WO1990007683A1 - Dispositif a cycle de carnot renverse en conditions transcritiques - Google Patents
Dispositif a cycle de carnot renverse en conditions transcritiques Download PDFInfo
- Publication number
- WO1990007683A1 WO1990007683A1 PCT/NO1989/000089 NO8900089W WO9007683A1 WO 1990007683 A1 WO1990007683 A1 WO 1990007683A1 NO 8900089 W NO8900089 W NO 8900089W WO 9007683 A1 WO9007683 A1 WO 9007683A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- refrigerant
- pressure
- capacity
- heat exchanger
- receiver
- Prior art date
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Classifications
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B1/00—Compression machines, plants or systems with non-reversible cycle
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B45/00—Arrangements for charging or discharging refrigerant
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B40/00—Subcoolers, desuperheaters or superheaters
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B41/00—Fluid-circulation arrangements
- F25B41/20—Disposition of valves, e.g. of on-off valves or flow control valves
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B9/00—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point
- F25B9/002—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point characterised by the refrigerant
- F25B9/008—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point characterised by the refrigerant the refrigerant being carbon dioxide
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2309/00—Gas cycle refrigeration machines
- F25B2309/06—Compression machines, plants or systems characterised by the refrigerant being carbon dioxide
- F25B2309/061—Compression machines, plants or systems characterised by the refrigerant being carbon dioxide with cycle highest pressure above the supercritical pressure
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2400/00—General features or devices for refrigeration machines, plants or systems, combined heating and refrigeration systems or heat-pump systems, i.e. not limited to a particular subgroup of F25B
- F25B2400/04—Refrigeration circuit bypassing means
- F25B2400/0411—Refrigeration circuit bypassing means for the expansion valve or capillary tube
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2400/00—General features or devices for refrigeration machines, plants or systems, combined heating and refrigeration systems or heat-pump systems, i.e. not limited to a particular subgroup of F25B
- F25B2400/04—Refrigeration circuit bypassing means
- F25B2400/0415—Refrigeration circuit bypassing means for the receiver
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2400/00—General features or devices for refrigeration machines, plants or systems, combined heating and refrigeration systems or heat-pump systems, i.e. not limited to a particular subgroup of F25B
- F25B2400/16—Receivers
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2600/00—Control issues
- F25B2600/17—Control issues by controlling the pressure of the condenser
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2600/00—Control issues
- F25B2600/25—Control of valves
- F25B2600/2501—Bypass valves
Definitions
- This invention relates to vapour compression cycle devices such as refrigerators, air-conditioning units and heat pumps, using a refrigerant operating in a closed circuit under trans-critical conditions, and more particularly, to methods for modulating and controlling the capacity of such devices.
- a conventional vapour compression cycle device for refri ⁇ geration, air-conditioning or heat pump purposes is shown in principle in Fig. 1.
- the device consists of a compressor (1), a condensing heat exchanger (2), a throttling valve (3) and a evaporating heat exchanger (4). These components are connected in a closed flow circuit, in which a refrigerant is circulated.
- the operating principle of a vapour compres ⁇ sion cycle device is as follows: The pressure and tempera ⁇ ture of the refrigerant vapour is increased by the compres ⁇ sor (1), before it enters the condenser (2) where it is cooled and condensed, giving off heat to a secondary cool ⁇ ant.
- the high-pressure liquid is then throttled to the eva ⁇ porator pressure and temperature by means of the expansion valve (3).
- the evaporator (4) the refrigerant boils and absorbs heat from its surroundings.
- the vapour at the eva ⁇ porator outlet is drawn into the compressor, completing the cycle.
- refrige ⁇ rants as for instance R-12, CF 2 C1 2
- refrigerant A number of different substances or mixtures of substances may be used as a refrigerant.
- the choice of refrigerant is among others influenced by the condensation temperature, as the critical temperature of the fluid sets the upper limit for the condensation to occur. In order to maintain a reasonable efficiency, it is normally desirable to use a refrigerant with critical temperature at least 20-30K above the condensation temperature. Near- critical temperatures are normally avoided in design and operation of conventional systems.
- Capacity control of the conventional vapour compression cycle device is achieved mainly by regulating the mass flow of refrigerant passing through the evaporator. This is done e.g. by controlling the compressor capacity, throttling or bypassing. These methods involve more complicated flow cir ⁇ cuit and components, need for additional equipment and ac- cesories, reduced part-load efficiency and other compli ⁇ cations.
- a common type of liquid regulation device is a thermostatic expansion valve, which is controlled by the superheat at the evaporator outlet. Proper valve operation under varying operating conditions is achieved by using a considerable part of the evaporator to superheat the refrigerant, resul ⁇ ting in a low heat transfer coefficient.
- thermodynamic losses occur due to large temperature differences when giving off heat to a secondary coolant with large temperature increase, as in heat pump applications or when the available secondary cool ⁇ ant flow is small.
- Another object of the present invention is to provide a vapour compression cycle avoiding use of CFC refrigerants, and at the same time offering possibility to apply several attractive refrigerants with respect to safety, environ ⁇ mental hazards and price.
- Further object of the present invention is to provide a new method of capacity control, which involves operation at mainy constant refrigerant mass flow rate and simple capa ⁇ city modulation by valve operation.
- Still another object of the present invention is to provide a cycle rejecting heat at gliding temperature, reducing heat-exchange losses in applications where secondary coolant flow is small or when the secondary coolant is to be heated to a relatively high temperature.
- thermodynamic properties in the super-critical state are utilized to con ⁇ trol the refrigerating and heating capacity of the device.
- the present invention involves the regulation of specific enthalpy at evaporator inlet by deliberate use of the pres ⁇ sure and/or temperature before throttling for capacity con ⁇ trol. Capacity is controlled by varying the refrigerant enthalpy difference in the evaporator, by changing the spe ⁇ cific enthalpy of the refrigerant before throttling. In the super-critical state this can be done by varying the pres ⁇ sure and temperature independently. In a preferred embodi ⁇ ment this modulation of specific enthalpy is done by varying the pressure before throttling.
- the refrigerant is cooled down as far as it is feasible by means of the available cooling medium, and the pressure regulated to give the re ⁇ quired enthalpy.
- Another embodiment involves modulation of enthalpy by variation of the refrigerant temperature before throttling. This is done by controlling the heat rejection from the device.
- Fig. 1 is a schematic representation of a conventional (sub- critical) vapour compression cycle device.
- Fig. 2 is a schematic representation of a trans-critical vapour compression cycle device constructed in accordance with a preferred embodiment of the invention.
- This embodi ⁇ ment includes a volume as an integral part of the evaporator system, holding refrigerant in the liquid state.
- Fig. 3 is a schematic representation of a trans-critical vapour compression cycle device constructed in accordance with a second embodiment of the invention.
- This embodiment includes an intermediate pressure receiver connected direct ⁇ ly into the flow circuit between two valves.
- Fig. 4 is a schematic representation of a trans-critical vapour compression cycle device constructed in accordance with a third embodiment of the invention.
- This embodiment includes a special receiver to hold refrigerant as liquid or in the super-critical state.
- Fig. 5 is a graph illustrating the relationship of pressure versus enthalpy of the trans-critical vapour compression cycle device of Fig. 2, 3 or 4, at different operating con ⁇ ditions.
- Fig. 6 is a collection of graphs illustrating the control of refrigerating capacity by the method of pressure control in accordance with the present invention. The results shown are measured in a laboratory demonstration system built accord ⁇ ing to a preferred embodiment of the invention.
- Fig. 7 is a collection of graphs illustrating the control of refrigerating capacity by control of the heat rejection, in accordance with the present invention. The results shown are measured in a laboratory demonstration system build accord ⁇ ing to a preferred embodiment of the present invention.
- Fig. 8 is test results showing the relationship of tempera ⁇ ture versus entropy of the trans-critical vapour compression cycle device of Fig. 2, operating at different high-side pressures, employing carbon dioxide as refrigerant Detailed description of the invention
- a trans-critical vapour compression cycle device includes a refrigerant, of which critical temperature is between the temperature of the heat inlet and the mean temperature of heat submittal, and a closed working fluid circuit where the refrigerant is circu ⁇ lated.
- Suitable working fluids may be by the way of examples: ethy- len (C 2 H 4 ), diborane (B 2 H 6 ), carbon dioxide (C0 2 ), ethane (C 2 H 6 ) and nitrogen oxide (N 2 0).
- the closed working fluid circuit consists of a refrigerant flow loop with an integrated storage segment.
- Fig. 2 shows a preferred embodiment of the invention where the storage segment is an integral part of the evaporator system.
- the flow circuit includes a compressor 10 connected in series to a heat exchanger 11, a counterflow heat exchanger 12 and a throttling valve 13.
- the throttling valve can be replaced by an optional expansion device.
- An evaporating heat exchanger 14, a liquid separator/receiver 16 and the low-pressure side of the counterflow heat exchanger 12 are connected in flow communication intermediate the throttling valve 13 and the inlet 19 of the compressor 10.
- the liquid receiver 16 is connected to the evaporator outlet 15, and the gas phase outlet of the receiver 16 is connected to the counterflow heat exchanger 12.
- the counterflow heat exchanger 12 is not absolutely neces ⁇ sary for the functioning of the device but improves its efficiency, in particular its rate of response to a capacity increase requirement. It also serves to return oil to the compressor.
- a liquid phase line from the receiver (16) (shown with broken line in Fig. 2) is connect ⁇ ed to the suction line either before the counterflow heat exchanger (12) at 17 or after it at 18, or anywhere between these points.
- the liquid flow i.e. refrigerant and oil, is controlled by a suitable conventional liquid flow restrict ⁇ ing device (not shown in the figure). By allowing some ex- cess liquid refrigerant to enter the vapour line, a liquid surplus at the evaporator outlet is obtained.
- the storage segment of the working fluid circuit includes a receiver 22 integrated in the flow circuit between a valve 21 and the throttling valve 13.
- the other components 10-14 of the flow circuit is identical to the components of the previous embodiment, although the heat exchanger 12 can be omitted without any great consequence.
- the pressure in the receiver 22 is kept intermediate the high-side and low-side pressures of the flow circuit.
- the storage segment of the working fluid circuit includes a special receiver 25, where the pressure is kept between the high-side pressure and the low-side pressure of the flow circuit.
- the storage segment further consists of the valves 23 and 24 which are connected to the high pressure and low pressure part of the flow circuit respectively.
- the refrigerant is compressed to a suitable supercritical pressure in the compressor 10, the compressor outlet 20 is shown as state “a” in Fig. 5.
- the refrigerant is circulated through the heat exchanger 11 where it is cooled to state "b", giving off heat to a suitable cooling agent, e.g. cooling air or water.
- a suitable cooling agent e.g. cooling air or water.
- the refrig ⁇ erant can be further cooled to state "c" in the counterflow heat exchanger 12, before throttling to state "d".
- a two-phase gas/liquid mixture is formed, shown as state “d” in Fig. 3.
- the refrigerant absorbs heat in the evaporator 14 by eva ⁇ poration of the liquid phase.
- the refrigerant vapour can be superheated in the counterflow heat exchanger 12 to state “f" before it enters the compressor inlet 19, making the cycle complete.
- the evaporator outlet condition "e” will be in the two-phase region due to the liquid surplus at the evaporator outlet. Modulation of the trans-critical cycle device capacity is accomplished by varying the refrigerant state at the eva ⁇ porator inlet, i.e. point "d" in Fig. 5.
- the refrigerating capacity per unit of refrigerant mass flow corresponds to the enthalpy difference between state “d” and state “e”; This enthalpy difference is found as a horizontal distance in the enthalpy-pressure diagram. Fig. 5.
- Throttling is a constant enthalpy process, thus the enthalpy in point “d” is equal to the enthalpy in point "c".
- the ref igerating capacity (in k ) at constant refrigerant mass flow can be controlled by varying the en ⁇ thalpy at point "c".
- the high-pressure single-phase refrigerant vapour is not conden ⁇ sed but reduced in temperature in the heat exchanger 11.
- the terminal temperature of the refrigerant in the heat ex ⁇ changer (point “b” ) will be some degrees above the entering cooling air or water temperature, if counterflow is used.
- the high-pressure vapour can then be cooled a few degrees lower, to point "c", in the counterflow heat exchanger 12. The result is, however, that at constant cooling air or water inlet temperature, the temperature at point "c" will be mainly constant, independent of the pressure level in the high side.
- modulation of device capacity is accomplished by varying the pressure in the highside, while the temperature in point "c" is mainly constant.
- the curvature of the iso ⁇ therms near the critical point result in a variation of enthalpy with pressure, as shown in Fig. 5.
- the figure shows a reference cycle (a-b-c-d-e-f) , a cycle with reduced capa ⁇ city due to reduced high side pressure (a'-b'-c'-d'-e-f) and a cycle with increased capacity due to higher pressure in the high side (a"-b"-c"-d"-e-f) .
- the evaporator pressure is assumed to be constant.
- the pressure in the high-pressure side is independent of temperature, because it is filled with a single phase fluid. To vary the pressure it is necessary to vary the mass of refrigerant in the high side, i.e. to add or remove some of the instant refrigerant charge in the high side. These vari ⁇ ations must be taken up by a buffer, to avoid liquid over ⁇ flow or drying up of the evaporator.
- the refrigerant mass in the high side can be in ⁇ creased by temporarily reducing the opening of the throt ⁇ tling valve 13. Due to the incidentally reduced refrigerant flow to the evaporator, the excess liquid fraction at the evaporator outlet (15) will be reduced. The liquid refri ⁇ gerant flow from the receiver 16 into the suction line is however constant. Consequently, the balance between the liquid flow entering and leaving the receiver 16 is shifted, resulting in a net reduction in receiver liquid content and a corresponding accumulation of refrigerant in the high pressure side of the flow circuit.
- the increase in high side charge involves increasing pres ⁇ sure and thereby higher refrigerating capacity. This mass transfer from the low-pressure to the high-pressure side of the circuit will continue until balance between refrigerat ⁇ ing capacity and load is found.
- Opening of the throttling valve 13 will increase the excess liquid fraction at the evaporator outlet 15, because the evaporated amount of refrigerant is mainly constant. The difference between this liquid flow entering the receiver and the liquid flow from the receiver into the suction line, will accumulate. The result is a net transport of refri ⁇ gerant charge from the high side to the low side of the flow circuit, with the reduction in the high side charge stored in liquid state in the receiver. By reducing the high-side charge and thereby pressure, the capacity of the device is reduced, until balance is found.
- the refrigerant mass in the high side can be increased by simultaneously shutting the valve 21 and modulating the throttling valve 13 to provide the evaporator with suf ⁇ ficient liquid flow. This will reduce the refrigerant flow from the high side into the receiver through valve 21, while refrigerant mass is transferred from the low side to the high side by the compressor.
- Reduction of high-side charge is obtained by opening the valve 21 while keeping the flow through the throttling valve 13 mainly constant. This will transfer mass from the high- side of the flow circuit to the receiver 22.
- the refrigerant mass in the high side can be increased by opening the valve 24 and simultaneously reducing the flow through the throttling valve 13.
- refrigerant charge is accumulated in the high-pressure side due to reduced flow through the throttling valve 13.
- Sufficient liquid flow to the evaporator is obtained by opening the valve 24.
- a reduction in the high side charge can be accomplished by opening the valve 23 to transfer some refrigerant charge from the high side to the receiver. Capacity control of the device is thus accomplished by modulation of the valves 23 and 24, and simultaneously operating the throttling valve 13.
- the preferred embodiment of the invention has the advantage of simplicity, with capacity con ⁇ trol by operation of one valve only. Furthermore, the trans- critical vapour compression cycle device built according to this embodiment has a certain self-regulating capability by adapting to changes in cooling load through changes in liquid content in the receiver 16, involving changes in highside charge and thus cooling capacity. In addition, the operation with liquid surplus at evaporator outlet gives favourable heat transfer characteristics.
- the second embodiment as indicated in Fig. 3, has the ad ⁇ vantage of simplified valve operation. Valve 21 only regu ⁇ lates the pressure in the high side of the device, and the throttling valve 13 only assures that the evaporator is fed sufficiently. A conventional thermostatic valve can thus be used for throttling.
- Oil return to the compressor is easily achieved by allowing the refrigerant to flow through the receiver.
- This embodiment does not offer the capa ⁇ city control function at high-side pressures below the cri ⁇ tical pressure.
- the volume of the receiver 22 must be rela ⁇ tively large since it is only operating between the dis ⁇ charge pressure and the liquid line pressure.
- Still another embodiment as indicated in Fig. 4 has the advantage of operating as a conventional vapour compression cycle device, when it is running at stable conditions.
- the valves 23 and 24, connecting the receiver 25 to the flow circuit, are activated only during capacity control.
- This embodiment requires use of three different valves during periods of capacity change.
- Trans-critical vapour compression cycle devices built ac ⁇ cording to the described embodiments can be applied in seve ⁇ ral areas.
- the technology is well suitable in small and medium-sized stationary and mobile air-conditioning units, small and medium-sized refrigerators/freezers and in smaller heat pump units.
- One of the most promising applications is in automotive air-conditioning, where the present need for a new, non-CFC, lightweight and efficient alternative to R12- systems is urgent.
- the laboratory test device uses water as heat source, i.e. the water is refrigerated by heat exchange with boiling CO 2 in the evaporator 14. Water is also used as cooling agent, being heated by C0 2 in the heat exchanger 11.
- the test de ⁇ vice includes a 61 ccm reciprocating compressor (10) and a receiver (16) with total volume of 4 liters.
- the system also includes a counterflow heat exchanger (12) and liquid line connection from the receiver to point 17, as indicated in Fig. 2.
- the throttling valve 13 is operated manually.
- This example shows how control of refrigerating capacity is obtained by varying the position of the throttling valve 13, thereby varying the pressure in the high-side of the flow circuit.
- the specific refrigerant enthalpy at the evaporator inlet is controlled, resulting in modulation of refrigerating capacity at constant mass flow.
- the water inlet temperature to the evaporator 14 is kept constant at 20°C, and the water inlet temperature to the heat exchanger 11 is kept constant at 35°C.
- Water circu ⁇ lation is constant both in the evaporator 14 and the heat exchanger 11.
- the compressor is running at constant speed.
- Fig. 6 shows the variation of refrigerating capacity (Q), compressor shaft work (W), high ⁇ ide pressure (p H ), C0 2 mass flow (m), C0 2 temperature at evaporator outlet (t # ), C0 2 temperature at the outlet of heat exchanger 11 (t b ) and liquid level in the receiver (h) when the throttling valve 13 is operated as indicated at the top of the figure.
- the adjustment of throttling valve position is the only mani ⁇ pulation.
- capacity (Q) is easily controlled by operating the throttling valve (13). It is further clear from the figure that at stable conditions, the circulating mass flow of CO 2 (m) is mainly constant and independent of the cooling capacity. The CO 2 temperature at the outlet of heat exchanger 11 (t b ) is also mainly constant. The graphs show that the variation of capacity is a result of varying high side pressure (p H ) only.
- the water inlet temperature to the evaporator is kept constant at 20°C, and the compressor is running at constant speed.
- the cooling capacity can be kept mainly constant when the ambient temperature is rising, by in ⁇ creasing the high side pressure.
- the refrigerant mass flow is mainly constant, as shown.
- Increased high-side pressures involve a reduction in receiver liquid content, as indicated by the liquid level readings.
- FIG. 7 shows the variation of refrigerating capacity (Q) when the circulation rate of cooling water (m w ) is regulated as shown at the top of the figure.
- the mass flow of C0 2 (m), the high-side pressure (p H ) and the water inlet temperature to heat exchanger 11 (ti) are kept constant.
- the compressor is running at constant speed and both the temperature and flow rate of water entering the evaporator are kept constant.
- the refrigerating capacity is easily controlled by variation of the water flow, as shown in the figure. Mass flow of C0 2 is mainly constant.
- Fig. 8 is a graphic representation of trans critical cycles in the entropy/temperature diagram. The cycles shown in the diagram are based on measurements on the laboratory test device, during operation at five different high-side pressures. The evaporator pressure is kept constant, refrigerant is C0 2 .
- the diagram gives a good impression of the capacity control principle, indicating the changes in specific enthalpy (h) at evaporator inlet caused by variation of the high-side pressure (p) .
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- General Engineering & Computer Science (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Chemical & Material Sciences (AREA)
- Compression-Type Refrigeration Machines With Reversible Cycles (AREA)
- Devices That Are Associated With Refrigeration Equipment (AREA)
- Heating, Cooling, Or Curing Plastics Or The Like In General (AREA)
- Separation, Recovery Or Treatment Of Waste Materials Containing Plastics (AREA)
- Air-Conditioning For Vehicles (AREA)
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Abstract
La présente invention utilise la régulation de l'enthalpie spécifique à l'entrée de l'évaporateur par utilisation délibérée de la pression et/ou de la température avant l'étranglement pour obtenir un réglage de la capacité. La capacité est réglée par variation de la différence d'enthalpie du réfrigérant dans l'évaporateur et par modification de l'enthalpie spécifique du réfrigérant avant l'étranglement. En état surcritique, ce réglage peut être assuré par variation de la pression et de la température séparément. Dans un mode de réalisation préféré, cette modulation de l'enthalpie spécifique est effectuée par variation de la pression avant étranglement. Le réfrigérant est refroidi à une température aussi basse qu'il est possible de descendre au moyen du milieu de refroidissement disponible et la pression est régulée pour produire l'enthalpie requise. Dans un autre mode de réalisation, on utilise la modulation de l'enthalpie par variation de la température du réfrigérant avant étranglement, ce qui est effectué par réglage du rejet de chaleur depuis le dispositif.
Priority Applications (14)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE68908181T DE68908181T3 (de) | 1989-01-09 | 1989-09-06 | Verfahren zum betrieb eines kaltdampfprozesses unter trans- oder überkritischen bedingungen. |
EP89910211A EP0424474B2 (fr) | 1989-01-09 | 1989-09-06 | Procede pour operer un cycle de carnot renverse en conditions transcritiques ou supercritiques |
JP1509515A JPH0718602B2 (ja) | 1989-01-09 | 1989-09-06 | 超臨界蒸気圧縮サイクルの運転方法およびその装置 |
KR1019900701990A KR0126550B1 (ko) | 1989-01-09 | 1989-09-06 | 증기압축 사이클의 용량조정방법 및 그 사이클을 포함하는 자동차 공기조화장치 |
UA93003690A UA27758C2 (uk) | 1989-01-09 | 1989-09-06 | Спосіб регулювання тиску на боці високого тиску пристрою і холодильний чи нагрівальний пристрій (варіанти) |
DE8989910211A DE68908181D1 (de) | 1989-01-09 | 1989-09-06 | Verfahren zum betrieb eines kaltdampfprozesses unter trans- oder ueberkritischen bedingungen. |
CA002018250A CA2018250C (fr) | 1989-09-06 | 1990-06-05 | Dispositif a cycle de compression de vapeur trans-critique |
AU56968/90A AU635031B2 (en) | 1989-09-06 | 1990-06-08 | Trans-critical vapour compression cycle device |
PL28596690A PL285966A1 (en) | 1989-01-09 | 1990-07-06 | Circulation device for compression of criotical process steam |
HU904128A HU213995B (en) | 1989-09-06 | 1990-07-06 | Method for controlling the capacity of steam-compression cycle and apparatus for carrying out steam-compression cycle of controlled capacity particularly air-conditioning apparatus of automatic operation |
ES9001955A ES2025443A6 (es) | 1989-09-06 | 1990-07-19 | Metodo para regular la capacidad de un ciclo de compresion de vapor y dispositivo acondicionador de aire para automocion. |
BR909004438A BR9004438A (pt) | 1989-09-06 | 1990-09-06 | Processo para a regulagem da capacidade de um ciclo de compressao a vapor e dispositivo de condicionamento de ar para automotivos |
DK214690A DK167985B1 (da) | 1989-01-09 | 1990-09-07 | Fremgangsmaade ved regulering af et kompressionskoelesystem og varme/koeleanordning til udoevelse af fremgangsmaaden |
NO903903A NO171810C (no) | 1989-01-09 | 1990-09-07 | Fremgangsmaate ved regulering av et kompresjonskuldesystemsamt kjoeleanordning for utfoerelse av fremgangsmaaten |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NO890076A NO890076D0 (no) | 1989-01-09 | 1989-01-09 | Luftkondisjonering. |
NO890076 | 1989-01-09 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO1990007683A1 true WO1990007683A1 (fr) | 1990-07-12 |
Family
ID=19891609
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/NO1989/000089 WO1990007683A1 (fr) | 1989-01-09 | 1989-09-06 | Dispositif a cycle de carnot renverse en conditions transcritiques |
Country Status (10)
Country | Link |
---|---|
EP (1) | EP0424474B2 (fr) |
JP (1) | JPH0718602B2 (fr) |
KR (1) | KR0126550B1 (fr) |
DE (2) | DE68908181D1 (fr) |
DK (1) | DK167985B1 (fr) |
NO (2) | NO890076D0 (fr) |
PL (1) | PL285966A1 (fr) |
RU (1) | RU2039914C1 (fr) |
UA (1) | UA27758C2 (fr) |
WO (1) | WO1990007683A1 (fr) |
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- 1989-09-06 JP JP1509515A patent/JPH0718602B2/ja not_active Expired - Lifetime
- 1989-09-06 KR KR1019900701990A patent/KR0126550B1/ko not_active IP Right Cessation
- 1989-09-06 DE DE8989910211A patent/DE68908181D1/de not_active Expired - Lifetime
- 1989-09-06 UA UA93003690A patent/UA27758C2/uk unknown
- 1989-09-06 WO PCT/NO1989/000089 patent/WO1990007683A1/fr active IP Right Grant
- 1989-09-06 DE DE68908181T patent/DE68908181T3/de not_active Expired - Lifetime
- 1989-09-06 EP EP89910211A patent/EP0424474B2/fr not_active Expired - Lifetime
-
1990
- 1990-07-06 RU SU904830938A patent/RU2039914C1/ru not_active IP Right Cessation
- 1990-07-06 PL PL28596690A patent/PL285966A1/xx unknown
- 1990-09-07 DK DK214690A patent/DK167985B1/da not_active IP Right Cessation
- 1990-09-07 NO NO903903A patent/NO171810C/no not_active IP Right Cessation
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WO1993006423A1 (fr) * | 1991-09-16 | 1993-04-01 | Sinvent A/S | Procede de regulation de pression en partie haute dans un dispositif a cycle de carnot renverse transcritique |
KR100331717B1 (ko) * | 1991-12-27 | 2002-08-08 | 신벤트에이.에스 | 증기압축사이클장치의하이사이드압력을제어하는장치 |
WO1993013370A1 (fr) * | 1991-12-27 | 1993-07-08 | Sinvent A/S | Dispositif a cycle de compression de vapeur transcritique avec element a volume variable en partie haute |
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AU662589B2 (en) * | 1991-12-27 | 1995-09-07 | Sinvent As | Transcritical vapor compression cycle device with a variable high side volume element |
US5655378A (en) * | 1992-12-11 | 1997-08-12 | Sinvent A/S | Trans-critical vapor compression device |
WO1994014016A1 (fr) * | 1992-12-11 | 1994-06-23 | Sinvent A/S | Dispositif de compression trans-critique de vapeur |
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Also Published As
Publication number | Publication date |
---|---|
DE68908181D1 (de) | 1993-09-09 |
DE68908181T3 (de) | 1998-06-18 |
EP0424474A1 (fr) | 1991-05-02 |
DK214690A (da) | 1990-11-06 |
DE68908181T2 (de) | 1994-04-14 |
NO903903D0 (no) | 1990-09-07 |
KR910700437A (ko) | 1991-03-15 |
NO171810C (no) | 1993-05-05 |
PL285966A1 (en) | 1991-03-25 |
DK167985B1 (da) | 1994-01-10 |
EP0424474B1 (fr) | 1993-08-04 |
DK214690D0 (da) | 1990-09-07 |
DE68908181T4 (de) | 1995-06-14 |
UA27758C2 (uk) | 2000-10-16 |
NO890076D0 (no) | 1989-01-09 |
NO171810B (no) | 1993-01-25 |
RU2039914C1 (ru) | 1995-07-20 |
EP0424474B2 (fr) | 1997-11-19 |
JPH03503206A (ja) | 1991-07-18 |
JPH0718602B2 (ja) | 1995-03-06 |
NO903903L (no) | 1990-09-07 |
KR0126550B1 (ko) | 1998-04-03 |
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