The present invention relates to a compressor unit comprising a cylinder and a piston that delimit a compressor chamber, a linear drive for driving a relative movement of the cylinder and piston and a capsule that surrounds at least the cylinder and the piston.
Such a capsule is conventionally used as a reservoir for gas to be compressed, from which the gas is sucked into the compressor chamber, and a pipeline for drawing off the compressed gas is guided out of the compressor chamber through the interior.
One problem with these conventional compressor units is that the gas-filled interior and the capsule surrounding the same not only absorb operating noise from the compressor, but also prevent the release of heat into the environment. Heat which is generated during operation of the compressor by means of adiabatic compression of the gas in the compressor chamber, partly passes over into the cylinder and piston and finally heats the gas in the interior around the cylinder and piston. This heating process reduces the quantity of gas which is sucked in and compressed in each movement cycle of the piston, thereby negatively affecting the degree of efficiency of the compressor.
A further problem is associated with the design of the conventional linear compressors. These generally include a permanent magnet armature which can be linearly moved to and fro in an air gap of an electromagnet. These linear drives are characterized in that the driving force acting on the armature can be directly transferred to the piston without interconnected levers or suchlike and consequently practically without any frictional losses, but, contrary to a conventional rotary drive, the amplitude of the piston movement is not predefined in a constructionally-specific fashion, but can instead be influenced by the intensity of the magnetic field acting on the armature. To achieve a high degree of efficiency of the compressor, the compressor chamber at the upper dead center of the piston movement should be as small as possible, but it should also be prevented that the cylinder and piston strike one another at the dead center in order to keep the operating noise of the compressor and the stresses within a limit.
The object of the present invention is to specify a compressor unit of the type cited in the introduction, which enables an efficient dissipation of the heat which is released in the compressor chamber and/or despite a high degree of efficiency prevents excessive stress on the material or noise development as a result of the cylinder and piston striking one another.
The object is achieved by an outlet opening of the compressor chamber opening into an interior of the capsule instead of an intake opening, in the case of a compressor unit comprising a cylinder and a piston, which delimit a compressor chamber, a linear drive for driving a relative movement of the cylinder and piston and a capsule, which at least surrounds the cylinder and the piston. As a result, if the compressor unit is operated, the interior of the capsule is under high pressure. Although the compressed gas ejected by the compressor chamber is significantly warmer than the low pressure gas previously ingested, so that the cylinder and piston, if they essentially release their heat into the environment only by way of the gas in the interior, cannot be colder than this gas during stationary operation, its heat conductivity as a result of its high density is greater by a multiple than that of the uncompressed gas, so that an overheating of the cylinder and piston can consequently be reliably prevented.
A further effect which results from the presence of the compressed gas in the capsule surrounding the cylinder and piston is that the high pressure of the compressed gas acts on the rear of the piston. The linear drive 1 must therefore essentially only provide driving power in an expansion phase of the compressor chamber, if the piston is withdrawn from the cylinder counter to the pressure of the compressed gas in the interior. The counter movement of the piston requires hardly any external drive force, since the pressure of the gas in the interior is essentially sufficient to repel the piston. If the linear drive were not to provide any driving power during the compression phase, the piston would then come to a standstill shortly before the upper dead center, if the pressures in the compression chamber and in the interior of the capsule become the same. A small amount of operating energy of the linear drive during the compression phase is sufficient to overcome this pressure equalization position and to expel the contents of the compressor chamber. The energy with which the cylinder and piston could strike one another in the case of pressure fluctuations lies in the order of magnitude of this drive energy and can therefore be kept significantly lower than in the case of a compressor, in which the linear drive in the compression phase must work against the pressure developing in the compressor chamber.
The piston in the cylinder is preferably gas-pressure mounted. By comparison with oil lubrication, the gas pressure mounting is advantageous in that it enables a practically frictionless piston movement. The heat dissipation from the piston via a gas thrust bearing is less efficient than via an oil film, but this is not critical in the present case since the piston is able to output sufficient heat via the high pressure gas of the interior.
To feed the gas thrust bearing, bores are preferably provided in a casing of the cylinder, which connect a gap between the casing and a lateral surface of the piston to the interior.
Furthermore, channels for supplying pressurized gas from the compressor chamber into the gap can extend between a face surface and the lateral face of the piston. These channels facilitate maintenance of the gas thrust bearing in the vicinity of the upper dead center, if, as a result of the pressure equalization and/or the overpressure in the compressor chamber, the inflow of gas from the interior via the bores of the casing ceases.
The channels can be embodied as bores or as open grooves.
The outlet opening of the compressor chamber can be formed in the piston. An entire face surface of the cylinder is thus available in order to accommodate there an inlet valve with a large cross-sectional surface and accordingly minimal drop in pressure.
A suction gas line is preferably routed through the interior to the compressor chamber in order to supply the suction gas rapidly and with minimal heating by means of the pressurized gas from the interior of the compressor chamber.
Further features and advantages of the invention result from the subsequent description of exemplary embodiments with reference to the appended Figures, in which;
The linear compressor unit shown in
A compressor includes a cylinder 7 and a piston 6 which can be moved in the cylinder 7. The piston 6 is coupled to the armature 4 by way of a piston rod 5. The cylinder 7 is fixedly connected to the electromagnet 3 by way of a frame part 24, with which the return springs 23 also engage. The design comprising linear drive 1 and compressor is hermetically enclosed in a capsule 8 and suspended so as to be oscillatable by way of springs (not shown) which engage with the frame part 24 and the capsule 8.
An elastic pipeline 9 extends through a wall of the capsule 8 to a prechamber 10 of the cylinder. The prechamber 10 is separated from a compressor chamber 12 delimited by the cylinder 7 and the piston 6 by a non-return valve 11. A further non-return valve 13 is arranged opposite the non-return valve in a face surface 14 of the piston 6. This is embodied in the present case in the manner of a circular truncated cone and forms the valve seat with its lateral surface in a passage of the piston base. The smaller base surface of the circular truncated cone projects opposite the base of the piston 6 and forms a stop surface.
To drive the oscillation movement of the armature 4 and of the piston 6 effectively, the frequency of the alternating current is attuned to the resonance frequency of the oscillating system comprising linear drive 1, compressor and return springs 23. The amplitude of the oscillation movement is dependent on the electrical power fed by the supply circuit into the electromagnets 3. This may be different in the positive and negative half wave of the alternating current, in particular, it may be larger in the half wave driving an expansion movement of the compressor, than in the half wave driving a compression movement.
If the linear drive 1 drives the piston 6 to an oscillation movement, in an expansion phase of the compression chamber 12, low pressure gas is sucked into the compressor chamber 12 via the pipeline 9 and the prechamber 10. If towards the end of a compression phase of the compressor the pressure in the compressor chamber 12 exceeds the pressure in the interior 16 sufficiently in order to overcome a closing force of the non-return valve 13, the non-return valve 13 opens and the compressed gas escapes into the interior 16 of the capsule 8. In variation, provision can also be made, if the non-return valve 13 projects relative to the base of the piston 6, for said non-return valve to be opened by striking the overhang on the front wall of the cylinder. During stationary operation, the pressure in the interior 16 is only marginally lower than the maximum pressure achieved in the compressor chamber 12, so that the non-return valve 13 only opens briefly before the top dead center is reached. The linear drive 1 therefore operates during the overall expansion phase of the compressor chamber 12 against the pressure of the interior 16, whereas in a compression phase, the pressure in the interior 16 is almost sufficient to compress the gas in the compressor chamber 12. The power which the supply circuit feeds into the electromagnets 3 can therefore be significantly less in a half wave driving the compressor than in a half wave driving the expansion. No complicated monitoring of the piston movement is thus necessary in order to ensure that the piston 6 does not strike the face surface of the cylinder 7, or at least does not do so with excessive force.
Shortly before the piston 6 reaches its upper dead center during the course of a compression movement of the piston 6, a pressure equalization results between the compressor chamber 12 and the interior 16 and the gas flow through the bores 19 is disrupted. Numerous bores 21 extending diagonally from the face surface 14 toward the lateral surface 18 of the piston 6 convey the flow of pressurized gas out of the compressor chamber 12 into the gap 20, if the piston 6 approaches the top dead center by way of the pressure equalization position. The flow direction of the gas in the gap 20 consequently reverses during the piston movement, while over a large part of the piston path, from the lower dead center to the pressure equalization position, the pressure in the compressor chamber 12 is lower than in the interior 16 and gas flows through the bores 19 and the gap 20 into the compressor chamber 12, the gas flow in the vicinity of the upper dead center proceeds from the compressor chamber 12 to the interior 16. The piston 6 is thus effectively gas pressure-mounted on both reversal points, if its speed is zero and the duration is accordingly high, and it is only if the piston passes through the pressure equalization position that the gas thrust bearing briefly breaks down. As the piston is moved at this point, the time at which the bearing effect is interrupted is short and the risk of the piston 6 sliding into the cylinder 7 before the bearing effect is used again is minimal
Number | Date | Country | Kind |
---|---|---|---|
10 2008 007 661.9 | Feb 2008 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/EP2009/050962 | 1/28/2009 | WO | 00 | 7/23/2010 |