Supercritical carbon dioxide power cycle for waste heat recovery

Information

  • Patent Grant
  • 9341084
  • Patent Number
    9,341,084
  • Date Filed
    Thursday, October 10, 2013
    10 years ago
  • Date Issued
    Tuesday, May 17, 2016
    8 years ago
Abstract
Aspects of the invention disclosed herein generally provide heat engine systems and methods for recovering energy, such as by generating electricity from thermal energy. In one configuration, a heat engine system contains a working fluid (e.g., sc-CO2) within a working fluid circuit, two heat exchangers configured to be thermally coupled to a heat source (e.g., waste heat), two expanders, two recuperators, two pumps, a condenser, and a plurality of valves configured to switch the system between single/dual-cycle modes. In another aspect, a method for recovering energy may include monitoring a temperature of the heat source, operating the heat engine system in the dual-cycle mode when the temperature is equal to or greater than a threshold value, and subsequently, operating the heat engine system in the single-cycle mode when the temperature is less than the threshold value.
Description
BACKGROUND

Heat is often created as a byproduct of industrial processes and is discharged when liquids, solids, and/or gasses that contain such heat are exhausted into the environment or otherwise removed from the process. This heat removal may be necessary to avoid exceeding safe and efficient operating temperatures in the industrial process equipment or may be inherent as exhaust in open cycles. Useful thermal energy is generally lost when this heat is not recovered or recycled during such processes. Accordingly, industrial processes often use heat exchanging devices to recover the heat and recycle much of the thermal energy back into the process or provide combined cycles, utilizing this thermal energy to power secondary heat engine cycles.


Waste heat recovery can be significantly limited by a variety of factors. For example, the exhaust stream may be reduced to low-grade (e.g., low temperature) heat, from which economical energy extraction is difficult, or the heat may otherwise be difficult to recover. Accordingly, the unrecovered heat is discharged as “waste heat,” typically via a stack or through exchange with water or another cooling medium. Moreover, in other settings, heat is available from renewable sources of thermal energy, such as heat from the sun or geothermal sources, which may be concentrated or otherwise manipulated.


In multiple-cycle systems, waste heat is converted to useful energy via two or more components coupled to the waste heat source in multiple locations. While multiple-cycle systems are successfully employed in some operating environments, generally, multiple-cycle systems have limited efficiencies in most operating environments. In some applications, the waste heat conditions (e.g., temperature) can fluctuate, such that the waste heat conditions are temporarily outside the optimal operating range of the multiple-cycle systems. Coupling multiple, discrete cycle systems is one solution. However, multiple independent cycle systems introduce greater system complexity due to the increased number of system components, especially when the system includes additional turbo- or turbine components. Such multiple independent cycle systems are complex and have increased control and maintenance requirements, as well as additional expenses and footprint demands.


Therefore, there is a need for a heat engine system and a method for recovering energy, such that the system and method have an optimized operating range for a heat recovery power cycle, minimized complexity, and maximized efficiency for recovering thermal energy and producing mechanical energy and/or electrical energy.


SUMMARY

Embodiments of the invention generally provide heat engine systems and methods for recovering energy, such as by producing mechanical energy and/or generating electrical energy, from a wide range of thermal sources, such as a waste heat source. In one or more exemplary embodiments disclosed herein, a heat engine system contains a working fluid within a working fluid circuit having a high pressure side and a low pressure side. The working fluid generally contains carbon dioxide and at least a portion of the working fluid circuit contains the working fluid in a supercritical state. The heat engine system further contains a first heat exchanger and a second heat exchanger, such that each of the first and second heat exchangers is fluidly coupled to and in thermal communication with the high pressure side of the working fluid circuit, configured to be fluidly coupled to and in thermal communication with a heat source stream (e.g., a waste heat stream), and configured to transfer thermal energy from the heat source stream to the working fluid within the working fluid circuit. The heat engine system also contains a first expander fluidly coupled to and downstream of the first heat exchanger on the high pressure side of the working fluid circuit and a second expander fluidly coupled to and downstream of the second heat exchanger on the high pressure side of the working fluid circuit.


The heat engine system further contains a first recuperator and a second recuperator fluidly coupled to the working fluid circuit. The first recuperator may be fluidly coupled to and downstream of the first expander on the low pressure side of the working fluid circuit and fluidly coupled to and upstream of the first heat exchanger on the high pressure side of the working fluid circuit. In some embodiments, the first recuperator may be configured to transfer thermal energy from the working fluid received from the first expander to the working fluid received from the first and second pumps when the system is in the dual-cycle mode. The second recuperator may be fluidly coupled to and downstream of the second expander on the low pressure side of the working fluid circuit and fluidly coupled to and upstream of the second heat exchanger on the high pressure side of the working fluid circuit. In some embodiments, the second recuperator may be configured to transfer thermal energy from the working fluid received from the second expander to the working fluid received from the first pump when the system is in dual-cycle mode and is inactive when the system is in the single-cycle mode.


The heat engine system further contains a condenser, a first pump, and a second pump fluidly coupled to the working fluid circuit. The condenser may be fluidly coupled to and downstream of the first and second recuperators on the low pressure side of the working fluid circuit. The condenser may be configured to remove thermal energy from the working fluid passing through the low pressure side of the working fluid circuit. The condenser may also be configured to control or regulate the temperature of the working fluid circulating through the working fluid circuit. The first pump may be fluidly coupled to and downstream of the condenser on the low pressure side of the working fluid circuit and fluidly coupled to and upstream of the first and second recuperators on the high pressure side of the working fluid circuit. The second pump may be fluidly coupled to and downstream of the condenser on the low pressure side of the working fluid circuit and fluidly coupled to and upstream of the first recuperator on the high pressure side of the working fluid circuit. In some exemplary embodiments, the second pump may be a turbopump, the second expander may be a drive turbine, and the drive turbine may be coupled to the turbopump and operable to drive the turbopump when the heat engine system is in the dual-cycle mode.


In some exemplary embodiments, the heat engine system further contains a plurality of valves operatively coupled to the working fluid circuit and configured to switch the heat engine system between a dual-cycle mode and a single-cycle mode. In the dual-cycle mode, the first and second heat exchangers and the first and second pumps are active as the working fluid is circulated throughout the working fluid circuit. However, in the single-cycle mode, the first heat exchanger and the first expander are active and at least the second heat exchanger and the second pump are inactive as the working fluid is circulated throughout the working fluid circuit.


In some examples, the plurality of valves may include a valve disposed between the condenser and the second pump, wherein the valve is closed during the single-cycle mode of the heat engine system and the valve is open when the heat engine system is in the dual-cycle mode. In other examples, the plurality of valves may include a valve disposed between the first pump and the first recuperator, the valve may be configured to prohibit flow of the working fluid from the first pump to the first recuperator when the heat engine system is in the dual-cycle mode and to allow fluid flow therebetween during the single-cycle mode of the heat engine system.


In other exemplary embodiments, the plurality of valves may include five or more valves operatively coupled to the working fluid circuit for controlling the flow of the working fluid. A first valve may be operatively coupled to the high pressure side of the working fluid circuit and disposed downstream of the first pump and upstream of the second recuperator. A second valve may be operatively coupled to the low pressure side of the working fluid circuit and disposed downstream of the second recuperator and upstream of the condenser. A third valve may be operatively coupled to the high pressure side of the working fluid circuit and disposed downstream of the first pump and upstream of the first recuperator. A fourth valve may be operatively coupled to the high pressure side of the working fluid circuit and disposed downstream of the second pump and upstream of the first recuperator. A fifth valve may be operatively coupled to the low pressure side of the working fluid circuit and disposed downstream of the condenser and upstream of the second pump.


In some examples, the working fluid from the low pressure side of the first recuperator and the working fluid from the low pressure side of the second recuperator combine at a point on the low pressure side of the working fluid circuit, such that the point is disposed upstream of the condenser and downstream of the second valve. In some configurations, each of the first, second, fourth, and fifth valves may be in an opened-position and the third valve may be in a closed-position when the heat engine system is in the dual-cycle mode. Alternatively, during the single-cycle mode of the heat engine system, each of the first, second, fourth, and fifth valves may be in a closed-position and the third valve may be in an opened-position.


In other embodiments disclosed herein, the plurality of valves may be configured to actuate in response to a change in temperature of the heat source stream. For example, when the temperature of the heat source stream becomes less than a threshold value, the plurality of valves may be configured to switch the system to the single-cycle mode. Also, when the temperature of the heat source stream becomes equal to or greater than the threshold value, the plurality of valves may be configured to switch the system to the dual-cycle mode.


In other embodiments disclosed herein, the plurality of valves may be configured to switch the system between the dual-cycle mode and the single-cycle mode, such that in the dual-cycle mode, the plurality of valves may be configured to direct the working fluid from the condenser to the first and second pumps, and subsequently, direct the working fluid from the first pump to the second heat exchanger and/or direct the working fluid from the second pump to the first heat exchanger. In the single-cycle mode, the plurality of valves may be configured to direct the working fluid from the condenser to the first pump and from the first pump to the first heat exchanger, and to substantially cut-off or stop the flow of the working fluid to the second pump, the second heat exchanger, and the second expander.


In one or more embodiments disclosed herein, a method for recovering energy from a heat source (e.g., waste heat source) is provided and includes operating a heat engine system in a dual-cycle mode and subsequently switching the heat engine system from the dual-cycle mode to a single-cycle mode. In the dual-cycle mode, the method includes operating the heat engine system by heating a first mass flow of a working fluid in the first heat exchanger fluidly coupled to and in thermal communication with a working fluid circuit and a heat source stream and expanding the first mass flow in a first expander fluidly coupled to the first heat exchanger via the working fluid circuit. The first heat exchanger may be configured to transfer thermal energy from the heat source stream to the first mass flow of the working fluid within the working fluid circuit. In many exemplary embodiments, the working fluid contains carbon dioxide and at least a portion of the working fluid circuit contains the working fluid in a supercritical state.


Also, in the dual-cycle mode, the method includes heating a second mass flow of the working fluid in the second heat exchanger fluidly coupled to and in thermal communication with the working fluid circuit and the heat source stream and expanding the second mass flow in a second expander fluidly coupled to the second heat exchanger via the working fluid circuit. The second heat exchanger may be configured to transfer thermal energy from the heat source stream to the second mass flow of the working fluid within the working fluid circuit. The method further includes, in the dual-cycle mode, at least partially condensing the first and second mass flows in one or more condensers fluidly coupled to the working fluid circuit, pressurizing the first mass flow in a first pump fluidly coupled to the condenser via the working fluid circuit, and pressurizing the second mass flow in a second pump fluidly coupled to the condenser via the working fluid circuit.


In the single-cycle mode, the method includes operating the heat engine system by de-activating the second heat exchanger, the second expander, and the second pump, directing the working fluid from the condenser to the first pump, and directing the working fluid from the first pump to the first heat exchanger. The method may include de-activating the second recuperator and directing the working fluid from the second pump to the first recuperator while switching to the single-cycle mode.


In other embodiments, the method includes operating the heat engine system in the dual-cycle mode by further transferring heat via the first recuperator from the first mass flow downstream of the first expander and upstream of the condenser to the first mass flow downstream of the second pump and upstream of the first heat exchanger, transferring heat via the second recuperator from the second mass flow downstream of the second expander and upstream of the condenser to the second mass flow downstream of the first pump and upstream of the second heat exchanger, and switching to the single-cycle mode further includes de-activating the second recuperator and directing the working fluid from the second pump to the first recuperator.


In some embodiments, the method further includes monitoring a temperature of the heat source stream, operating the heat engine system in the dual-cycle mode when the temperature is equal to or greater than a threshold value, and subsequently, operating the heat engine system in the single-cycle mode when the temperature is less than the threshold value. In some examples, the threshold value of the temperature of the heat source stream is within a range from about 300° C. to about 400° C., such as about 350° C. In one aspect, the method may include automatically switching from operating the heat engine system in the dual-cycle mode to operating the heat engine system in the single-cycle mode with a programmable controller once the temperature is less than the threshold value. In another aspect, the method may include manually switching from operating the heat engine system in the dual-cycle mode to operating the heat engine system in the single-cycle mode once the temperature is less than the threshold value.





BRIEF DESCRIPTION OF THE DRAWINGS

Embodiments of the present disclosure are best understood from the following detailed description when read with the accompanying Figures. It is emphasized that, in accordance with the standard practice in the industry, various features are not drawn to scale. In fact, the dimensions of the various features may be arbitrarily increased or reduced for clarity of discussion.



FIG. 1 schematically illustrates a heat engine system, operating in dual-cycle mode, according to exemplary embodiments described herein.



FIG. 2 schematically illustrates the heat engine of FIG. 1, operating in single-cycle mode, according to exemplary embodiments described herein.



FIG. 3 illustrates a flowchart of a method for extracting energy from heat source, according to exemplary embodiments described herein.





DETAILED DESCRIPTION

Embodiments of the invention generally provide heat engine systems and methods for recovering energy (e.g., generating electricity) with such heat engine systems. FIGS. 1 and 2 schematically illustrate a heat engine system 100, according to an exemplary embodiment described herein. The heat engine system 100 is flexible and operates efficiently over a wide range of conditions of the heat source or stream (e.g., waste heat source or stream) from which the heat engine system 100 extracts energy. As will be discussed in further detail below, FIG. 1 illustrates the heat engine system 100 in dual-cycle mode, while FIG. 2 illustrates the heat engine system 100 in single-cycle mode. The dual-cycle mode may be particularly suitable for use with heat sources having temperatures greater than a predetermined threshold value, while the single-cycle mode may be particularly useful with heat sources having temperatures less than the threshold value. In some examples, the threshold value of the temperature of the heat source and/or the heat source stream is within a range from about 300° C. to about 400° C., such as about 350° C. Since the heat engine system 100 is capable of switching between the two modes of operation, for example, back-and-forth without limitation, the heat engine system 100 may operate at an increased efficiency over a broader range of heat source temperatures as compared to other heat engines. Although referred to herein as “dual-cycle” and “single-cycle” modes, it will be appreciated that the dual-cycle mode can include three or more cycles operating at once, and the single-cycle mode is intended to be indicative of a reduced number of active cycles, as compared to “dual-cycle” mode, but can include one or more cycles operating at once.


Referring now specifically to FIG. 1, the heat engine system 100 contains a first heat exchanger 102 and a second heat exchanger 104 fluidly coupled to and in thermal communication with a heat source stream 105, such as a waste heat stream. The heat source stream 105 may flow from or otherwise be derived from a heat source 106, such as a waste heat source or other source of thermal energy. In an exemplary embodiment, the first and second heat exchangers 102, 104 are coupled in series with respect to the heat source stream 105, such that the first heat exchanger 102 is disposed upstream of the second heat exchanger 104 along the heat source stream 105. Therefore, the first heat exchanger 102 generally receives the heat source stream 105 at a temperature greater than the temperature of the heat source stream 105 received by the second heat exchanger 104 since a portion of the thermal energy or heat was recovered by the first heat exchanger 102 prior to the heat source stream 105 flowing to the second heat exchanger 104.


The first and second heat exchangers 102, 104 may be or include one or more of suitable types of heat exchangers, for example, shell-and-tubes, plates, fins, printed circuits, combinations thereof, and/or any others, without limitation. Furthermore, it will be appreciated that additional heat exchangers may be employed and/or the first and second heat exchangers 102, 104 may be provided as different sections of a common heat exchanging unit. Since the first heat exchanger 102 may be exposed to the heat source stream 105 at greater temperatures, a greater amount of recovered thermal energy may be available for conversion to useful power by the expansion devices coupled to the first heat exchanger 102, relative to the recovered thermal energy available for conversion by the expansion devices coupled to the second heat exchanger 104.


The heat engine system 100 further contains a working fluid circuit 110, which is fluidly coupled to the first and second heat exchangers 102, 104. The working fluid circuit 110 may be configured to provide working fluid to and receive heated working fluid from one or both of the first and second heat exchangers 102, 104 as part of a first or “primary” circuit 112 and a second or “secondary” circuit 114. The primary and secondary circuits 112, 114 may thus enable collection of thermal energy from the heat source via the first and second heat exchangers 102, 104, for conversion into mechanical and/or electrical energy downstream.


The working fluid may be or contain carbon dioxide (CO2) and mixtures containing carbon dioxide. Carbon dioxide as a working fluid for power generating cycles has many advantages as a working fluid, such as non-toxicity, non-flammability, easy availability, and relatively inexpensive. Due in part to its relatively high working pressure, a carbon dioxide system can be built that is much more compact than systems using other working fluids. The high density and volumetric heat capacity of carbon dioxide with respect to other working fluids makes carbon dioxide more “energy dense” meaning that the size of all system components can be considerably reduced without losing performance. It should be noted that use of the terms carbon dioxide (CO2), supercritical carbon dioxide (sc-CO2), or subcritical carbon dioxide (sub-CO2) is not intended to be limited to carbon dioxide of any particular type, source, purity, or grade. For example, industrial grade carbon dioxide may be contained in and/or used as the working fluid without departing from the scope of the disclosure.


The working fluid circuit 110 contains the working fluid and has a high pressure side and a low pressure side. In exemplary embodiments, the working fluid contained in the working fluid circuit 110 is carbon dioxide or substantially contains carbon dioxide and may be in a supercritical state (e.g., sc-CO2) and/or a subcritical state (e.g., sub-CO2). In one example, the carbon dioxide working fluid contained within at least a portion of the high pressure side of the working fluid circuit 110 is in a supercritical state and the carbon dioxide working fluid contained within the low pressure side of the working fluid circuit 110 is in a subcritical state and/or supercritical state.


In other exemplary embodiments, the working fluid in the working fluid circuit 110 may be a binary, ternary, or other working fluid blend. The working fluid blend or combination can be selected for the unique attributes possessed by the fluid combination within a heat recovery system, as described herein. For example, one such fluid combination includes a liquid absorbent and carbon dioxide mixture enabling the combined fluid to be pumped in a liquid state to high pressure with less energy input than required to compress carbon dioxide. In another exemplary embodiment, the working fluid may be a combination of supercritical carbon dioxide (sc-CO2), subcritical carbon dioxide (sub-CO2), and/or one or more other miscible fluids or chemical compounds. In yet other exemplary embodiments, the working fluid may be a combination of carbon dioxide and propane, or carbon dioxide and ammonia, without departing from the scope of the disclosure.


The use of the term “working fluid” is not intended to limit the state or phase of matter of the working fluid or components of the working fluid. For instance, the working fluid or portions of the working fluid may be in a fluid phase, a gas phase, a supercritical state, a subcritical state, or any other phase or state at any one or more points within the heat engine system 100 or fluid cycle. The working fluid may be in a supercritical state over certain portions of the working fluid circuit 110 (e.g., the high pressure side), and in a subcritical state or a supercritical state over other portions of the working fluid circuit 110 (e.g., the low pressure side). In other exemplary embodiments, the entire working fluid circuit 110 may be operated and controlled such that the working fluid is in a supercritical or subcritical state during the entire execution of the working fluid circuit 110.


The heat source 106 and/or the heat source stream 105 may derive thermal energy from a variety of high-temperature sources. For example, the heat source stream 105 may be a waste heat stream such as, but not limited to, gas turbine exhaust, process stream exhaust, or other combustion product exhaust streams, such as furnace or boiler exhaust streams. Accordingly, the heat engine system 100 may be configured to transform waste heat or other thermal energy into electricity for applications ranging from bottom cycling in gas turbines, stationary diesel engine gensets, industrial waste heat recovery (e.g., in refineries and compression stations), and hybrid alternatives to the internal combustion engine. In other exemplary embodiments, the heat source 106 may derive thermal energy from renewable sources of thermal energy such as, but not limited to, a solar thermal source and a geothermal source. While the heat source 106 and/or the heat source stream 105 may be a fluid stream of the high temperature source itself, in other exemplary embodiments, the heat source 106 and/or the heat source stream 105 may be a thermal fluid in contact with the high temperature source. Thermal energy may be transferred from the thermal fluid to the first and second heat exchangers 102, 104, and further be transferred from the first and second heat exchangers 102, 104 to the working fluid in the working fluid circuit 110.


In various exemplary embodiments, the initial temperature of the heat source 106 and/or the heat source stream 105 entering the heat engine system 100 may be within a range from about 400° C. (about 752° F.) to about 650° C. (about 1,202° F.) or greater. However, the working fluid circuit 110 containing the working fluid (e.g., sc-CO2) disclosed herein is flexible with respect to the temperature of the heat source stream and thus may be configured to efficiently extract energy from the heat source stream at lesser temperatures, for example, at a temperature of about 400° C. (about 752° F.) or less, such as about 350° C. (about 662° F.) or less, such as about 300° C. (about 572° F.) or less. Accordingly, the heat engine system 100 may include any sensors in or proximal to the heat source stream, for example, to determine the temperature, or another relevant condition (e.g., mass flow rate or pressure) of the heat source stream, to determine whether single or dual-cycle mode is more advantageous.


In an exemplary embodiment, the heat engine system 100 includes a power turbine 116, which may also be referred to as a first expander, as part of the primary circuit 112. The power turbine 116 is fluidly coupled to the first heat exchanger 102 via the primary circuit 112 and receives fluid from the first heat exchanger 102. The power turbine 116 may be any suitable type of expansion device, such as, for example, a single or multistage impulse or reaction turbine. Further, the power turbine 116 may be representative of multiple discrete turbines, which cooperate to expand the working fluid provided from the first heat exchanger 102, whether in series or in parallel. The power turbine 116 may be disposed between the high pressure side and the low pressure side of the working fluid circuit 110 and fluidly coupled to and in thermal communication with the working fluid. The power turbine 116 may be configured to convert thermal energy to mechanical energy by a pressure drop in the working fluid flowing between the high and the low pressure sides of the working fluid circuit 110.


The power turbine 116 is generally coupled to a generator 113 via a shaft 115, such that the power turbine 116 rotates the shaft 115 and the generator 113 converts such rotation into electricity. Therefore, the generator 113 may be configured to convert the mechanical energy from the power turbine 116 into electrical energy. Also, the generator 113 may be generally electrically coupled to an electrical grid (not shown) and configured to transfer the electrical energy to the electrical grid. It will be appreciated that speed-altering devices, such as gear boxes (not shown), may be employed in such a connection between or with the power turbine 116, the shaft 115, and/or the generator 113, or the power turbine 116 may be directly coupled to the generator 113.


The heat engine system 100 also contains a first recuperator 118, which is fluidly coupled to the power turbine 116 and receives working fluid therefrom, as part of the primary circuit 112. The first recuperator 118 may be any suitable heat exchanger or set of heat exchangers, and may serve to transfer heat remaining in the working fluid downstream of the power turbine 116 after expansion. For example, the first recuperator 118 may include one or more plate, fin, shell-and-tube, printed circuit, or other types of heat exchanger, whether in parallel or in series.


The heat engine system 100 also contains one or more condensers 120 fluidly coupled to the first recuperator 118 and configured to receive the working fluid therefrom. The condenser 120 may be, for example, a standard air or water-cooled condenser but may also be a trim cooler, adsorption chiller, mechanical chiller, a combination thereof, and/or the like. The condenser 120 may additionally or instead include one or more compressors, intercoolers, aftercoolers, or the like, which are configured to chill the working fluid, for example, in high ambient temperature regions and/or during summer months. Examples of systems that can be provided for use as the condenser 120 include the condensing systems disclosed in commonly assigned U.S. application Ser. No. 13/290,735, filed Nov. 7, 2011, and published as U.S. Pub. No. 2013/0113221, which is incorporated herein by reference in its entirety to the extent consistent with the present application.


The heat engine system 100 also contains a first pump 126 as part of the primary circuit 112 and/or the secondary circuit 114. The first pump 126 may a motor-driven pump or a turbine-driven pump and may be of any suitable design or size, may include multiple pumps, and may be configured to operate with a reduced flow rate and/or reduced pressure head as compared to a second pump 117. A reduced flow rate of the working fluid may be desired since less thermal energy may be available for extraction from the heat source stream during a startup process or a shutdown process. Furthermore, the first pump 126 may operate as a starter pump. Accordingly, during startup of the heat engine system 100, the first pump 126 may operate to power the drive turbine 122 to begin the operation of the second pump 117.


The first pump 126 may be fluidly coupled to the working fluid circuit 110 upstream of the first recuperator 118 and upstream of the second recuperator 128 to provide working fluid at increased pressure and/or flowrate. In one embodiment, the heat engine system 100 may be configured to utilize the first pump 126 as part of the primary circuit 112. The working fluid may be flowed from the first pump 126, through the third valve 136, through the high pressure side of the first recuperator 118, and then supplied back to the first heat exchanger 102, closing the loop on the primary circuit 112. In another embodiment, the heat engine system 100 may be configured to utilize the first pump 126 as part of the secondary circuit 114. The working fluid may be flowed from the first pump 126, through the first valve 130, through the high pressure side of the second recuperator 128, and then supplied back to the second heat exchanger 104, closing the loop on the secondary circuit 114.


Therefore, the primary circuit 112 may be configured to provide the working fluid to circulate in a cycle, whereby the working fluid exits the outlet of the first heat exchanger 102, flows through the power turbine throttle valve 150, flows through the power turbine 116, flows through the low pressure side (or cooling side) of the first recuperator 118, flows through point 134, flows through the condenser 120, flows through the first pump 126, flows through the third valve 136, flows through the high pressure side (or heating side) of the first recuperator 118, and enters the inlet of the first heat exchanger 102 to complete the cycle of the primary circuit 112.


In another exemplary embodiment described herein, when sufficient thermal energy is available from the heat source 106 and the heat source stream 105, the secondary circuit 114 may be active and configured to support the operation of the primary circuit 112, for example, by driving a turbopump, such as the second pump 117. To that end, the heat engine system 100 contains the drive turbine 122, which is fluidly coupled to the second heat exchanger 104 and may be configured to receive working fluid therefrom, as part of the secondary circuit 114. The drive turbine 122 may be any suitable axial or radial, single or multistage, impulse or reaction turbine, or any such turbines acting in series or in parallel. Further, the drive turbine 122 may be mechanically linked to a turbopump, such as the second pump 117 via a shaft 124, for example, such that the rotation of the drive turbine 122 causes rotation of the second pump 117. In some exemplary embodiments, the drive turbine 122 may additionally or instead drive other components of the heat engine system 100 or other systems (not shown), may power a generator, and/or may be electrically coupled to one or more motors configured to drive any other device.


The heat engine system 100 may also include a second recuperator 128, as part of the secondary circuit 114, which is fluidly coupled to the drive turbine 122 and configured to receive working fluid therefrom in the secondary circuit 114. The second recuperator 128 may be any suitable heat exchanger or set of heat exchangers, and may serve to transfer heat remaining in the working fluid downstream of the drive turbine 122 after expansion. For example, the second recuperator 128 may include one or more plates, fins, shell-and-tubes, printed circuits, or other types of heat exchanger, whether in parallel or in series.


The second recuperator 128 may be fluidly coupled with the condenser 120 via the working fluid circuit 110. The low pressure side or cooling side of the second recuperator 128 may be fluidly coupled downstream of the drive turbine 122 and upstream of the condenser 120. The high pressure side or heating side of the second recuperator 128 may be fluidly coupled downstream of the first pump 126 and upstream of the second heat exchanger 104. Accordingly, the condenser 120 may receive a combined flow of working fluid from both the first and second recuperators 118, 128. In another exemplary embodiment, the condenser 120 may receive separate flows from the first and second recuperators 118, 128 and may mix the flows in the condenser 120. In other exemplary embodiments, the condenser 120 may be representative of two condensers, which may maintain the flows as separate streams, without departing from the scope of the disclosure. In the illustrated exemplary embodiment, the primary and secondary circuits 112, 114 may be described as being “overlapping” with respect to the condenser 120, as the condenser 120 is part of both the primary and secondary circuits 112, 114.


The heat engine system 100 further includes a second pump 117 as part of the secondary circuit 114 during dual-cycle mode of operation. The second pump 117 may be fluidly coupled to and disposed downstream of the condenser 120 on the low pressure side of the working fluid circuit 110, such that the outlet of the condenser 120 is upstream of the inlet of the second pump 117. Also, the second pump 117 may be fluidly coupled to and disposed upstream of the first recuperator 118 on the high pressure side of the working fluid circuit 110, such that the inlet of the first recuperator 118 is upstream of the outlet of the second pump 117.


The second pump 117 may be configured to receive at least a portion of the working fluid condensed in the condenser 120, as part of the secondary circuit 114 during the dual-cycle mode of operation. The second pump 117 may be any suitable turbopump or a component of a turbopump, such as a centrifugal turbopump, which is suitable to pressurize the working fluid, for example, in liquid form, at a desired flow rate to a desired pressure. In one or more embodiments, the second pump 117 may be a turbopump and may be powered by an expander or turbine, such as a drive turbine 122. In one specific exemplary embodiment, the second pump 117 may be a component of a turbopump unit 108 and coupled to the drive turbine 122 by the shaft 124, as depicted in FIGS. 1 and 2. However, in other embodiments, the second pump 117 may be at least partially driven by the power turbine 116 (not shown). In an alternative embodiment, instead of being coupled to and driven by the drive turbine 122 or another turbine, the second pump 117 may be coupled to and driven by an electric motor, a gas or diesel engine, or any other suitable device.


Therefore, the secondary circuit 114 provides the working fluid to circulate in a cycle, whereby the working fluid exits the outlet of the second heat exchanger 104, flows through the turbo pump throttle valve 152, flows through the drive turbine 122, flows through the low pressure side (or cooling side) of the second recuperator 128, flows through the second valve 132, flows through the condenser 120, flows through the fifth valve 142, flows through the second pump 117, flows through the fourth valve 140, and then is discharged into the primary circuit 112 at the point 134 on the working fluid circuit 110 downstream of the third valve 136 and upstream of the high pressure side of the first recuperator 118. From the primary circuit 112, upon setting the third valve 136 and the fifth valve 142 in closed-positions and the first valve 130 in an opened-position, the secondary circuit 114 further provides that the working fluid flows through the first pump 126, flows through the first valve 130, flows through the high pressure side of the second recuperator 128, and then supplied back to the second heat exchanger 104, closing the loop on the secondary circuit 114.


The heat engine system 100 contains a variety of components fluidly coupled to the working fluid circuit 110, as depicted in FIGS. 1 and 2. The working fluid circuit 110 contains high and low pressure sides during actual operation of the heat engine system 100. Generally, the portions of the high pressure side of the working fluid circuit 110 are disposed downstream of the pumps, such as the first pump 126 and the second pump 117, and upstream of the turbines, such as the power turbine 116 and the drive turbine 122. Inversely, the portions of the low pressure side of the working fluid circuit 110 are disposed downstream of the turbines, such as the power turbine 116 and the drive turbine 122, and upstream of the pumps, such as the first pump 126 and the second pump 117.


In an exemplary embodiment, a first portion of the high pressure side of the working fluid circuit 110 may extend from the first pump 126, through the first valve 130, through the second recuperator 128, through the second heat exchanger 104, through the turbo pump throttle valve 152, and into the drive turbine 122. In another exemplary embodiment, a second portion of the high pressure side of the working fluid circuit 110 may extend from the second pump 117, through the fourth valve 140, through the first recuperator 118, through the first heat exchanger 102, through the power turbine throttle valve 150, and into the power turbine 116. In another exemplary embodiment, a first portion of the low pressure side of the working fluid circuit 110 may extend from the drive turbine 122, through the second recuperator 128, through the second valve 132, through the condenser 120, and either into the first pump 126 and/or through the fifth valve 142, and into the second pump 117. In another exemplary embodiment, a second portion of the low pressure side of the working fluid circuit 110 may extend from the power turbine 116, through the first recuperator 118, through the condenser 120, and either into the first pump 126 and/or through the fifth valve 142, and into the second pump 117.


Some components of the heat engine system 100 may be fluidly coupled to both the high and low pressure sides, such as the turbines, the pumps, and the recuperators. Therefore, the low pressure side or the high pressure side of a particular component refers to the respective low or high pressure side of the working fluid circuit 110 fluidly coupled to the component. For example, the low pressure side (or cooling side) of the second recuperator 128 refers to the inlet and the outlet on the second recuperator 128 fluidly coupled to the low pressure side of the working fluid circuit 110. In another example, the high pressure side of the power turbine 116 refers to the inlet on the power turbine 116 fluidly coupled to the high pressure side of the working fluid circuit 110 and the low pressure side of the power turbine 116 refers to the outlet on the power turbine 116 fluidly coupled to the low pressure side of the working fluid circuit 110.


The heat engine system 100 also contains a plurality of valves operable to control the mode of operation of the heat engine system 100. The plurality of valves may include five or more valves. For example, the heat engine system 100 contains a first valve 130, a second valve 132, a third valve 136, a fourth valve 140, and a fifth valve 142. In an exemplary embodiment, the first valve 130 may be operatively coupled to the high pressure side of the working fluid circuit 110 and may be disposed downstream of the first pump 126 and upstream of the second recuperator 128. The second valve 132 may be operatively coupled to the low pressure side of the working fluid circuit 110 in the secondary circuit 114 and may be disposed downstream of the second recuperator 128 and upstream of the condenser 120. Further, in embodiments of the heat engine system 100 in which the primary and secondary circuits 112, 114 overlap to share the condenser 120, the second valve 132 may be disposed upstream of the point 134 where the primary and secondary circuits 112, 114 combine, mix, or otherwise come together upstream of the condenser 120. The third valve 136 may be operatively coupled to the high pressure side of the working fluid circuit 110 and may be disposed downstream of the first pump 126 and upstream of the first recuperator 118. The fourth valve 140 may be operatively coupled to the high pressure side of the working fluid circuit 110 and may be disposed downstream of the second pump 117 and upstream of the first recuperator 118. The fifth valve 142 may be operatively coupled to the low pressure side of the working fluid circuit 110 and may be disposed downstream of the condenser 120 and upstream of the second pump 117.



FIG. 1 illustrates a dual-cycle mode of operation, according to an exemplary embodiment of the heat engine system 100. In dual-cycle mode, both the primary and secondary circuits 112, 114 are active, with a first mass flow “m1” of working fluid coursing through the primary circuit 112, a second mass flow “m2” of working fluid coursing through the secondary circuit 114, and a combined flow “m1+m2” thereof coursing through overlapping sections of the primary and secondary circuits 112, 114, as indicated.


During the dual-cycle mode of operation, in the primary circuit 112, the first mass flow m1 of the working fluid recovers energy from the higher-grade heat coursing through the first heat exchanger 102. This heat recovery transitions the first mass flow m1 of the working fluid from an intermediate-temperature, high-pressure working fluid provided to the first heat exchanger 102 during steady-state operation to a high-temperature, high-pressure first mass flow m1 of the working fluid exiting the first heat exchanger 102. In an exemplary embodiment, the working fluid may be at least partially in a supercritical state when exiting the first heat exchanger 102.


The high-temperature, high-pressure (e.g., supercritical state/phase) first mass flow m1 is directed in the primary circuit 112 from the first heat exchanger 102 to the power turbine 116. At least a portion of the thermal energy stored in the high-temperature, high-pressure first mass flow m1 is converted to mechanical energy in the power turbine 116 by expansion of the working fluid. In some examples, the power turbine 116 and the generator 113 may be coupled together and the generator 113 may be configured to convert the mechanical energy into electrical energy, which can be used to power other equipment, provided to a grid, a bus, or the like. In the power turbine 116, the pressure, and, to a certain extent, the temperature of the first mass flow m1 of the working fluid is reduced; however, the temperature still remains generally in a high temperature range of the primary circuit 112. Accordingly, the first mass flow m1 of the working fluid exiting the power turbine 116 is a low-pressure, high-temperature working fluid. The low-pressure, high-temperature first mass flow m1 of the working fluid may be at least partially in gas phase.


The low-pressure, high-temperature first mass flow m1 of the working fluid is then directed to the first recuperator 118. The first recuperator 118 is coupled to the primary circuit 112 downstream of the power turbine 116 on the low-pressure side and upstream of the first heat exchanger 102 on the high-pressure side. Accordingly, a portion of the heat remaining in the first mass flow m1 of the working fluid exiting from the power turbine 116 is transferred to a low-temperature, high-pressure first mass flow m1 of the working fluid, upstream of the first heat exchanger 102. As such, the first recuperator 118 acts as a pre-heater for the first mass flow m1 proceeding to the first heat exchanger 102, thereby providing the intermediate temperature, high-pressure first mass flow m1 of the working fluid thereto. Further, the first recuperator 118 acts as a pre-cooler for the first mass flow m1 of the working fluid proceeding to the condenser 120, thereby providing an intermediate-temperature, low-pressure first mass flow m1 of the working fluid thereto.


Upstream of or within the condenser 120, the intermediate-temperature, low-pressure first mass flow m1 may be combined with an intermediate-temperature, low-pressure second mass flow m2 of the working fluid. However, whether combined or not, the first mass flow m1 may proceed to the condenser 120 for further cooling and, for example, at least partial phase change to a liquid. In an exemplary embodiment, the combined mass flow m1+m2 of the working fluid is directed to the condenser 120, and subsequently split back into the two mass flows m1, m2 as the working fluid is directed to the discrete portions of the primary and secondary circuits 112, 114.


The condenser 120 reduces the temperature of the working fluid, resulting in a low-pressure, low-temperature working fluid, which may be at least partially condensed into liquid phase. In dual-cycle mode, the first mass flow m1 of the low-pressure, low-temperature working fluid is split from the combined mass flow m1+m2 and passed from the condenser 120 to the second pump 117 for pressurization. The second pump 117 may add a nominal amount of heat to the first mass flow m1 of the working fluid, but is provided primarily to increase the pressure thereof. Accordingly, the first mass flow m1 of the working fluid exiting the second pump 117 is a high-pressure, low-temperature working fluid. The first mass flow m1 of the working fluid is then directed to the first recuperator 118, for heat transfer with the high-temperature, low-pressure first mass flow m1 of the working fluid, downstream of the power turbine 116. The first mass flow m1 of the working fluid exiting the first recuperator 118 as an intermediate-temperature, high-pressure first mass flow m1 of the working fluid, and is directed to the first heat exchanger 102, thereby closing the loop of the primary circuit 112.


During dual-cycle mode, as shown in FIG. 1, the second mass flow m2 of combined flow m1+m2 working fluid from the condenser 120 is split off and directed into the secondary circuit 114. The second mass flow m2 may be directed to the first pump 126, for example. The first pump 126 may heat the fluid to a certain extent; however, the primary purpose of the first pump 126 is to pressurize the working fluid. Accordingly, the second mass flow m2 of the working fluid exiting the first pump 126 is a low-temperature, high-pressure second mass flow m2 of the working fluid.


The low-temperature, high-pressure second mass flow m2 of the working fluid is then routed to the second recuperator 128 for preheating. The second recuperator 128 is coupled to the secondary circuit 114 downstream of the first pump 126 on the high-pressure side, upstream of the second heat exchanger 104 on the high-pressure side, and downstream of the drive turbine 122 on the low-pressure side. The second mass flow m2 of the working fluid from the first pump 126 is preheated in the recuperator 128 to provide an intermediate-temperature, high-pressure second mass flow m2 of the working fluid to the second heat exchanger 104.


The second mass flow m2 of the working fluid in the second heat exchanger 104 is heated to provide a high-temperature, high-pressure second mass flow m2 of the working fluid. In an exemplary embodiment, the second mass flow m2 of the working fluid exiting the second heat exchanger 104 may be in a supercritical state. The high-temperature, high-pressure second mass flow m2 of the working fluid may then be directed to the drive turbine 122 for expansion to drive the second pump 117, for example, thus closing the loop on the secondary circuit 114.


During dual-cycle mode, the first, second, fourth, and fifth valves 130, 132, 140, 142 may be open (each valve in an opened-position), while the third valve 136 may be closed (valve in a closed-position), as shown in an exemplary embodiment. As indicated by the solid lines depicting fluid conduits therebetween, the first, second, fourth, and fifth valves 130, 132, 140, 142—in opened-positions—allow fluid communication therethrough. As such, the first pump 126 is in fluid communication with the second recuperator 128 via the first valve 130, and the second recuperator 128 is in fluid communication with the condenser 120 via the second valve 132. Further, the second pump 117 is in fluid communication with the first recuperator 118 via the fourth valve 140, and the condenser 120 is in fluid communication with the second pump 117 via the fifth valve 142. In contrast, as depicted by the dashed line for conduit 138, although they are fluidly coupled as the term is used herein, fluid communication between the first pump 126 and the first recuperator 118 is generally prohibited by the third valve 136 in a closed-position.


Such configuration of the valves 130, 132, 136, 140, 142 maintains the separation of the discrete portions of the primary and secondary circuits 112, 114 upstream and downstream of, for example, the condenser 120. Accordingly, the secondary circuit 114 may be operable to recover thermal energy from the heat source stream 105 in the second heat exchanger 104 and employ such thermal energy to, for example, power the drive turbine 122, which drives the second pump 117 of the primary circuit 112. The primary circuit 112, in turn, may recover a greater amount of thermal energy from the heat source stream 105 in the first heat exchanger 102, as compared to the thermal energy recovered by the secondary circuit 114 in the second heat exchanger 104, and may convert the thermal energy into shaft rotation and/or electricity as an end-product for the heat engine system 100.



FIG. 2 schematically depicts the heat engine system 100 of FIG. 1, but with the opened/closed-positions of the valves 130, 132, 136, 140, 142 being changed to provide the single-cycle mode of operation for the heat engine system 100, according to an exemplary embodiment. In the single-cycle mode of operation, the heat engine system 100 may be utilized with less or a reduced number of active components and conduits of the working fluid circuit 110 than in the dual-cycle mode of operation. Active components and conduits contain the working fluid flowing or otherwise passing therethrough during normal operation of the heat engine system 100. Inactive components and conduits have a reduced flow or lack flow of the working fluid passing therethrough during normal operation of the heat engine system 100. The inactive components and conduits are indicated in FIG. 2 by dashed lines, according to one exemplary embodiment among many contemplated. More particularly, the flow of the working fluid to the second heat exchanger 104 may be substantially cut-off in the single-cycle mode, thereby de-activating the second heat exchanger 104. The flow of the working fluid to the second heat exchanger 104 may be initially cut-off due to reduced temperature of the heat source stream 105 from the heat source 106, component failure, or for other reasons. In one configuration, the heat engine system 100 may include a sensor (not shown) which may monitor the temperature of the heat source stream 105, for example, as the heat source stream 105 enters the first heat exchanger 102. Once the sensor reads or otherwise measures a temperature of less than a threshold value, for example, the heat engine system 100 may be switched, either manually or automatically with a programmable controller, to operate in single-cycle mode. Once the temperature becomes equal to or greater than the threshold value, the heat engine system 100 may be switched back to the dual-cycle mode. In some embodiments, the threshold value of the temperature of the heat source and/or the heat source stream 105 may be within a range from about 300° C. (about 572° F.) to about 400° C. (about 752° F.), more narrowly within a range from about 320° C. (about 608° F.) to about 380° C. (about 716° F.), and more narrowly within a range from about 340° C. (about 644° F.) to about 360° C. (about 680° F.), for example, about 350° C. (about 662° F.).


As indicated, the first heat exchanger 102 may be active, while the second heat exchanger 104 is inactive or de-activated. Thus, splitting of the combined flow of the working fluid to feed both heat exchangers 102, 104, described herein for the dual-cycle mode of operation, may no longer be required and a single mass flow “m” of the working fluid to the first heat exchanger 102 may develop. Additionally, flow of the working fluid to the drive turbine 122 and the second recuperator 128 may also be cut-off or stopped, as the working fluid flows may be provided to recover thermal energy via the second heat exchanger 104, as discussed above, which is now inactive.


Since the drive turbine 122, powered by thermal energy recovered in the second heat exchanger 104 during the dual-cycle mode of operation, is also inactive or deactivated during the single-cycle mode of operation, the second pump 117 may lack a driver. Accordingly, the second pump 117 may be isolated and deactivated via closure of the fourth and fifth valves 140, 142. However, as is known for thermodynamic cycles, the working fluid in the active primary circuit 112 requires pressurization, which, in the single-cycle mode of operation, may be provided by the first pump 126. By closure of the fifth valve 142 and opening of the third valve 136, the working fluid is directed from the condenser 120 and to the first pump 126 for pressurization. Thereafter, the working fluid proceeds to the first recuperator 118 and then to the first heat exchanger 102.


Although described as two-way control valves, it will be appreciated that the valves 130, 132, 136, 140, 142 may be provided by any suitable type of valve. For example, the second and fourth valves 132, 140 may function to stop back-flow into inactive portions of the heat engine system 100. More particularly, in an exemplary embodiment, the fifth valve 142 prevents fluid from flowing through the second pump 117 and to the fourth valve 140, while the first valve 130 prevents fluid from flowing through the second recuperator 128, second heat exchanger 104, and drive turbine 122 to the second valve 132. The function of the second and fourth valves 132, 140, thus, is to prevent reverse flow into the inactive components. As such, the second and fourth valves 132, 140 may be one-way check valves. Furthermore, in another configuration, the first and third valves 130, 136, for example, may be combined and replaced with a three-way valve, without departing from the scope of the disclosure. Since a single three-way valve may effectively provide the function of two two-way valves, reference to the first and third valves 130, 136 together is to be construed to literally include a single three-way valve, or a valve with greater than three ways (e.g., four-way), that provides the function described herein.


The heat engine system 100 further contains a power turbine throttle valve 150 fluidly coupled to the working fluid circuit 110 upstream of the inlet of the power turbine 116 and downstream of the outlet of the first heat exchanger 102. The power turbine throttle valve 150 may be configured to modulate, adjust, or otherwise control the flowrate of the working fluid passing into the power turbine 116, thereby providing control of the power turbine 116 and the amount of work energy produced by the power turbine 116. Also, the heat engine system 100 further contains a turbo pump throttle valve 152 fluidly coupled to the working fluid circuit 110 upstream of the inlet of the drive turbine 122 of the turbopump unit 108 and downstream of the outlet of the second heat exchanger 104. The turbo pump throttle valve 152 may be configured to modulate, adjust, or otherwise control the flowrate of the working fluid passing into the drive turbine 122, thereby providing control of the drive turbine 122 and the amount of work energy produced by the drive turbine 122. The power turbine throttle valve 150 and the turbo pump throttle valve 152 may be independently controlled by the process control system (not shown) that is communicably connected, wired and/or wirelessly, with the power turbine throttle valve 150, the turbo pump throttle valve 152, and other components and parts of the heat engine system 100.



FIG. 3 illustrates a flowchart of a method 200 for extracting energy from heat source stream. The method 200 may proceed by operation of one or more embodiments of the heat engine system 100, as described herein with reference to FIGS. 1 and/or 2 and may thus be best understood with continued reference thereto. The method 200 may include operating a heat engine system in a dual-cycle mode, as at 202. The method 200 may further include sensing the temperature or another condition of heat source stream fed to the system, as at 204, for example, as the heat source stream is fed into a first heat exchanger, which is thermally coupled to the heat source (e.g., waste heat source or stream). This may occur prior to, during, or after initiation of operation of the dual-cycle mode at 202. If the temperature of the heat source stream is less than a threshold value, the method 200 may switch the system to operate in a single-cycle mode, as at 206. In some examples, the threshold value of the temperature may be within a range from about 300° C. to about 400° C., more narrowly within a range from about 320° C. to about 380° C., and more narrowly within a range from about 340° C. to about 360° C., such as about 350° C. The sensing at 204 may be iterative, may be polled on a time delay, may operate on an alarm, trigger, or interrupt basis to alert a controller coupled to the system, or may simply result in a display to an operator, who may then toggle the system to the appropriate operating cycle.


Operating the heat engine system in dual-cycle mode, as at 202, may include heating a first mass flow of working fluid in the first heat exchanger thermally coupled to a heat source, as at 302. Operating at 202 may also include expanding the first mass flow in a first expander, as at 304. Operating at 202 may also include heating a second mass flow of working fluid in a second heat exchanger thermally coupled to the heat source, as at 306. Operating at 202 may further include expanding the second mass flow in a second expander, as at 308. Additionally, operating at 202 may include at least partially condensing the first and second mass flows in one or more condensers, as at 310. Operating at 202 may include pressurizing the first mass flow in a first pump, as at 312. Operating at 202 may also include pressurizing the second mass flow in a second pump, as at 314.


In an exemplary embodiment, operating at 202 may include transferring heat from the first mass flow downstream of the first expander and upstream of the condenser to the first mass flow downstream of the first pump and upstream of the first heat exchanger. Further, operating at 202 may also include transferring heat from the second mass flow downstream of the second expander and upstream of the condenser to the second mass flow downstream of the second pump and upstream of the second heat exchanger.


Switching at 204 may include de-activating the second heat exchanger, the second expander, and the first pump, as at 402. Switching at 204 may also include directing the working fluid from the condenser to the second pump, as at 404. Switching at 204 may also include directing the working fluid from the first pump to the first heat exchanger, as at 406. In embodiments including first and second recuperators, switching at 204 may also include de-activating the second recuperator and directing the working fluid from the second pump to the first recuperator.


Exemplary Embodiments

In one or more exemplary embodiments disclosed herein, as depicted in FIGS. 1 and 2, a heat engine system 100 contains a working fluid within a working fluid circuit 110 having a high pressure side and a low pressure side. The working fluid generally contains carbon dioxide and at least a portion of the working fluid circuit 110 contains the working fluid in a supercritical state. The heat engine system 100 further contains a first heat exchanger 102 and a second heat exchanger 104, such that each of the first and second heat exchangers 102, 104 may be fluidly coupled to and in thermal communication with the high pressure side of the working fluid circuit 110, configured to be fluidly coupled to and in thermal communication with a heat source stream 105 (e.g., a waste heat stream), and configured to transfer thermal energy from the heat source stream 105 to the working fluid within the working fluid circuit 110. The heat source stream 105 may flow from or otherwise be derived from a heat source 106, such as a waste heat source or other source of thermal energy. The heat engine system 100 also contains a first expander, such as a power turbine 116, fluidly coupled to and disposed downstream of the first heat exchanger 102 on the high pressure side of the working fluid circuit 110 and a second expander, such as a drive turbine 122, fluidly coupled to and disposed downstream of the second heat exchanger 104 on the high pressure side of the working fluid circuit 110.


The heat engine system 100 further contains a first recuperator 118 and a second recuperator 128 fluidly coupled to the working fluid circuit 110. The first recuperator 118 may be fluidly coupled to and disposed downstream of the power turbine 116 on the low pressure side of the working fluid circuit 110 and fluidly coupled to and disposed upstream of the first heat exchanger 102 on the high pressure side of the working fluid circuit 110. In some embodiments, the first recuperator 118 may be configured to transfer thermal energy from the working fluid received from the power turbine 116 to the working fluid received from the first and second pumps 126, 117 when the heat engine system 100 is in the dual-cycle mode. The second recuperator 128 may be fluidly coupled to and disposed downstream of the drive turbine 122 on the low pressure side of the working fluid circuit 110 and fluidly coupled to and disposed upstream of the second heat exchanger 104 on the high pressure side of the working fluid circuit 110. In some embodiments, the second recuperator 128 may be configured to transfer thermal energy from the working fluid received from the drive turbine 122 to the working fluid received from the first pump 126 when the heat engine system 100 is in dual-cycle mode and is inactive when the heat engine system 100 is in the single-cycle mode.


The heat engine system 100 further contains a condenser 120, a first pump 126, and a second pump 117 fluidly coupled to the working fluid circuit 110. The condenser 120 may be fluidly coupled to and disposed downstream of the first recuperator 118 and the second recuperator 128 on the low pressure side of the working fluid circuit 110. The condenser 120 may be configured to remove thermal energy from the working fluid passing through the low pressure side of the working fluid circuit 110. The condenser 120 may also be configured to control or regulate the temperature of the working fluid circulating through the working fluid circuit 110. The first pump 126 may be fluidly coupled to and disposed downstream of the condenser 120 on the low pressure side of the working fluid circuit 110 and fluidly coupled to and disposed upstream of the first recuperator 118 and the second recuperator 128 on the high pressure side of the working fluid circuit 110. The second pump 117 may be fluidly coupled to and disposed downstream of the condenser 120 on the low pressure side of the working fluid circuit 110 and fluidly coupled to and disposed upstream of the first recuperator 118 on the high pressure side of the working fluid circuit 110. In some exemplary embodiments, the second pump 117 may be a turbopump, the second expander may be the drive turbine 122, and the drive turbine 122 may be coupled to the turbopump and operable to drive the turbopump when the heat engine system 100 is in the dual-cycle mode.


In some exemplary embodiments, the heat engine system 100 further contains a plurality of valves operatively coupled to the working fluid circuit 110 and configured to switch the heat engine system 100 between a dual-cycle mode and a single-cycle mode. In the dual-cycle mode, the first and second heat exchangers 102, 104 and the first and second pumps 126, 117 are active as the working fluid is circulated throughout the working fluid circuit 110. However, in the single-cycle mode, the first heat exchanger 102 and the power turbine 116 are active and at least the second heat exchanger 104 and the second pump 117 are inactive as the working fluid is circulated throughout the working fluid circuit 110.


In other exemplary embodiments, the plurality of valves may include five or more valves operatively coupled to the working fluid circuit 110 for controlling the flow of the working fluid. A first valve 130 may be operatively coupled to the high pressure side of the working fluid circuit 110 and disposed downstream of the first pump 126 and upstream of the second recuperator 128. A second valve 132 may be operatively coupled to the low pressure side of the working fluid circuit 110 and disposed downstream of the second recuperator 128 and upstream of the condenser 120. A third valve 136 may be operatively coupled to the high pressure side of the working fluid circuit 110 and disposed downstream of the first pump 126 and upstream of the first recuperator 118. A fourth valve 140 may be operatively coupled to the high pressure side of the working fluid circuit 110 and disposed downstream of the second pump 117 and upstream of the first recuperator 118. A fifth valve 142 may be operatively coupled to the low pressure side of the working fluid circuit 110 and disposed downstream of the condenser 120 and upstream of the second pump 117.


In some examples, the plurality of valves may include a valve, such as the fourth valve 140, disposed between the condenser 120 and the second pump 117, wherein the fourth valve 140 is closed when the heat engine system 100 is in the single-cycle mode and the fourth valve 140 is open when the heat engine system 100 is in the dual-cycle mode. In other examples, the plurality of valves may include a valve, such as the third valve 136, disposed between the first pump 126 and the first recuperator 118, the third valve 136 may be configured to prohibit flow of the working fluid from the first pump 126 to the first recuperator 118 when the heat engine system 100 is in the dual-cycle mode and to allow fluid flow therebetween when the heat engine system 100 is in the single-cycle mode.


In some examples, the working fluid from the low pressure side of the first recuperator 118 and the working fluid from the low pressure side of the second recuperator 128 combine at a point 134 on the low pressure side of the working fluid circuit 110, such that the point 134 may be disposed upstream of the condenser 120 and downstream of the second valve 132. In some configurations, each of the first, second, fourth, and fifth valves 130, 132, 140, 142 may be in an opened-position and the third valve 136 may be in a closed-position when the heat engine system 100 is in the dual-cycle mode. Alternatively, when the heat engine system 100 is in the single-cycle mode, each of the first, second, fourth, and fifth valves 130, 132, 140, 142 may be in a closed-position and the third valve 136 may be in an opened-position.


In other embodiments disclosed herein, the plurality of valves may be configured to actuate in response to a change in temperature of the heat source stream 105. For example, when the temperature of the heat source stream 105 becomes less than a threshold value, the plurality of valves may be configured to switch the heat engine system 100 to the single-cycle mode. Also, when the temperature of the heat source stream 105 becomes equal to or greater than the threshold value, the plurality of valves may be configured to switch the heat engine system 100 to the dual-cycle mode. In some examples, the threshold value of the temperature of the heat source stream 105 is within a range from about 300° C. to about 400° C., such as about 350° C.


In other embodiments disclosed herein, the plurality of valves may be configured to switch the heat engine system 100 between the dual-cycle mode and the single-cycle mode, such that in the dual-cycle mode, the plurality of valves may be configured to direct the working fluid from the condenser 120 to the first and second pumps 126, 117, and subsequently, direct the working fluid from the first pump 126 to the second heat exchanger 104 and/or direct the working fluid from the second pump 117 to the first heat exchanger 102. In the single-cycle mode, the plurality of valves may be configured to direct the working fluid from the condenser 120 to the first pump 126 and from the first pump 126 to the first heat exchanger 102, and to substantially cut-off or stop the flow of the working fluid to the second pump 117, the second heat exchanger 104, and the drive turbine 122.


In one or more embodiments disclosed herein, a method for recovering energy from a heat source (e.g., waste heat source) is provided and includes operating a heat engine system 100 in a dual-cycle mode and subsequently switching the heat engine system 100 from the dual-cycle mode to a single-cycle mode. In the dual-cycle mode, the method includes operating the heat engine system 100 by heating a first mass flow of a working fluid in the first heat exchanger 102 fluidly coupled to and in thermal communication with a working fluid circuit 110 and a heat source stream 105 and expanding the first mass flow in a power turbine 116 fluidly coupled to the first heat exchanger 102 via the working fluid circuit 110. The first heat exchanger 102 may be configured to transfer thermal energy from the heat source stream 105 to the first mass flow of the working fluid within the working fluid circuit 110. In many exemplary embodiments, the working fluid contains carbon dioxide and at least a portion of the working fluid circuit 110 contains the working fluid in a supercritical state.


Also, in the dual-cycle mode, the method includes heating a second mass flow of the working fluid in the second heat exchanger 104 fluidly coupled to and in thermal communication with the working fluid circuit 110 and the heat source stream 105 and expanding the second mass flow in a second expander, such as the drive turbine 122, fluidly coupled to the second heat exchanger 104 via the working fluid circuit 110. The second heat exchanger 104 may be configured to transfer thermal energy from the heat source stream 105 to the second mass flow of the working fluid within the working fluid circuit 110. The method further includes, in the dual-cycle mode, at least partially condensing the first and second mass flows in one or more condensers, such as the condenser 120, fluidly coupled to the working fluid circuit 110, pressurizing the first mass flow in a first pump 126 fluidly coupled to the condenser 120 via the working fluid circuit 110, and pressurizing the second mass flow in a second pump 117 fluidly coupled to the condenser 120 via the working fluid circuit 110.


In the single-cycle mode, the method includes operating the heat engine system 100 by de-activating the second heat exchanger 104, the drive turbine 122, and the second pump 117, directing the working fluid from the condenser 120 to the first pump 126, and directing the working fluid from the first pump 126 to the first heat exchanger 102. The method may include de-activating the second recuperator 128 and directing the working fluid from the second pump 117 to the first recuperator 118 while switching to the single-cycle mode.


In other embodiments, the method includes operating the heat engine system 100 in the dual-cycle mode by further transferring heat via the first recuperator 118 from the first mass flow “m1” downstream of the power turbine 116 and upstream of the condenser 120 to the first mass flow m1 downstream of the second pump 117 and upstream of the first heat exchanger 102, transferring heat via the second recuperator 128 from the second mass flow “m2” downstream of the drive turbine 122 and upstream of the condenser 120 to the second mass flow m2 downstream of the first pump 126 and upstream of the second heat exchanger 104, and switching to the single-cycle mode further includes de-activating the second recuperator 128 and directing the working fluid from the second pump 117 to the first recuperator 118.


In some embodiments, the method further includes monitoring a temperature of the heat source stream 105, operating the heat engine system 100 in the dual-cycle mode when the temperature is equal to or greater than a threshold value, and subsequently, operating the heat engine system 100 in the single-cycle mode when the temperature is less than the threshold value. In some examples, the threshold value of the temperature of the heat source stream 105 is within a range from about 300° C. to about 400° C., such as about 350° C. In one aspect, the method may include automatically switching from operating the heat engine system 100 in the dual-cycle mode to operating the heat engine system 100 in the single-cycle mode with a programmable controller once the temperature is less than the threshold value. In another aspect, the method may include manually switching from operating the heat engine system 100 in the dual-cycle mode to operating the heat engine system 100 in the single-cycle mode once the temperature is less than the threshold value.


It is to be understood that the present disclosure describes several exemplary embodiments for implementing different features, structures, or functions of the disclosure. Exemplary embodiments of components, arrangements, and configurations are described herein to simplify the present disclosure; however, these exemplary embodiments are provided merely as examples and are not intended to limit the scope of the invention. Additionally, the present disclosure may repeat reference numerals and/or letters in the various exemplary embodiments and across the Figures provided herein. This repetition is for the purpose of simplicity and clarity and does not in itself dictate a relationship between the various exemplary embodiments and/or configurations discussed in the various Figures. Moreover, the formation of a first feature over or on a second feature in the present disclosure may include embodiments in which the first and second features are formed in direct contact, and may also include embodiments in which additional features may be formed interposing the first and second features, such that the first and second features may not be in direct contact. Finally, the exemplary embodiments described herein may be combined in any combination of ways, e.g., any element from one exemplary embodiment may be used in any other exemplary embodiment without departing from the scope of the disclosure.


Additionally, certain terms are used throughout the written description and claims for referring to particular components. As one skilled in the art will appreciate, various entities may refer to the same component by different names, and as such, the naming convention for the elements described herein is not intended to limit the scope of the disclosure, unless otherwise specifically defined herein. Further, the naming convention used herein is not intended to distinguish between components that differ in name but not function. Further, in the written description and the claims, the terms “including,” “containing,” and “comprising” are used in an open-ended fashion, and thus should be interpreted to mean “including, but not limited to”. All numerical values in this disclosure may be exact or approximate values unless otherwise specifically stated. Accordingly, various embodiments of the disclosure may deviate from the numbers, values, and ranges disclosed herein without departing from the intended scope. Furthermore, as it is used in the claims or specification, the term “or” is intended to encompass both exclusive and inclusive cases, i.e., “A or B” is intended to be synonymous with “at least one of A and B,” unless otherwise expressly specified herein.


The foregoing has outlined features of several embodiments so that those skilled in the art may better understand the present disclosure. Those skilled in the art should appreciate that they may readily use the present disclosure as a basis for designing or modifying other processes and structures for carrying out the same purposes and/or achieving the same advantages of the embodiments introduced herein. Those skilled in the art should also realize that such equivalent constructions do not depart from the spirit and scope of the present disclosure, and that they may make various changes, substitutions and alterations herein without departing from the spirit and scope of the present disclosure.

Claims
  • 1. A heat engine system, comprising: a working fluid circuit comprising a working fluid, wherein the working fluid comprises carbon dioxide and at least a portion of the working fluid circuit contains the working fluid in a supercritical state;a first heat exchanger fluidly coupled to and in thermal communication with the working fluid circuit, configured to be fluidly coupled to and in thermal communication with a heat source stream, and configured to transfer thermal energy from the heat source stream to the working fluid within the working fluid circuit;a second heat exchanger fluidly coupled to and in thermal communication with the working fluid circuit, configured to be fluidly coupled to and in thermal communication with the heat source stream, and configured to transfer thermal energy from the heat source stream to the working fluid within the working fluid circuit;a first expander fluidly coupled to the working fluid circuit and the first heat exchanger and disposed downstream of the first heat exchanger;a second expander fluidly coupled to the working fluid circuit and the second heat exchanger and disposed downstream of the second heat exchanger;a first recuperator fluidly coupled to the working fluid circuit, the first expander, and the first heat exchanger, the first recuperator disposed downstream of the first expander and upstream of the first heat exchanger;a second recuperator fluidly coupled to the working fluid circuit, the second expander, and the second heat exchanger, the second recuperator disposed downstream of the second expander and upstream of the second heat exchanger;a condenser fluidly coupled to the working fluid circuit and the first and second recuperators and disposed downstream of the first and second recuperators;a first pump fluidly coupled to the working fluid circuit, the condenser, and the first and second recuperators, the first pump disposed downstream of the condenser and upstream of the first and second recuperators;a second pump fluidly coupled to the working fluid circuit, the condenser, and the first recuperator, the second pump disposed downstream of the condenser and upstream of the first recuperator; anda plurality of valves operatively coupled to the working fluid circuit and configured to switch the heat engine system between a dual-cycle mode, in which the first and second heat exchangers and the first and second pumps are active, and a single-cycle mode, in which the first heat exchanger and the first expander are active and at least the second heat exchanger and the second pump are inactive,wherein the second pump is a turbopump, the second expander is a drive turbine, and the drive turbine is coupled to the turbopump and operable to drive the turbopump when the heat engine system is in the dual-cycle mode.
  • 2. The heat engine system of claim 1, wherein the plurality of valves includes a valve disposed between the condenser and the second pump, wherein the valve is closed during the single-cycle mode of the heat engine system and the valve is open when the heat engine system is in the dual-cycle mode.
  • 3. The heat engine system of claim 1, wherein the plurality of valves includes a valve disposed between the first pump and the first recuperator, the valve configured to prohibit flow of the working fluid from the first pump to the first recuperator during the dual-cycle mode of the heat engine system and to allow flow of the working fluid therebetween during the single-cycle mode of the heat engine system.
  • 4. The heat engine system of claim 1, wherein the plurality of valves further comprises: a first valve operatively coupled to the working fluid circuit, disposed downstream of the first pump, and disposed upstream of the second recuperator;a second valve operatively coupled to the working fluid circuit, disposed downstream of the second recuperator, and disposed upstream of the condenser;a third valve operatively coupled to the working fluid circuit, disposed downstream of the first pump, and disposed upstream of the first recuperator;a fourth valve operatively coupled to the working fluid circuit, disposed downstream of the second pump, and disposed upstream of the first recuperator; anda fifth valve operatively coupled to the working fluid circuit, disposed downstream of the condenser, and disposed upstream of the second pump.
  • 5. The heat engine system of claim 4, wherein each of the first, second, fourth, and fifth valves is in an opened-position during the dual-cycle mode of the heat engine system and a closed-position during the single-cycle mode of the heat engine system, and the third valve is in an opened-position during the single-cycle mode of the heat engine system and a closed-position during the dual-cycle mode of the heat engine system.
  • 6. The heat engine system of claim 4, further comprising a point on the working fluid circuit disposed downstream of the first and second recuperators and disposed upstream of the condenser, wherein the second valve is disposed upstream of the point and downstream of the second recuperator.
  • 7. A heat engine system, comprising: a working fluid circuit comprising a working fluid, wherein the working fluid comprises carbon dioxide and at least a portion of the working fluid circuit contains the working fluid in a supercritical state;a first heat exchanger fluidly coupled to and in thermal communication with the working fluid circuit, configured to be fluidly coupled to and in thermal communication with a heat source stream, and configured to transfer thermal energy from the heat source stream to the working fluid within the working fluid circuit;a second heat exchanger fluidly coupled to and in thermal communication with the working fluid circuit, configured to be fluidly coupled to and in thermal communication with the heat source stream, and configured to transfer thermal energy from the heat source stream to the working fluid within the working fluid circuit;a first expander fluidly coupled to the working fluid circuit and the first heat exchanger and disposed downstream of the first heat exchanger;a second expander fluidly coupled to the working fluid circuit and the second heat exchanger and disposed downstream of the second heat exchanger;a first recuperator fluidly coupled to the working fluid circuit, the first expander, and the first heat exchanger, the first recuperator disposed downstream of the first expander and upstream of the first heat exchanger;a second recuperator fluidly coupled to the working fluid circuit, the second expander, and the second heat exchanger, the second recuperator disposed downstream of the second expander and upstream of the second heat exchanger;a condenser fluidly coupled to the working fluid circuit and the first and second recuperators and disposed downstream of the first and second recuperators;a first pump fluidly coupled to the working fluid circuit, the condenser, and the first and second recuperators, the first pump disposed downstream of the condenser and upstream of the first and second recuperators;a second pump fluidly coupled to the working fluid circuit, the condenser, and the first recuperator, the second pump disposed downstream of the condenser and upstream of the first recuperator; anda plurality of valves operatively coupled to the working fluid circuit and configured to switch the heat engine system between a single-cycle mode and a dual-cycle mode, wherein the plurality of valves further comprises: a first valve operatively coupled to the working fluid circuit, disposed downstream of the first pump, and disposed upstream of the second recuperator;a second valve operatively coupled to the working fluid circuit, disposed downstream of the second recuperator, and disposed upstream of the condenser;a third valve operatively coupled to the working fluid circuit, disposed downstream of the first pump, and disposed upstream of the first recuperator;a fourth valve operatively coupled to the working fluid circuit, disposed downstream of the second pump, and disposed upstream of the first recuperator; anda fifth valve operatively coupled to the working fluid circuit, disposed downstream of the condenser, and disposed upstream of the second pump,wherein each of the first, second, fourth, and fifth valves is in an opened-position during the dual-cycle mode of the heat engine system and a closed-position during the single-cycle mode of the heat engine system, and the third valve is in an opened-position during the single-cycle mode of the heat engine system and a closed-position during the dual-cycle mode of the heat engine system.
  • 8. The heat engine system of claim 7, further comprising a point on the working fluid circuit disposed downstream of the first and second recuperators and disposed upstream of the condenser, wherein the second valve is disposed upstream of the point and downstream of the second recuperator.
  • 9. The heat engine system of claim 7, wherein the second pump is a turbopump, the second expander is a drive turbine, and the drive turbine is coupled to the turbopump and operable to drive the turbopump during the dual-cycle mode of the heat engine system.
  • 10. A method for recovering energy from a heat source, comprising: operating a heat engine system in a dual-cycle mode, comprising: heating a first mass flow of a working fluid in a first heat exchanger fluidly coupled to and in thermal communication with a working fluid circuit and a heat source stream, wherein the first heat exchanger is configured to transfer thermal energy from the heat source stream to the first mass flow of the working fluid within the working fluid circuit, the working fluid comprises carbon dioxide, and at least a portion of the working fluid circuit contains the working fluid in a supercritical state;expanding the first mass flow in a first expander fluidly coupled to the first heat exchanger via the working fluid circuit;heating a second mass flow of the working fluid in a second heat exchanger fluidly coupled to and in thermal communication with the working fluid circuit and the heat source stream, wherein the second heat exchanger is configured to transfer thermal energy from the heat source stream to the second mass flow of the working fluid within the working fluid circuit;expanding the second mass flow in a second expander fluidly coupled to the second heat exchanger via the working fluid circuit;at least partially condensing the first and second mass flows in one or more condensers fluidly coupled to the working fluid circuit;pressurizing the first mass flow in a first pump fluidly coupled to the condenser via the working fluid circuit;pressurizing the second mass flow in a second pump fluidly coupled to the condenser via the working fluid circuit;transferring heat via a first recuperator from the first mass flow downstream of the first expander and upstream of the condenser to the first mass flow downstream of the second pump and upstream of the first heat exchanger; andtransferring heat via a second recuperator from the second mass flow downstream of the second expander and upstream of the condenser to the second mass flow downstream of the first pump and upstream of the second heat exchanger; andswitching the heat engine system from the dual-cycle mode to a single-cycle mode, comprising: de-activating the second heat exchanger, the second expander, and the second pump;directing the working fluid from the condenser to the first pump;directing the working fluid from the first pump to the first heat exchanger; andde-activating the second recuperator and directing the working fluid from the second pump to the first recuperator.
  • 11. The method of claim 10, further comprising: monitoring a temperature of the heat source stream;operating the heat engine system in the dual-cycle mode when the temperature is equal to or greater than a threshold value; andoperating the heat engine system in the single-cycle mode when the temperature is less than the threshold value.
  • 12. The method of claim 11, further comprising automatically switching from operating the heat engine system in the dual-cycle mode to operating the heat engine system in the single-cycle mode with a programmable controller once the temperature is less than the threshold value, wherein the threshold value of the temperature is within a range from 300° C. to 400° C.
  • 13. The method of claim 11, further comprising manually switching from operating the heat engine system in the dual-cycle mode to operating the heat engine system in the single-cycle mode once the temperature is less than the threshold value, wherein the threshold value of the temperature is within a range from 300° C. to 400° C.
CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims benefit of U.S. Prov. Appl. No. 61/712,907, entitled “Supercritical Carbon Dioxide Power Cycle for Waste Heat Recovery,” and filed Oct. 12, 2012, which is incorporated herein by reference in its entirety to the extent consistent with the present application.

US Referenced Citations (399)
Number Name Date Kind
2575478 Wilson Nov 1951 A
2634375 Guimbal Apr 1953 A
2691280 Albert Oct 1954 A
3095274 Crawford Jun 1963 A
3105748 Stahl Oct 1963 A
3237403 Feher Mar 1966 A
3277955 Laszlo Oct 1966 A
3401277 Larson Sep 1968 A
3622767 Koepcke Nov 1971 A
3630022 Jubb Dec 1971 A
3736745 Karig Jun 1973 A
3772879 Engdahl Nov 1973 A
3791137 Jubb Feb 1974 A
3830062 Morgan et al. Aug 1974 A
3939328 Davis Feb 1976 A
3971211 Wethe Jul 1976 A
3982379 Gilli Sep 1976 A
3998058 Park Dec 1976 A
4009575 Hartman, Jr. Mar 1977 A
4029255 Heiser Jun 1977 A
4030312 Wallin Jun 1977 A
4049407 Bottum Sep 1977 A
4070870 Bahel Jan 1978 A
4099381 Rappoport Jul 1978 A
4119140 Cates Oct 1978 A
4150547 Hobson Apr 1979 A
4152901 Munters May 1979 A
4164848 Gilli Aug 1979 A
4164849 Mangus Aug 1979 A
4170435 Swearingen Oct 1979 A
4182960 Reuyl Jan 1980 A
4183220 Shaw Jan 1980 A
4198827 Terry et al. Apr 1980 A
4208882 Lopes Jun 1980 A
4221185 Scholes Sep 1980 A
4233085 Roderick Nov 1980 A
4236869 Laurello Dec 1980 A
4248049 Briley Feb 1981 A
4257232 Bell Mar 1981 A
4287430 Guido Sep 1981 A
4336692 Ecker Jun 1982 A
4347711 Noe Sep 1982 A
4347714 Kinsell Sep 1982 A
4372125 Dickenson Feb 1983 A
4384568 Palmatier May 1983 A
4391101 Labbe Jul 1983 A
4420947 Yoshino Dec 1983 A
4428190 Bronicki Jan 1984 A
4433554 Rojey Feb 1984 A
4439687 Wood Mar 1984 A
4439994 Briley Apr 1984 A
4448033 Briccetti May 1984 A
4450363 Russell May 1984 A
4455836 Binstock Jun 1984 A
4467609 Loomis Aug 1984 A
4467621 O'Brien Aug 1984 A
4475353 Lazare Oct 1984 A
4489562 Snyder Dec 1984 A
4489563 Kalina Dec 1984 A
4498289 Osgerby Feb 1985 A
4516403 Tanaka May 1985 A
4538960 Iino et al. Sep 1985 A
4549401 Spliethoff Oct 1985 A
4555905 Endou Dec 1985 A
4558228 Larjola Dec 1985 A
4573321 Knaebel Mar 1986 A
4578953 Krieger Apr 1986 A
4589255 Martens May 1986 A
4636578 Feinberg Jan 1987 A
4674297 Vobach Jun 1987 A
4694189 Haraguchi Sep 1987 A
4697981 Brown et al. Oct 1987 A
4700543 Krieger Oct 1987 A
4730977 Haaser Mar 1988 A
4756162 Dayan Jul 1988 A
4765143 Crawford Aug 1988 A
4773212 Griffin Sep 1988 A
4798056 Franklin Jan 1989 A
4813242 Wicks Mar 1989 A
4821514 Schmidt Apr 1989 A
4867633 Gravelle Sep 1989 A
4892459 Guelich Jan 1990 A
4986071 Voss Jan 1991 A
4993483 Harris Feb 1991 A
5000003 Wicks Mar 1991 A
5050375 Dickinson Sep 1991 A
5083425 Hendriks et al. Jan 1992 A
5098194 Kuo Mar 1992 A
5102295 Pope Apr 1992 A
5104284 Hustak, Jr. et al. Apr 1992 A
5164020 Wagner Nov 1992 A
5176321 Doherty Jan 1993 A
5203159 Koizumi Apr 1993 A
5228310 Vandenberg Jul 1993 A
5291960 Brandenburg Mar 1994 A
5320482 Palmer et al. Jun 1994 A
5335510 Rockenfeller Aug 1994 A
5358378 Holscher Oct 1994 A
5360057 Rockenfeller Nov 1994 A
5392606 Labinov Feb 1995 A
5440882 Kalina Aug 1995 A
5444972 Moore Aug 1995 A
5483797 Rigal et al. Jan 1996 A
5488828 Brossard Feb 1996 A
5490386 Keller Feb 1996 A
5503222 Dunne Apr 1996 A
5531073 Bronicki Jul 1996 A
5538564 Kaschmitter Jul 1996 A
5542203 Luoma Aug 1996 A
5570578 Saujet Nov 1996 A
5588298 Kalina Dec 1996 A
5600967 Meckler Feb 1997 A
5634340 Grennan Jun 1997 A
5647221 Garris, Jr. Jul 1997 A
5649426 Kalina Jul 1997 A
5676382 Dahlheimer Oct 1997 A
5680753 Hollinger Oct 1997 A
5738164 Hildebrand Apr 1998 A
5754613 Hashiguchi May 1998 A
5771700 Cochran Jun 1998 A
5789822 Calistrat Aug 1998 A
5813215 Weisser Sep 1998 A
5833876 Schnur Nov 1998 A
5862666 Liu Jan 1999 A
5873260 Linhardt Feb 1999 A
5874039 Edelson Feb 1999 A
5894836 Wu Apr 1999 A
5899067 Hageman May 1999 A
5903060 Norton May 1999 A
5918460 Connell Jul 1999 A
5941238 Tracy Aug 1999 A
5943869 Cheng Aug 1999 A
5946931 Lomax Sep 1999 A
5973050 Johnson Oct 1999 A
6037683 Lulay Mar 2000 A
6041604 Nicodemus Mar 2000 A
6058930 Shingleton May 2000 A
6062815 Holt May 2000 A
6065280 Ranasinghe May 2000 A
6066797 Toyomura May 2000 A
6070405 Jerye Jun 2000 A
6082110 Rosenblatt Jul 2000 A
6105368 Hansen Aug 2000 A
6112547 Spauschus Sep 2000 A
6129507 Ganelin Oct 2000 A
6158237 Riffat Dec 2000 A
6164655 Bothien Dec 2000 A
6202782 Hatanaka Mar 2001 B1
6223846 Schechter May 2001 B1
6233938 Nicodemus May 2001 B1
6282900 Bell Sep 2001 B1
6282917 Mongan Sep 2001 B1
6295818 Ansley Oct 2001 B1
6299690 Mongeon Oct 2001 B1
6341781 Matz Jan 2002 B1
6374630 Jones Apr 2002 B1
6393851 Wightman May 2002 B1
6432320 Bonsignore Aug 2002 B1
6434955 Ng Aug 2002 B1
6442951 Maeda Sep 2002 B1
6446425 Lawlor Sep 2002 B1
6446465 Dubar Sep 2002 B1
6463730 Keller Oct 2002 B1
6484490 Olsen Nov 2002 B1
6539720 Rouse et al. Apr 2003 B2
6539728 Korin Apr 2003 B2
6571548 Bronicki Jun 2003 B1
6581384 Benson Jun 2003 B1
6598397 Hanna Jul 2003 B2
6644062 Hays Nov 2003 B1
6657849 Andresakis Dec 2003 B1
6668554 Brown Dec 2003 B1
6684625 Kline Feb 2004 B2
6695974 Withers Feb 2004 B2
6715294 Anderson Apr 2004 B2
6734585 Tornquist May 2004 B2
6735948 Kalina May 2004 B1
6739142 Korin May 2004 B2
6751959 McClanahan et al. Jun 2004 B1
6769256 Kalina Aug 2004 B1
6799892 Leuthold Oct 2004 B2
6808179 Bhattacharyya Oct 2004 B1
6810335 Lysaght Oct 2004 B2
6817185 Coney Nov 2004 B2
6857268 Stinger Feb 2005 B2
6910334 Kalina Jun 2005 B2
6918254 Baker Jul 2005 B2
6921518 Johnston Jul 2005 B2
6941757 Kalina Sep 2005 B2
6960839 Zimron Nov 2005 B2
6960840 Willis Nov 2005 B2
6962054 Linney Nov 2005 B1
6964168 Pierson Nov 2005 B1
6968690 Kalina Nov 2005 B2
6986251 Radcliff Jan 2006 B2
7013205 Hafner et al. Mar 2006 B1
7021060 Kalina Apr 2006 B1
7022294 Johnston Apr 2006 B2
7033533 Lewis-Aburn et al. Apr 2006 B2
7036315 Kang May 2006 B2
7041272 Keefer May 2006 B2
7047744 Robertson May 2006 B1
7048782 Couch May 2006 B1
7062913 Christensen Jun 2006 B2
7096665 Stinger Aug 2006 B2
7096679 Manole Aug 2006 B2
7124587 Linney Oct 2006 B1
7174715 Armitage Feb 2007 B2
7194863 Ganev Mar 2007 B2
7197876 Kalina Apr 2007 B1
7200996 Cogswell Apr 2007 B2
7234314 Wiggs Jun 2007 B1
7249588 Russell Jul 2007 B2
7278267 Yamada Oct 2007 B2
7279800 Bassett Oct 2007 B2
7287381 Pierson Oct 2007 B1
7305829 Mirolli Dec 2007 B2
7313926 Gurin Jan 2008 B2
7340894 Miyahara et al. Mar 2008 B2
7340897 Zimron Mar 2008 B2
7406830 Valentian Aug 2008 B2
7416137 Hagen et al. Aug 2008 B2
7453242 Ichinose Nov 2008 B2
7458217 Kalina Dec 2008 B2
7458218 Kalina Dec 2008 B2
7464551 Althaus et al. Dec 2008 B2
7469542 Kalina Dec 2008 B2
7516619 Pelletier Apr 2009 B2
7600394 Kalina Oct 2009 B2
7621133 Tomlinson Nov 2009 B2
7654354 Otterstrom Feb 2010 B1
7665291 Anand Feb 2010 B2
7665304 Sundel Feb 2010 B2
7685821 Kalina Mar 2010 B2
7730713 Nakano Jun 2010 B2
7735335 Uno Jun 2010 B2
7770376 Brostmeyer Aug 2010 B1
7775758 Legare Aug 2010 B2
7827791 Pierson Nov 2010 B2
7838470 Shaw Nov 2010 B2
7841179 Kalina Nov 2010 B2
7841306 Myers Nov 2010 B2
7854587 Ito Dec 2010 B2
7866157 Ernst Jan 2011 B2
7900450 Gurin Mar 2011 B2
7950230 Nishikawa May 2011 B2
7950243 Gurin May 2011 B2
7972529 Machado Jul 2011 B2
7997076 Ernst Aug 2011 B2
8096128 Held et al. Jan 2012 B2
8099198 Gurin Jan 2012 B2
8146360 Myers Apr 2012 B2
8281593 Held Oct 2012 B2
8419936 Berger et al. Apr 2013 B2
8544274 Ernst Oct 2013 B2
20010015061 Viteri et al. Aug 2001 A1
20010020444 Johnston Sep 2001 A1
20010030952 Roy Oct 2001 A1
20020029558 Tamaro Mar 2002 A1
20020066270 Rouse et al. Jun 2002 A1
20020078696 Korin Jun 2002 A1
20020078697 Lifson Jun 2002 A1
20020082747 Kramer Jun 2002 A1
20030000213 Christensen Jan 2003 A1
20030061823 Alden Apr 2003 A1
20030154718 Nayar Aug 2003 A1
20030182946 Sami Oct 2003 A1
20030213246 Coll et al. Nov 2003 A1
20030221438 Rane et al. Dec 2003 A1
20040011038 Stinger Jan 2004 A1
20040011039 Stinger et al. Jan 2004 A1
20040020185 Brouillette et al. Feb 2004 A1
20040020206 Sullivan et al. Feb 2004 A1
20040021182 Green et al. Feb 2004 A1
20040035117 Rosen Feb 2004 A1
20040083731 Lasker May 2004 A1
20040083732 Hanna et al. May 2004 A1
20040088992 Brasz et al. May 2004 A1
20040097388 Brask et al. May 2004 A1
20040105980 Sudarshan et al. Jun 2004 A1
20040107700 McClanahan et al. Jun 2004 A1
20040159110 Janssen Aug 2004 A1
20040211182 Gould Oct 2004 A1
20050022963 Garrabrant et al. Feb 2005 A1
20050056001 Frutschi Mar 2005 A1
20050096676 Gifford, III et al. May 2005 A1
20050109387 Marshall May 2005 A1
20050137777 Kolavennu et al. Jun 2005 A1
20050162018 Realmuto et al. Jul 2005 A1
20050167169 Gering et al. Aug 2005 A1
20050183421 Vaynberg et al. Aug 2005 A1
20050196676 Singh et al. Sep 2005 A1
20050198959 Schubert Sep 2005 A1
20050227187 Schilling Oct 2005 A1
20050252235 Critoph et al. Nov 2005 A1
20050257812 Wright et al. Nov 2005 A1
20060010868 Smith Jan 2006 A1
20060060333 Chordia et al. Mar 2006 A1
20060066113 Ebrahim et al. Mar 2006 A1
20060080960 Rajendran et al. Apr 2006 A1
20060112693 Sundel Jun 2006 A1
20060182680 Keefer et al. Aug 2006 A1
20060211871 Dai et al. Sep 2006 A1
20060213218 Uno et al. Sep 2006 A1
20060225421 Yamanaka et al. Oct 2006 A1
20060225459 Meyer Oct 2006 A1
20060249020 Tonkovich et al. Nov 2006 A1
20060254281 Badeer et al. Nov 2006 A1
20070001766 Ripley et al. Jan 2007 A1
20070017192 Bednarek et al. Jan 2007 A1
20070019708 Shiflett et al. Jan 2007 A1
20070027038 Kamimura et al. Feb 2007 A1
20070056290 Dahm Mar 2007 A1
20070089449 Gurin Apr 2007 A1
20070108200 McKinzie, II May 2007 A1
20070119175 Ruggieri et al. May 2007 A1
20070130952 Copen Jun 2007 A1
20070151244 Gurin Jul 2007 A1
20070161095 Gurin Jul 2007 A1
20070163261 Strathman Jul 2007 A1
20070195152 Kawai et al. Aug 2007 A1
20070204620 Pronske et al. Sep 2007 A1
20070227472 Takeuchi et al. Oct 2007 A1
20070234722 Kalina Oct 2007 A1
20070245733 Pierson et al. Oct 2007 A1
20070246206 Gong et al. Oct 2007 A1
20080000225 Kalina Jan 2008 A1
20080006040 Peterson et al. Jan 2008 A1
20080010967 Griffin et al. Jan 2008 A1
20080023666 Gurin Jan 2008 A1
20080053095 Kalina Mar 2008 A1
20080066470 MacKnight Mar 2008 A1
20080135253 Vinegar et al. Jun 2008 A1
20080163625 O'Brien Jul 2008 A1
20080173450 Goldberg et al. Jul 2008 A1
20080211230 Gurin Sep 2008 A1
20080250789 Myers et al. Oct 2008 A1
20080252078 Myers Oct 2008 A1
20090021251 Simon Jan 2009 A1
20090085709 Meinke Apr 2009 A1
20090107144 Moghtaderi et al. Apr 2009 A1
20090139234 Gurin Jun 2009 A1
20090139781 Straubel Jun 2009 A1
20090173337 Tamaura et al. Jul 2009 A1
20090173486 Copeland Jul 2009 A1
20090180903 Martin et al. Jul 2009 A1
20090205892 Jensen et al. Aug 2009 A1
20090211251 Peterson et al. Aug 2009 A1
20090211253 Radcliff et al. Aug 2009 A1
20090266075 Westmeier et al. Oct 2009 A1
20090293503 Vandor Dec 2009 A1
20100024421 Litwin Feb 2010 A1
20100077792 Gurin Apr 2010 A1
20100083662 Kalina Apr 2010 A1
20100102008 Hedberg Apr 2010 A1
20100122533 Kalina May 2010 A1
20100146949 Stobart et al. Jun 2010 A1
20100146973 Kalina Jun 2010 A1
20100156112 Held et al. Jun 2010 A1
20100162721 Welch et al. Jul 2010 A1
20100205962 Kalina Aug 2010 A1
20100218513 Vaisman et al. Sep 2010 A1
20100218930 Proeschel Sep 2010 A1
20100263380 Biederman et al. Oct 2010 A1
20100287934 Glynn et al. Nov 2010 A1
20100300093 Doty Dec 2010 A1
20100326076 Ast et al. Dec 2010 A1
20110027064 Pal et al. Feb 2011 A1
20110030404 Gurin Feb 2011 A1
20110048012 Ernst et al. Mar 2011 A1
20110061384 Held et al. Mar 2011 A1
20110061387 Held et al. Mar 2011 A1
20110088399 Briesch et al. Apr 2011 A1
20110179799 Allam et al. Jul 2011 A1
20110185729 Held Aug 2011 A1
20110192163 Kasuya Aug 2011 A1
20110203278 Kopecek et al. Aug 2011 A1
20110259010 Bronicki et al. Oct 2011 A1
20110299972 Morris Dec 2011 A1
20110308253 Ritter Dec 2011 A1
20120047892 Held et al. Mar 2012 A1
20120067055 Held Mar 2012 A1
20120128463 Held May 2012 A1
20120131918 Held May 2012 A1
20120131919 Held May 2012 A1
20120131920 Held May 2012 A1
20120131921 Held May 2012 A1
20120159922 Gurin Jun 2012 A1
20120159956 Gurin Jun 2012 A1
20120174558 Gurin Jul 2012 A1
20120186219 Gurin Jul 2012 A1
20120247134 Gurin Oct 2012 A1
20120247455 Gurin et al. Oct 2012 A1
20120261090 Durmaz et al. Oct 2012 A1
20120306206 Agrawal et al. Dec 2012 A1
20130019597 Kalina Jan 2013 A1
20130033037 Held et al. Feb 2013 A1
20130036736 Hart et al. Feb 2013 A1
20130113221 Held May 2013 A1
Foreign Referenced Citations (93)
Number Date Country
2794150 Nov 2011 CA
1165238 Nov 1997 CN
1432102 Jul 2003 CN
101614139 Dec 2009 CN
202055876 Nov 2011 CN
202544943 Nov 2012 CN
202718721 Feb 2013 CN
2632777 Feb 1977 DE
19906087 Aug 2000 DE
10052993 May 2002 DE
0 277 777 Jun 1992 EP
1977174 Oct 2008 EP
1998013 Dec 2008 EP
2419621 Feb 2012 EP
2446122 May 2012 EP
2478201 Jul 2012 EP
2500530 Sep 2012 EP
2550436 Jan 2013 EP
856985 Dec 1960 GB
2010974 Jul 1979 GB
2075608 Nov 1981 GB
58-193051 Nov 1983 JP
60040707 Mar 1985 JP
61-152914 Jul 1986 JP
01-240705 Sep 1989 JP
H 03-215139 Sep 1991 JP
05-321612 Dec 1993 JP
06-331225 Nov 1994 JP
08028805 Feb 1996 JP
09-100702 Apr 1997 JP
2641581 May 1997 JP
09-209716 Aug 1997 JP
2858750 Dec 1998 JP
H11270352 May 1999 JP
2000257407 Sep 2000 JP
2001-193419 Jul 2001 JP
2002-097965 Apr 2002 JP
2003529715 Oct 2003 JP
2004-239250 Aug 2004 JP
2004-332626 Nov 2004 JP
2005030727 Feb 2005 JP
2005-533972 Nov 2005 JP
2006037760 Feb 2006 JP
2006177266 Jul 2006 JP
2007-198200 Sep 2007 JP
4343738 Oct 2009 JP
2011-017268 Jan 2011 JP
100191080 Jun 1999 KR
10-2007-0086244 Aug 2007 KR
10-0766101 Oct 2007 KR
10-0844634 Jul 2008 KR
10-20100067927 Jun 2010 KR
1020110018769 Feb 2011 KR
1069914 Sep 2011 KR
1103549 Jan 2012 KR
10-2012-0058582 Jun 2012 KR
2012-0068670 Jun 2012 KR
2012-0128753 Nov 2012 KR
2012-0128755 Nov 2012 KR
WO 9105145 Apr 1991 WO
WO 9609500 Mar 1996 WO
0071944 Nov 2000 WO
WO 0144658 Jun 2001 WO
WO 2006060253 Jun 2006 WO
WO 2006137957 Dec 2006 WO
WO 2007056241 May 2007 WO
WO 2007079245 Jul 2007 WO
WO 2007082103 Jul 2007 WO
WO 2007112090 Oct 2007 WO
WO 2008039725 Apr 2008 WO
2008101711 Aug 2008 WO
WO 2009045196 Apr 2009 WO
WO 2009058992 May 2009 WO
2010083198 Jul 2010 WO
WO 2010074173 Jul 2010 WO
WO 2010121255 Oct 2010 WO
WO 2010126980 Nov 2010 WO
WO 2010151560 Dec 2010 WO
WO 2011017450 Feb 2011 WO
WO 2011017476 Feb 2011 WO
WO 2011017599 Feb 2011 WO
WO 2011034984 Mar 2011 WO
WO 2011094294 Aug 2011 WO
WO 2011119650 Sep 2011 WO
WO 2012074905 Jun 2012 WO
WO 2012074907 Jun 2012 WO
WO 2012074911 Jun 2012 WO
WO 2012074940 Jun 2012 WO
WO 2013055391 Apr 2013 WO
WO 2013059687 Apr 2013 WO
WO 2013059695 Apr 2013 WO
WO 2013070249 May 2013 WO
WO 2013074907 May 2013 WO
Non-Patent Literature Citations (89)
Entry
Alpy, N., et al., “French Atomic Energy Commission views as regards SCO2 Cycle Development priorities and related R&D approach,” Presentation, Symposium on SCO2 Power Cycles, Apr. 29-30, 2009, Troy, NY, 20 pages.
Angelino, G., and Invernizzi, C.M., “Carbon Dioxide Power Cycles using Liquid Natural Gas as Heat Sink”, Applied Thermal Engineering Mar. 3, 2009, 43 pages.
Bryant, John C., Saari, Henry, and Zanganeh, Kourosh, “An Analysis and Comparison of the Simple and Recompression Supercritical CO2 Cycles” Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 8 pages.
Chapman, Daniel J., Arias, Diego A., “An Assessment of the Supercritical Carbon Dioxide Cycle for Use in a Solar Parabolic Trough Power Plant”, Presentation, Abengoa Solar, Apr. 29-30, 2009, Troy, NY, 20 pages.
Chapman, Daniel J., Arias, Diego A., “An Assessment of the Supercritical Carbon Dioxide Cycle for Use in a Solar Parabolic Trough Power Plant”, Paper, Abengoa Solar, Apr. 29-30, 2009, Troy, NY, 5 pages.
Chen, Yang, Lundqvist, P., Johansson, A., Platell, P., “A Comparative Study of the Carbon Dioxide Transcritical Power Cycle Compared with an Organic Rankine Cycle with R123 as Working Fluid in Waste Heat Recovery”, Science Direct, Applied Thermal Engineering, Jun. 12, 2006, 6 pages.
Chen, Yang, “Thermodynamic Cycles Using Carbon Dioxide as Working Fluid”, Doctoral Thesis, School of Industrial Engineering and Management, Stockholm, Oct. 2011, 150 pages., (3 parts).
Chordia, Lalit, “Optimizing Equipment for Supercritical Applications”, Thar Energy LLC, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 7 pages.
Combs, Osie V., “An Investigation of the Supercritical CO2 Cycle (Feher cycle) for Shipboard Application”, Massachusetts Institute of Technology, May 1977, 290 pages.
Di Bella, Francis A., “Gas Turbine Engine Exhaust Waste Heat Recovery Navy Shipboard Module Development”, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 8 pages.
Dostal, V., et al., A Supercritical Carbon Dioxide Cycle for Next Generation Nuclear Reactors, Mar. 10, 2004, 326 pages., (7 parts).
Dostal, Vaclav and Kulhanek, Martin, “Research on the Supercritical Carbon Dioxide Cycles in the Czech Republic”, Czech Technical University in Prague, Symposium on SCO2 Power Cycles, Apr. 29-30, 2009, Troy, NY, 8 pages.
Dostal, Vaclav, and Dostal, Jan, “Supercritical CO2 Regeneration Bypass Cycle—Comparison to Traditional Layouts”, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 5 pages.
Eisemann, Kevin, and Fuller, Robert L., “Supercritical CO2 Brayton Cycle Design and System Start-up Options”, Barber Nichols, Inc., Paper, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 7 pages.
Eisemann, Kevin, and Fuller, Robert L., “Supercritical CO2 Brayton Cycle Design and System Start-up Options”, Presentation, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 11 pages.
Feher, E.G., et al., “Investigation of Supercritical (Feher) Cycle”, Astropower Laboratory, Missile & Space Systems Division, Oct. 1968, 152 pages.
Fuller, Robert L., and Eisemann, Kevin, “Centrifugal Compressor Off-Design Performance for Super-Critical CO2” , Barber Nichols, Inc. Presentation, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 20 pages.
Fuller, Robert L., and Eisemann, Kevin, “Centrifugal Compressor Off-Design Performance for Super-Critical CO2”, Paper, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 12 pages.
Gokhstein, D.P. and Verkhivker, G.P. “Use of Carbon Dioxide as a Heat Carrier and Working Substance in Atomic Power Stations”, Soviet Atomic Energy, Apr. 1969, vol. 26, Issue 4, pp. 430-432.
Gokhstein, D.P.; Taubman, E.I.; Konyaeva, G.P., “Thermodynamic Cycles of Carbon Dioxide Plant with an Additional Turbine After the Regenerator”, Energy Citations Database, Mar. 1973, 1 Page, Abstract only.
Hejzlar, P. et al.., “Assessment of Gas Cooled Gas Reactor with Indirect Supercritical CO2 Cycle” Massachusetts Institute of Technology, Jan. 2006, 10 pages.
Hoffman, John R., and Feher, E.G, “150 kwe Supercritical Closed Cycle System”, Transactions of the ASME, Jan. 1971, pp. 70-80.
Jeong, Woo Seok, et al., “Performance of S—CO2 Brayton Cycle with Additive Gases for SFR Application”, Korea Advanced Institute of Science and Technology, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 5 pages.
Johnson, Gregory A., & McDowell, Michael, “Issues Associated with Coupling Supercritical CO2 Power Cycles to Nuclear, Solar and Fossil Fuel Heat Sources”, Hamilton Sundstrand, Energy Space & Defense-Rocketdyne, Apr. 29-30, 2009, Troy, NY, Presentation, 18 pages.
Kawakubo, Tomoki, “Unsteady Roto-Stator Interaction of a Radial-Inflow Turbine with Variable Nozzle Vanes”, ASME Turbo Expo 2010: Power for Land, Sea, and Air; vol. 7: Turbomachinery, Parts A, B, and C; Glasgow, UK, Jun. 14-18, 2010, Paper No. GT2010-23677, pp. 2075-2084, (1 page, Abstract only).
Kulhanek, Martin, “Thermodynamic Analysis and Comparison of S—CO2 Cycles”, Presentation, Czech Technical University in Prague, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 14 pages.
Kulhanek, Martin, “Thermodynamic Analysis and Comparison of S—CO2 Cycles”, Paper, Czech Technical University in Prague, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 7 pages.
Kulhanek, Martin., and Dostal, Vaclav, “Supercritical Carbon Dioxide Cycles Thermodynamic Analysis and Comparison”, Abstract, Faculty Conference held in Prague, Mar. 24, 2009, 13 pages.
Ma, Zhiwen and Turchi, Craig S., “Advanced Supercritical Carbon Dioxide Power Cycle Configurations for Use in Concentrating Solar Power Systems”, National Renewable Energy Laboratory, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 4 pages.
Moisseytsev, Anton, and Sienicki, Jim, “Investigation of Alternative Layouts for the Supercritical Carbon Dioxide Brayton Cycle for a Sodium-Cooled Fast Reactor”, Supercritical CO2 Power Cycle Symposium, Troy, NY, Apr. 29, 2009, 26 pages.
Munoz De Escalona, Jose M., “The Potential of the Supercritical Carbon Dioxide Cycle in High Temperature Fuel Cell Hybrid Systems”, Paper, Thermal Power Group, University of Seville, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 6 pages.
Munoz De Escalona, Jose M., et al., “The Potential of the Supercritical Carbon Dioxide Cycle in High Temperature Fuel Cell Hybrid Systems”, Presentation, Thermal Power Group, University of Seville, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 19 pages.
Muto, Y., et al., “Application of Supercritical CO2 Gas Turbine for the Fossil Fired Thermal Plant”, Journal of Energy and Power Engineering, Sep. 30, 2010, vol. 4, No. 9, 9 pages.
Muto, Yasushi, and Kato, Yasuyoshi, “Optimal Cycle Scheme of Direct Cycle Supercritical CO2 Gas Turbine for Nuclear Power Generation Systems”, International Conference on Power Engineering-2007, Oct. 23-27, 2007, Hangzhou, China, pp. 86-87.
Noriega, Bahamonde J.S., “Design Method for s—CO2 Gas Turbine Power Plants”, Master of Science Thesis, Delft University of Technology, Oct. 2012, 122 pages., (3 parts).
Oh, Chang, et al., “Development of a Supercritical Carbon Dioxide Brayton Cycle: Improving PBR Efficiency and Testing Material Compatibility”, Presentation, Nuclear Energy Research Initiative Report, Oct. 2004, 38 pages.
Oh, Chang; et al., “Development of a Supercritical Carbon Dioxide Brayton Cycle: Improving VHTR Efficiency and Testing Material Compatibility”, Presentation, Nuclear Energy Research Initiative Report, Final Report, Mar. 2006, 97 pages.
Parma, Ed, et al., “Supercritical CO2 Direct Cycle Gas Fast Reactor (SC-GFR) Concept” Presentation for Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 40 pages.
Parma, Ed, et al., “Supercritical CO2 Direct Cycle Gas Fast Reactor (SC-GFR) Concept”, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 9 pages.
Parma, Edward J., et al., “Supercritical CO2 Direct Cycle Gas Fast Reactor (SC-GFR) Concept”, Presentation, Sandia National Laboratories, May 2011, 55 pages.
PCT/US2006/049623—Written Opinion of ISA dated Jan. 4, 2008, 4 pages.
PCT/US2007/001120—International Search Report dated Apr. 25, 2008, 7 pages.
PCT/US2007/079318—International Preliminary Report on Patentability dated Jul. 7, 2008, 5 pages.
PCT/US2010/031614—International Search Report dated Jul. 12, 2010, 3 pages.
PCT/US2010/031614—International Preliminary Report on Patentability dated Oct. 27, 2011, 9 pages.
PCT/US2010/039559—International Preliminary Report on Patentability dated Jan. 12, 2012, 7 pages.
PCT/US2010/039559—Notification of Transmittal of the International Search Report and Written Opinion of the International Searching Authority, or the Declaration dated Sep. 1, 2010, 6 pages.
PCT/US2010/044476—International Search Report dated Sep. 29, 2010, 23 pages.
PCT/US2010/044681—International Search Report and Written Opinion mailed Oct. 7, 2010, 10 pages.
PCT/US2010/044681—International Preliminary Report on Patentability dated Feb. 16, 2012, 9 pages.
PCT/US2010/049042—International Search Report and Written Opinion dated Nov. 17, 2010, 11 pages.
PCT/US2010/049042—International Preliminary Report on Patentability dated Mar. 29, 2012, 18 pages.
PCT/US2011/029486—International Preliminary Report on Patentability dated Sep. 25, 2012, 6 pages.
PCT/US2011/029486—International Search Report and Written Opinion dated Nov. 16, 2011, 9 pages.
PCT/US2011/062266—International Search Report and Written Opinion dated Jul. 9, 2012, 12 pages.
PCT/US2011/062198 (EPS-070)—International Search Report and Written Opinion dated Jul. 2, 2012, 9 pages.
PCT/US2011/062201—International Search Report and Written Opinion dated Jun. 26, 2012, 9 pages.
PCT/US2011/062204—International Search Report dated Nov. 1, 2012, 10 pages.
PCT/US2011/62207—International Search Report and Written Opinion dated Jun. 28, 2012, 7 pages.
PCT/US2012/000470—International Search Report dated Mar. 8, 2013, 10 pages.
PCT/US2012/061151—International Search Report and Written Opinion dated Feb. 25, 2013, 9 pages.
PCT/US2012/061159—International Search Report dated Mar. 2, 2013, 10 pages.
Persichilli, Michael, et al., “Supercritical CO2 Power Cycle Developments and Commercialization: Why sCO2 can Displace Steam” Echogen Power Systems LLC, Power-Gen India & Central Asia 2012, Apr. 19-21, 2012, New Delhi, India, 15 pages.
Saari, Henry, et al., “Supercritical CO2 Advanced Brayton Cycle Design”, Presentation, Carleton University, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 21 pages.
San Andres, Luis, “Start-Up Response of Fluid Film Lubricated Cryogenic Turbopumps (Preprint)”, AIAA/ASME/SAE/ASEE Joint Propulsion Conference, Cincinnati, OH, Jul. 8-11, 2007, 38 pages.
Sarkar, J., and Bhattacharyya, Souvik, “Optimization of Recompression S—CO2 Power Cycle with Reheating” Energy Conversion and Management 50 (May 17, 2009), pp. 1939-1945.
Tom, Samsun Kwok Sun, “The Feasibility of Using Supercritical Carbon Dioxide as a Coolant for the Candu Reactor”, The University of British Columbia, Jan. 1978, 156 pages.
VGB PowerTech Service GmbH, “CO2 Capture and Storage”, A VGB Report on the State of the Art, Aug. 25, 2004, 112 pages.
Vidhi, Rachana, et al., “Study of Supercritical Carbon Dioxide Power Cycle for Power Conversion from Low Grade Heat Sources”, Presentation, University of South Florida and Oak Ridge National Laboratory, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 17 pages.
Vidhi, Rachana, et al., “Study of Supercritical Carbon Dioxide Power Cycle for Power Conversion from Low Grade Heat Sources”, Paper, University of South Florida and Oak Ridge National Laboratory, Supercritical CO2 Power Cycle Symposium, May 24-25, 2011, Boulder, CO, 8 pages.
Wright, Steven A., et al., “Modeling and Experimental Results for Condensing Supercritical CO2 Power Cycles”, Sandia Report, Jan. 2011, 47 pages.
Wright, Steven A., et al., “Supercritical CO2 Power Cycle Development Summary at Sandia National Laboratories”, May 24-25, 2011, (1 page, Abstract only).
Wright, Steven, “Mighty Mite”, Mechanical Engineering, Jan. 2012, pp. 41-43.
Yoon, Ho Joon, et al., “Preliminary Results of Optimal Pressure Ratio for Supercritical CO2 Brayton Cycle coupled with Small Modular Water Cooled Reactor”, Presentation, Korea Advanced Institute of Science and Technology and Khalifa University of Science, Technology and Research, Boulder, CO, May 25, 2011, 18 pages.
Yoon, Ho Joon, et al., “Preliminary Results of Optimal Pressure Ratio for Supercritical CO2 Brayton Cycle coupled with Small Modular Water Cooled Reactor”, Paper, Korea Advanced Institute of Science and Technology and Khalifa University of Science, Technology and Research, May 24-25, 2011, Boulder, CO, 7 pages.
CN Search Report for Application No. 201080035382.1, 2 pages.
CN Search Report for Application No. 201080050795.7, 2 pages.
PCT/US2011/062198—Extended European Search Report dated May 6, 2014, 9 pages.
PCT/US2011/055547—Extended European Search Report dated May 28, 2014, 8 pages.
PCT/US2013/055547—Notification of Transmittal of the International Search Report and the Written Opinion of the International Searching Authority, or the Declaration dated Jan. 24, 2014, 11 pages.
PCT/US2013/064470—Notification of Transmittal of the International Search Report and the Written Opinion of the International Searching Authority, or the Declaration dated Jan. 22, 2014, 10 pages.
PCT/US2013/064471—Notification of Transmittal of the International Search Report and the Written Opinion of the International Searching Authority, or the Declaration dated Jan. 24, 2014, 10 pages.
PCT/US2014/013154—International Search Report dated May 23, 2014, 4 pages.
PCT/US2014/013170—Notification of Transmittal of the International Search Report and the Written Opinion of the International Searching Authority, or the Declaration dated May 9, 2014, 12 pages.
PCT/US2014/023026—Notification of Transmittal of the International Search Report and the Written Opinion of the International Searching Authority, or the Declaration dated Jul. 22, 2014, 11 pages.
PCT/US2014/023990—Notification of Transmittal of the International Search Report and the Written Opinion of the International Searching Authority, or the Declaration dated Jul. 17, 2014, 10 pages.
PCT/US2014/026173—Notification of Transmittal of the International Search Report and the Written Opinion of the International Searching Authority, or the Declaration dated Jul. 9, 2014, 10 pages.
Renz, Manfred, “The New Generation Kalina Cycle”, Contribution to the Conference: “Electricity Generation from Enhanced Geothermal Systems”, Sep. 14, 2006, Strasbourg, France, 18 pages.
Thorin, Eva, “Power Cycles with Ammonia-Water Mixtures as Working Fluid”, Doctoral Thesis, Department of Chemical Engineering and Technology Energy Processes, Royal Institute of Technology, Stockholm, Sweden, 2000, 66 pages.
Related Publications (1)
Number Date Country
20140102101 A1 Apr 2014 US
Provisional Applications (1)
Number Date Country
61712907 Oct 2012 US