This description relates to a system for heat transfer.
Heat transport systems are used to transport heat from one location (the heat source) to another location (the heat sink). Heat transport systems can be used in terrestrial or extraterrestrial applications. For example, heat transport systems may be integrated by satellite equipment that operates within zero- or low-gravity environments. As another example, heat transport systems can be used in electronic equipment, which often requires cooling during operation.
Loop Heat Pipes (LHPs) and Capillary Pumped Loops (CPLs) are passive two-phase heat transport systems. Each includes an evaporator thermally coupled to the heat source, a condenser thermally coupled to the heat sink, fluid that flows between the evaporator and the condenser, and a fluid reservoir for expansion of the fluid. The fluid within the heat transport system can be referred to as the working fluid. The evaporator includes a primary wick and a core that includes a fluid flow passage. Heat acquired by the evaporator is transported to and discharged by the condenser. These systems utilize capillary pressure developed in a fine-pored wick within the evaporator to promote circulation of working fluid from the evaporator to the condenser and back to the evaporator. The primary distinguishing characteristic between a LHP and a CPL is the location of the loop's reservoir, which is used to store excess fluid displaced from the loop during operation. In general, the reservoir of a CPL is located remotely from the evaporator, while the reservoir of a LHP is co-located with the evaporator.
According to one general aspect, a system includes a primary evaporator operable to facilitate heat transfer by evaporating received liquid to obtain vapor, the primary evaporator including a first port for receiving the liquid from a liquid line, a second port for outputting the vapor to a vapor line, and a third port for outputting excess liquid received from the liquid line to an excess fluid line. A condensing system is operable to receive the vapor from the vapor line, to condense at least some of the vapor, and to output the liquid to the liquid line. A reservoir is in fluid communication with the condensing system, and the liquid is obtained at least partially from the reservoir. In the system, a primary loop includes the condensing system, the primary evaporator, the liquid line, and the vapor line, the primary loop being operable to provide a heat transfer path, and a secondary loop includes the condensing system, the primary evaporator, the liquid line, the vapor line, and the excess fluid line. The secondary loop is operable to provide a venting path for removing other vapor that is present within the liquid from the primary evaporator.
Implementations may include one or more of the following features. For example, the liquid in the primary evaporator and received from the liquid line may include the excess liquid in excess of a liquid amount necessary to maintain saturation of a primary wick within a core of the primary evaporator. In this case, the primary evaporator may include a secondary wick that is operable to perform phase separation of the other vapor from the liquid for output through the excess fluid line. Further, the primary wick and the secondary wick of the primary evaporator may maintain capillary pumping of the liquid, the excess liquid, and the vapor, so as to maintain flow control to and through the primary evaporator.
A mechanical pump may be included that is operable to facilitate the heat transfer by actively pumping the liquid for evaporation by the primary evaporator, and for output as the excess liquid flows through the third port to the excess fluid line. In this case, the reservoir may be positioned between an output of the condensing system and an input of the mechanical pump, or the mechanical pump may be positioned between an input of the condensing system and an output of the primary evaporator.
A bypass valve may be included in parallel with the mechanical pump, and may be operable to bypass the mechanical pump during a passive pumping operation of the liquid for evaporation by the primary evaporator. The mechanical pump may include a liquid pump that is oriented in series with the liquid line and positioned between the condensing system and the primary evaporator, or a vapor compressor that is oriented in series with the vapor line and positioned between the primary evaporator and the condensing system.
A sensor may be included that is operable to communicate a saturation level of a wick of the primary evaporator to the mechanical pump, wherein a pumping pressure delivered by the mechanical pump is adjusted, based on the saturation level, so as to maintain saturation of the wick with the liquid. A liquid bypass valve may be connected between the liquid line and the vapor line and may be operable to maintain constant pump speed operations of the mechanical pump. The primary evaporator may include a primary wick and a secondary wick, compositions of which may comprise metal.
A priming system may be included within the secondary loop, and the priming system may include a secondary evaporator coupled to the vapor line, and a secondary reservoir may be in fluid communication with the secondary evaporator and coupled to the primary evaporator by the excess fluid line, wherein the priming system may be operable to provide the liquid to the primary evaporator at least partially from the secondary reservoir. The condensing system may include a first condenser within the primary loop and coupled to the liquid line and to the vapor line, and a second condenser within the secondary loop and coupled to the excess fluid line and to the secondary reservoir.
The third port of the primary evaporator may be primarily used to output the excess liquid to the excess fluid line, and the third port may include a subport for outputting the other vapor to a vapor line, such that the vapor line is included within the secondary loop.
The liquid line may be coaxial to and contained within the excess fluid line. A second primary evaporator may be connected in parallel with the primary evaporator within the primary loop. A back pressure regulator may be oriented in series with the vapor line and positioned between the primary evaporator and the condensing system, and may be operable to substantially equalize heat load between the primary evaporator and the secondary primary evaporator. In this case, the back pressure regulator may restrict vapor from reaching the condensing system until a vapor space of the primary evaporator and of the second primary evaporator is substantially devoid of liquid.
A second primary evaporator may be oriented in series with the primary evaporator within the primary loop. The condensing system may include a plurality of condensers connected in parallel to one another. In this case, liquid outputs may be associated with each of the plurality of condensers and may be operable to output the liquid to the primary evaporator, and condenser regulators may be coupled to the liquid outputs and operable to regulate liquid flow therefrom.
A second primary evaporator may be connected with the primary evaporator within the primary loop, and a thermal storage unit may be coupled to the second primary evaporator. A second primary evaporator may be connected with the primary evaporator within the primary loop, and first and second flow controllers may be connected to the primary evaporator and the second primary evaporator, respectively, and may be operable to regulate liquid flow to the primary evaporator and the second primary evaporator, respectively, so as to ensure a substantially equal heat load distribution between the evaporators.
A second primary evaporator may be connected with the primary evaporator within the primary loop, and a condensing heat exchanger may be coupled to the second primary evaporator. A spray-cooled evaporator may be coupled to the condensing heat exchanger by way of a mechanical pump. The condensing system may include a body-mounted radiator, or may include a deployable or steerable radiator.
According to another general aspect, liquid is evaporated from a primary wick of a primary evaporator to thereby obtain vapor, the vapor is output through a vapor line coupled to the primary evaporator, and the vapor from the vapor line is condensed within a condensing system. The liquid is returned to the primary evaporator through a liquid line coupled to the primary evaporator, where a saturation amount of the liquid is provided so as to maintain a saturation of the primary wick during the evaporating. Excess liquid beyond the saturation amount is provided to the primary evaporator at least partially from a reservoir, through the liquid line, and the excess liquid and other vapor within the primary evaporator is swept to the condensing system.
Implementations may include one or more of the following features. For example, in evaporating liquid from the primary wick of the primary evaporator capillary pumping of the liquid, the excess liquid, and the vapor may be maintained, so as to maintain flow control to and through the primary evaporator.
Also, in outputting the vapor, the vapor may be output through a first port of the primary evaporator. In returning the liquid and providing excess liquid, the liquid and excess liquid may be returned through a second port of the primary evaporator. In sweeping the excess liquid and undesired vapor, the excess liquid and undesired vapor may be swept from a third port of the primary evaporator.
Outputting the vapor may include outputting the vapor through a first port of the primary evaporator. Returning the liquid and providing excess liquid may include returning the liquid and excess liquid through a second port of the primary evaporator, and sweeping the excess liquid and other vapor may include sweeping the excess liquid from a third port of the primary evaporator, and sweeping the other vapor from a fourth port of the primary evaporator.
Sweeping the excess liquid and other vapor may include separating the liquid and excess liquid from the other vapor with a secondary wick of the primary evaporator. Providing the excess liquid may include pumping the excess liquid from the reservoir using a mechanical pump. In this case, the mechanical pump may be bypassed using a bypass valve in parallel with the mechanical pump, during a passive pumping operation of the liquid for evaporation by the primary evaporator.
Pumping the excess liquid may include pumping the liquid and the excess liquid using a liquid pump that is oriented in series with the liquid line and positioned between the condensing system and the primary evaporator, or may include pumping the vapor to the condensing system using a vapor compressor that is oriented in series with the vapor line and positioned between the primary evaporator and the condensing system.
Providing excess liquid may include providing the excess liquid from a priming system in which the reservoir is in fluid communication with a secondary evaporator, where the reservoir may be coupled to the primary evaporator. In this case, condensing the vapor may include condensing the vapor within a first condenser of the condensing system, the first condenser being coupled to the liquid line and to the vapor line, and sweeping the excess liquid and undesired vapor may include condensing undesired vapor within a second condenser of the condensing system, where the second condenser may be coupled to a mixed fluid line and to the reservoir.
According to another general aspect, a system includes a heat transfer system including a main evaporator having a core, a primary wick, a secondary wick, a first port, a second port, and a third port, as well as a condenser coupled to the main evaporator by a liquid line and a vapor line. A heat transfer system loop is defined by the condenser, the liquid line, the vapor line, the first port, and the second port. A venting system is configured to remove vapor bubbles from the core of the main evaporator. The venting system includes a pumping system operable to provide excess liquid to the main evaporator beyond a saturation amount of liquid needed for saturating the primary wick, and a reservoir in fluid communication with the pumping system and providing the excess liquid. The vapor bubbles are vented from the core of the main evaporator through the third port, and a venting loop is defined by the condenser, the liquid line, the vapor line, the first port of the main evaporator, and the third port of the main evaporator.
Implementations may include one or more of the following features. For example, the pumping system may include a mechanical pump.
The primary wick and the secondary wick of the main evaporator may maintain capillary pumping of the liquid, the excess liquid, and the vapor, so as to maintain flow control to and through the primary evaporator. In this case, the pumping system may include a secondary evaporator in fluid communication with the reservoir and coupled to the vapor line. Further, the reservoir may be in fluid communication with the secondary wick of the main evaporator through a mixed fluid line coupled to the third port of the main evaporator. The excess liquid may be substantially removed from the core of the main evaporator through a fourth port of the main evaporator.
Other features will be apparent from the description, the drawings, and the claims.
Like reference symbols in the various drawings generally indicate like elements.
As discussed above, in a loop heat pipe (LHP), the reservoir is co-located with the evaporator, the reservoir is thermally and hydraulically connected with the evaporator through a heat-pipe-like conduit. In this way, liquid from the reservoir can be pumped to the evaporator, thus ensuring that the primary wick of the evaporator is sufficiently wetted or “primed” during start-up. Additionally, the design of the LHP reduces depletion of liquid from the primary wick of the evaporator during steady-state or transient operation of the evaporator within a heat transport system. Moreover, vapor and/or bubbles of non-condensable gas (NCG bubbles) vent from a core of the evaporator through the heat-pipe-like conduit into the reservoir.
Conventional LHPs require liquid to be present in the reservoir prior to start-up, that is, application of power to the evaporator of the LHP. However, liquid will not be present in the reservoir prior to start-up if, prior to start-up of the LHP, the working fluid in the LHP is in a supercritical state in which a temperature of the LHP is above the critical temperature of the working fluid. The critical temperature of a fluid is the highest temperature at which the fluid can exhibit a liquid-vapor equilibrium. For example, the LHP may be in a supercritical state if the working fluid is a cryogenic fluid, that is, a fluid having a boiling point below 150° C., or if the working fluid is a sub-ambient fluid, that is, a fluid having a boiling point below the temperature of the environment in which the LHP is operating.
Conventional LHPs also require liquid returning to the evaporator to be subcooled, that is, cooled to a temperature that is lower than the boiling point of the working fluid. Such a constraint makes it impractical to operate LHPs at a sub-ambient temperature. For example, if the working fluid is a cryogenic fluid, the LHP is likely operating in an environment having a temperature greater than the boiling point of the fluid.
Referring to
The heat transfer system 105 includes a main evaporator 115, and a condenser 120 coupled to the main evaporator 115 by a liquid line 125 and a vapor line 130. The condenser 120 is in thermal communication with a heat sink 165, and the main evaporator 115 is in thermal communication with a heat source Qin 116. The heat transfer system 105 also may include a hot reservoir 147 coupled to the vapor line 130 for additional pressure containment, as needed. In particular, the hot reservoir 147 increases the volume of the heat transport system 100. If the working fluid is at a temperature above its critical temperature, that is, the highest temperature at which the working fluid can exhibit liquid-vapor equilibrium, its pressure is proportional to the mass in the heat transport system 100 (the charge) and inversely proportional to the volume of the system. Increasing the volume with the hot reservoir 147 lowers the fill pressure.
The main evaporator 115 includes a container 117 that houses a primary wick 140 within which a core 135 is defined. The main evaporator 115 includes a bayonet tube 142 and a secondary wick 145 within the core 135. The bayonet tube 142, the primary wick 140, and the secondary wick 145 define a liquid passage 143, a first vapor passage 144, and a second vapor passage 146. The secondary wick 145 provides phase control, that is, liquid/vapor separation in the core 135, as discussed in U.S. application Ser. No. 09/896,561, filed Jun. 29, 2001, which is incorporated herein by reference in its entirety. As shown, the main evaporator 115 has three ports, a liquid inlet 137 into the liquid passage 143, a vapor outlet 132 into the vapor line 130 from the second vapor passage 146, and a fluid outlet 139 from the liquid passage 143 (and possibly the first vapor passage 144, as discussed below). Further details on the structure of a three-port evaporator are discussed below with respect to
The priming system 110 includes a secondary or priming evaporator 150 coupled to the vapor line 130 and a reservoir 155 co-located with the secondary evaporator 150. The reservoir 155 is coupled to the core 135 of the main evaporator 115 by a secondary fluid line 160 and a secondary condenser 122. The secondary fluid line 160 couples to the fluid outlet 139 of the main evaporator 115. The priming system 110 also includes a controlled heat source Qsp 151 in thermal communication with the secondary evaporator 150.
The secondary evaporator 150 includes a container 152 that houses a primary wick 190 within which a core 185 is defined. The secondary evaporator 150 includes a bayonet tube 153 and a secondary wick 180 that extend from the core 185, through a conduit 175, and into the reservoir 155. The secondary wick 180 provides a capillary link between the reservoir 155 and the secondary evaporator 150. The bayonet tube 153, the primary wick 190, and the secondary wick 180 define a liquid passage 182 coupled to the secondary fluid line 160, a first vapor passage 181 coupled to the reservoir 155, and a second vapor passage 183 coupled to the vapor line 130. The reservoir 155 is thermally and hydraulically coupled to the core 185 of the secondary evaporator 150 through the liquid passage 182, the secondary wick 180, and the first vapor passage 181. Vapor and/or NCG bubbles from the core 185 of the secondary evaporator 150 are swept through the first vapor passage 181 to the reservoir 155 and condensable liquid is returned to the secondary evaporator 150 through the secondary wick 180 from the reservoir 155. The primary wick 190 hydraulically links liquid within the core 185 of the secondary evaporator 150 to the controlled heat source Qsp 151, permitting liquid at an outer surface of the primary wick 190 to evaporate and form vapor within the second vapor passage 183 when heat is applied to the secondary evaporator 150.
The reservoir 155 is cold-biased, and thus, it is cooled by a cooling source that will allow it to operate, if unheated, at a temperature that is lower than the temperature at which the heat transfer system 105 operates. In one implementation, the reservoir 155 and the secondary condenser 122 are in thermal communication with the heat sink 165 that is thermally coupled to the condenser 120. For example, the reservoir 155 can be mounted to the heat sink 165 using a shunt 170, which may be made of a heat conductive material, such as aluminum, for example. In this way, the temperature of the reservoir 155 tracks the temperature of the condenser 120.
Though not shown in
Referring also to
Initially, the reservoir 155 is cold-biased by, for example, mounting the reservoir 155 to the heat sink 165 (step 305). The reservoir 155 may be cold-biased to a temperature below the critical temperature of the working fluid, which, as discussed, is the highest temperature at which the working fluid can exhibit liquid-vapor equilibrium. For example, if the fluid is ethane, which has a critical temperature of 33° C., the reservoir 155 is cooled to below 33° C. As the temperature of the reservoir 155 drops below the critical temperature of the working fluid, the reservoir 155 partially fills with a liquid condensate formed by the working fluid. The formation of liquid within the reservoir 155 wets the secondary wick 180 and the primary wick 190 of the secondary evaporator 150 (step 310).
Meanwhile, power is applied to the priming system 110 by applying heat from the controlled heat source Qsp 151 to the secondary evaporator 150 (step 315) to enhance or initiate circulation of fluid within the heat transfer system 105. Vapor output by the secondary evaporator 150 is pumped through the vapor line 130 and through the condenser 120 (step 320) due to capillary pressure at the interface between the primary wick 190 and the second vapor passage 183. As vapor passes through the condenser 120, it is converted to liquid (step 325). The liquid formed in the condenser 120 is pumped to the main evaporator 115 of the heat transfer system 105 (step 330). When the main evaporator 115 is at a higher temperature than the critical temperature of the fluid, the liquid entering the main evaporator 115 evaporates and cools the main evaporator 115. This process (steps 315-330) continues, causing the main evaporator 115 to reach a set point temperature (step 335), at which point the main evaporator 115 is able to retain liquid and be wetted and to operate as a capillary pump. In one implementation, the set point temperature is the temperature to which the reservoir 155 has been cooled. In another implementation, the set point temperature is a temperature below the critical temperature of the working fluid. In a further implementation, the set point temperature is a temperature above the temperature to which the reservoir 155 has been cooled.
Once the set point temperature has been reached (step 335), the heat transport system 100 operates in a main mode (step 340) in which heat from the heat source Qin 116 that is applied to the main evaporator 115 is transferred by the heat transfer system 105. Specifically, in the main mode, the main evaporator 115 develops capillary pumping to promote circulation of the working fluid through the heat transfer system 105. Also, in the main mode, the temperature of the reservoir 155 may be reduced below the set point temperature of the main evaporator 115. The rate at which the heat transfer system 105 cools down during the main mode depends, in part, on the cold-biasing of the reservoir 155 because the temperature of the main evaporator 115 closely follows the temperature of the reservoir 155. Additionally, though not necessarily, a heater can be used to further control or regulate the temperature of the reservoir 155 during the main mode (step 340). Furthermore, in the main mode, the power applied to the secondary evaporator 150 by the controlled heat source Qsp 151 is reduced, thus bringing the heat transfer system 105 down to a normal operating temperature for the fluid. For example, in the main mode, the heat load from the controlled heat source Qsp 151 to the secondary evaporator 150 is kept at a value equal to or in excess of heat conditions, as defined below. In one implementation, the heat load from the heat source Qsp is kept to about 5 to 10% of the heat load applied to the main evaporator 115 from the heat source Qin 116.
Thus, in the
At any time during operation, the heat transfer system 105 can experience heat conditions that cause formation of vapor on the liquid side of the evaporator, such as those resulting from heat conduction across the primary wick 140 and parasitic heat applied to the liquid line 125. Specifically, heat conduction across the primary wick 140 can cause liquid in the core 135 to form vapor bubbles, which, if left within the core 135, would grow and block off liquid otherwise supplied to the primary wick 140, thus causing the main evaporator 115 to fail. One such heat condition is caused by parasitic heat input into the liquid line 125 (referred to as “parasitic heat gains”), which causes liquid within the liquid line 125 to form vapor.
To reduce the adverse impact of heat conditions such as those discussed above, the priming system 110 operates at a power level Qsp 450 that is greater than or equal to the sum of the head conduction and the parasitic heat gains. As mentioned above, for example, the priming system 110 can operate at 5 to 10% of the power to the heat transfer system 105. In particular, fluid that includes a combination of vapor bubbles and liquid is swept out of the core 135 for discharge into the secondary fluid line 160 leading to the secondary condenser 122. In particular, vapor that forms within the core 135 travels along the bayonet tube 143 and directly into the fluid outlet port 139. Furthermore, vapor that forms within the first vapor passage 144 travels into the fluid outlet port 139 by either traveling through the secondary wick 145 (if the pore size of the secondary wick 145 is large enough to accommodate vapor bubbles) or through an opening (not shown) at an end of the secondary wick 145 near the outlet port 139 that provides a clear passage from the first vapor passage 144 to the outlet port 139. The secondary condenser 122 condenses the bubbles in the fluid and pushes the fluid to the reservoir 155 for reintroduction into the heat transfer system 105.
Similarly, to reduce parasitic heat input to the liquid line 125, the secondary fluid line 160 and the liquid line 125 can form a coaxial configuration such that the secondary fluid line 160 surrounds and insulates the liquid line 125 from surrounding heat. This implementation is discussed further below with reference to
As shown in
As mentioned, in one implementation, ethane may be used as the fluid in the heat transfer system 105. Although the critical temperature of ethane is 33° C., for the reasons generally described above, the heat transport system 100 can start up from a supercritical state in which the heat transport system 100 is at a temperature of 70° C. As power Qsp is applied to the secondary evaporator 150, the temperatures of the condenser 120 and the reservoir 155 drop rapidly (between times 452 and 410). A trim heater can be used to control the temperature of the reservoir 155 and thus the condenser 120 to −10° C. To startup the main evaporator 115 from the supercritical temperature of 70° C., a heat load or power input Qsp of 10 W is applied to the secondary evaporator 150. Once the main evaporator 115 is primed, the power input from the controlled heat source Qsp 151 to the secondary evaporator 150 and the power applied to and through the trim heater both may be reduced to bring the temperature of the heat transport system 100 down to a nominal operating temperature of about −50° C. For instance, during the main mode, if a power input Qin of 40 W is applied to the main evaporator 115, the power input Qsp to the secondary evaporator 150 can be reduced to approximately 3 W while operating at −45° C. to mitigate the 3 W lost through heat conditions (as discussed above). As another example, the main evaporator 115 can operate with power input Qin from about 10 W to about 40 W with 5 W applied to the secondary evaporator 150 and with the temperature 405 of the reservoir 155 at approximately −45° C.
Referring to
Referring to
Referring to
Whether using a three-port or four-port evaporator design, design considerations of heat transport systems such as the heat transport systems 100 and 700 may include various advantageous features. For example, with specific reference to elements of the heat transport system 100 (although similar comments may generally apply to the heat transport system 700 of
In one implementation, the vapor line 130 is made with smooth-walled stainless steel tubing having an outer diameter (OD) of 3/16″ and the liquid line 125 and the secondary fluid line 160 are made of smooth-walled stainless steel tubing having an OD of ⅛″. The lines 125, 130, 160 may be bent in a serpentine route and plated with gold to minimize parasitic heat gains. Additionally, the lines 125, 130, 160 may be enclosed in a stainless steel box with heaters to simulate a particular environment during testing. The stainless steel box can be insulated with multi-layer insulation (MLI) to minimize heat leaks through panels of the heat sink 165.
In one implementation, the condenser 122 and the secondary fluid line 160 are made of tubing having an OD of 0.25 inch. The tubing is bonded to the panels of the heat sink 165 using, for example, epoxy. Each panel of the heat sink 165 is an 8×19 inch direct condensation, aluminum radiator that uses a 1/16-inch thick face sheet. KAPTON™ heaters can be attached to the panels of the heat sink 165, near the condenser 120 to prevent inadvertent freezing of the working fluid. During operation, temperature sensors such as thermocouples can be used to monitor temperatures throughout the heat transport system 100.
The heat transport system 100 may be implemented in any circumstances where the critical temperature of the working fluid of the heat transfer system 105 is below the ambient temperature at which the heat transport system 100 is operating. The heat transport system 100 can be used to cool down components that require cryogenic cooling. Referring to
The miniaturized system 800 reduces mass, increases flexibility, and provides thermal switching capability when compared with traditional thermally switchable vibration-isolated systems. Traditional thermally switchable, vibration-isolated systems require two flexible conductive links (FCLs), a cryogenic thermal switch (CTSW), and a conduction bar (CB) that form a loop to transfer heat from the cryogenic component to the cryogenic cooling source. In the miniaturized system 800, thermal performance is enhanced because the number of mechanical interfaces is reduced. Heat conditions at mechanical interfaces account for a large percentage of heat gains within traditional thermally switchable, vibration-isolated systems. The CB and two FCLs are replaced with the low-mass, flexible, thin-walled tubing used for the coil configurations 805 of the miniaturized system 800.
Moreover, the miniaturized system 800 can function in a wide range of heat transport distances, which permits a configuration in which the cooling source (such as the cryocooler 810) is located remotely from the cryogenic component 816. The coil configurations 805 have a low mass and low surface area, thus reducing parasitic heat gains through the lines 125 and 160. The configuration of the cooling source 810 within the miniaturized system 800 facilitates integration and packaging of the miniaturized system 800 and reduces vibrations on the cooling source 810, which becomes particularly important in infrared sensor applications. In one implementation, the miniaturized system 800 was tested using neon, operating at 25 to 40 K.
Referring to
The heat transfer system 105 may be used in medical applications, or in applications where equipment must be cooled to below-ambient temperatures. As another example, the heat transfer system 105 may be used to cool an infrared (IR) sensor that operates at cryogenic temperatures to reduce ambient noise. The heat transfer system 105 may be used to cool a vending machine, which often houses items that preferably are chilled to sub-ambient temperatures. The heat transfer system 105 may be used to cool components such as a display or a hard drive of a computer, such as a laptop computer, handheld computer, or a desktop computer. The heat transfer system 105 can be used to cool one or more components in a transportation device such as an automobile or an airplane.
Other implementations are within the scope of the following claims. For example, the condenser 120 and heat sink 165 can be designed as an integral system, such as, for example, a radiator. Similarly, the secondary condenser 122 and heat sink 165 can be formed from a radiator. The heat sink 165 can be a passive heat sink (such as a radiator) or a cryocooler that actively cools the condensers 120, 122.
In another implementation, the temperature of the reservoir 155 is controlled using a heater. In a further implementation, the reservoir 155 is heated using parasitic heat. In another implementation, a coaxial ring of insulation is formed and placed between the liquid line 125 and the secondary fluid line 160, which surrounds the insulation ring.
More particularly, the heat transport system 1000 includes multiple heat transfer systems 1005 and a priming system 1011 configured to convert fluid from within the heat transfer systems 1005 into a liquid capable of priming the heat transfer systems 1005. The heat transfer systems 1005 each include four-port evaporators 600 that are coupled to one or more condensers 1015 by a vapor line 1020 and a fluid line 1025. The priming system 1011 includes a cold-biased reservoir 1030 hydraulically and thermally connected to a priming evaporator 1035.
Similarly to the four-port, parallel arrangement shown in
Moreover, as illustrated by
More particularly, the actively pumped heat transport system 1100 includes multiple heat transfer systems 1105, having evaporators 600, and a mechanical pump 1110 that is arranged in series between a condenser 1115 (and a vapor line 1120 feeding the condenser 1115) and the evaporators 600, along a liquid line 1125. A reservoir 1130 is disposed between the mechanical pump 1110 and the condenser 1115, where the reservoir 1130 may be used for, for example, managing excess fluid flow, fine temperature control through cold-biasing, and other features and uses as described herein and as are known.
The actively pumped heat transport system 1100 including the mechanical pump 1110 shares certain features and advantages with the passive heat transport systems described above with respect to
The mechanical pump 1110 thus provides a source of pumping power for moving fluid through the primary loop and/or the secondary loop of the heat transport system 1100. This pumping power may be used during various operations of the heat transport system 1100, and may be in addition to, or in the alternative to, other sources of pumping power.
For example, the pumping power provided by the mechanical pump 1110 may be used to provide liquid to the evaporators 600 during a start-up operation of the evaporators 600, perhaps in conjunction with a separate priming system. Such a priming system may include, for example, the priming system 110 of
The mechanical pump 1110 also may be used during steady-state operation of the heat transport system 1100, either continuously or intermittently, as needed to maintain a desired operational state of the heat transport system 1100. For example, the mechanical pump 1110 may be activated during start-up of the heat transport system 1100, and then may be bypassed or otherwise de-activated during steady-state operation of the heat transport system 1100, unless and until a secondary pumping source (e.g., passive pumping supplied by capillary pressure) is insufficient to provide adequate heat transfer. In this sense, the heat transport system 1100 may be considered a dual-pumping system, in which mechanical pumping, capillary pumping, or some combination of both, is available on an as-needed basis to an operator or designer of the heat transport system 1100. In particular, for instance, when the heat transport system 1100 is used to provide heat transfer over relatively large distances (e.g., 10 meters or more), the mechanical pump 1110 may be required to be used continuously to ensure adequate pumping power.
As a final example, and as discussed in more detail below, pumping power of the mechanical pump 1110 also may be used to ensure sweeping or venting of vapor bubbles from the cores of the evaporators 600. As such, a use or extent of the pumping power of the mechanical pump 1110 may be dependent on the extent to which such vapor bubbles exist (or are thought to exist) within the evaporator cores or, similarly, may be dependent on the extent to which conditions for creating such vapor bubbles within the evaporator cores exist within and around the heat transport system 1100.
As just referenced, and as described above in detail, the construction of three- and/or four-port evaporators permit control and management of liquid and vapor phases within the evaporator core(s). Specifically, for example, fluid within the cores 615 of evaporators 600 that includes a combination of liquid and vapor bubbles may be swept out of the cores 615 for discharge into the secondary liquid channels 640 and vapor channels 645 (or into the mixed secondary fluid line 160 in a three-port evaporator configuration).
As also described above, such mixed-phase fluid within the core 615 may result from various causes. For example, the mixed-phase fluid may result from heat conduction across the primary wick 620 and/or parasitic heat gains through the liquid line 1125 (e.g., when routing the liquid line through a “hot” environment). Whatever the cause of the mixed-phase flow, the heat transport system 1100 (using the mechanical pump 1110), and the systems described above (using the priming or secondary evaporators 150/710/1011 and associated reservoirs), are operable to provide excess liquid to the evaporators 600, above and beyond the minimum needed to maintain operation of the heat transport system (e.g., an amount needed to maintain saturation of the wicks and associated capillary pumping).
As a result, the heat transport system 1100, and the systems described above, are able to use this excess liquid to vent or sweep the gaseous portion of the mixed-phase flow from the evaporators 600, using the secondary flow loops that include the secondary liquid/vapor channels 640/645 or the mixed secondary fluid line 160. In this way, excess vapor enters the secondary loop either through the secondary wick 635 (if feasible for a given pore size of the secondary wick 635), or through an opening at an end of the secondary wick near an outlet port for the secondary loop(s), and is returned to the condenser 1115 for condensation and subsequent return through the liquid line 1125 and/or to the reservoir 1130.
In one implementation, an amount of excess liquid provided to the cores of the evaporators 600 is optimized. In this implementation, the amount of excess liquid is sufficient to sweep all of the evaporator cores present in the system, but not substantially more than this amount, since excess fluid in the heat transport system 1100 may affect performance and reliability of the heat transport system 1100. However, sweeping all of the evaporators 600 may be problematic, particularly, for example, when the evaporators 600 are not powered equally or, in the limiting case, where one of the evaporators 600 receives no heat (or actually acts as a condenser).
One technique for optimizing an amount of excess fluid flow to the evaporators 600 includes an appropriate selection of line diameters of the evaporator wicks, and/or for the liquid line 1125 or the vapor line 1120. By selecting these line diameters appropriately, an amount of excess fluid beyond that required for operation of the evaporators 600 may be reduced or minimized, while still ensuring that the amount of excess fluid is sufficient to completely sweep or vent all of the evaporators 600.
More particularly, in an implementation such as the one just described, such line sizing may be a factor in determining an efficiency of the sweeping of the evaporators 600. In the case of
One parameter for describing the appropriate sizing criteria includes a ratio of the flow resistance of the sweepage line(s) 640/645 (or, in
With such complete sweepage being provided, the heat transport system 1100 may use a narrow-diameter, small-pore, metal wick (e.g., 1 micron pore metal wick), which provides high thermal conductivity and increased pumping capability, relative to the polyethylene wicks that often are used in conventional heat transport systems. Such polyethylene wicks may be used despite their reduced pumping capacity, in part due to their relatively wide diameter and large pore size, which tends to reduce their thermal conductivity and, therefore, tends to reduce a presence of vapor within the liquid line 1125 and liquid core 615.
In other words, since the structure and function of the heat transport system 1100 enable venting or sweeping of such undesirable vapor from the core 615, the heat transport system 1100 may not be required to resort to disadvantageous measures to avoid the presence of this vapor in the first place. As a result, the system 110 may enjoy the advantages of narrow-diameter, small-pore, metal wicks, and, in particular, increased pumping against gravity by a factor of ten, relative to polyethylene wicks, for example. Similarly, the heat transport system 1100 may not require subcooled liquid to be returned to the core 615, such that the liquid line 1125 may be routed through hotter environments than are feasible with conventional systems that do not offer vapor sweepage, as it is described herein.
Accordingly, the heat transport system 1100 may provide many advantageous features for the transport and disposal of heat. For example, in addition or as an alternative to one or more of the features just described, the mechanical pump 1110 of the heat transport system 1100 may provide increased flow, increased flow controllability, and increased waste heat transportation and rejection, relative to passive systems (for example, heat transport may occur on the order of 50 kW or more, over a distance of 10 meters or more). As another example, the mechanically pumped heat transport system 1100 may greatly reduce temperature gradients across phased array antennas that may include thousands of elements arranged in complex arrays, thereby reducing an overall size of such arrays and reducing or eliminating the need for separate heat pipes to maintain acceptable element temperatures within the arrays.
The heat transport system 1100 offers one or more of the following or other advantages over conventional actively pumped systems as well, including those that have been deployed, for example, in geosynchronous communication satellites. For instance, the two-phase nature of the heat transport system 1100 is beneficial to heat transfer at the thermal interfaces, and reduces required pumping power. Additionally, the sweepage of excess vapor and its complete condensation within the condenser 1115 may reduce an amount of mixed fluid (i.e., two-phase) flow experience by the mechanical pump 1110. As a result, a lifetime and reliability of the mechanical pump 1110 may be improved, since vapor within a liquid mechanical pump such as the mechanical pump 1110 tends to provide excessive stress within the pump.
In addition to some or all of these and other advantages, the heat transport system 1100 is compatible with a wide variety of thermal management components and features. Accordingly,
In
The mixed fluid line 1208 is shown as a dotted line in
Further, the mixed fluid line 1208 may be used in conjunction with a secondary evaporator 1214, which, when used with a (cold-biased) reservoir 1216 in one of the various manners described above, provides for advantages such as, for example, operation of the system 1200 (or the heat transport system 1100) in a passive mode, in which the mechanical pump 1202 (or 1110) is bypassed, perhaps using a pump bypass valve 1218, and the system 1200 (or 1100) relies solely on capillary pumping for fluid flow.
To the extent that the system 1200 uses fine-pore metal wicks, as described above with respect to
As referred to above with respect to
The above discussion of a general operation of the system 1200 included reference to the evaporators 1206, similar in structure and function to one or more of the various evaporators discussed herein, and using a cold plate as a heat transfer surface. However, it is a strength of the system 1200 that multiple types and arrangements of evaporators and heat transfer surfaces may be used.
For example, in
Further in
In particular, such a separate loop may be used to connect the spray-cooled evaporator 1228 to the system 1200, due to the fact that a nozzle pressure drop (e.g., 0.7 bar) of the spray-cooled evaporator 1228 relative to a capillary pressure rise (e.g., 0.4 bar) in the system 1200 may make parallel arrangement of the spray-cooled evaporator 1228 difficult in some use environments. In other implementations, however, the spray-cooled evaporator 1228 may be integral to the system 1200, instead of being coupled through the condensing heat exchanger 1226.
The spray-cooled evaporator 1228 may be used for efficient thermal control of high heat flux sources. For example, 500 W/cm2 has been demonstrated with a heat transport system using ammonia as the working fluid. A loop using the spray-cooled evaporator 1228 may be operated near saturation in order to maximize heat transfer.
Such a spray-cooled evaporator 1228 may be particularly useful, for example, in spacecraft thermal management. For instance, in spacecraft electronics, heat fluxes at transistor gates are approaching 1 MW/in2. As component size continues to shrink and heat fluxes rise further, state-of-the-art systems may be used to offset the associated increases in local temperature drops. The significantly higher heat-transfer coefficient afforded by spray cooling, using the spray-cooled evaporator 1228, may be advantageous in this respect.
Factors to consider in using the spray-cooled evaporator 1228 include, for example, nozzle optimization and scalability of the spray-cooled evaporator 1228 to extended surface areas. In one implementation, the spray-cooled evaporator 1228 may be used for cooling laser diode applications.
In
Also, it should be apparent from
Similarly, many types of condenser configurations may be used. For example, the condenser 1212 referred to above may include a body-mounted radiator, while a condenser 1232 may include a multi-fold, deployable or steerable radiator. Particularly in high-power spacecraft, these radiators may be direct condensation or may use discrete heat pipes, depending on, for example, system reliability factors and/or a mass of micro-meteoroid shielding. As just mentioned, the condenser 1232 also may be made steerable for non-geostationary applications, in order, for example, to minimize radiator backloading. Gimbaled heat transport systems used in conventional telecom satellite systems may be used to enable such steerable radiators. Further, passive two-phase loops (e.g., LHPs) also may be incorporated into two-axis gimbaled systems. Other examples of condenser configurations are discussed below with respect to
Finally with respect to
The choice of whether to use the liquid pump 1202 or the vapor compressor 1302 is typically a design consideration. Generally, the liquid pump 1202 offers lighter weight and increased pumping power relative to the vapor compressor 1302 (due to, for example, the lower volumetric flow rate of the former). On the other hand, the vapor compressor 1302 offers heat pumping (i.e., an increased condensation temperature), which may reduce radiator heat and overall system mass and, additionally, may offer a longer operational lifetime.
The liquid pump 1202 may include, for example, a hermetically sealed, magnetically driven, centrifugal design. Other liquid pumps for space station applications, e.g., waste water and carbon dioxide, also may be used.
The vapor compressor 1302 may be a variable-speed compressor, and may include, for example, a hermetically sealed, oil-less centrifugal compressor with gas or magnetic bearings. A low-lift heat pump, which includes a similar compressor, also may be used. Further examples of specific types of pumps are provided below and, in particular, with respect to
As also illustrated in
Further in
Referring to
Also in
Referring to
Referring to
More specifically, as should be apparent from the above discussion, the secondary evaporator 1602 is thermally and hydraulically connected to a cold-biased reservoir 1604. As described with respect to
Further, an isothermalized plate or structure 1622 may be included. Such a structure may be useful, for example, in settings where a constant temperature surface is desired or required, such as, for example, some laser systems. To the extent that such systems require a constant temperature surface, it may be efficient to use the (waste) heat being transported by the system 1600 to keep the structure 1622 at a constant temperature. When the structure 1622 is used, a flow regulator 1624 (perhaps similar to the regulators 1402 of
A liquid line heat exchanger 1628 is used to provide subcooling of the liquid before it is routed to the evaporators. Also, as just referred to, the vapor return line 1626 returns vapor to the secondary evaporator 1602 and to the BPR 1606. The BPR 1606, generally speaking, ensures that no vapor reaches the condensers unless a vapor space for all evaporators in the system is devoid of liquid. As such, heat load sharing among the many parallel (or series) evaporators may be increased. An example of the BPR 1606 is discussed in detail below with respect to
In
In
In
Thus, the BPR 1606 typically is positioned at the inlet to the condenser, where the vapor line 2002 meets the condenser inlet header 2004. As such, the unsealed end 2012 of the internal wick 2008 is thermally linked to a cooling source 2020 (e.g., radiator or other heat sink), and is connected to the condenser inlet header 2004 end of the BPR 1606. The other end 2010 (sealed end of the internal wick 2008) is connected in series to the vapor line 2002.
The BPR 1606 ensures that no vapor reaches the condenser unless the vapor space for all evaporators in the system is devoid of liquid. As such, heat load sharing among the many parallel or series evaporators in the system may be increased. The BPR 1606 typically uses pores 2022 selected such that the pore size is larger than the pore size(s) of any of the system evaporators. Thus, as vapor is produced, it is contained within all the evaporator vapor side space, and is thereby given an opportunity to condense. The vapor clears all evaporator vapor side space of liquid and, once that condition is achieved, pushes through the BPR wick 2008 and allows flow to reach the connected condenser.
In
A tube 2110 defines a body of the isolator 2100 that includes a wick 2112 and a flow annulus 2114. Along with a swage seal 2116, the wick 2112 and flow annulus 2114 enable isolation of the liquid flow to an associated evaporator, through the liquid outlet port 2108. If the associated evaporator experiences pump failure, it may be bypassed by the isolator 2100 until repair may be effected.
Similarly, in
In
The internal wicking structure 2308 includes a continuous wick element 2312 with the same capillary pumping radius 2314 (rpevap) as an evaporator wick that hydraulically links the liquid line 2302 to one or more wick segments 2316, 2318, and 2320 with larger capillary pumping radii (rp1, rp2, and rp3). The capillary sensor 2300 is thermally coupled to one or more heat sources 2322.
In operation, the temperature sensors 2310 measure envelope temperature above each wick segment 2316, 2318, 2320, and/or temperature differences between the envelopes above each wick segment 2316, 2318, 2320. Temperature increases on the envelope indicate that the wick segment below the envelope may no longer be saturated with liquid, due to inability of the wick segment to support the pressure difference between the vapor line 2304 and the liquid line 2302. Thus, temperature feedback may be used to adjust a pumping pressure delivered by the mechanical pump 1102 by, for example, adjusting pump speed or adjusting a position of an associated pump bypass valve, in order to maintain saturation of the appropriate wick segment(s).
In
In operation, temperature increases on the envelope indicate that the wick segment between the sensor and the vapor manifold may no longer be saturated with liquid due to, for example, an inability of the wick segment to support a pressure difference between the vapor line 2304 and the liquid line 2302. Then, temperature feedback may be used to adjust the pumping pressure delivered by the mechanical pump, by either adjusting pump speed or the position of a pump bypass valve, to maintain saturation of the appropriate wick segment(s).
As shown in
As described, such thermal management systems absorb waste heat from a wide range of sources, including, for example, waste heat of electronics and power conditioning equipment, high-powered spacecraft, antennas, batteries, and laser systems. Military applications, such as space-based radar and lasers, offer a wide suite of potential heat sources and the elements required for their thermal management. Accordingly, such military applications, such as those requiring counterspace detection and offensive force projection capabilities, may benefit from such thermal management systems, which provide high heat transport capability and high heat rejection, as well as high flux heat acquisition and efficient thermal storage, all the while minimizing system mass and maintaining operational reliability over the mission life. Commercial applications, such as, for example, soda-dispensing machines and notebook computers, also may benefit from the implementations of heat transport systems discussed herein, or variations thereof.
This application is a continuation of application Ser. No. 10/890,382, filed Jul. 14, 2004, which claims priority to U.S. Provisional Application Ser. No. 60/486,467, filed Jul. 14, 2003, and is a continuation-in-part of U.S. Patent Application Ser. No. 10/602,022, filed Jun. 24, 2003, now U.S. Pat. No. 7,004,240, issued Feb. 28, 2006, which claims priority to U.S. Provisional Patent Application Ser. No. 60/391,006, filed Jun. 24, 2002, and is a continuation-in-part of U.S. Patent Application Ser. No. 09/896,561, filed Jun. 29, 2001, now U.S. Pat. No. 6,889,754, issued May 10, 2005, which itself claims priority to U.S. Patent Provisional Application Ser. No. 60/215,588, filed Jun. 30, 2000. These applications are herein incorporated in their entirety.
Number | Date | Country | |
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60486467 | Jul 2003 | US | |
60391006 | Jun 2002 | US | |
60215588 | Jun 2000 | US |
Number | Date | Country | |
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Parent | 10890382 | Jul 2004 | US |
Child | 12426001 | US |
Number | Date | Country | |
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Parent | 10602022 | Jun 2003 | US |
Child | 10890382 | US | |
Parent | 09896561 | Jun 2001 | US |
Child | 10890382 | US |