WO2012154066A1 - Magnetic bearing and magnetic bearing mode of action - Google Patents
Magnetic bearing and magnetic bearing mode of action Download PDFInfo
- Publication number
- WO2012154066A1 WO2012154066A1 PCT/PL2012/000027 PL2012000027W WO2012154066A1 WO 2012154066 A1 WO2012154066 A1 WO 2012154066A1 PL 2012000027 W PL2012000027 W PL 2012000027W WO 2012154066 A1 WO2012154066 A1 WO 2012154066A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- rings
- magnetic
- magnets
- magnetic bearing
- bearing
- Prior art date
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
- F16C32/0408—Passive magnetic bearings
- F16C32/0423—Passive magnetic bearings with permanent magnets on both parts repelling each other
- F16C32/0429—Passive magnetic bearings with permanent magnets on both parts repelling each other for both radial and axial load, e.g. conical magnets
-
- 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
- F16C32/0408—Passive magnetic bearings
- F16C32/0423—Passive magnetic bearings with permanent magnets on both parts repelling each other
- F16C32/0427—Passive magnetic bearings with permanent magnets on both parts repelling each other for axial load mainly
Definitions
- This invention relates to magnetic bearing, which stabilizes the rotation of rotating machine parts using neodymium magnets at the same time in radial and axial direction.
- the invention applies in particular to the oscillating and vibrating machinery, tank stirrers, horizontal transport systems, such as conveyor belts, conveyors, spiral feeders, rotating machines motors, generators, turbines, pumps and compressors, both in chemically aggressive, dirty, humid or dusty enviroment.
- magnetic bearings where the sources of the levitating interactions are dynamic effects of magnetic forces emanating from the electromagnets called electromagnetic actuators.
- electromagnetic actuators In such systems, a distinction is made independently axial controlled magnetic bearings (parallel to the axis of the rotor) and radial controlled magnetic bearings (perpendicular to the axis of the rotor).
- axial controlled magnetic bearings parallel to the axis of the rotor
- radial controlled magnetic bearings perpendicular to the axis of the rotor
- the essence of magnetic bearing solutions according to the invention lies in its structure, consisting of two components of mobile and stationary one, arranged alternately, which are characterized by opposite polarization vectors and are equipped with magnetic rings 3 and 4, built from group of points magnets of any section or full magnets in the shape of rings or ring segments, which interact with each other preferably in places where the magnetic field lines have the opposite turn.
- the essence of the mode of action of the magnetic bearing according to the invention is the combination of many separate and opposite arrangement of magnetic fields, mobile and stationary, as shown in Figure 4A, into one coherent rotating magnetic field system, as shown in Figure 4B, where there is mutual centering mobile magnetic systems relative to stationary magnetic systems, as a result of new waveforms generated magnetic field lines, the distance h between the axis of the rings 3 and axis of the rings 4 is between 0.5 a ⁇ h ⁇ 1.5 a, where a is the width of the rings 3 and rings 4, as shown in Figure 4 A and Figure 4B.
- Figure 1A shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single stationary magnetic ring formed from a series of magnet points in the shape of a cylinder and two mobile systems built from a single magnetic ring, also created from a series of point magnets in the shape of a cylinder.
- Figure IB shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single stationary magnetic ring formed from a series of point magnets in the shape of a trapezoid and two mobile systems built from a single magnetic ring, also created from a series of point magnets in the shape of a trapezoid.
- Figure ID shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single stationary magnetic ring formed from a segments of one annular magnet and two mobile systems built from a single magnetic ring, also formed from a segments of one annular magnet.
- Figure IE shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single stationary magnetic ring formed from a series of point magnets in the shape of a cylinder and two mobile systems built from a single magnetic ring formed from from one whole annular magnet.
- Figure 2 shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single mobile magnetic ring formed from a series of point magnets in the shape of a cylinder and two stationary systems built from a single magnetic ring, also created from a series of point magnets in the shape of a cylinder.
- Figure 3 shows in isometric view the assembly of an exemplary magnetic bearing system, built from a dual stationary magnetic rings formed from a series of point magnets in the shape of a cylinder and two mobile systems built from a dual magnetic rings, also created from a series of point magnets in the shape of a cylinder.
- Figure 4A shows a schematic cross-sectional view of magnetic field lines before the magnetic merger of mobile and stationary parts
- Figure 4B shows a schematic cross-sectional view of magnetic field lines after the magnetic merger of mobile and stationary parts corresponding to the arrangement in working status.
- Preferred features of the bearing of the invention are simple design and extended the life of the bearings due to lack of friction, as well as vibration damping of the rotating machine parts such as engines, rotors and generators, compressors and pumps, rotors, and the rotating centrifuge parts, gears, etc.
- the technical advantage of the invention is any scale of the point neodymium magnets, and any number of rings of this magnets, which are characteristics directly affect the strength of the magnetic bearing. No friction, no lubricant medium and the opportunity to work in any environment make the applicability of the bearings according to the invention are extremely versatile.
Abstract
This invention relates to magnetic bearing and magnetic bearing mode of action, stabilizing the rotation of rotating machine parts using neodymium magnets both in radial and axial direction, the bearing is composed of one stationary mounting component 1 and the two rotating components 2, wherein components 1 and 2 are equipped with magnetic rings 3 and 4 and are constructed from a series of point magnets of any section or full magnets in the shape of ring segments, and the polarization components 1 and 2 are opposed, in the bearing there is a mutual centering mobile magnetic systems relative to stationary magnetic systems as a result of new waveforms generated magnetic field lines, and the distance h between the axis of the rings 3 and axis of the rings 4 is between 0.5 a < h < 1.5 a, where a is the width of the rings 3 and rings 4.
Description
Magnetic bearing and magnetic bearing mode of action.
This invention relates to magnetic bearing, which stabilizes the rotation of rotating machine parts using neodymium magnets at the same time in radial and axial direction.
The invention applies in particular to the oscillating and vibrating machinery, tank stirrers, horizontal transport systems, such as conveyor belts, conveyors, spiral feeders, rotating machines motors, generators, turbines, pumps and compressors, both in chemically aggressive, dirty, humid or dusty enviroment.
There are examples of magnetic bearings, where the sources of the levitating interactions are dynamic effects of magnetic forces emanating from the electromagnets called electromagnetic actuators. In such systems, a distinction is made independently axial controlled magnetic bearings (parallel to the axis of the rotor) and radial controlled magnetic bearings (perpendicular to the axis of the rotor). Thus constructed systems are unstable and in need of an external control system to stabilize the position of a rotating object.
Such solutions are based on a completely different method of action than the object of the invention, they need the continuous power and as such are not taken into account for the present state of the art.
It is also known from patent specification EN 20 832, ball bearing lubricated with magnetic fluid, which is mounted on the spherical shaft pin (1), adjacent to the acetabulum (3), preferably porous, saturated liquid density (7) placed in the housing (5) and separating the pin from the permanent magnet (4) located in the socket housing, with both sides of the magnet and the acetabulum are multi-edge pole pieces (6) is also embedded in the socket housing. Magnetic fluid, located in the gaps formed between the surface of the spigot and performances polepieces a bearing seal and the fluid at the contact of the shaft and the acetabulum is a lubricating layer.
There are also examples of passive magnetic bearings, the source of impacts on the levitating object are static interaction of magnetic forces of permanent magnets, especially neodymium. It is also known patent number of solutions, which contain solutions with permanent magnets as a source of influence, but different in its construction in comparison to the invention.
Analyzed in detail publications: JP 7123634, U.S. 5495221, WO 9716882, U.S. 5831362, U.S. 5894181, U.S. 61 18199, WO 0184693, U.S. 2002047404, U.S. 200207488. Analysis of the above publications did not show similar solutions to the invention in terms of spatial design solutions. The main difference between the invention and the above solutions concerns the mode of action of the magnetic bearing.
In the bearing according to the invention there is a group of points magnetic fields, which center and stabilize the rotating central magnetic field. Thus, controlling the position of the rotor is followed spontaneously only through preferred potentials of the mobile and immobile magnetic fields, which also tend to seek the lowest energy state, which provides a centering and stabilization of a rotating central magnetic field.
The essence of magnetic bearing solutions according to the invention lies in its structure, consisting of two components of mobile and stationary one, arranged alternately, which are characterized by opposite polarization vectors and are equipped with magnetic rings 3 and 4, built from group of points magnets of any section or full magnets in the shape of rings or ring segments, which interact with each other preferably in places where the magnetic field lines have the opposite turn.
The essence of the mode of action of the magnetic bearing according to the invention is the combination of many separate and opposite arrangement of magnetic fields, mobile and stationary, as shown in Figure 4A, into one coherent rotating magnetic field system, as shown in Figure 4B, where there is mutual centering mobile magnetic systems relative to stationary magnetic systems, as a result of new waveforms generated magnetic field lines, the distance h between the axis of the rings 3 and axis of the rings 4 is between 0.5 a < h < 1.5 a, where a is the width of the rings 3 and rings 4, as shown in Figure 4 A and Figure 4B.
The invention has been visualized in the accompanying drawings in the embodiments, in which:
Figure 1A shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single stationary magnetic ring formed from a series of magnet points in the shape of a cylinder and two mobile systems built from a single magnetic ring, also created from a series of point magnets in the shape of a cylinder.
Figure IB shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single stationary magnetic ring formed from a series of point magnets in the shape of a trapezoid and two mobile systems built from a single magnetic ring, also created from a series of point magnets in the shape of a trapezoid.
Figure ID shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single stationary magnetic ring formed from a segments of one annular magnet and two mobile systems built from a single magnetic ring, also formed from a segments of one annular magnet.
Figure IE shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single stationary magnetic ring formed from a series of point magnets in the shape of a cylinder and two mobile systems built from a single magnetic ring formed from from one whole annular magnet.
Figure 2 shows in isometric view the assembly of an exemplary magnetic bearing system, built from a single mobile magnetic ring formed from a series of point magnets in the shape of a cylinder and two stationary systems built from a single magnetic ring, also created from a series of point magnets in the shape of a cylinder.
Figure 3 shows in isometric view the assembly of an exemplary magnetic bearing system, built from a dual stationary magnetic rings formed from a series of point magnets in the shape of a cylinder and two mobile systems built from a dual magnetic rings, also created from a series of point magnets in the shape of a cylinder.
Figure 4A shows a schematic cross-sectional view of magnetic field lines before the magnetic merger of mobile and stationary parts,
Figure 4B shows a schematic cross-sectional view of magnetic field lines after the magnetic merger of mobile and stationary parts corresponding to the arrangement in working status.
Preferred features of the bearing of the invention are simple design and extended the life of the bearings due to lack of friction, as well as vibration damping of the rotating machine parts such as engines, rotors and generators, compressors and pumps, rotors, and the rotating centrifuge parts, gears, etc.
The technical advantage of the invention is any scale of the point neodymium magnets, and any number of rings of this magnets, which are characteristics directly affect the strength of the magnetic bearing. No friction, no lubricant medium and the opportunity to work in any environment make the applicability of the bearings according to the invention are extremely versatile.
Claims
1. Magnetic bearing with magnets, characterized in that it is composed of one stationary mounting component 1 and two mobile rotating components 2, the components 1 and 2 are equipped with magnetic rings 3 and 4, which are constructed from a series of point magnets of any section or full magnets in the shape of rings or slices.
2. Magnetic bearing with magnets, characterized in that it is composed of two stationary mounting components 1 and one mobile rotating component 2, the components 1 and 2 are equipped with magnetic rings 3 and 4, which are constructed from a series of point magnets of any section or full magnets in the shape of rings or slices.
3. Magnetic bearing of claim 1, 2, characterized in that the rings are shaped of the uniform magnetic rings.
4. Magnetic bearing of claim 1, 2, characterized in that the rings are shaped of the magnetic ring segments.
5. Magnetic bearing of claim 1, 2, characterized in that the rings are shaped of the points magnets of any cross-section.
6. Magnetic bearing of claim 1, 2, characterized in that the magnetic rings are in the form of mixed systems consisting of a single ring or ring segments or points magnets of any cross-section.
7. Magnetic bearing of claim 1, 2, characterized in that the components 1 and 2 have any number of rings 3 and 4, the polarization of all rings 3 mounted on the component 1 and all rings 4 mounted on the component 2 are identical.
8. Magnetic bearing according to claim 1, 2, characterized in that the polarization components 1 and 2 are the opposite.
9. The magnetic bearing mode of action according to the invention is characterized in that in the bearing multiple separate and opposed magnetic systems are connected into one coherent magnetic system, where there is a mutual centering mobile magnetic systems relative to stationary magnetic systems as a result of new waveforms generated magnetic field lines, and the distance h between the axis of the rings 3 and axis of the rings 4 is between 0.5 a < h <1.5 a, where a is the width of the rings 3 and rings 4.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
PLP.394800 | 2011-05-06 | ||
PL394800A PL394800A1 (en) | 2011-05-06 | 2011-05-06 | Magnetic bearing and magnetic bearing mode of action |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2012154066A1 true WO2012154066A1 (en) | 2012-11-15 |
Family
ID=46321425
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/PL2012/000027 WO2012154066A1 (en) | 2011-05-06 | 2012-04-30 | Magnetic bearing and magnetic bearing mode of action |
Country Status (2)
Country | Link |
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PL (1) | PL394800A1 (en) |
WO (1) | WO2012154066A1 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
IT201600069910A1 (en) * | 2016-07-05 | 2018-01-05 | Spinning Top Energy S R L | FLYWHEEL ACCUMULATOR |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
PL423034A1 (en) * | 2017-10-02 | 2019-04-08 | Artur Łukasiewicz | Magnetic bearing |
Citations (14)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE2116686A1 (en) * | 1971-04-06 | 1972-10-19 | Doerfler G | Magnet bearings |
JPS5536635A (en) * | 1978-09-04 | 1980-03-14 | Sumitomo Special Metals Co Ltd | Magnetic bearing |
JPS6353315A (en) * | 1986-08-20 | 1988-03-07 | Secoh Giken Inc | Bearing device for rotary shaft |
JPH01204211A (en) * | 1988-02-09 | 1989-08-16 | Hitachi Ltd | Revolving head device |
JPH0293119A (en) * | 1988-09-29 | 1990-04-03 | Fuji Elelctrochem Co Ltd | Magnetic bearing device |
JPH07123634A (en) | 1993-10-20 | 1995-05-12 | Mitsubishi Heavy Ind Ltd | Passive-type magnetic bearing |
US5495221A (en) | 1994-03-09 | 1996-02-27 | The Regents Of The University Of California | Dynamically stable magnetic suspension/bearing system |
WO1997016882A1 (en) | 1995-11-03 | 1997-05-09 | The Regents Of The University Of California | Passive magnetic bearing element with minimal power losses |
US5831362A (en) | 1994-11-01 | 1998-11-03 | The University Of Houston | Magnet-superconductor flywheel and levitation systems |
US5894181A (en) | 1997-07-18 | 1999-04-13 | Imlach; Joseph | Passive magnetic bearing system |
US6118199A (en) | 1997-01-28 | 2000-09-12 | Magnetal Ab | Magnetic bearings |
WO2001084693A1 (en) | 2000-05-01 | 2001-11-08 | Indigo Energy, Inc. | Full levitation bearing system with improved passive radial magnetic bearings |
US20020007488A1 (en) | 2000-06-19 | 2002-01-17 | Dan Kikinis | Transparent object management for removable media recorders |
US20020047404A1 (en) | 2000-07-04 | 2002-04-25 | Norbert Coenen | Rotor spinning device with a contactless, passive, radial bearing for the spinning rotor |
-
2011
- 2011-05-06 PL PL394800A patent/PL394800A1/en not_active Application Discontinuation
-
2012
- 2012-04-30 WO PCT/PL2012/000027 patent/WO2012154066A1/en active Application Filing
Patent Citations (14)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE2116686A1 (en) * | 1971-04-06 | 1972-10-19 | Doerfler G | Magnet bearings |
JPS5536635A (en) * | 1978-09-04 | 1980-03-14 | Sumitomo Special Metals Co Ltd | Magnetic bearing |
JPS6353315A (en) * | 1986-08-20 | 1988-03-07 | Secoh Giken Inc | Bearing device for rotary shaft |
JPH01204211A (en) * | 1988-02-09 | 1989-08-16 | Hitachi Ltd | Revolving head device |
JPH0293119A (en) * | 1988-09-29 | 1990-04-03 | Fuji Elelctrochem Co Ltd | Magnetic bearing device |
JPH07123634A (en) | 1993-10-20 | 1995-05-12 | Mitsubishi Heavy Ind Ltd | Passive-type magnetic bearing |
US5495221A (en) | 1994-03-09 | 1996-02-27 | The Regents Of The University Of California | Dynamically stable magnetic suspension/bearing system |
US5831362A (en) | 1994-11-01 | 1998-11-03 | The University Of Houston | Magnet-superconductor flywheel and levitation systems |
WO1997016882A1 (en) | 1995-11-03 | 1997-05-09 | The Regents Of The University Of California | Passive magnetic bearing element with minimal power losses |
US6118199A (en) | 1997-01-28 | 2000-09-12 | Magnetal Ab | Magnetic bearings |
US5894181A (en) | 1997-07-18 | 1999-04-13 | Imlach; Joseph | Passive magnetic bearing system |
WO2001084693A1 (en) | 2000-05-01 | 2001-11-08 | Indigo Energy, Inc. | Full levitation bearing system with improved passive radial magnetic bearings |
US20020007488A1 (en) | 2000-06-19 | 2002-01-17 | Dan Kikinis | Transparent object management for removable media recorders |
US20020047404A1 (en) | 2000-07-04 | 2002-04-25 | Norbert Coenen | Rotor spinning device with a contactless, passive, radial bearing for the spinning rotor |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
IT201600069910A1 (en) * | 2016-07-05 | 2018-01-05 | Spinning Top Energy S R L | FLYWHEEL ACCUMULATOR |
WO2018007931A1 (en) * | 2016-07-05 | 2018-01-11 | Spinning Top Energy S.R.L. | Flywheel kinetic accumulator |
US20190312482A1 (en) * | 2016-07-05 | 2019-10-10 | Spinning Top Energy S.R.L. | Flywheel kinetic accumulator |
US10804767B2 (en) | 2016-07-05 | 2020-10-13 | Spinning Top Energy S.R.L. | Flywheel kinetic accumulator |
Also Published As
Publication number | Publication date |
---|---|
PL394800A1 (en) | 2012-11-19 |
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