JPH01219391A - Magnetic bearing unit - Google Patents
Magnetic bearing unitInfo
- Publication number
- JPH01219391A JPH01219391A JP4783788A JP4783788A JPH01219391A JP H01219391 A JPH01219391 A JP H01219391A JP 4783788 A JP4783788 A JP 4783788A JP 4783788 A JP4783788 A JP 4783788A JP H01219391 A JPH01219391 A JP H01219391A
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnet
- rotating body
- electromagnet
- rotor
- magnetic 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.)
- Pending
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
- F16C32/044—Active magnetic bearings
-
- 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
Landscapes
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Non-Positive Displacement Air Blowers (AREA)
- Magnetic Bearings And Hydrostatic Bearings (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
産業上の利用分野
この発明は、磁気軸受装置、さらに詳しくは、たとえば
真空用スピンドルなどに用いられる1軸制御4軸受動安
定磁気軸受装置に関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetic bearing device, and more particularly, to a single-axis controlled four-axis passively stable magnetic bearing device used in, for example, a vacuum spindle.
従来の技術
真空用スピンドルなどに用いられる磁気軸受装置として
、従来、回転体の回転軸回りの自由度を除く5自由度を
すべて電磁石の吸引力を調節して位置決めする5自由度
能動制御軸受のほか、能動的に制御する自由度を減少さ
せた3軸制御式磁気軸受が知られている(特開昭61−
277896号参照)。この3軸制御式磁気軸受装置は
、永久磁石と能動型アキシアル磁気軸受により軸方向の
位置決めがなされ、1箇所に設けられた2軸の能動型ラ
ジアル磁気軸受と前記の永久磁石とアキシアル磁気軸受
に夷る受動的なラジアル復元力により半径方向の位置決
めがなされるものである。Conventional technology As a magnetic bearing device used in a vacuum spindle, etc., a 5-degree-of-freedom active control bearing is conventionally used, in which positioning is performed by adjusting the attractive force of an electromagnet in all 5 degrees of freedom, excluding the degree of freedom around the rotation axis of a rotating body. In addition, a three-axis controlled magnetic bearing with a reduced degree of freedom for active control is known (Japanese Unexamined Patent Application Publication No. 1983-1999).
277896). This 3-axis controlled magnetic bearing device uses a permanent magnet and an active axial magnetic bearing to determine its position in the axial direction. Positioning in the radial direction is performed by a passive radial restoring force.
発明が解決しようとする課題
上記の3軸制御式磁気軸受は、5自由度能動制御磁気軸
受に比較して安価であるが、それでも、3軸分の磁気軸
受とその制御回路などが必要であり、かなり高価なもの
である。Problems to be Solved by the Invention Although the above three-axis controlled magnetic bearing is cheaper than a five-degree-of-freedom active control magnetic bearing, it still requires magnetic bearings for three axes and their control circuits. , which is quite expensive.
この発明の目的は、上記の問題を解決し、3軸制御式磁
気軸受よりさらに安価で、しかも回転体を完全非接触状
態に安定良く支持できる1軸制御4軸受動安定磁気軸受
装置を提供することにある。An object of the present invention is to solve the above problems and provide a single-axis controlled four-axis passive stable magnetic bearing device that is cheaper than a three-axis controlled magnetic bearing and that can stably support a rotating body in a completely non-contact state. There is a particular thing.
課題を解決するための手段
この発明による磁気軸受装置は、回転体にその軸方向の
磁力を作用させて回転可能に軸受する永久磁石型軸受と
、この軸受が回転体に及ぼす磁力とは逆方向の磁力を回
転体に及ぼす電磁石と、回転体の半径方向の振れ回り量
を検出する振れ回り量検出手段と、振れ回り量が増大し
た場合に回転体の位置を前記永久磁石型軸受の相互間隔
が減少するよう変化させるために前記電磁石の磁力を変
化させる手段とを備えていることを特徴とするものであ
る。Means for Solving the Problems A magnetic bearing device according to the present invention includes a permanent magnet type bearing that rotatably supports a rotating body by applying magnetic force in the axial direction of the rotating body, and a permanent magnet type bearing in which the magnetic force exerted on the rotating body is in the opposite direction. an electromagnet that applies a magnetic force to the rotating body; a whirling amount detection means for detecting the amount of whirling of the rotary body in the radial direction; and means for changing the magnetic force of the electromagnet so as to decrease the magnetic force of the electromagnet.
作 用
回転体の振れ回り量が増大すると、電磁石の磁力が変化
し、回転体の位置が変化して、永久磁石型軸受の相互間
隔が減少する。このため、永久磁石型軸受の磁力が増大
して、半径方向の剛性が大きくなる。したがって、回転
体の振れ回り量が小さくなり、回転体は安定良く支持さ
れて回転する。When the whirling amount of the working rotating body increases, the magnetic force of the electromagnet changes, the position of the rotating body changes, and the mutual spacing between the permanent magnet type bearings decreases. Therefore, the magnetic force of the permanent magnet type bearing increases, and the rigidity in the radial direction increases. Therefore, the amount of whirling of the rotating body is reduced, and the rotating body is stably supported and rotated.
実 施 例
第1図は、この発明による磁気軸受装置の機械的構成の
1例を示す。Embodiment FIG. 1 shows an example of the mechanical configuration of a magnetic bearing device according to the present invention.
この磁気軸受装置は1軸制御4軸受動安定磁気軸受装置
であり、水平円板状のベース(1)の上面に、上下両端
が開口した円筒状の上部ハウジング(2)が、ベース(
1)の下面に、上端のみが開口した短円筒状の下部ハウ
ジング(3)がそれぞれ固定されている。ベース(1)
の中心には、これを上下に貫通するシャフト挿入穴(4
)が形成されている。ベース(1)の上面には、シャフ
ト挿入穴(4)より内径が大きくて上部ハウジング(2
)の内径より外径の小さい円筒部(la)が−体に形成
されている。ベース(1)の下面には、シャフト挿入穴
(4)より内径が大きくて下部ハウジング(3)と内径
の等しい円形凹所(5)が形成されている。This magnetic bearing device is a 1-axis controlled 4-axis passive stable magnetic bearing device, in which a cylindrical upper housing (2) with open upper and lower ends is mounted on the upper surface of a horizontal disc-shaped base (1).
A short cylindrical lower housing (3) with only its upper end open is fixed to the lower surface of each of the housings (1). Base (1)
In the center of the shaft is a shaft insertion hole (4
) is formed. The upper surface of the base (1) has an inner diameter larger than the shaft insertion hole (4) and an upper housing (2).
) A cylindrical portion (la) having an outer diameter smaller than the inner diameter is formed into a negative body. A circular recess (5) having an inner diameter larger than the shaft insertion hole (4) and the same inner diameter as the lower housing (3) is formed on the lower surface of the base (1).
上部ハウジング(2)内の上部に、水平円板状の永久磁
石支持部材(8)がスペーサ(7)を介して固定されて
いる。この支持部材(6)の下面中心部に、円筒部(8
a)が一体に形成されている。A horizontal disk-shaped permanent magnet support member (8) is fixed to the upper part of the upper housing (2) via a spacer (7). A cylindrical portion (8
a) are integrally formed.
下部ハウジング(3)内の下部に、ベース(1)の凹所
(5)にはめられたスペーサ(8)を介して、水平円板
状の電磁石支持部材(9)が固定されている。この支持
部材(9)の中心部には、これを上下に貫通するセンサ
取付穴(lO)が形成され、この穴(lO)の下部には
水平円板状のセンサ取付部材(11)がはめ止められて
いる。A horizontal disk-shaped electromagnet support member (9) is fixed to the lower part of the lower housing (3) via a spacer (8) fitted in a recess (5) of the base (1). A sensor mounting hole (lO) is formed in the center of this support member (9), passing through it vertically, and a horizontal disc-shaped sensor mounting member (11) is fitted into the lower part of this hole (lO). It's stopped.
ベース(1)のシャフト挿入穴(4)に垂直なシャフト
(12)が隙間をあけて上下貫通状に挿入されている。A vertical shaft (12) is inserted vertically through the shaft insertion hole (4) of the base (1) with a gap therebetween.
ベース(1)の円筒部(la)より上方に突出したシャ
フト(12)の上部に、上部ハウジング(2)内のスペ
ーサ(7)と円筒部(la)の間に位置する筒状体(1
3)の中心円板部(13a)が固定されている。ベース
(1)の凹所(5)より下方に突出したシャフト(12
)の下部に、凹所(5)内のスペーサ(8)の内側に位
置する水平円板状の永久磁石取付部材(14)およびロ
ータディスク(15)が固定され、電磁石支持部材(9
)のセンサ取付穴(10)にはまったシャフト(12)
の下端部には下端が綴じた円筒状のターゲット(1B)
が固定されている。そして、シャフト(12)とこれに
固定された上記の部品により、ロータ(回転体)(R)
が構成されている。A cylindrical body (1) located between the spacer (7) in the upper housing (2) and the cylindrical part (la) is attached to the upper part of the shaft (12) that protrudes upward from the cylindrical part (la) of the base (1).
The central disk portion (13a) of 3) is fixed. The shaft (12) protrudes downward from the recess (5) of the base (1).
), a horizontal disk-shaped permanent magnet mounting member (14) and a rotor disk (15) located inside the spacer (8) in the recess (5) are fixed to the lower part of the electromagnet support member (9
) Shaft (12) fitted into sensor mounting hole (10)
A cylindrical target (1B) with the bottom end bound at the bottom end of the
is fixed. Then, the shaft (12) and the above-mentioned parts fixed thereto rotate the rotor (rotating body) (R).
is configured.
上部ハウジング(2)内の永久磁石支持部材(6)と筒
状体(13)の間に、上部永久磁石型軸受(17)が設
けられている。この軸受(17)は、永久磁石支持部材
(6)の下面に固定された環状永久磁石(17a)と筒
状体(13)の上端面に固定された環状永久磁石(17
b)とからなり、これらの永久磁石(17a) (17
b)が互いに吸引力を及ぼすように異極同志対向させら
れている。ベース(1)とシャフト(12)に固定され
た永久磁石取付部材(14)の間にも、下部永久磁石型
軸受(18)が設けられている。この軸受(18)は、
ベース(1)の凹所(5)内の下面に固定された環状永
久磁石(18a)と永久磁石取付部材(14)の上面に
固定された環状永久磁石(18b)とからなり、これら
の永久磁石(18a) (18b)が互いに吸引力を及
ぼすように異極間志対向させられている。そして、これ
ら上下の永久磁石型軸受(17)(1B)により、ロー
タ(R)が上向きに吸引されている。下部ノ1ウジング
(3)内の電磁石支持部材(9)に、シャフト(12)
に固定されたロータディスク(15)に対向してロータ
(R)を下向きに吸引する電磁石(19)が設けられて
いる。ベース(1)の円筒部(la)内にモータステー
タ(20)が、シャフト(12)にこれに対応するモー
タロータ(21)が設けられている。An upper permanent magnet type bearing (17) is provided between the permanent magnet support member (6) and the cylindrical body (13) in the upper housing (2). This bearing (17) consists of an annular permanent magnet (17a) fixed to the lower surface of the permanent magnet support member (6) and an annular permanent magnet (17a) fixed to the upper end surface of the cylindrical body (13).
b), and these permanent magnets (17a) (17
b) are placed opposite to each other so as to exert an attractive force on each other. A lower permanent magnet type bearing (18) is also provided between the base (1) and the permanent magnet mounting member (14) fixed to the shaft (12). This bearing (18) is
Consists of an annular permanent magnet (18a) fixed to the lower surface of the recess (5) of the base (1) and an annular permanent magnet (18b) fixed to the upper surface of the permanent magnet mounting member (14). The magnets (18a) and (18b) are opposed to each other so as to exert an attractive force on each other. The rotor (R) is attracted upward by these upper and lower permanent magnet type bearings (17) (1B). The shaft (12) is attached to the electromagnet support member (9) in the lower housing (3).
An electromagnet (19) is provided facing the rotor disk (15) fixed to the rotor (R) and attracting the rotor (R) downward. A motor stator (20) is provided within the cylindrical portion (la) of the base (1), and a corresponding motor rotor (21) is provided on the shaft (12).
シャフト(12)の上端部は永久磁石支持部材(6)の
円筒部(6a)内に入っており、この円筒部(8a)内
には上部保護軸受(22)が設けられている。The upper end of the shaft (12) is placed within a cylindrical portion (6a) of the permanent magnet support member (6), and an upper protection bearing (22) is provided within this cylindrical portion (8a).
また、ベース(1)のシャフト挿入穴(4)内に、下部
保護軸受(23)が設けられている。なお、ロータ(R
)回転中は、上下の保護軸受(22) (23)とシャ
フト(12)の間には若干の隙間が生じるようになって
いる。Further, a lower protection bearing (23) is provided in the shaft insertion hole (4) of the base (1). In addition, the rotor (R
) During rotation, a slight gap is created between the upper and lower protective bearings (22) (23) and the shaft (12).
下部ハウジング(3)内の電磁石支持部材(9)に固定
されたセンサ取付部材(11)の上面に、シャフト(1
2)に固定されたターゲット(1B)に対向して、ロー
タ(R)の軸方向(上下方向)の位置を検出するための
軸方向センサ(24)が設けられている。また、上部ハ
ウジング(2)の周壁に、ロータ(R)の筒状体(13
)の外周面に対向して、その半径方向の振れ回り量を検
出するための半径方向センサ(25)が設けられている
。A shaft (1
An axial direction sensor (24) for detecting the position of the rotor (R) in the axial direction (vertical direction) is provided opposite to the target (1B) fixed to the rotor (2). Further, the cylindrical body (13) of the rotor (R) is attached to the peripheral wall of the upper housing (2).
) is provided with a radial sensor (25) facing the outer circumferential surface of the rotor for detecting the amount of whirling in the radial direction.
第2図は、磁気軸受装置の電磁石制御部分の電気的構成
の1例を示す。軸方向センサ(24)の出力は軸方向位
置検出回路(26)によりロータ(R)の軸方向の変位
に比例する信号に変換され、この検出回路(26)の出
力が制御回路(27)に入力する。なお、軸方向変位は
、定常状態よりロータ(R)が上昇した場合を正、ロー
タ(13)が下降した場合を負としており、軸方向位置
検出回路(26)の出力は、ロータ(R)が上昇すると
大きくなり、ロータ(R)が下降すると小さくなる。−
方、半径方向センサ(25)の出力は振れ回り量検出回
路(28)によりロータ(R)の振れ回り量に比例する
信号に変換され、この検出回路(28)の出力が制御回
路(27)に入力する。そして、制御回路(27)は、
これら検出回路(26)(28)からの信号を処理して
、電磁石(19)を駆動する電力増幅器り29)に制御
信号を出力する。FIG. 2 shows an example of the electrical configuration of the electromagnet control portion of the magnetic bearing device. The output of the axial direction sensor (24) is converted by the axial position detection circuit (26) into a signal proportional to the axial displacement of the rotor (R), and the output of this detection circuit (26) is sent to the control circuit (27). input. Note that the axial displacement is positive when the rotor (R) rises from the steady state, and negative when the rotor (13) descends from the steady state.The output of the axial position detection circuit (26) is It increases as the rotor (R) rises, and decreases as the rotor (R) descends. −
On the other hand, the output of the radial direction sensor (25) is converted into a signal proportional to the amount of whirling of the rotor (R) by the whirling amount detection circuit (28), and the output of this detection circuit (28) is sent to the control circuit (27). Enter. And the control circuit (27)
The signals from these detection circuits (26) and (28) are processed and a control signal is output to a power amplifier 29) that drives the electromagnet (19).
第3図は、制御回路(27)の1例を示す。軸方向位置
検出回路(2B)の出力は、比例微分要素(PIl要素
(31)により、軸方向変位に比例する量と軸方向変
位の微分値に比例する量の和に変換され、このPIl要
素31)の出力が増幅器(32)を経て加算器(33)
に入力する。軸方向位置検出回路(26)の出力は、ま
た、積分要素(l要素)(34)により、軸方向変位の
積分値に比例する信号に変換され、このl要素(34)
の出力が調整要素(35)に入力する。一方、振れ回り
量検出回路(28)の出力は、調整要素(35)に入力
する。調整要素(35)はたとえば加算器よりなり、こ
れによりl要素(34)の出力と振れ回り量検出回路(
28)の出力すなわち振れ回り量とが加算されて加算器
(33)に送られる。そして、加算器(83)により、
増幅器(32)の出力と調整要素(35)の出力が加算
されて、電力増幅器(29)に送られる。FIG. 3 shows an example of the control circuit (27). The output of the axial position detection circuit (2B) is converted by a proportional differential element (PIl element (31)) into the sum of an amount proportional to the axial displacement and an amount proportional to the differential value of the axial displacement, and this PIl element The output of 31) passes through an amplifier (32) to an adder (33).
Enter. The output of the axial position detection circuit (26) is also converted by an integral element (l element) (34) into a signal proportional to the integral value of the axial displacement, and this l element (34)
The output of is input to the adjustment element (35). On the other hand, the output of the whirling amount detection circuit (28) is input to the adjustment element (35). The adjustment element (35) is composed of, for example, an adder, which allows the output of the l element (34) and the whirling amount detection circuit (
28), that is, the amount of whirling, are added together and sent to an adder (33). Then, by the adder (83),
The output of the amplifier (32) and the output of the regulating element (35) are summed and sent to the power amplifier (29).
第4図は振れ回り量検出回路(28)の1例を示し、第
5図はその各部の信号を示す。ロータ(R)に振れ回り
が生じると、半径方向センサ(25)には第5図(a)
のような交流出力があられれる。FIG. 4 shows an example of the whirling amount detection circuit (28), and FIG. 5 shows signals of each part thereof. When the rotor (R) whirls around, the radial direction sensor (25) is detected as shown in Fig. 5 (a).
An AC output like this can be obtained.
このセンサ(25)の出力は、絶対値回路(36)によ
り同図(b)のように余波整流される。この出力は、さ
らに、ローパスフィルタ(37)により平滑化されて同
図(C)のような直流電圧となり、この電圧は振れ回り
量に比例している。The output of this sensor (25) is rectified by the absolute value circuit (36) as shown in FIG. 2(b). This output is further smoothed by a low-pass filter (37) to become a DC voltage as shown in FIG. 3(C), and this voltage is proportional to the whirling amount.
制御回路(27)から調整要素(35)を除いた回路、
すなわち、l要素(34)の出力がそのまま加算器(3
3)に入力するものは、磁気軸受装置において電磁石を
制御する通常のPID制御回路である。A circuit obtained by removing the adjustment element (35) from the control circuit (27),
In other words, the output of the l element (34) is directly sent to the adder (3
The input to 3) is a normal PID control circuit that controls the electromagnet in a magnetic bearing device.
次に、まず、制御回路(27)から調整要素(35)を
除いたものについて、動作を説明する。Next, first, the operation of the control circuit (27) excluding the adjustment element (35) will be described.
この場合、増幅器(32)の出力すなわち軸方向変位に
比例する量と軸方向変位の微分値に比例する量の和の信
号と1要素(34)の出力すなわち軸方向変位の積分値
に比例する信号が加算器(33)により加算されて、電
力増幅器(29)に送られる。In this case, the output of the amplifier (32), that is, the signal of the sum of the amount proportional to the axial displacement and the amount proportional to the differential value of the axial displacement, and the output of one element (34), that is, the signal proportional to the integral value of the axial displacement. The signals are summed by an adder (33) and sent to a power amplifier (29).
定常状態では、上下の永久磁石型軸受(17) (18
)がロータ(R)を上向きに吸引し、電磁石(19)が
ロータ(R)を下向きに吸引している。このとき、軸受
(17)(1g)の永久磁石(17a) (17b)
(18a) (18b)の諸元を適当に選択することに
より、軸受(17)(18)による上向きの吸引力をロ
ータ(R)の重量より著しく大きくして、この重量の影
響を無視できるようにすることができる。そして、電磁
石(19)には、永久磁石型軸受(17) (18)の
上向きの吸引力と大きさの等しい下向きの吸引力が生じ
るような電流が定常的に流される。回転体(R)が上昇
して、軸方向位置検出回路(2B)の出力が大きくなる
と、電磁石(19)に流れる電流が大きくなって、回転
体(R)は下降させられる。In steady state, upper and lower permanent magnet type bearings (17) (18
) attracts the rotor (R) upward, and the electromagnet (19) attracts the rotor (R) downward. At this time, the permanent magnets (17a) (17b) of the bearing (17) (1g)
By appropriately selecting the specifications of (18a) and (18b), the upward suction force by the bearings (17) and (18) can be made significantly larger than the weight of the rotor (R), so that the influence of this weight can be ignored. It can be done. A current is constantly passed through the electromagnet (19) to generate a downward attractive force that is equal in magnitude to the upward attractive force of the permanent magnet bearings (17, 18). When the rotating body (R) rises and the output of the axial position detection circuit (2B) increases, the current flowing through the electromagnet (19) increases and the rotating body (R) is lowered.
逆に、回転体(R)が下降して、軸方向位置検出回路(
2B)の出力が小さ(なると、電磁石(19)に流れる
電流が小さくなって、回転体(R)は上昇させられる。Conversely, the rotating body (R) descends and the axial position detection circuit (
2B) becomes small (when the output of the electromagnet (19) becomes small, the current flowing through the electromagnet (19) becomes small, and the rotating body (R) is raised.
これにより、軸方向の力の釣合いが保たれ、軸方向の位
置決めが可能となる。また、永久磁石型軸受(17)(
18)および電磁石(19)の吸引力により、半径方向
にも受動的に安定しており、電磁石(19)を制御する
だけの1軸制御によりロータ(R)を完全非接触状態に
支持して回転させることが可能である。This maintains the balance of axial forces and enables axial positioning. In addition, permanent magnet type bearing (17) (
18) and the attractive force of the electromagnet (19), it is passively stabilized in the radial direction, and the rotor (R) is supported in a completely non-contact state by uniaxial control that only controls the electromagnet (19). It is possible to rotate.
ところで、このように制御回路(27)から調整要素(
35)を除いた回路では、ロータ(R)の半径方向の運
動に対しては全く制御を行なわないため、様々な不安定
が生じる。By the way, in this way, the adjustment element (
In the circuits other than 35), various instability occurs because the radial movement of the rotor (R) is not controlled at all.
ところが、上記の制御回路(27)では、ロータ(R)
の振れ回り量による調整要素(35)が設けられている
ので、次に説明するように、回転体(R)の振れ回り量
を小さくして、安定に回転させることができる。However, in the above control circuit (27), the rotor (R)
Since the adjustment element (35) according to the amount of whirl is provided, the amount of whirl of the rotating body (R) can be reduced and the rotating body (R) can be rotated stably, as will be explained next.
調整要素(35)は、I要素(34)の出力を振れ回り
量分だけ変化させ、その結果、電磁石(19)に流れる
電流が振れ回り量分だけ小さくなるように制御回路(1
7)の出力が制御される。そして、振れ回り量が0のと
きには、I要素(34)の出力がそのまま加算器に送ら
れ、前述の調整要素(35)がない場合と同様の制御が
行われる。ロータ(R)に振れ回りが生じると、前述の
ように、電磁石(19)に流れる電流が振れ回り量分だ
け小さくなるため、ロータ(R)が上昇させられ、上下
の永久磁石型軸受(17) (1g)の間隔が小さくな
る。The adjustment element (35) changes the output of the I element (34) by the amount of whirl, and as a result, the control circuit (1) changes the current flowing through the electromagnet (19) by the amount of whirl.
7) output is controlled. When the amount of whirling is 0, the output of the I element (34) is sent as is to the adder, and the same control as in the case without the adjustment element (35) described above is performed. When whirling occurs in the rotor (R), the current flowing through the electromagnet (19) decreases by the whirling amount, as described above, so the rotor (R) is raised and the upper and lower permanent magnet type bearings (17 ) (1g) becomes smaller.
永久磁石型軸受(17)(1g)の間隔が小さくなると
、その分だけ吸引力が大きくなり、その結果、回転体(
R)の半径方向の剛性が高くなり、振れ回り量が小さく
なる。As the distance between the permanent magnet bearings (17) (1g) becomes smaller, the attractive force increases accordingly, and as a result, the rotating body (
The rigidity of R) in the radial direction is increased, and the amount of whirling is reduced.
発明の効果
この発明の磁気軸受装置によれば、上述のように、1つ
の電磁石だけを制御すればよいので、3軸制御式磁気軸
受よりさらに安価にすることができ、しかも回転体の振
れ回り量を小さくしてこれを完全非接触状態に安定良く
支持することができる。Effects of the Invention According to the magnetic bearing device of the present invention, as described above, since only one electromagnet needs to be controlled, the cost can be lower than that of a three-axis control type magnetic bearing, and moreover, the swing of the rotating body can be reduced. By reducing the amount, it is possible to stably support this in a completely non-contact state.
第1図はこの発明の1実施例を示す磁気軸受装置の垂直
断面図、第2図は磁気軸受装置の電磁石制御部分の電気
的構成の1例を示すブロック図、第3図は制御回路の1
例を示すブロック図、第4図は振れ回り量検出回路の1
例を示すブロック図、第5図は振れ回り量検出回路の各
部の信号を示すグラフである。
(17)(18)−・・永久磁石型軸受、(17a)
(17b) (18a)(18b)・・・環状永久磁石
、(19)・・・電磁石、(25)・・・半径方向セン
サ、(27)・・・制御回路、(28)・・・振れ回り
量検出回路、(R)・・・ロータ(回転体)。
以 上
特許出願人 光洋精工株式会社FIG. 1 is a vertical sectional view of a magnetic bearing device showing one embodiment of the present invention, FIG. 2 is a block diagram showing an example of the electrical configuration of the electromagnet control portion of the magnetic bearing device, and FIG. 3 is a control circuit diagram. 1
A block diagram showing an example, Fig. 4 is one of the whirling amount detection circuits.
FIG. 5, a block diagram showing an example, is a graph showing signals of each part of the whirling amount detection circuit. (17) (18) --- Permanent magnet type bearing, (17a)
(17b) (18a) (18b)... Annular permanent magnet, (19)... Electromagnet, (25)... Radial direction sensor, (27)... Control circuit, (28)... Runout Rotation amount detection circuit, (R)...rotor (rotating body). Patent applicant: Koyo Seiko Co., Ltd.
Claims (1)
する永久磁石型軸受と、この軸受が回転体に及ぼす磁力
とは逆方向の磁力を回転体に及ぼす電磁石と、回転体の
半径方向の振れ回り量を検出する振れ回り量検出手段と
、振れ回り量が増大した場合に回転体の位置を前記永久
磁石型軸受の相互間隔が減少するよう変化させるために
前記電磁石の磁力を変化させる手段とを備えていること
を特徴とする磁気軸受装置。A permanent magnet type bearing applies a magnetic force in the axial direction to a rotating body so that it can rotate, an electromagnet applies a magnetic force on the rotating body in the opposite direction to the magnetic force that this bearing exerts on the rotating body, and a permanent magnet bearing applies a magnetic force in the radial direction of the rotating body. whirling amount detection means for detecting the whirling amount of the permanent magnet type bearing; and changing the magnetic force of the electromagnet in order to change the position of the rotating body so that the mutual distance between the permanent magnet type bearings decreases when the whirling amount increases. A magnetic bearing device comprising means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4783788A JPH01219391A (en) | 1988-02-29 | 1988-02-29 | Magnetic bearing unit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4783788A JPH01219391A (en) | 1988-02-29 | 1988-02-29 | Magnetic bearing unit |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH01219391A true JPH01219391A (en) | 1989-09-01 |
Family
ID=12786479
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4783788A Pending JPH01219391A (en) | 1988-02-29 | 1988-02-29 | Magnetic bearing unit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01219391A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20130260999A1 (en) * | 2012-04-03 | 2013-10-03 | The Boeing Company | Open-core flywheel architecture |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5815718A (en) * | 1981-07-21 | 1983-01-29 | Nissan Diesel Motor Co Ltd | Intake device for inertially-supercharged internal combustion engine |
| JPS5829408A (en) * | 1981-08-13 | 1983-02-21 | デルタ工業株式会社 | Reclining apparatus of automobile seat |
| JPS5879695A (en) * | 1981-11-06 | 1983-05-13 | Seiko Instr & Electronics Ltd | Axial molecular pump |
| JPS59731A (en) * | 1982-06-28 | 1984-01-05 | Hitachi Ltd | Join operation processing system |
-
1988
- 1988-02-29 JP JP4783788A patent/JPH01219391A/en active Pending
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5815718A (en) * | 1981-07-21 | 1983-01-29 | Nissan Diesel Motor Co Ltd | Intake device for inertially-supercharged internal combustion engine |
| JPS5829408A (en) * | 1981-08-13 | 1983-02-21 | デルタ工業株式会社 | Reclining apparatus of automobile seat |
| JPS5879695A (en) * | 1981-11-06 | 1983-05-13 | Seiko Instr & Electronics Ltd | Axial molecular pump |
| JPS59731A (en) * | 1982-06-28 | 1984-01-05 | Hitachi Ltd | Join operation processing system |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20130260999A1 (en) * | 2012-04-03 | 2013-10-03 | The Boeing Company | Open-core flywheel architecture |
| US9729025B2 (en) * | 2012-04-03 | 2017-08-08 | The Boeing Company | Open-core flywheel architecture |
| US10826348B2 (en) | 2012-04-03 | 2020-11-03 | The Boeing Company | Open-core flywheel architecture |
| US11070107B2 (en) | 2012-04-03 | 2021-07-20 | The Boeing Company | Open-core flywheel architecture |
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