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JPS62270823A - Magnetic bearing - Google Patents

Magnetic bearing

Info

Publication number
JPS62270823A
JPS62270823A JP61112387A JP11238786A JPS62270823A JP S62270823 A JPS62270823 A JP S62270823A JP 61112387 A JP61112387 A JP 61112387A JP 11238786 A JP11238786 A JP 11238786A JP S62270823 A JPS62270823 A JP S62270823A
Authority
JP
Japan
Prior art keywords
rotor
yokes
stator
magnetic
gap magnetic
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
Application number
JP61112387A
Other languages
Japanese (ja)
Other versions
JPH0242126B2 (en
Inventor
Tsutomu Murakami
力 村上
Atsushi Nakajima
厚 中島
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.)
National Aerospace Laboratory of Japan
Original Assignee
National Aerospace Laboratory of Japan
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 National Aerospace Laboratory of Japan filed Critical National Aerospace Laboratory of Japan
Priority to JP61112387A priority Critical patent/JPS62270823A/en
Publication of JPS62270823A publication Critical patent/JPS62270823A/en
Publication of JPH0242126B2 publication Critical patent/JPH0242126B2/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
    • F16C32/0459Details 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)
  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Mechanical Engineering (AREA)
  • Magnetic Bearings And Hydrostatic Bearings (AREA)

Abstract

PURPOSE:To eliminate a non-modulation gap and facilitate design and control with simple construction using less number of electromagnetic coils by furnishing a rotor and a stator each having two yokes forming two sets of gap magnetic paths facing each other. CONSTITUTION:Flux PHI1 is passed from N to S pole of a permanent magnet 9 of a rotor 1. That is, from a gap magnetic path G1 via solenoid yokes 6, 7 of the stator, the flux PHI1 shall flow into a gap magnetic path G1. Then the flux PHI1 shall flow into the yoke 5 from the yoke 7 through a gap magnetic path G2 for returning to the S pole, and thereby magnetic attraction force is applied to said gap magnetic paths G1, G2 between the yokes 4, 6 and 7, 5. Displacement of the rotor 1 is sensed by a location sensor 13 for X axis, and current is allowed to flow in solenoids 12a, 12c to allow a flux PHI2 to flow in such a direction as to set off change of the attraction force of the flux PHI1 caused by the permanent magnet 9. Thereby the whole attraction force is balance, and the rotor 1 is restored to the neutral position as original.

Description

【発明の詳細な説明】 3、発明の詳細な説明 [産業上の利用分野コ 本発明は、永久磁石の吸引力と電磁コイルの電磁吸引力
との相互作用により、ステータ部に対しロータ部を非接
触で支持する簡素な構造の磁気軸受に関するものである
Detailed Description of the Invention 3. Detailed Description of the Invention [Industrial Field of Application] The present invention provides a mechanism for attracting a rotor to a stator by an interaction between the attractive force of a permanent magnet and the electromagnetic attractive force of an electromagnetic coil. This invention relates to a magnetic bearing with a simple structure that supports contactless support.

[従来の技術] 磁気軸受とは回転している物体を支持!る力として、磁
気力を利用する軸受である。この磁気軸受は摩擦か疲労
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、真空拳高温会低温等の特殊な環境に対する適合
性が優れていること等の著しい特色があるために、近年
盛んに研究がなされている。そして、この用途としては
例えば遠心分離器、分子ポンプ、ジャイロスコープ、精
密測定器、人工衛星用制御機器等への使用が有望視され
ている。
[Prior technology] Magnetic bearings support rotating objects! This is a bearing that uses magnetic force to generate force. These magnetic bearings have been developed in recent years due to their remarkable features such as no life limit due to friction or fatigue, extremely low frictional torque, and excellent suitability for special environments such as high temperatures and low temperatures. There is a lot of research going on. As for this application, for example, use in centrifugal separators, molecular pumps, gyroscopes, precision measuring instruments, control equipment for artificial satellites, etc. is considered to be promising.

しかしながら、従来の磁気軸受は1個当り8個の電磁コ
イルを用いたものが多く、その構造が複雑であると共に
、永久磁石の磁束だけが通過する所謂非変調ギャップを
有しているために、設計及び制御が困難となり、電源の
負担が大きくがる。
However, most conventional magnetic bearings use eight electromagnetic coils each, and their structure is complex, as well as having a so-called non-modulation gap through which only the magnetic flux of the permanent magnet passes. This makes design and control difficult and increases the burden on the power supply.

[発明の目的] 本発明の目的は、電磁コイルの数を少なくした比較的簡
易な構成で、かつ非変調ギャップが存在せず、設計及び
制御が容易な磁気軸受を提供することにある。
[Object of the Invention] An object of the present invention is to provide a magnetic bearing that has a relatively simple configuration with a reduced number of electromagnetic coils, has no non-modulation gap, and is easy to design and control.

[発明の概要] 上述の目的を達成するための本発明の要旨は、互いに対
向する2組の空隙磁路を形成する2枚ずつのヨークをそ
れぞれ有するロータ部とステータ部とから成り、前記ロ
ータ部は前記ヨーク間に永久磁石を挟着し、前記ステー
タ部は前記ヨーク間に3個以上の鉄心を配置し、これら
の鉄心にそれぞれコイルを巻回した電磁コイルを有する
ことを特徴とする磁気軸受である。
[Summary of the Invention] The gist of the present invention for achieving the above-mentioned object is to provide a rotor section comprising a rotor section and a stator section each having two yokes forming two sets of air gap magnetic paths facing each other, The stator part has a permanent magnet sandwiched between the yokes, and the stator part has three or more iron cores arranged between the yokes, and has an electromagnetic coil with a coil wound around each of these iron cores. It is a bearing.

[発明の実施例] 本発明を図示の実施例に基づいて詳細に説明する。[Embodiments of the invention] The present invention will be explained in detail based on illustrated embodiments.

第1図は磁気軸受の断面図、第2図は第1図の■−■線
に沿った断面図であり、回転中心部にロータ部1が設け
られ、その周囲にステータ部2が配置されたインナーロ
ータ方式となっている。
Fig. 1 is a cross-sectional view of the magnetic bearing, and Fig. 2 is a cross-sectional view taken along the line ■-■ in Fig. 1, in which a rotor part 1 is provided at the center of rotation, and a stator part 2 is arranged around it. It is an inner rotor type.

そして、ロータ部lは軸3に取り付けられており、この
軸3の他端には同様のロータ部が設けられている。ロー
タ部1は円環状の第1.第2のヨーク4.5を有し、こ
れらのヨーク4.5に空隙磁路G1. G2を介して対
向して、ステータ部2には円環状の第1、第2の電磁ヨ
ーク6.7が設けられている。なお、ステータ部2の第
1、第2のiW電磁ヨーク、7は放射状に4個に分割さ
れ、それらの間には非磁性体8が介在されている。ロー
タ部1の第1、第2のヨーク4.5間には円環状の永久
磁石9が配置されている。ステータ部2の第1.第2の
電磁ヨーク6.7間には、電磁ヨーク6.7の分割と対
応して4個の鉄心10a、10b、loc、10dが介
在されティる。そして、各鉄心10a、10b、foe
、lOdにはそれぞれコイルlla、llb、lie、
1lclが巻回され、独立に磁束を発生できる電磁コイ
ル12a、12b、12c、12dが構成されている。
The rotor portion 1 is attached to a shaft 3, and a similar rotor portion is provided at the other end of the shaft 3. The rotor portion 1 has an annular first rotor. It has second yokes 4.5, and these yokes 4.5 are provided with an air gap magnetic path G1. Annular first and second electromagnetic yokes 6.7 are provided on the stator portion 2, facing each other via G2. The first and second iW electromagnetic yokes 7 of the stator section 2 are radially divided into four parts, and a nonmagnetic material 8 is interposed between them. An annular permanent magnet 9 is arranged between the first and second yokes 4.5 of the rotor section 1. The first section of the stator section 2. Between the second electromagnetic yokes 6.7, four iron cores 10a, 10b, loc, and 10d are interposed corresponding to the divisions of the electromagnetic yokes 6.7. And each iron core 10a, 10b, foe
, lOd have coils lla, llb, lie, respectively.
1lcl is wound, and constitutes electromagnetic coils 12a, 12b, 12c, and 12d that can independently generate magnetic flux.

またロータ部lの側部には、X軸方向のロータ部1の変
位を検出するための位置センサ13、Y軸方向用の位置
センサ14が設けられている。
Furthermore, a position sensor 13 for detecting displacement of the rotor part 1 in the X-axis direction and a position sensor 14 for the Y-axis direction are provided on the side of the rotor part 1.

−°)ンサ14からは同様にして電磁コイル12b、’
  12dに電流が供与される。なお、ロータ部1の永
久磁石9は非磁性体から成る保護環15により周設され
、ステータ部2には非磁性体から成る連結部16が取り
付けられ、その他端部には同様のステータ部が設けられ
ている。
-°) From the sensor 14, the electromagnetic coils 12b,'
A current is applied to 12d. The permanent magnets 9 of the rotor part 1 are surrounded by a protective ring 15 made of a non-magnetic material, a connecting part 16 made of a non-magnetic material is attached to the stator part 2, and a similar stator part is attached to the other end. It is provided.

作動時においては、ロータ部lの永久磁石9のN極から
S極へ磁束φ工が通過、即ち空隙磁路G1からステータ
部2の電磁ヨーク6.7を通り、空隙磁路Glへ磁束φ
lが流れ込み、磁束φ1は電磁ヨーク7から空隙磁路C
2を通って電磁ヨーク5に流れS極に戻ることになり、
ヨーク4・6及び7ψ5間の空隙磁路G1、G2には磁
気吸引力が作用することになる。この磁気吸引力は理想
的な状態を考えてみれば全ての方向において相殺され、
ロータ部lは半径方向の成る方向に変位することなく、
不安定に平衡した状態にあり得るが、実際には製作上の
精度や重力の影響等からロータ部1が□平径方向に変位
することは避けられない0例え−円 ・−■ ト°ば、ロータ部1がX軸の正方向に微小量移動するi 壬、1と、ステータ部2とロータ部1との右側の空隙磁
:=ノ 路G1. G2が狭く、左側の空隙磁路C1,G2が大
きくなる。従って、右側の空隙磁路G1. G2の磁気
抵抗が小さくなるために、この部分における永久磁石9
からの磁束φ1は更に増加し、この間の吸引力は増加し
、左側の空隙磁路G1、G2を通る磁束φ1は減少する
ので、ロータ部1は益々右側に引き寄せられることにな
る。
During operation, a magnetic flux φ passes from the N pole to the S pole of the permanent magnet 9 of the rotor section l, that is, the magnetic flux φ passes from the air gap magnetic path G1 through the electromagnetic yoke 6.7 of the stator section 2 to the air gap magnetic path Gl.
l flows into the magnetic flux φ1 from the electromagnetic yoke 7 to the air gap magnetic path C.
2 to the electromagnetic yoke 5 and return to the S pole.
A magnetic attraction force acts on the air gap magnetic paths G1 and G2 between the yokes 4 and 6 and 7ψ5. Considering an ideal situation, this magnetic attraction force is canceled out in all directions,
The rotor portion l is not displaced in the radial direction,
Although it may be in an unstable equilibrium state, in reality, it is inevitable that the rotor section 1 will be displaced in the □ flat radial direction due to manufacturing precision and the influence of gravity. , the rotor section 1 moves a minute amount in the positive direction of the X-axis. G2 is narrow, and the air gap magnetic paths C1 and G2 on the left side are large. Therefore, the right air gap magnetic path G1. Since the magnetic resistance of G2 is small, the permanent magnet 9 in this part
The magnetic flux φ1 from the magnetic flux φ1 further increases, the attractive force increases during this time, and the magnetic flux φ1 passing through the left air gap magnetic paths G1 and G2 decreases, so that the rotor portion 1 is increasingly drawn to the right side.

この変位はX軸周の位置センサ13によって検出され、
電磁コイル12&、12cに制御回路からの制御信号に
基づく電流を流し、永久磁石9による磁束φ工の吸引力
の変化を打ち消すような方向、つまり右側の空隙磁路G
1、G2において永久磁石9の磁束φ1と逆方向に通過
し、左側の空隙磁路G1、G2では磁束φ1と同方向に
磁束φ2を流すことになる。この磁束φ2によって、永
久磁石9からの磁束φ1の変位による変化を相殺し、右
側の空隙磁路Gl、 G2においては吸引力を減少させ
This displacement is detected by the position sensor 13 around the X-axis,
A current is applied to the electromagnetic coils 12 & 12c based on the control signal from the control circuit, and the direction is such that the change in the attraction force of the magnetic flux φ due to the permanent magnet 9 is canceled out, that is, the air gap magnetic path G on the right side.
1 and G2, the magnetic flux φ2 passes in the opposite direction to the magnetic flux φ1 of the permanent magnet 9, and in the left air gap magnetic paths G1 and G2, the magnetic flux φ2 flows in the same direction as the magnetic flux φ1. This magnetic flux φ2 offsets the change in the magnetic flux φ1 from the permanent magnet 9 due to displacement, and reduces the attractive force in the right air gap magnetic paths Gl and G2.

〕 一4側の空隙磁路G1. G2では吸引力を増加するこ
と電 はY軸方向についても全く同様である。
] Air gap magnetic path G1 on the 14th side. In G2, the attraction force is increased in exactly the same way in the Y-axis direction.

この場合に、ステータ部2の第1、第2の電磁ヨーク6
.7を実施例のように電磁コイル12a〜12d毎に分
割しておくことにより、電磁コイル12a、12cから
の磁束φ2はX軸、Y軸上に存在する分割部のみを通過
することになり、その他の分割部には流入することが少
ないので、磁束を効率良く吸引のために使用することが
可能となる。なお、実施例のような分割部を設ける代り
に、電磁ヨーク6.7の一部に切込みを設けても同様に
相当の効果が得られる。この磁気軸受はヨークの数が少
ないためにスラスト方向の剛性が若干劣るので、無重力
状態における使用においては問題はないとしても、重力
の存在する場所においては軸方向を水平としてスラスト
方向に重力の影響がないように配置するか、又はスラス
ト方向の磁気軸受を併用することが好ましい。
In this case, the first and second electromagnetic yokes 6 of the stator section 2
.. By dividing 7 into the electromagnetic coils 12a to 12d as in the embodiment, the magnetic flux φ2 from the electromagnetic coils 12a and 12c passes only through the divided portions existing on the X-axis and the Y-axis. Since less of the magnetic flux flows into other divided parts, it is possible to efficiently use the magnetic flux for attraction. It should be noted that a considerable effect can be similarly obtained by providing a notch in a part of the electromagnetic yoke 6.7 instead of providing a divided portion as in the embodiment. Since this magnetic bearing has a small number of yokes, its rigidity in the thrust direction is slightly inferior, so although there is no problem when using it in zero gravity, in a place where gravity exists, the axial direction is horizontal and the thrust direction is affected by gravity. It is preferable to arrange the bearing so that there is no magnetic bearing, or to use a magnetic bearing in the thrust direction.

;部1の周囲に配置したインナーロータ型とした′i −が、ステータ部2の周囲にロータ部1を配するアウタ
ーロータ型とすることもできる。更に、実施例ではステ
ータ部2のヨークを4個に分割した例を示したが、少な
くとも3個に分割すれば制御が可能である。
'i-', which is an inner rotor type arranged around the part 1, can also be made into an outer rotor type where the rotor part 1 is arranged around the stator part 2. Further, in the embodiment, an example is shown in which the yoke of the stator section 2 is divided into four parts, but control is possible if the yoke is divided into at least three parts.

[発明の効果] 以上説明したように本発明に係る磁気軸受は、電磁コイ
ルの数を減少することによって装置の構成を簡素化し、
かつ非変調ギャップを無くすことにより使用電力の電源
の負担を小さくする利点を有している。
[Effects of the Invention] As explained above, the magnetic bearing according to the present invention simplifies the configuration of the device by reducing the number of electromagnetic coils, and
Moreover, by eliminating the non-modulation gap, it has the advantage of reducing the burden on the power supply of the power used.

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

図面は本発明に係る磁気軸受の一実施例を示し、第1図
はその断面図、第2図は第1図の■−■線に沿った断面
図である。 符号1はロータ部、2はステータ部、3は軸、4.5は
ヨーク、6.7は電磁ヨーク、9は永久磁石、10は鉄
心、11はコイル、12は電磁コ−へ 一ルル、13.14は位置センサである。 特許出願人  航空宇宙技術研究所長 第1図 第2図
The drawings show an embodiment of the magnetic bearing according to the present invention, and FIG. 1 is a cross-sectional view thereof, and FIG. 2 is a cross-sectional view taken along the line ■-■ in FIG. 1 is a rotor part, 2 is a stator part, 3 is a shaft, 4.5 is a yoke, 6.7 is an electromagnetic yoke, 9 is a permanent magnet, 10 is an iron core, 11 is a coil, 12 is an electromagnetic coil, 13 and 14 are position sensors. Patent applicant Director of Aerospace Technology Research Institute Figure 1 Figure 2

Claims (1)

【特許請求の範囲】 1、互いに対向する2組の空隙磁路を形成する2枚ずつ
のヨークをそれぞれ有するロータ部とステータ部とから
成り、前記ロータ部は前記ヨーク間に永久磁石を挟着し
、前記ステータ部は前記ヨーク間に3個以上の鉄心を配
置し、これらの鉄心にそれぞれコイルを巻回した電磁コ
イルを有することを特徴とする磁気軸受。 2、前記ステータ部のヨークは、前記コイルに対応して
3個以上に分割した特許請求の範囲第1項に記載の磁気
軸受。 3、前記ステータ部のヨークは、前記コイルに対応して
その境界部の磁気抵抗を大とした特許請求の範囲第1項
に記載の磁気軸受。
[Scope of Claims] 1. Consists of a rotor section and a stator section each having two yokes forming two sets of air gap magnetic paths facing each other, and the rotor section has a permanent magnet sandwiched between the yokes. The magnetic bearing is characterized in that the stator section has three or more iron cores arranged between the yokes and electromagnetic coils each having a coil wound around each of the iron cores. 2. The magnetic bearing according to claim 1, wherein the yoke of the stator portion is divided into three or more parts corresponding to the coils. 3. The magnetic bearing according to claim 1, wherein the yoke of the stator portion has a large magnetic resistance at a boundary portion corresponding to the coil.
JP61112387A 1986-05-16 1986-05-16 Magnetic bearing Granted JPS62270823A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61112387A JPS62270823A (en) 1986-05-16 1986-05-16 Magnetic bearing

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61112387A JPS62270823A (en) 1986-05-16 1986-05-16 Magnetic bearing

Publications (2)

Publication Number Publication Date
JPS62270823A true JPS62270823A (en) 1987-11-25
JPH0242126B2 JPH0242126B2 (en) 1990-09-20

Family

ID=14585401

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61112387A Granted JPS62270823A (en) 1986-05-16 1986-05-16 Magnetic bearing

Country Status (1)

Country Link
JP (1) JPS62270823A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04116341U (en) * 1991-03-27 1992-10-16 三菱自動車工業株式会社 Information input device for electronic information processing equipment

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4928854A (en) * 1972-07-14 1974-03-14
JPS5316807A (en) * 1976-07-30 1978-02-16 Nasa Energy accumulator

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4928854A (en) * 1972-07-14 1974-03-14
JPS5316807A (en) * 1976-07-30 1978-02-16 Nasa Energy accumulator

Also Published As

Publication number Publication date
JPH0242126B2 (en) 1990-09-20

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