1. Field of the Invention
The present invention relates to vapor compression systems and, more particularly, to a transcritical multi-stage vapor compression system.
2. Description of the Related Art
Vapor compression systems are used in a variety of applications including heat pump, air conditioning, and refrigeration systems. Such systems typically employ working fluids, or refrigerants, that remain below their critical pressure throughout the entire vapor compression cycle. Some vapor compression systems, however, such as those employing carbon dioxide as the refrigerant, typically operate as transcritical systems wherein the refrigerant is compressed to a pressure exceeding its critical pressure and wherein the suction pressure of the refrigerant is less than the critical pressure of the refrigerant. The basic structure of such a system includes a compressor for compressing the refrigerant to a pressure that exceeds its critical pressure. Heat is then removed from the refrigerant in a first heat exchanger, e.g., a gas cooler. The pressure of the refrigerant discharged from the gas cooler is reduced in an expansion device and the low pressure refrigerant then enters a second heat exchanger, e.g., an evaporator, where it absorbs thermal energy before being returned, as a vapor, to the compressor.
The expansion devices employed in such systems are often variable expansion valves that can be adjusted to control the operation of the system. It is also known to combine such variably adjustable expansion valves with a flash tank and a two stage compressor whereby the variably adjustable expansion valves are disposed on the inlet and outlet side of the flash tank. The flash gas tank also includes an economizer line conveying refrigerant vapor from the tank to a point between the two stages of the compressor assembly. The variable expansion valves upstream and downstream of the flash gas tank can be used to regulate the quantity of refrigerant contained within the flash tank and thereby also regulate the pressure within the gas cooler.
One problem associated with use of such variable expansion valves is that they are expensive. Another problem is that they have moving parts and therefore are subject to mechanical failure.
An inexpensive and reliable apparatus for adjusting the efficiency and capacity of a transcritical multi-stage vapor compression system is desirable.
The present invention provides a transcritical vapor compression system that includes a non-variable expansion device, such as a capillary tube, and a refrigerant storage vessel that contains a variable mass of refrigerant. By controlling the mass of refrigerant within the refrigerant storage tank, the remaining charge of refrigerant actively circulating within the vapor compression system is also controlled. Further, by controlling the charge of actively circulated refrigerant, the gas cooler pressure and, consequently, the capacity and efficiency of the vapor compression system can be regulated.
The invention comprises, in one form thereof, a transcritical vapor compression system including a fluid circuit circulating a refrigerant in a closed loop. The fluid circuit has operably disposed therein, in serial order, a compressor, a first heat exchanger, at least one non-variable expansion device and a second heat exchanger. The compressor compresses the refrigerant from a low pressure to a supercritical pressure. The first heat exchanger is positioned in a high pressure side of the fluid circuit and contains refrigerant at a first supercritical pressure. The second heat exchanger is positioned in a low pressure side of the fluid circuit and contains refrigerant at a second subcritical pressure. The at least one non-variable expansion device reduces the pressure of the refrigerant from a supercritical pressure to a relatively lower pressure wherein the at least one non-variable expansion device defines a pressure reduction substantially equivalent to the pressure difference between the first pressure and the second pressure. A refrigerant storage vessel is in fluid communication with the fluid circuit and has a variable mass of refrigerant stored therein.
The present invention comprises, in another form thereof, a transcritical vapor compression system including a fluid circuit circulating a refrigerant in a closed loop. The fluid circuit has operably disposed therein, in serial order, a compressor, a first heat exchanger, at least one non-variable expansion device and a second heat exchanger. The compressor compresses the refrigerant from a low pressure to a supercritical pressure. The first heat exchanger is positioned in a high pressure side of the fluid circuit and contains refrigerant at a first supercritical pressure. The second heat exchanger is positioned in a low pressure side of the fluid circuit and contains refrigerant at a second subcritical pressure. The at least one non-variable expansion device reduces the pressure of the refrigerant from a supercritical pressure to a relatively lower pressure wherein the at least one non-variable expansion device defines a pressure reduction substantially equivalent to the pressure difference between the first pressure and the second pressure. A refrigerant storage vessel is in fluid communication with the non-variable expansion device between the first and second heat exchangers. A temperature adjustment device is disposed in thermal exchange with the refrigerant storage vessel wherein a temperature of refrigerant in the refrigerant storage vessel is adjustable with the temperature adjustment device.
The present invention comprises, in yet another form thereof, a method of controlling a transcritical vapor compression system. A fluid circuit circulating a refrigerant in a closed loop is provided. The fluid circuit has operably disposed therein, in serial order, a compressor, a first heat exchanger, at least one non-variable expansion device and a second heat exchanger. The refrigerant is compressed from a low pressure to a supercritical pressure in the compressor. Thermal energy is removed from the refrigerant in the first heat exchanger. The pressure of the refrigerant is reduced in the at least one non-variable expansion device wherein the at least one non-variable expansion device defines a pressure reduction substantially equivalent to the pressure difference between a first supercritical pressure of the refrigerant in the first heat exchanger and a second subcritical pressure of the refrigerant in the second heat exchanger. Thermal energy is added to the refrigerant in the second heat exchanger. A refrigerant storage vessel in fluid communication with the fluid circuit is provided and the mass of the refrigerant within the refrigerant storage vessel is controlled to thereby regulate the capacity of the system.
An advantage of the present invention is that the capacity and efficiency of the system can be regulated with inexpensive non-moving parts. Thus, the system of the present invention is less costly and more reliable than prior art systems.
The above mentioned and other features and objects of this invention, and the manner of attaining them, will become more apparent and the invention itself will be better understood by reference to the following description of an embodiment of the invention taken in conjunction with the accompanying drawings, wherein:
Corresponding reference characters indicate corresponding parts throughout the several views. Although the exemplification set out herein illustrates an embodiment of the invention, the embodiment disclosed below is not intended to be exhaustive or to be construed as limiting the scope of the invention to the precise form disclosed.
A vapor compression system 30 in accordance with the present invention is schematically illustrated in
After the pressure of the refrigerant is reduced by expansion device 42, the refrigerant enters yet another heat exchanger in the form of an evaporator 44 positioned in a high pressure side of the fluid circuit. The refrigerant absorbs thermal energy in the evaporator 44 as the refrigerant is converted from a liquid phase to a vapor phase. The evaporator 44 may be of a conventional construction well known in the art. After exiting evaporator 44, the refrigerant is returned to compression mechanism 32 and the cycle is repeated.
Also included in system 30 is a refrigerant storage vessel in the form of a flash gas tank 50 having a variable mass of refrigerant stored therein. In illustrated system 30, flash gas tank 50 is in fluid communication with system 30 between gas cooler 38 and non-variable expansion device 42 and stores a variable mass of refrigerant as discussed in greater detail below.
As shown in
In operation, the illustrated embodiment of system 30 is a transcritical system utilizing carbon dioxide as the refrigerant wherein the refrigerant is compressed above its critical pressure and returns to a subcritical pressure with each cycle through the vapor compression system. Refrigerant enters the expansion device 42 at the supercritical pressure. The pressure of the refrigerant is lowered to a subcritical pressure as the refrigerant passes through expansion device 42.
Capacity control for such a transcritical system differs from a conventional vapor compression system wherein the refrigerant remains at subcritical pressures throughout the vapor compression cycle. In such subcritical systems, capacity control is often achieved using thermal expansion valves to vary the mass flow through the system and the pressure within the condenser is primarily determined by the ambient temperature. In a transcritical system, the capacity of the system is often regulated by controlling the pressure within the high pressure gas cooler while maintaining a substantially constant mass flow rate. The pressure within the gas cooler may be regulated by controlling the total charge of refrigerant circulating in the system wherein an increase in the total charge results in an increase in the mass and pressure of the refrigerant within the gas cooler, e.g., cooler 38, and an increase in the capacity of the system. On the other hand, a decrease in the circulating charge results in a decrease in the pressure within the gas cooler and a decrease in the capacity of the system. The efficiency of the system will also vary with changes in the pressure in gas cooler 38. However, gas cooler pressures that correspond to the optimal efficiency of system 30 and the maximum capacity of system 30 will generally differ.
By regulating the mass of the refrigerant contained within flash gas tank 50, the total charge of the refrigerant that is actively circulating within system 30 can be controlled and, thus, the pressure of gas cooler 38 and the capacity and efficiency of system 30 can also be controlled. The mass of refrigerant contained within tank 50 may be controlled by various means including the regulation of the temperature of tank 50 or the regulation of the available storage volume within tank 50 for containing refrigerant.
In the embodiment of
An electronic control unit (ECU) 54 may be used to control the operation of the heater/cooler 52 based upon temperature and/or pressure sensor readings obtained at appropriate locations in the system, e.g., temperature and pressure data obtained at the inlet and outlet of gas cooler 38 and evaporator 44 and in flash gas tank 50 and thereby determine the current capacity of the system and load being placed on the system. Manole describes another method of determining the pressure of a gas cooler in a transcritical system by taking external temperature measurements of the gas cooler in U.S. Provisional Patent Application Ser. No. 60/505,817 entitled METHOD AND APPARATUS FOR DETERMINING SUPERCRITICAL PRESSURE IN HEAT EXCHANGER filed on Sep. 25, 2003 which may also be used with the present invention and is hereby incorporated herein by reference. The pressure within gas cooler 38 may also be determined by taking temperature measurements of the ECU 54 may also control the operation of the heater/cooler 52 based upon work done by compressor 32 as measured with a multimeter or the pressure at the exit of compressor 32 as measured with a pressure gauge. As described above heater/cooler 52 is controllable such that refrigerant may be accumulated or released in or from the flash gas tank 50 to thereby increase or decrease the capacity of the system to correspond to the load placed on the system.
In the embodiment of
The thermodynamic properties of carbon dioxide are shown in the graph of
The area below lines 82, 84 represents the two phase subcritical region where boiling of carbon dioxide takes place at a constant pressure and temperature. The area above point 86 represents the supercritical region where cooling or heating of the carbon dioxide does not change the phase (liquid/vapor) of the carbon dioxide. The phase of carbon dioxide in the supercritical region is commonly referred to as “gas” instead of liquid or vapor.
The lines Qmax and COPmax represent gas cooler discharge values for maximizing the capacity and efficiency respectively of the system. The central line positioned therebetween represents values that provide relatively high, although not maximum, capacity and efficiency. Moreover, if the system is operated to correspond to the central line, when the system fails to operate according to design parameters defined by this central line, the system will suffer a decrease in either the capacity or efficiency and an increase in the other value unless such variances are of such magnitude that they represent a point no longer located between the Qmax and COPmax lines.
Point A represents the refrigerant properties as discharged from compression mechanism 32 and at the inlet of gas cooler 38. Point B represents the refrigerant properties at the outlet of gas cooler 38 and the inlet to expansion device 42. Point C represents the refrigerant properties at the inlet of evaporator 44 and outlet of expansion device 42. Point D represents the refrigerant properties at the inlet to compression mechanism 32 and the outlet of evaporator 44. Movement from point D to point A represents the compression of the refrigerant. As can be seen, compressing the refrigerant both raises its pressure and its temperature. Moving from point A to point B represents the cooling of the high pressure refrigerant at a constant pressure in gas cooler 38. Movement from point B to point C represents the action of expansion device 42 which lowers the pressure of the refrigerant to a subcritical pressure.
More specifically, in the embodiment illustrated in
Movement from point C to point D represents the action of evaporator 44. Since the refrigerant is at a subcritical pressure in evaporator 44, thermal energy is transferred to the refrigerant to change it from a liquid phase to a gas phase at a constant temperature and pressure. The capacity of the system (when used as a cooling system) is determined by the mass flow rate through the system and the length of line C-D which in turn is determined by the specific enthalpy of the refrigerant at the evaporator inlet, i.e., the location of point C. Thus, reducing the specific enthalpy at the evaporator inlet without substantially changing the mass flow rate and without altering the other operating parameters of system 30, will result in a capacity increase in the system. This can be done by decreasing the mass of refrigerant contained in flash gas tank 50, thereby increasing both the mass and pressure of refrigerant contained in gas cooler 38. If the refrigerant in gas cooler 38 is still cooled to the same gas cooler discharge temperature, this increase in gas cooler pressure will shift line A–B upwards and move point B to the left (as depicted in
During compression of the refrigerant, vapor at a relatively low pressure and temperature enters compression mechanism 32 and is discharged therefrom at a higher temperature and a supercritical discharge pressure. When tank 50 relies upon temperature regulation to control the mass of refrigerant contained therein, tank 50 is advantageously positioned to receive refrigerant at a point after the refrigerant has been cooled in gas cooler 38. The mass of refrigerant contained within tank 50 is dependent upon the density of the refrigerant and the available storage volume within tank 50. The density of the refrigerant is, in turn, dependent upon the relative amounts of the liquid phase fraction 46 and the vapor phase fraction 48 of the refrigerant that is contained within tank 50. By increasing the quantity of the liquid phase refrigerant 46 in tank 50, the mass of the refrigerant contained therein is also increased. Similarly, the mass of the refrigerant contained in tank 50 may be decreased by decreasing the quantity of liquid phase refrigerant 46 contained therein. By reducing the temperature of the refrigerant within tank 50 below the saturation temperature of the refrigerant, the quantity of liquid phase refrigerant 46 contained within tank 50 may be increased. Similarly, by raising the temperature of tank 50, and the refrigerant contained therein, some of the liquid phase refrigerant 46 can be evaporated and the quantity of the liquid phase refrigerant 46 contained therein may be reduced. A system in which a vessel containing a variable mass of refrigerant is provided between two stages of a multi-stage compressor mechanism is described by Manole in a U.S. patent application entitled MULTI-STAGE VAPOR COMPRESSION SYSTEM WITH INTERMEDIATE PRESSURE VESSEL, Ser. No. 10/653,581, filed on Sep. 2, 2003, and is hereby incorporated herein by reference.
In the embodiment of
Several exemplary embodiments of the flash gas tank 50 and the heater/cooler 52 are represented in
Embodiment 50b regulates the temperature of tank 50b by providing a means of imparting heat to the contents of tank 50b. In embodiment 50b schematically represented in
Embodiment 50c is schematically represented in
Embodiment 50d is schematically represented in
Other embodiments of flash gas tanks having a variable storage volume may utilize expandable/contractible chambers that are formed using flexible bladders. Various other embodiments of such tanks that may be used with the present invention are described in greater detail by Manole, et al. in a U.S. patent application entitled APPARATUS FOR THE STORAGE AND CONTROLLED DELIVERY OF FLUIDS, Ser. No. 10/653,502, filed on Sep. 2, 2003, and is hereby incorporated herein by reference.
Second embodiment 30a of a vapor compression system in accordance with the present invention is schematically represented in
After the refrigerant is cooled in gas cooler 38, the pressure of the refrigerant is then reduced by first expansion device 42a. Advantageously, expansion device 42a reduces the pressure of the refrigerant to a subcritical pressure and the refrigerant collects in flash gas tank 50 as part liquid 46 and part vapor 48. The liquid refrigerant 46 collects at the bottom of the flash gas tank 50 and is again expanded by second expansion device 42b. The refrigerant then enters evaporator 44 where it is boiled and cools a secondary medium, such as air, that may be used, for example, to cool a refrigerated cabinet. The refrigerant discharged from the evaporator 44 then enters the compression mechanism 32 to repeat the cycle.
By heating or cooling the flash gas tank 50, the mass of refrigerant in the flash gas tank 50, and the gas cooler 38, can be regulated to control the pressure in the gas cooler. An ECU can monitor the pressure in the cooler 38 and control heater/cooler 52 accordingly.
If the pressure in the gas cooler 38 is above a desired pressure, the power consumption of compressor 32 is also above a desired level. The ECU can operate the heater/cooler 52 to lower the temperature of the tank 50, thereby increasing the amount of charge in the flash gas tank 50, and decreasing both the amount of charge and the pressure in the gas cooler 38. Conversely, if the pressure in the gas cooler 38 is below the desired pressure, the ECU can operate the heater/cooler 52 to increase the temperature of the tank 50, thereby increasing both the amount of charge and the pressure in the gas cooler 38. As the pressure in the gas cooler 38 changes, the heater/cooler 52 to heat or cool the flash gas tank 50 as needed so that a desirable gas cooler pressure and a desirable system capacity and efficiency can be achieved.
By selectively controlling the operation of the heater/cooler 52, the amount of charge stored in the flash gas tank 50 can be varied, which in turn varies the mass of refrigerant, and pressure, in gas cooler 38, to achieve the gas cooler pressure corresponding to the desired capacity and/or efficiency. As discussed above, by regulating the pressure in the gas cooler 38, the specific enthalpy of the refrigerant at the entry of the evaporator 44 (point C in
Third embodiment 30b of a vapor compression system in accordance with the present invention is schematically represented in
The fan 92 and the heat exchanger 90 form a temperature adjustment device capable of adjusting the temperature of the refrigerant in the flash gas tank 50. Thus, the fan 92 and the heat exchanger 90 can regulate the pressure of the refrigerant in the gas cooler 38 and the capacity and efficiency of the system 30b. Other details of the system 30b are similar to that of systems 30, 30a and thus are not discussed herein.
Fan 92 may also be used without heat exchanger 90 wherein fan 92, blows air directly on flash gas tank 50 in order to change the temperature of the refrigerant therein.
Fourth embodiment 30c of a vapor compression system in accordance with the present invention is schematically represented in
In this embodiment, the first compressor 32a compresses the refrigerant from a low pressure to an intermediate pressure. The cooler 36 is positioned between the compressors 32a, 32b to cool the intermediate refrigerant. After the fluid line 33 communicates the refrigerant to the second compressor 32b, the second compressor 32b compresses the refrigerant from the intermediate pressure to the supercritical pressure.
In the embodiment of
The systems discussed above are described as including a fan 92 or other form of a heater/cooler 52 in order to change the temperature of the refrigerant within the flash gas tank 50. The present invention is not limited to these exemplary embodiments of a heating or cooling device, however. Rather, the present invention may include alternative devices capable of heating or cooling the refrigerant, such as a Peltier device, for example. Peltier devices are well known in the art and, with the application of a DC current, move heat from one side of the device to the other side of the device and, thus, could be used for either heating or cooling purposes.
In the embodiments in which the temperature of the flash gas tank is regulated to vary the mass of refrigerant contained therein, the temperature of the refrigerant contained within the flash gas tank may also be regulated by using a heating/cooling device to adjust the temperature of the refrigerant in the fluid circuit immediately upstream of the flash gas tank and thereby indirectly control the temperature of the refrigerant within the tank by controlling the temperature of the refrigerant entering the tank. For example, a Peltier device, or other heating/cooling device, could be mounted on the fluid line entering tank 50 in proximity to tank 50, e.g., between expansion device 42a and tank 50 in the embodiments of
It is also possible to add a filter or filter-drier immediately upstream of any of the expansion devices included in the above embodiments. Such a filter can prevent any sort of contamination in the system, e.g., copper filings, abrasive materials or brazing debris, from collecting in the expansion device and thereby obstructing the passage of refrigerant.
While this invention has been described as having an exemplary design, the present invention may be further modified within the spirit and scope of this disclosure. This application is therefore intended to cover any variations, uses, or adaptations of the invention using its general principles. Particularly, the components of the various embodiments described herein may be combined in numerous ways within the scope of the present invention.
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