
(The stator yoke notches and split parts are not shown). Also, these divisions 29.30.
31.32にはそれぞれ4個の電磁コイル33.34.
35% 36が巻回されている。これらの電磁コイルは
対向する電磁コイル同士即ち33.35及び34,36
が直列的又は並列的に接続され、第2のステータヨーク
21 に於いては、電磁コイルによる2種類の電磁回路
が存在することになり、上下都合せて4種類の電流をこ
れらの電磁コイルに独立的に流すことができるようにな
っている。31.32 each have four electromagnetic coils 33.34.
35% 36 are wound. These electromagnetic coils are opposite electromagnetic coils, namely 33.35 and 34,36.
are connected in series or in parallel, and in the second stator yoke 21, there are two types of electromagnetic circuits using electromagnetic coils, and a total of four types of current are applied to these electromagnetic coils. It is now possible to flow independently.
同、実施例に於いては、第2.第3のロータヨーク9.
10、及び第2、第3のステータヨーク21.22は、
例えば電磁鋼板等・から成る積層板を使用して高速回転
時の渦電流の損失を少なくするようになっている。又、
この磁気軸受には5個の位置検出器、即ちロータ部1の
軸方向の位置を検出するための第1の位置検出器41、
ロータ部1の上部のX軸、Y軸それぞれの方向の位置を
検出するための第2、第3の位置検出器42.43、ロ
ータ部2の下部のX軸、Y軸それぞれの位置を検出する
第4.第6の位置検出器44 、 45 (但し45
は図示せず)がロータ部1の周囲に配置されている。こ
れらの位置検出器・(5個)はそれぞれ図示しない制御
回路に接続され、この制御回路からの制御信号が各電磁
コイル′に流れるようになっている。即ち、第1の電磁
コイル2oには第1の位置検出器41の出力に基づく電
力が供給され第2のステータヨーク2102種類のコイ
ルには第2、第3の位置検出器42.43がそれぞれ対
応してお9、第3のステータヨーク22の電磁コイルに
は第4、第5の位置検出器44.45がそれぞれ対応し
て制御電流を供給するように構成されている。又、46
、・46は緊急用のベアリングであり、ロータ部1のケ
ーシング47又は48が停止時又は緊急時に接触し得る
ようになっている。In the same example, Section 2. Third rotor yoke9.
10, and the second and third stator yokes 21 and 22,
For example, eddy current loss during high-speed rotation is reduced by using a laminated plate made of electromagnetic steel plates or the like. or,
This magnetic bearing has five position detectors, namely a first position detector 41 for detecting the axial position of the rotor section 1;
Second and third position detectors 42 and 43 for detecting the position of the upper part of the rotor part 1 in the X-axis and Y-axis directions, respectively, and the position of the lower part of the rotor part 2 in the X-axis and Y-axis directions, respectively. 4th thing to do. Sixth position detectors 44, 45 (however, 45
(not shown) are arranged around the rotor portion 1. These position detectors (5 pieces) are each connected to a control circuit (not shown), and a control signal from this control circuit flows to each electromagnetic coil'. That is, the first electromagnetic coil 2o is supplied with power based on the output of the first position detector 41, and the second stator yoke 2102 types of coils are supplied with second and third position detectors 42 and 43, respectively. Correspondingly, fourth and fifth position detectors 44 and 45 are configured to supply control currents to the electromagnetic coils of the third stator yoke 22, respectively. Also, 46
, 46 are emergency bearings with which the casing 47 or 48 of the rotor section 1 can come into contact when stopped or in an emergency.
本発明の実施例は上述の構成を有するので、第1の永久
磁石7により発生する磁束φ、は北極Nから発し、第2
のロータヨーク9、第3の空隙磁路23、第2のステー
タヨーク21 を経由し、第1のステータヨーク15の
開口部の端部18及び19から第1の空隙磁路16及び
第2の空隙磁路17を通過して第1のロータヨーク4に
達し第1の永久磁石7の南極Sに戻る。−又、第2の永
久磁石8を基に発生する磁束φ2は前述の磁束φ、の通
路と上下対称に流れることになり、電磁コイル20の内
側を流れる磁束は相殺して流れない。尚、永久磁石7.
8の極性を逆にすれば磁束φ1、φ2は逆の順序で流れ
ることは勿論である。今ここで、第1の電磁コイル20
に電流が供給されていない場合を考えてみると、第1、
wpI2の空隙磁路16.17には磁束φいφ2により
それぞれ軸方向に互いに吸引する吸引力が作用すること
になる。そして第1及び第2の空隙磁路16,17に作
用する吸引力は。Since the embodiment of the present invention has the above-described configuration, the magnetic flux φ generated by the first permanent magnet 7 is emitted from the north pole N, and the magnetic flux φ, generated by the first permanent magnet 7
The first air gap magnetic path 16 and the second air gap are connected from the opening ends 18 and 19 of the first stator yoke 15 via the rotor yoke 9, the third air gap magnetic path 23, and the second stator yoke 21. It passes through the magnetic path 17, reaches the first rotor yoke 4, and returns to the south pole S of the first permanent magnet 7. -Furthermore, the magnetic flux φ2 generated based on the second permanent magnet 8 flows vertically symmetrically with the path of the aforementioned magnetic flux φ, and the magnetic flux flowing inside the electromagnetic coil 20 cancels out and does not flow. In addition, permanent magnet 7.
Of course, if the polarity of 8 is reversed, the magnetic fluxes φ1 and φ2 will flow in the reverse order. Now here, the first electromagnetic coil 20
Considering the case where no current is supplied to the first,
Magnetic fluxes φ and φ2 act on the air gap magnetic paths 16 and 17 of wpI2 to attract each other in the axial direction. And the attractive force acting on the first and second air gap magnetic paths 16 and 17 is as follows.
はぼ相殺されロータ部1とステータ部20間に中立位置
が存在することになる。然しなから実際にはロータ部1
の自重等によりそのままではこの中立位置が保持される
仁とは極めて困難であり、例えばロータ部1は下方に移
動し、第1の空隙磁路16が開き、第2の空隙磁路17
が狭くなる。すると第1の空隙磁路16では磁気抵抗が
大となり、磁束φ、もφ2も減少し、逆に第2の空隙磁
路17では磁束φ1もφ、も増大して、ロータ部1が下
方に移行する傾向は更に大となる。そこで軸方向位置を
検出する第1の位置検出器41によりロータ部1の軸方
向変位を検出して軸方向制御回路に出力するこきによ抄
、第1の電磁コイル2oに電流が供給され、前述の場合
で言えば、第1の空隙磁路16から第2の空隙磁路17
方向に向う点線で示す磁束へを発生させる。かくするこ
とにより、第1の空隙磁路16の吸引力を強め、第2の
空隙磁路17の吸引力を弱めることになるので第1の空
隙磁路・16の間隔を狭くシ、第2の空隙磁路17の間
隔を開くようにロータ部1が軸方向に移動することにな
る。このようにしてロータ部1の軸方向位置を第1の位
置検出器41 で検出しながら、軸方向制御回路により
第1の電磁コイル20に供給する電流を調整することに
なり、ロータ部1は軸方向の所定位置でステータ部2に
対して非接触状態で安定することになる。The positions are approximately canceled out, and a neutral position exists between the rotor section 1 and the stator section 20. However, in reality, the rotor part 1
It is extremely difficult to maintain this neutral position as it is due to its own weight, etc. For example, the rotor section 1 moves downward, the first air gap magnetic path 16 opens, and the second air gap magnetic path 17 opens.
becomes narrower. Then, in the first air-gap magnetic path 16, the magnetic resistance increases, and the magnetic fluxes φ and φ2 decrease, and conversely, in the second air-gap magnetic path 17, the magnetic fluxes φ1 and φ increase, causing the rotor section 1 to move downward. The trend towards migration will become even greater. Therefore, a current is supplied to the first electromagnetic coil 2o, which detects the axial displacement of the rotor part 1 by the first position detector 41 that detects the axial position and outputs it to the axial control circuit. In the above case, from the first air gap magnetic path 16 to the second air gap magnetic path 17
A magnetic flux is generated in the direction shown by the dotted line. By doing this, the attractive force of the first air gap magnetic path 16 is strengthened and the attractive force of the second air gap magnetic path 17 is weakened, so the interval between the first air gap magnetic path 16 is narrowed and the second air gap magnetic path 16 is narrowed. The rotor section 1 moves in the axial direction so as to widen the gap between the air gap magnetic paths 17. In this way, while the axial position of the rotor section 1 is detected by the first position detector 41, the current supplied to the first electromagnetic coil 20 is adjusted by the axial direction control circuit. It becomes stable in a non-contact state with respect to the stator portion 2 at a predetermined position in the axial direction.
又、ロータ部1及びステータ部2の第3の空隙磁路23
では、前述の第1の永久磁石7による磁束φ、が外側の
第2のロータヨーク9から内側の第2のステータヨーク
21に流れ込んでいる。今、第2図に於いてロータ部1
がX軸の左側方向に変位したとすると、第3の空隙磁路
23のうち右側が狭くな沙、左側が広くなるととKなり
、狭くなった空隙磁路部分に磁束φ、が集中し吸引力が
強ま9、益々狭くなるようにロータ部1の変位を助長す
ることになる。そこで第2の位置検出器42により変位
を検出し、X軸方向に位置する電磁コイル34及び34
に電流を供給し、点線で示すように、第2のステータヨ
ーク21を左側から右側に通過して第2のロータヨーク
9に流れ、ロータヨーク9を廻り込んで再び左側に戻っ
てくるような磁束φ4を発生させることによ抄、狭くな
った部分の吸引力を弱め、広がった部分の吸引力を強く
することKよりロータ部1を元の中立位置に戻すことが
可能となる。又、第1のロータヨークがY軸方向に変位
した場合も同様であり、更には第3のロータヨーク10
がX軸又はY軸方向に変位した場合でも、同様に第4又
は第5の位置検出器44.45を用いて行なうことがで
きる。Moreover, the third air gap magnetic path 23 of the rotor part 1 and the stator part 2
In this case, the magnetic flux φ caused by the first permanent magnet 7 described above flows from the outer second rotor yoke 9 to the inner second stator yoke 21. Now, in Fig. 2, rotor section 1
If is displaced to the left side of the X-axis, the right side of the third air gap magnetic path 23 becomes narrower, and the left side becomes wider, and the magnetic flux φ is concentrated in the narrowed air gap magnetic path and is attracted. The force increases 9 and promotes the displacement of the rotor portion 1 so that it becomes increasingly narrow. Therefore, the displacement is detected by the second position detector 42, and the electromagnetic coils 34 and 34 located in the X-axis direction are
As shown by the dotted line, the magnetic flux φ4 passes through the second stator yoke 21 from the left side to the right side, flows to the second rotor yoke 9, goes around the rotor yoke 9, and returns to the left side again. By generating K, the rotor section 1 can be returned to its original neutral position by weakening the suction force in the narrowed part and increasing the suction force in the widened part. The same applies when the first rotor yoke is displaced in the Y-axis direction, and furthermore, the third rotor yoke 10
Even when is displaced in the X-axis or Y-axis direction, the fourth or fifth position detector 44, 45 can be used in the same manner.
これらの制御は単にロータ部1を中立位置に戻すだけで
はなく、意識的に一方に片寄らせることもできる。従っ
てロータ部1の上下の位置制御をそれぞれ独立的に行な
い、第2又は第3のロータヨーク9.10 を片寄らせ
ることによってロータ部1をステータ部2に対して傾斜
させることが可能となる。従って本発明に係る磁気軸受
では、軸方向、水平2方向、傾斜2方向の1軸制御が実
現でき、これらの制御は人工衛星等の姿勢制御に極めて
有利である。These controls not only simply return the rotor section 1 to the neutral position, but also allow the rotor section 1 to be intentionally biased to one side. Therefore, the rotor section 1 can be tilted relative to the stator section 2 by controlling the upper and lower positions of the rotor section 1 independently, and by shifting the second or third rotor yoke 9.10. Therefore, the magnetic bearing according to the present invention can realize uniaxial control in the axial direction, two horizontal directions, and two directions of inclination, and these controls are extremely advantageous for attitude control of artificial satellites and the like.
実施例に於いては磁束φ1、うを発生する永久磁石をロ
ータ部IK介在させたが、必ずしもどれら紘ロータ部1
ではなくステータ部2に配置しても支障はなく、更には
ロータ部1とステータ部2の双方に設けることも可能で
ある。又、第2、第8のステータヨーク21.22は半
径方向に4個に分割したが、これらは3個以上に分割す
れば制御が可能であり、電磁コイルはこの分割部の全て
に巻回するのではなく2個以上K・巻回すれば理論的に
制御ができる。In the embodiment, a permanent magnet that generates magnetic flux φ1 is interposed in the rotor portion IK, but it is not necessarily the case that the permanent magnet that generates the magnetic flux φ1 is located in the rotor portion IK.
There is no problem even if it is arranged in the stator section 2 instead of the rotor section 1, and it is also possible to provide it in both the rotor section 1 and the stator section 2. Furthermore, although the second and eighth stator yokes 21 and 22 are divided into four parts in the radial direction, they can be controlled by dividing them into three or more parts, and the electromagnetic coil is wound around all of these divided parts. Theoretically, control can be achieved by winding two or more K.
以上説明したように本発明に係る磁気軸受は、5個の位
置検出器を用いて1軸制御を可能としたものであり、次
に挙げるような長所を有する。As explained above, the magnetic bearing according to the present invention enables single-axis control using five position detectors, and has the following advantages.
(1)、玉軸制御型なので振動、振れ廻りが小さく、制
御をしない受動安定軸を有するものよりも軸受剛性が大
きい。(1) Since it is a ball shaft control type, vibration and runout are small, and the bearing rigidity is greater than a bearing with a passive stable shaft that does not have control.
Q)、磁界変調型なので制御が容易であり電力消費量が
小さい。Q) Since it is a magnetic field modulation type, control is easy and power consumption is low.
O)・、使用する永久磁石は軸方向着磁型なので永久磁
石の製作が容易となる。O). Since the permanent magnet used is an axially magnetized type, it is easy to manufacture the permanent magnet.
(4)、2個の永久磁石を1軸制御に共通に用いている
ので、永久磁石の使用数が少なく構造が簡単となる。(4) Since two permanent magnets are commonly used for uniaxial control, the number of permanent magnets used is small and the structure is simple.
(5)、全ゆる方向の微少な首振り制御所謂ジン/(リ
ングが可能となる。(5) Slight swing control in all directions is possible.
図面は本発明に係る磁気軸受の一実施例を示すものであ
り、第1図はその縦断面図、第2図は第1図に於ける■
−■線に沿り九断藺図である。
符号1はロータ部、2はステータ部、4.9.10はロ
ータヨーク、7.8は永久磁石、16.17.23.2
4は空隙磁路、16.21.22はステータヨーク、2
0.33.34.35.36は電磁コイル、41 、
42.43.44は位置検出器である。
特許出願人 航空宇宙技術研究所長第1W!J
2
第2WJThe drawings show an embodiment of the magnetic bearing according to the present invention, and FIG. 1 is a longitudinal cross-sectional view thereof, and FIG.
This is a nine-section map along the -■ line. 1 is the rotor part, 2 is the stator part, 4.9.10 is the rotor yoke, 7.8 is the permanent magnet, 16.17.23.2
4 is the air gap magnetic path, 16.21.22 is the stator yoke, 2
0.33.34.35.36 is an electromagnetic coil, 41,
42, 43, and 44 are position detectors. Patent applicant: Aerospace Technology Research Institute Director 1st W! J 2 2nd WJ
Claims (1)
部とから成り、ロータ部又はステータ部又は両者に軸方
向に着磁した2個の円筒形と等価の第1、第2の永久磁
石を設け、ロータ部とステータ部のヨーク間に、前記第
1及び第2の永久磁石の磁束が分岐して軸方向に相互に
逆方向に通過する第1及び第2の空隙磁路を形成し、ス
テータ部に設ゆた第1の電磁コイルにより発生する磁束
が前記第1、第2の空隙磁路を直列に通過するようにし
、ロータ部とステータ部の軸方向両端部には、ステータ
ヨークをロータヨークがそれぞれ円周状に囲み、これら
の間に前記第1の永久磁石、第2の永久磁石の磁束がそ
れぞれ半径方向に通過する第3、第4の空隙磁路を形成
し、ステータ部の軸方同両端部のステータヨークは放射
状に少なくとも8個にほぼ分割し、それぞれ少なくとも
2組ずつの゛電磁コイルを巻回し、これらの電磁コイル
により発生する磁束がそれぞれ第3、第49空隙磁路を
通過させるようにすると共に、軸方向、ロータ部軸方向
両端部のそれぞれの軸方向と直交する対称2方向の計6
方向の位置を検出するた゛めにロータ部周囲に少なくと
も5個の位置検出器を配置し、各位置検出器の出力を基
に対応する電磁コイルに供給する電流を制御するようK
したことを特徴とする1軸制御型磁気軸受。1. Consisting of a rotor part and a stator part that can rotate relative to each other in a non-contact manner, two permanent magnets equivalent to two cylindrical shapes are magnetized in the axial direction of the rotor part, the stator part, or both. and forming first and second air gap magnetic paths between the yokes of the rotor part and the stator part, in which the magnetic fluxes of the first and second permanent magnets branch and pass in mutually opposite directions in the axial direction. , the magnetic flux generated by the first electromagnetic coil installed in the stator section passes through the first and second air gap magnetic paths in series, and a stator yoke is provided at both axial ends of the rotor section and the stator section. are circumferentially surrounded by a rotor yoke, forming third and fourth air gap magnetic paths through which the magnetic fluxes of the first and second permanent magnets pass in the radial direction, respectively, and the stator portion The stator yoke at both ends of the same axial direction is roughly divided radially into at least eight parts, each of which is wound with at least two sets of electromagnetic coils, and the magnetic flux generated by these electromagnetic coils is distributed to the third and forty-ninth air gap magnets, respectively. A total of six directions are provided in two symmetrical directions perpendicular to the axial direction and at both axial ends of the rotor part.
At least five position detectors are arranged around the rotor to detect the position in the direction, and the current supplied to the corresponding electromagnetic coil is controlled based on the output of each position detector.
A single-axis control type magnetic bearing characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56182088A JPS5854285B2 (en) | 1981-11-13 | 1981-11-13 | Five-axis controlled magnetic bearing |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56182088A JPS5854285B2 (en) | 1981-11-13 | 1981-11-13 | Five-axis controlled magnetic bearing |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5884221A true JPS5884221A (en) | 1983-05-20 |
| JPS5854285B2 JPS5854285B2 (en) | 1983-12-03 |
Family
ID=16112147
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56182088A Expired JPS5854285B2 (en) | 1981-11-13 | 1981-11-13 | Five-axis controlled magnetic bearing |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5854285B2 (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2923877A1 (en) * | 2007-11-16 | 2009-05-22 | Thales Sa | MAGNETIC BEARING CENTER WITH DOUBLE FLOORS |
| CN104989727A (en) * | 2015-06-05 | 2015-10-21 | 中国人民解放军国防科学技术大学 | Combined-type five-degree-of-freedom electromagnetic bearing |
| CN105020270A (en) * | 2015-06-05 | 2015-11-04 | 中国人民解放军国防科学技术大学 | Combined five-freedom-degree electromagnetic bearing |
-
1981
- 1981-11-13 JP JP56182088A patent/JPS5854285B2/en not_active Expired
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2923877A1 (en) * | 2007-11-16 | 2009-05-22 | Thales Sa | MAGNETIC BEARING CENTER WITH DOUBLE FLOORS |
| US7911100B2 (en) | 2007-11-16 | 2011-03-22 | Thales | Dual-stage centering magnetic bearing |
| CN104989727A (en) * | 2015-06-05 | 2015-10-21 | 中国人民解放军国防科学技术大学 | Combined-type five-degree-of-freedom electromagnetic bearing |
| CN105020270A (en) * | 2015-06-05 | 2015-11-04 | 中国人民解放军国防科学技术大学 | Combined five-freedom-degree electromagnetic bearing |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5854285B2 (en) | 1983-12-03 |
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