Self loading cylindrical autolubricated gas bearing
This invention relates in general to bearing structures and more particularly it relates to the loading of bearings of the autolubricated gas type, and to the means for raising the onset of &#34;half-frequency whirl&#34; in this type of bearing. By raising the onset, or in other words the frequency at which it occurs, of &#34;half frequency whirl&#34; above the operating range of the bearing, we can for all practical purposes eliminate its occurrence; provision of a satisfactory bearing for the rotors of precision instruments, and in particular for the rotors of precision gyroscopes, is a very serious problem. The principal requirements for rotor bearings in precision gyroscopes are: consistency of elastic properties, freedom from vibration, long life, and self servicing. In addition, simplicity and low cost are important requirements. 
     Bearing vibration in a precision gyroscope sets a limit upon the degree to which dynamic balance is obtained and gives rise to disturbing torques. In addition, vibration components obscure the precession of the gyroscope. Vibration in the gyroscope also results in wear of components. 
     Auto-lubricated gas type bearings are finding wide spread application in the support of rotors on precision gyroscopes, due to many attractive features, such as low and constant friction, no contamination from lubricants, high reliability, and hence infinite life under constant operation. Under actual operation, autolubricated gas bearings frequently become unstable. This instability appears as a whirling of the bearing shaft with a rapidly increasing amplitude and with subsequent destruction to the bearing. This whirling instability occurs at slightly less than half the rotor speed and hence is called &#34;half-frequency whirl&#34;. Various attempts have been made to raise the onset of this instability by preloading the bearing. Efforts in the present state-of-the-art are to increase the rotor weight and thereby load the bearing. 
     Gas bearings are known, in which the pressure of the supporting gas in the bearing gap, like the pressure in the oil film of a hydrodynamically lubricated bearing, is built up by the rotary movement of the shaft due to viscosity forces. In these bearings, there is a possibility that the member carried by the gas film or gas cushion, due to the compressibility of the gas in the bearing gap and particularly in the relatively large distribution spaces, will be set in vibration, either through self-excitation or through the effects of external interfering forces, such as unbalance. The present invention prevents the onset of &#34;half-frequency whirl&#34; even when the bearing is unloaded and does not reduce the stiffness and ultimate load carrying ability of the bearing. The present state-of-the-art is to prevent whirl in plane cylindrical bearings by machining grooves, or flats on the cylindrical surfaces. These solutions drastically reduce the load carrying ability of the bearings and increase their compliance. The novel structure disclosed herein is to build the cylindrical gas bearing in two or more sections, which are slightly eccentric with respect to each other, thereby loading one section of the bearing against another. Each of the bearing sections then operates with a slight eccentricity. 
     Accordingly, the principal object of this invention is to provide a bearing structure for high speed applications in which the onset of half-frequency whirl is raised above the operating frequency of the bearing. 
     Another object of this invention is to provide a bearing structure which causes self loading. 
     Still another object of this invention is to provide a gas autolubricated cylindrical bearing characterized by its extreme rigidity and lack of vibration. 
     An object of this invention is to provide an autolubricated cylindrical gas bearing suitable for use in scientific instruments. 
     It is another object of this invention to provide an instrument gas bearing whose vibration is substantially less than any known hydrodynamic gas bearing heretofore known. 
    
    
     Other objects of the invention will become apparent from the following description taken in connection with the accompanying drawings in which: 
     FIG. 1 is a side section view of a preferred embodiment of this invention; 
     FIG. 2 is a section view taken at the section 2--2 of FIG. 1; and 
     FIG. 3 is a section view taken at the section 3--3 of FIG. 1. 
    
    
     Referring to FIG. 1, there is shown a shaft 4, hydrodynamically supported in a bearing 10. The bearing is designed, enveloping said shaft, so that under load a wedged shaped gap exists between the shaft 4 and the bearing 10. Gas at relatively low pressure in larger gaps, such as 13 and 15, is squeezed by viscous drag into the narrow gaps, such as 14 and 16, thereby generating pressure or lift. The ability of a fluid to provide a hydrodynamic wedge is particularly the result of the viscosity and density of the fluid whereby the fluid resists changes in shape; also aiding in the creation of the wedge is the eccentricity and velocity of the shaft relative to the bearing. The eccentricity produces an additional converging area in which high pressures are also developed. 
     The shaft 4 is rotatably mounted within bearing 10 about an axis of rotation defined by axis C. Located parallel to and positioned on opposite sides of axis C are axes C&#39; and C&#34;. Axes C&#39; and C&#34; are spaced equal distances from axis C. The shaft 4, having a diameter D 1 , is comprised of at least three eccentric sections 6, 7 and 8. These sections are eccentrically mounted with respect to the shafts&#39; rotational axis C. Sections 6 and 8 are symmetrically mounted with respect to axis C&#39;, while section 7 is symmetrically mounted with respect to axis C&#34;. Section 6 is equal in length d to section 8 and section 7 is equal in length, 2d to sections 7 and 8 combined. 
     Sections 6 and 8 form right circular cylinders having an axis of symmetry defined as C&#39; and also having a diameter D 2 . Section 7 forms a right circular cylinder having its axis of symmetry defined as C&#34;, and having a diameter equal to D 2 . The diameter D 1  of shaft 4 is slightly greater than the diameters D 2  of sections 6 and 8. It is to be understood that the center cylinder part 7 need not be the same diameter as the end cylinders 6 and 8. FIG. 2 discloses a sectional view taken from FIG. 1 at points 2--2. With the shaft 4 rotating at a relatively high rate of speed ω(angular frequency), a first pressure area will be set up in the gap 13 and a second pressure area will be set up in the gap 14. Due to the eccentric mounting of member 6, the pressure in gap 14 will be greater than the pressure in gap 13. This will also be true for section 8. This difference in pressure tends to force the sections 6 and 8 to assume a rotational center which will equalize the pressure in the gaps. 
     Referring to FIG. 3, there is shown a sectional view taken along the line 3--3 of shaft 4. In operation, when shaft 4 is rotated at high rates of speed, a first pressure zone 15 and a second pressure zone 16 is generated by the eccentrically mounted section 7. The pressure in zone 16 is greater than the pressure in zone 15, and this difference in pressure tends to force the section 7 to define a new rotational center located such that the pressure in zones 15 and 16 are equalized. 
     For the purposes of clarity, it will be assumed that these forces are acting on the shaft 4 while the shaft is stationary, although in operation the forces are rotating along with the shaft. Referring back to FIG. 1, it can be seen that the pressure in gaps 14 are equal and opposite to the pressure in gap 16. The pressure differential of sections 6, 7 and 8 tends to load these sections one against another which has the effect of continually keeping the bearing under load throughout its running condition. By self-loading the bearing, the onset of &#34;half-frequency whirl&#34; is raised to such a value that throughout the operating range of the shaft this phenomena does not occur. 
     While there has been described a preferred embodiment of the present invention, it will be appreciated that the invention is not limited thereto but that various modifications may be made without departing from the scope of the appended claims.