BACKGROUND OF THE INVENTION
1. Field of the Invention
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The present invention relates to a swash plate
type compressor. More particularly, the present
invention relates to a swash plate type compressor for
compressing gas when a single head piston, engaged with a
swash plate which is rotated together with a drive shaft,
via a pair of shoes, is linearly reciprocated in a
cylinder bore.
2. Description of the Related Art
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In general, in a swash plate type compressor
used for air conditioning in a vehicle, a swash plate is
attached to a drive shaft in a crank chamber, and a
rotational motion of the swash plate driven by the drive
shaft is converted into a reciprocating motion of single
head pistons inserted into respective cylinder bores.
Refrigerant gas, which has returned to the compressor
from an external refrigerating circuit, is sucked from a
suction chamber into the cylinder bore according to the
linear motion of the single head piston and is compressed
in the cylinder bore by the single head piston and then
discharged into a discharge chamber. In this swash plate
type compressor, the returned refrigerant is directly
introduced into the cylinder bore without passing through
the crank chamber. Therefore, lubrication of the sliding
parts arranged in the crank chamber mainly relies on
lubricant supplied into the crank chamber together with
blow-by gas.
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Many of the compressors used for this purpose
are of the variable capacity type, and the weight must be
reduced because they are mounted on vehicles for air
conditioning, and further the weight of the single head
piston must be reduced as much as possible. The reason
is that the controlling property to control the capacity
at high speed operation is deteriorated when the mass of
the single head piston is large. That is, when the mass
of the piston is large, in the case of changing over from
the suction stroke to the compression stroke, a high
intensity force of inertia of the piston acts in a
direction so that an inclination angle of the swash plate
is increased. Therefore, irrespective of the adjustment
of pressure in the crank chamber, the capacity exceeds a
proper value, and capacity control becomes unstable.
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In view of the above circumstances, in order to
reduce the weight of the single head piston, there are
some proposals in which the single head piston is made
hollow. However, in order to make the single head piston
hollow, it is necessary to provide a process in which two
members are welded. Therefore, the manufacturing cost is
inevitably raised.
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On the other hand, according to the piston
disclosed in Japanese Unexamined Patent Publication No.
9-203378, the weight of the piston is reduced in such a
manner that a through-hole section, which passes through
the piston body in the rotary direction of the swash
plate, is formed. However, a sliding face, which is
formed by this through-hole section and located on a side
close to the drive shaft, is includes a redundant region
on which a side force does not concentrate. Therefore,
the object of reducing the piston weight cannot be
sufficiently attained.
SUMMARY OF THE INVENTION
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It is an object of the present invention to provide
a single head piston characterized in that the weight is
small, the manufacturing is easy and, further, the piston
can smoothly slide.
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In a swash plate type compressor of an embodiment of
the present invention, both faces of a swash plate, which
is tiltably supported by a drive shaft, are interposed
between shoes arranged at a neck section of a single head
piston, so that a rotary motion of the swash plate is
converted into a linear reciprocating motion of the
single head piston inserted into a cylinder bore, and a
piston stroke is changed by adjusting a difference in the
pressures acting on the single head piston. The single
head piston includes: a head section engaged in the
cylinder bore; a side force pressure receiving wall
extending from the lower side of the head section to the
neck section; and a guiding wall extending from the upper
side of the head section to the neck section, wherein the
neck section is connected with at least the side force
pressure receiving wall by a rib.
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In this connection, expressions of the upper and the
lower side of the head section are based on the posture
of the piston in the cylinder bore located right above
the axial center of the drive shaft.
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The present invention may be more fully understood
from the description of preferred embodiments of the
invention set forth below, together with the accompanying
drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
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- Fig. 1 is a vertical cross-sectional view of a swash
plate type compressor of an embodiment of the present
invention;
- Fig. 2 is a perspective view showing an embodiment
of a piston;
- Fig. 3 is an enlarged view exaggeratedly showing a
primary portion in a state in which the piston located
close to the top dead point is inclined;
- Fig. 4 is a plan view of the piston shown in Fig. 2;
- Fig. 5A is a cross-sectional view taken on line A -
A in Fig. 3;
- Fig. 5B is a cross-sectional view taken on line B -
B in Fig. 3;
- Fig. 6 is a graph showing a relation between a
rotary angle of the swash plate and an intensity of the
side force acting on the piston;
- Fig. 7 is a schematic illustration showing a phase
upon which a high intensity of side force concentrates;
and
- Fig. 8 is a front view showing another embodiment of
the piston.
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DESCRIPTION OF THE PREFERRED EMBODIMENTS
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Referring to Figs. 1 and 2, an embodiment of the
swash plate type compressor of the present invention will
be explained below.
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As shown in Fig. 1, the front housing 1 is joined to
a front end face of the cylinder block 2. The rear
housing 3 is joined to a rear end face of the cylinder
block 2 via the valve plate 4. The front housing 1,
cylinder block 2 and rear housing 3 compose housing
assembly of the compressor. A suction chamber 3a and a
discharge chamber 3b are formed enclosed by the rear
housing 3 and the valve plate 4. Refrigerant gas is
directly introduced from an external refrigerating
circuit (not shown) into the suction chamber 3a via the
inlet 3c.
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The valve plate 4 includes a suction port 4a, a
suction valve 4b, a discharge port 4c and a discharge
valve 4d. The crank chamber 5 is formed enclosed by the
front housing 1 and the cylinder block 2. The drive
shaft 6 is pivotally supported by the front housing 1 and
cylinder block 2 via a pair of bearings 7. The drive
shaft 6 penetrates the crank chamber 5. The support hole
2b is formed at the center of the cylinder block 2. A
rear end portion of the drive shaft 6 is inserted into
the support hole 2b and supported by an inner
circumferential face of the support hole 2b via the
bearing 7.
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The lug plate 8 is fixed to the drive shaft 6. The
swash plate 9 is supported by the drive shaft 6 in the
crank chamber 5 in such a manner that it can be slid in
the axial direction L and it can be tilted with respect
to the drive shaft 6. The swash plate 9 is connected
with the lug plate 8 via the hinge mechanism 10. The
hinge mechanism 10 is composed of a support arm 19 formed
on the lug plate 8 and a pair of guide pins 20 formed on
the swash plate 9. The guide pins 20 are slidably
inserted into a pair of guide holes 19a formed in the
support arm 19. The hinge mechanism 10 rotates the swash
plate 9 integrally with the drive shaft 6. At the same
time, the hinge mechanism 10 guides the swash plate 9
when the swash plate 9 is moved in the axial direction L
and inclined with respect to drive shaft 6.
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A plurality of cylinder bores 2a are formed in the
cylinder block 2 round the drive shaft 6 and extend in
the axial direction L of the drive shaft 6. The single
head piston 11, which will be referred to as a piston
hereinafter, is housed in the cylinder bore 2a. The
groove 16 is formed at the neck section 11a of the piston
11, and hemispherical sections of a pair of shoes 12 are
relatively slidably engaged with inner wall faces of the
groove 16 which are opposed to each other. The swash
plate 9 is slidably interposed between the planes of both
shoes 12. A rotary motion of the swash plate 9 is
converted into a linear reciprocating motion of the
piston 11 via the shoes 12. The piston 11 is
reciprocated in the cylinder bore 2a in the longitudinal
direction. In the suction stroke in which the piston
moves from the top dead center to the bottom dead center,
refrigerant gas in the suction chamber 3a pushes the
suction valve 4b open and flows into the cylinder bore 2a
via the suction port 4a. In the compression stroke in
which the piston 11 is moved from the bottom dead center
to the top dead center, refrigerant gas in the cylinder
bore 2a is compressed and pushes the discharge valve 4d
open and flows through the discharge port 4c into the
discharge chamber 3b.
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The thrust bearing 21 is arranged between the lug
plate 8 and the front housing 1. The piston 11 is given
a compressive reaction force in accordance with the
compression of refrigerant gas. This compressive
reaction force is received by the front housing 1 via the
piston 11, the swash plate 9, the lug plate 8 and the
thrust bearing 21.
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As can be seen in Fig. 2, a rotation restricter 22
is integrally formed in the neck section 11a of the
piston 11. Since the diameter of the circumferential
face of the rotation restricter 22 is substantially the
same as that of the inner circumferential face of the
front housing 1, even when the piston 11 is given a
torque, the center of which is the axial center, the
piston 11 can be prevented from rotating by the contact
with the inner circumferential face of the front housing
1.
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As can be seen in Fig. 1, a supply passage 13
connects the discharge chamber 3b with the crank chamber
5. The electromagnetic valve 14 is attached to the rear
housing 3 and located in the middle of the supply passage
13. When the solenoid 14a of the electromagnetic valve
14 is magnetized, the valve body 14b closes the valve
hole 14c. When the solenoid 14a is demagnetized, the
valve body 14b opens the valve hole 14c.
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A bleed passage 6a is formed in the drive shaft 6.
The inlet of the bleed passage 6a is open to the crank
chamber 5, and the outlet of the bleed passage 6a is open
to the inside of the support hole 2b. The bleed hole 2c
connects the inside of the support hole 2b with the
suction chamber 3a.
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When the supply passage 13 is closed by the
magnetization of the solenoid 14a, no refrigerant gas at
high pressure is supplied from the discharge chamber 3b
into the crank chamber 5. Under the above condition,
refrigerant gas only flows out from the crank chamber 5
into the suction chamber 3a via the bleed passage 6a and
the bleed hole 2c. Therefore, pressure in the crank
chamber 5 becomes close to the low pressure in the
suction chamber 3a. Due to the foregoing, pressure in
the crank chamber 5 is decreased, and an inclination
angle of the swash plate 9 increased to the maximum as
shown in Fig. 1. Therefore, the discharge capacity of
the compressor becomes the maximum.
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When the supply passage 13 is opened by
demagnetization of the solenoid 14a, refrigerant gas of
high pressure is supplied from the discharge chamber 3b
into the crank case 5, so that the pressure in the crank
chamber 5 is increased. In this way, the pressure in the
crank chamber 5 is raised, and finally the inclination
angle of the swash plate 9 is decreased to the minimum,
so that the discharge capacity of the compressor becomes
the minimum.
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When the stopper 9a provided on the front face of
the swash plate 9 comes into contact with the lug plate
8, the swash plate 9 is restricted so that it cannot be
inclined beyond the predetermined maximum angle. On the
other hand, when the swash plate 9 comes into contact
with the ring 15 attached to the drive shaft 6, the
minimum inclination angle of the swash plate 9 is
restricted.
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As described above, when the supply passage 13 is
closed and opened by the magnetization and
demagnetization of the solenoid 14a, pressure in the
crank chamber 5 can be adjusted. When pressure in the
crank chamber 5 changes, the inclination angle of the
swash plate 9 is changed. According to the change in the
inclination angle of the swash plate 9, the piston stroke
is changed, so that the discharge capacity of the
compressor can be adjusted. When control is conducted by
a controller not shown, the solenoid 14a of the
electromagnetic valve 14 is selectively magnetized and
demagnetized according to the information such as a
cooling load. That is, the discharge capacity of the
compressor is adjusted according to the cooling load.
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Aluminum alloy is used for the cylinder block 2
having the cylinder bore 2a. Aluminum alloy is also used
for the piston 11. Preferably, hyper-eutectic aluminum
silicon alloy is used for the cylinder block 2 having the
cylinder bore 2a and is also used for the piston 11. On
an outer circumferential face of the piston 11, there is
provided a coat of fluororesin (PTFE) so that the direct
contact of the same metal can be avoided and a clearance
between the piston 11 and the cylinder bore 2a can be
reduced to as small as possible. In order to reduce the
weight so as to enhance the capacity control property and
also in order to ensure the lubricating property of the
piston 11 with respect to the cylinder bore 2a, the
piston 11 has the following characteristics.
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The piston 11 shown in Figs. 2, 5A and 5B includes:
a head section 11b engaged with the cylinder bore 2a; a
side force pressure receiving wall 11c1 (referred to as a
pressure receiving wall hereinafter) extending from the
lower side of the head section 11b to the neck section
11a, specifically extending from a position unevenly
distributed on the preceding side of the swash plate in
the rotary direction to the neck section 11a; and a guide
wall 11c2 extending from the upper side of the head
section 11b to the neck section 11a. The neck section
11a is connected with the pressure receiving wall 11c1
and the guide wall 11c2, respectively, by ribs 11d1, 11d2.
That is, a space formed between the neck section 11a and
the head section 11b of the piston 11 is open except for
the pressure receiving wall 11c1, the guide wall 11c2 and
the ribs 11d1, 11d2 as shown by the reference numeral 17
in the drawing. In this connection, when the compressor
is stopped, the swash plate 9 is transferred to a posture
of a smaller capacity by the biassing force of a spring
not shown so that the swash plate 9 can prepare for the
next starting operation. At this time, the guide wall
11c2 is linked with the swash plate 9, so that a twist of
the piston 11, which advances into the cylinder bore 2a,
can be effectively prevented.
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In this case, consideration is given to the side
force acting on the piston 11. The piston 11 is given a
reaction force (side force) from the inner
circumferential face of the cylinder bore 2a which is
caused by the compressive reaction force generated in the
process of reciprocation and also by the force of
inertia.
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To explain in more detail, as shown in Figs. 3 and
4, when the piston 11 is located at a position close to
the top dead point, the compressive reaction force acting
on the piston 11 becomes the maximum. This compressive
reaction force and the force of inertia of the piston 11
act on the swash plate 9. The piston 11 softens a high
intensity reaction force Fs according to resultant force
F0 of the compressive reaction force and force of inertia
from the swash plate 9 which is inclined with respect to
a face perpendicular to the axis L of the drive shaft 6.
According to the inclination angle of the swash plate 9,
this reaction force Fs can be resolved into a component
force f1 which is directed in the moving direction of the
piston 11 and a component force f2 which is directed in
the direction of axial center L of the drive shaft 6. As
can be seen in Fig. 4, the component force f3 is
generated by rotation R of the swash plate 9 in the same
manner. These component forces f2 and f3 tilt the piston
11 with respect to the axial center of the cylinder bore
2a. The pressure receiving wall 11c1 unevenly
distributed on the preceding side of the swash plate 9 in
the rotary direction R receives a high intensity reaction
force (side force) Fa from the inner circumferential face
of a portion close to the opening of the cylinder bore 2a
according to the component forces f2 and f3.
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A position at which side force Fa acts on the piston
11 is changed by the movement of the piston 11. The
circumstances will be explained in detail below.
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Fig. 6 is a graph showing a relation between a
rotary angle of the swash plate 9, that is, a moving
position of the piston 11, and an intensity of the side
force Fa acting on the piston 11. On this graph, a
rotary angle of the swash plate 9 is set at 0° when the
piston 11 is located at the top dead point. Side force
Fa successively acts on the overall circumference in the
same direction as the direction of rotation R of the
drive shaft 6.
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Fig. 7 is a schematic illustration for explaining a
phase upon which a high intensity portion of side force
Fa concentrates. Fig. 7 is a view of the piston 11 taken
from a side on which the rotary direction R of the drive
shaft 6 is clockwise. In this view, the piston 11 is
viewed from the side of the neck section 11a. Virtual
straight line M, which passes through the axial center L
of the drive shaft 6 and the axial center of the piston
11, is drawn, and this virtual straight line M crosses
the circumferential face of the piston 11 at cross points
P1 and P2. Cross point P1, which is distant from axial
center L of the drive shaft 6, is set at the 12 o'clock
position.
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From the point in time at which the piston 11 is
located at the top dead center to the point in time at
which the swash plate 9 is rotated by 90° in the
direction of arrow R, compressed refrigerant gas
remaining in the cylinder bore 2a expands again in
accordance with the movement of the piston 11 from the
top dead center to the bottom dead center. After the
completion of the expansion, refrigerant gas starts to be
sucked into the cylinder bore 2a. Under the above
condition, no compressive reaction force acts on the
swash plate 9, and force F0 acting on the swash plate 9
is mainly a force of inertia of the piston 11.
Accordingly, even in this state, the piston 11 receives
reaction force Fs, which is mainly based on the force of
inertia, from the swash plate 9. However, force F0
acting on the swash plate 9 actually becomes 0 under the
above conditions. Therefore, side force Fa hardly acts
on the piston 11.
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While the swash plate 9 rotates from 0° to 90°, side
force Fa becomes negative. This means that the direction
of each force described above is reversed.
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When the swash plate 9 is further rotated by 90° in
the direction of arrow R and the piston 11 comes to the
bottom dead position, the side force acts at the 12
o'clock position, however, the intensity of the side
force is much lower than that of the side force in the
case shown in Fig. 3.
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Side force Fa acting on the piston 11 becomes
maximum at the end of the compression stroke in which the
rotary angle of the swash plate 9 is directed from 270°
to 360°. This highest side force Fa is received in range
T' of 4 to 6 o'clock as shown in Fig. 6. Consequently,
the range of pressure receiving circumferential face T
may be a circumferential face from 4 to 6 o'clock,
however, when consideration is given to enhancement of
the mechanical strength, the range of pressure receiving
circumferential face T is extended to a circumferential
face from 3 to 7 o'clock. However, as long as the
mechanical strength allows, it is preferable that the
range of pressure receiving circumferential face T is
made to come close to the aforementioned circumferential
face T'.
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To sum up, when pressure receiving circumferential
face T is reinforced by the necessary minimum wall
thickness so as to enhance the mechanical strength, the
aforementioned pressure receiving wall 11c1 can be
obtained. On this pressure receiving wall 11c1, when the
redundant wall thickness portion is removed to the
utmost, a crescent-shaped thickness portion, which is
substantially inclined, can be formed, that is, the
ultimate reduction in the weight can be attained.
Further, the inner face of the pressure receiving wall
11c1 is inclined in the same direction as the flowing
direction Q of drops of lubricant which spread from the
sliding contact interface between the swash plate 9 and
the shoes 12 and are affected by a centrifugal force.
Therefore, the cylinder bore 2a can be more smoothly
lubricated.
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In the above embodiment, the neck section 11a of the
piston 11 is connected with the pressure receiving wall
11c1 and the guide wall 11c2 by the ribs 11d1, 11d2.
However, as shown by the piston 11A in Fig. 8, when
consideration is given to the mechanical strength, it
possible to put the piston 11A into practical use in
which the neck section 11a of the piston 11 is connected
with only the lower rib 11d1. According to this piston,
the weight can be further reduced. Depending upon the
type of refrigerant gas and the selection of the pressure
condition of the compressor, it is possible to attach a
piston ring for adjusting a quantity of blow-by gas to
the head section of the piston and also it is possible to
form oil grooves for enhancing the sliding property of
the piston. Further, in the case of an embodiment in
which the rotary direction of the swash plate 9 is
inverted, of course, the aforementioned circumferential
face T' is transferred to the range of 6 to 8 o'clock.
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As the detail are described above, in the piston
used for the compressor of the present invention, a space
formed between the neck section and the head section is
open except for the side force pressure receiving wall,
the guide wall and the ribs. Therefore, the ultimate
reduction in weight can be attained. On the other hand,
drops of lubricant which have spread from the sliding
interface between the swash plate and the shoes are
effectively supplied into the cylinder bore via this open
space. Therefore, smooth sliding of the piston can be
positively guaranteed. In the case where the
aforementioned pressure receiving wall is formed and is
unevenly distributed and inclined onto the preceding side
of the swash plate in the rotary direction, drops of
lubricant, which have spread from the sliding interface
between the swash plate and the shoes, are influenced by
a centrifugal force and made to flow. These drops of
lubricant can be appropriately guided on the inner face
of the pressure receiving wall inclined in the same
direction as the flowing direction of the drops of
lubricant. Therefore, a sufficient quantity of lubricant
can be supplied.
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While the invention has been described by reference
to specific embodiments chosen for purposes of
illustration, it should be apparent that numerous
modifications could be made thereto by those skilled in
the art without departing from the basic concept and
scope of the invention.