JPH0222497Y2 - - Google Patents

Info

Publication number
JPH0222497Y2
JPH0222497Y2 JP12121485U JP12121485U JPH0222497Y2 JP H0222497 Y2 JPH0222497 Y2 JP H0222497Y2 JP 12121485 U JP12121485 U JP 12121485U JP 12121485 U JP12121485 U JP 12121485U JP H0222497 Y2 JPH0222497 Y2 JP H0222497Y2
Authority
JP
Japan
Prior art keywords
stator
magnetic bearing
groove
divided
thrust 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.)
Expired
Application number
JP12121485U
Other languages
Japanese (ja)
Other versions
JPS6228920U (en
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 filed Critical
Priority to JP12121485U priority Critical patent/JPH0222497Y2/ja
Publication of JPS6228920U publication Critical patent/JPS6228920U/ja
Application granted granted Critical
Publication of JPH0222497Y2 publication Critical patent/JPH0222497Y2/ja
Expired 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
    • 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
    • F16C32/044Active magnetic bearings
    • F16C32/0474Active magnetic bearings for rotary movement
    • F16C32/048Active magnetic bearings for rotary movement with active support of two degrees of freedom, e.g. radial magnetic bearings

Landscapes

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

Description

【考案の詳細な説明】 〔産業上の利用分野〕 この考案は、回転体を軸方向に沿つて、非接触
状態で浮上させる吸引制御形スラスト磁気軸受の
ステータ構造に関する。
[Detailed Description of the Invention] [Industrial Application Field] This invention relates to a stator structure for an attraction-controlled thrust magnetic bearing that levitates a rotating body along the axial direction in a non-contact manner.

〔従来の技術〕[Conventional technology]

高速で回転する回転体を支承する方法として、
磁気力を利用した磁気軸受がよく知られている。
このうち、吸引制御スラスト磁気軸受としては、
たとえば第6図に示すような構成のものが広く使
用されている。
As a method of supporting a rotating body rotating at high speed,
Magnetic bearings that utilize magnetic force are well known.
Among these, as suction control thrust magnetic bearings,
For example, a configuration as shown in FIG. 6 is widely used.

この吸引制御スラスト磁気軸受においては、シ
ヤフト1の右側軸端にスラスト磁気軸受2があ
り、他方左側にはラジアル磁気軸3およびモータ
(図示せず)が設けられている。スラスト磁気軸
受2は、シヤフト1に固着されたロータヨーク2
3とステータ21,22及び変位センサ24から
構成されている。ステータ21,22はそれぞれ
ステータヨーク211,221と励磁コイル21
2,222からなる円環状のものであり、それぞ
れの磁極面213,223はロータヨーク23と
空隙を介して平行に対面している。このように、
円環状に構成するのは、ロータヨーク23に生じ
る渦電流を小さくするためであり、これによつて
渦電流に起因するドラツグトルクを小さくすると
いう効果を有している。
In this suction control thrust magnetic bearing, a thrust magnetic bearing 2 is provided at the right end of the shaft 1, and a radial magnetic shaft 3 and a motor (not shown) are provided on the left side. The thrust magnetic bearing 2 is attached to a rotor yoke 2 fixed to the shaft 1.
3, stators 21 and 22, and a displacement sensor 24. The stators 21 and 22 are stator yokes 211 and 221 and excitation coil 21, respectively.
2, 222, and each magnetic pole surface 213, 223 faces the rotor yoke 23 in parallel with a gap therebetween. in this way,
The purpose of the annular configuration is to reduce the eddy current generated in the rotor yoke 23, and this has the effect of reducing the drag torque caused by the eddy current.

一方、ラジアル磁気軸受3はシヤフト1に固着
されたロータ32と、その外側に空隙を介してと
り囲むように配置されたステータ31と、半径方
向の変位を検出する変位センサ33とからなつて
いる。そして、これら全てがケーシング4内に納
められており、ステータ21,22,31及び変
位センサ24,33がそれぞれケーシング4に固
定されている。このスラスト磁気軸受2またはラ
ジアル磁気軸受3の動作原理は、概ね変位センサ
24または33の信号を受けて磁気軸受制御装置
(図示せず)が働き、ステータ21,22又は3
1に電流を供給して磁気吸引力を発生させること
によより、ロータヨーク23またはロータ32を
非接触状態で浮上させるものである。
On the other hand, the radial magnetic bearing 3 consists of a rotor 32 fixed to the shaft 1, a stator 31 disposed outside of the rotor 32 so as to surround the rotor 32 with a gap in between, and a displacement sensor 33 that detects displacement in the radial direction. . All of these are housed in the casing 4, and the stators 21, 22, 31 and displacement sensors 24, 33 are fixed to the casing 4, respectively. The principle of operation of the thrust magnetic bearing 2 or the radial magnetic bearing 3 is that a magnetic bearing control device (not shown) operates in response to a signal from the displacement sensor 24 or 33, and the stator 21, 22 or 3
The rotor yoke 23 or the rotor 32 is levitated in a non-contact state by supplying current to the rotor 1 to generate magnetic attraction force.

このような構成において、スラスト磁気軸受2
のステータ22の内径は、ロータヨーク23の内
径近くまで小さくすることができるので、磁極面
積を広くとれる。その結果として、吸引力を大き
くすることができる。しかし、ステータ21の内
径は、分解,組立てや製作上の面でラジアル磁気
軸受3のロータ32の外径よりも大きくすること
が必要である。そのため、ステータ21の内径を
シヤフト1の外径小くまで小さくすることができ
ず、シヤフトを左側へ吸引する吸引力を大きくす
ることが不可能であつた。
In such a configuration, the thrust magnetic bearing 2
Since the inner diameter of the stator 22 can be reduced to nearly the inner diameter of the rotor yoke 23, the magnetic pole area can be increased. As a result, the suction force can be increased. However, the inner diameter of the stator 21 needs to be larger than the outer diameter of the rotor 32 of the radial magnetic bearing 3 in terms of disassembly, assembly, and manufacturing. Therefore, it has been impossible to reduce the inner diameter of the stator 21 to the outer diameter of the shaft 1, and it has been impossible to increase the suction force that attracts the shaft to the left.

この問題点を解決するため、第7図に示すよう
にステータヨーク211を複数部分に分割した構
造のものが提案されている(特開昭57−61813号
公報参照)。
In order to solve this problem, a structure in which the stator yoke 211 is divided into a plurality of parts as shown in FIG. 7 has been proposed (see Japanese Patent Laid-Open No. 57-61813).

この構造によると、ステータヨーク211の内
径はシヤフト1の外径近くまで小さくすることが
できるが、分割部分の近傍の回転中のロータヨー
ク23内には渦電流が生じ、ドラツグトルクが大
きくなるという欠点が発生する。
According to this structure, the inner diameter of the stator yoke 211 can be reduced to be close to the outer diameter of the shaft 1, but there is a drawback that eddy currents are generated in the rotating rotor yoke 23 near the divided portions, increasing drag torque. Occur.

〔考案が解決しようとする問題点〕[Problem that the invention attempts to solve]

本考案は、従来技術におけるこのような欠点に
鑑み、スラスト磁気軸受のステータを容易に分解
組立てすると共に、渦電流の発生を極力抑えつつ
磁気吸引力を大きくとれるようにすることを目的
とする。
In view of these shortcomings in the prior art, it is an object of the present invention to easily disassemble and assemble the stator of a thrust magnetic bearing, and to increase the magnetic attraction force while suppressing the generation of eddy currents as much as possible.

〔問題点を解決するための手段〕[Means for solving problems]

本考案は、その目的を達成すべく、E形断面を
した円環状ステータアーマチヤを直径方向に沿つ
て複数に分割し、各分割部分の両端に内側溝から
中間部磁極の背面部を通つて外側溝に連通する連
通溝を設け、該連通溝を介して外側溝及び内側溝
とを通るように励磁コイルを巻回したことを特徴
とする。
In order to achieve this objective, the present invention divides an annular stator armature with an E-shaped cross section into a plurality of parts along the diameter direction, and connects the inner groove at both ends of each divided part to the back surface of the intermediate magnetic pole. It is characterized in that a communication groove communicating with the outer groove is provided, and the excitation coil is wound so as to pass through the outer groove and the inner groove via the communication groove.

〔実施例〕〔Example〕

次いで、実施例を用いて本考案の特徴を具体的
に説明する。
Next, the features of the present invention will be specifically explained using examples.

第1図は本考案によるステータの斜視図であ
り、径方向に2分割した端面部分を示している。
211はステータヨークであり、212は励磁コ
イルである。この端面部分の形状を理解しやすく
するためステータヨーク211の製作,手順の一
例を示す。まず、断面がE形の円環状のステータ
ヨークを径方向に2分割して第2図のような形状
を得る。次に、破線で示したように、磁極部を除
く端面部を一部除去して連通溝10を設け、第3
図の形状を得る。このようにしてできた内側溝9
から端面の磁極背面部の連通溝10を通つて外側
溝8に至る空間に励磁コイルを巻回する。こうし
て得られたのが第1図に示したものである。そし
て、これを2個接合して第4図のように1つのス
テータを構成する。
FIG. 1 is a perspective view of a stator according to the present invention, showing an end face portion divided into two in the radial direction.
211 is a stator yoke, and 212 is an exciting coil. An example of the procedure for manufacturing the stator yoke 211 will be shown to make it easier to understand the shape of this end face portion. First, an annular stator yoke with an E-shaped cross section is divided into two in the radial direction to obtain a shape as shown in FIG. Next, as shown by the broken line, a part of the end face except for the magnetic pole part is removed to provide a communication groove 10, and a third
Get the shape of the figure. Inner groove 9 created in this way
An excitation coil is wound in a space extending from the magnetic pole to the outer groove 8 through the communication groove 10 on the back side of the magnetic pole on the end face. The result obtained in this way is shown in FIG. Then, two of these are joined to form one stator as shown in FIG.

このような方法によると、励磁コイル212に
よつてできる磁極の一方は、内外両側の磁極面
7,6に現れ、もう一方の磁極は中間の磁極面5
に現れる。これらの磁極は、それぞれが分割され
た端面までのびているので、端面部分における磁
束の低減を無視することができる程度に抑えられ
る。このように構成されたステータと対面するロ
ータヨークにあつては、回転することによつて受
ける磁束の変化が小さく、渦電流に起因するドラ
ツグトルクも殆ど生じない。またステータが分割
可能に構成されているので、ステータ内径をラジ
アルまたはモータのロータ外径よりも小さくして
も分解,組立ての作業に何等支障を来すことがな
い。また、磁極面積を大きくして、吸引力を増大
させることもできる。
According to this method, one of the magnetic poles formed by the excitation coil 212 appears on both the inner and outer magnetic pole surfaces 7 and 6, and the other magnetic pole appears on the intermediate magnetic pole surface 5.
appears in Since each of these magnetic poles extends to the divided end face, the reduction in magnetic flux at the end face portion can be suppressed to a negligible level. The rotor yoke facing the stator configured in this manner receives only a small change in magnetic flux as it rotates, and almost no drag torque due to eddy currents occurs. Furthermore, since the stator is configured to be separable, even if the stator inner diameter is made smaller than the radial or motor rotor outer diameter, there will be no problem in disassembly and assembly operations. Moreover, the attractive force can also be increased by increasing the magnetic pole area.

上記の実施例では、ステータヨークを2分割と
しているが、3つ以上の分割をしても同じことで
あることは言うまでもない。即ち、製作上の作業
性を勘案して、分割数を自由に選択するとよい。
また、第5図に示すように、断面がC形またはH
形をしたステータヨークを用い、その半径方向の
分割端面部の磁極が端面まで延びた形状にしても
同じ効果が得られる。
In the above embodiment, the stator yoke is divided into two parts, but it goes without saying that the same effect can be achieved even if the stator yoke is divided into three or more parts. That is, it is preferable to freely select the number of divisions in consideration of manufacturing workability.
Also, as shown in Figure 5, the cross section is C-shaped or H-shaped.
The same effect can be obtained by using a shaped stator yoke in which the magnetic poles of the radially divided end face portion extend to the end face.

〔考案の効果〕[Effect of idea]

以上に説明したように、本考案によるとき、ス
ラスト磁気軸受のステータヨークが径方向に沿つ
て複数に分割されているので組立てが容易であ
る。そして、回転中のロータヨークに生じる渦電
流を大きすることなく、その内径をシヤフト外径
近くまで小さくすることができることからして、
ドラツグトルクを増すことなく、軸方向の吸引力
を増大することが可能となる。
As described above, according to the present invention, the stator yoke of the thrust magnetic bearing is divided into a plurality of parts along the radial direction, so that assembly is easy. Considering that the inner diameter of the rotating rotor yoke can be reduced to near the outer diameter of the shaft without increasing the eddy current generated in the rotating rotor yoke,
It becomes possible to increase the suction force in the axial direction without increasing the drag torque.

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

第1図は、本考案第1実施例におけるステータ
の分割片を示し、第2図及び第3図はその分割片
の製造手法を説明するものであり、第4図は2個
の分割片を円環状にくみたててステータを構成し
た状態を示す。また第5図は本考案第2実施例の
ステータをを示すものである。更に、第6図は従
来方法における励気軸受の構成例を示し、第7図
はその側面図である。 211:ステータアーマチヤ、21:励磁用コ
イル、8:外側溝、9:外側溝、10:連通溝。
FIG. 1 shows the divided pieces of the stator in the first embodiment of the present invention, FIGS. 2 and 3 explain the manufacturing method of the divided pieces, and FIG. 4 shows the two divided pieces. The stator is shown assembled into an annular shape. FIG. 5 shows a stator according to a second embodiment of the present invention. Furthermore, FIG. 6 shows an example of the configuration of an excitation bearing in a conventional method, and FIG. 7 is a side view thereof. 211: Stator armature, 21: Excitation coil, 8: Outer groove, 9: Outer groove, 10: Communication groove.

Claims (1)

【実用新案登録請求の範囲】 1 E形断面をした円環状ステータアーマチヤを
直径方向に沿つて複数に分割し、各分割部分の
両端に内側溝から中間部磁極の背面部を通つて
外側溝に連通する連通溝を設け、該連通溝を介
して外側溝及び内側溝とを通るように励磁コイ
ルを巻回したことを特徴とする吸引制御形スラ
スト磁気軸受のステータ。 2 分割して励磁コイルを巻回した2つのステー
タアーマチヤを、分割前の円環状となるよう端
面部を互いに対面させて固定する実用新案登録
請求の範囲1.記載のスラスト磁気軸受のステー
タ。 3 分割数を3つ以上とする実用新案登録請求の
範囲1.又は2.記載のスラスト磁気軸受のステー
タ。 4 断面形状がC形またはH形であることを特徴
とする実用新案登録請求の範囲1.,2.又は3.記
載のスラスト磁気軸受のステータ。
[Claims for Utility Model Registration] 1. An annular stator armature with an E-shaped cross section is divided into a plurality of parts along the diameter direction, and an outer groove is formed at both ends of each divided part from the inner groove through the back surface of the intermediate magnetic pole. 1. A stator for an attraction-controlled thrust magnetic bearing, characterized in that a communication groove is provided that communicates with the outer groove, and an excitation coil is wound so as to pass through the outer groove and the inner groove through the communication groove. 2. A stator for a thrust magnetic bearing according to claim 1, in which two stator armatures each having a divided excitation coil wound thereon are fixed with their end faces facing each other so as to form an annular shape before division. 3. A stator for a thrust magnetic bearing according to claim 1 or 2 of the utility model registration claim, which has three or more divisions. 4. A stator for a thrust magnetic bearing according to claim 1., 2. or 3., characterized in that the cross-sectional shape is C-shaped or H-shaped.
JP12121485U 1985-08-06 1985-08-06 Expired JPH0222497Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12121485U JPH0222497Y2 (en) 1985-08-06 1985-08-06

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12121485U JPH0222497Y2 (en) 1985-08-06 1985-08-06

Publications (2)

Publication Number Publication Date
JPS6228920U JPS6228920U (en) 1987-02-21
JPH0222497Y2 true JPH0222497Y2 (en) 1990-06-18

Family

ID=31010272

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12121485U Expired JPH0222497Y2 (en) 1985-08-06 1985-08-06

Country Status (1)

Country Link
JP (1) JPH0222497Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6681802B2 (en) * 2016-08-01 2020-04-15 株式会社Ihi Diskless thrust magnetic bearing and 3-axis active control magnetic bearing

Also Published As

Publication number Publication date
JPS6228920U (en) 1987-02-21

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