[2] Chlorine containing refrigerants have been phased out in most of the world due to their ozone destroying potential. Hydrofluoro carbons (HFCs) have been used as replacement refrigerants, but these refrigerants still have high global warming potential. "Natural"refrigerants, such as carbon dioxide and propane, have been proposed as replacement fluids. Unfortunately, there are problems with the use of many of these fluids as well. Carbon dioxide has a low critical point, which causes most air conditioning systems utilizing carbon dioxide to run partially above the critical point, or to run transcritical, under most conditions. The pressure of any subcritical fluid is a function of temperature under saturated conditions (when both liquid and vapor are present). However, when the temperature of the fluid is higher than the critical temperature (supercritical), the pressure becomes a function of the density of the fluid.

[3] When a vapor compression system is run transcritical, it is advantageous to regulate the high pressure component of the system. By regulating the high pressure of the system, the capacity and/or efficiency of the system can be controlled and optimized.

[4] In the prior art, the high pressure component of a vapor compression system has been regulated by adjusting a valve located at the exit of the gas cooler, allowing for control of system capacity and efficiency. Suction line heat exchangers and storage tanks have also been employed to increase system capacity and efficiency.

SUMMARY OF THE INVENTION [5] A transcritical vapor compression system includes a compressor, a gas cooler, an expansion machine, and an evaporator. Refrigerant is circulated though the closed circuit cycle. Preferably, carbon dioxide is used as the refrigerant. As carbon dioxide has a low critical point, systems utilizing carbon dioxide as a refrigerant usually require the vapor compression system to run transcritical. When the system is run transcritical, it is advantageous to regulate the high pressure component of the vapor compression system to control and optimize the capacity and/or efficiency of the system.

[6] The expansion machine is a work recovery device which extracts energy from the expansion process. The expansion machine increases the efficiency of the system by providing a more isentropic expansion process. Increasing the flowrate through the expansion machine causes more mass to leave the high pressure part of the system, decreasing the instantaneous refrigerant mass in the high pressure part of the system, decreasing the high pressure in the system. Decreasing the flowrate through the expansion machine causes less mass to leave the high pressure part of the system, increasing the instantaneous refrigerant mass in the high pressure part of the system, increasing the high pressure in the system.

[7] In one example, after expansion, the refrigerant flow enters a separator tank.

The vapor phase of the expanded flow is recompressed in a recompressor and injected into the high pressure part of the system. Preferably, the refrigerant is injected at the input of the gas cooler. The recompressor is directly linked to the expansion machine.

By controlling the flowrate through the recompressor, the flowrate through the expansion machine, and therefore the high pressure component of the system, is controlled. A first valve positioned between the expanded flow and the recompressor regulates the amount of flow provided to the recompressor and the flowrate through the recompressor. The high pressure in the gas cooler is monitored by a control. As the pressure in the gas cooler changes, the control adjusts the first valve to achieve the optimal system pressure.

[8] If the first valve is closed, the amount of flow provided to the recompressor decreases, decreasing the load which the recompressor applies on the expansion machine and increasing the flowrate through the expansion machine which causes the supercritical pressure in the system to decrease. If the first valve is opened, the amount of flow provided to the recompressor increases, increasing the load which the recompressor applies on the expansion machine, decreasing the flowrate through the expansion machine and increasing the supercritical pressure in the system.

[9] The system can further include a second valve positioned between the expanded flow and the evaporator to operate as an economized cycle. The second valve controls the superheat at the suction of the compressor to vary the mass flowrate through the evaporator. The cool vapor flow bypasses the evaporator through a vapor bypass line to cool the suction of the compressor.

[10] In another example, the refrigerant from the suction of the compressor is recompressed in the compressor. Alternately, refrigerant from the gas cooler exchanges heat with refrigerant from the recompressor in a heat exchanger. This refrigerant from the heat exchanger is then recompressed. These alternative examples each include provisions for control of the flowrate through the expansion machine to control and optimize the capacity and/or efficiency of the system.

[11] These and other features of the present invention will be best understood from the following specification and drawings.

BRIEF DESCRIPTION OF THE DRAWINGS [12] The various features and advantages of the invention will become apparent to those skilled in the art from the following detailed description of the currently preferred embodiment. The drawings that accompany the detailed description can be briefly described as follows: [13] Figure 1 illustrates a schematic diagram of a prior art vapor compression system; [14] Figure 2 illustrates a thermodynamic diagram of a transcritical vapor compression system; [15] Figure 3a illustrates a schematic diagram of a first example of the transcritical vapor compression system including a recompressor to regulate the expander machine flowrate to control the high pressure component of the system; [16] Figure 3b illustrates a schematic diagram of a first example of the transcritical vapor compression system including a recompressor regulated by a motor to regulate the expander machine flowrate to control the high pressure component of the system; [17] Figure 4a illustrates a schematic diagram of a second example of a transcritical vapor compression system including a recompressor to regulate the expander machine flowrate to control the high pressure component of the system; and [18] Figure 4b illustrates a schematic diagram of a second example of a transcritical vapor compression system including a recompressor regulated by a motor to regulate the expander machine flowrate to control the high pressure component of the system; [19] Figure 5a illustrates a schematic diagram of a third example of a transcritical vapor compression system including a recompressor to regulate the expander machine flowrate to control the high pressure component of the system; and [20] Figure 5b illustrates a schematic diagram of a third example of a transcritical vapor compression system including a recompressor regulated by a motor to regulate the expander machine flowrate to control the high pressure component of the system.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT [21] Figure 1 illustrates a prior art vapor compression system 20 including a compressor 22 having a motor 30, a heat rejecting heat exchanger (a gas cooler in transcritical cycles) 24, an expansion valve 26, and a heat accepting heat exchanger (an evaporator) 28.

[22] Refrigerant circulates though the closed circuit cycle 20. Preferably, carbon' dioxide is used as the refrigerant. While carbon dioxide is illustrated, other refrigerants may be used. Because carbon dioxide has a low critical point, systems utilizing carbon dioxide as a refrigerant usually require the vapor compression system 20 to run transcritical. When the system 20 is run transcritical, it is advantageous to regulate the high pressure component of the vapor compression system 20. By regulating the high pressure of the system 20, the capacity and/or efficiency of the system 20 can be controlled and optimized.

[23] The refrigerant exits the compressor 22 at high pressure and enthalpy, shown by point A in Figure 2. As the refrigerant flows through the gas cooler 24 at high pressure, it loses heat and enthalpy, exiting the gas cooler 24 with low enthalpy and high pressure, indicated as point B. As the refrigerant passes through the expansion valve 26, the pressure drops isenthalpicly, shown by point C. After expansion, the refrigerant passes through the evaporator 28 and exits at a high enthalpy and low pressure, represented by point D. After the refrigerant passes through the compressor 22, it is again at high pressure and enthalpy, completing the cycle.

[24] The supercritical pressure in the high pressure component of the system 20 is a function of temperature and density. Density is a function of both mass and volume.

The volume inside the high pressure component of the system 21 is typically constant and the temperature of the high pressure part of the system 20 is generally not controlled to maximize system 20 efficiency. Therefore, the supercritical pressure of a transcritical system 20 is controlled by controlling the mass of refrigerant inside the high pressure component of the system 20. The mass in the high pressure component of the system 20 is a function of the mass flowrate exiting the compressor 22 and the mass flowrate entering the expansion valve 26. Therefore, controlling the flowrate through the expansion valve 26 can directly control the supercritical pressure in the high pressure component of the transcritical system 20 can be directly controlled.

[25] Figure 3a schematically illustrates a first example of the system 21 of the present invention. The system 21 includes an expansion machine 27. The expansion machine 27 is a work recovery device which extracts energy from the expansion process. The amount of energy available for extraction in the expansion machine 27 is a product of the flowrate through the expansion machine 27, the enthalpy difference between isenthalpic (constant enthalpy) and isentropic (constant entropy) expansion between the inlet and exit pressure of the expansion machine 27, and the expansion efficiency. The product is generally a function of the pressure difference between the high pressure and the low pressure and the mass flowrate through the expansion machine 27.

[26] The expansion machine 27 increases the efficiency of the system 21 by providing a more isentropic (constant entropy) expansion process, as opposed to a isenthalpic (constant enthalpy) expansion process that is provided by use of the prior art expansion valve 26 or orifice. This more isentropic expansion process decreases the enthalpy of the refrigerant entering the evaporator 28, allowing more heat to be absorbed in the evaporator 28 and thus increasing the cooling capacity of the system 21. The expansion machine 27 additionally increases the efficiency of the system 21 by capturing the energy of expansion and using this energy to offset normal system energy requirements.

[24] By regulating the flowrate through the expansion machine 27, the high pressure in the system 21 can be controlled. Increasing the flowrate of refrigerant through the expansion machine 27 causes more mass to leave the high pressure part of the system 21, decreasing the instantaneous refrigerant mass in the high pressure part of the system 21 and the high pressure in the system 21. Decreasing the flowrate through the expansion machine 27 causes less mass to leave the high pressure part of the system 21, increasing the instantaneous refrigerant mass in the high pressure part of the system 21 and the high pressure in the system 21.

[27] The flowrate of refrigerant through the expansion machine 27 is a function of the speed of expansion machine 27, the pressure difference between the high pressure part and the low pressure parts of the system 21, and the displacement of the expansion machine 27 if the expansion machine 27 is a displacement type expansion machine 27, such as a piston, rotary, scroll, or screw type expansion machine. By regulation of any of the above functions, the high pressure part of the system 21 can be regulated. For example, increasing the speed of the expansion machine 27 allows more refrigerant flow to pass through the expansion machine 27, decreasing the instantaneous refrigerant mass in the high pressure part of the system 21 and the pressure in the high pressure part of the system 21. Decreasing the speed of the expansion machine 27 allows less refrigerant to pass through the expansion machine 27, increasing the refrigerant mass in the high pressure part of the system and increasing the pressure in the high pressure part of the system 21. An operating frequency of the expansion machine 27 can also control the expansion machine 27 flowrate.

[28] In another example, increasing the displacement of the expansion machine 27 allows more refrigerant flow to pass through the expansion machine 27, decreasing the instantaneous refrigerant mass in the high pressure part of the system 21 and decreasing the pressure in the high pressure part of the system 21. Decreasing the displacement of the expansion machine 27 allows less refrigerant to pass through the expansion machine 27, increasing the instantaneous refrigerant mass in the high pressure part of the system 21 and increasing the pressure in the high pressure part of the system 21.

[29] After expansion in the expansion machine 27, the refrigerant flow enters a separator tank 30 which separates the refrigerant into vapor and liquid. The vapor refrigerant enters a recompressor 32 that recompresses the vapor refrigerant. The recompressed vapor refrigerant is injected along a path 35 at any higher pressure component of the system 21. The recompressor 32 is directly linked to the expansion machine 27 by line 34. In one example, the recompressed flow is injected at the inlet of the gas cooler 24.

[30] The energy recovered by the expansion process is used to recompress the vapor phase of the expanded flow in the recompressor 32. The energy recovered by the expansion machine 27 can also be used to decrease the energy requirements of the system 21, increasing system 21 efficiency. The power requirements of the recompressor 32 are a function of the amount of the refrigerant flow through to the recompressor 32, the displacement of the recompressor 32, the pressure differential between the inlet and the outlet of the recompressor 32 and the efficiency of the recompressor 32.

[31] By controlling the amount of refrigerant flow provided to the recompressor 32, the massflow rate of refrigerant through the expansion machine 27 can be controlled.

The refrigerant flow through the recompressor 32 is a function of the refrigerant density at the inlet of the recompressor 32, the displacement of the recompressor 32, and the speed of the recompressor 32. By regulating of any these functions, the refrigerant flow through the recompressor 32, the load on the expansion machine 27, the speed of the expansion machine 27, and therefore the flowrate through the expansion machine 27 can be regulated.

[32] A first valve 36 having an orifice and positioned between the expanded flow and the inlet of the recompressor 32 is controlled to regulate the amount of flow provided to the recompressor 32. The first valve 36 is controlled by a control 38 and is actuated by increasing or decreasing the diameter of the orifice. The control 38 monitors the high pressure in the gas cooler 24 and adjusts the actuation of the first valve 36 to achieve the optimal pressure. The control 38 may be the main control for cycle 21. Once the desired pressure has been determined, the control 38 adjusts the first valve 36 to regulate the high pressure. The factors used to determine the optimum pressure are within the skill of a worker in the art. By regulating the high pressure in the gas cooler 24, the enthalpy of the refrigerant at the entry of the evaporator 28 can be modified, controlling the capacity and/or efficiency of the system 20.

[33] If the pressure in the gas cooler 24 is below the optimal pressure, the efficiency of the system 21 could be increased. The control 38 opens or increases the size of the orifice in the first valve 36, increasing the amount of flow provided to the recompressor 32 and the load on the expansion machine 27. The amount of refrigerant flow through the expansion machine 27 decreases, increasing the instantaneous mass in the supercritical part of the system 21 and the supercritical pressure.

[34] If the pressure in the gas cooler 24 is above the optimal pressure, an excessive amount of energy is used to compress the refrigerant. The control 38 closes or decreases the size of the orifice in the first valve 36, decreasing the amount of flow provided to the recompressor 32and the load on the expansion machine 27, The amount of flow through the expansion machine 27 increases, decreasing the instantaneous mass in the supercritical part of the system 21 and the supercritical pressure.

[35] The system 21 can also include a second valve 40 positioned between the expanded flow and the evaporator 28 and operate as an economized cycle. The second valve 40 controls the superheat at the suction of the compressor 22 and varies the mass flowrate through the evaporator 28. By closing the second valve 40, the vapor flow in the separator tank 30 bypasses the evaporator 28 through a vapor bypass line 42 to the suction of the compressor 22.

[36] As shown in Figure 3b, the amount of refrigerant flow through the recompressor 32 can be regulated by employing and regulating a motor 33 that provides power to the recompressor 32. The speed of the motor 33 is controlled by the control 38. The control 38 monitors the high pressure in the gas cooler 24 and adjusts the speed of the motor 33 to achieve the optimal pressure. If the motor 33 is employed to regulate the flowrate through the expansion machine 27, the first valve 36 is not necessary.

[37] If the control 38 detects that the pressure in the gas cooler 24 is below the optimal pressure, the control 38 decreases the speed of the motor 33, decreasing the speed and flowrate through the recompressor 32 and the expansion machine 27.

When the expansion machine 27 flowrate is decreased, the instantaneous mass in the supercritical part of the system 21 increases, increasing the supercritical pressure in the system 21. If the control detects that the pressure in the gas cooler 24 is above the optimal pressure the control 38 increases the speed of the motor 33, increasing the speed and flowrate through the recompressor 32 and the expansion machine 27.

When the expansion machine 27 flowrate is increased, the instantaneous mass in the supercritical part of the system 21 decreases, decreasing the supercritical pressure in the system 21.

[38] Figure 4a schematically illustrates a second example of the system 19. The system 19 includes a second compression device 39 in parallel to the main compression device 22. The refrigerant flow to the second compression device 39 is drawn along a path 37 from the suction of the compressor 22 before or after a suction accumulator 29. The flowrate of the expansion machine 27, and thus the pressure in the supercritical portion of the system 19, can be regulated by regulating the flow to the second compression device 39. The flow to the second compression device 39 is regulated by operating the regulating valve 36 which controls the speed of the expansion machine 27.

[39] Alternately, as shown in Figure 4b, the flow of the second compression device 39 is regulated by controlling the speed of motor 33, as described for system 21. If the system 19 includes a motor 33, the regulating valve 36 is not needed. The system , 19 can also include a storage tank or accumulator 29 which contains the excess charge in the system 19.

[40] A third example of the invention is schematically illustrated as the system 18 in Figure 5a. In this example, the flow drawn from the discharge of the expansion machine 27 exchanges heat with the flow provided to the expansion machine 27 in a heat exchanger 25, allowing the liquid in the flow to be vaporized while providing a cooling benefit to the flow leaving the gas cooler 24. This flow is then provided to the recompressor 32. The flowrate of the expansion machine 27, and therefore the pressure in the supercritical portion of the system 18, is regulated by regulating the flow to the recompressor 32. The flow to the recompressor 32 is regulated by operating a regulating valve 36, which can be located before or after the heat exchanger 25.

[41] Alternately, as shown in Figure 5b, the flow to the recompressor 32 is regulated by controlling the speed of a motor 33, as described for system 21. If the system 18 includes a motor 33, the regulating valve 36 is not needed. The system 18 can also include a storage tank or accumulator 29 which contains the excess charge in the system 18.

[42] Although a number of examples of the invention have been disclosed and illustrated, it is to be understood that the flowrate of the expansion machine 27 can be varied in other methods. One skilled in the art would know how to adjust the flowrate through the expansion machine 27.

[43] The foregoing description is only exemplary of the principles of the invention.

Many modifications and variations of the present invention are possible in light of the above teachings. The preferred embodiments of this invention have been disclosed, however, so that one of ordinary skill in the art would recognize that certain modifications would come within the scope of this invention. It is, therefore, to be understood that within the scope of the appended claims, the invention may be practiced otherwise than as specifically described. For that reason the following claims should be studied to determine the true scope and content of this invention.