Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6237246B2 - - Google Patents
[go: Go Back, main page]

JPS6237246B2 - - Google Patents

Info

Publication number
JPS6237246B2
JPS6237246B2 JP5940281A JP5940281A JPS6237246B2 JP S6237246 B2 JPS6237246 B2 JP S6237246B2 JP 5940281 A JP5940281 A JP 5940281A JP 5940281 A JP5940281 A JP 5940281A JP S6237246 B2 JPS6237246 B2 JP S6237246B2
Authority
JP
Japan
Prior art keywords
rotor
magnetic bearing
thrust
radial
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
JP5940281A
Other languages
Japanese (ja)
Other versions
JPS57173614A (en
Inventor
Shiro Hagiwara
Kazuo Tsucha
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP5940281A priority Critical patent/JPS57173614A/en
Publication of JPS57173614A publication Critical patent/JPS57173614A/en
Publication of JPS6237246B2 publication Critical patent/JPS6237246B2/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
    • F16C32/0444Details of devices to control the actuation of the electromagnets
    • F16C32/0451Details of controllers, i.e. the units determining the power to be supplied, e.g. comparing elements, feedback arrangements with P.I.D. control
    • 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

Landscapes

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

Description

【発明の詳細な説明】 この発明は、電磁石や永久磁石の吸引力を利用
して、回転体を機械的な接触部なしに支持する磁
気軸受に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic bearing that supports a rotating body without mechanical contact by using the attractive force of an electromagnet or a permanent magnet.

従来、この種の装置としては第1図に示すもの
があつた。図において1はロータ、2はスラスト
磁気軸受用回転磁極、3a,3bはそれぞれスラ
スト磁気軸受用電磁石、4は放射状に磁化された
リング状永久磁気、5aはラジアル磁気軸受用固
定磁極、5bはラジアル磁気軸受用回転磁極、6
はステータ、7は位置センサ、8は位置センサ回
路、9は演算増幅器、10は位相補償回路、11
は電力増幅器である。
Conventionally, there has been a device of this type as shown in FIG. In the figure, 1 is a rotor, 2 is a rotating magnetic pole for a thrust magnetic bearing, 3a and 3b are electromagnets for a thrust magnetic bearing, 4 is a radially magnetized ring-shaped permanent magnet, 5a is a fixed magnetic pole for a radial magnetic bearing, and 5b is a radial magnetic bearing. Rotating magnetic pole for magnetic bearing, 6
is a stator, 7 is a position sensor, 8 is a position sensor circuit, 9 is an operational amplifier, 10 is a phase compensation circuit, 11
is a power amplifier.

ロータ1には磁極2,5bが装着され、ステー
タ6には電磁石3a,3b、磁極5aが装着さ
れ、これらの間に働く吸引力によつてロータ1は
軸のまわりに回転しながらステータ6に対し所定
の関係位置に機械的な接触部なしに支持される。
The rotor 1 is equipped with magnetic poles 2, 5b, and the stator 6 is equipped with electromagnets 3a, 3b, and a magnetic pole 5a.The rotor 1 is rotated around its axis by the attractive force that acts between them, and is attached to the stator 6. On the other hand, it is supported in a predetermined relative position without mechanical contact.

第2図は第1図に示すスラスト磁気軸受の動作
を示す説明図で、第1図と同一符号は同一部分を
示し、図に示す実線矢印はロータ1に装着された
リング状永久磁石4のN極から出てS極にもどる
磁束であつて、回転磁極2を通つて上下方向に別
れ、空隙を経てスラスト磁気軸受用磁石3a,3
bの鉄心に流入し、再び空隙を経て回転磁極2に
達しS極にもどる。電磁石3aの鉄心と回転磁極
2との空隙(以下、上部空隙という)と、電磁石
3bの鉄心と回転磁極2との空隙(以下、下部空
隙という)とが等しくなる位置(スラスト方向の
位置)にロータ1があれば上部空隙と下部空隙の
磁束(実線で示す磁束だけを考える)の大きさは
互に等しくなりロータ1に働く上下方向(スラス
ト方向)の吸引力は釣合う。しかし、この釣合点
は不安定であり、たとえばロータ1が少しでも下
方へ動くと下部空隙の磁束による吸引力の方が強
くなり、ロータ1は益々下方へ動くことになる。
すなわちロータ1のスラスト方向の位置とロータ
1に装着された永久磁石4による吸引力との関係
は正帰還の関係になつている。そこで電磁石3
a,3bの吸引力を制御してロータ1の位置と綜
合的な吸引力との関係を負帰還の関係にしてスラ
スト方向の位置制御を安定化させる。
FIG. 2 is an explanatory diagram showing the operation of the thrust magnetic bearing shown in FIG. 1. The same reference numerals as in FIG. The magnetic flux that comes out from the north pole and returns to the south pole passes through the rotating magnetic pole 2, separates in the vertical direction, and passes through the air gap to the thrust magnetic bearing magnets 3a, 3.
It flows into the iron core b, passes through the air gap again, reaches the rotating magnetic pole 2, and returns to the S pole. At a position (position in the thrust direction) where the air gap between the iron core of the electromagnet 3a and the rotating magnetic pole 2 (hereinafter referred to as the upper air gap) and the air gap between the iron core of the electromagnet 3b and the rotating magnetic pole 2 (hereinafter referred to as the lower air gap) are equal. If the rotor 1 exists, the magnitudes of the magnetic fluxes in the upper gap and the lower gap (consider only the magnetic flux shown by the solid line) are equal to each other, and the vertical (thrust direction) attractive forces acting on the rotor 1 are balanced. However, this equilibrium point is unstable, and if the rotor 1 moves downward even slightly, the attractive force due to the magnetic flux in the lower air gap becomes stronger, causing the rotor 1 to move further downward.
That is, the relationship between the position of the rotor 1 in the thrust direction and the attractive force by the permanent magnet 4 attached to the rotor 1 is a positive feedback relationship. So electromagnet 3
By controlling the suction forces of a and 3b, the relationship between the position of the rotor 1 and the total suction force is a negative feedback relationship, thereby stabilizing position control in the thrust direction.

ロータ1のスラスト方向の変位は2個の位置セ
ンサ7によつて検出され、変位によつて定まる電
気信号が発生され、位置センサ回路8、演算増幅
器9により2個の位置センサ7の出力が平均化さ
れ、位相補償回路10、電力増幅器11を経て電
磁石3a,3bのコイルを励磁する。電磁石3
a,3bにより発生する磁束は第2図に点線矢印
で示す方向に発生し、上部空隙では永久磁石4に
よる磁束(実線矢印)と加わり、下部空隙では永
久磁石4による磁束を減少させる。
The displacement of the rotor 1 in the thrust direction is detected by the two position sensors 7, an electric signal determined by the displacement is generated, and the outputs of the two position sensors 7 are averaged by the position sensor circuit 8 and the operational amplifier 9. It passes through a phase compensation circuit 10 and a power amplifier 11 to excite the coils of the electromagnets 3a and 3b. Electromagnet 3
The magnetic flux generated by a and 3b is generated in the direction shown by the dotted arrow in FIG. 2, and is added to the magnetic flux (solid arrow) by the permanent magnet 4 in the upper gap, and reduces the magnetic flux by the permanent magnet 4 in the lower gap.

したがつて、たとえばロータ1が下方へ動く
と、位置センサ7からの出力電圧が増加して電磁
石3a,3bにより発生する磁束が増加し、その
結果上部空隙の磁束は増加し下部空隙の磁束は減
少してロータ1は上方へ吸引され、このような負
帰還のフイードバツク制御によつてロータ1のス
ラスト方向の位置は所定の位置に保たれる。
Therefore, for example, when the rotor 1 moves downward, the output voltage from the position sensor 7 increases and the magnetic flux generated by the electromagnets 3a and 3b increases, and as a result, the magnetic flux in the upper air gap increases and the magnetic flux in the lower air gap increases. The rotor 1 is sucked upward, and the thrust direction position of the rotor 1 is maintained at a predetermined position by such negative feedback feedback control.

位相補償回路10は上述のフイードバツク制御
の特性を良好にするためのもので、たとえば、演
算増幅器9から変位に比例する電圧を入力して、
この変位に比例する電圧と変位の時間微分すなわ
ち速度に比例する電圧との和の電圧を作り電力増
幅器11に入力する。速度に比例する電圧が加算
された信号によつてフイードバツク制御が行われ
るとロータ1のスラスト方向の運動にダンピング
を与えることができる。
The phase compensation circuit 10 is for improving the characteristics of the above-mentioned feedback control. For example, by inputting a voltage proportional to the displacement from the operational amplifier 9,
A voltage that is the sum of the voltage proportional to this displacement and the time derivative of the displacement, that is, the voltage proportional to the speed is generated and input to the power amplifier 11. When feedback control is performed using a signal to which a voltage proportional to the speed is added, damping can be applied to the motion of the rotor 1 in the thrust direction.

次にロータ1のラジアル方向の変位に対して
は、リング状永久磁石4の吸引力によつて受動的
に復元力が働く。すなわち、磁極2に対向する電
磁石3a,3bの磁極がその対向位置から外れよ
うとすると、これを元の対向位置へ引き戻す力が
作用するのである。然しながら電磁石3a,3b
の磁極とこれに対向する磁極2との間に作用する
ラジアル方向の復元力では不充分なため、第1図
に示すようにロータ1の両端に磁極5bを設け、
これに対向して磁極5aをステータ6に設けてラ
ジアル磁気軸受を構成している。
Next, with respect to the displacement of the rotor 1 in the radial direction, a restoring force is passively exerted by the attractive force of the ring-shaped permanent magnet 4. That is, when the magnetic poles of the electromagnets 3a and 3b facing the magnetic pole 2 try to move away from their opposing positions, a force acts to pull them back to their original opposing positions. However, the electromagnets 3a and 3b
Since the restoring force in the radial direction that acts between the magnetic pole of
A magnetic pole 5a is provided on the stator 6 to form a radial magnetic bearing.

従来の磁気軸受制御装置は上述のように構成さ
れているので、ラジアル方向に対しては磁気吸引
力による復元力だけが働き、ダンピング力が作用
しないという欠点があつた。ロータ1のラジアル
方向の変位をx、時間をtとすれば、ロータ1の
ラジアル方向の運動は最も簡単には mdx/dt=−k1dx/dt−k2x…(1) によつて表すことができる。ここにm,k1,k2
それぞれ定数でmdx/dtはロータ1にラジアル
方向 の加速度を与える力、−k1dx/dtはロータ1の運動
に ダンピングを与える力、−k2xは磁気吸引力によ
る復元力である。第1図に示す構造では磁気吸引
力は復元力−k2xだけを発生させるが、ダンピン
グを与える力は発生させないため、上記の式(1)に
おける定数k1の値は比較的小さく、したがつて変
位xは振動的に変化し、ロータ1は定数mと定数
k2とで定められる周期で大きく振動し、この振動
の振幅を減衰させることが困難であるという欠点
を生じた。
Since the conventional magnetic bearing control device is configured as described above, it has the disadvantage that only the restoring force due to the magnetic attraction force acts in the radial direction, and no damping force acts. If the displacement of the rotor 1 in the radial direction is x and the time is t, then the movement of the rotor 1 in the radial direction is most simply md 2 x/dt 2 =-k 1 dx/dt-k 2 x...(1) It can be expressed by Here, m, k 1 and k 2 are each constant, md 2 x/dt 2 is the force that gives acceleration to the rotor 1 in the radial direction, -k 1 dx/dt is the force that gives damping to the motion of the rotor 1, -k 2 x is the restoring force due to magnetic attraction. In the structure shown in Figure 1, the magnetic attraction force generates only a restoring force -k 2 x, but does not generate a damping force, so the value of the constant k 1 in equation (1) above is relatively small and As a result, the displacement x changes vibrationally, and the rotor 1 has a constant m and a constant
The disadvantage is that it vibrates greatly at a period determined by k 2 and that it is difficult to dampen the amplitude of this vibration.

この発明は上記のような従来のものの欠点を除
去するためになされたもので、ロータ1のスラス
ト方向の運動とラジアル方向の運動を力学的に連
成させ、ラジアル方向の速度に比例する信号をも
スラスト磁気軸受制御装置にフイードバツクさせ
ることによつてラジアル方向にもダンピング力を
与えることができる磁気軸受制御装置を提供する
ことを目的としている。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and it dynamically couples the motion of the rotor 1 in the thrust direction and the radial direction, and generates a signal proportional to the speed in the radial direction. Another object of the present invention is to provide a magnetic bearing control device that can also apply damping force in the radial direction by providing feedback to the thrust magnetic bearing control device.

以下、この発明の実施例を図面により説明す
る。第3図はこの発明の一実施例を示すブロツク
図であつて、第1図と同一符号は同一又は相当部
分を示し、7aは第1図の7に相当する位置セン
サ、8aは第1図の8に相当する位置センサ回
路、9aは第1図の9に相当する演算増幅器で、
7a,8a,9aを綜合してスラスト位置センサ
装置と称し、7bは上部ラジアル方向位置セン
サ、7cは下部ラジアル方向位置センサで第1図
の位置センサ7に類似のものであり、8bは位置
センサ回路8aに類似の位置センサ回路、9bは
3入力演算増幅器、10a,10bはそれぞれ第
1図の10に相当する位相補償回路、12はセン
サ支持金物である。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 3 is a block diagram showing an embodiment of the present invention, in which the same reference numerals as in FIG. 1 indicate the same or corresponding parts, 7a is a position sensor corresponding to 7 in FIG. 9a is an operational amplifier corresponding to 9 in FIG.
7a, 8a, and 9a are collectively referred to as a thrust position sensor device, 7b is an upper radial direction position sensor, 7c is a lower radial direction position sensor, which is similar to the position sensor 7 in FIG. 1, and 8b is a position sensor. A position sensor circuit similar to the circuit 8a, 9b a three-input operational amplifier, 10a and 10b phase compensation circuits corresponding to 10 in FIG. 1, and 12 a sensor support hardware.

ロータ1のラジアル方向の運動とスラスト方向
の運動を連成させるため、ロータの重心を幾何学
的中心よりずらせてある。上部のラジアル磁気軸
受と下部のラジアル磁気軸受とのばね定数(式(1)
の定数k2)を互に相違させることによつてもラジ
アル方向の運動とスラスト方向の運動を連成させ
ることができる。
In order to couple the motion of the rotor 1 in the radial direction and the thrust direction, the center of gravity of the rotor is shifted from the geometric center. The spring constant of the upper radial magnetic bearing and the lower radial magnetic bearing (Equation (1)
The motion in the radial direction and the motion in the thrust direction can also be coupled by making the constants k 2 ) different from each other.

第3図の7b,7c,8bを総称してラジアル
位置センサ装置と称することにし、このラジアル
位置センサ装置の出力を位相補償回路10bで位
相補償した上で、演算増幅器9bを介してスラス
ト方向の制御ループにフイードバツクさせてい
る。これによりスラスト磁気軸受による磁気的な
ダンピング力を生じこれがラジアル方向の運動と
連成されてラジアル方向の運動に対するダンピン
グ力となりラジアル方向の振動を充分に減衰させ
る。
7b, 7c, and 8b in FIG. 3 are collectively referred to as a radial position sensor device, and the output of this radial position sensor device is phase-compensated by a phase compensation circuit 10b, and then sent to the thrust direction via an operational amplifier 9b. Feedback is provided to the control loop. This generates a magnetic damping force by the thrust magnetic bearing, which is coupled with the radial motion and becomes a damping force against the radial motion, sufficiently damping the radial vibration.

以上のように、この発明によればラジアル方向
の変位を表す電気信号をスラスト磁気軸受制御系
にフイードバツクさせてラジアル方向のダンピン
グ力を発生させるので、ラジアル方向のアクチユ
エータ(actuator)を別に設ける必要がなく、安
価で信頼性の高い装置を得ることができる。
As described above, according to the present invention, a damping force in the radial direction is generated by feeding back an electric signal representing displacement in the radial direction to the thrust magnetic bearing control system, so it is not necessary to separately provide an actuator in the radial direction. Therefore, an inexpensive and highly reliable device can be obtained.

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

第1図は従来の装置の一例を示すブロツク図、
第2図は第1図に示す装置の動作を示す説明図、
第3図はこの発明の一実施例を示すブロツク図で
ある。 1…ロータ、2…スラスト磁気軸受用回転磁
極、3a,3b…スラスト磁気軸受用電磁石、4
…リング状永久磁石、5a,5b…ラジアル磁気
軸受用磁極、6…ステータ、7a,7b,7c…
位置センサ、8a,8b…位置センサ回路、9
a,9b…演算増幅器、10a,10b…位相補
償回路。なお、図中同一符号は同一又は相当部分
を示す。
FIG. 1 is a block diagram showing an example of a conventional device.
FIG. 2 is an explanatory diagram showing the operation of the device shown in FIG. 1;
FIG. 3 is a block diagram showing one embodiment of the present invention. 1... Rotor, 2... Rotating magnetic pole for thrust magnetic bearing, 3a, 3b... Electromagnet for thrust magnetic bearing, 4
...Ring-shaped permanent magnet, 5a, 5b...Magnetic pole for radial magnetic bearing, 6...Stator, 7a, 7b, 7c...
Position sensor, 8a, 8b...Position sensor circuit, 9
a, 9b... operational amplifier, 10a, 10b... phase compensation circuit. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] 1 軸のまわりに回転するロータをステータに対
し所定の関係位置に機械的な接触部なしに磁気軸
受により支持するよう制御する磁気軸受制御装置
において、上記ロータの上記ステータに対するス
ラスト方向の変化によつて定まる電気信号を検出
するスラスト位置センサ装置と、このスラスト位
置センサ装置の出力を位相補償して増幅したスラ
スト位置制御出力により上記磁気軸受のスラスト
磁気軸受用電磁石を制御して上記スラスト方向の
位置をフイードバツク制御する手段と、上記ロー
タの上記ステータに対するラジアル方向の変位に
よつて定まる電気信号を検出するラジアル位置セ
ンサ装置と、このラジアル位置センサ装置の出力
を位相補償して増幅した出力を上記スラスト位置
制御出力に加えて上記スラスト磁気軸受用電磁石
を制御し上記ラジアル方向の運動に対する制動を
与える手段とを備えたことを特徴とする磁気軸受
制御装置。
1. In a magnetic bearing control device that controls a rotor rotating around an axis to be supported by a magnetic bearing at a predetermined relative position with respect to a stator without mechanical contact, a change in the thrust direction of the rotor with respect to the stator a thrust position sensor device that detects an electric signal determined by a radial position sensor device for detecting an electric signal determined by the radial displacement of the rotor with respect to the stator; A magnetic bearing control device characterized by comprising means for controlling the thrust magnetic bearing electromagnet and applying braking to the movement in the radial direction in addition to a position control output.
JP5940281A 1981-04-20 1981-04-20 Controller for magnetic bearing Granted JPS57173614A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5940281A JPS57173614A (en) 1981-04-20 1981-04-20 Controller for magnetic bearing

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5940281A JPS57173614A (en) 1981-04-20 1981-04-20 Controller for magnetic bearing

Publications (2)

Publication Number Publication Date
JPS57173614A JPS57173614A (en) 1982-10-26
JPS6237246B2 true JPS6237246B2 (en) 1987-08-11

Family

ID=13112242

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5940281A Granted JPS57173614A (en) 1981-04-20 1981-04-20 Controller for magnetic bearing

Country Status (1)

Country Link
JP (1) JPS57173614A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0198708A (en) * 1987-10-07 1989-04-17 Ebara Res Co Ltd Radial magnetic bearing device

Also Published As

Publication number Publication date
JPS57173614A (en) 1982-10-26

Similar Documents

Publication Publication Date Title
US4036565A (en) Pump construction
US4585282A (en) Magnetic levitation system
US4167296A (en) Protective control system for magnetic suspension and magnetically suspended devices
JP3068834B2 (en) Radial and axial bearings for rotors with large radii
US4983869A (en) Magnetic bearing
JPH08505826A (en) Direct torque control moment gyroscope
JPH06288431A (en) Vibration resistant device
US20130207496A1 (en) System and method for performing magnetic levitation in an energy storage flywheel
JPS6237246B2 (en)
JPH08322194A (en) Axial magnetic levitation motor and rotating machine employing it
JP3712519B2 (en) Disc type bearingless rotating machine
EP0378678A1 (en) Electromagnetic bearings.
JPS58137618A (en) Magnetic bearing
JPH0788875B2 (en) Vibration control device
JPH0686576A (en) Electromagnetic actuator
JP2668476B2 (en) Anti-vibration device
JP2519537Y2 (en) Magnetic bearing control circuit
JP2546997B2 (en) Non-contact support method
JP2897416B2 (en) Anti-vibration device
JPH06294444A (en) Vibration resisting device
JP2001295842A (en) Magnetic bearing device
Mizuno et al. Repulsive magnetic bearing stabilized by the motion control of magnets with a piezoelectric actuator
JPH04337112A (en) Damping mechanism for magnetic bearing
JPS58136600A (en) Magnetic bearing flywheel for artificial satellite
JP2579519B2 (en) Magnetic bearing control device with resonance suppression function