Thermal management systems
11835270 · 2023-12-05
Assignee
Inventors
- Igor Vaisman (Carmel, IN, US)
- Joshua Peters (Knoxville, TN, US)
- Martin Seifert (West Simsbury, CT, US)
Cpc classification
F25B2400/0409
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B49/00
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B2700/197
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B41/31
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
F25B19/00
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B41/31
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Abstract
Thermal management systems include an open circuit refrigeration system featuring a receiver configurable to store a refrigerant fluid, an evaporator configurable to extract heat from a heat load when the heat load contacts the evaporator, and an exhaust line, where the receiver, the evaporator, and the exhaust line are connected to form a refrigerant fluid flow path, and a first control device configurable to control a vapor quality of the refrigerant fluid at an outlet of the evaporator along the refrigerant fluid flow path.
Claims
1. A thermal management system, comprising: an open circuit refrigeration system comprising: a receiver configured to store a refrigerant fluid comprising ammonia and including a liquid refrigerant fluid; an evaporator attached to a heat load and configured to extract heat from the heat load when the heat load contacts the evaporator having an inlet and an outlet; a vapor quality sensor that produces a sensor signal that is a measure of a vapor quality of the refrigerant fluid emerging from an outlet of the evaporator; a controller that receives the sensor signal from the vapor quality sensor and produces one or more electrical control signals; an expansion valve responsive to at least one of the one or more electrical control signals to control the vapor quality of the refrigerant fluid at the outlet of the evaporator with, with the vapor quality being a value of a ratio of mass of vapor to mass of liquid plus vapor, the vapor quality controlled, according to a set point temperature value, and with the expansion valve and the evaporator configured to maintain the vapor quality that emerges from the outlet of the evaporator, so as not to exceed a critical vapor quality defined as one (1), and with the vapor quality further being a value that is less than a value of vapor quality at which dryout occurs in the evaporator; an exhaust line configured to receive all of the refrigerant fluid emerging from the outlet of the evaporator, with the receiver, the evaporator, the outlet, the expansion valve, and the exhaust line coupled to form a refrigerant fluid flow path, and with all of the refrigerant fluid from the exhaust line discharged so that all of the refrigerant fluid emerging from the outlet of the evaporator is discharged and is not returned to the receiver; and a heat exchanger coupled to the refrigerant fluid flow path, the heat exchanger comprising: a first fluid path positioned so that liquid refrigerant fluid from the receiver flows through the first fluid path to the expansion valve; and a second fluid path positioned so that refrigerant vapor from the evaporator flows through the second fluid path to transfer heat from the refrigerant vapor in the second fluid path to the liquid refrigerant fluid in the first fluid path.
2. The system of claim 1, the system further comprising: a flow control device positioned downstream from the evaporator along the refrigerant fluid flow path.
3. The system of claim 2, wherein the flow control device is configured to control a temperature of the heat load.
4. The system of claim 2 wherein the flow control device comprises a back pressure regulator.
5. The system of claim 4, wherein the back pressure regulator is configured to receive refrigerant fluid vapor generated in the evaporator and to regulate refrigerant fluid pressure upstream from the back pressure regulator along the refrigerant fluid flow path.
6. The system of claim 5, wherein the back pressure regulator is further configured to perform an expansion of the refrigerant fluid vapor.
7. The system of claim 1, wherein the expansion valve is configured to: receive the liquid refrigerant fluid from the receiver at a first pressure; expand the liquid refrigerant fluid to generate a refrigerant fluid mixture at a second pressure, with the refrigerant fluid mixture comprising the liquid refrigerant fluid and a refrigerant fluid vapor; and direct the refrigerant fluid mixture into the evaporator.
8. The system of claim 1, wherein the expansion valve controls the vapor quality to be in a range of 0.5 to less than 1.0.
9. The system of claim 1 wherein the expansion valve comprises a first actuation assembly that is adjustable based on the one or more electrical control signals, the vapor quality sensor transmits on the one or more electrical control signals to the expansion valve based on a difference in capacitance between liquid and vapor phases of the refrigerant fluid.
10. A thermal management method, comprising: transporting a liquid refrigerant fluid comprising ammonia from a receiver in a first direction through a heat exchanger attached to a heat load, an expansion valve, an evaporator, and an outlet of the evaporator that is configured to extract heat from the heat load when the heat load contacts the evaporator, and transporting refrigerant vapor fluid from the evaporator through the heat exchanger in a second direction toward an exhaust line configured to receive all refrigerant fluid from the outlet of the evaporator, while transferring heat from the refrigerant vapor fluid transported along the second direction to the liquid refrigerant fluid transported along the first direction; producing by a vapor quality sensor, a sensor signal that is a measure of a vapor quality of the refrigerant fluid emerging from the outlet of the evaporator; controlling with the expansion valve the vapor quality, with the vapor quality being a value of a ratio of mass of vapor to mass of liquid plus vapor, with the vapor quality controlled, according to a set point temperature value, and with the expansion valve and the evaporator configured to maintain the vapor quality that emerges from the outlet of the evaporator, so as not to exceed critical vapor quality defined as one (1), and further being a value that is less than a value of vapor quality at which dryout occurs in the evaporator; receiving, by the exhaust line, all of the refrigerant fluid emerging from the outlet of the evaporator; and discharging all of the refrigerant vapor fluid from the exhaust line so that all of the refrigerant fluid emerging from the outlet of the evaporator is discharged and is not returned to the receiver.
11. The method of claim 10, further comprising: directing the liquid refrigerant fluid from the receiver at a first pressure into expansion valve; expanding the liquid refrigerant fluid in the expansion valve to generate a refrigerant fluid mixture at a second pressure, wherein the refrigerant fluid mixture comprises liquid refrigerant fluid and refrigerant fluid vapor; and directing the refrigerant fluid mixture out of the expansion valve and into the evaporator.
12. The method of claim 11, further comprising: separating the refrigerant fluid mixture generated in the expansion valve into the refrigerant fluid vapor and the liquid refrigerant fluid; directing at least a portion of the refrigerant fluid vapor along a flow path that bypasses the evaporator; and directing the liquid refrigerant fluid into the evaporator.
13. The method of claim 12, further comprising directing the at least a portion of the refrigerant fluid vapor into the heat exchanger and along the second direction through the heat exchanger.
14. The method of claim 10 further comprising: after transporting the liquid refrigerant fluid through the evaporator and prior to transporting the refrigerant vapor fluid toward the exhaust line, transporting the refrigerant vapor fluid through a flow control device; and controlling a temperature of the heat load by operation of the flow control device.
15. The method of claim 14, further comprising: adjusting the flow control device based on a first attribute corresponding to a property of the liquid refrigerant fluid; and adjusting the flow control device based on an attribute corresponding to a property of the heat load.
Description
DESCRIPTION OF DRAWINGS
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DETAILED DESCRIPTION
I. General Introduction
(15) Cooling of high heat flux loads that are also highly temperature sensitive can present a number of challenges. On one hand, such loads generate significant quantities of heat that is extracted during cooling. In conventional closed-cycle refrigeration systems, cooling high heat flux loads typically involves circulating refrigerant fluid at a relatively high mass flow rate. However, closed-cycle system components that are used for refrigerant fluid circulation—including compressors and condensers—are typically heavy and consume significant power. As a result, many closed-cycle systems are not well suited for deployment in mobile platforms—such as on small vehicles—where size and weight constraints may make the use of large compressors and condensers impractical.
(16) On the other hand, temperature sensitive loads such as electronic components and devices may require temperature regulation within a relatively narrow range of operating temperatures. Maintaining the temperature of such a load to within a small tolerance of a temperature set point can be challenging when a single-phase refrigerant fluid is used for heat extraction, since the refrigerant fluid itself will increase in temperature as heat is absorbed from the load.
(17) Directed energy systems that are mounted to mobile vehicles such as trucks may present many of the foregoing operating challenges, as such systems may include high heat flux, temperature sensitive components that require precise cooling during operation in a relatively short time. The thermal management systems disclosed herein, while generally applicable to the cooling of a wide variety of thermal loads, are particularly well suited for operation with such directed energy systems.
(18) In particular, the thermal management systems and methods disclosed herein include a number of features that reduce both overall size and weight relative to conventional refrigeration systems, and still extract excess heat energy from both high heat flux, highly temperature sensitive components and relatively temperature insensitive components, to accurately match temperature set points for the components. At the same time the disclosed thermal management systems require no significant power to sustain their operation. Whereas certain conventional refrigeration systems used closed-circuit refrigerant flow paths, the systems and methods disclosed herein use open-cycle refrigerant flow paths. Depending upon the nature of the refrigerant fluid, exhaust refrigerant fluid may be incinerated as fuel, chemically treated, and/or simply discharged at the end of the flow path.
II. Thermal Management Systems with Open Circuit Refrigeration Systems
(19)
(20) Receiver 102 is typically implemented as an insulated vessel that stores a refrigerant fluid at relatively high pressure.
(21) In general, receiver 102 can have a variety of different shapes. In some embodiments, for example, the receiver is cylindrical. Examples of other possible shapes include, but are not limited to, rectangular prismatic, cubic, and conical. In certain embodiments, receiver 102 can be oriented such that outlet port 204 is positioned at the bottom of the receiver. In this manner, the liquid portion of the refrigerant fluid within receiver 102 is discharged first through outlet port 204, prior to discharge of refrigerant vapor.
(22) Returning to
(23) Mechanical expansion valves (usually called thermostatic or thermal expansion valves) are typically flow control devices that enthalpically expand a refrigerant fluid from a first pressure to an evaporating pressure, controlling the superheat at the evaporator exit. Mechanical expansion valves generally include an orifice, a moving seat that changes the cross-sectional area of the orifice and the refrigerant fluid volume and mass flow rates, a diaphragm moving the seat, and a bulb at the evaporator exit. The bulb is charged with a fluid and it hermetically fluidly communicates with a chamber above the diaphragm. The bulb senses the refrigerant fluid temperature at the evaporator exit (or another location) and the pressure of the fluid inside the bulb, transfers the pressure in the bulb through the chamber to the diaphragm, and moves the diaphragm and the seat to close or to open the orifice.
(24) Typical electrical expansion valves include an orifice, a moving seat, a motor or actuator that changes the position of the seat with respect to the orifice, a controller, and pressure and temperature sensors at the evaporator exit. The controller calculates the superheat for the expanded refrigerant fluid based on pressure and temperature measurements at the evaporator exit. If the superheat is above a set-point value, the seat moves to increase the cross-sectional area and the refrigerant fluid volume and mass flow rates to match the superheat set-point value. If the superheat is below the set-point value the seat moves to decrease the cross-sectional area and the refrigerant fluid flow rates.
(25) Examples of suitable commercially available expansion valves that can function as first control device 104 include, but are not limited to, thermostatic expansion valves available from the Sporlan Division of Parker Hannifin Corporation (Washington, MO) and from Danfoss (Syddanmark, Denmark).
(26) Evaporator 106 can be implemented in a variety of ways. In general, evaporator 106 functions as a heat exchanger, providing thermal contact between the refrigerant fluid and heat load 110. Typically, evaporator 106 includes one or more flow channels extending internally between an inlet and an outlet of the evaporator, allowing refrigerant fluid to flow through the evaporator and absorb heat from heat load 110.
(27) A variety of different evaporators can be used in system 100. In general, any cold plate may function as the evaporator of the open circuit refrigeration systems disclosed herein. Evaporator 106 can accommodate any refrigerant fluid channels (including mini/micro-channel tubes), blocks of printed circuit heat exchanging structures, or more generally, any heat exchanging structures that are used to transport single-phase or two-phase fluids. The evaporator and/or components thereof, such as fluid transport channels, can be attached to the heat load mechanically, or can be welded, brazed, or bonded to the heat load in any manner.
(28) In some embodiments, evaporator 106 (or certain components thereof) can be fabricated as part of heat load 110 or otherwise integrated into heat load 110.
(29) Returning to
(30) In general, a wide range of different mechanical and electrical/electronic devices can be used as second control device 108. Typically, mechanical back pressure regulating devices have an orifice and a spring supporting the moving seat against the pressure of the refrigerant fluid stream. The moving seat adjusts the cross-sectional area of the orifice and the refrigerant fluid volume and mass flow rates.
(31) Typical electrical back pressure regulating devices include an orifice, a moving seat, a motor or actuator that changes the position of the seat in respect to the orifice, a controller, and a pressure sensor at the evaporator exit or at the valve inlet. If the refrigerant fluid pressure is above a set-point value, the seat moves to increase the cross-sectional area of the orifice and the refrigerant fluid volume and mass flow rates to re-establish the set-point pressure value. If the refrigerant fluid pressure is below the set-point value, the seat moves to decrease the cross-sectional area and the refrigerant fluid flow rates.
(32) In general, back pressure regulators are selected based on the refrigerant fluid volume flow rate, the pressure differential across the regulator, and the pressure and temperature at the regulator inlet. Examples of suitable commercially available back pressure regulators that can function as second control device 108 include, but are not limited to, valves available from the Sporlan Division of Parker Hannifin Corporation (Washington, MO) and from Danfoss (Syddanmark, Denmark).
(33) A variety of different refrigerant fluids can be used in system 100. For open circuit refrigeration systems in general, emissions regulations and operating environments may limit the types of refrigerant fluids that can be used. For example, in certain embodiments, the refrigerant fluid can be ammonia having very large latent heat; after passing through the cooling circuit, the ammonia refrigerant can be disposed of by incineration, by chemical treatment (i.e., neutralization), and/or by direct venting to the atmosphere.
(34) In certain embodiments, the refrigerant fluid can be an ammonia-based mixture that includes ammonia and one or more other substances. For example, mixtures can include one or more additives that facilitate ammonia absorption or ammonia burning.
(35) More generally, any fluid can be used as a refrigerant in the open circuit refrigeration systems disclosed herein, provided that the fluid is suitable for cooling heat load 110 (e.g., the fluid boils at an appropriate temperature) and, in embodiments where the refrigerant fluid is exhausted directly to the environment, regulations and other safety and operating considerations do not inhibit such discharge.
(36) During operation of system 100, cooling can be initiated by a variety of different mechanisms. In some embodiments, for example, system 100 includes a temperature sensor attached to load 110 (as will be discussed subsequently). When the temperature of load 110 exceeds a certain temperature set point (i.e., threshold value), a controller connected to the temperature sensor can initiate cooling of load 110.
(37) Alternatively, in certain embodiments, system 100 operates essentially continuously—provided that the refrigerant fluid pressure within receiver 102 is sufficient—to cool load 110. As soon as receiver 102 is charged with refrigerant fluid, refrigerant fluid is ready to be directed into evaporator 106 to cool load 110. In general, cooling is initiated when a user of the system or the heat load issues a cooling demand.
(38) Upon initiation of a cooling operation, refrigerant fluid from receiver 102 is discharged from outlet 204, through optional valve 120 if present, and is transported through conduit 112 to first control device 104, which directly or indirectly controls vapor quality at the evaporator outlet. In the following discussion, first control device 104 is implemented as an expansion valve. However, it should be understood that more generally, first control device 104 can be implemented as any component or device that performs the functional steps described below and provides for vapor quality control at the evaporator outlet.
(39) Once inside the expansion valve, the refrigerant fluid undergoes constant enthalpy expansion from an initial pressure p.sub.r (i.e., the refrigerant fluid pressure) to an evaporation pressure p.sub.e at the outlet of the expansion valve. In general, the evaporation pressure p.sub.e depends on a variety of factors, most notably the desired temperature set point value (i.e., the target temperature) at which load 110 is to be maintained and the heat input generated by the load 110. The initial pressure in the receiver tends to be in equilibrium with the surrounding temperature and is different for different refrigerants. The pressure in the evaporator depends on the evaporating temperature, which is lower than the heat load temperature and is defined during design of the system. The system is operational as long as the receiver-to-evaporator pressure difference is sufficient to drive adequate refrigerant fluid flow through the expansion valve.
(40) After undergoing constant enthalpy expansion in the expansion valve, the liquid refrigerant fluid is converted to a mixture of liquid and vapor phases at the temperature of the fluid and evaporation pressure pc. The two-phase refrigerant fluid mixture is transported via conduit 114 to evaporator 106.
(41) When the two-phase mixture of refrigerant fluid is directed into evaporator 106, the liquid phase absorbs heat from load 110, driving a phase transition of the liquid refrigerant fluid into the vapor phase. Because this phase transition occurs at (nominally) constant temperature, the temperature of the refrigerant fluid mixture within evaporator 106 remains unchanged, provided at least some liquid refrigerant fluid remains in evaporator 106 to absorb heat.
(42) Further, the constant temperature of the refrigerant fluid mixture within evaporator 106 can be controlled by adjusting the pressure p.sub.e of the refrigerant fluid, since adjustment of p.sub.e changes the boiling temperature of the refrigerant fluid. Thus, by regulating the refrigerant fluid pressure p.sub.e upstream from evaporator 106 (e.g., using second control device 108), the temperature of the refrigerant fluid within evaporator 106 (and, nominally, the temperature of heat load 110) can be controlled to match a specific temperature set-point value for load 110, ensuring that load 110 is maintained at, or very near, a target temperature.
(43) The pressure drop across the evaporator causes drop of the temperature of the refrigerant mixture (which is the evaporating temperature), but still the evaporator can be configured to maintain the heat load temperature within in the set tolerances.
(44) In some embodiments, for example, the evaporation pressure of the refrigerant fluid can be adjusted by second control device 108 to ensure that the temperature of thermal load 110 is maintained to within ±5 degrees C. (e.g., to within ±4 degrees C., to within ±3 degrees C., to within ±2 degrees C., to within ±1 degree C.) of the temperature set point value for load 110.
(45) As discussed above, within evaporator 106, a portion of the liquid refrigerant in the two-phase refrigerant fluid mixture is converted to refrigerant vapor by undergoing a phase change. As a result, the refrigerant fluid mixture that emerges from evaporator 106 has a higher vapor quality (i.e., the fraction of the vapor phase that exists in refrigerant fluid mixture) than the refrigerant fluid mixture that enters evaporator 106.
(46) As the refrigerant fluid mixture emerges from evaporator 106, a portion of the refrigerant fluid can optionally be used to cool one or more additional thermal loads. Typically, for example, the refrigerant fluid that emerges from evaporator 106 is nearly in the vapor phase. The refrigerant fluid vapor (or, more precisely, high vapor quality fluid vapor) can be directed into a heat exchanger coupled to another thermal load, and can absorb heat from the additional thermal load during propagation through the heat exchanger. Examples of systems in which the refrigerant fluid emerging from evaporator 106 is used to cool additional thermal loads will be discussed in more detail subsequently.
(47) The refrigerant fluid emerging from evaporator 106 is transported through conduit 116 to second control device 108, which directly or indirectly controls the upstream pressure, that is, the evaporating pressure p.sub.e in the system. After passing through second control device 108, the refrigerant fluid is discharged as exhaust through conduit 118, which functions as an exhaust line for system 100. Refrigerant fluid discharge can occur directly into the environment surrounding system 100. Alternatively, in some embodiments, the refrigerant fluid can be further processed; various features and aspects of such processing are discussed in further detail below.
(48) It should be noted that the foregoing steps, while discussed sequentially for purposes of clarity, occur simultaneously and continuously during cooling operations. In other words, refrigerant fluid is continuously being discharged from receiver 102, undergoing continuous expansion in first control device 104, flowing continuously through evaporator 106 and second control device 108, and being discharged from system 100, while thermal load 110 is being cooled.
(49) During operation of system 100, as refrigerant fluid is drawn from receiver 102 and used to cool thermal load 110, the receiver pressure p.sub.r falls. If the refrigerant fluid pressure p.sub.r (i.e., the initial refrigerant pressure) in receiver 102 is reduced to a value that is too low, the pressure differential p.sub.r−p.sub.e may not be adequate to drive sufficient refrigerant fluid mass flow to provide adequate cooling of thermal load 110. Accordingly, when the refrigerant fluid pressure p.sub.r in receiver 102 is reduced to a value that is sufficiently low, the capacity of system 100 to maintain a particular temperature set point value for load 110 may be compromised. Therefore, the pressure in the receiver or pressure drop across the expansion valve (or any related refrigerant fluid pressure or pressure drop in system 100) can be an indicator of the remaining operational time. An appropriate warning signal can be issued (e.g., by a system controller) to indicate that in a certain period of time, the system may no longer be able to maintain adequate cooling performance; operation of the system can even be halted if the refrigerant fluid pressure in receiver 102 reaches the low-end threshold value.
(50) It should be noted that while in
III. System Operational Control
(51) As discussed in the previous section, by adjusting the pressure p.sub.e of the refrigerant fluid, the temperature at which the liquid refrigerant phase undergoes vaporization within evaporator 106 can be controlled. Thus, in general, the temperature of heat load 110 can be controlled by a device or component of system 100 that regulates the pressure of the refrigerant fluid within evaporator 106. Typically, second control device 108 (which can be implemented as a back pressure regulator) adjusts the upstream refrigerant fluid pressure in system 100. Accordingly, second control device 108 is generally configured to control the temperature of heat load 110, and can be adjusted to selectively change a temperature set point value (i.e., a target temperature) for heat load 110.
(52) Another important system operating parameter is the vapor quality of the refrigerant fluid emerging from evaporator 106. The vapor quality, which is a number from 0 to 1, represents the fraction of the refrigerant fluid that is in the vapor phase. Because heat absorbed from load 110 is used to drive a constant-temperature evaporation of liquid refrigerant to form refrigerant vapor in evaporator 106, it is generally important to ensure that, for a particular volume of refrigerant fluid propagating through evaporator 106, at least some of the refrigerant fluid remains in liquid form right up to the point at which the exit aperture of evaporator 106 is reached to allow continued heat absorption from load 110 without causing a temperature increase of the refrigerant fluid. If the fluid is fully converted to the vapor phase after propagating only partially through evaporator 106, further heat absorption by the (now vapor-phase) refrigerant fluid within evaporator 106 will lead to a temperature increase of the refrigerant fluid and heat load 110.
(53) On the other hand, liquid-phase refrigerant fluid that emerges from evaporator 106 represents unused heat-absorbing capacity, in that the liquid refrigerant fluid did not absorb sufficient heat from load 110 to undergo a phase change. To ensure that system 100 operates efficiently, the amount of unused heat-absorbing capacity should remain relatively small.
(54) The evaporator 106 may be configured to maintain exit vapor quality below the critical vapor quality defined as “1.” Vapor quality is the ratio of mass of vapor to mass of liquid+vapor and is generally kept in a range of approximately 0.5 to almost 1.0; more specifically 0.6 to 0.95; more specifically 0.75 to 0.9 more specifically 0.8 to 0.9 or more specifically about 0.8 to 0.85. “Vapor quality” thus when defined as mass of vapor/total mass (vapor+liquid), in this sense, the vapor quality cannot exceed “1” or be equal to a value less than “0.”
(55) In practice, vapor quality may be expressed as an “equilibrium thermodynamic quality” that is calculated as follows:
X=(h−h′)/(h″−h′), where h—is any one of specific enthalpy, specific entropy or specific volume, ′—means saturated liquid and ″—means saturated vapor. In this case X can be mathematically below 0 or above 1, unless the calculation process is forced to operate differently. Either approach is acceptable.
(56) In addition, the boiling heat transfer coefficient that characterizes the effectiveness of heat transfer from load 110 to the refrigerant fluid is typically very sensitive to vapor quality. When the vapor quality increases from zero to a certain value, called a critical vapor quality, the heat transfer coefficient increases. When the vapor quality exceeds the critical vapor quality, the heat transfer coefficient is abruptly reduced to a very low value, causing dryout within evaporator 106. In this region of operation, the two-phase mixture behaves as superheated vapor.
(57) In general, the critical vapor quality and heat transfer coefficient values vary widely for different refrigerant fluids, and heat and mass fluxes. For all such refrigerant fluids and operating conditions, the systems and methods disclosed herein control the vapor quality at the outlet of the evaporator such that the vapor quality approaches the threshold of the critical vapor quality.
(58) To make maximum use of the heat-absorbing capacity of the two-phase refrigerant fluid mixture, the vapor quality of the refrigerant fluid emerging from evaporator 106 should nominally be equal to the critical vapor quality. Accordingly, to both efficiently use the heat-absorbing capacity of the two-phase refrigerant fluid mixture and also ensure that the temperature of heat load 110 remains approximately constant at the phase transition temperature of the refrigerant fluid in evaporator 106, the systems and methods disclosed herein are generally configured to adjust the vapor quality of the refrigerant fluid emerging from evaporator 106 to a value that is less than or equal to the critical vapor quality.
(59) Another important operating consideration for system 100 is the mass flow rate of refrigerant fluid within the system. Evaporator 106 can be configured to provide minimal mass flow rate controlling maximal vapor quality, which is the critical vapor quality. By minimizing the mass flow rate of the refrigerant fluid according to the cooling requirements for heat load 110, system 100 operates efficiently. Each reduction in the mass flow rate of the refrigerant fluid (while maintaining the same temperature set point value for heat load 110) means that the charge of refrigerant fluid added to reservoir 102 initially lasts longer, providing further operating time for system 100.
(60) Within evaporator 106, the vapor quality of a given quantity of refrigerant fluid varies from the evaporator inlet (where vapor quality is lowest) to the evaporator outlet (where vapor quality is highest). Nonetheless, to realize the lowest possible mass flow rate of the refrigerant fluid within the system, the effective vapor quality of the refrigerant fluid within evaporator 106—even when accounting for variations that occur within evaporator 106—should match the critical vapor quality as closely as possible.
(61) In summary, to ensure that the system operates efficiently and the mass flow rate of the refrigerant fluid is relatively low, and at the same time the temperature of heat load 110 is maintained within a relatively small tolerance, system 100 adjusts the vapor quality of the refrigerant fluid emerging from evaporator 106 to a value such that an effective vapor quality within evaporator 106 matches, or nearly matches, the critical vapor quality.
(62) In system 100, first control device 104 is generally configured to control the vapor quality of the refrigerant fluid emerging from evaporator 106. As an example, when first control device 104 is implemented as an expansion valve, the expansion valve regulates the mass flow rate of the refrigerant fluid through the valve. In turn, for a given set of operating conditions (e.g., ambient temperature, initial pressure in the receiver, temperature set point value for heat load 110, heat load 110), the vapor quality determines mass flow rate of the refrigerant fluid emerging from evaporator 106.
(63) First control device 104 typically controls the vapor quality of the refrigerant fluid emerging from evaporator 106 in response to information about at least one thermodynamic quantity that is either directly or indirectly related to the vapor quality. Second control device 108 typically adjusts the temperature of heat load 110 (via upstream refrigerant fluid pressure adjustments) in response to information about at least one thermodynamic quantity that is directly or indirectly related to the temperature of heat load 110. The one or more thermodynamic quantities upon which adjustment of first control device 104 is based are different from the one or more thermodynamic quantities upon which adjustment of second control device 108 is based.
(64) In general, a wide variety of different measurement and control strategies can be implemented in system 100 to achieve the control objectives discussed above. Generally, first control device 104 is connected to a first measurement device and second control device 108 is connected to a second measurement device. The first and second measurement devices provide information about the thermodynamic quantities upon which adjustments of the first and second control devices are based. The first and second measurement devices can be implemented in many different ways, depending upon the nature of the first and second control devices.
(65) As an example,
(66) The member, coupled to the pressure-sensing bulb, also moves in response to changes in superheat of the refrigerant fluid. The other end of the mechanical member is typically connected to an actuation assembly in the mechanical expansion valve. The actuation assembly includes, for example, a movable diaphragm that adjusts the orifice diameter within the valve. As the pressure-sensing bulb deforms in response to changes in superheat of the refrigerant fluid downstream from the second heat load, the mechanical deformation is coupled through the member to the diaphragm, which moves in concert to adjust the orifice diameter. In this manner, fully automated, responsive control of the mechanical expansion valve is achieved based on changes in superheat of the refrigerant fluid.
(67) As shown in
(68) Mechanical back pressure regulators suitable for use in the systems disclosed herein can generally have a variety of different configurations. Certain back pressure regulators, for example, have a small diameter passageway or conduit in a housing or body of the regulator that admits a small quantity of refrigerant fluid vapor that exerts pressure on an internal mechanism (for example, a spring-coupled valve stem) to adjust the size of the orifice. Effectively, in the above example, the passageway or conduit functions as a measurement device for the mechanical back pressure regulator, and the spring-coupled valve stem functions as an actuation assembly.
(69) It should generally be understood that various control strategies, control devices, and measurement devices can be implemented in a variety of combinations in the systems disclosed herein. Thus, for example, either or both of the first and second control devices can be implemented as mechanical devices, as described above. In addition, systems with mixed control devices in which one of the first or second control devices is a mechanical device and the other control device is implemented as an electronically-adjustable device can also be implemented, along with systems in which both the first and second control devices are electronically-adjustable devices that are controlled in response to signals measured by one or more sensors.
(70) In some embodiments, the systems disclosed herein can include measurement devices featuring one or more system sensors and/or measurement devices that measure various system properties and operating parameters, and transmit electrical signals corresponding to the measured information.
(71) Shown in
(72) System 500 also includes optional pressure sensors 606 and 608 positioned at the inlet and outlet, respectively, of evaporator 106. Pressure sensor 606 measures and transmits information about the refrigerant fluid pressure upstream from evaporator 106, and pressure sensor 608 measures and transmits information about the refrigerant fluid pressure downstream from evaporator 106. This information is used (e.g., by a system controller) to calculate the refrigerant fluid pressure drop across evaporator 106.
(73) As above, in certain embodiments, pressure sensors 606 and 608 are replaced by a single pressure differential sensor, a first end of which is connected adjacent to the evaporator inlet and a second end of which is connected adjacent to the evaporator outlet. The pressure differential sensor measures and transmits information about the refrigerant fluid pressure drop across evaporator 106.
(74) To measure the evaporating pressure (p.sub.e), sensor 608 is optionally positioned between the inlet and outlet of evaporator 106, i.e., internal to evaporator 106. In such a configuration, sensor 608 can provide a direct a direct measurement of the evaporating pressure.
(75) To measure refrigerant fluid pressure at other locations within system 500, sensor 608 can also optionally be positioned at a location different from the one shown in
(76) System 500 includes an optional temperature sensor 614 which is positioned adjacent to an inlet or an outlet of evaporator 106, or between the inlet and the outlet. Sensor 614 measures temperature information for the refrigerant fluid within evaporator 106 (which represents the evaporating temperature) and transmits an electronic signal corresponding to the measured information. System 500 also includes an optional temperature sensor 616 attached to heat load 110, which measures temperature information for the load and transmits an electronic signal corresponding to the measured information.
(77) System 500 includes an optional temperature sensor 610 adjacent to the outlet of evaporator 106 that measures and transmits information about the temperature of the refrigerant fluid as it emerges from evaporator 106.
(78) In certain embodiments, the systems disclosed herein are configured to determine superheat information for the refrigerant fluid based on temperature and pressure information for the refrigerant fluid measured by any of the sensors disclosed herein. The superheat of the refrigerant vapor refers to the difference between the temperature of the refrigerant fluid vapor at a measurement point in the system and the saturated vapor temperature of the refrigerant fluid defined by the refrigerant pressure at the measurement point in the system.
(79) To determine the superheat associated with the refrigerant fluid, a system controller (as will be described in greater detail subsequently) receives information about the refrigerant fluid vapor pressure after emerging from a heat exchanger downstream from evaporator 106, and uses calibration information, a lookup table, a mathematical relationship, or other information to determine the saturated vapor temperature for the refrigerant fluid from the pressure information. The controller also receives information about the actual temperature of the refrigerant fluid, and then calculates the superheat associated with the refrigerant fluid as the difference between the actual temperature of the refrigerant fluid and the saturated vapor temperature for the refrigerant fluid.
(80) The foregoing temperature sensors can be implemented in a variety of ways in system 500. As one example, thermocouples and thermistors can function as temperature sensors in system 500. Examples of suitable commercially available temperature sensors for use in system 500 include, but are not limited to the 88000 series thermocouple surface probes (available from OMEGA Engineering Inc., Norwalk, CT).
(81) System 500 includes a vapor quality sensor 612 that measures vapor quality of the refrigerant fluid emerging from evaporator 106. Typically, sensor 612 is implemented as a capacitive sensor that measures a difference in capacitance between the liquid and vapor phases of the refrigerant fluid. The capacitance information is used to directly determine the vapor quality of the refrigerant fluid (e.g., by a system controller). Alternatively, sensor 612 can determine the vapor quality directly based on the differential capacitance measurements and transmit an electronic signal that includes information about the refrigerant fluid vapor quality. Examples of commercially available vapor quality sensors that is used in system 600 include, but are not limited to HBX sensors (available from HB Products, Hasselager, Denmark).
(82) It should be appreciated that in the foregoing discussion, any one or various combinations of two sensors discussed in connection with system 500 can correspond to the first measurement device connected to first control device 104, and any one or various combination of two sensors can correspond to a second measurement device connected to second control device 108. In general, as discussed previously, the first measurement device provides information corresponding to a first thermodynamic quantity to the first control device, and the second measurement device provides information corresponding to a second thermodynamic quantity to the second control device, where the first and second thermodynamic quantities are different, and therefore allow the first and second control device to independently control two different system properties (e.g., the vapor quality of the refrigerant fluid and the heat load temperature, respectively).
(83) In some embodiments, one or more of the sensors shown in system 500 are connected directly to first control device 104 and/or to second control device 108. The first and second control device is configured to adaptively respond directly to the transmitted signals from the sensors, thereby providing for automatic adjustment of the system's operating parameters. In certain embodiments, the first and/or second control device can include processing hardware and/or software components that receive transmitted signals from the sensors, optionally perform computational operations, and activate elements of the first and/or second control device to adjust the control device in response to the sensor signals.
(84) In some embodiments, the systems disclosed herein include a system controller that receives measurement signals from one or more system sensors and transmits control signals to the first and/or second measurement device to independently adjust the refrigerant fluid vapor quality and the heat load temperature.
(85) In addition, controller 122 is optionally connected to first control device 104 and second control device 108. In embodiments where either first control device 104 or second control device 108 (or both) is/are implemented as a device controllable via an electrical control signal, controller 122 is configured to transmit suitable control signals to the first and/or second control device to adjust the configuration of these components. In particular, controller 122 is optionally configured to adjust first control device 104 to control the vapor quality of the refrigerant fluid in system 600, and optionally configured to adjust second control device 108 to control the temperature of heat load 110.
(86) During operation of system 600, controller 122 typically receives measurement signals from one or more sensors. The measurements can be received periodically (e.g., at consistent, recurring intervals) or irregularly, depending upon the nature of the measurements and the manner in which the measurement information is used by controller 122. In some embodiments, certain measurements are performed by controller 122 after particular conditions—such as a measured parameter value exceeding or falling below an associated set point value—are reached.
(87) It should generally understood that the systems disclosed herein can include a variety of combinations of the various sensors described above, and controller 122 can receive measurement information periodically or aperiodically from any of the various sensors. Moreover, it should be understood any of the sensors described can operate autonomously, measuring information and transmitting the information to controller 122 (or directly to the first and/or second control device), or alternatively, any of the sensors described above can measure information when activated by controller 122 via a suitable control signal, and measure and transmit information to controller 122 in response to the activating control signal.
(88) By way of example, Table 1 summarizes various examples of combinations of types of information (e.g., system properties and thermodynamic quantities) that is measured by the sensors of system 600 and transmitted to controller 122, to allow controller 122 to generate and transmit suitable control signals to first control device 104 and/or second control device 108. The types of information shown in Table 1 can generally be measured using any suitable device (including combination of one or more of the sensors discussed herein) to provide measurement information to controller 122.
(89) TABLE-US-00001 TABLE 1 Measurement Information Used to Adjust First Control Device FCM Evap Press Press Rec Evap Evap HL Drop Drop Pres VQ SH VQ P/T Temp Measurement FCM x x Information Press Used to Drop Adjust Evap x x Second Press Control Drop Device Rec x x Press VQ x x SH x x Evap x x VQ Evap x x x x x x x P/T HL x x x x x x x Temp FCM Press Drop = refrigerant fluid pressure drop across first control device Evap Press Drop = refrigerant fluid pressure drop across evaporator Rec Press = refrigerant fluid pressure in receiver VQ = vapor quality of refrigerant fluid SH = superheat of refrigerant fluid Evap VQ = vapor quality of refrigerant fluid at evaporator outlet Evap P/T = evaporation pressure or temperature HL Temp = heat load temperature
(90) For example, in some embodiments, first control device 104 is adjusted (e.g., automatically or by controller 122) based on a measurement of the evaporation pressure (p.sub.e) of the refrigerant fluid and/or a measurement of the evaporation temperature of the refrigerant fluid. With first control device 104 adjusted in this manner, second control device 108 is adjusted (e.g., automatically or by controller 122) based on measurements of one or more of the following system parameter values: the pressure drop across first control device 104, the pressure drop across evaporator 106, the refrigerant fluid pressure in receiver 102, the vapor quality of the refrigerant fluid emerging from evaporator 106 (or at another location in the system), the superheat value of the refrigerant fluid, and the temperature of thermal load 110.
(91) In certain embodiments, first control device 104 is adjusted (e.g., automatically or by controller 122) based on a measurement of the temperature of thermal load 110. With first control device 104 adjusted in this manner, second control device 108 is adjusted (e.g., automatically or by controller 122) based on measurements of one or more of the following system parameter values: the pressure drop across first control device 104, the pressure drop across evaporator 106, the refrigerant fluid pressure in receiver 102, the vapor quality of the refrigerant fluid emerging from evaporator 106 (or at another location in the system), the superheat value of the refrigerant fluid, and the evaporation pressure (p.sub.e) and/or evaporation temperature of the refrigerant fluid.
(92) In some embodiments, system controller 122 adjusts second control device 108 based on a measurement of the evaporation pressure p.sub.e of the refrigerant fluid downstream from first control device 104 (e.g., measured by pressure sensors 604 or 606) and/or a measurement of the evaporation temperature of the refrigerant fluid (e.g., measured by temperature sensor 614). With second control device 108 adjusted based on this measurement, system controller 122 can adjust first control device 104 based on measurements of one or more of the following system parameter values: the pressure drop (p.sub.r−p.sub.e) across first control device 104, the pressure drop across evaporator 106, the refrigerant fluid pressure in receiver 102 (p.sub.r), the vapor quality of the refrigerant fluid emerging from evaporator 106 (or at another location in the system), the superheat value of the refrigerant fluid in the system, and the temperature of thermal load 110.
(93) In certain embodiments, controller 122 adjusts second control device 108 based on a measurement of the temperature of thermal load 110 (e.g., measured by sensor 124). Controller 122 can also adjust first control device 104 based on measurements of one or more of the following system parameter values: the pressure drop (p.sub.r−p.sub.e) across first control device 104, the pressure drop across evaporator 106, the refrigerant fluid pressure in receiver 102 (p.sub.r), the vapor quality of the refrigerant fluid emerging from evaporator 106 (or at another location in the system), the superheat value of the refrigerant fluid in the system, the evaporation pressure (p.sub.e) of the refrigerant fluid, and the evaporation temperature of the refrigerant fluid.
(94) To adjust either first control device 104 or second control device 108 based on a particular value of a measured system parameter value, controller 122 compares the measured value to a set point value (or threshold value) for the system parameter. Certain set point values represent a maximum allowable value of a system parameter, and if the measured value is equal to the set point value (or differs from the set point value by 10% or less (e.g., 5% or less, 3% or less, 1% or less) of the set point value), controller 122 adjusts first control device 104 and/or second control device 108 to adjust the operating state of the system, and reduce the system parameter value.
(95) Certain set point values represent a minimum allowable value of a system parameter, and if the measured value is equal to the set point value (or differs from the set point value by 10% or less (e.g., 5% or less, 3% or less, 1% or less) of the set point value), controller 122 adjusts first control device 104 and/or second control device 108 to adjust the operating state of the system, and increase the system parameter value.
(96) Some set point values represent “target” values of system parameters. For such system parameters, if the measured parameter value differs from the set point value by 1% or more (e.g., 3% or more, 5% or more, 10% or more, 20% or more), controller 122 adjusts first control device 104 and/or second control device 108 to adjust the operating state of the system, so that the system parameter value more closely matches the set point value.
(97) In the foregoing examples, measured parameter values are assessed in relative terms based on set point values (i.e., as a percentage of set point values). Alternatively, in some embodiments, measured parameter values can be assessed in absolute terms. For example, if a measured system parameter value differs from a set point value by more than a certain amount (e.g., by 1 degree C. or more, 2 degrees C. or more, 3 degrees C. or more, 4 degrees C. or more, 5 degrees C. or more), then controller 122 adjusts first control device 104 and/or second control device 108 to adjust the operating state of the system, so that the measured system parameter value more closely matches the set point value.
(98) In certain embodiments, refrigerant fluid emerging from evaporator 106 is used to cool one or more additional thermal loads.
(99) Heat exchanger 902 includes one or more flow channels through which high vapor quality refrigerant fluid flows after leaving evaporator 106. During operation, as the refrigerant fluid vapor passes through the flow channels, it absorbs heat energy from second thermal load 904, cooling second thermal load 904. Typically, second thermal load 904 is not as sensitive as thermal load 110 to fluctuations in temperature. Accordingly, while second thermal load 904 is generally not cooled as precisely relative to a particular temperature set point value as thermal load 110, the refrigerant fluid vapor provides cooling that adequately matches the temperature constraints for second thermal load 904.
(100) Although in
(101) Although evaporator 106 and heat exchanger 902 are implemented as separate components in
(102) In
(103) In certain embodiments, as shown in
(104) In some embodiments, controller 122 can adjust second control device 108 based on measurements of the superheat value of the refrigerant fluid vapor that are performed downstream from a second thermal load that is cooled by the superheated refrigerant fluid vapor.
(105) Although heat exchanger 902 and second heat load 904 are positioned upstream from second control device 108 in
(106) Further, in some embodiments, sensor 1002 is positioned downstream from second control device 108. As discussed above, measured superheat information is used to adjust first control device 104 (e.g., to indirectly control vapor quality at the outlet of evaporator 106).
(107) In certain embodiments, the thermal management systems disclosed herein can include a recuperative heat exchanger for transferring heat energy from the refrigerant fluid emerging from evaporator 106 to refrigerant fluid upstream from first control device 104.
(108) As the two refrigerant fluid streams flow in opposite directions within recuperative heat exchanger 1102, heat is transferred from the refrigerant fluid emerging from evaporator 106 to the refrigerant fluid entering first control device 104. Heat transfer between the refrigerant fluid streams can have a number of advantages. For example, recuperative heat transfer can increase the refrigeration effect in evaporator 106, thereby reducing the refrigerant mass transfer rate implemented to handle the heat load presented by thermal load 110. Further, by reducing the refrigerant mass transfer rate through evaporator 106, the amount of refrigerant used to provide cooling duty in a given period of time is reduced. As a result, for a given initial quantity of refrigerant fluid introduced into receiver 102, the operational time over which the system can operate before an additional refrigerant fluid charge is needed can be extended. Alternatively, for the system to effectively cool thermal load 110 for a given period of time, a smaller initial charge of refrigerant fluid into receiver 102 can be used.
(109) Because the liquid and vapor phases of the two-phase mixture of refrigerant fluid generated following expansion of the refrigerant fluid in first control device 104 is used for different cooling applications, in some embodiments, the system can include a phase separator to separate the liquid and vapor phases into separate refrigerant streams that follow different flow paths within the system.
(110) Because the liquid phase of the refrigerant fluid is more dense than the vapor phase, phase separator 1202 can separate the two refrigerant phases by gravitational action, drawing off the vapor phase near the top of the phase separator and the liquid phase near the bottom of the phase separator as shown in
(111) Separating the liquid and vapor phases into two different refrigerant fluid streams can have a number of advantages. For example, by directing a nearly vapor-free liquid refrigerant fluid into the inlet of evaporator 106, the fluid channels within the evaporator can have smaller cross-sectional areas than fluid channels that carry a mixture of liquid and vapor phases of the refrigerant fluid. By reducing the cross-sectional areas of the fluid channels, the overall system weight is reduced.
(112) Further, eliminating (or nearly eliminating) the refrigerant vapor from the refrigerant fluid stream entering evaporator 106 can help to reduce the cross-section of the evaporator and improve film boiling in the refrigerant channels. In film boiling, the liquid phase (in the form of a film) is physically separated from the walls of the refrigerant channels by a layer of refrigerant vapor, leading to poor thermal contact and heat transfer between the refrigerant liquid and the refrigerant channels. Reducing film boiling improves the efficiency of heat transfer and the cooling performance of evaporator 106.
(113) In addition, by eliminating (or nearly eliminating) the refrigerant vapor from the refrigerant fluid stream entering evaporator 106, distribution of the liquid refrigerant within the channels of evaporator 106 is made easier. In certain embodiments, vapor present in the refrigerant channels of evaporator 106 can oppose the flow of liquid refrigerant into the channels. Diverting the vapor phase of the refrigerant fluid before the fluid enters evaporator 106 can help to reduce this difficulty.
(114) In addition to phase separator 1202, or as an alternative to phase separator 1202, in some embodiments the systems disclosed herein can include a phase separator downstream from evaporator 106. Such a configuration is used when the refrigerant fluid emerging from evaporator is not entirely in the vapor phase, and still includes liquid refrigerant fluid.
(115)
IV. Additional Features of Thermal Management Systems
(116) The foregoing examples of thermal management systems illustrate a number of features that is included in any of the systems within the scope of this disclosure. In addition, a variety of other features is present in such systems.
(117) In certain embodiments, refrigerant fluid that is discharged from evaporator 106 and passes through conduit 116 and second control device 108 is directly discharged as exhaust from conduit 118 without further treatment. Direct discharge provides a convenient and straightforward method for handling spent refrigerant, and has the added advantage that over time, the overall weight of the system is reduced due to the loss of refrigerant fluid. For systems that are mounted to small vehicles or are otherwise mobile, this reduction in weight is important.
(118) In some embodiments, however, refrigerant fluid vapor is further processed before it is discharged. Further processing may be desirable depending upon the nature of the refrigerant fluid that is used, as direct discharge of unprocessed refrigerant fluid vapor may be hazardous to humans and/or may deleterious to mechanical and/or electronic devices in the vicinity of the system. For example, the unprocessed refrigerant fluid vapor may be flammable or toxic, or may corrode metallic device components. In situations such as these, additional processing of the refrigerant fluid vapor may be desirable.
(119)
(120) As another example, where the refrigerant fluid vapor is highly chemically reactive, the refrigerant fluid vapor is exposed to one or more chemical agents that oxidize, reduce, or otherwise react with the refrigerant fluid vapor to yield a less reactive product that is collected for disposal or discharged from apparatus 802.
(121) In certain embodiments, refrigerant processing apparatus 802 is implemented as an adsorptive sink for the refrigerant fluid. Apparatus 802 can include, for example, an adsorbent material bed that binds particles of the refrigerant fluid vapor, trapping the refrigerant fluid within apparatus 802 and preventing discharge. The adsorptive process can sequester the refrigerant fluid particles within the adsorbent material bed, which can then be removed from apparatus 802 and sent for disposal.
(122) In some embodiments, where the refrigerant fluid is flammable, refrigerant processing apparatus 802 is implemented as an incinerator. Incoming refrigerant fluid vapor is mixed with oxygen or another oxidizing agent and ignited to combust the refrigerant fluid. The combustion products is discharged from the incinerator or collected (e.g., via an adsorbent material bed) for later disposal.
(123) As an alternative, refrigerant processing apparatus 802 can also be implemented as a combustor of an engine or another mechanical power-generating device. Refrigerant fluid vapor from conduit 118 is mixed with oxygen, for example, and combusted in a piston-based engine or turbine to perform mechanical work, such as providing drive power for a vehicle or driving a generator to produce electricity. In certain embodiments, the generated electricity is used to provide electrical operating power for one or more devices, including thermal load 110. For example, thermal load 110 can include one or more electronic devices that are powered, at least in part, by electrical energy generated from combustion of refrigerant fluid vapor in refrigerant processing apparatus 802.
(124) As shown in
(125) Particularly during start-up of the systems disclosed herein, liquid refrigerant may be present in conduits 116 and/or 118, because the systems generally begin operation before heat load 110 and/or heat load 904 are activated. Accordingly, phase separator 804 functions in a manner similar to phase separators 1202 and 1302 described above, to separate liquid refrigerant fluid from refrigerant vapor. The separated liquid refrigerant fluid is re-directed to another portion of the system, or retained within phase separator 804 until it is converted to refrigerant vapor. By using phase separator 804, liquid refrigerant fluid is prevented from entering refrigerant processing apparatus 802.
V. Integration with Power Systems
(126) In some embodiments, the refrigeration systems disclosed herein can combined with power systems to form integrated power and thermal systems, in which certain components of the integrated systems are responsible for providing refrigeration functions and certain components of the integrated systems are responsible for generating operating power.
(127) The energy released from combustion of the refrigerant fluid can be used by engine 1402 to generate electrical power, e.g., by using the energy to drive a generator. The electrical power is delivered via electrical connection 1404 to thermal load 110 to provide operating power for the load. For example, in certain embodiments, thermal load 110 includes one or more electrical circuits and/or electronic devices, and engine 1402 provides operating power to the circuits/devices via combustion of refrigerant fluid. Byproducts of the combustion process is discharged from engine 1402 via exhaust conduit 1406, as shown in
(128) Various types of engines and power-generating devices are implemented as engine 1402 in system 1400. In some embodiments, for example, engine 1402 is a conventional four cycle piston-based engine, and the waste refrigerant fluid is introduced into a combustor of the engine. In certain embodiments, engine 1402 is a gas turbine engine, and the waste refrigerant fluid is introduced via the engine inlet to the afterburner of the gas turbine engine.
(129) As discussed above in connection with
VI. Start-Up and Temporary Operation
(130) In certain embodiments, the thermal management systems disclosed herein operate differently at, and immediately following, system start-up, compared to the manner in which the systems operate after an extended running period. Upon start-up, refrigerant fluid in receiver 102 may be relatively cold, and therefore the receiver pressure (p.sub.r) may be lower than a typical receiver pressure during extended operation of the system. However, if receiver pressure p.sub.r is too low, the system may be unable to maintain a sufficient mass flow rate of refrigerant fluid through evaporator 106 to adequately cool thermal load 110.
(131) As discussed in connection with
(132) During operation, controller 122 can activate heater 208 to maintain the temperature of the refrigerant fluid in receiver 102. By maintaining the refrigerant fluid temperature, the vapor pressure of the refrigerant fluid, and also the pressure p.sub.r, are maintained such that the refrigerant fluid is delivered to evaporator 106.
(133) Optionally, during cold start-up, system controller 122 activates heater 208 to evaporate portion of the refrigerant fluid in receiver 102 and raise the vapor pressure and refrigerant fluid pressure p.sub.r in receiver. This allows the system to deliver refrigerant fluid into evaporator 106 at a sufficient mass flow rate. As the refrigerant fluid in receiver 102 warms up heater 208 is deactivated by system controller 122. By heating refrigerant fluid within receiver 102 at start-up, the thermal management system can begin to cool thermal load 110 after a relatively short warm-up period. To heat refrigerant fluid in receiver 102, for example, heater 208 can deliver heat that is received from a waste heat source in the system (e.g., heat recirculated from another component in the system) ensuring that relatively little or no power is consumed to generate the heat. In cold weather, the refrigerant fluid can also be pre-heated prior to being introduced into receiver 102.
(134) System controller 122 can also activate heater 208 to re-heat refrigerant fluid in receiver 102 between cooling cycles. Thus, for example, when the thermal management system runs periodically to provide intermittent cooling of thermal load 110, controller 122 can activate heater 208 when the thermal management system is not running to ensure that when thermal management system operation resumes, the receiver pressure p.sub.r in receiver 102 is sufficient to deliver refrigerant fluid to evaporator 106 at the desired mass flow rate almost immediately. During the system operation the heater typically provides heat input at a reduced rate to maintain an acceptable refrigerant fluid pressure in receiver 102. Insulation around receiver 102 can help to reduce heating demands.
VII. Integration with Directed Energy Systems
(135) The thermal management systems and methods disclosed herein can be implemented as part of (or in conjunction with) directed energy systems such as high energy laser systems. Due to their nature, directed energy systems typically present a number of cooling challenges, including certain heat loads for which temperatures are maintained during operation within a relatively narrow range.
(136)
(137) To regulate the temperatures of various components of directed energy systems such as laser diodes 1502 and amplifier 1504, such systems can include components and features of the thermal management systems disclosed herein. In
(138) High energy laser system 1500 is one example of a directed energy system that can include various features and components of the thermal management systems and methods described herein. However, it should be appreciated that the thermal management systems and methods are general in nature, and is applied to cool a variety of different heat loads under a wide range of operating conditions.
VIII. Hardware and Software Implementations
(139) Controller 122 can generally be implemented as any one of a variety of different electrical or electronic computing or processing devices, and can perform any combination of the various steps discussed above to control various components of the disclosed thermal management systems.
(140) System controller 122 can generally, and optionally, include any one or more of a processor (or multiple processors), a memory, a storage device, and input/output device. Some or all of these components are interconnected using a system bus. The processor is capable of processing instructions for execution. In some embodiments, the processor is a single-threaded processor. In certain embodiments, the processor is a multi-threaded processor. Typically, the processor is capable of processing instructions stored in the memory or on the storage device to display graphical information for a user interface on the input/output device, and to execute the various monitoring and control functions discussed above. Suitable processors for the systems disclosed herein include both general and special purpose microprocessors, and a sole processor or one of multiple processors for any kind of computer or computing device.
(141) The memory stores information within the system, and is a computer-readable medium, such as a volatile or non-volatile memory. The storage device is capable of providing mass storage for the controller 122. In general, the storage device can include any non-transitory tangible media configured to store computer readable instructions. For example, the storage device can include a computer-readable medium and associated components, including: magnetic disks, such as internal hard disks and removable disks; magneto-optical disks; and optical disks. Storage devices suitable for tangibly embodying computer program instructions and data include all forms of non-volatile memory, including by way of example semiconductor memory devices, such as EPROM, EEPROM, and flash memory devices; magnetic disks such as internal hard disks and removable disks; magneto-optical disks; and CD-ROM and DVD-ROM disks. Processors and memory units of the systems disclosed herein is supplemented by, or incorporated in, ASICs (application-specific integrated circuits).
(142) The input/output device provides input/output operations for controller 122, and can include a keyboard and/or pointing device. In some embodiments, the input/output device includes a display unit for displaying graphical user interfaces and system related information.
(143) The features described herein, including components for performing various measurement, monitoring, control, and communication functions, are implemented in digital electronic circuitry, or in computer hardware, firmware, or in combinations of them. Methods steps is implemented in a computer program product tangibly embodied in an information carrier, e.g., in a machine-readable storage device, for execution by a programmable processor (e.g., of system controller 122), and features are performed by a programmable processor executing such a program of instructions to perform any of the steps and functions described above. Computer programs suitable for execution by one or more system processors include a set of instructions that are used, directly or indirectly, to cause a processor or other computing device executing the instructions to perform certain activities, including the various steps discussed above.
(144) Computer programs suitable for use with the systems and methods disclosed herein is written in any form of programming language, including compiled or interpreted languages, and is deployed in any form, including as stand-alone programs or as modules, components, subroutines, or other units suitable for use in a computing environment.
(145) In addition to one or more processors and/or computing components implemented as part of controller 122, the systems disclosed herein can include additional processors and/or computing components within any of the control device (e.g., first control device 104 and/or second control device 108) and any of the sensors discussed above. Processors and/or computing components of the control device and sensors, and software programs and instructions that are executed by such processors and/or computing components, can generally have any of the features discussed above in connection with controller 122.
OTHER EMBODIMENTS
(146) A number of embodiments have been described. Nevertheless, it will be understood that various modifications may be made without departing from the spirit and scope of the disclosure. Accordingly, other embodiments are within the scope of the following claims.