The present invention relates to a hermetic compressor for use in refrigerator, air-conditioner and refrigerating plant or the like.
Recently, highly efficient and down-sized hermetic compressors with reduced noise emission have been required for refrigerating plants and the like.
U.S. Pat. No. 5,228,843 or Japanese Patent Laid-Open Application No. 2001-503833 discloses conventional hermetic compressors.
Now, a conventional hermetic compressor is described with reference to the drawings.
An operation of the hermetic compressor with the aforementioned configuration is described. Rotor 4A of motor element 50 rotates crankshaft 10A, and the rotation movement of eccentric section 12 travels to piston 30 via coupler 31. As piston 30 reciprocates in compression chamber 22, refrigerant gas flows into enclosed container 10 from the refrigerating system (not shown) through suction pipe 39. The flowed in refrigerant gas is sucked into muffling space 41 through opening 45 of suction muffler 40.
Next, the refrigerant gas flowing intermittently into compression chamber 22 via suction valve 35 through passage 44 and suction inlet opening 34 is compressed and then discharged to the refrigerating system. Here, at the time when the refrigerant gas is sucked into compression chamber 22, opening/shutting movements of movable valve 33 generate pressure pulsations in the refrigerant gas and the pressure pulsations propagate in a direction opposite to the stream of the above refrigerant gas. The pressure pulsations of the refrigerant gas attenuate and muffle in repeated expansion and contraction during the flow of refrigerant gas through communication passage 44, muffling space 41 and opening 45 in suction muffler 40 having respective different cross sectional areas.
In the aforementioned conventional configuration, however, pressure pulsations generated in the refrigerant gas by opening/shutting movements of movable valve 33 do not attenuate sufficiently. In addition, the pressure waves have large values at the passage opening 43 disposed at the end of muffling space 41. In muffling space 41, sound propagating compressional waves form standing waves for some natural frequencies by reflection. The sound pressure is high in dense portions (hereafter referred to as anti-node) of the standing waves and low in non-dense portions (hereafter referred to as node) of the standing waves. Among a distribution of the standing waves, the node is not produced at the end of muffling space 41. The problem is, therefore, that the noises do not attenuate sufficiently for some natural frequencies in the conventional art. Additionally, in the aforementioned conventional art, the refrigerant gas sucked through opening 45 is discharged to muffling space 41 having a large space capacity before being sent to communication passage 44. Here, the refrigerant gas receives heat energy from inner surfaces of muffling space 41 resulting in reduction of refrigerant gas density to cause a reduced refrigerating capacity.
Moreover, the resonance frequency of communication passage 44 that is determined by the length of communication passage 44 is difficult to adjust in the conventional art because communication passage 44 can not be extended any more. Consequently, pressure pulsations in communication passage 44 varied by the resonance frequency can not be maximized at the time just before the opening time of movable valve 33. The problem is that the volume of refrigerant gas flowing into compression chamber 22 decreases to cause a poor refrigerating capacity and efficiency.
The present invention aims to provide a hermetic compressor with a reduced noise emission in the muffling space of the suction muffler and an improved refrigerating capacity and efficiency to solve the aforementioned problems.
The present invention aims to provide a hermetic compressor comprising: a compression element; a motor element to drive rotatably the compression element; and an enclosed container that encloses the compression element and the motor element, and stores lubrication oil.
The compression element includes: a cylinder block with a compression chamber; a valve plate forming a suction valve together with a movable valve to close an opening of the compression chamber of the cylinder block; a head forming a high-pressure chamber fixed to the cylinder block via the valve plate; and a suction muffler having a muffling space.
The suction muffler includes: two rooms and a communication space communicationg the two rooms; a first communication passage communicating the movable valve with the muffling space and extending into the muffling space to form an opening in the muffling space; and a second communication passage form communicating the enclosed container with the muffling space and extending into the muffling space to form an opening in the muffling space, wherein the openings in the muffling space from the first and the second communication passages are disposed in one of the two rooms, and the other room of the two rooms together with the communication space form a resonance muffler whose resonance frequency matches with a cavity resonance frequency of the enclosed container.
Now, an exemplary embodiment of the hermetic compressor disclosed in the present invention is described with reference to the drawings. The drawings are shown in schematic views and are not dimensioned correctly with regard to respective positioning.
Enclosed container 101 contains motor element 105 constituted by stator 103A with winding 103a and rotor 104, and compressor element 106 driven by motor element 105 as shown in
The resonance frequency is adjusted to approx. 750 Hz using the length of first communication passage 142 of approx. 70 mm. The frequency corresponds to triple that of the primary natural frequency of movable valve 133 of 250 Hz.
On the other hand, the frequency does not correspond to any one of the frequency group including; the cavity resonance frequency in enclosed container 101 of approx. 500 Hz; the primary natural frequency of movable valve 133 of approx. 250 Hz; the secondary natural frequency of the movable valve 133 of approx. 500 Hz; and the natural frequency of enclosed container 101 of approx. 2.5 kHz.
The resonance frequency is adjusted to approx. 1.2 kHz using the length of second communication passage 143 of 60 mm. The frequency does not correspond to any one of the frequency group including; the cavity resonance frequency of enclosed container 101 of approx. 500 Hz; the primary natural frequency of movable valve 133 of approx. 250 Hz; the secondary natural frequency of the movable valve 133 of approx. 500 Hz; and the natural frequency of enclosed container 101 of approx. 2.5 kHz.
Moreover, both of first opening 142a of first communication passage 142 and second opening 143a of second communication passage 143 are located in room B 140b of muffling space 141. The locations of the openings are allowed to correspond to a node of natural frequency of 2.5 kHz of enclosed container 101.
Next, an operation of the hermetic compressor with the aforementioned configuration is described. Rotor 104 of motor element 105 rotates crankshaft 110 accompanying the rotary movement of eccentric section 112 that is conducted to piston 130 via coupler 131. As piston 130 reciprocates in compression chamber 122, refrigerant gas R134a flows into enclosed container 101 from the refrigerating system (not shown). The refrigerant gas first flows into enclosed container 101 through suction pipe 139. Then, the refrigerant gas is released to room B 140b via second communication passage 143 of suction muffler 140. Next, traveling through suction hole 134 via first communication passage 142, the refrigerant gas flows into compression chamber 122, when movable valve 133 is opened, and is compressed then discharged to the refrigerating system. Movable valve 133 opens and shuts when refrigerant gas R134a is sucked into compression chamber 122.
The opening/shutting movement of movable valve 133 generates pressure pulsations of various frequencies. The pressure pulsations propagate in a direction opposite to the stream of the aforementioned refrigerant gas. Among the pressure pulsations, 500 Hz wave that is a natural frequency of cavity resonance acts as an oscillation source when the wave reaches into enclosed container 101.
Consequently, 500 Hz band noises, corresponding to the natural frequency of cavity resonance of enclosed container 101, increase in enclosed container 101. However, 500 Hz band noises in the pressure pulsations attenuate greatly in room B 140b because a resonance muffler having the resonance frequency of approx. 500 Hz is produced by room A 140a together with communication space 140c. Additionally, both of the resonance frequency of first communication passage 142 of approx. 750 Hz and the resonance frequency of second communication passage 143 of approx. 1.2 kHz do not meet the frequency of 500 Hz. Attenuating also in both first communication passage 142 and second communication passage 143, the 500 Hz band noises generated by the pressure pulsations are further hard to propagate into enclosed container 101. As mentioned above, the oscillating power caused by the cavity resonance in enclosed container 101 is reduced with the use of refrigerant gas R134a. Consequently, 500 Hz band noises caused by the cavity resonance in enclosed container 101 can be suppressed to a low level.
Additionally, among pulsation components generated by opening/shutting movements of movable valve 133, 2.5 kHz band noises induce a resonance with a natural frequency of enclosed container 101 when released into the space of enclosed container 101. Then, the sound phenomenon occurs in enclosed container 101. On the other hand, both of first opening 142a of first communication passage 142 and second opening 143a of second communication passage 143 open at positions corresponding to the nodes of vibration mode of 2.5 kHz band noises in muffling space 141. Consequently, 2.5 kHz band noises generated by opening/shutting movements of movable valve 133 attenuate greatly in the muffling space. In addition to this, both of approx. 750 Hz resonance frequency of first communication passage 142 and approx. 1.2 kHz resonance frequency of second communication passage 143 do not meet the frequency of 2.5 kHz. Namely, 2.5 kHz band noises caused by pressure pulsation attenuate also in both of first communication passage 142 and second communication passage 143. The 2.5 kHz band noises are thus further suppressed to propagate into enclosed container 101. The configuration can prevent 2.5 kHz band noises from propagating from suction muffler 140 into enclosed container 101. Noises caused by resonance of 2.5 kHz band in enclosed container can be thus prevented.
Additionally, first communication passage 142 has the resonance frequency of approx. 750 Hz and second communication passage 143 has the resonance frequency of approx. 1.2 kHz respectively. Both of these frequencies do not meet any one of the primary natural frequency of movable valve 133 of approx. 250 Hz and the secondary natural frequency of approx. 500 Hz. Therefore, though having a large energy close to fundamental wave energy, the pressure pulsations generated by opening/shutting movements of movable valve 133 to suck refrigerant gas R134a into compression chamber 122 attenuate in first communication passage 142 and second communication passage 143 resulting in the pressure pulsations being suppressed at a low level when released in enclosed container 101.
On the other hand, upon operation of the compressor, movable valve 133 opens and shuts suction hole 134 in response to the reciprocating movements of piston 130. In this regard, movable valve 133 performs plural opening/shutting movements per one reciprocating motion of piston 130 according to its own natural frequency. At the instant when movable valve 133 opens to suck the refrigerant gas into compression chamber 122, negative pressure waves are generated in the vicinity of suction hole 134. The negative pressure waves propagate through first communication passage 142 and reflect at first opening 142a to return back soon in the vicinity of suction hole 134 after being converted to positive pressure waves. Consequently, the pressure adjacent to movable valve 133 increases contrarily.
Therefore, an integral multiple of the natural frequency of movable valve 133 is adopted for the resonance frequency ratio determined by the length and diameter of first communication passage 142. Then, opening/shutting timing of movable valve 133 is tuned in the pressure wave in first communication passage 142. Consequently, the pressure adjacent to movable valve 133 can be increased while movable valve 133 opens. Namely, a supercharging effect can be expected.
Consequently, efficiency of the hermetic compressor increases because refrigerant gas volume sucked into compression chamber 122 increases to improve the suction efficiency due to the aforementioned supercharging effect. In addition, first communication passage 142 is inflected with an angle of approx. 50 degrees. The structure can reduce the flow resistance of refrigerant gas. The angle is preferably not smaller than 0 deg. and not larger than 60 deg., and the flow resistance runs up rapidly if the angle exceeds 75 degrees.
Moreover, first opening 142a of first communication passage 142 and second opening 143a of second communication passage 143 open adjacent each other in room B 140b. The structure allows refrigerant gas R134a to be sucked into room B 140b of suction muffler 140 from second communication passage 143 to be drawn into compression chamber 122 through first communication passage 142 via suction valve 134 with little heat received. Dense refrigerant gas, therefore, can be drawn into compression chamber 122 to provide a highly efficient compression performance.
Needless to say, other refrigerant gas than R134a adopted in the description can perform the same purpose of this invention.
The present invention provides a hermetic compressor that can reduce noise emission caused by cavity resonance in the enclosed container and to have a highly efficient compression performance due to reduced heat influence on refrigerant gas.
Number | Date | Country | Kind |
---|---|---|---|
2001-371248 | Dec 2001 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/JP02/12637 | 12/3/2002 | WO | 00 | 3/12/2004 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO03/048574 | 6/12/2003 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
5228843 | Novolan et al. | Jul 1993 | A |
5496156 | Harper et al. | Mar 1996 | A |
5734134 | Park | Mar 1998 | A |
6186751 | Rigo | Feb 2001 | B1 |
6206655 | Tanaka et al. | Mar 2001 | B1 |
6415888 | An et al. | Jul 2002 | B1 |
6547032 | Yoon et al. | Apr 2003 | B1 |
6547535 | Kueon | Apr 2003 | B1 |
6692238 | Myung et al. | Feb 2004 | B1 |
Number | Date | Country |
---|---|---|
0 897 060 | Feb 1999 | EP |
0 984 162 | Mar 2000 | EP |
2000-130147 | May 2000 | JP |
Number | Date | Country | |
---|---|---|---|
20040241011 A1 | Dec 2004 | US |