1. Field
The present invention relates general to rotational bearings, and more particularly to monolithic rotational flexure bearings and methods of manufacture.
2. Description of Related Art
Rotational bearings are well known in the art for providing and supporting rotational motion in a wide variety of applications. Conventional journal and roller bearings, for example, have had much success in providing unlimited range of rotation angles while maintaining a relatively stable axis of rotation. Typically, a rotational bearing includes a fixed or stationary portion and a rotating portion. The stationary portion may be attached to a larger frame or base, and the rotating portion may be coupled to an element or feature that is desired to rotate relative to the stationary portion.
Conventional roller (or mechanical) bearings utilize one or more balls or rollers disposed between a stationary and rotating portion of the rotational bearing. Such bearings are generally cheap to manufacture and may be used in a wide variety of applications. Mechanical roller bearings, however, typically suffer from noise and vibration resulting, for example, from the stack of tolerances between the elements and rollers disposed therebetween. Accordingly, conventional roller bearings are generally not desirable for applications requiring precise rotational motion, e.g., with little or no axial/radial runout or small rotational angles (e.g., less than one degree) are desired. Additionally, conventional roller bearings typically include multiple parts that may require repair or lubrication periodically.
Conventional fluid bearings utilize a thin layer of liquid or gas to provide lubrication and support between the stationary and rotating portion of the bearing. For example, journal bearings typically use a fluid such as oil (but other liquids or gasses may be used) to lubricate the interface between moving portions of the rotational bearing. Fluid bearings generally have better frictional characteristics than mechanical bearings, and are generally optimized for high speed rotational motions, e.g., in disk drive motor or the like. A drawback of fluid bearings, however, includes that they generally operate poorly at low speeds and suffer from leaks or contamination of the fluid. For example, leaks or particle contamination of the lubricating fluid may cause changes in friction, which drastically reduce the performance of the bearing.
Conventional journal and roller bearings have had much success in providing an unlimited range of rotation angles with a relatively stable axis of rotation. The use of such bearings in applications that require small (or extremely limited) rotation angles, however, are generally hampered by tribology (friction-related) issues. For example, various physical phenomena including stiction, stick-slipping, and contact wearing of the bearing are well known conundrums of conventional bearings. These effects may become more problematic when repeatable and accurate small angles of rotations are desired of the rotational bearing.
Accordingly, a rotational bearing having relatively small radial and/or axial runout over small angles of rotation is desired.
According to one aspect described herein, an exemplary rotational flexure bearing is provided. In one example, the rotational flexure bearing includes a stationary portion, a rotating portion, and at least one flexure element. The stationary portion, rotating portion, and at the at least one flexure element are monolithically formed with each other. The rotating portion is coupled to the stationary portion through the at least one flexure element, thereby allowing relative rotation of the rotating portion with respect to the stationary portion. The stationary portion may include a center axis portion along a rotational axis of the flexure bearing and opposing fixed plates on either end, the rotating portion positioned between the opposing fixed plates. The flexure elements may extend from the center axis portion to the rotating portion. The flexure bearing may include between 2 and 6 flexure elements (or more).
In one example, a monolithically formed rotational flexure bearing may be integrated with a larger device, e.g., a cavity laser device. A portion of the rotational bearing, e.g., the stationary portion, may be integrated or monolithically formed as part of the device, e.g., formed with the base or package of the system.
According to another aspect, an exemplary method of manufacturing a rotational flexure bearing is provided. In one example, the method includes forming a rotational flexure bearing in a monolithic structure. The rotational flexure bearing includes a stationary portion, a rotating portion, and at least one flexure element, where the rotating portion is coupled to the stationary portion through the at least one flexure element, thereby allowing relative rotation of the rotating portion with respect to the stationary portion. In one example, the rotational flexure bearing is formed through a material subtraction process such as machining etching, electro static discharge machining, or the like. In another example, the rotational flexure bearing is formed through a material addition process such as casting, molding, rapid prototyping, or the like.
The present invention is better understood upon consideration of the detailed description below in conjunction with the accompanying drawings and claims.
The following description is presented to enable a person of ordinary skill in the art to make and use the various aspects and examples of the inventions. Descriptions of specific materials, techniques, and applications are provided only as examples. Various modifications to the examples described herein will be readily apparent to those of ordinary skill in the art, and the general principles defined herein may be applied to other examples and applications without departing from the spirit and scope of the inventions. Thus, the present inventions are not intended to be limiting to the examples described and shown, but are to be accorded the scope consistent with the appended claims.
According to one aspect, an exemplary monolithic rotational flexure bearing is provided herein. Broadly speaking, flexure-based bearings are devices which operate on the principle of elastic deformation of one or more elements—typically in flexion. The flexure bearing includes a stationary portion, a rotating portion, and at least one flexure element. The at least one flexure element allows relative rotation of the stationary portion and the rotating portion. In one example, the stationary portion, rotating portion, and at least one flexure element are monolithically formed with each other, thereby providing a highly reliable and accurate rotational bearing.
In one example, a monolithic rotational flexure bearing includes a discrete number of elastically flexure elements, symmetrically disposed around an axis of rotation, thereby allowing rotation of the rotating portion of the bearing with little to no axial runout (e.g., little to no movement of the axis of rotation). In one example, features of the flexure bearing are obtained by removing material from a single monolithic structure to form the desired elements of the rotational bearing. Material may be removed using any suitable material removal technique(s) such as conventional machining, Electro-Discharge Machining (EDM), or the like. In other examples, features of the bearing may be obtained by material addition techniques such as casting, molding, rapid prototyping, and the like to form the flexure bearing as a monolithic structure. The flexure bearing may be made from a variety of materials, including, e.g., metals, sintered metal powders, polymers, single crystals, and the like. Additionally, in some examples, the flexure bearing may advantageously be fabricated in-situ, e.g., built directly connecting the rotating portion and the stationary portion within a device.
A monolithic rotational flexure bearing may provide one-dimensional rotational freedom with a limited rotational range (e.g., on the order of a few thousandths of radians), where the rotational axis is well defined and stable over the entire range of rotation. Additionally, a monolithic design of the flexure bearing reduces drawbacks of typical conventional journal bearings (such as friction-related lifetime issues and lubrication-related sensitivity to particulates).
According to another aspect, an exemplary method of forming a monolithic rotational bearing is provided herein. The exemplary method includes removing material from a monolithic structure to define a rotational portion, a stationary portion, and one or more flexure elements disposed between the rotational portion and the stationary portion, thereby providing a rotation flexure bearing. The monolithic structure may include a cylindrical shaped structure, wherein material is removed to define fixed plates connected to a central portion of the structure, the fixed plates on either of the cylindrical structure along the axis of rotation. Apertures may be formed in the fixed plates symmetrically around the axis of the cylindrical shape. Material may then be removed from the central portion of the monolithic structure to form flexure elements connecting the fixed plates with the central portion of the monolithic structure.
A rotational bearing design that lends itself to be incorporated into an assembly, e.g., to produce monolithic packages, is also a desirable feature. Incorporation into a larger assembly may reduce the number of parts and reduce or eliminate joining hardware. One exemplary application and use of a monolithic rotational flexure bearing as described herein includes integration of the bearing with a cavity laser system. The bearing provides, e.g., stable, repeatable position and orientation of the rotation axis of a rotating element within the laser system. In the context of external cavity laser design and manufacturing, in order to provide as broad a mode-hop-free wavelength tuning range as possible, it is desirable for the designer to define (and the assembly operator to rely) on a stable, repeatable position and orientation of the rotation axis of a rotating element (e.g., a retro-reflector prism in this example). Further, for applications (such as a laser package) that will be subject to harsh or inaccessible environments such as space, where there is a desire for long life and little to no maintenance required, it becomes desirable to use a monolithic flexure-based rotational bearing to reduce problems caused by contamination and routine maintenance. Even for ordinary environments, the cost-of-ownership advantage of a simpler, sturdier bearing will offer apparent advantages. Those of ordinary skill in the art will recognize that various other applications and uses are possible and contemplated.
In operation, rotating portion 102 rotates relative to stationary portion 110 through flexure elements 104. In this example, stationary portion 110 includes fixed plates 110t and 110b, which may be attached to or integrated with a device, package, or the like, and rotating portion 102 may be attached or integrated with an element or device desired to rotate relative to stationary portion 110. For example, a member may extend away from rotating portion 102 and an actuator, e.g., a piezoelectric actuator or the like, may deflect the member causing rotation of rotating portion 102 relative to stationary portion 110. The terms “rotating” and “stationary” with respect to rotating portion 102 and stationary portion 110 are used for illustrative purposes only; in other examples, rotating portion 102 may be held stationary with respect to a platform or package with stationary portion 110 adapted to rotate relative to rotating portion 102. Further, in other examples, both rotating portion 102 and stationary portion 110 are capable of rotating relative to each other.
In this example, fixed plates 110t and 110b further include apertures 107 disposed generally around the axis of rotation and defining bridges 106 between apertures 107. Bridges 106 connect fixed plates 110t and 110b to the fixed center portion 108, and bridges 106 are equally spaced (e.g., angles of 120° between them). Furthermore, bridges 106 on stationary portion 110t are shifted relative to bridges 106 on stationary portion 110b by an angle that is half of the angle between bridges 106 (e.g., 60°). The arrangement and shift of bridges 106 in this example allow for an economical fabrication of the device following the material removal techniques as will be described in greater detail below. Those of skill in the art will recognize, however, that other configurations, e.g., numbers and positions of bridges or similar structures, are possible and contemplated and depend on the manufacturing techniques, desired applications, and the like.
In this exemplary design, the minimum number of bridges is two per fixed plate 110t and 110b and can be increased depending on the particular implementation. The number of flexure elements 104 is twice that of bridges in this configuration, e.g., flexure bearing 100 includes three bridges 106 per fixed plate 110t and 110b and includes six total flexure elements 104 between rotating portion 102 and center stationary portion 108. Exemplary flexure bearing 100 may provide a rotational bearing having a limited range of rotation with minimal axial runout. For example, over a small range of rotations, e.g., less than one degree to a few thousandths of radians, axial runout may be greatly reduced or eliminated relative to conventional flexure bearing designs.
The range of rotation is generally determined (at least in part) by the elastic limit of the material from which the bearing is fabricated as well as the geometry of the flexure elements, rotational portion, and stationary portion. In one example, the range of rotation is on the order of a few thousandths of a radian. The torque constant (rotation angle per applied torque) and the fundamental vibration frequency (unloaded) are generally a function of the elastic modulus, density of the material, geometry of the bearing. Those of ordinary skill in the art will recognize that the torque constant, range of rotation, and the like may be tuned for specific applications by changing the geometry, materials, dimensions, etc., of the flexure elements of the rotational flexure bearing.
Additionally, the exemplary flexure bearing may be manufactured from a monolithic structure. Symmetrically disposing the flexure elements may allow rotation with reduced or no axial runout (translation of the rotation axis). In other examples, however, flexure elements may be disposed asymmetrically and/or circumferentially around only a portion of the rotational axis (see, e.g.,
The diameter of the cylindrical block at both ends is reduced as shown in
Slots 309 are then formed in
Openings 307 are formed on both end plates 310t and 310b in
Center block 302 is then processed through openings 307 formed in end plates 310t and 310b as shown in
Exemplary flexure bearing 500 provides the ability to define the location of the rotation axis of a laser tuning device 564 in the design of the laser system 501, facilitating the assembly process. This may result in an improved stability of the rotational axis, producing a wider band of laser wavelength tuning, free of mode-hops. The simpler design added to the absence of contact elements and lubrication provides a rotational coupling with reduced concern over particle contamination and maintenance. Further, higher torque stiffness of the exemplary flexure bearing (e.g., compared to roller bearings) makes it more robust against mechanical noises (e.g., shock and vibration) by shifting higher the frequencies of natural modes of vibration.
Additionally, an actuator such as piezoelectric transducer 580 (shown in
In one example, the piezoelectric transducer 580 is included in a cavity formed within foundation 502 and is positioned between a static wall or member of foundation 502 and a portion of arm 582. Piezoelectric transducer 580 may further be pre-loaded during the assembly or manufacturing process. Additionally, in one example, a flexible element 583 (shown in
Additionally, flexure bearing 500 may further include a counter-weight 592 to further enhance rotational characteristics of the system. In particular, counter-weight 592 may distribute the weight of the arm 582 such that the center of gravity of arm 582 (including all that is attached to arm 582) is at or near the axis or rotation. This design may reduce the effect of translational vibrations or shock events that might otherwise translate into rotational movement of arm 582, thereby eliminating or greatly reducing the broadening of the laser line width (e.g., in laser applications).
The piezoelectric transducer in conjunction with the flexible bearing provides a quiet and stable driving device for wavelength tuning for such external cavity lasers. The exemplary flexure bearing confines the pivot so as to eliminate the mode hops, and the piezoelectric transducer controls the laser frequency with very fine wavelength tuning increment. This fine control of the wavelength results from the precise translation movement of the piezoelectric transducer. It will be understood by those of skill in the art that the exemplary monolithic rotational flexure bearings may be used in a variety of other applications. The present example, e.g., a cavity laser system, is provided only to illustrate one possible application.
In operation, rotating portion 602 rotates relative to a stationary portion through flexure elements 604. As shown in
In this example, tuning arm 682 is attached to the foundation 660 through six flexure elements 604, shown as blades, located symmetrically with respect to the pivot axis (axis of the center hole in the tuning arm) and the main axis of the tuning arm 682. The geometry (length, thickness, radii, or blends) and the number of flexure elements 604 may be defined in more than one configuration in order to satisfy various combinations of tuning (rotation) range and stiffness. While the tuning range is a functional parameter of the system (e.g., a laser system or the like), the stiffness is generally related to the natural frequency of the tuning arm 682, and also affects the piezoelectric element selection for actuator 680. In one example, the system may be designed by selecting a piezoelectric element for actuator 680 first and then determining a suitable geometry for flexure elements 604 to match the stiffness with the characteristics of the piezoelectric element. Additionally, the relative position of the actuator 680 (e.g., a piezoelectric element) may affect the tuning range, e.g., flipping the piezoelectric element with respect to the main axis of the tuning arm 682 would generate the same tuning range but in the opposite direction.
Additionally, in one example, a flexible element 683 is incorporated into arm 682, at the point of attachment to piezoelectric transducer 680. Additionally, another flexible element 684 (shown in
Additionally, flexure bearing 600 may further include a counter-weight 692 to further enhance rotational characteristics of the system. In particular, counter-weight 692 may distribute the weight of the arm 682 such that the center of gravity of arm 682 (including all that is attached to arm 682) is at or near the axis or rotation. This design may reduce the effect of translational vibrations or shock events that might otherwise translate into rotational movement of arm 682, thereby eliminating or greatly reducing the broadening of the laser line width (e.g., in laser applications).
The example of
It is noted that balancing tuning arm 682 (using counter-weight 692 and/or material removal process from tuning arm 682, for example) as described with respect to this and other examples herein, may reduce sensitivity to external/ambient noise (vibrations, shocks, and the like), especially when applied to micro-mechanical components/systems.
The foundation 660 may provide all the features needed to house optical elements (e.g. diodes, gratings, etc.) and includes the tuning (rotating) arm 682 and counter-weight 692 integrated therewith. In one example, the tuning arm 682 is carved out from the initial blank and left connected to static features of foundation 660 through flexure elements 602. As described above, the geometry and configuration of flexure elements 602 are design parameters that can be changed to obtain a variety of rotational characteristics.
In one example, the tuning range (in GHz) of an exemplary device including a flexure bearing and tuning arm is a function of the voltage applied to a piezoelectric element, e.g., actuator 680. In one exemplary device, such as that shown in
The concept of a monolithic foundation with integrated flexure bearing(s) as described herein can be applied to other uses where it is desired to rotate an element or elements (optical, mechanical, electrical, etc.) in a narrow (e.g., on the order of 1 mrad) range at frequencies on the order of 10 kHz, for example. Applications include, but are not limited to, modulated scanning mirrors, micro-manipulators (two tuning arms working in tandem), micro-valves (where the tuning arm would squeeze a flow tubing), brakes (where the tuning arm, in the unenergized mode, would touch and press onto a rotating drum keeping it from moving—energizing the piezoelectric element would “release” the drum), and high-precision angle sensors (where the piezoelectric element, driven in sensor mode, would detect angular changes of the order of 0.01 arcsec (or 0.05 microrad)).
It will be understood that the foregoing description and drawings of preferred embodiment in accordance with the present invention are merely illustrative of the various principles of the invention, and that various modifications can be made by those skilled in the art without departing from the scope and spirit of the invention. For example, various examples described herein may be combined and altered with other devices and methods. Further, numerous other devices and processes not explicitly described herein may utilize the exemplary flexure bearing described as will be recognized by those of ordinary skill in the art. Additionally, within the description, particular examples have been discussed and how these examples are thought to address certain disadvantages in related art. This discussion is not meant, however, to restrict the various examples to methods and/or systems that actually address or solve the disadvantages. Accordingly, the present invention is defined by the appended claims and should not be limited by the description herein.
This application is related to and claims benefit of previously filed U.S. provisional patent application Ser. No. 60/636,374, filed Dec. 15, 2004, and entitled “Rugged, Tunable Extended Cavity Diode Laser for Spaceflight Applications”; the entire content of which is hereby incorporated by reference in its entirety as if fully set forth herein.
This invention was made with Government support under a Prime Contract between the Institute and NASA and JPL subcontract number 1245238. The Government has certain rights in the invention.
Number | Date | Country | |
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60636374 | Dec 2004 | US |