1. Field of the Invention
The invention relates generally to multi-cylinder compressors for use in air conditioning systems for vehicles. More particularly, the invention relates to multi-cylinder compressors having a plurality of suction ports formed through a valve plate, in which the suction ports are spaced from each other so as to reduce noise or vibration, or both, generated by the compressor.
2. Description of Related Art
Referring to
Compressor 1 also includes a rotor 21, a crank chamber 30, and a swash plate 13. Specifically, rotor 21 is fixed to drive shaft 10, such that drive shaft 10 and rotor 21 rotate together. Crank chamber 30 is formed between front housing 17 and cylinder block 16, and swash plate 13 is positioned inside crank chamber 30. Swash plate 13 is slidably connected to each piston 25 via a pair of shoes 14 positioned between swash plate 13 and each of pistons 25. Swash plate 13 includes a penetration hole 13c formed therethrough at a center portion of swash plate 13, and drive shaft 10 extends through penetration hole 13c. Rotor 21 includes a pair of rotor arms 21a, and a pair of oblong holes 21b formed through rotor arms 21a, respectively. Swash plate 13 further includes a pair of swash plate arms 13a, and a pair of pins 13b extend from swash plate arms 13a, respectively. A hinge mechanism 19 includes rotor arms 21a, swash plate arms 13a, oblong holes 21b, and pins 13b, and rotor 21 is connected to swash plate 13 by hinge mechanism 19. Specifically, one of pins 13b is inserted into and slidably engages an inner wall of one of oblong holes 21b, and another of pins 13b is inserted into and slidably engages an inner wall of another of oblong holes 21b. Moreover, because each of pins 13b is slidably disposed within their corresponding oblong hole 21b, the tilt angle of swash plate 13 may be varied with respect to drive shaft 10, such that the fluid displacement of compressor 1 also may be varied.
Compressor 1 further includes a valve plate 40 having a vertical center axis 110 which is perpendicular to axis 20 of drive shaft 10, a discharge chamber 70, a suction chamber 80, and a suction gas inlet passage 60. Suction chamber 80 extends around discharge chamber 70. Moreover, valve plate 40 has a plurality of cylinder suction ports 90 and a plurality of discharge ports 101 formed therethrough. Specifically, referring to
Compressor 1 also may include an electromagnetic clutch (not shown). When the electromagnetic clutch is activated, a driving force from an external driving source (not shown) is transmitted to drive shaft 10, such that drive shaft 10, rotor 21, and swash plate 13 rotate about axis 20 of drive shaft 10. Moreover, swash plate 13 also moves back and forth in a wobbling motion, such that only movement in a direction parallel to axis 20 of drive shaft 10 is transferred from swash plate 13 to pistons 25. Consequently, each piston 25 reciprocates within its corresponding cylinder bore 16a. In operation, a fluid, e.g., a refrigerant, is introduced into suction chamber 80 via suction gas inlet passage 60. During a suction stroke of piston 25, the fluid flows through the corresponding suction port 90 into a corresponding compression chamber 50 which is formed by a top portion of a corresponding piston 25, the walls of a corresponding cylinder bore 16a, and valve plate 40. The fluid subsequently is compressed by piston 25 during a compression stroke, and the compressed fluid flows into discharge chamber 70 via discharge ports 101.
Nevertheless, during the operation of compressor 1, dynamic pressure pulsations in suction chamber 80 are generated by the reciprocating motion of pistons 25, and the dynamic pressure pulsations pass to compression chamber 50 during the suction stroke of pistons 25. Such dynamic pressure pulsations reduce a performance of compressor 1, and also increase noise or vibration, or both, within compressor 1. The dynamic pressure pulsations also may affect a timing of an opening or a closing, or both, of a suction valve (not numbered). In attempting to decrease this noise, vibration, or both, a method of designing such known, multi-cylinder compressors includes the steps of kinematically determining a mass flow rate within suction chamber 80, i.e., a mass of a fluid delivered to suction chamber 80 per unit of time. Moreover, based on known relationships for determining dynamic pressure pulsations in suction chamber 80, the method also includes the steps of increasing a depth 120 of suction chamber 80, and increasing a width 130 of suction chamber 80, in which a cross-sectional area of suction chamber 80 equals depth 120·width 130. Further, based on the known relationships, the method includes the step of increasing a mean radius of suction chamber 80, in which suction chamber 80 has a varying radius measured from a center of discharge chamber 70. Specifically, depth 120, width 130, and the mean radius of suction chamber 80 are inverse factors of the known relationship. Consequently, when the kinematic mass flow rate is factored into the relationship, increasing any of depth 120, width 130, and the mean radius of suction chamber 80 theoretically decreases the dynamic pressure pulsations within suction chamber 80.
Therefore, a need has arisen for multi-cylinder compressors which overcome these and other shortcomings of the related art. A technical advantage of the present invention is that the suction ports may be spaced from each other so as to reduce noise or vibrations, or both, generated by the compressor. Another technical advantage of the present invention is that the mean radius of the suction chamber and the diameter of the suction gas inlet passage may be selected so as to reduce noise or vibrations, or both, generated by the compressor. Specifically, the mean radius of the suction chamber and the diameter of the suction gas inlet passage may be selected such that each frequency component of a mass flow rate within the suction chamber is not within a predetermined range, e.g., 25 Hz, of at least one resonant frequency of the suction chamber.
In an embodiment of the present invention, a multi-cylinder compressor is described. The compressor comprises a valve plate having a plurality of cylinder suction ports formed therethrough, and a plurality of cylinder bores centered on an arc having a radius (R). The cylinder bores are substantially equally spaced from each other, and have a diameter (D). The compressor also comprises a suction chamber having a substantially annular shape and adapted to be in fluid communication with each of the cylinder bores via the suction ports. Moreover, a center of a first of the suction ports is radially offset in a predetermined direction from a center of a predetermined suction port by a first angle, in which the predetermined suction port has a diameter (d), and the first angle equals {[(360°/N)·([N−1]−n)]+X°}. In this formula, N is a number of the suction ports formed through the valve plate, n is a number of the suction ports positioned between the first suction port and the predetermined suction port in a direction opposite to the predetermined direction, and X° is a predetermined angle which is less than or equal to {(sin−1[(D−d)/2·R])·57.3°/Radian} and greater than or equal to −{(sin−1[(D−d)/2·R]·57.3°/Radian}, and which is not equal to 0°. Specifically, Radians may be converted into degrees using a conversion factor equal to (630/11)°/Radian, i.e., about 57.3°/Radian.
In another embodiment of the present invention, a suction manifold joining a plurality of cylinders in a suction chamber is described. The suction manifold comprises a plurality of cylinder bores centered on an arc having a radius (R). The cylinder bores are substantially equally spaced from each other, and have a diameter (D). The suction manifold also comprises a valve plate comprising a plurality of cylinder suction ports formed therethrough. Moreover, a center of a first of the suction ports is radially offset in a predetermined direction from a center of a predetermined suction port by a first angle, in which the predetermined suction port has a diameter (d), and the first angle equals {[(360°/N)·([N−1]−n)]+X°}. In this formula, N is a number of the suction ports formed through the valve plate, n is a number of the suction ports positioned between the first suction port and the predetermined suction port in a direction opposite to the predetermined direction, and X° is a predetermined angle which is less than or equal to {(sin−1[(D−d)/2·R]·57.3°/Radian} and greater than or equal to −{(sin−1[(D−d)/2·R]57.3°/Radian}, and which is not equal to 0°.
In yet another embodiment of the present invention, a multi-cylinder compressor is described. The compressor comprises a valve plate having a plurality of cylinder suction ports formed therethrough, in which a first suction port is positioned adjacent to a second suction port, and the second suction port is positioned adjacent to a third suction port. The compressor also comprises a plurality of cylinder bores, and a suction chamber having a substantially annular shape and adapted to be in fluid communication with each of the cylinder bores via the suction ports. Moreover, the second suction port is radially offset from the first suction port by a first angle, and the third suction port is radially offset from the second suction port by a second angle, in which the first angle is greater than or less than, but not equal to, the second angle.
In still another embodiment of the present invention, a valve plate assembly is described. The valve plate assembly comprises a valve plate having a plurality of cylinder suction ports formed therethrough. A first suction port is positioned adjacent to a second suction port, and the second suction port is positioned adjacent to a third suction port. Moreover, the second suction port is radially offset from the first suction port by a first angle, and the third suction port is radially offset from the second suction port by a second angle, in which the first angle is greater than or less than the second angle.
In still yet another embodiment of the present invention, a method of designing a multi-cylinder compressor is described. The compressor comprises a valve plate having a plurality of cylinder suction ports formed therethrough, and a plurality of cylinder bores. The compressor also comprises a suction chamber having a substantially annular shape and adapted to be in fluid communication with each of the cylinder bores via the suction ports, in which the suction chamber has a varying radius. The compressor further comprises a suction gas inlet passage connected to the suction chamber. The method comprises the steps of selecting an operating speed for the compressor, selecting a depth for the suction chamber, selecting a width for the suction chamber, and selecting a first mean radius for the suction chamber. The method also comprises the steps of selecting a first diameter for the suction gas inlet passage, and determining a frequency response of a mass flow rate within the suction chamber. Moreover, the method comprises the step of determining a first dynamic pressure response within the suction chamber.
Other objects, features, and advantages of the present invention will be apparent to persons of ordinary skill in the art in view of the following detailed description of the invention and the accompanying drawings.
For a more complete understanding of the present invention, the needs satisfied thereby, and the objects, features, and advantages thereof, reference now is made to the following descriptions taken in connection with the accompanying drawings.
a is a graph of a frequency response of a mass flow rate in a suction chamber, and
Preferred embodiments of the present invention and their advantages may be understood by referring to
Referring to
Compressor 100 also includes a rotor 21, a crank chamber 30, and a swash plate 13. Specifically, rotor 21 is fixed to drive shaft 10, such that drive shaft 10 and rotor 21 rotate together. Crank chamber 30 is formed between front housing 17 and cylinder block 16, and swash plate 13 may be positioned inside crank chamber 30. Swash plate 13 may be slidably connected to each piston 25 via a pair of shoes 14 positioned between swash plate 13 and each of pistons 25. Swash plate 13 may include a penetration hole 13c formed therethrough at a center portion of swash plate 13, and drive shaft 10 may extend through penetration hole 13c. Rotor 21 includes a pair of rotor arms 21a and a pair of oblong holes 21b formed through rotor arms 21a, respectively. Swash plate 13 further may include a pair of swash plate arms 13a and at least one pin 13b extending from swash plate arms 13a. A hinge mechanism 19 includes rotor arms 21a, swash plate arms 13a, oblong holes 21b, and pin 13b, and rotor 21 may be connected to swash plate 13 by hinge mechanism 19. Moreover, the tilt angle of swash plate 13 may be varied with respect to drive shaft 10, such that the fluid displacement of compressor 100 also may be varied.
Compressor 100 further may include a valve plate 40 having a vertical center axis 110, a discharge chamber 70, a suction chamber 80, and a suction gas inlet passage 60. Suction chamber 80 may have a substantially annular shape, and may extend around discharge chamber 70. In an embodiment, suction chamber 80 may have a varying radius, and a mean radius (r) of suction chamber 80 may be between about 46 mm and about 54 mm. Further, suction gas inlet passage 60 may have a diameter (Di) between about 6 mm and about 14 mm. Moreover, valve plate 40 may have a plurality of cylinder suction ports 900, e.g., suction ports 900a–900g in a seven-cylinder compressor, and a plurality of discharge ports 101 formed therethrough. As shown in
Referring to
In an embodiment, angle θx may equal {[(360°/N)·([N−1]−n)]+Xx°}, in which N is a number of suction ports 900 formed through valve plate 40, e.g., seven suction ports 900, n is a number of suction ports 900 positioned between a particular suction port 900a–900g which is associated with angle θx and suction port 900a in a direction opposite to the predetermined direction, e.g., a counterclockwise direction, and Xx° is a predetermined angle, e.g., a predetermined angle X1°–X6°. For example, θ1 may equal {[(360°/N)·([N−1]−n)]+X1°}, θ2 may equal {[(360°/N)·([N−1]−n)]+X2°}, θ3 may equal {[(360°/N)·([N−1]−n)]+X3°}, θ4 may equal {[(360°/N)·([N−1]−n)]+X4°}, θ5 may equal {[(360°/N)·([N−1]−n)]+X5°}, and θ6 may equal {[(360°/N)·([N−1]−n)]+X6°}. If each of predetermined angles X1°–X6°=0°, center portions 950a–950g may be equiangularly centered on radius (R), e.g., as shown in
Referring to
For example, if the predetermined direction is clockwise, and the particular suction port 900a–900g which is associated with angle θx is suction port 900d, i.e., when θx is θ3, then θ3 in the clockwise direction equals {[(360°/7)·([7−1]−3)]+X3°}={[3·(360°/7)]+X3°}. Specifically, suctions ports 900e, 900f, and 900g are positioned between suction port 900d and suction port 900a in a direction opposite to the predetermined direction, i.e., in the counterclockwise direction. Similarly, if the predetermined direction is counterclockwise, and the particular suction port 900a–900g which is associated with angle θx is suction port 900d, i.e., when θx is θ3, then θ3 in the counterclockwise direction equals {[(360°/7)·([7−1]−2)]+X3°}={[4·(360°/7)]+X3°}. Specifically, suctions ports 900b and 900c are positioned between suction port 900d and suction port 900a in a direction opposite to the predetermined direction, i.e., in the clockwise direction.
Referring to
In this embodiment, a first of suction ports 900 may be positioned adjacent to a second of suction ports 900, and the second of suction ports 900 may be positioned adjacent to a third of suction ports 900. Moreover, the angle formed between the first of suction ports 900 and the second of suction ports 900 may be different than, i.e., greater than or less than, the angle formed between the second of suction ports 900 and the third of suction ports 900. For example, angle θa may be greater than or less than angle θb, or angle θb may be greater than or less than angle θc, or angle θc may be greater than or less than angle θd, or angle θd may be greater than or less than angle θe, or angle θe may be greater than or less than angle θf, or angle θf may be greater than or less than angle θg, or angle θg may be greater than or less than angle θa, and combinations thereof. In an embodiment, the angle formed between the first suction port 900, e.g., suction port 900c, and the second suction port 900, e.g., suction port 900d, may be between about 10° and about 30° greater than the angle formed between the second suction port 900 and the third suction port 900, e.g., suction port 900e. In another embodiment, the angle formed between the first suction port 900 and the second suction port 900 may be between about 10° and about 30° less than the angle formed between the second of suction ports 900 and the third of suction ports 900. Nevertheless, it will be understood by those of ordinary skill in the art that a maximum difference between the angle formed between the first suction port 900 and the second suction port 900, and the angle formed between the second suction port 900 and the third suction port 900 depends on a position of cylinder bores 16a, the diameter (D) of cylinder bores 16a, the diameter (d) of suction ports 900, and the number of cylinder bores 16a. Specifically, the difference between the angle formed between the first suction port 900 and the second suction port 900, and the angle formed between the second suction port 900 and the third suction port 900, may not position suction ports 900 outside their corresponding cylinder bore 16a.
Referring to
In step 812, a first frequency response of a mass flow rate within suction chamber 80 is determined. The first frequency response of the mass flow rate within suction chamber 80 may depend on the operating speed of compressor 100, the depth of suction chamber 80, the width of suction chamber 80, the first mean radius of suction chamber 80, the first diameter of suction gas inlet passage 60, and the number of suction ports 900. Referring to
Further, the first resultant simulated pressure pulsation response in suction chamber 80 may be compared to an experimentally obtained pressure pulsation response, and the kinematic mass flow rate associated with each suction port 900 may be adjusted iteratively in order to match the first resultant simulated pressure pulsation amplitudes with the experimentally obtained pressure pulsation amplitudes to obtain a first modified mass flow rate. Simulation method 110 may continue, e.g., the first modified flow rate may be adjusted to a second modified flow rate based on a comparison between a second resultant simulated pressure pulsation response and the experimentally obtained pressure pulsation response, until a particular resultant simulated pressure pulsation response amplitudes match the experimentally obtained pressure pulsation response amplitudes. When the particular resultant simulated pressure pulsation response amplitudes match the experimentally obtained pressure pulsation response amplitudes, an actual modified mass flow rate is determined. For example, the first modified mass flow rate at a particular frequency within a frequency spectrum may be equal to the kinematic mass flow rate plus an oscillation component, in which the oscillation component equals a scaler component {acute over (α)} times an error between the resultant simulated pressure pulsation response and the experimentally obtained pressure pulsation response at the particular frequency. The first modified mass flow rate may be determined at each frequency within the frequency spectrum. Moreover, the scaler component {acute over (α)} and the error may be different at each frequency. Specifically, the error may be positive or negative depending on whether the resultant simulated pressure pulsation response is greater than or less than the experimentally obtained pressure pulsation response at that particular frequency. Similarly, the second modified mass flow rate at the particular frequency within the frequency spectrum may be equal to the first modified mass flow rate plus the oscillation component. Referring to
In step 814, a first dynamic pressure response within suction chamber 80 is determined. For example, the first dynamic pressure response within suction chamber 80 may depend on the actual modified mass flow rate. Specifically, after the actual modified mass flow rate is determined, simulation method 110 may be employed using the actual modified mass flow rate to determine first dynamic pressure response. Simulation method 110 operates substantially the same as described-above respect to determining the actual modified mass flow rate, except that the mass flow rate used in simulation 110 is not adjusted, and simulation 110 continues until the pressure pulsations associated with each suction port 900 have been determined and summed using a superposition technique to produce the first dynamic pressure pulsation response. In another embodiment of the present invention, method 800 further may comprise steps 816 and 818. In step 816, the first mean radius of suction chamber 80 is changed to a second mean radius, or the first diameter of suction gas inlet passage 60 is changed to a second diameter, or both. In step 818, a second dynamic pressure response within suction chamber 80 may be determined. Because the first mean radius of suction chamber 80 is different than the second mean radius of suction chamber 80, or because the first diameter of suction gas inlet passage 60 is different than the second diameter of suction gas inlet passage 60, or both, the second dynamic pressure response may be different than the first dynamic pressure response.
The above-described method may be repeated for a predetermined number of mean radiuses for suction chamber 80, e.g., five different mean radiuses for suction chamber 80, and for a predetermined number of diameters for suction gas inlet passage 60, e.g., five different diameters for suction gas inlet passage 60. Moreover, a dynamic pressure response within suction chamber 80 may be determined for each combination of suction chamber 80 mean radius and suction gas inlet passage 60 diameter, and compressor 100 may be designed based on the various dynamic pressure responses. For example, the mean radius of suction chamber 80 and the diameter of suction gas inlet passage 60 may be selected so as to minimize the dynamic pressure response within suction chamber 80 within the predetermined range of frequencies, e.g., between about 400 Hz and about 600 Hz.
While not willing to be bound by a theory, it is believed that the dynamic pressure response for a single suction port 900 may be expressed by the following formula:
in which r is the mean radius of suction chamber 80, A is the cross-sectional area of suction chamber 80, i.e., A=depth 120·width 130, c is the speed of sound in a gas, ρ is the density of fluid within suction chamber 80, Q(nω) is the mass flow rate of fluid within suction chamber 80 transformed into the frequency domain as a volume flow rate, TQn (ω) is a transfer function between a flow rate at suction gas inlet passage 60 and suction port 900, i.e., TQn (ω)=Q2n/Q1n, in which Q2n is the volume flow rate at suction port 900 and Q1n is the volume flow rate at suction gas inlet passage 60, N is a number of suction ports 900, ζk is a modal damping ratio for each modek, θ1 is an angle of a center of suction gas inlet passage 60, and θ2 is an angle of center portion 950 of suction port 900. When any of depth 120, width 130, and the mean radius of suction chamber 80 increase, the denominator of the above-described formula increases. Nevertheless, based on the formula TQn(ω)=Q2n/Q1n, Q2n(nω)/TQn(nω)=Q1n, i.e., the volume flow rate at suction gas inlet passage 60. Consequently, increasing the diameter of suction gas inlet passage 60 also may increase the numerator of the above-described formula. Further, for some increases in the diameter of suction gas inlet passage 60, the increase in the numerator may be greater than the increase in the denominator. Moreover, changes in θ2 for any one of suction ports 900 also may affect the numerator in the above-described formula, which may cause pressure pulsations to increase or decrease depending on the change in θ2.
Embodiments of the present invention will be further clarified by consideration of the following examples, which are intended to be purely exemplary of the invention.
Referring to
Referring again to
Moreover, as shown in
Referring to
While the invention has been described in connecting with preferred embodiments, it will be understood by those of ordinary skill in the art that other variations and modifications of the preferred embodiments described above may be made without departing from the scope of the invention. Other embodiments will be apparent to those of ordinary skill in the art from a consideration of the specification or practice of the invention disclosed herein. It is intended that the specification and the described examples are considered as exemplary only, with the true scope and spirit of the invention indicated by the following claims.
This application claims the benefit of U.S. Provisional Patent Application No. 60/407,978, filed Sep. 5, 2002, which is incorporated herein by reference.
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