The current application is a 371 National Phase application based on International Application PCT/JP2012/007318, filed Nov. 15, 2012, which claims priority to Japanese Patent Application 2011-251426 filed on Nov. 17, 2011, the contents of which are incorporated herein by reference in their entirety.
The present invention relates to an ejector-type refrigeration cycle device that has an ejector and plural evaporators. The ejector serves as a refrigerant pressure reduction device and also as a refrigerant circulation device.
Conventionally, an ejector-type refrigeration cycle device provided with plural ejectors and plural evaporators is known from a patent document 1 or the like. As shown in
A second ejector 24 is provided for drawing an outlet refrigerant of a third evaporator 27, and the second ejector 24 has its refrigerant suction port 24b connected to the outlet side of the third evaporator 27.
A branch passage 22 is provided on an upstream side of the first ejector 15 and branches at a branch part Z, and a high pressure refrigerant on a downstream side of a radiator 13 flows into the second ejector 24 through this branch passage 22. A downstream side of the second ejector 24 is connected to the outlet side of the first evaporator 16.
The first and second evaporators 16 and 19 are constituted as one evaporator unit, and such evaporator unit composed of the first and second evaporators 16 and 19 cools a first cooling object space, and the third evaporator 27 cools a second cooling object space.
The first ejector 15 is disposed exclusively for the evaporator unit composed of the first and second evaporators 16 and 19, and the second ejector 24 is disposed exclusively for the third evaporator 27.
Thereby, a refrigerant flow amount of the evaporator unit and a refrigerant flow amount of the third evaporator 27 can be appropriately adjusted with an exclusive ejector, respectively.
Since the refrigerant is branched into a second ejector 24 side and into a third evaporator 27 side at a branch part X disposed on an upstream side of the second ejector 24, the refrigerant flow amount which flows into the second ejector 24 becomes small. Therefore, it is necessary to form a nozzle part 24a of the second ejector 24 to have a small size, and a degree of difficulty of manufacturing the nozzle part 24a with high processing accuracy may be further increased. In
Patent document 1: Japanese Unexamined Patent Publication No. 2007-24412
In view of the foregoing matters describing above, it is an objective of the present disclosure to provide an ejector-type refrigeration cycle device in which a readily-manufacturable second ejector may be used.
According to a first aspect of the present disclosure, an ejector-type refrigeration cycle device includes: a compressor discharging a refrigerant; a radiator which cools the refrigerant discharged from the compressor; a first ejector and a second ejector, each of which draws the refrigerant from a refrigerant suction port by using a high-speed refrigerant flow jetted from a nozzle part; a first suction-side evaporator connected to the refrigerant suction port of the first ejector; and a second suction-side evaporator connected to the refrigerant suction port of the second ejector. In the ejector-type refrigeration cycle device, a flow amount of the refrigerant in the second ejector is smaller than a flow amount of the refrigerant in the first ejector. Furthermore, the refrigerant branched at a branch part that is positioned on a downstream refrigerant side of the radiator and on an upstream refrigerant side of the first ejector flows into the second ejector, and the refrigerant branched on a downstream refrigerant side of the second ejector flows into the second suction-side evaporator.
Thus, the refrigerant is not branched, on the upstream side of the second ejector, to a side of the second ejector and to a side of the second suction-side evaporator, and thereby the refrigerant flow amount in the second ejector can be increased as compared with a case where the refrigerant is branched to the side of the second ejector and to the side of the second suction-side evaporator on the upstream side of the second ejector. Therefore, the nozzle part may have a large size, thereby making it possible to use the readily-manufacturable second ejector in the refrigeration cycle device.
According to a second aspect of the present disclosure, an ejector-type refrigeration cycle device includes: a compressor discharging a refrigerant; a radiator which cools the refrigerant discharged from the compressor; a first ejector and a second ejector, each of which draws the refrigerant from a refrigerant suction port by using a high-speed refrigerant flow jetted from a nozzle part; a first suction-side evaporator connected to the refrigerant suction port of the first ejector; and a second suction-side evaporator connected to the refrigerant suction port of the second ejector. In the ejector-type refrigeration cycle device, a flow amount of the refrigerant in the second ejector is smaller than a flow amount of the refrigerant in the first ejector. Furthermore, the refrigerant branched at a branch part that is positioned on a downstream refrigerant side of the compressor and on an upstream refrigerant side of the radiator flows into the second ejector, and the refrigerant branched on a downstream refrigerant side of the radiator and on an upstream refrigerant side of the first ejector flows into the second suction-side evaporator.
Since a gas phase refrigerant with a low density, discharged from the compressor, flows into the second ejector, the nozzle part of the second ejector may have a large size as compared with a case where a liquid phase refrigerant with a high density flows. Therefore, the readily-manufacturable second ejector may be used.
In an ejector-type refrigeration cycle device according to a third aspect of the present disclosure, the second ejector may have a double cylinder structure which has an inner cylinder and an outer cylinder. In this case, a suction flow drawn from the refrigerant suction port may flow through a flow passage formed in an inside of the inner cylinder, and a drive flow jetted from the nozzle part may flow through a flow passage formed in a space between the inner cylinder and the outer cylinder.
Since a width dimension of the flow passage through which the suction flow flows is expandable as compared with a case where the suction flow flows through the inside of the inner cylinder, the manufacturing of the second ejector can be made easy.
In an ejector-type refrigeration cycle device according to a fourth aspect of the present disclosure, the second ejector may be configured such that the nozzle part of the second ejector is formed at one end portion of a cylindrical member, and a mixing part and a diffuser part of the second ejector are formed at an other end portion of the cylindrical member. Furthermore, the mixing part may mix the high-speed refrigerant flow jetted from the nozzle part and a suction refrigerant drawn from the refrigerant suction port, the diffuser part may reduce a speed of the refrigerant mixed in the mixing part and may increase a pressure of the refrigerant mixed in the mixing part, and the nozzle part and the mixing part may be connected smoothly.
In this case, as compared with a case where the second ejector has a double cylinder structure, the structure of the second ejector is simplified thereby improving the ease of manufacturing thereof.
An ejector-type refrigeration cycle device according to a fifth aspect of the present disclosure may further include a throttle mechanism decompressing the refrigerant which flows into the second suction-side evaporator. In this case, the throttle mechanism may have a structure swirling the refrigerant flowing therein.
In such manner, a state where the gas phase refrigerant is abundant on an inner side of the swirl than on an outer side of the swirl is realized. For this reason, as compared with a case where the refrigerant is not swirled, the refrigerant flow amount flowing out from the throttle mechanism is decreased.
In the following, plural embodiments for realizing the present disclosure are explained with reference to the drawings. In the plural embodiments, the same reference numerals may be assigned to the same parts in the preceding embodiment, for avoiding redundant explanations and for the brevity of the description. When a part of an embodiment is explained, explanation of the other part of the same embodiment is left to at least one of the preceding embodiments. A partial combination of plural embodiments may be considered to be within the scope of the present disclosure not necessarily for an explicitly-described case but also for a non-explicitly-described case unless such combination has a hindrance thereof.
As such compressor 11, a variable capacity type compressor which adjusts its refrigerant discharge capacity by changing a discharge volume may be used or a fixed capacity type compressor which adjusts a refrigerant discharge capacity by changing an operation ratio of a compressor operation based on connection and disconnection of an electromagnetic clutch may be used. Further, if an electrically-driven compressor is used as the compressor 11, the refrigerant discharge capacity can be adjusted by adjusting the number of rotations of an electric motor.
A radiator 13 is disposed on a refrigerant discharge side of the compressor 11. The radiator 13 performs heat exchange between the high pressure refrigerant discharged from the compressor 12 and an outside air (i.e., air outside a passenger compartment) blown by a cooling fan which is not illustrated, and cools the high pressure refrigerant.
Here, when a usual fluorocarbon refrigerant is used as a refrigerant of the ejector-type refrigeration cycle device 10, the radiator 13 is used as a condenser which cools and condenses the refrigerant, because a subcritical cycle is formed in which the high pressure does not exceed a critical pressure of the refrigerant. On the other hand, when a carbon dioxide (CO2) or the like is used as the refrigerant, the refrigerant simply radiates heat in a supercritical state, thereby not being condensed, because a supercritical cycle is formed in which the high pressure of such refrigerant exceeds the critical pressure. Hereafter, a subcritical cycle in which the radiator 13 acts as a condenser is taken as an example for the explanation of the present embodiment.
A throttle mechanism 14 is disposed at a downstream side portion of the refrigerant flow relative to the radiator 13, and a first ejector 15 is disposed at a downstream side portion of the throttle mechanism 14.
The throttle mechanism 14 is a pressure reduction device which adjusts a flow amount of the refrigerant, and may be specifically consist of a fixed diaphragm like a capillary tube or an orifice. An electric control valve in which a valve opening degree (i.e., a throttle opening degree of a passage) is adjusted by an electric actuator may also be used as the throttle mechanism 14.
The first ejector 15 serves as a refrigerant circulation device (i.e., a momentum transfer type pump) which circulates the refrigerant with a suction effect of the refrigerant flow jetted at a high speed while serving as a pressure reduction device which decompresses the refrigerant.
In the first ejector 15, there is provided with (i) a nozzle part 15a which reduces a passage area size of an intermediate pressure refrigerant which flows in from the throttle mechanism 14 and decompresses and expands the intermediate pressure refrigerant iso-entropically and (ii) a refrigerant suction port 15b which is disposed in connection with a refrigerant jetting port of the nozzle part 15a and draws the refrigerant from a second evaporator 19 mentioned later.
Further, in a downstream side portion of the nozzle part 15a and the refrigerant suction port 15b, a mixing part 15c which mixes the high-speed refrigerant flow which is jetted from the nozzle part 15a and the suction refrigerant of the refrigerant suction port 15b is disposed. Further, on a downstream side of the mixing part 15c, a diffuser part 15d which serves as a pressure boost part is disposed. The diffuser part 15d is formed in a shape in which a refrigerant passage area size is gradually increased toward downstream, and achieves a refrigerant pressure boosting effect by reducing a speed of the refrigerant flow, that is, in other words, achieves an energy conversion effect for converting a speed energy of the refrigerant to a pressure energy.
A first evaporator 16 is connected to a downstream side of the diffuser part 15d of the first ejector 15, and a gas-liquid separator 17 is connected to a refrigerant flow downstream side of this first evaporator 16. The refrigerant flow downstream side of the gas-liquid separator 17 is connected to a suction side of the compressor 11.
On the other hand, a first branch passage 18 branches from a branch part Z1 positioned in an upstream part of the first ejector 15 (i.e., an intermediate part between the throttle mechanism 14 and the first ejector 15), and the downstream side of this first branch passage 18 is connected to the refrigerant suction port 15b of the first ejector 15. A second evaporator 19 (i.e., a first suction-side evaporator) is disposed in this first branch passage 18.
In the present embodiment, the two evaporators 16 and 19 and the first ejector 15 are combined to have a one-body structure, and the two evaporators 16 and 19 and the first ejector 15 consist of an evaporator unit 20 in the one-body structure. Although there may be various examples of how such one-body structure is made, which combines the two evaporators 16 and 19 and the first ejector 15, a soldering structure which combines the two evaporators 16 and 19 and the first ejector 15 by soldering may be preferable from a productivity improvement view point.
That is, flat shape tubes which constitute the refrigerant passage of the two evaporators 16 and 19 (not shown), corrugated fins alternatingly layered with the flat shape tubes (not shown), tank parts distributing and collecting to and from many tubes (not shown) and other parts are formed by using metal such as aluminum, and, each of those parts of the two evaporators 16 and 19 and the first ejector 15 are assembled temporarily in a predetermined structure, and the temporarily assembled structure is brought into a heat furnace, and each of those parts of the two evaporators 16 and 19 and the first ejector 15 are combined to have one body by soldering.
An evaporator unit 20 which is a one-body combination of the two evaporators 16 and 19 and the first ejector 15 is stored in an in-compartment unit case (not shown) of an air-conditioner for vehicles. Further, an air passage that is defined in the indoor unit case receives air (i.e., a cooling object air) that is blown by an electric blower 21 as indicated by an arrow A, and this blown air is cooled by the two evaporators 16 and 19.
A cold wind cooled by the two evaporators 16 and 19 is sent into the same cooling object space, more practically, into an in-vehicle passenger compartment space (not shown), and, in such manner, the passenger compartment space is air-conditioned by the two evaporators 16 and 19. Here, from among the two evaporators 16 and 19, the first evaporator 16 connected to the downstream side flow passage of the first ejector 15 is disposed on an upstream side of an air flow A, the second evaporator 19 connected to the refrigerant suction port 15b of the first ejector 15 is disposed on the downstream side of the air flow A.
On the other hand, the second branch passage 22 branches from a branch part Z2 positioned in an upstream part of the throttle mechanism 14 (i.e., an intermediate portion between the radiator 13 and the throttle mechanism 14), and a downstream side of this second branch passage 22 is connected to a merge part Z3 positioned on an outlet side of the first evaporator 16.
The second branch passage 22 also has a throttle mechanism 23 disposed therein, and the second ejector 24 is disposed in a downstream side portion of this throttle mechanism 23. The throttle mechanism 23 is a pressure reduction device which adjusts the refrigerant flow amount, and may be specifically consist of a fixed diaphragm like a capillary tube or an orifice. An electric control valve in which a valve opening degree (i.e., a throttle opening degree of a passage) is adjusted by an electric actuator may also be used as the throttle mechanism 23.
The second ejector 24 serves as a refrigerant circulation device (i.e., a momentum transfer type pump) which circulates the refrigerant with the suction operation of the refrigerant flow jetted at a high speed while serving as a pressure reduction device which decompresses the refrigerant.
In the second ejector 24, there is provided with (i) a nozzle part 24a which reduces a passage area size of an intermediate pressure refrigerant which flows in from the throttle mechanism 23 and decompresses and expands the intermediate pressure refrigerant iso-entropically, and (ii) a refrigerant suction port 24b which is in connection with a refrigerant jetting port of the nozzle part 24a and draws the refrigerant from a third evaporator 27 mentioned later.
Further, in a downstream side portion of the nozzle part 24a and the refrigerant suction port 24b, a mixing part 24c which mixes the high-speed refrigerant flow which is jetted from the nozzle part 24a and the suction refrigerant of the refrigerant suction port 24b is disposed. Further, on a downstream side of the mixing part 24c, a diffuser part 24d which serves as a pressure boost part is disposed. The diffuser part 24d is formed in a shape in which a refrigerant passage area size is gradually increased, and achieves a refrigerant pressure boosting effect by reducing a speed of the refrigerant flow, that is, in other words, achieves an energy conversion effect for converting a speed energy of the refrigerant to a pressure energy.
A refrigerant distributor 25 is connected to a downstream side of the diffuser part 24d of the second ejector 24. The refrigerant distributor 25 provides a vapor-liquid separation function for separating gas from liquid by swirling the refrigerant, a liquid pool function for pooling a separated liquid-phase refrigerant, and a refrigerant distribution function which flows a high dryness refrigerant (i.e., a gas phase rich refrigerant) to flow toward a first outlet 25a and flows a low dryness refrigerant (i.e., a liquid phase rich refrigerant) to flow toward a second outlet 25b.
The first outlet 25a of the refrigerant distributor 25 is connected to the merge part Z3 positioned on the outlet side of the first evaporator 16. The second outlet 25b of the refrigerant distributor 25 is connected to a throttle mechanism 26. In such manner, an outlet side refrigerant of the second ejector 24 is separated into gas and liquid by the refrigerant distributor 25, flowing a liquid-phase refrigerant into the throttle mechanism 26 and flowing the gas-phase refrigerant into the compressor 11. Therefore, returning of a liquid refrigerant back into the compressor 11 is securely prevented.
A refrigerant flow downstream side of the throttle mechanism 26 is connected to the third evaporator 27 (i.e., a second suction-side evaporator). Further, a refrigerant flow downstream side of the third evaporator 27 is connected to the refrigerant suction port 24b of the second ejector 24.
In the present embodiment, the third evaporator 27, the second ejector 24, the refrigerant distributor 25, and the throttle mechanism 26 are assembled to have a one-body structure, and the third evaporator 27, the second ejector 24, the refrigerant distributor 25, and the throttle mechanism 26 consist of an evaporator unit 28 in the one-body structure.
Although there may be various examples of how such one-body structure is made, which combines the third evaporator 27, the second ejector 24, the refrigerant distributor 25 and the throttle mechanism 26; a soldering structure which combines the third evaporator 27, the second ejector 24, the refrigerant distributor 25, and the throttle mechanism 26 by soldering may be preferable from a productivity improvement view point.
That is, flat shape tubes which constitute the refrigerant passage of the third evaporator 27 (not shown), corrugated fins alternatingly layered with the flat shape tubes (not shown), tank parts distributing and collecting to and from many tubes (not shown) and other parts are formed by using metal such as aluminum, and, each of those parts of the third evaporator 27, the second ejector 24, the refrigerant distributer 25 and the throttle mechanism 26 are assembled temporarily in a predetermined structure, and the temporarily assembled structure is brought into a heat furnace, and each of those parts of the third evaporator 27, the second ejector 24, the refrigerant distributer 25 and the throttle mechanism 26 are combined to have one body by soldering.
The evaporator unit 28 which is a one-body combination of the third evaporator 27, the second ejector 24, the refrigerant distributor 25, and the throttle mechanism 26 is disposed in an in-vehicle refrigerator (not shown) that is installed in an in-vehicle passenger compartment, and cools an inner space of the in-vehicle refrigerator with the third evaporator 27. More specifically, an electric blower 29 which blows an inner space air to the third evaporator 27 is disposed in an inside of the in-vehicle refrigerator, and the blown air from the electric blower 29 is cooled by the third evaporator 27, and a cold wind is blown into the inner space of the in-vehicle refrigerator.
Next, a concrete structure of the second ejector 24 is explained based on
Therefore, an intermediate pressure refrigerant Gn which flows in from the throttle mechanism 23 (i.e., henceforth designated as a drive flow) flows through a flow passage formed in an inside of the inner cylinder 241 of the second ejector 24, a refrigerant Ge from the third evaporator 27 (i.e., henceforth designated as a suction flow) flows through a flow passage formed in a space between the outer cylinder 242 and inner cylinder 241 of the second ejector 24.
The nozzle part 24a is formed with metal, takes an approximately cylindrical shape and has a taper-shaped tip part that points to a flow direction of the refrigerant. Further, the nozzle part 24a is formed to change the refrigerant passage area size in an inside thereof to decompress the refrigerant in an equi-entropic manner.
More specifically, the refrigerant passage formed in an inside of the nozzle part 24a has a tapered space in which the refrigerant passage area size gradually decreases toward a downstream side from an upstream side of the refrigerant flow, and a throttle part at a tip of the tapered space where the refrigerant passage area size is smallest, and a widening part in which the refrigerant passage area size gradually expands toward a downstream side of the refrigerant flow from the throttle part.
In other words, the nozzle part 24a of the present embodiment is formed as a Laval nozzle, and makes a flow speed of the refrigerant in the throttle part to exceed a sonic speed. Of course, the nozzle part 24a may be formed as a tapered nozzle. Further, at the tip of the widening part of the nozzle part 24a, a refrigerant jetting port for jetting the refrigerant is formed.
The outer cylinder 242 is formed with metal, and takes an approximately cylindrical shape, just like the nozzle part 24a, and, in an inside thereof, an accommodation space 24f in which the nozzle part 24a is accommodated and a diffuser part 24d are formed.
The accommodation space 24f is formed as a cylindrical space which extends in an axial direction of the nozzle part 24a from a refrigerant flow upstream side and a tapered space which has a cross-section area that is perpendicular to the axial direction of the nozzle part 24a gradually decreased toward the refrigerant flow direction from the cylindrical space, so that the accommodation space 24f is fitted to an outside shape of the nozzle part 24a.
On the other hand, the diffuser part 24d is a space which has a cross-section area that is perpendicular to the axial direction of the nozzle part 24a gradually increased toward the refrigerant flow direction. The refrigerant suction port 24b is formed in the outer cylinder 242.
Next, a concrete structure of the refrigerant distributor 25 is explained based on
The swirl part 25c has an inlet 25e into which the refrigerant flows and the first outlet 25a from which the high dryness refrigerant (i.e., a gas phase rich refrigerant) flows out formed thereon. The liquid pool part 25d has the second outlet 25b from which the low dryness refrigerant (i.e., a liquid phase rich refrigerant) flows out formed thereon.
The swirl part 25c is formed in a cylindrical shape extending horizontally, with one end of which having the inlet 25e of the refrigerant formed thereon, and with the other end of which the first outlet 25a formed thereon. The liquid pool part 25d is positioned at a lower side of the swirl part 25c. The liquid pool part 25d is in communication with the swirl part 25c via a communication opening 25f.
That is, the flow direction of the swirling refrigerant in the refrigerant distributor 25 is the same as an inflow direction of the refrigerant flowing in from the inlet 25e. Further, the refrigerant distributor 25 may be provided as an accumulator in which the flow direction of the swirling refrigerant is perpendicular to the inflow direction of the refrigerant. In such an accumulator, a swirl part which swirls the refrigerant is formed at least in a vertically-extending cylindrical shape, and the inlet of the refrigerant is formed at least in an upper part of the swirl part.
Next, a concrete configuration of the throttle mechanism 26 is explained based on
The throttle mechanism 26 is provided with a body part 26b which forms in an inside of a swirl space SS which swirls the refrigerant flowing in from a refrigerant inflow opening 26a. The body part 26b is formed as a hollow container made with metal, an outer shape of which is an approximate column shape. The swirl space SS formed in an inside of the body part 26b includes a column shape space that is fitted to an outer shape of the body part 26b.
The refrigerant inflow opening 26a is formed as a side of one axial end (i.e., an upper side of
Thereby, as shown by a thick line arrow in
A refrigerant outlet 26c is formed on the other axial end of the axis of the body part 26b (i.e., a lower side of
The refrigerant passage cross-section area size of the refrigerant outlet 26c is smaller than the cross-section area size of the swirl space SS. Therefore, the refrigerant outlet 26c achieves a fixed throttle function which decompresses the refrigerant by decreasing the refrigerant passage area size.
Since a centrifugal force acts on the refrigerant which swirls in the swirl space SS, when a gas-liquid two phase refrigerant flows in from the refrigerant inflow opening 26a, a liquid phase refrigerant having a high density is unevenly distributed on an outer side relative to a center of the swirl. Therefore, when a gas-liquid two phase refrigerant flows in from the refrigerant inflow opening 26a, the gas phase refrigerant is abundant on an inner side rather than the outer side relative to a center line of swirl.
Further, according to the effect of the above-mentioned centrifugal force, the refrigerant pressure near the center of the swirl becomes lower than the pressure of the outer side. Since the refrigerant pressure near the center of the swirl lowers as the centrifugal force increases, the refrigerant pressure near the center of the swirl decreases as the swirl speed of the refrigerant which swirls in the swirl space SS increases.
Therefore, by sufficiently increasing the swirl speed and by causing a decompression boiling of the refrigerant, the gas phase refrigerant rich state is realized on the inner side than on the outer side relative to the center of the swirl, even when the liquid phase refrigerant flows in from the refrigerant inflow opening 26a. Therefore, in comparison to a case where the refrigerant is not swirled in the swirl space SS, the refrigerant flow amount flowing out from the refrigerant outlet 26c is decreased.
Next, the operation of the first embodiment is explained based on the Mollier diagram in
The refrigerant flow which flows toward the throttle mechanism 14 from the branch part Z2 is decompressed by the throttle mechanism 14, and serves as an intermediate pressure refrigerant (i.e., the b5 point→the c5 point), and this intermediate pressure refrigerant is, at the branch part Z1, split into a refrigerant flow which flows toward the first ejector 15 and a refrigerant flow which flows toward the first branch passage 18.
The refrigerant flow which has flown into the first ejector 15 is decompressed by the nozzle part 15a, and expands (i.e., the c5 point→the d5 point). Therefore, a pressure energy of the refrigerant is converted to a speed energy by the nozzle part 15a, and the refrigerant is jetted from a jetting opening of the nozzle part 15a at a high speed. Due to the decrease of the refrigerant pressure at such time, the refrigerant that has passed through the second evaporator 19 in the first branch passage 18 is drawn from the refrigerant suction port 15b.
The refrigerant which jetted from the nozzle part 15a and the refrigerant drawn from the refrigerant suction port 15b are mixed at the mixing part 15c on the downstream side of the nozzle part 15a, and flows into the diffuser part 15d. In the diffuser part 15d, due to the expansion of the passage area size, a speed (i.e., an expansion) energy of the refrigerant is converted to a pressure energy, thereby causing arise of the refrigerant pressure.
Then, the refrigerant flowing out from the diffuser part 15d of the first ejector 15 joins the refrigerant which has flown out from the refrigerant distributor 25 at the merge part Z3 that has passed through the first evaporator 16. In the first evaporator 16, a low temperature low pressure refrigerant absorbs heat from the blown air that flows along the arrow A direction and evaporates.
The refrigerant which has joined at the merge part Z3 is separated into gas and liquid by the gas-liquid separator 17 (i.e., the d5 point→the e5 point), and the separated gas phase refrigerant is drawn by the compressor 11 (i.e., the e5 point→the f5 point), and is compressed again (i.e., the f5 point→the a5 point).
On the other hand, the refrigerant flow which has flown into the first branch passage 18 flows into the second evaporator 19. In the second evaporator 19, a low pressure refrigerant absorbs heat from the blown air along the arrow A direction, and evaporates (omitted from
Further, the refrigerant flow which has been split at the branch part Z2 and has flown into the second branch passage 22 is decompressed by the throttle mechanism 23, and serves as an intermediate pressure refrigerant, and this intermediate pressure refrigerant flows into the second ejector 24 (i.e., the c5 point→the g5 point).
The refrigerant flow which has flown into the second ejector 24 is decompressed by the nozzle part 24a, and expands. Therefore, a pressure energy of the refrigerant is converted to a speed energy by the nozzle part 24a, and is jetted from the jetting opening of the nozzle part 24a at a high speed. Due to the decrease of the refrigerant pressure in this case, the refrigerant that has passed through the third evaporator 27 is drawn from the refrigerant suction port 24b.
The refrigerant which is jetted from the nozzle part 24a and the refrigerant drawn by the refrigerant suction port 24b are mixed at the mixing part 24c on the downstream side of the nozzle part 24a and flow into the diffuser part 24d (i.e., the g5 point→the h5 point). In the diffuser part 24d, by an expansion of the passage area size, a speed (i.e., an expansion) energy of the refrigerant is converted to a pressure energy, thereby causing a rise of the refrigerant pressure (i.e., the h5 point→the i5 point).
Then, the refrigerant which has flown out from the diffuser part 24d flows into the refrigerant distributor 25. In the refrigerant distributor 25 the refrigerant flowing out from the diffuser part 24d is separated into gas and liquid (i.e., the i5 point→the j5 point, the i5 point→the k5 point). The refrigerant separated by the refrigerant distributor 25 joins the refrigerant which has flown out from the first evaporator 16 at the merge part Z3 (i.e., the j5 point→the e5 point).
On the other hand, the liquid phase refrigerant separated by the refrigerant distributor 25 is decompressed by the throttle mechanism 26, and it becomes a low pressure refrigerant (i.e., the k5 point→the l5 point), and the low pressure refrigerant decompressed by the throttle mechanism 26 flows into the third evaporator 27. In the third evaporator 27, a low pressure refrigerant absorbs heat from the blown air B from the electric blower 29 and evaporates (i.e., the l5 point→the m5 point). The refrigerant after this evaporation is drawn into the second ejector 24 from the refrigerant suction port 24b (i.e., the m5 point→the h5 point). The blown air B which became a cold wind by the heat absorption in the third evaporator 27 is blown into the inner space of the in-vehicle refrigerator (not shown).
As described above, since, in the present embodiment, the refrigerant on the downstream side of the diffuser part 15d of the first ejector 15 is supplied to the first evaporator 16 and the refrigerant on a first branch passage 18 side is supplied to the second evaporator 19, a cooling effect is caused simultaneously in the first and second evaporators 16 and 19. Therefore, the cold wind cooled by both of the first and second evaporators 16 and 19 is blown into the passenger compartment space 22 which is the cooling object space, and the passenger compartment space 22 is cooled.
At such time, the refrigerant evaporation pressure of the first evaporator 16 is a pressure after boosting by the diffuser part 15d, and, on the other hand, the outlet side of the second evaporator 19 is connected to the refrigerant suction port 15b of the first ejector 15, thereby the lowest pressure just after the decompression by the nozzle part 15a is applied to the second evaporator 19.
Thereby, the refrigerant evaporation pressure (i.e., refrigerant evaporation temperature) of the second evaporator 19 is controlled to be lower than the refrigerant evaporation pressure (i.e., refrigerant evaporation temperature) of the first evaporator 16. Further, the first evaporator 16 having the high refrigerant evaporation temperature is disposed on the upstream side in the flow direction A of the blown air and the second evaporator 19 having the low refrigerant evaporation temperature is disposed on the downstream side in the flow direction A of the blown air, a temperature difference between the refrigerant evaporation temperature in the first evaporator 16 and the blown air and a temperature difference between the refrigerant evaporation temperature in the second evaporator 19 and the blown air are both securely reserved.
For this reason, the cooling capacity of both of the first and second evaporators 16 and 19 is effectively achieved. Therefore, the cooling performance for the passenger compartment space 22 which is a common cooling object space can be effectively achieved by the combination of the first and second evaporators 16 and 19.
Further, since the first and second evaporators 16 and 19 are combined as one evaporator unit 20, while being able to pack the first and second evaporators 16 and 19 into a one small unit structure, an assemble work for installing the one evaporator unit 20 into a unit case (not shown) is easily performed at one stroke.
On the other hand, since the inner space of the in-vehicle refrigerator (not shown) is cooled by the third evaporator 27 provided in the second branch passage 22, a separate cooling object space in an inside of the in-vehicle refrigerator is independently cooled by the third evaporator 27.
Since the first ejector 15 is disposed exclusively for the evaporator unit 20 that is made from the first and second evaporators 16 and 19, and the second ejector 24 is disposed exclusively for the third evaporator 27, it is easy to appropriately adjust the refrigerant flow amount of the evaporator unit 20 and the refrigerant flow amount of the third evaporator 27 respectively by the exclusive ejectors, and a high cooling capacity is achieved for both of the evaporator unit 20 and the third evaporator 27.
Further, since the refrigerant to the third evaporator 27 branches on the downstream side of the second ejector 24 according to the present embodiment, the refrigerant flow amount in the second ejector 24 is increased in comparison to the conventional technique shown in
Further, according to the present embodiment, the refrigerant flow amount flowing out from the refrigerant outlet 26c is decreased by swirling the refrigerant with the throttle mechanism 26 as mentioned above.
Further, when no swirl is caused, it is necessary to have a smaller flow amount by making the device to have a smaller size, thereby making it difficult to manufacture the device, and also making the device more prone to clogging of foreign matter. That is, for the same flow amount, the swirl case allows a larger device volume than the non-swirl case, thereby making it easier to manufacture the device, and also making the device to be clog-free.
According to the second embodiment, as shown in
The internal heat exchanger 30 provides a heat exchange function which exchanges heat between the high pressure refrigerant flowing out from the radiator 13 and the low pressure refrigerant (i.e., a gas-liquid two phase refrigerant) that has passed through the merge part Z3. Therefore, the high pressure refrigerant flowing out from the radiator 13 is cooled by the internal heat exchanger 30, and the low pressure refrigerant (i.e., a gas-liquid two phase refrigerant) that has passed through the merge part Z3 absorbs heat in the internal heat exchanger 30 to become a gas phase refrigerant. Therefore, the gas-liquid separator 17 of the first embodiment described above can be removed.
Also, in the present embodiment, the refrigerant distributor 25 may comprise an accumulator in which a direction of swirl of the refrigerant flowing therein may be configured to have a right angle against (i.e., may be perpendicular to) the inflow direction of the refrigerant flowing into the accumulator, just like the first embodiment. The other portions may have the same configuration as the first embodiment.
According to the third embodiment, as shown in
The fourth evaporator 31 is disposed at a position between the refrigerant distributor 25 and the merge part Z3. The high dryness refrigerant flowing out from the refrigerant distributor 25 evaporates in the fourth evaporator 31, and becomes a gas phase refrigerant. Therefore, the gas-liquid separator 17 of the first embodiment described above can be removed.
As a use purpose of the fourth evaporator 31, cooling of the passenger compartment space for assisting the first and second evaporators 16 and 19 and/or cooling of the inside space of the in-vehicle refrigerator for assisting the third evaporator 27 may be considered, for example. The other portions may have the same configuration as the first embodiment.
Further, as shown in
Further, as shown in
Further, in an example of
Although the refrigerant distributor 25 has the liquid pool part 25d which pools the liquid-phase refrigerant separated at the swirl part 25c in the first embodiment described above, the refrigerant distributor 25 may be configured differently, that is, as shown in
According to the first embodiment described above, the refrigerant distributor 25 separates gas and liquid by swirling the refrigerant. However, in the fifth embodiment, the refrigerant distributor 25 may separate gas and liquid by utilizing the gravity as shown in
In the above-mentioned embodiment, an intermediate pressure refrigerant (i.e., a gas-liquid two phase refrigerant) flows into the second ejector 24. However, in the sixth embodiment, as shown in
More specifically, a third branch passage 33 branches from a branch part Z4 positioned between the compressor 11 and the radiator 13, and a downstream side of the third branch passage 33 is connected to the merge part Z3. The second ejector 24 is disposed in the third branch passage 33. Further, an open-close valve 34 which opens and closes the third branch passage 33 is also disposed in the third branch passage 33.
The downstream side of the second branch passage 22 is connected to the refrigerant suction port 24b of the second ejector 24. In the second branch passage 22, the throttle mechanism 26 and the third evaporator 27 are disposed.
The operation of the present embodiment is explained based on the Mollier diagram of
The refrigerant flow which flows toward the throttle mechanism 14 from the branch part Z2 is decompressed by the throttle mechanism 14, and becomes an intermediate pressure refrigerant, and this intermediate pressure refrigerant is split at the branch part Z1 into a refrigerant flow toward the first ejector 15 and a refrigerant flow toward the first branch passage 18, and the refrigerant flow flowing into the first ejector 15 is decompressed by the nozzle part 15a and expands (i.e., the b14 point→the c14 point).
Therefore, a pressure energy of the refrigerant is converted to a speed energy by the nozzle part 15a, and the refrigerant is jetted from the jetting opening of the nozzle part 15a at high speed. Due to the fall of the refrigerant pressure fall at such time, the refrigerant that has passed through the second evaporator 19 in the first branch passage 18 is drawn from the refrigerant suction port 15b.
The refrigerant jetted from the nozzle part 15a and the refrigerant drawn by the refrigerant suction port 15b are mixed by the mixing part 15c on a downstream side of the nozzle part 15a, and flow into the diffuser part 15d. In the diffuser part 15d, by the expansion of the passage area size, a speed (i.e., expansion) energy of the refrigerant is converted to a pressure energy, thereby the pressure of the refrigerant increases.
Then, the refrigerant flowing out from the diffuser part 15d of the first ejector 15 passes through the first evaporator 16. In the first evaporator 16, a low temperature and low pressure refrigerant absorbs heat from the blown air that flows along the arrow A direction, and evaporates (i.e., the c14 point→the d14 point).
The refrigerant which has passed the first evaporator 16 joins the gas phase refrigerant flowing out from the second ejector 24 at the merge part Z3 (i.e., the d14 point→the e14 point). The refrigerant which joined at the merge part Z3 is drawn by the compressor 11, and is compressed again (i.e., the e14 point→the a14 point). Further, as shown in
On the other hand, the refrigerant flow which has flown into the first branch passage 18 is decompressed by the throttle mechanism 32, and becomes a low pressure refrigerant, and the low pressure refrigerant flows into the second evaporator 19. In the second evaporator 19, a low pressure refrigerant absorbs heat from the blown air flowing along the arrow A direction and evaporates (i.e., omitted from
Further, the refrigerant flow which has been split at the branch part Z2 and has flown into the second branch passage 22 is decompressed by the throttle mechanism 26, and becomes a low pressure refrigerant (i.e., the b14 point→the f14 point), and the low pressure refrigerant flows into the third evaporator 27.
In the third evaporator 27, the low pressure refrigerant absorbs heat from the blown air B flowing from the electric blower 29, and evaporates (i.e., the f14 point→the g14 point). The refrigerant after this evaporation is drawn into the second ejector 24 from the refrigerant suction port 24b (i.e., the g14 point→the h14 point). The blown air B from which heat is absorbed and which has become a cold air in the third evaporator 27 is blown into the inner space of the in-vehicle refrigerator (not shown).
The gas phase refrigerant in a high temperature and high pressure state from the branch part Z4 to the second ejector 24 is decompressed by the nozzle part 24a of the second ejector 24, and expands (i.e., the a14 point→the i14 point). Therefore, a pressure energy of the refrigerant is converted to a speed energy by the nozzle part 24a, and the refrigerant is jetted from the nozzle part 24a at high speed. Due to the decrease of the refrigerant pressure in this case, the refrigerant that has passed through the third evaporator 27 is drawn from the refrigerant suction port 24b.
The refrigerant which is jetted from the nozzle part 24a and the refrigerant drawn by the refrigerant suction port 24b are mixed at the mixing part 24c on the downstream side of the nozzle part 24a and flow into the diffuser part 24d (i.e., the i14 point→the h14 point). In the diffuser part 24d, by an expansion of the passage area size, a speed (i.e., expansion) energy of the refrigerant is converted to a pressure energy, thereby raising the pressure of the refrigerant.
Then, the refrigerant flowing out from the diffuser part 24d joins the refrigerant which has passed through the first evaporator 16 at the merge part Z3 (i.e., the h14 point→the e14 point). The joined refrigerant which has joined at the merge part Z3 is drawn by the compressor 11, and is compressed again (i.e., the e14 point→the a14 point).
Since the refrigerant which flows in the second ejector 24 is a gas phase refrigerant having low density according to the present embodiment, the size of the second ejector 24 is made larger in comparison to a case in which a liquid phase refrigerant having high density flows in the second ejector 24. Therefore, manufacturing of the second ejector 24 is made easy.
According to the seventh embodiment, as shown in
The internal heat exchanger 35 provides a function which exchanges heat between the high pressure refrigerant which flows from the branch part Z2 toward the throttle mechanism 26 and the low pressure refrigerant (i.e., a gas-liquid two phase refrigerant) that has passed through the third evaporator 27. Therefore, the high pressure refrigerant which flows from the branch part Z2 toward the throttle mechanism 26 is cooled by the internal heat exchanger 35, and the low pressure refrigerant (i.e., a gas-liquid two phase refrigerant) that has passed through the third evaporator 27 absorbs heat in the internal heat exchanger 35, and becomes a gas phase refrigerant.
Further, the internal heat exchanger 35 may also be configured to provide a function that exchanges heat between the high pressure refrigerant which flows from the radiator 13 to the branch part Z2 and the low pressure refrigerant (i.e., a gas-liquid two phase refrigerant) that has passed through the third evaporator 27.
Further, as shown in
Further, as shown in
According to the above-mentioned embodiment, the second ejector 24 has a double cylinder structure, and the drive flow Gn flows through a flow passage formed in an inside of the inner cylinder 241 and the suction flow Ge flows through a flow passage formed between the inner cylinder 241 and the outer cylinder 242. However, according to the eighth embodiment, as shown in
The inner cylinder 241 has a constant outer diameter. The outer cylinder 242 has a tapered part in which the inner diameter is gradually decreased from the upstream side toward the downstream side along the refrigerant flow, a throttle part that is formed at a tip of the tapered part at which the inner diameter is decreased to the minimum, and a widening part in which the inner diameter gradually expands toward the downstream side of the refrigerant flow from the throttle part. Thereby, the nozzle part 24a formed by the outer cylinder 242 can be used as a Laval nozzle.
In the second ejector 24 of the present embodiment shown in
In an example of
By swirling the drive flow Gn in the nozzle part 24a, a gas-liquid separation of the drive flow Gn is performed by the centrifugal force, and a liquid film is formed on an inner wall at a throttle part of the nozzle part 24a. Thereby, the liquid film at the throttle part serves as a start point of boiling of the drive flow Gn, for promoting the boiling. The promoted boiling at the throttle part causes an atomization of liquid drops, and, with the gas refrigerant generated by the promoted boiling, the atomized liquid drops are accelerated. As a result, a nozzle efficiency is improved and the pressure of the second ejector 24 increases. In such case, the nozzle efficiency is defined as an energy conversion efficiency at the time of converting a pressure energy of the refrigerant to a kinetic energy in the nozzle part.
In an example of
Although the second ejector 24 has a double cylinder structure in the above embodiment, the second ejector 24 may be formed, as shown in
The second ejector 24 is formed as a cylindrical member, on one end of which the nozzle part 24a is formed, and the mixing part 24c and the diffuser part 24d are formed in other part thereof, and the nozzle part 24a and mixing part 24c are connected smoothly, and the refrigerant suction port 24b is formed at a smoothly connecting portion which smoothly connects the nozzle part 24a and the mixing part 24c.
Since the nozzle part 24a and mixing part 24c are connected smoothly, the flow passage sectional area size changes continuously between the nozzle part 24a and the mixing part 24c. Thereby, a swirl loss is reduced.
Further, the ejector tank 40 is a cylindrical member in which both ends are opened, and an inlet 40a is formed on a side of the tank 40 for drawing the suction refrigerant Ge. At a position between an outer circumferential surface of the second ejector 24 and an inner circumferential surface of the ejector tank 40, an O ring 41 for preventing a leakage of the suction refrigerant Ge toward an outside is disposed.
In an example of
By swirling the drive flow Gn in the nozzle part 24a, the gas-liquid separation of the drive flow Gn is performed by the centrifugal force, and a liquid film is formed on an inner wall of the throttle part of the nozzle part 24a, and a boiling of the drive flow Gn is promoted, and the nozzle efficiency is improved, and the pressure rise in the second ejector 24 is caused.
Further, since the suction flow Ge which flows into the mixing part 24c from the refrigerant suction port 24b is swirled in an opposite direction relative to the swirl direction of the drive flow Gn, swirling of the drive flow Gn in the mixing part 24c is canceled by the swirling of the suction flow Ge. As a result, the kinetic energy of swirling of the drive flow Gn can be utilized as a kinetic energy of straight movement.
Although the throttle mechanism 26 in the above embodiment is configured to swirl the refrigerant by having the refrigerant flow to flow along the tangent direction, a groove 26d in a spiral shape may be provided in the throttle mechanism 26, as illustratively shown in
Without being limited to the above-described embodiments, the present disclosure may have various changes and/or modifications as described below.
(1) Although the third evaporator 27 is used for cooling the inner space of the in-vehicle refrigerator in each of the above-mentioned embodiments, the use of the third evaporator 27 is not limited to the above. That is, the third evaporator 27 may also be used as the internal heat exchanger of a refrigeration cycle device, or as a device for cooling of an in-vehicle battery, or as a heat exchanger for cooling a seat air-conditioner, or the like.
(2) Although the refrigeration cycle device for vehicles is explained in each of the above-mentioned embodiments, the present embodiment may also be applicable, without being limited thereto, to a refrigeration cycle device for stationary use or the like.
(3) In each of the above-mentioned embodiments, what kind of refrigerant should be used is not specified. However, the refrigerant may be the one that is usable in both of the supercritical cycle and the subcritical cycle of steam compression type, such as a chloro-fluorocarbon type, a chloro-fluorocarbon alternative of HC type, a carbon dioxide (CO2), or the like.
Further, the chloro-fluorocarbon is a general term for representing an organic compound composed of carbon, fluoride, chlorine, and hydrogen in this case, and it is widely used as the refrigerant. The chloro-fluorocarbon type refrigerant includes an HCFC (i.e., a hydro-chloro-fluorocarbon) type refrigerant, an HFC (i.e., a hydro-fluorocarbon) type refrigerant, or the like, which are called as a chloro-fluorocarbon alternative due to their non-destructive characters for an ozone layer.
Further, the HC (hydrocarbon) type refrigerant includes hydrogen and carbon, and is a refrigerant material which exists in nature. The HC type refrigerant includes an R600a (i.e., isobutane), an R290 (i.e., propane), or the like.
(4) In each of the above-mentioned embodiments, a variable flow amount type ejector which can adjust a flow amount by adjusting the refrigerant flow passage area size of the nozzles 15a and 24a may be used as the first and second ejectors 15 and 24.
Number | Date | Country | Kind |
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2011-251426 | Nov 2011 | JP | national |
Filing Document | Filing Date | Country | Kind |
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PCT/JP2012/007318 | 11/15/2012 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2013/073185 | 5/23/2013 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
3447339 | Rietdijk | Jun 1969 | A |
6158237 | Riffat | Dec 2000 | A |
6857286 | Ohta | Feb 2005 | B2 |
7779647 | Takeuchi | Aug 2010 | B2 |
20040123624 | Ohta | Jul 2004 | A1 |
20060266072 | Takeuchi | Nov 2006 | A1 |
20100313582 | Oh | Dec 2010 | A1 |
20110259039 | Ma | Oct 2011 | A1 |
20120116594 | Aidoun | May 2012 | A1 |
20120234026 | Oh | Sep 2012 | A1 |
20120291461 | Verma | Nov 2012 | A1 |
20130111935 | Zou | May 2013 | A1 |
Number | Date | Country |
---|---|---|
2004-198002 | Jul 2004 | JP |
2007-003171 | Jan 2007 | JP |
2007-024412 | Feb 2007 | JP |
2007-078318 | Mar 2007 | JP |
2010-048549 | Mar 2010 | JP |
Entry |
---|
International Search Report and Written Opinion of the ISA for PCT/JP2012/007318, ISA/JP, mailed Dec. 25, 2012, with translations thereof. |
Number | Date | Country | |
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20140345318 A1 | Nov 2014 | US |