Axial flow fluid compressor

Abstract: A compressor includes a cylinder (5), and a roller piston (6) located in the cylinder, and a helical groove formed on the outer periphery of the piston. A helical blade (9) is fitted in the groove and divides the space between the inner periphery of the cylinder and the outer periphery of the piston into operating chambers (8) which have volumes gradually decreasing with distance from one end of the cylinder. The helical blade (9) has dimensions satisfying the following formula: (1+µ²) (α/β) < (L+µB) in which B: axial width, T: radial height, L: exposed height, and µ: frictional coefficient, and in which α = (B²+2TL-L²)/2+{-B²(1-µ²)+µBT+µ²TL}/(1-µ²) β = T-L+{ µB(1+µ²)+(2µ(µ(µT-B)}/(1-µ²)

Description: This invention relates to fluid compressors of the type which can be used in the refrigerating apparatus of a refrigerator or air conditioner. In the refrigerating apparatus, the compressor is used to compress the refrigerating medium. Reciprocating compressors and rotary compressors are known to be suitable compressors for this function. Recently a new type of axial flow compressor has been developed in which a helical blade is employed. A feature of this type of compressor is that it has a reduced number of parts and an improved compression efficiency, as compared with the prior art compressors. Compressors of this type are disclosed in US-A-2401189, US-A-4871304, US-A-4872820 and US-A-4 875 842. Claim 1 is characterised by reference to US-A-4875842. The helical blade is fitted in a helical groove at the periphery of a rotatable piston and the blade is freely movable in the radial direction in the groove. In use, the helical blade separates high and low pressure regions, respectively, and can experience elastic deformation. For this reason, the helical blade is affected by the force caused by the pressure difference between high and low pressure regions. Because of this force, the helical blade tends to deform, wear, break and/or to reduce the durability thereof. Accordingly, an object of this invention is to provide a compressor of this type with a helical blade of greater durability. According to a first aspect of the present invention, a fluid compressor comprises a rotatable cylinder; means for rotating the cylinder; a roller piston mounted in an eccentric manner in the cylinder and rotatable in synchronism with said cylinder; a helical groove formed in the peripheral surface of said piston; and a helical blade accommodated in said groove and in contact with the cylinder; said blade being freely movable in said groove radially of the piston, wherein said helical blade has a width B in the direction along the axis of said roller piston and a maximum exposed height L max measured above said helical groove, characterised in that the width B satisfies the following formula: B > L max. According to a second aspect of the present invention, a fluid compressor comprises a rotatable cylinder; means for rotating the cylinder; a roller piston mounted in an eccentric manner in the cylinder and rotatable in synchronism with said cylinder; a helical groove formed in the peripheral surface of said piston; and a helical blade accommodated in said groove and in contact with the cylinder; said blade being freely movable in said groove radially of the piston, wherein said helical blade has a width B in the direction along the axis of said roller piston, a height T in the direction perpendicular to said axial direction, and exposed height L measured above said helical groove, and a frictional coefficient µ; characterised in that the width B satisfies the following formula: (1+µ²)(a/β) < (L+µβ) in which a = (B²+2TL-L²)/2 + {-B²(1-µ²)+µBT+µ²TL}/(1-µ²) β = T-L+{µB(1+µ²)+2µ(µT-B)}/(1-µ²), respectively. In order that the invention may be more readily understood, it will now be described, by way of example only, with reference to the accompanying drawings, in which:- Figure 1 is a longitudinal sectional view showing the general construction of the compressor in accordance with the invention; Figure 2 is a side view showing the roller piston component of the compressor shown in Figure 1, in accordance with the invention; Figure 3 is a side view showing the helical blade component of the compressor of Figure 1; Figure 4 is a longitudinal sectional view of the compressor mechanism sub-assembly of the compressor of Figure 1; Figure 5 is an enlarged schematic view of the portion of the roller piston on which the helical blade is mounted; Figure 6 is an enlarged schematic view of the portion of the roller piston on which the helical blade is mounted showing a distribution of pressure forces around the helical blade; Figure 7 is an enlarged schematic view of the roller piston portion on which the helical blade is mounted showing counter forces acting on the helical blade; Figure 8 is a graph showing variation of counter forces on the blade when the width of the helical blade is changed; Figure 9 is an enlarged schematic view of the roller piston portion on which the helical blade is mounted showing the counter forces acting on the helical blade when width of helical blade is designed so as to make the counter force F₁ zero; Figure 10 is a graph showing variation of the largest blade surface force according to the width of the blade; and Figures 11a, 11b and Figures 12a and 12b are enlarged schematic cross-sectional views of the helical blade to describe experimental results. Referring to Figure 1, a compressor 1 has a closed casing 2, a compressor mechanism 3 accommodated in the closed casing 2, and an electric motor 4 providing rotating power to the compressor mechanism 3. The compressor mechanism 3 has a cylinder 5 in the form of a sleeve, with a roller piston 6 accommodated in said cylinder 5 and arranged in an eccentric manner relative to the central axis of the cylinder. A helical groove 7 is formed in the periphery of roller piston 6 so as to have decreasing pitch in the direction of the discharge end of the compressor (left-hand end in the figure), a helical blade 9 is mounted in said helical groove in a manner to move freely in and out in the radial direction to form compressing spaces 8 between the inner wall of the cylinder 5 and the piston surface, which spaces become smaller towards the left side in the figure. The radial movement of the blade in the groove and the eccentric location of the roller piston enables a portion of the periphery of the piston to engage with the inner peripheral wall of the cylinder in a linear manner in the axial direction of the piston and cylinder. Journal bearings 10a and 10b support opposite ends of the cylinder 5 and are fixed oppositely each each in the inner wall of said casing, with sliding journal bearings 12a and 12b being formed in the body of said journal bearings 10a and 10b and supporting stub shafts 11a and 11b projecting from the ends of the roller piston. Tally pin 13 projecting radially internally from the cylinder is provided to rotate roller piston 6 synchronously with the cylinder 5, and a tally hole 14 is formed on the roller piston 6. Further, the space 26 at the left-hand side of the figure and formed with the cylinder 5 and the roller piston 6 communicates through a hole 15 formed in a portion of the journal bearing 10a to the space 16 in which electric motor 4 is provided within the casing 2. Also, the space 27 at the right-hand side of Figure 1 communicates through the hole 17 formed in a portion of the journal bearing 10b to the low pressure gas supply tube 18. The electric motor 4 is an induction motor and is comprised of rotor 19 fixedly mounted on the external surface of the cylinder, and a stator 20 is arranged outside the rotor 19 and affixed on the internal surface of the casing 2. Further, in Figure 1, discharge tubing to discharge compressed gas is shown by reference 23 and lubricant oil to lubricate the journal bearings is shown by reference 24. The helical blade 9 is, as shown in Figure 3, made of solidified artificial resin of the types to be discussed hereinafter and is mounted in the helical groove 7 formed on the roller piston, as shown in Figure 4. Figure 5 is an enlarged cross-sectional view of the portion designed "A" in Figure 4. In the helical blade 9, in Figure 5, the side surface portion in the lower pressure side, shown as 30, is the portion most susceptible to wear. Thus, during operation, the helical blade 9 is apt to press against the lower pressure side in the slant condition and to be supported at three points (a, b and c) by the pressure difference, as shown in Figure 6. In this condition, around the helical blade 9, the following pressures occur:- high pressure P₁ on the high pressure side, a high pressure P₁ as a back pressure on the surfaces accommodated in the groove 7, a low pressure P₂ and a high pressure P₁ from a back pressure on the low pressure surface and a low pressure P₂ on the surface opposite to the internal surface of the cylinder. Also, at the three supporting points (a, b, and c), concentrated reaction forces F₁, F₂ and F₃ act as counter forces from cylinder 5 and roller piston 6, as shown in Figure 7. Further, on the helical blade, frictional forces act in accordance with the reaction force F₁, F₂ and F₃, respectively. Frictional forces are defined as µF₁, µF₂ and µF₃ respectively when the frictional coefficient is defined by µ. The instantaneous directions of the frictional forces change by the relative motion among helical blade 9, cylinder 5 and roller piston 6 in one rotation cycle of the compressor mechanism and the distribution of forces at one instant of time is shown in Fig. 7. These frictional forces act on the helical blade, and by these forces low pressure side as shown at 30 is subject to increased wear except for embodiments in accordance with the present invention. Specifically, in this embodiment of the present invention, wear is suppressed by designing cross-sectional form of the helical blade 9 as follows: In Fig. 7, the balance equation of the forces and the moments are described as follows: Balance of forces: P₁T + F₁ + µF₃ = P₂L + P₁(T-L) + F₂ P₂B + F₃ + µF₂ + µF₁ = P₁B wherein in the units of F₁, F₂ and F₃ in above equations (1) and (2) are kgf/m Balance of moments: Further, assume the following dimension of the blades: T - blade height; L - exposed height; B - blade width; respectively. In this case, exposed height L varies between zero and the difference of the dimensions between the cylinder inner diameter and the outer diameter of roller piston during one rotation in the operation of the compressor. Thus, when the pressure P₁ and P₂, blade dimension T, L and B and frictional coefficient are given, counter forces F₁, F₂ and F₃ received by blade are calculated from aforesaid three formulas (1), (2) and (3), as following formulas: F₂ = (α/β)(P₁-P₂) F₃ = {-2µF₂+(B+µL)(P₁-P₂)}/(1-µ²) F₁ = {(1+µ²)F₂-(L+µB)(P₁-P₂)}/(1-µ²) wherein; α = (B²+2TL-L²)/2 + {-B²(1-µ²)+µBT+µ²TL}/(1-µ²) β = T-L+{ µB(1+µ²)+2µ(µT-B)/(1-µ²). Now, when pressures P₁ and P₂ and blade dimensions T and L are given, reaction forces F₁, F₂ and F₃ are given as a function of blade width as shown in Fig. 8. In accordance with an increase of blade width B, since the effect of the moment of reaction force F₃ increases, reaction forces F₁ and F₂ become small. Thus at the borderline of the width of blade B where F₁0, the mode of the reaction forces varies as shown in Fig. 9, with the reaction forces changing from concentrated forces to distributed forces. When the reaction force changes to such a distributed condition, compression operation can be continued without causing excess blade wear. The condition for the force change is given from equation (6) as follows: (1+µ²)(α/β)<(L+µB) In Fig. 10, there is shown an example in which reaction force F₂ changes to a distributed force from a concentrated force as a function of blade width B. For the pressure difference (P₁-P₂) = 3.2 Kgf/cm² , and blade dimensions T(variable), L = 1.8mm, and frictional coefficient µ = 0.1, the threshold value of blade width B for the change is given at B = 2.2mm. When using a blade having larger width than that value, F₁ becomes zero and F₂ becomes a distributed load and is able to improve durability of the helical blade. According to the present invention the dimension of the cross-section of the helical blade 9 is also designed as follows. For µ = o (there is no friction between the blade and the piston), the equation (1) is changed as follows; B = B₀ > L max For µ > o (there is some friction), the equation (8) is changed as follows; B > B₀ Therefore the present invention is characterized in that the helical blade has a width B in the direction along the axis of the roller piston, wherein the width B is at least always greater than the maximum value of the exposing height from the helical groove L max, that is, B > L max. The helical blade according to present invention is preferably made of the solidified artificial resin materials described hereunder. (1) Heat resisting high molecular weight compounds such as polyimides, polyamideimides, and polyetherketones. (2) Fluorine-contained polymers including liquid crystal polymer as reinforcing-members such as aromatic polyamides and aromatic polyesters. (3) Fluorine-contained polymers including glass fibers as reinforcing-members and wherein the glass fibers are dissolved and removed from the surface of the blade with hydrofluoric acid. (4) Fluorine-contained polymers including glass fibers as reinforcing-members and the combination of at least one high molecular weight compound and a liquid crystal polymer, both of which are the same as described above, and wherein the glass fibers are dissolved and removed from the surface of the blade with hydrofluoric acid. Further, a metal facing plate can optionally be put on the helical blade made of the materials described above with the surface of the metal plate disposed for contacting the inner surface of the cylinder and/or the low pressure side of the rotor groove. Fig. 9 shows a schematic of a facing plate 32 (shown dotted) positioned on blade 9 to contact the low pressure side of helical groove 7. Generally, facing plate 32 can be 10-20% of the width B of blade 9 and should be formed of a metal exhibiting low frictional resistance to sliding movement against the material of rotor piston 6. In the following, the operation of the compressor in accordance with the afore-said description will be described. When the electric motor 4 is caused to rotate, cylinder 5 rotates at the same rotating speed as that of rotor 19 of said motor. Also, roller piston 6 rotates synchronously with cylinder 5 by means of the tally function of tally pin 13 and tally hole 14. As stated before, the longitudinal axis of the roller piston 6 is offset by a distance e from the longitudinal axis of the cylinder 5 (see Figure 1), and also the helical blade is provided such as to move freely radially in and out from the helical groove, the blade decreasing in pitch in the direction from the suction side of the compressor (right side in Figure 1). Therefore, the compression space 8 defined by the cylinder 8, the roller piston 6 and the helical blade 9 moves towards left side of Figure 1 so as to reduce its volume and consequently a low pressure gas inhaled from right end space 27 is compressed as it moves to the left-hand space 26. The compressed gas thus moved is discharged through hole 15 into space 16 in the casing and thus the function of the compressor is provided. Further, when, as in this case, the cross-sectional dimensions of the helical blade are designed to satisfy equation (7), the durability of the helical blade 9 can be improved. Figure 11 shows the performance in terms of changes in the cross-section of the helical blade after testing conducted in an actual machine. Fig. 11(a) shows the case of F₁ > 0 and in this case wear of 0.16mm is observed after 100 hours of operation. Also Fig. 11(b) shows the case of F₁ = 0, thus satisfying equation (7), wear of 0.09mm only is observed after 100 hours of operation. From these facts, the usefulness of the present invention may be understood. While the relationship defined by equations (8) and (9) are helpful for initial design considerations and for very low friction coefficients, the following examples demonstrate the surprising results achievable when the blade width is configured in accordance with the equation (7) for wear tests of the same duration. Figs. 12(a) and 12(b) present test results for a compressor rotor having dimensions of T = 3.4mm, L = 2.4mm and µ = 0.1. In Fig. 12(a), the blade width B was chosen based on the value obtained when the dimension values were substituted in the equation (1+µ²)(α/β) < (L+µB) and the requirement of B > 2.9mm was calculated. For the Fig. 12(a) test, B was selected to be ε 3.0mm and the wear observed (δ₁) was 0.06mm. For comparison, Fig. 12(b) is the case of B = 2.5mm, that is, satisfying the approximate design relationship B > L max of equations (8) and (9), and maximum amount of wear δ₂ was 0.12mm. Moreover, the distributed wear found in the Fig. 12(a) configuration test is clearly preferred to the cavity wear found in the Fig. 12(b) test. While the blade design configurations resulting from the application of approximate equations (8) and (9) are still highly useful and are to be preferred over the conventional blade constructions, the blade configurations resulting from the application of equation (7) are highly preferred, particularly for large values of µ.

Claims: A fluid compressor comprising a rotatable cylinder (5); means (4) for rotating the cylinder; a roller piston (6) mounted in an eccentric manner in the cylinder and rotatable in synchronism with said cylinder (5); a helical groove (7) formed in the peripheral surface of said piston (6); and a helical blade (9) accommodated in said groove (7) and in contact with the cylinder (5); said blade (9) being freely movable in said groove (7) radially of the piston (6), wherein said helical blade (9) has a width B in the direction along the axis of said roller piston (6) and a maximum exposed height L max measured above said helical groove (7), characterised in that the width B satisfies the following formula: B> L max. A fluid compressor according to claim 1, wherein said helical blade (9) has a height T in the direction perpendicular to said axial direction, and exposed height L measured above said helical groove (7), and a frictional coefficient µ; wherein the width B further satisfies the following formula: (1+µ²) (a/β) < (L+µβ) in which a = (B²+2TL-L²)/2 +{-B²(1-µ²)+µBT+µ²TL}/(1-µ²) β = T-L+{µB(1+µ²)+2µ(µT-B)}/(1-µ²), respectively. The fluid compressor according to claim 1 or 2, wherein the helical blade (9) is made of at least one material selected from the group consisting of heat resisting high molecular weight compounds, namely, polyimides, polyamideimides, and polyetherketones. The fluid compressor according to claim 1 or 2, wherein the helical blade (9) is made of at least one material selected from the group consisting of fluorine-contained polymers, the blade (9) further including liquid crystal polymers as reinforcing members. The fluid compressor according to claim 1 or 2, wherein the helical blade (9) is made of at least one material selected from the group consisting of fluorine-contained polymers, the blade (9) further including glass fibres as reinforcing members but with the glass fibres removed from the surface of the blade. The fluid compressor according to claim 3, 4 or 5, wherein the blade (9) is provided with a metal facing plate. The fluid compressor according to any preceding claim, wherein the value of L is about 1.8 mm to 2.4 mm and the value of µ is about 0.1. A fluid compressor comprising a rotatable cylinder (5); means (4) for rotating the cylinder; a roller piston (6) mounted in an eccentric manner in the cylinder and rotatable in synchronism with said cylinder; a helical groove (7) formed in the peripheral surface of said piston; and a helical blade (9) accommodated in said groove and in contact with the cylinder; said blade being freely movable in said groove radially of the piston, wherein said helical blade has a width B in the direction along the axis of said roller piston, a height T in the direction perpendicular to said axial direction, and exposed height L measured above said helical groove (7), and a frictional coefficient µ; characterised in the the width B satisfies the following formula: (1+µ²) (a/β) < (L+µβ) in which α = (B²+2TL-L²)/2 +{-B²(1-µ²)+µBT+µ²TL}/(1-µ²) β = T-L+{µB(1+µ²)+2µ(µT-B)}/(1-µ²), respectively.

Inventors: SUMIDA KAZUHISA C O INTELL PRO, SUMIDA, KAZUHISA, C/O INTELL. PROPERTY DIV.
Applicants: TOSHIBA KK, KABUSHIKI KAISHA TOSHIBA
Application year: 1992
Main classification: F04C18
IPC codes: F04C18