No federal funds were used to develop or create the invention disclosed and described in the patent application.
Not Applicable
Active magnetic bearing technology provides for the support of a machine rotor by means of the force of electromagnetic attraction between stator and rotor components constructed of ferromagnetic materials through which magnetic circuits are created by electrical coils. One example of an active magnetic bearing is disclosed in U.S. Pat. No. 5,111,102, which is incorporated by reference herein in its entirety. This force of attraction is quite different from the principle of all mechanical bearings that react loads by pushing against them. While mechanical bearings act to repulse loads, magnetic bearings may operate by attracting loads by acting from the opposite side of the rotor.
A ferromagnetic structure is typically required for both the stator and rotor components; typically this is in the form of standard electrical steel lamination packs. These may be oriented in the transverse plane of the rotor for radial bearings. For axial bearings the lamination packs may be oriented in the longitudinal direction of the rotor. The magnetic circuits are developed by the flow of electrical current in coils mounted around the magnetic cores.
Present state of the art for magnetic bearing technology requires enveloping the rotor completely by magnetic circuits of alternating polarity. This not only allows the largest load capacity to be developed, but it also provides for linearization of the relationship between the bearing force developed and the rotor displacement in the gap between rotor and stator. Linearization may allow for the use of less sophisticated controls for practical implementation.
In the case of a radial magnetic bearing 16a, the conventional arrangement commonly dictates that the machine rotor is usually enveloped by the radial magnetic bearing 16a over a full 360°. This type of configuration is shown generally in the foreground of
Disadvantages of these pure electromagnetic designs include the large space that these bearings occupy inside the machine, and the associated cost of building these large bearings 16a, 16b and their associated power electronics. The large space requirement is more than just a penalty in machine size. Large bearings 16a, 16b increase the span between the machine bearings supporting a rotor, which increase is almost always a detrimental effect on the rotor dynamics because the resultant rotor natural frequencies (critical speeds) are often located in the operating speed range causing excessive machine vibration. In the worst scenarios this can mean a complete inability to operate the machine.
Another disadvantage of pure magnetic bearing 16a, 16b designs is the relatively low stiffness of the magnetic suspension created by the bearings 16a, 16b at high frequencies of excitation. This often limits the ability of the magnetic bearing 16a, 16b system to control the placement of critical speeds to push them out of the operating speed range of the machine rotor.
Finally, these conventional designs typically lack any type of redundancy or overload protection and a separate auxiliary bearing must also be employed to protect the rotor and machine internals in the event of magnetic bearing 16a, 16b failure or overload. This auxiliary bearing is typically some type of mechanical bearing, which requires additional space and cost.
Tilting pad journal bearings are another type of bearing commonly found in the prior art that may be configured as a magnetic bearing 16a, 16b. Generally, tilting pad journal bearings may employ an array of bearing pads mounted adjacent some type of rotor. The bearing pads may be biased toward the rotor. One specific type of tilting pad journal bearing is disclosed in U.S. Pat. No. 7,611,286, which is incorporated by reference herein in its entirety.
Air bearings are another type of bearing commonly found in the prior art. Generally, air bearings may utilize a thin film of pressurized air to provide a load-bearing interface between surfaces. As such, air bearings are typically non-contacting bearings. One specific type of non-contacting porous air bearing is disclosed in U.S. Pat. No. 7,908,885 as well as U.S. application Ser. No. 13/733,806, and another air bearing is disclosed in U.S. Pat. No. 8,517,665, all of which are incorporated by reference herein in their entireties.
A perspective view of a first illustrative embodiment of a radial magnetic bearing 16a (foreground) and a first illustrative embodiment of an axial magnetic bearing 16b (background) is shown in
In order that the advantages of the invention will be readily understood, a more particular description of the invention briefly described above will be rendered by reference to specific embodiments illustrated in the appended drawings. Understanding that these drawings depict only typical embodiments of the invention and are not therefore to be considered limited of its scope, the invention will be described and explained with additional specificity and detail through the use of the accompanying drawings.
Before the various embodiments of the present invention are explained in detail, it is to be understood that the invention is not limited in its application to the details of construction and the arrangements of components set forth in the following description or illustrated in the drawings. The invention is capable of other embodiments and of being practiced or of being carried out in various ways. Also, it is to be understood that phraseology and terminology used herein with reference to device or element orientation (such as, for example, terms like “front”, “back”, “up”, “down”, “top”, “bottom”, and the like) are only used to simplify description of the present invention, and do not alone indicate or imply that the device or element referred to must have a particular orientation. In addition, terms such as “first”, “second”, and “third” are used herein and in the appended claims for purposes of description and are not intended to indicate or imply relative importance or significance.
Referring now to the drawings, wherein like reference numerals designate identical or corresponding parts throughout the several view,
In the illustrative embodiment of the radial hybrid bearing 10 and the axial hybrid bearing 10′, the gas bearing portion(s) and the magnetic bearing portion(s) may be configured to occupy the same axial space, and thereby provide dual functionality augmenting each other. This scheme may be employed to facilitate a measure of bearing redundancy; if one bearing type fails (gas or magnetic), the remaining bearing may still provide for continuous operation, albeit at a likely higher vibration level. Such redundancy may require a change in the magnetic bearing control algorithm in the event of a gas bearing failure. In the event of a magnetic bearing failure the gas bearing clearance may be automatically adjusted to compensate for the lack of magnetic bearing support as the rotor seeks a new equilibrium position with respect to the bearing pads supported on their individual spring supports, thereby effectively changing the bore of the bearing 10, 10′. Thus, the hybrid bearings 10, 10′ may provide an intrinsic auxiliary bearing functionality. Protection against large overloads may be enabled with a simple bump stop constructed of self-lubricating materials, many of which bump stops are known to those of ordinary skill in the art and will not be described further herein.
Whereas there are several types of gas bearings operating on both hydrostatic and hydrodynamic operating principles, the type that may most readily integrate with magnetic bearing technology is the porous air bearing, a type of hydrostatic gas bearing. These bearings may be comprised of several discrete bearing pads 23, 23′.
As shown in
An illustrative bearing pad 23′ that may be used with certain embodiments of an axial hybrid bearing 10′ is shown in
The bearing pads 23, 23′ for use with porous air bearings are typically constructed of a porous carbon or similar media, wherein all but the active bearing surface (active surface 23a, 23a′) is typically sealed to retain internal gas pressure. Surfaces other than the active surface 23a, 23′ are referred to herein as sealed surfaces 23b, 23b′. Special compounds are used in the porous air bearing industry to provide this sealing capability. Clean pressurized air or gas may be introduced through a port 23d in a sealed surface 23b, 23b′ and naturally flows to the active surface 23a, 23a′ where it encounters the rotor 30, 30′ and reacts the load of the bearing. Any suitable compressed fluid source may be used to supply pressurized gas/air to the bearing pads 23, 23′, and the scope of the hybrid bearing 10, 10′ is in no way limited by the structure and/or method used for the compressed fluid source.
The pressurized air or gas may be supplied to each bearing pad 23, 23′ via any suitable conduit, and may enter the porous media at any suitable location. For example, in one embodiment the pressurized air or gas enters the bearing pad 23, 23′ on the side thereof. In another embodiment the pressurized air or gas enters the bearing pad 23, 23′ through a conduit formed in the post 25. Accordingly, the hybrid bearings 10, 10′ disclosed herein are in no way limited by the location and/or structure employed to deliver pressurized gas or air to a bearing pad 23, 23′. The mating rotor 30, 30′ component is typically a finely machined solid steel surface that is engaged with the shaft 12. However, the typical rotor 30, 30′ of a conventional radial magnetic bearing (which is often configured as a sleeve) with tightly packed laminations also may suffice, such as the radial bearing rotor 30 shown in
In order to coordinate stable rotor 30, 30′ position control with the magnetic bearing controller, and simultaneously limit the gas/air consumption to that only required for rotor 30, 30′ support and hybrid bearing 10, 10′ cooling, the clearance of the active surface 23a, 23a′ in a gas sector 22, 22′ with respect to the rotor 30, 30′ surface may be controlled to just a few microns statically. When gas pressure is applied to the hybrid bearing 10, 10′, the high gas-film stiffness may overcome the stiffness of the structure that supports the bearing pad 23, 23′, which may cause the bearing pads 23, 23′ to back away from the rotor 30, 30′ surface to develop a full film at a stable equilibrium position with respect to the rotor 30, 30′. The running clearance of the gas sectors 22, 22′ may be substantially less than the clearance of the magnetic sectors 24, 24′. Accordingly, the bearing pads 23, 23′ may be proud relative to the magnetic sectors 24, 24′. This configuration is best shown for the embodiment of an axial bearing stator 20′ shown in
The coil 26′, which provides the magnetic field via an electric current, may be configured such that it forms one or more complete circles within the axial bearing stator 20′, as best shown in
The volumetric flow rate requirement for the gas sector(s) 22, 22′ may be very low because of the tight clearance between the bearing pads 23, 23′ and the rotor 30, 30′ even after pressurization. Additionally, the difference in clearances between the rotor 30 and the magnetic sector(s) 24, and between the rotor 30 and gas sector(s) 22 may often require that the radius of curvature of the bearing pad(s) 23 be different than that of the magnetic sectors 24 for a radial hybrid bearing 10.
The number and size of bearing pads 23, 23′ may be dictated by the rotor 30, 30′ size and the load on the bearing 10, 10′. Usually about 50% of the supply pressure of the air/gas to the bearing pad 23, 23′ can be recovered as useful bearing surface loading to counteract loads. In the herein disclosed hybrid bearings 10, 10′, the supply air or gas may not only used to supply the bearing “muscle”, but also may supply a ready means of cooling the hybrid bearings 10, 10′ (and specifically the magnetic sectors 24, 24′ thereof) by dissipating heat generated in the bearing gap between the rotor 30, 30′ and stator 20, 20′. In such a configuration, the temperature of the gas increases as it passes the hybrid bearing 10, 10′ surfaces and is exhausted outside the bearing compartment.
The gas bearing film stiffness may be much higher than the stiffness of the magnetic sectors 24, 24′ at all frequencies above zero (static conditions), but even this high film stiffness may be incapable of preventing momentary contact between the rotor 30, 30′ and the active surface 23a, 23a′ of the gas bearing pad 23, 23′ during upset conditions. Generally, it may be desirable to prevent and/or mitigate hard rotor 30, 30′ contact (impact) with the active surface 23a, 23a′ due to the low compressive strength of the porous material in many bearing pads 23, 23′. In addition, the high coefficient of friction of the porous material in the bearing pads 23, 23′ may give rise to adverse rotor 30, 30′ behavior (e.g. shaft whirl) upon contact.
To ameliorate hard contact conditions between the rotor 30, 30′ and the bearing pads 23, 23′, spring mounting of the bearing pads 23, 23′ may be used on the back side of the bearing pads 23, 23′, usually with one or more posts that engage a ball-and-socket connection. Importantly, this spring mounting also may be used to ensure the coordination of rotor 30, 30′ position control with the magnetic bearing controller as well as allowing/providing the proper amount of hybrid bearing 10, 10′ cooling flow as discussed above. Therefore, the spring mounting requires a proper selection of the gas bearing support spring deflection vs. force characteristic to allow the development of a stable gas film that properly works in conjunction with the magnetic sectors 24, 24′; Belleville springs are good candidates for this. However, often a trial-and-error method may be required to properly balance the support spring deflection vs. force characteristic for a given hybrid bearing 10, 10′ and/or application thereof. A hard bump stop may be included to limit maximum rotor 30, 30′ motion while preventing contact of the other rotor 30, 30′ and stator 20, 20′ components. This bump stop can be a short axial length bushing of self-lubricating material for radial hybrid bearing 10 designs. For axial hybrid bearing 10′ designs, sectors of an axial bearing rotor 30′ thrust washer constructed of self-lubricating materials may be needed. However, any other structure and/or method to mitigate hard contact between the rotor 30, 30′ and bearing pads 23, 23′ may be used without limitation.
The first illustrative embodiment of a radial hybrid bearing 10 design for a machine with a horizontal rotor may be to place active magnetic bearing coils 26 in the upper quadrants (magnetic sector 24) of the radial bearing stator 20 and use gas bearing pads 23 in the lower 180° segment (gas sector 22) of the radial hybrid bearing 10 to lift the radial bearing rotor 30, a configuration which is shown in the illustrative embodiment from an axial perspective in
Both the gas sectors 22 and magnetic sectors 24 of the radial bearing stator may feature an interface with a conventional radial magnetic bearing rotor 30, which radial bearing rotor 30 may be comprised of tightly packed electrical steel laminations as best shown in
An illustrative embodiment of an axial hybrid bearing 10′ (which may be configured as a thrust bearing) having a horizontal axial bearing rotor 30′ orientation is shown in
In a machine with a vertically oriented rotor, the radial side loads are markedly less than in a horizontal configuration, but the axial hybrid bearing 10′ may be configured to react the entire static load. Accordingly, the shaft weight may be reacted by a multitude of properly sized gas bearing pads 23′ underneath a thrust collar (axial bearing rotor 30′). The upper side of the axial hybrid bearing 10′ in such a configuration may be occupied by a magnetic bearing and/or one or more magnetic sectors 24′ sized to assist the lower gas bearing and/or gas sectors 22′, particularly by reacting dynamic loads via its capability to develop a force of attraction at high frequency. Magnetic bearing coils 26′ may or may not be used on the lower axial bearing stator 20′ according to the application requirements. Where both an axial hybrid bearing 10′ and radial hybrid bearing 10 occupy the same space, the axial bearing stator 20′ may be sectioned into gas sectors 22′ and magnetic sectors 24′ to accommodate gas bearing pads 23′ that run from the basic hybrid bearing 10′ ID to the hybrid bearing 10′ OD, while the coils 26′ for the magnetic sectors 24′ may be retained in their full annular 360° form as best shown in
A radial hybrid bearing 10 may also provide advantages over the prior art in machines with vertically oriented rotors. One such advantage is a decrease in size and cost of the bearing assembly. Such size reductions may allow a shorter span between bearings with an attendant reduction in machinery vibration issues.
In embodiments of radial hybrid bearings 10 that lack a double-sided magnetic sector(s) 24 that is identical on either side of the rotor 30, linearization of the magnetic attractive force vs. rotor 30 displacement characteristic may be recovered by special software algorithms that are in common usage already for so-called Class B control. A square root function of the bearing current command is typically employed.
The optimal dimensions and/or configuration of the gas sector(s) 22, 22′; bearing pad(s) 23, 23′; magnetic sector(s) 24, 24′; coil(s) 26, 26′ and rotor 30, 30′ will vary from one embodiment of the radial hybrid bearing 10 and axial hybrid bearing 10′ to the next, and are therefore in no way limiting to the scope thereof. The various elements of the hybrid bearing 10, 10′ may be formed of any material that is suitable for the application for which the hybrid bearing 10, 10′ is used. Such materials include but are not limited to metals and their metal alloys, polymeric materials, and/or combinations thereof.
Although the specific embodiments pictured and described herein pertain to a radial hybrid bearing 10 having one gas sector 22 and one magnetic sector 24 and an axial hybrid bearing 10′ having four gas sectors 22′ and four magnetic sectors 24′, the hybrid bearing 10 may be configured with other orientations and/or with different quantities of the various elements having different shapes and/or orientations. Accordingly, the scope of the hybrid bearing 10, 10′ is in no way limited by the specific shape and/or dimensions of the gas sector(s) 22, 22′; bearing pad(s) 23, 23′; magnetic sector(s) 24, 24′; coil(s) 26, 26′ and rotor 30, 30′ or the relative quantities, dimensions, orientations, and/or positions thereof.
Having described the preferred embodiments, other features, advantages, and/or efficiencies of the hybrid bearing 10, 10′ will undoubtedly occur to those versed in the art, as will numerous modifications and alterations of the disclosed embodiments and methods, all of which may be achieved without departing from the spirit and scope of the hybrid bearing 10, 10′ as disclosed and claimed herein. It should be noted that the hybrid bearing 10, 10′ is not limited to the specific embodiments pictured and described herein, but are intended to apply to all similar apparatuses for providing any of the advantages of a hybrid bearing 10, 10′. Modifications and alterations from the described embodiments will occur to those skilled in the art without departure from the spirit and scope of hybrid bearing 10, 10′.
This application claims priority from provisional U.S. Pat. App. No. 61/724,179 filed on Nov. 8, 2012, which is incorporated by reference herein in its entirety.
Number | Date | Country | |
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61724179 | Nov 2012 | US |