In recent years, attention has been focused on methods of high heat flux removal at low surface temperatures. This is due in large part to the advancing requirements of the electronics industry that prevent high temperature heat transfer due to the operating conditions of electronics. Though the heat transfer process is very complex and still not completely understood, many evaporative spray cooling experiments have been performed which indicated the high heat removal capability of this cooling technique. The spray technique generally works in the following way; a spray nozzle is used to atomize a pressurized liquid, and the resulting droplets are impinged onto a heated surface. A thin film of liquid is formed on the heat transfer surface in which nucleate boiling takes place. The droplet impingement simultaneously causes intense convection and free surface evaporation. When a liquid with a high latent heat of vaporization (such as water) is used, over 1 kW/cm2 of heat removal capability has been demonstrated.
The temperature of the cooled surface is determined by the boiling point of the liquid. Since the resulting heat transfer coefficient is very large (50,000 to 500,000 W/m2C) the surface temperature will be only a few degrees centigrade above the boiling point of liquid.
This type of cooling technique is most appropriately implemented when used to cool high heat flux devices such as power electronics, microwave and radio frequency generators, and diode laser arrays.
Prior art describes processes and devices related to cooling of small, individual electronic chips. This can be seen in, for example, U.S. Pat. Nos. 5,854,092; 5,718,117; and 5,220,804. This prior art uses a liquid spray to cool individual electronic components, or an array of these individual components located at discrete distances from each other. Since the electronic components (the heat sources) are individual devices with spaces between, the liquid spray cones do not overlap or interact with each other. The typical size of an electronic chip is 2 cm2 in area and is spaced at a distance of 0.5 to 1 cm. This allows the prior art to cool these chips with an impinging spray without interfering with the spray process of the surrounding chips.
As stated above, diode laser arrays and microwave generators are devices that can be cooled with this type of impinging spray technology. Current market forces are driving these devices to increased power and size requirements. As a result, high heat flux devices are now being designed with surface areas much larger than 2 cm2. New high heat flux devices will be 100 cm2 to 1000 cm2. The entire large surface area will need to be cooled at the same high heat flux rate as the small devices were in the prior art. However, the prior art does not detail a method to cool such a large device. Prior art only details a method to cool several small individual devices.
It may be thought that a large surface could be cooled with an array of nozzles spraying down on the large surface in the same way a single nozzle sprays down on a small surface, as shown in the prior art. However, it has been shown in a study with air jet impingement that scaling in this way is not possible. Simply put, the effectiveness of the jets or sprays in the center of the array interact with each other in a way that considerably reduces the ability to transfer heat. This is a result of the fluid flow accumulating as the fluid moves outward from the stagnation point. A good portion of the impinging droplets are vaporized with this system, however, this is not so for all the liquid. The remaining liquid will flow off the heated surface and be returned to the pump. When the surface is large, the fluid from the nozzles at the center of the surface will need to travel across the entire surface before exiting at the edges. This can be called the “spray liquid run-off problem.”
The subject invention pertains to a method and apparatus for high heat flux heat transfer. The subject invention can be utilized to transfer heat from a heat source to a coolant such that the transferred heat can be effectively transported to another location. Examples of heat sources from which heat can be transferred from include, for example, fluids and surfaces. The coolant to which the heat is transferred can be sprayed onto a surface which is in thermal contact with the heat source, such that the coolant sprayed onto the surface in thermal contact with the heat absorbs heat from the surface and carries the absorbed heat away as the coolant leaves the surface. The surface can be, for example, the surface of an interface plate in thermal contact with the heat source or a surface integral with the heat source. The coolant sprayed onto the surface can initially be a liquid and remain a liquid after absorbing the heat, or can in part or in whole be converted to a gas or vapor after absorbing the heat. The coolant can be sprayed onto the surface, for example, as a stream of liquid after being atomized, or in other ways which allow the coolant to contact the surface and absorb heat. Once the heat is absorbed by the coolant, the coolant can be transported to another location so as to transport the absorbed heat as well.
The subject invention pertains to a method and apparatus for cooling surfaces and/or devices. In a specific embodiment, the subject invention can incorporate a spray nozzle and a cooling/electronic interface surface. The spray nozzle may use pressurized liquid (commonly known as pressure atomizer nozzles), pressurized liquid and pressurized vapor (commonly known as vapor assist nozzles), and/or pressurized vapor nozzle (commonly known as vapor blast or vapor atomizer nozzles) to develop the atomized liquid spray used in the cooling process.
The subject invention also relates to a heal transfer apparatus having an enhanced surface which can increase the rate of heat transfer from the surface to an impinging fluid. The subject enhanced surface can be incorporated with any of the heat transferred surfaces disclosed in the subject patent application or incorporated with other heat transfer surfaces. The subject invention also pertain to heat transfer apparatus, such as heat transfer plates, which incorporate the subject enhanced surfaces. The subject enhanced surfaces can also be utilized for heat desorbtion from a surface.
In a specific embodiment, the cooling/electronic interface surface can be compartmentalized such that spray entering one compartment is impeded from crossing over to adjacent compartments. In a further specific embodiment, a plurality of nozzles can each spray into one of a plurality of compartments such that spray from each individual nozzle is applied to a specific target area. For example, each nozzle may spray one compartment. The excess liquid which enters each compartment can then be forced out of the compartment in a counter-parallel flow from the spray direction rather than a perpendicular flow as in prior art, so as to correct the liquid run-off problem. The shape and depths of the compartments can vary according to the type of nozzle used to atomize the liquid coolant. Preferably, the subject compartments incorporate side walls which can redirect the exiting flow in a pattern that is not perpendicular to the incoming flow.
The atomized spray can be directed onto the rear surface of the compartmentalized interface plate. The spray is preferably positioned to create the most even application of atomized liquid onto the entire rear surface. The liquid can be sprayed at a temperature near its boiling point. Thus, when the liquid hits the heated surface in the rear of the compartment, the liquid can begin to boil. The heat from the electronics, or other heat source, is transferred through the interface into the boiling liquid spray at a very high rate. The created coolant vapor and excess liquid exit the compartment in a direction that is not perpendicular to the incoming flow. Under the operating conditions of an open loop system, the boiling point of the liquid coolant must be at ambient pressure since the evaporating environment is exposed to the ambient. Under these conditions, the heat removed by the developed vapor is released to the atmosphere. However, not all vaporized coolants can be responsibly released to the atmosphere, due, for example, to environmental concerns. In addition, coolants with boiling points other than ambient may be preferred. Accordingly, specific embodiments of the subject invention can be operated in a closed loop.
In a closed loop system, the interface plate can be located within a sealed housing so that the spray and the resultant vapor is trapped within the sealed housing. Under this condition, the pressure within the housing can influence the boiling point of the coolant and the operating temperature. As the coolant vaporizes, it carries the heat from, for example, electronics, away from the interface plate. Since the system is now closed, the vapor can be condensed and the heat released out of the housing through a condenser. The condenser can incorporate, for example, a standard heat exchanger or can operate via a sub-cooled mist of the coolant sprayed within the housing. The mist can be sub-cooled below the saturation temperature of the coolant within the housing via an external heat exchanger. As the sub-cooled liquid spray contacts the saturated vapor, heat is transferred to the spray and the vapor condenses on the liquid droplets and flows to a liquid reservoir.
The coolant can be drawn from the liquid reservoir, for example, by a liquid pump or via venturi action of a vapor atomizer nozzle. The liquid then flows through the nozzle and is once again sprayed onto the interface plate. The circulation of the coolant within the closed process depends on the type of atomizer used. If pressure atomizer nozzles are used, then a liquid pump can suffice. If vapor assist nozzles or vapor atomizer nozzles are used, then both a vapor compressor and a liquid pump can be used in the circulation of the coolant.
Typically, the heat gained by the liquid in the closed system is transferred to a refrigerant of a vapor compression cycle via a heat exchanger. The vapor compression cycle increases the temperature of the now warmer refrigerant and allows it to release the heat to the environment. This is commonly known as the chiller loop.
An additional feature can be added to the closed system that combines it with a vapor compression cycle without the heat exchanger interface between the two loops. This combination involves using a refrigerant as the coolant in both loops. Under this scenario, liquid refrigerant can be atomized onto the interface plate. Vapor and excess liquid refrigerant can be expelled from the compartment and flow into the housing. The saturated vapor can be removed from the housing with a vapor compressor and can be compressed to a temperature above ambient temperature of the final heat sink, for example atmospheric air. The now superheated vapor can flow through a heat exchanger releasing the heat to the final heat sink. As the heat is released, the superheated vapor condenses to liquid refrigerant. As is common to vapor compression cycles, the higher pressure saturated liquid can flow through an expansion valve. The liquid is allowed to expand to the pressure of the housing, cools to its saturation temperature within the housing, and flows to the liquid reservoir ready to begin the process once again.
The subject invention pertains to a method and apparatus for high heat flux heat transfer. The subject invention can be utilized to transfer heat from a heat source to a coolant such that the transferred heat can be effectively transported to another location. Examples of heat sources from which heat can be transferred from include, for example, fluids and surfaces. The coolant to which the heat is transferred can be sprayed onto a surface which is in thermal contact with the heat source, such that the coolant sprayed onto the surface in thermal contact with the heat absorbs beat from the surface and carries the absorbed heat away as the coolant leaves the surface. The surface can be, for example, the surface of an interface plate in thermal contact with the heat source or a surface integral with the heat source. The coolant sprayed onto the surface can initially be a liquid and remain a liquid after absorbing the heat, or can in part or in whole be converted to a gas or vapor after absorbing the heat. The coolant can be sprayed onto the surface, for example, as a stream of liquid after being atomized, or in other ways which allow the coolant to contact the surface and absorb heat. Once the heat is absorbed by the coolant, the coolant can be transported to another location so as to transport the absorbed heat as well.
In a specific embodiment, the subject invention relates to a cooling process which begins, as shown in
A specific embodiment of an interface plate 3 in accordance with the subject invention is shown in FIG. 2A. The cooling plate 3 shown in
The number of compartments can be determined by the area of each compartment, the widths of the compartment walls 21, and the total area of desired cooling. Each compartment can have one or more nozzles which spray into the compartment. In a specific embodiment, the one or more nozzles spray onto the heated surface 2 at the bottom of the compartment.
In a specific embodiment of the subject invention, partition walls 21 can be removed and a plurality of spray nozzles can spray surface 2 such that the spray of the adjacent nozzles does not overlap and the liquid coolant sprayed onto surface 2 travels along the surface of surface liquid 2 until running into the liquid coolant sprayed onto surface 2 by an adjacent nozzle. As the flows of coolant from adjacent spray nozzles collide, the collision can change the momentum of the flows such that at least a portion, and preferably essentially all, of the combined flow flows away from surface 2. Accordingly, after the collision of adjacent flows, a substantial portion of the combined flow's momentum can then be in a direction perpendicular to surface 2. In addition, the combined flow may have a certain amount of momentum parallel to surface 2, such that the combined flow flows as a river, above surface 2, near the portion of surface 2 where the collision of the two adjacent flows occurs. The direction of these river flows depends, among other factors, on the spray patterns of the adjacent spray nozzles, the speed of the spray, and the form of the coolant being sprayed onto surface 2. When partition walls are present, how far out partition walls 21 protrude from surface 2 can impact how the coolant which impinges on surface 2 flows away from cell 23. Partition walls 21 can protrude sufficiently far such that coolant impinging on surface 2, upon reaching the end of the partition wall, continues away from interface plate 3. Alternatively, if partition walls are made to protrude less, coolant reaching the ends of the partition walls can, at least in part, flow in a river flow along the ends of the partition walls. Again, the exact nature of how the coolant flows after reaching the ends of the partition walls is dependent, among other factors, on the spray patterns of the adjacent spray nozzles, the speed of the spray, and the size and form of the coolant being spraying onto surface 2.
A manifold of spray nozzles in accordance with a specific embodiment of the subject invention is shown in FIG. 3. The spray nozzles 5 can be attached to manifold 30 with liquid inlet port 32 and vapor inlet port 34. A specific assembly of spray nozzle manifold 30 and compartmentalized interface plate 3 is shown in FIG. 4. In the embodiment shown in
In alternative embodiments, surface 2 can be a surface of a heat source such as an electronics circuit chip, power electron device, microwave or radio frequency generator, or diode laser array. In the situation where surface 2 is a surface of a heat source, partition walls 21 can be integral with the surface 2 of the heat source, or partition walls 21 can be part of a separate interface plate 3 without a surface 1 or surface 2 such that the partition walls themselves are the interface plate 3. In the latter case, interface plate 3, comprising partition walls 21 can be pressed against surface 2 of the beat source. If desired, a means for creating a seal between the partition walls 21 and surface 2. Such a sealing means can reduce, or substantially eliminate, flow of coolant between the ends of partition walls 21 and surface 2. In a specific embodiment, such means for sealing can be attached to the ends of partition walls 21 which will contact surface 2 of the heat source, such that as the ends of partition walls 21 are pressed against surface 2 a seal between the ends of partition walls 21 and surface 2 is created so as to reduce, or substantially eliminate, flow of coolant between the ends of partition walls 21 and surface 2. In a specific embodiment, interface plate 3 can be fixedly positioned with respect to a manifold of spray nozzles such that the manifold-interface plate combination can be brought into contact with a surface 2 of a heat source and operated to remove heat from surface 2 of the heat source.
Spray nozzles in accordance with the subject invention can spray, for example, jet sprays of coolant and or atomized sprays of coolant. Jet spray nozzles can spray liquid coolant in, for example, a solid cone or sheet such that the coolant hits the surface and breaks up. The coolant can then flow across surface 2. Atomizing spray nozzles can atomize the coolant into droplets of appropriate size and can provide the droplets with an appropriate velocity. Although a variety of droplet sizes and velocities can be utilized in accordance with the subject invention, in a specific embodiment an atomizing spray nozzle can be used which produces droplets having mean diameters in a range from about 10 microns to about 200 microns and provides the droplets a velocity in a range from about 5 meters per second to about 50 meters per second. Preferably, the size and velocity of the particles are such that the effects of gravity are neglible. Utilizing small droplets at high velocity can allow the method and apparatus of the subject invention to be used with heated surfaces 2 oriented in a variety of directions (e.g. vertical or horizontal) and can make it easier to provide coverage of the surface 2 with the spray coolant.
With high velocity spraying, a layer of coolant can form on surface 2 such that boiling occurs within the layer. As boiling occurs, bubbles will tend to grow causing the portion of surface 2 under the bubble to not be wetted. However, the constant bombardment of liquid spray droplets onto surface 2 can help displace the bubbles and prevent the bubbles from growing larger. In this way, a larger portion of surface 2 can be kept wetted so as to increase heat transfer. Spray patterns from atomizing spray nozzles in accordance with the subject invention can be, for example, round, square, rectangular (which can be referred to as a fan spray pattern), or other shape appropriate to the shape of surface 2 and/or the partition walls 21. Preferably, for each shape spray pattern, an even spray pattern is achieved by the atomizing spray nozzle.
The subject method and apparatus can be utilized as an open system where the coolant which is converted to gas or vapor upon spraying onto surface 2 can escape, for example, into the environment. In such an open system, the coolant which remains in liquid form can be collected and reused. If desired, the collected liquid coolant can be cooled before reuse, or spraying back onto surface 2. The subject method and apparatus can also be utilized as a closed system where at least a portion, and preferably essentially all, of the coolant which is converted to gas or vapor upon spraying onto surface 2, as well as the coolant which remains in liquid form, can be collected and reused. In a specific embodiment, the subject method can utilize a sealed housing, which can maintain a pressure different from the environment, to contain the coolant and collect and process the coolant.
Referring to
To condense the vapor and remove the heat acquired from the heat source, a condenser can be placed within the housing. The condenser can consist of a standard vapor to liquid heat exchanger with cold liquid supplied via a vapor compression cycle to the liquid ports of the heat exchanger. The warm vapor condenses on the heat exchanger, releasing its heat to the vapor compression cycle and flows into the reservoir.
A more efficient method of condensing the vapor and removing the heat involves adding another set of spray nozzles 56 to spray sub-cooled liquid coolant into the housing. A portion of the pressurized liquid from pump 9 can be sent to a heat exchanger 54 via tubing 52, rather than to manifold 30, to sub-cool a portion of the pressurized liquid coolant. Heat exchanger 54 can be, for example, a liquid-to-liquid heat exchanger cooled with liquid on one side of the exchanger. Liquid from a vapor compression cycle can be used for this purpose. If the saturation temperature of the housing 50 is above ambient, the heat exchanger 54 can be a vapor-to-liquid heat exchanger cooled by ambient air. The sub-cooled liquid coolant can then be directed to one or more pressure atomizer nozzles 56 and sprayed within the housing. The saturated vapor generated within the housing can contact the sub-cooled droplets. The saturated vapor can condense on the sub-cooled droplets to form larger droplets, which can flow into the reservoir to be reused in the process.
Referring to
Again referring to
The pressurized vapor used to power the one or more spray nozzles 5 can port directly back into the spray nozzle manifold. Depending on the nozzle used, the liquid from the reservoir 58 can either be pumped to the liquid port of the spray nozzle manifold or sucked through it via venturi action, for example through tubing 60. The second port from compressor 55 can discharge vapor at the desired pressure to complete the vapor compression cooling cycle. The superheated compressed vapor can then be channeled to condenser 75. Within the condenser, which can utilize, for example, an air, gas, or liquid heat exchanger, the high temperature compressed vapor can be cooled and condensed to a saturated liquid. The cooled saturated liquid can exit the condenser and be channeled to an expansion valve, turbine, or nozzle 95. The expansion valve, turbine, or nozzle can cause the pressure of the saturated liquid coolant to drop to the pressure and corresponding saturation temperature of the evaporator housing 50. The mixed quality liquid can then exit the expansion valve, turbine, or nozzle 95 and be channeled to the liquid reservoir 58 waiting to be reused. Using a turbine rather than an expansion valves would allow the recapture of the energy normally lost through the expansion valves. Using a nozzle can allow for direct spraying of the liquid coolant onto heat transfer surface 2 if, for example, a pressure atomizer nozzle is used. Alternatively, with respect to the embodiment shown in
The system described in this example can utilize the technique of spraying coolant onto a surface in order to transfer heat from the surface to the coolant and can also utilize the spraying of coolant onto a surface to transfer heat from the coolant to the surface. By spraying a first, hot, coolant onto a first surface of a dividing wall and a second coolant onto an opposite surface of the dividing wall, heat can be transferred from the first coolant to the second coolant. In this example, a housing with a dividing wall, two fluid spray nozzle assemblies and two fluid outlets can be utilized. The dividing wall in the housing separates the two flows in the heat exchanger. One fluid is sprayed on one side of the wall and the other is sprayed on the other side of the wall. The intense convection that develops from either the direct impingement and/or the evaporation for a two-phase flow design allows for a very small heat exchanger to exchange a considerable amount of heat.
Referring to
Heat can then be transferred between the fluids through wall 60. The convection heat transfer coefficient that is developed with both single phase and two-phase spray impingement is very high. This high coefficient allows the heat exchanger to be much more compact in size and efficient when compared to current heat exchanger technology. Wall 60 can be a flat surface or an engineered spray cooling surface such as a honeycomb or cubic chamber style surface, such as described in the subject application. Additionally, fins or other surface extension mechanism can be added to wall 60 to increase the effective surface area to increase the heat transfer through the wall 60.
The system described in this example can be utilized with various embodiments of the subject invention. Specific embodiments in accordance with the subject invention can comprise three main components: a compressor, a condenser, and a spray cooling expansion valve interface assembly. The cycle can begin with the compressor pulling in coolant vapor from the spray cooling assembly, and the coolant vapor being compressed to a temperature above ambient. The hot vapor can then flow through a heat exchanger to condense the vapor to liquid. The compressed hot liquid can be expanded through a nozzle and sprayed onto the spray cooling interface, or heated surface 2. Interface plate 3, as in the other embodiments of the subject invention, can be a separate plate in thermal contact with a heat source, or can be integral with a heat source, for example, a wall of a device producing heat which needs to be removed. A heat source, such as a laser diode or other heat exchange medium, attached on the other side of the interface can be cooled by the expanding and evaporating liquid. The liquid coolant can be vaporized as it removes the heat from the heat source via the interface. In embodiments where some of the coolant is not vaporized as it departs from the interface, an accumulator can be inserted between the coolant departing the interface and the compressor in order to reduce the amount, or prevent, liquid coolant from entering the compressor. A transfer pump can be used to transfer excess liquid from the accumulator to the liquid supply line to the nozzle.
Referring to
Under some operating conditions, excess liquid can be sprayed from the impingement nozzle 40 for enhanced heat transfer. In this case, accumulator 16, as shown in
This example describes a phase separator which can be utilized with subject spray impingement evaporator for vapor compression cycles in accordance with the subject invention. A spray impingement evaporator can be added to a vapor compression cycle to improve the heat transfer capabilities of the evaporator. The process can begin with a compressor taking in vapor from an accumulator. The compressed hot vapor exiting the compressor goes to a condenser to change the phase of the vapor to liquid. The liquid can then be expanded through an expansion valve. As liquid coolant is pumped from the accumulator to the phase separator, the liquid in the phase separator can be at a higher pressure than in the accumulator which receives vapor and liquid coolant from the impingement evaporator through, for example, tubing 75. The cooled liquid can then be used in a spray impingement evaporator. The spray can be achieved, for example, either through the use of another compressor, enlarging the existing compressor, and/or a utilizing liquid coolant pump.
The addition of the phase separator in this cycle in accordance with this example can allow the process to use at least a portion of the energy normally wasted in the expansion device to power the spray nozzles. The process enhancement can add the phase separator after the expansion valve. However, in this case the pressure drop across the expansion valve can be small. This allows a liquid vapor mixture at high pressure to collect in the phase separator. The high pressure fluid can then be used directly to power the spray nozzle in the spray impingement evaporator. Since the fluid is in both liquid and vapor phase, either a pressure atomizer or vapor atomizing nozzle can be used in the evaporator. A transfer pump may be used to transfer excess liquid from the accumulator to the phase separator.
Referring to
Referring to
The subject invention also relates to a heat transfer apparatus having an enhanced surface which can increase the rate of heat transfer from the surface to an impinging fluid. The subject enhanced surface can be incorporated with any of the heat transferred surfaces disclosed in the subject patent application or incorporated with other heat transfer surfaces. The subject invention also pertain to heat transfer apparatus, such as heat transfer plates, which incorporate the subject enhanced surfaces. The subject enhanced surfaces can also be utilized for heat desorbtion from a surface. In a specific embodiment, the subject system can comprise: a housing, a fluid pump or compressor, a nozzle array consisting of one or more nozzles, and a high heat flux source interface plate. The process begins with the housing. The housing contains the working fluid. The process as shown in
Evaporative spray cooling is enhanced by maintaining the thinnest liquid layer possible on the heat transfer surface. Pressure atomizer nozzles use high pressure liquid and vapor atomizer nozzles use compressed vapor to atomize the liquid coolant. Both types of nozzles can be used to produce a high velocity and lower droplet density spray. The result is a spray of liquid coolant onto the extended surface area which takes advantage of the additional surface area.
The pump 346 draws in the liquid coolant and pressurizes it to the desired pressure. The pressurized liquid goes to the liquid inlet port of spray nozzle 353. Compressor 350 draws in coolant vapor and pressurizes it to the desired pressure. The pressurized coolant vapor is sent to the vapor inlet port on spray nozzle 353. The compressed vapor and the pressurized liquid coolant combine in nozzle 353 to form small liquid droplets with a high velocity.
The spray nozzle 353 can be a vapor atomizer nozzle as shown using both compressed vapor and liquid coolant or a pressure atomizer nozzle, not shown, which uses only pressurized liquid.
The droplets impinge on cooling plate 360. Multiple surface area enhancements 370 are connected to cooling plate 360 as shown in
In a specific embodiment, protrusions, and/or indentations, having a height and/or depth, to diameter ratio of between about 0 to about 10 can be utilized. In further specific embodiments, a height, and/or depth, to diameter ratio of between about 1 and about 5 can be utilized. In another embodiment, protrusions, and/or indentations, having a height to spacing between adjacent protrusions, and/or indentations, ratio of between about 2 and 4 can be utilized. In a further embodiment, a height, and/or depth, to diameter ratio of about 3 can be utilized. In a specific embodiment, the number of protrusions, and/or indentations, density/spray cooling area is between about 1 and about 100 per square centimeter. In a further specific embodiment, the number of protrusions, and/or indentations, density/spray cooling area is between about 10 and about 20 per square centimeter. In a specific embodiment, the subject surface enhancements can increase the surface area, as compared to a smooth surface, by about 1 to about 5 times. In a further specific embodiment, the subject surface enhancements can increase the surface area by about 1.1 to about 2. In a specific embodiment, the center to center spacing of the subject protrusions, and/or indentations is between about (0.1) d and about 10d, where d is the diameter (or mean diameter) of the protrusions, and/or indentations. In a further specific embodiment, the center to center spacing is about d. In a specific embodiment, the roughness of the subject enhanced surface can have a RMS of between about optically smooth and about 100 micrometers.
The vapor coolant can then flow to a condenser, such as coil 342. The vapor condenses on the condenser coil 342 and forms liquid. The liquid then flows into reservoir 345. A heat extractors 341, removes the heat from the condenser 342 via thermal connection 340. The heat extraction can be a refrigeration cycle or an ambient heat exchanger.
A series of control devices including thermocouples, flow meters and level indicators are used to control the process in order to maintain the desired operating conditions.
All patents, patent applications, provisional applications, and publications referred to or cited herein are incorporated by reference in their entirety, including all figures and tables, to the extent they are not inconsistent with the explicit teachings of this specification
Sample and embodiments described herein are for illustrative purposes only and that various modifications or changes in light thereof will be suggested to persons skilled in the art and are to be included within the spirit and purview of this application and the scope of the appended claims.
This application is a continuation-in-part application of U.S. Ser. No. 10/115,510, filed Apr. 2, 2002, now U.S. Pat. No. 6,571,569, which claims the benefit of U.S. Ser. No. 60/350,857, filed Jan. 22, 2002; U.S. Ser. No. 60/350,871, filed Jan. 22, 2002; U.S. Ser. No. 60/350,687, filed Jan. 22, 2002; U.S. Ser. No. 60/290,368, filed May 12, 2001; U.S. Ser. No. 60/286,288, filed Apr. 26, 2001; U.S. Ser. No. 60/286,771, filed Apr. 26, 2001; and U.S. Ser. No. 60/286,289, filed Apr. 26, 2001. This application is also a continuation-in-part application of U.S. Ser. No. 10/342,669, filed Jan. 14, 2003, which claims the benefit of U.S. Ser. No. 60/398,244, filed Jul. 24, 2002.
Number | Name | Date | Kind |
---|---|---|---|
4068495 | Alger et al. | Jan 1978 | A |
4141224 | Alger et al. | Feb 1979 | A |
4306278 | Fulton et al. | Dec 1981 | A |
4413345 | Altman | Nov 1983 | A |
4444495 | Bramwell et al. | Apr 1984 | A |
4776181 | Maule | Oct 1988 | A |
4791634 | Miyake | Dec 1988 | A |
5105430 | Mundinger et al. | Apr 1992 | A |
5220804 | Tilton et al. | Jun 1993 | A |
5263536 | Hulburd et al. | Nov 1993 | A |
5353865 | Adiutori et al. | Oct 1994 | A |
5406807 | Ashiwake et al. | Apr 1995 | A |
5453641 | Mundinger et al. | Sep 1995 | A |
5471491 | Phillips et al. | Nov 1995 | A |
5526372 | Albrecht et al. | Jun 1996 | A |
5606201 | Lutz | Feb 1997 | A |
5687577 | Ballard et al. | Nov 1997 | A |
5718117 | McDunn et al. | Feb 1998 | A |
5768103 | Kobrinetz et al. | Jun 1998 | A |
5818692 | Denney, Jr. et al. | Oct 1998 | A |
5854092 | Root et al. | Dec 1998 | A |
5880931 | Tilton et al. | Mar 1999 | A |
5907473 | Przilas et al. | May 1999 | A |
5943211 | Havey et al. | Aug 1999 | A |
5992159 | Edwards et al. | Nov 1999 | A |
5999404 | Hileman | Dec 1999 | A |
6064572 | Remsburg | May 2000 | A |
6085833 | Kimura et al. | Jul 2000 | A |
6108201 | Tilton et al. | Aug 2000 | A |
6223814 | Moresco et al. | May 2001 | B1 |
6498725 | Cole et al. | Dec 2002 | B2 |
6542371 | Webb | Apr 2003 | B1 |
20010002541 | Patel et al. | Jun 2001 | A1 |
20040060313 | Tilton et al. | Apr 2004 | A1 |
Number | Date | Country |
---|---|---|
1 356 114 | Jun 1974 | GB |
62 119947 | Jun 1987 | JP |
Number | Date | Country | |
---|---|---|---|
20030226371 A1 | Dec 2003 | US |
Number | Date | Country | |
---|---|---|---|
60398244 | Jul 2002 | US | |
60350857 | Jan 2002 | US | |
60350871 | Jan 2002 | US | |
60350687 | Jan 2002 | US | |
60290368 | May 2001 | US | |
60286288 | Apr 2001 | US | |
60286771 | Apr 2001 | US | |
60286289 | Apr 2001 | US |
Number | Date | Country | |
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Parent | 10342669 | Jan 2003 | US |
Child | 10348850 | US | |
Parent | 10115510 | Apr 2002 | US |
Child | 10342669 | US |