An improvement in an absorption refrigeration and/or heating system including apparatus (157) to convert the pressure energy and/or phase change energy in the solution and/or refrigerant of the absorption system into mechanical energy, with additional apparatus to replace or supplement the externally supplied mechanical energy motive device (152) in the system with the converted mechanical energy. The system includes a first positive displacement pump (98) for conveying the absorbent solution from the absorber to the generator with first positive displacement apparatus (98) driven by a motive device (152) that is activated by the externally supplied energy. A second pump (158) is provided that is driven by the system pressure energy. Each of the pumping apparatus is being independently driven and connected to the other only by fluid connection.
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1. In an absorption refrigeration and/or heating system having components connected in series, including at least one generator, a condenser, an evaporator, and an absorber, wherein refrigerant is absorbed and desorbed or expelled in an absorbent solution, and the application of heat and externally supplied mechanical energy is combined and converted to pressure energy that is applied to, or removed, from a solution of refrigerant and absorbent, and having means to recover a portion of the pressure energy for addition to the mechanical energy, the improvement comprising:
(a) means to convert the pressure energy and/or phase change energy in the solution and/or refrigerant to mechanical energy, (b) means to replace or supplement the externally supplied mechanical energy in the system with the converted mechanical energy, (c) said system including first positive displacement pump means for conveying the absorbent solution from the absorber to the at least one generator means, with said first pump means driven by a motive means that is activated by the externally supplied mechanical energy, and (d) a second pump means driven and controlled by the system pressure energy, as determined by the first positive displacement pump means with each pumping means independently driven, and connected to the other, only by fluid connection means.
3. The system and improvement of
the outlet of the first pump means is in fluid connection with the inlet of the second pump means.
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This invention relates to a cooling and heating system which operates on the absorption and phase change heat exchange principle. More particularly it relates to a continuous heat actuated, air cooled, multiple effect generator cycle absorption system.
In further aspects, this invention relates to improvements to the system constructed for use with an absorption refrigeration solution pair comprising a nonvolatile absorbent and a highly volatile refrigerant which is highly soluble in the absorbent. A disclosed refrigerant pair is ammonia as the refrigerant and sodium thiocyanate as the absorbent.
The background of this invention is found in U.S. Pat. No. 4,646,541 (hereinafter the Prior Patent) which discloses the general subject matter of this invention. This invention therefore should be considered with reference to this Prior Patent which includes the common inventors F. Bert Cook and Edward A. Reid Jr. and is assigned to the same assignee as this invention.
U.S. Pat. Nos. 4,742,693, 4,719,767, 4,691,532, 4,742,687, and 4,722,193 are sibling patents of the Prior Patent and are pertinent to the disclosure of this invention providing further background information on this subject matter.
In the quest for improvement in Absorption Refrigeration and Heat Pump Systems, the common measure of performance is the often referred to "coefficient of performance", i.e., COP. As used herein, coefficient of performance, i.e. COP is defined as the energy transferred at the load in a unit of time divided by the energy provided to the system in the same unit of time which is well understood by those skilled in the art. Other measures of performance include reduction in complexity; or stated conversely, apparatus and system simplification.
Absorption systems are usually very efficient during the heating cycle, when a source of heat, such as a natural gas flame is used. On the other hand, these systems are less efficient in the cooling cycle.
Air cooled refrigeration circuits of the mechanical vapor compression type have also been demonstrated which can be reversed to provide either heating or cooling to a load by switching the flow of an intermediate heat transfer solution typically consisting of water and antifreeze solutions such as ethylene glycol, etc.
Liquid cooled absorption refrigeration circuits using the double effect generator cycle to achieve high efficiency are commercially available. However, these systems using water as the refrigerant are not suitable for use in heating a conditioned space (the heating load) since the refrigerant freezes at 32° F. and therefore cannot be used in a space heating system at ambient outside temperatures below approximately 40° F.
Absorption refrigeration and heat pump systems are well known in their basic operating characteristics and need little further description except to establish the definitions and context in which this invention will be later described.
In a typical system a refrigerant water or other phase change material is dissolved in an absorbent (typically lithium bromide or other salts) and these are often called the "solution pair". The refrigerant is absorbed or desorbed (expelled) in or out of solution with the absorbent to varying degrees throughout the system and the heat of absorption is added or extracted to produce heating and cooling effects.
The solution pair enters a generator where it is subjected to heat and the applied heat desorbs (expels) a portion of the refrigerant in the form of a vapor which is conveyed to the condenser. There, external cooling condenses the refrigerant vapor to liquid, which is conveyed through an expansion valve, into an evaporator where heat is gained. In the refrigeration system operation the heat gained in the evaporator is from the cooling load.
The low pressure vapor then passes to an absorber where cooling allows the absorbent solution to absorb the refrigerant vapor. The solution is then conveyed to a recuperator by a pump. The recuperator is a counter-flow heat exchanger where heat from the absorbent/refrigerant solution flowing from the generator to the absorber, heats the returning solution pair flowing from the absorber to the generator. In the heating cycle, the cooling applied at the absorber and/or the condenser is the heat delivered to the heating load.
As a matter of convenience and terminology herein, each part of the absorption system which operates at the same pressure is termed a chamber.
Conventional absorption refrigeration/heating systems are two chamber systems although three chamber systems appear in the prior art and have seen limited use. When operated as heat pumps two chamber systems give respectable heating performance but give poor cooling performance.
Using ammonia (NH3) as the refrigerant and water (H2 O) as the sorbent, heat pumping can occur from an ambient air source which is at temperatures below freezing. Where the air is treated as if it were dry so that no defrosting is necessary, the typical two chamber NH3 /H2 O heat pump would represent a significant improvement over what would be expected of a simple furnace. However, since heat pumps are more expensive than furnaces, cooling season performance benefits are needed to justify the added expense. In other words, the heat pump must act as an air conditioner also to offset the additional cost of the heat pump combined with separate installation of an air conditioner with a furnace.
For cooling, an NH3 /H2 O system is predicted to have a COP equal to about 0.5. This low performance index causes unreasonable fuel (or energy) costs from excessive fuel (or energy) use.
Three-chamber systems of various types have been suggested which would improve the performance by staging the desorption process into effects. This allows for increasing the actual temperature at which the driving heat is added to the system (cycle). Until the invention of U.S. Pat. No. 4,646,541 it was thought that this increase in temperature would represent an unreasonably high pressure, especially from ammonia/water systems, and would force the system to operate in regions for which data is not readily available.
In addition the pressure has tended to rule out ammonia/water in a three-chamber system. The search for organic materials such as halogenated hydrocarbons and other refrigerants as a replacement for the ammonia has been limited by fluid stability at these higher temperatures. separator 91 second generator 81 through an expansion valve of energy recovery motor or expansion valve 105, and through a condenser 100 by way of a connection 94. Additional refrigerant vapor 82 from separator 91 92 is conveyed to the condenser 100 through the connection 94.
From the condenser 100 liquid refrigerant 82 is conveyed through a third recuperator 107, to an evaporator 115, by way of an expansion valve 110.
Cool low pressure refrigerant is returned from the evaporator 115 through the recuperator 107, exchanging heat with the warm liquid refrigerant 82, and passing to an accumulator 205.
In the accumulator 205, excess refrigerant 82 is collected which may have occurred as a result of changes in the amount of refrigerant contained in the condenser 100 and evaporator 115 because of their operation at different conditions, especially differences between cooling, heating, and defrost modes of operation. By this arrangement, the system refrigerant concentration may ideally be controlled between about 46% and about 32%.
From the accumulator 205 refrigerant joins the weak solution 89 at the connection 93. From the connection 93 the combined weak solution and refrigerant pass through the absorber 97 to a purge pot 99 thence to the inlet of a solution pump 98. By this process weak solution 89 absorbs vaporous refrigerant 82 becoming a strong solution 83 in the absorber 97, and is pumped by a solution pump 98 back to the first generator means 80, passing successively through recuperators 95 and 86.
This improvement invention includes a separate hydronic subsystem through which a working fluid is conveyed among the various components of the double effect absorption refrigeration system, and between the load and heat source or sink.
Referring again to FIG. 1, the subsystem is depicted as a single fine line, which is connected to the inlet 113 of the condenser 100 and passes through to a first four-way fluid valve 101 which is set to continue the flow to the inlet 103 of the absorber 97. After passing through the absorber 97, the fluid is conveyed from an outlet 104 to a second four-way valve 106, and fed to an inlet of a first outdoor heat exchanger 108. From the first heat exchanger 108 the working fluid is conveyed through a pump 109 to a third four-way valve 112 which has been positioned to return the working fluid to an inlet 113 of the condenser 100. By means of these connections, the heat of condensation and absorption of the hot refrigerant 82 is exchanged to the working fluid in the condenser 100 and absorber 97 which transfer the heat through the working fluid to the ambient outside air by heat exchange in the first heat exchanger 108. A fan 114 induces air flow across the first heat exchanger 108 increasing the rate of heat exchange to the outside ambient air.
In this cooling mode operation, the outlet 104 of the absorber 97 is connected from a joinder 116 through the first four-way valve 101 to the inlet 118 of the evaporator 115 at a joinder 117. No flow takes place between the joinders 116 and 117 in this mode, because there is no differential pressure in the working fluid between these two points and there is no return path. Therefore, flow cannot occur.
In this mode of operation, the working fluid is conveyed from an inlet 118 through the evaporator 115 to an outlet 119. From the outlet 119 of the evaporator 115, the working fluid is conveyed to four-way valve 106 and thence to the indoor second heat exchanger 121, via valve 106 121 where air from the conditioned space passes in heat exchange relationship with the working fluid. A fan 122 induces air flow across the coils of heat exchanger 121.
From the indoor heat exchanger 121, the working fluid is conveyed by a pump 123 past the joinder 117 and through the third valve 112 to the inlet 118 of the evaporator 115.
In this mode of operation the working fluid is cooled as it passes in heat exchange relationship with the cooled refrigerant in the evaporator 115. The cooled working fluid transfers this cooling to the indoor conditioned air in the second indoor heat exchanger 121.
Referring to FIG. 2, the double effect generator absorption system and operation remains the same for the heat pumping mode. However in this heating mode, the working fluid subsystem is switched by means of changes in the position of four-way valves 106 and 112. The four-way valve 101 remains in the previous position as shown for the cooling mode of FIG. 1.
In this arrangement the hot working fluid from the condenser 100 is conveyed through outlet 102 and four-way valve 101 to the inlet 103 of the absorber 97. The subsystem provides cooling to the absorber because the combined refrigerant and weak solution are at higher temperature, so that the necessary absorption process takes place in the absorption refrigeration system. The working fluid is heated further thereby and leaves the absorber 97 by way of outlet 104 to the four-way valve 106 which is reversed from the previous cooling mode of operation. The working fluid now passes to the second heat exchanger 121 where it exchanges heat with the conditioned air of the living space (the load). Being cooled from the air in the living space, pump 123 directs the working fluid back through valve 112 to the inlet 113 of the condenser 100.
In this normal heating mode position of the four-way valves 106 and 112, the working fluid is conveyed from the evaporator 115 through the outdoor heat exchanger 108 where it receives heat from the outdoor air before returning to the evaporator inlet 118. The fan 114 may be operated intermittently depending on the outdoor air temperature and humidity conditions to reduce frost build up on the heat exchange surfaces. When the subsystem valves 106 and 112 are operating in this position, heat pumping occurs from the outside air to the evaporator raising the temperature of operation of the subsystem providing for a theoretical COP of higher than 1∅
It will be seen that in comparison to the system described in the Prior Patent, simplification and important reductions in first costs and operating reliability have been achieved.
When the system is operating in the heating mode the first outdoor heat exchanger 108 is in communication with the evaporator and is absorbing heat from the surrounding outside ambient air environment. Under certain conditions of outside temperature and humidity the exterior surface of heat exchanger 108 will accumulate frost from the moisture in the surrounding atmosphere. An accumulation of frost on the surfaces of the outdoor heat exchanger 108 reduces its heat exchange efficiency hindering heat pumping operation and reducing the overall system performance. Various solutions have been proposed and are used in prior practices to overcome this problem, such prior systems are inconvenient and draw down the COP of the unit by the requirement of additional heat energy, such as by electrical resistance or the requirement for an auxiliary boiler.
However, in the operation of the system of this invention, defrosting is accomplished when four-way valves 112 and 101 are reversed and four-way valve 106 remains as positioned for the heating mode. Air flow across the second first heat exchanger 108 is interrupted by shutting off the fan 114. The warm working fluid from the condenser is directed through the heat exchanger 108 melting the frost. Heat from the absorber continues to be directed through the second indoor heat exchanger 121 providing heat to the conditioned space although temporarily at a reduced rate for a short time. It is a feature of this invention that heat continues to flow to the load from the absorber 97 during the defrost cycle. In the conventional arrangements that have been provided to answer the frosting problem of air transfer heat pumps, it is a practice to cut off the heat pump completely and use electrical resistance heaters to provide heating during defrosting. This invention to the contrary, maintains heat flow from the heat pump during defrosting and in most circumstances defrosting can be completed before heat is required in excess of that available during defrost operation. At the end of the defrost cycle, all the working fluid reversing valves are returned to their normal heating mode position, and the air flow over the first heat exchanger 108 is restored.
Conventional controls are provided to sense the loss of efficiency resulting from frost build-up and the defrost cycle is operated automatically.
As an alternative, the working fluid from the absorber 97 may be passed through a heat exchanger relationship with a storage tank for domestic hot water when all the heat of the absorber means is not needed at the load, for instance when the outside ambient air is not cold or the system is operating in the cooling mode.
As shown in FIG. 13, a domestic hot water heater and tank 370 is located within the residence to which the heat pump system of this invention is installed. The outlet 104 of the absorber 97 is connected to an inlet 371 of a heat exchange coil 372 in the hot water heater 370. An outlet of coil 372 is connected to the inlet of the absorber 97. A second source of heat 375 such as a gas burner is also provided to the hot water tank 370.
This domestic hot water heating subsystem is included in combination to take advantage of the excess heat available at the absorber under circumstances where the full heating capacity of the system is not required for the ambient conditions being serviced by the load. Such excess heat may be available in either the cooling mode or heating modes mode when the system is not loaded to its designed capacity. In those circumstances when the system is not operating or there is no excess heat available at the absorber 97, the auxiliary burner may be operated to assure that there is the required domestic hot water available.
A configuration for a living space, residential air conditioning and heating embodiment of this invention is shown in FIGS. 5 and 6, in which an air conditioning and heat unit 165 is located outside a residence and constructed in rectangular format on a base 167, and includes a housing 166. The housing 166 includes an upper aperture 169. The aperture is positioned above an ambient air inductive means such as the fan 114 (See FIG. 1). The generator/recuperator means 220 is located below aperture 169. The first heat exchanger 108 comprises three sides of the unit 165. Conveniently positioned as shown on the fourth side, are the solution pump 98, purge pot 99, evaporator 115, condenser 100, absorber 97, and recuperator 105 107. The separators 91 and 92 (as shown in FIG. 8 in longitudinally vertical position) are positioned nearby. Pumps 123 and 109 for conveying the working fluid are juxtaposed to the solution pumps 98 and 157. The second heat exchanger 121 and the fan 122 are located within the living space.
Referring to FIGS. 5, 6, and 7, an embodiment of a double effect generator/recuperator means 220 is shown as apparatus which integrates in one interrelated assembly the various components and modules that are associated with the use of the heat generated in a heat source 84. To facilitate understanding, numerical designations are the same as and refer to like components in the system shown in FIG. 1.
Generator Module
As shown in FIG. 7, a generator unit or module 220 is generally symmetrically constructed about a substantial vertical central axis. Generator module 220 includes a generator housing 221 that may be circular in the plan view (FIG. 6) and which is constructed on a generator frame base 222 that may be the same or distinct from the base 167 of the heating and air conditioning unit 165 165 (FIGS. 5 and 6). Generator unit 220 contains a circular floor 230 attached to the generator housing 221 above the generator base 222 so as to contain insulating material 231. Generator floor 230 slopes gently from the center to the generator housing 221 so as to allow for the drainage of condensed moisture from the unit.
The generator housing 221 includes an upper generator shroud 223 and a generator ceiling 224 between which is placed insulating material 225. A cylindrical passage 226 is formed by a cylinder 227 joining the center portion of the shroud 223 and the center portion of the generator ceiling 224. A cylinder cap 228 seals the cylinder 227 from the surrounding atmosphere and provides a mounting surface to which generator blower 229 is attached. Cylinder cap 228 contains an aperture (not shown) that allows air from the blower 229 to enter the generator unit 220 through cylindrical passage 226.
A central driving heat source 84 providing external heat to the system, typically a gas burner, is centrally positioned substantially on a central axis 232 of unit 220. A gas source is not shown but it is to be understood to be of conventional piping design. Annular components surround the circular heat source 84 and include a first generator means (desorber means) 80, a first (high-temperature) recuperator means 86, a second generator means 81, and a second (low-temperature) recuperator means 95. Each component is constructed as a plurality of coils, juxtaposed one to the next, in a substantially or generally annular composite form i.e., vertically positioned toruses or helices. Components are juxtaposed one to the next, and radially more or less distant from the central axis 232, i.e., surrounding the source of heat 84 at varying distances. The generator 80 coils having fine fins that allow for the passage of hot gases between and among the coils so as to achieve maximum heat transfer. See, for example FIG. 5 item 200 of U.S. Pat. No. 4,742,693 which is herein incorporated by reference. First and second recuperators and the second generator have coils with a solid exterior surface that are wound in contact with each other.
The recuperators, 86 and 95, and second generator 81, have an inner tube and an outer tube arranged in what is often referred to as tube-in-tube construction. Preferably the inner tubes have helical flutes 233 to better effect heat transfer between the fluids in the inner and outer tubes. Fluted tubes are available commercially from suppliers such as Turbotec Products, Inc., Windsor, Conn., and Delta-T Limited, Tulsa, Okla. The liquid-liquid heat exchangers and absorbers have three flutes. Evaporators and condensers have four flutes and about three times as many flutes per foot. That is, not only do the evaporators and condensers have more flutes but they also are twisted more revolutions per foot.
Tubing materials are conventional, being chosen for good heat transfer through the walls of the tubing and corrosion resistance. Metals such as stainless steel and low alloy steels such as AISI 9260 and AISI 1075 are suitable. Generator 80 is typically of conventional single tube construction with small, fine fins.
In the preferred embodiment shown in FIG. 7, high-temperature air and combustion products (flue gas) 245 are generated in a first generator chamber and impinge upon the walls 131 of the tubular generator 80 being driven more or less downward and radially outward direction through the fins between the coils of generator 80 by blower 229. The hot combustion products 245 emerge through apertures 235 in cylindrical baffle 234 and flow downward along the solid inner cylindrical first recuperator housing baffle 236 where they emerge through apertures 238 in the bottom of inner recuperator housing 236.
The hot air and combustion products 245 then enter a second (recuperator) chamber 237 surrounding the first generator chamber through aperture 238 268 in the bottom housing 250 of the first recuperator chamber 237. The hot air and combustion products 245 impinge upon the coils of tube 249 of the first recuperator 86 while flowing in a generally upward direction. The warm combustion products and air 245 emerge into a third or outer chamber 240 of the generator unit from the second chamber 237 through apertures 312 located in the top portion of the outer recuperator housing 239. The warm combustion products and air 245 impinge upon the coils of tube 252 of the second generator 81 and the coils of tube 260 of the second recuperator 95 while flowing in a generally downward direction. Combustion products and air 245 emerge from the generator unit 220 through apertures 241 in the generator housing 221 located just above the generator floor 230.
The generator, recuperator, and other chambers are concentric cylindrical chambers juxtaposed one to the next. The general flow of combustion products and air is indicated by arrows in FIG. 7 as being generally in a serpentine fashion, i.e. downward in the first chamber, upward in the second chamber, and downward in the third chamber.
The first generator means 80 is made from a finned double-wound helical coil of tubing. Strong solution 83 enters the first generator 80 from the first (high temperature) recuperator 86 through inlet 137 at a temperature of about 385° F. and a pressure of 1480 1490 psia. The strong solution 83 is heated by the heat source 84 as it flows downward through the outer winding of helical coil and then upward through the inner winding of the helical coil emerging from the first generator means 80 through outlet 138 at a temperature of about 415° F. The strong solution 83 receives direct heat from the heat source 84 at a rate of about 36,000 btu/hr.
As shown in FIGS. 1 and 8, the heated strong solution 83 then enters the first (primary) separator 91 through separator inlet 242 where it separates into intermediate solution 85 and refrigerant vapor 82. The intermediate solution 85 leaves separator 91 through lower outlet 243. The refrigerant vapor 82 leaves separator 91 through upper outlet 244.
Returning to FIG. 7, the intermediate solution 85 enters the first recuperator 86 through inner fluted-tube inlet 246. First recuperator 86 consists of three rows of a fluted tube-in-tube helical windings located radially outwardly adjacent to first generator 80 and extending vertically for almost the length of the first generator 80. The first recuperator 86 is contained in the cylindrical first recuperator chamber 237 that is formed by inner cylindrical baffle 236, outer cylindrical recuperator housing 239, the generator unit ceiling 224 and first recuperator housing bottom 250. As the intermediate solution 85 passes through the fluted inner tube 248 of recuperator 86, it exchanges heat to the strong solution 83 in the outer tube 249 of the recuperator 86 at a rate of about 69,000 btu/hr and leaves through the inner tube outlet 247 at a temperature of 245° F. and a pressure of 1450 psia. Intermediate solution 85 is then throttled substantially isenthalpically through valve 87 (FIG. and arrives at the secondary generator 81 at a temperature of 245° F. and a pressure of 290 psia.
The intermediate solution 85 enters the second generator means 81 through outer tube inlet 251. The second generator 81 consists of two rows of fluted tube-in-tube helical windings located radially outwardly adjacent to firs recuperator 86 and extending vertically along the top portion of the first recuperator 86. The second generator 81 is contained in the upper portion of the cylindrical outer-most generator-unit chamber 240 that is formed by the outer cylindrical first recuperator housing 239, the generator unit housing 221, the generator unit ceiling 224 and the generator unit floor 230. As the intermediate solution 85 passes through the outer tube 252, approximately 18,000 btu/hr is transferred to it from the condensing refrigerant vapor 82 in the inner fluted tube 253. About an additional 1,000 btu/hr is transferred to the intermediate solution 85 in the outer tube 252 from the circulating flue gases 245. The intermediate solution 85 leaves the second generator 81 through second generator outer tube outlet 254 at a temperature of 255° F. and a pressure of 290 psia.
As shown in FIGS. 1 and 8, the heated intermediate solution 85 then enters the second (secondary) separator 92 through separator inlet 255 where it separates into weak solution 89 and refrigerant vapor 82. The weak solution 89 leaves separator 92 through lower outlet 256. The refrigerant vapor 82 leaves separator 92 through upper outlet 257.
Weak solution 89 leaves the separator 92 at a pressure of 290 psia and a temperature 255° F. and enters the second recuperator 95 through second recuperator inner fluted-tube inlet 258. The second recuperator 95 consists of two rows of fluted tube-in-tube helical windings located radially outwardly adjacent to first recuperator 86 and extending vertically along the lower-upper and lower portions of the first recuperator 86. The second recuperator 95 is contained in the lower upper and lower portions of the cylindrical outer-most generator-unit chamber 240 that is formed by the outer first recuperator housing 239, the generator unit housing 221, the generator unit ceiling 224 and the generator unit floor 230. As the weak solution 89 passes through the fluted inner tube 259 of the second recuperator 95, it transfers approximately 50,000 btu/hr to the strong solution 83 in outer tube 260 as the strong solution 83 is on its way to the first recuperator 86. The weak solution leaves the second recuperator 95 through the inner fluted-tube outlet 261 and is then throttled substantially isenthalpically through valve 96 (FIG. 1) and arrives at connection 93 at a temperature of 120° F. and a pressure of 70 psia.
High pressure vapor 82 from the upper outlet 244 of separator 91 enters the second generator 81 through inner fluted-tube inlet 262 at a temperature of 415° F. and pressure of 1480 psia. While circulating through fluted inner tube 253, the vapor is condensed liberating approximately 18,000 btu/hr to the intermediate solution 85 in outer tube 252. The condensed vapor 82 leaves the second generator 81 through inner fluted-tube outlet 263 at a temperature of about 260° F. Passage of the condensed vapor 82 through expansion valve 110 105 (FIG. 1) reduces its temperature to 120° F. and its pressure to 290 psia. The expanded vapor 82 is joined with the vapor 82 from the secondary separator 92 at connection 94 94 (FIG. 1).
After the vapor 82 is absorbed into the weak solution 89 in the absorber 97 and the resulting strong solution 83 passes through the purge pot 99 and pump 98, it enters the secondary recuperator 95 at a temperature of 120° F. and a pressure of 1550 psia through outer tube inlet 264. While circulating through the outer tube 260, the strong solution receives 50,000 btu/hr from the weak solution 89 in the inner fluid tube 259 and an additional 1,000 btu/hr from the circulating flue gases 245. On leaving the secondary recuperator 95 through outer tube outlet 265, the strong solution 83 is at a temperature of 230° F. and a pressure of 1520 psia.
From the secondary recuperator 95, the strong solution enters the primary recuperator 86 through outer tube inlet 266. While circulating through the outer tube 249, the strong solution 83 receives 69,000 btu/hr from the intermediate solution 85 circulating in the fluted inner tube 248 and an additional 1000 btu/hr from the circulating flue gases 245. The strong solution 83 leaves the primary recuperator 86 through outer tube outlet 267 at a temperature of 385° F. and a pressure of 1490 psia.
Although the preferred embodiment is shown and described, other arrangements may be suitable for different operating conditions. For example, the solutions within fluted tubes and that in the annulus may be switched one for the other, especially in the low temperature recuperator 95 where it might be preferable not to have the higher pressure fluid in the annulus.
Absorber and Condenser Module
Referring to FIG. 9, an integrated absorber/condenser module provides for the assembly of condenser 100 and absorber 97 components that are schematically shown in FIGS. 1-3. The absorber/condenser module integrates in one interrelated assembly the various components of the apparatus that are associated with the use of the heat generated in the driving heat source 84 for heating, cooling and defrosting.
It is to be noted that the primary (refrigerant) system, using preferably an ammonia/sodium thiocyanate refrigerant pair, is completely contained in the outside heating and air conditioning unit 165 and operates in continuous fashion without the switching of flows among the various components. The working subsystem, using preferably a water/glycol working fluid, transfers heat among the load (inside space), ambient outside air, and outside heat exchanger depending on whether the system is operating in a heating, cooling or defrosting mode.
Heat exchange between the refrigerant system and the hydronic working fluid subsystem occurs in the absorber/condenser module 270 and specifically in the absorber 97 and the condenser 100. The absorber/condenser module consists of an absorber 97, a purge pot 99, a condenser 100 and a third (tertiary) recuperator means 107. The condenser 100 and the tertiary recuperator 107 are is preferably fluted tube-in-tube construction. The absorber 97 as and condenser 100 are of fluted tube-in-cylinder construction.
The purge pot 99 is centrally positioned substantially on a central axis 271 of the annular components including the absorber 97, condenser 100 and the third recuperator 107. Each component is constructed as a substantially annular coil, or coils and/or plurality of vertically positioned toruses or helical tubings. The absorber 97 and the third recuperator 107 are juxtaposed to the condenser and are radially more distant from the central axis 271.
The absorber/condenser module 270 is contained in cylindrical housing 278 with a bottom 279 and top 280. Insulation 281 is provided between the cylindrical housing 278 and the outer most components.
The absorber 97 consists of two windings of fluted tube enclosed in a cylindrical space 276 formed by outer cylindrical absorber 284, outer condenser wall 285, absorber bottom 286 and absorber top 287. The inner and outer windings are separated by cylindrical baffle 289. Baffle 289 is attached to absorber top 287. Generally a winding may be considered as a plurality of coils juxtaposed one to the next in a generally annular composite form, i.e., a cylindrical helix.
Weak solution and refrigerant mixture enter the outer winding of fluted tube 288 at the top of the absorber, flow generally downward and then generally upward in the inner winding, i.e. in directions generally parallel to the axis of the absorption coils. Working fluid 275 enters cylindrical space 276 through inlet 103 and circulates generally downward and through and among the spaces formed by the juxtaposed fluted-tube outer windings. The working fluid 275 passes beneath the lower edge of baffle 289 and then circulates generally up and through and among the spaces formed by the juxtaposed fluted-tube inner windings. The working fluid leaves absorber 97 through outlet 104.
Weak solution 89 meets the refrigerant 82 at connection 93 and enters the absorber 97 through fluted inner-tube inlet 272 at a temperature of about 144° F. and a pressure of about 70 psia. The refrigerant 82 is absorbed into the weak solution 89 with release of an absorption heat of 52,000 btu/hr to the working fluid 275 circulating in cylindrical space 276. Strong solution 83 leaves the absorber 97 through fluted inner-tube outlet 277 at a temperature of about 118° F. and a pressure of about 70 psia.
After leaving absorber 97, strong solution 83 enters purge pot 99 through inlet 282 and exits the purge pot through outlet 283. The purge pot is used to periodically remove periodically non-condensable gases formed in the system through the vent line 310 and valve 311.
Preferably, the condenser 100 comprises a single winding of fluted tube 293 i.e., a plurality of coils juxtaposed one to the next in generally annular composite form, extending the vertical length of the absorber/condenser unit 270 and enclosed in the cylindrical condenser space 290 formed by inner cylindrical condenser wall 291, outer cylindrical condenser wall 285, absorber/condenser top 287 and condenser bottom 292 i.e., tube-in-cylinder construction. Although less preferred, tube-in-tube construction my may also be used. If tube-in-tube construction is used, the working fluid preferably circulates in the outer tube.
Hydronic working fluid enters the condenser space 290 through inlet 102 113, circulates around and through the spaces formed by the juxtaposed coils of fluted tube 293 in a direction generally parallel to center line 271 (in cross flow to the flow of vapor 82 in tube 293) and leaves through outlet 113 102. Refrigerant vapor 82 enters the condenser 100 through inlet 294 at a temperature of 120° F. and pressure of 290 psia. Vapor 82 condenses in fluted tube 293 transferring a condensation heat of 27,000 btu/hr to hydronic working fluid 275 circulating in condenser cylindrical space 290. Condensed refrigerant vapor 82 leaves the condenser through outlet 295 at a temperature of 100° F. and a pressure of 290 psia.
The third (tertiary) recuperator means 107 is a single fluted tube-in-tube winding juxtaposed radially outward from condenser 100. Condensed vapor 82 from condenser outlet 295 enters the tertiary recuperator 107 through fluted-tube inlet 296 and circulates through inner fluted tube 297 where it transfers 610 btu/hr to vapor 82 in the outer tube 298. Condensed vapor 82 leaves tertiary recuperator 107 through fluted-tube outlet 299 at a temperature of 90° F. and a pressure of 285 psia.
As shown in FIG. 4, evaporator 115 is a cylindrical unit with a cylindrical outer housing 300, a cylindrical inner housing 301, a top 303 and a bottom 304 forming cylindrical space 302. An annular winding of fluted tube 305 is contained in cylindrical space 302. Hydronic working fluid 275 enters the evaporator 115 through inlet 118 and circulates generally downward over, through and among the spaces formed from the juxtaposed windings of fluted tube 305. The hydronic fluid 275 leaves the bottom of evaporator 115 through outlet 119.
After leaving the tertiary recuperator 107, condensed vapor 82 passes through expansion value 110 after which it enters evaporator 115 at a pressure of 72 psia and a temperature of about 39° F. through evaporator inlet 307 306. The condensed vapor 82 evaporates in fluted tube 305 absorbing 36,000 btu/hr from the circulating hydronic working fluid in evaporator cylindrical space 302. The evaporated vapor 82 leaves evaporator 115 through outlet 306 307 at a temperature of about 53° F. and a pressure of about 72 psia.
After leaving the evaporator, the refrigerant vapor 82 enters the tertiary recuperator 107 through outer tube inlet 308, circulates through outer tube 298 receiving 610 btu/hr from the condensed vapor 82 in inner fluted tube 297, and leaving by outer tube outlet 309 at a temperature of about 67° F. and a pressure of about 71 psia. After leaving the tertiary recuperator, vapor 82 enters accumulator 205.
As shown in FIG. 4, evaporator 115 is a cylindrical unit with a cylindrical outer housing 300, a cylindrical inner housing 301, a top 303 and a bottom 304 forming cylindrical space 302. An annular winding of fluted tube 305 is contained in cylindrical space 302. Hydronic working fluid 275 enters the evaporator 115 through inlet 118 and circulates generally downward over, through and among the spaces formed from the juxtaposed windings of fluted tube 305. The hydronic fluid 275 leaves the bottom of evaporator 115 through outlet 119.
Although the preferred embodiment is shown and described, other arrangements may be suitable for different operating conditions. For example, the solutions within fluted tubes and that in the annulus may be switched one for the outer, especially in the low temperature recuperator 95 where it might be preferable not to have the higher pressure fluid in the annulus. The third recuperator 07 107 could also be mounted on the outside of the evaporator coil 115 in a fashion similar to the way it is shown as on the outside of the condenser 100. The purge pot 99 need not be inside the absorber/condenser. The chosen location however does conserve space. An expansion tank to allow for expansion and contraction of the heat transfer fluid (ethylene glycol/water) could similarly be placed inside the evaporator.
| ______________________________________ |
| HYDRONIC WORKING FLUID TEMPERATURES |
| INLET OUTLET |
| ______________________________________ |
| Condenser 105° F. |
| 110° F. |
| Absorber 110 120 |
| Evaporator 55 45 |
| Outdoor Heat Exchanger |
| Heating Mode 40 45 |
| Cooling Mode 120 105 |
| Indoor Heat Exchanger |
| Heating Mode 120 105 |
| Cooling Mode 45 55 |
| ______________________________________ |
In the operation of the absorption refrigeration system of this invention a mechanical energy input is necessary in addition to the thermal energy input. The necessary mechanical energy is primarily required for operation of the solution pump which circulates the solution pair through the system. In FIGS. 1, 2, and 3 the solution pump 98 is shown conveying the strong solution from the absorber 97 to the first generator means 80 by way of the second and first recuperators 95 and 86 respectively. In a system capacity of 36,000 BTU per hour, the mechanical energy required to raise the solution pressure to about 1200 PSIA is approximately 670 watts. Providing this mechanical energy using a convention electric motor and pump would require consumption of approximately 1200 watts of electrical power which would reduce the refrigeration cycle efficiency (COP) by approximately 11%. The Prior Patent describes an energy recovery system for recovering energy from the isenthalpic throttling valves required for the system.
In this invention, an alternate energy recovery system has been further refined as shown in FIGS. 10 and 11.
In FIG. 10, one embodiment of the improved energy recovery apparatus includes rotary motor means 152 driving a positive displacement solution pump means (which may be either rotary or reciprocating) 98 receiving strong solution from the purge pot 99. The solution pump 98 raises the strong solution to an intermediate pressure and conveys the solution to a second higher pressure solution pump 157, where the pressure is raised to the high pressure requirements of the system before conveying the strong solution through recuperators 95 and 86 to the first generator 80.
The second pump 157 may be located between low temperature recuperator 95 and high temperature recuperator 86, (shown in phamton 370). phantom in FIG. 1 as 157'). In that way both the pump 158 157 and motor(s) 157, 158 158 and 159 would all be at more nearly equal temperatures. Also, both pipes of the low temperature recuperator 95 would be at more nearly equal pressures--significantly lower than the primary generator pressure.
The solution pump 157 is driven by energy recovery means 158 and, alternatively, also by additional energy recovery means 159.
Solution pump 98 is preferably an electric motor driven pump of conventional design. Solution pump 157 may be either a rotary pump or a reciprocating pump more suitable for high pressure service, being driven by reciprocating expansion devices operating through the pressure let down of the expansion means 87 and 105.
In the construction according to FIG. 10, the energy recovery motors are not mechanically connected to the shaft of the motor 152 providing more flexibility in the operation of the solution pump and energy recovery arrangements than in the embodiment of the Prior Patent where the opposite direct connection was provided. Although the pressures generated in the pumps 98 and 157 are additive to produce a sum pressure at the generator 80, each pump is operating independently under the influence of an independent motive system.
In FIG. 11, the motor 152' drives a solution pump 98'. The second solution pump 157' 157" is driven in reciprocating motion by an energy recovery device 158' connected to the pressure expansion valve 87. In this alternative embodiment the strong solution enters the pumps 98' and 157' 157" at the same suction pressure. However, on the discharge side, the outlets from the pumps are combined at the same pressure. The flow to the generator 80 is the sum of the two flows.
In either the embodiment of FIG. 10 or the embodiment of FIG. 11 sufficient energy recovery is provided to contribute significantly to the increase the COP to a range of about 0.8 in cooling mode.
Referring to FIG. 12, an energy recovery motor combining components 157 and 158 is shown as energy recovery means 350. Unit 350 is fed by solution pump 98. The output of solution pump 98 is divided and passes through check valve means 351 and 352 to opposite ends of the reciprocating piston pump 350 comprising a cylinder 353 centrally divided into chambers 354 and 355 by opposite ends of a reciprocating piston 356. Piston 356 divides the chambers 354 and 355 into second chambers 357 and 358 respectively. Chambers 354 and 355 are provided with outlets through check valve means 360 and 361 respectively. Check valve means are connected together to provide a connection to the first primary generator means 80.
Solution 85 at high pressure is provided to the second chambers 357 and 358 respectively through control valves 362 and 363 respectively. Solution leaves the chambers 357 and 358 through control valve 364 and 365 to the secondary generator 81. The control valves 362, 363, 364 and 365 operate to time the admission of high pressure solution to the chambers 357 and 358 and cause the piston 356 to reciprocate raising the solution pressure to the higher level requirements at the primary generator 80. Energy recovery through reciprocating motion and devices of this type are available from the Recovery Engineering Inc. of Minneapolis, Minn. The details of their construction and operation are not a part of this invention.
It is herein understood that although the present invention has been specifically disclosed with the preferred embodiments and examples, modifications and variations of the concepts herein disclosed may be resolved to by those skilled in the art. Such modification and variations are considered to be within the scope of the invention and the appended claims.
Reid, Jr., Edward A., Cook, F. Bert
| Patent | Priority | Assignee | Title |
| Patent | Priority | Assignee | Title |
| 3473347, | |||
| 4646541, | Nov 13 1984 | Columbia Gas System Service Corporation | Absorption refrigeration and heat pump system |
| 4691532, | Nov 13 1984 | Columbia Gas System Service Corp | Dual cooling/heating system energy recovery |
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| 4843841, | Jun 10 1987 | Graco Inc. | Energy conserving refrigeration device |
| Executed on | Assignor | Assignee | Conveyance | Frame | Reel | Doc |
| Aug 31 1992 | Columbia Gas Service Corporation | (assignment on the face of the patent) | / |
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