1. Field of the Invention
The present invention relates to a linear compressor, particularly but not solely for use in refrigerators.
2. Summary of the Prior Art
Compressors, in particular refrigerator compressors, are conventionally driven by rotary electric motors. However, even in their most efficient form, there are significant losses associated with the crank system that converts rotary motion to linear reciprocating motion. Alternatively a rotary compressor which does not require a crank can be used but again there are high centripetal loads, leading to significant frictional losses. A linear compressor driven by a linear motor would not have these losses, and can be designed with a bearing load low enough to allow the use of aerostatic gas bearings as disclosed in U.S. Pat. No. 5,525,845, where a laterally compliant connecting rod allows for the low bearing load.
A discussion of aerostatic gas bearings is included in “Design of Aerostatic Bearings”, J W Powell, The Machinery Publishing Company Limited, London 1970. However with normal manufacturing tolerances and equipment production of effective gas bearings is difficult.
Conventional compressors are mounted within a hermetically sealed housing which in use acts as a reservoir of refrigerant gas. Refrigerant gas is drawn into the compressor from this reservoir and is exhausted through an exhaust conduit leading from the compressor, through the housing.
Operation of the compressor involves the reciprocation of moving parts leading to vibration of the compressor unit, in all three axis. To reduce the external noise effect of this vibration the compressor is mounted on isolation springs within the sealed housing.
With a linear compressor the piston vibrates relative to the cylinder in only one axis, with consequent reaction forces on whichever part, if either, is fixed. One solution proposed to this problem is to operate a pair of compressors synchronously in a balanced and opposed configuration. However this arrangement would be too complex and costly for use in a commodity item such as a domestic refrigerator. Another proposed solution is the addition of a resonant counterweight to reduce the vibration. However this approach limits the operation of the compressor because the counterweight is a negative feedback device and is limited to the fundamental unbalance force. A further solution is proposed in “Vibration characteristics of small rotary and linear cryogenic coolers for IR systems”, Gully and Hanes, Proceedings of the 6th International Cryocooler Conference, Plymouth, Mass., 1990. This solution involves independently supporting the piston part and the cylinder part of the compressor within the housing so that the “stator acts as a counterweight”. However in implementing this design in a domestic refrigerator there is a problem when the piston mass is low. In such a compressor, as the discharge pressure increases, the force of the compressed gas acts as a spring (the “gas spring”) which increases the running speed as the discharge pressure increases. This is a problem because the “third” vibration mode (where the piston and the cylinder vibrate in phase with each other but out of phase with the compressor shell) is only slightly above the desirable “second” mode (where the shell does not vibrate and the piston and cylinder are out of phase). Thus the shell starts to vibrate intolerably as the “gas spring” starts to operate and effectively raises the “second” mode frequency to, and eventually above, the “third” mode.
It is an object of the present invention to provide a compact linear compressor which goes some way to overcoming the abovementioned disadvantages.
Accordingly in a first aspect the present invention consists in a linear compressor including:
In a still further aspect the invention consists in a spring (particularly suited for linear compressors) having a pair of first mounting points for securement to a first body, and at least one second mounting point for securement to a second body reciprocable relative to said first body, and a spring arm spanning a path between said first mounting points by way of said second mounting point, at least a first section having a curve around one of said first mounting points and a second section having a curve around another said first mounting point, said first section and said second section meeting between said first mounting points at said second mounting point.
In a further aspect the invention may broadly be said to consist in a linear compressor having a piston part and a cylinder part reciprocal relative to one another, and a main spring as set forth above connecting between said piston part and said cylinder part.
In a further aspect the invention consists in;
To those skilled in the art to which the invention relates, many changes in construction and widely differing embodiments and applications of the invention will suggest themselves without departing from the scope of the invention as defined in the appended claims. The disclosures and the descriptions herein are purely illustrative and are not intended to be in any sense limiting.
A practical embodiment of the invention, shown in
This reciprocating movement draws gas in through a suction tube 12 through a suction port 26 through a suction muffler 20 and through a suction valve port 24 in a valve plate 21 into a compression space 28. The compressed gas then leaves through a discharge valve port 23, is silenced in a discharge muffler 19, and exits through a discharge tube 18.
The cylinder 9 is supported by the discharge tube 18 and the cylinder spring 14 which have a combined stiffness, cylinder, in the axial direction. The piston 11 is supported radially by gas bearings which will be described later. To get resonant oscillation of the piston and cylinder the main spring has a stiffness, main, such that the resonant frequency, fn, can be estimated from the relation,
Where piston, cylinder, are the sprung masses of the piston and cylinder springs, fn is usually 10 to 20 Hz less than the desired running frequency to allow for the increase in frequency due to the stiffness of the compressed gas, the cylinder springs 14 and 18, and piston spring 13. The stiffness of the piston spring piston is then selected according to the relationship
The spring forces are transferred to the piston via the rod end 25 and the radially compliant piston rod 24, to the piston. The electromagnetic forces are transferred to the piston via the piston flange 7, from the bi-polar magnets 22. These are bonded to each other and to the piston flange 7.
The compressor motor comprises a two part stator 5,6 and an armature 22. The magnetic interaction of the stator 5, 6 and armature 22 generates reciprocating force on the piston 11 (attached to the armature by flange 7).
An oscillating current in coils 1 and 2, not necessarily sinusoidal, will give rise to substantial movement of the piston 11 relative to the cylinder 9 provided the oscillation frequency is close to the natural resonant frequency of the mechanical system. This oscillating force creates a reaction force on the stator parts. Thus the stator 6 must be rigidly attached to the cylinder 9 by adhesive, shrink fit or clamp etc. The back iron is clamped or bonded to the stator mount 17.
The stator mount 17 also clamps the outer ends of the main spring 15 and also keeps the relatively weak outer stator round and concentric with the inner stator. The entire compressor assembly is hermetically sealed inside the compressor shell 30.
In the present invention it is proposed that the main spring 15 has a stiffness much greater than the stiffness of the effective cylinder spring, and of the piston spring. This “main spring” raises the “second” mode frequency above the “third” so that the “gas spring” then only separates the modal frequencies further.
The actual running frequency (the “second” mode frequency) is determined by a complicated relation of the mass of piston and cylinder and by the stiffness of the piston spring, cylinder spring, and main spring 15. Also when the discharge pressure is high the stiffness of the compressed gas must be added to that of the main spring. However, with the cylinder spring quite soft (say with a stiffness {fraction (1/100)} of the main spring) the running frequency is found reasonably accurately by:
External vibration due to sources other than from the fundamental due to piston/cylinder movement can be almost eliminated by reducing the oscillating mass and by ensuring that the piston and cylinder springs are relatively soft. The stiffness of the cylinder spring can be reduced to a minimum by having no cylinder spring at all, and using the inherent stiffness (from around 1000 N/m) of the discharge tube 18 (or where a cooling tube is used the stiffness of both discharge and cooling tube are combined ie 2000 N/m). This then means that the stiffness of the piston spring must be:
which is for a ten to one cylinder to piston mass ratio gives a very soft piston-spring (approx 100 to 200 N/m).
For the compressor to resonate at roughly 75 Hz, a piston mass of around 100 g and a ten to one cylinder to piston mass ratio, the main spring (main) needs to be about 20000 N/m. Typically the value of the gas spring will be lower than that of the main spring but not substantially lower. In the above case the running frequency might be expected to be 99 Hz where the gas spring (kgas) of approximately 15000 N/m.
The piston 11 is supported radially within the cylinder by aerostatic gas bearings.
The cylinder part of the compressor includes the cylinder 9 having a bore therethrough and a cylinder liner 10 within the bore. The cylinder liner 10 may be made from a suitable material to reduce piston wear. For example it may be formed from a fibre reinforced plastic composite such as carbon fibre reinforced nylon with 15% PTFE (preferred), or may be cast iron with the self lubricating effect of its graphite flakes. Referring to
The gas bearing passages 8 are formed as grooves 80 or 81 in either the bore 74 of the cylinder or in the outer wall 70 of the cylinder liner. These grooves 80 or 81 combine with the wall of the other cylinder or the cylinder liner to form enclosed passages 8 leading to the openings 31. It will be appreciated that while the grooves could be provided in either part they are more readily formed in the liner part than in the cylinder part, being on an outer surface rather than an inner surface. Being able to machine the grooves into a surface of one or other part rather than having to drill or bore passages is a significant manufacturing improvement.
It has been found that the pressure drop in the gas bearing passages needs to be similar to the pressure drop in the exit flow between the piston and the bore of the cylinder liner. Since the gap between the piston 11 and the cylinder liner bore 71 (for an effective compact compressor) is only 10 to 15 microns, the sectional dimensions of the passages 8 need to be very small, for example, 40 microns deep by 120 microns wide. These small dimensions make manufacture difficult.
However, with reference to
Higher running frequencies reduce motor size but require more spring stiffness, and consequently higher stresses in the springs. Thus it is important for compressor longevity that the highest quality spring material be used. In the conventional linear compressors main springs made from pressed spring steel sheet are often used. However, the edges cut in the pressing operation require careful polishing to regain the original strength of the spring steel sheet.
In the preferred embodiment of the present invention the main spring is formed from circular section music wire. As depicted in
The very high fatigue strength of music wire is utilised effectively and there is no need for a subsequent polishing operation. If increased lateral stiffness is required the music wire could be deformed by 10% to give an elliptical section. To simplify the attachment of the main spring square section wire could be used, or the connection ends of the spring may be stamped to a flattened shape, as depicted.
However, an alternative and preferred embodiment of the main spring is depicted in
In
The constant radius curves 63,64 are placed in torsion by the displacement (out of plane) of the piston mounting point 62 relative to the cylinder mounting points 60,61. Being constant radius the torsion stresses along each of the sections 60,61 are also substantially constant. The radial, or substantially radial direction at the cylinder mounting sections 67,68 reduces any torsion stresses at the cylinder mounting and improves mounting of the spring 59 to the cylinder part. The central mounting point 62 of the piston part, at a part of the spring having high torsion stresses, does not significantly complicate that mounting because that mounting can be made to encircle the spring arm and have a resilient (eg: rubber) boot to allow for movement within of the spring arm within the mounting. Movement of the spring arm within the mounting will be cyclical and, due to the symmetry of the spring (the spring is rotationally symmetric through 180 degrees) and the cyclic forces, should not cause the mounting to creep or walk along the spring arm. It should be noted that this spring configuration has been particularly developed for incorporating the wire formed approach rather than the stamped plate approach. However (subject to limitations in some more complex embodiments referred to below) springs of this geometric form could also be manufactured using the stamped plate method, but some of the advantages (eg: that the constant stresses are particular suitable with the wire which is of constant cross section) would not be realised.
It should be appreciated that variations on this spring are also possible without departing from the scope of the invention. On particular, if the spring is formed so that the spring arm is perpendicular to the line between the compressor mountings at the compressor mounting then the arm can continue to form an equivalent (although mirrored) loop, below or above the first loop, back to the other compressor mounting. That loop would of course have a second piston connection point below or above the first. At the other compressor connection point the ends can meet, or alternatively this second loop may be continued through the connection point to form a third loop, below (or above as necessary) the second loop, back to the first compressor mounting point (or at least to a mounting point immediately above or below). This chaining of loops can proceed to include as many loops as necessary to achieve a required spring constant. Clearly this is a planar spring configuration that cannot be constructed by stamped plate methods.
However the most preferred embodiment for the main spring is depicted in
In the most preferred embodiment the main spring takes a form other than that of a planar spring. It retains many of the conceptual features of the spring of
The spring 15 has a pair of free ends for mounting to one of the compressor parts, for example the cylinder part. The spring 15 has a further mounting point for mounting to the other compressor part, for example the piston part this further mounting point.
The spring 15 includes a pair of curved sections 63, 64 of substantially constant radius of curvature which each pass around the respective mounting end. Each of these curved sections extends over a length of approximately 360°. Each section curves smoothly at both of its ends. At the ends 65, 66 they curve such that the lengths 67, 68 of them at the cylinder mounting ends are radially aligned. This sharper curve 65, 66 is selected to maintain a substantially even stress distribution along the transition. The spring 15 of
In the manner depicted in
The constant radius curve 63, 64 are placed in torsion by the displacement of the piston mounting point 62 relative to the mounting points 60, 61. Being constant radius the torsion stress along each of the sections 63, 64 are also substantially constant. The radial or substantially radial direction at the cylinder mounting sections 67, 68 and at the piston mounting point 62 reduces any torsion stresses at the cylinder mounting ends and at the piston mounting point and improves mounting of the spring 15 to both the cylinder parts and the piston part.
Number | Date | Country | Kind |
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500681 | Oct 1999 | NZ | national |
500683 | Oct 1999 | NZ | national |
This application is a divisional application of U.S. patent application Ser. No. 10/110,886, which was accorded a filing date under 35 U.S.C. §371 of Jul. 15, 2002, which is the National Stage of International Application No. PCT/NZOO/00202 which has an international filing date of Oct. 17, 2000 and which was published in English on Apr. 26, 2001 under International Publication Number WO 01/29444.
Number | Date | Country | |
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Parent | 10110886 | Jul 2002 | US |
Child | 11042234 | Jan 2005 | US |