The Brayton thermodynamic cycle is commonly used in a variety of applications including aircraft turbofan propulsion, terrestrial power generation, and space power generation because it can scale to large power levels. The Brayton cycle can be recuperated or non-recuperated and can be open cycle or closed cycle. Normally, the Brayton cycle efficiency increases as the compressor pressure ratio increases, but for a given temperature ratio, the specific power begins to decrease with additional pressure ratio growth. This is because the turbine temperature limits prevent the addition of more thermal energy. If the turbine blade can be cooled, both higher efficiency and higher specific power can be achieved. Historically, open Brayton cycles have out-performed closed Brayton cycles because of the difficulty of cooling the turbine blade and the additional mass of heat exchanger recuperation. Closed cycle Brayton efficiency is a function of compressor pressure and temperature ratio, but also of the mass and effectiveness of the recuperator. In all cases, a higher turbine inlet temperature reduces system mass and increases both system efficiency and system specific power.
The Stirling cycle is widely used in lower power applications that require high thermal efficiency. Generally, the Stirling cycle is a closed cycle that does not scale well to higher power because of oscillating component amplitude and thermal surface heat transfer limits. The thermoacoustic Stirling cycle either generates a sound wave with thermal input, or it can operate in reverse to provide refrigeration using the energy from an incoming acoustic wave. The acoustic wave can generate electric power by either extracting the pressure wave with an oscillating piston, or for higher power levels, it can extract the velocity wave with a generator. While the acoustic Stirling cycle and piston Stirling cycle have comparable efficiencies, the acoustic Stirling cycle can operate over a larger range of temperature ratios and power levels when appropriately configured.
The following presents a simplified summary to provide a basic understanding of some aspects of the disclosed subject matter. This summary is not an extensive overview. It is not intended to identify key/critical elements or to delineate the scope of the claimed subject matter. Its sole purpose is to present some concepts in a simplified form as a prelude to the more detailed description presented later.
In one embodiment, a system includes a Brayton cycle engine having a compressor, a turbine, a hollow rotating shaft that extends between a first end and a second end, a hollow tubing that interconnects the first end and the second end, and a heat source. The system further includes a thermoacoustic Stirling cycle engine disposed within the hollow rotating shaft between the first and second ends thereof. The Stirling cycle engine includes a cold side heat exchanger disposed adjacent to the compressor, a hot side heat exchanger disposed adjacent to the turbine, and a regenerator disposed between the cold and hot side heat exchangers. A first power generator is disposed within the hollow tubing and located adjacent to the second end of the hollow rotating shaft. A second power generator is disposed around the hollow rotating shaft between the compressor and the turbine.
In another embodiment, a system includes a four-stage engine, wherein each stage is interconnected by a first hollow tubing and each stage includes a Brayton cycle engine that includes a compressor, a turbine, a hollow rotating shaft that extends between a first end and a second end, and a heat source. The system further includes a thermoacoustic Stirling cycle engine disposed within the hollow rotating shaft between the first and second ends thereof. The Stirling cycle engine includes a cold side heat exchanger disposed adjacent to the compressor, a hot side heat exchanger disposed adjacent to the turbine, and a regenerator disposed between the cold and hot side heat exchangers. A first power generator is disposed within the first hollow tubing and located adjacent to the second end of the hollow rotating shaft. Additionally, a second power generator disposed around the hollow rotating shaft between the compressor and the turbine.
In yet another embodiment, a system includes a four-stage engine, wherein a first hollow tubing connects each stage and each stage is arranged at our about 90 degrees apart from an adjacent stage. Each stage includes a Brayton cycle engine that includes a compressor, a turbine, a hollow rotating shaft that extends between a first end and a second end, and a heat source. A thermoacoustic Stirling cycle engine is disposed within the hollow rotating shaft between the first and second ends thereof. The Stirling cycle engine includes a cold side heat exchanger disposed adjacent to the compressor, a hot side heat exchanger disposed adjacent to the turbine, and a regenerator disposed between the cold and hot side heat exchangers. A first power generator is disposed within the first hollow tubing and located adjacent to the second end of the hollow rotating shaft. A second power generator is disposed around the hollow rotating shaft between the compressor and the turbine. A four-stage intercooling level fluidically is connected to and disposed under the four-stage engine, each stage comprising an intercooling acoustic heat exchanger being arranged at or about 90 degrees apart from an intercooling acoustic heat exchanger of an adjacent stage. Each stage is interconnected by a second hollow tubing having a four-stage reheating level fluidically connected to and disposed above the four-stage engine. Each stage comprises a reheating acoustic heat exchanger being arranged at or about 90 degrees apart from a reheating acoustic heat exchanger of an adjacent stage. Each stage is connected by a third hollow tubing. Additionally, a recuperator is centrally located with respect to the four-stage engine, the four-stage intercooling level, and the four-stage reheating level.
To the accomplishment of the foregoing and related ends, certain illustrative aspects of the claimed subject matter are described herein in connection with the following description and the annexed drawings. These aspects indicate various ways in which the subject matter may be practiced, all of which are intended to be within the scope of the disclosed subject matter. Other advantages and novel features may become apparent from the following detailed description when considered in conjunction with the drawings.
The embodiments set forth in the drawings are illustrative and examples in nature and not intended to limit the subject matter defined by the claims. The following detailed description of the illustrative embodiments can be understood when read in conjunction with the following drawings, where like structure is indicated with like reference numerals and in which:
As described herein, embodiments of disclosure are directed to a Brayton cycle and an acoustic Stirling cycle being combined into a new, synergistic cycle engine referred to herein as a “Strayton” engine or generator. Since each of the Brayton and Stirling cycles act as a topping cycle and bottoming cycle to the other, a unique thermodynamic combined cycle property is provided which otherwise is not possible. Normally, a first cycle is the topping cycle, and a second cycle is the bottoming cycle (such as, for example, a gas turbine Brayton engine acting as a topping cycle for a steam turbine Rankine engine which acts as the bottoming cycle, or a fuel cell acting as the topping cycle with a Stirling engine acting as the bottoming cycle). The unique Strayton cycle of the disclosure forms the basic building block for other configurations described herein.
Turning now to
The Strayton engine 102 generally includes a Brayton cycle engine 104 and a thermoacoustic Stirling engine 120 embedded within the Brayton cycle engine 104. In particular, the Brayton engine 104 generally includes a compressor 106, a turbine 108, a hollow rotating shaft 110 extending between a first end 112 and a second end 114, and a heat source 136. The first and second ends 112, 114 of the hollow rotating shaft 110 are interconnected by hollow tubing 116 to form a self-amplifying acoustic loop 128.
The Stirling engine 120 is disposed within the hollow rotating shaft 110 between the first and second ends 112, 114 thereof. The Stirling engine 120 generally includes a cold side heat exchanger 122 disposed adjacent to the compressor 106, a hot side heat exchanger disposed adjacent to the turbine 108, and a regenerator 126 disposed between the cold and hot side heat exchangers 122, 124. Each of the cold and hot side heat exchangers 122, 124 and regenerator 126 are located within the hollow rotating shaft 110.
During operation of the example thermal energy conversion power generation system 100, a heat source 136 supplies heat to the turbine 108. Heat transfer rate QH is drawn down through the blades of the turbine 108 and is used to power the Stirling cycle engine 120. In other words, the hot side heat exchanger 124 receives heat generated from the turbine 108 to thereby power the Stirling cycle engine 120. In this regard, the Stirling cycle engine 120 provides conductive cooling of the turbine 108. That is, pulling heat down through the blades of the turbine 108 has a cooling effect on the structure of the Strayton engine 102, thereby allowing the system 100 to reduce or remove turbine blade cooling flow. Overall, the waste heat generated from the Brayton cycle engine 104 acts as a topping cycle delivering thermal energy to the Stirling cycle engine 120 embedded within the hollow rotating shaft 110. In other words, the Brayton cycle engine 104 powers the Stirling cycle engine 120.
A recuperator 144 can be included to transfer some of the waste heat from the exhaust of the turbine 108 to the compressed air of the compressor 106. However, it is noted that the Stirling cycle engine 120 also provides thermal recuperation for the Brayton cycle engine 104. In this regard, using the cold side heat exchanger 122, wasted thermal power Qc from the Stirling cycle engine 120 is introduced to the Brayton cycle engine 104, directly before combustion at heat source 136, through a thrust bearing 134 that is paired with the cold side heat exchanger 122. As a result, the overall efficiency of the Brayton cycle engine 104 is increased. In other words, the waste heat generated from the thermoacoustic Stirling cycle engine 120 is transferred to the cold side heat exchanger 122 to create a recuperation cycle within the Brayton cycle engine 104, thereby increasing overall efficiency.
The thermal energy conversion power generation system 100 further includes a first power generator 140 disposed within the hollow tubing 116 and located adjacent to the second and 114 of the hollow rotating shaft 110. The first power generator 140 is configured to harness thermal acoustic energy from the loop 128 generated by the Stirling engine 120 and generate electric power therefrom. In some embodiments, the first power generator 140 is a bi-directional turbine generator which, when combined with the thermoacoustic Stirling engine 120 described herein, can operate over a large range of temperature ratios and power levels. The Stirling cycle engine 120 acts to amplify incoming power by approximately 1:3. Therefore, for example, if a 1 HP acoustic wave is input, 3 HP would be available for electric power generation with the first power generator 140. In this fashion, acoustic waves are generated on the cold end (i.e., the first end 112 adjacent to the cold side heat exchanger 122) via a no moving part standing wave thermoacoustic generator (not shown), which then activates the first power generator 140 disposed within hollow tubing 116 and located adjacent to the second end 114 of hollow rotating shaft 110. It is noted that multiple of the individual Strayton engine 102 illustrated in
A second power generator 142 is disposed around the hollow rotating shaft 110. In some embodiments, the second power generator 142 is located between the compressor 106 and the turbine 108. However, in other embodiments, it should be understood that the second power generator 142 could be located anywhere between the first and second ends 112, 114 of the hollow rotating shaft 110, such as between the compressor 106 and the first end 112 of the hollow rotating shaft 110. The second power generator 142 is configured to harness rotational energy from the hollow rotating shaft 110 and generate electric power therefrom. In some embodiments, the second power generator 142 is a permanent magnet generator. In some other embodiments, the second power generator 142 is a three-phase switched reluctance (“SR”) generator. SR generators are mechanically capable of very high-speed operation due to their simple and robust rotor construction without embedded permanent magnets or electrical windings. Moreover, SR generators are capable of high-temperature (e.g., above 300° C.) operation. As a result, SR generators are particularly suited to handle the high speed of the hollow rotating shaft 110 and the high temperatures associated with the Strayton engine 102.
Bearings 130 are included to rotationally support the hollow rotating shaft 110. In some embodiments, the bearings 130 are pressurized gas bearings for long lasting, no maintenance operation. The use of pressurized gas bearings also enables zero greenhouse gas emissions because no oil particulates are released into the atmosphere (forming contrails) from oil bearings which would otherwise be used. Additional pressurized gas bearings (not shown) can be used to rotationally support the first power generator 140 within the hollow rotating shaft 110. Moreover, the hollow rotating shaft 110 of the Brayton cycle engine 104 is separated from the non-rotating structures (e.g., hollow tubing 116) of the Stirling cycle engine 120 by a clearance seal 132. The clearance seal 132 is hermetically sealed from the environment but intentionally has a leakage path between the Brayton and Stirling cycles. As a result, the Brayton and Stirling cycle engines 104, 120 effectively share the same pressurized working fluid.
The pressurized working fluid in a closed Strayton generator system, such as Strayton generator 102, increases the system specific power by reducing the size of the compressor 106 and turbine 108, by increasing the rotational speed of the hollow rotating shaft 110, which reduces the required size of the second power generator 142 when a SR generator is used, and by increasing the efficiency of the first power generator 140 when a bi-directional turbine generator is used. In some embodiments, the pressurized working fluid used in the closed Strayton generator system, such as Strayton generator 102, can be a noble gas. In some particular embodiments, the pressurized working fluid can be selected from HeXe, HeAr, or HeN2.
It is noted that using the same pressurized, high molecular weight working fluid benefits both the Brayton cycle engine 104 and the Stirling cycle engine 120, but for different reasons. For the Brayton cycle engine 104, it reduces the required size of the compressor 106, turbine 108 and second power generator 142 by increasing the rotational speed. In other words, the inert high pressure, high molecular weight working fluid (e.g., He—Ar) makes the turbomachinery small enough to be cooled conductively. For the Stirling cycle engine 120, it increases the efficiency of the first power generator 140 (e.g., about 90% efficiency) when an acoustic bi-directional turbine is used. As a result, the Strayton engine 102 has a higher overall specific power and efficiency compared to a Brayton or Stirling cycle engine alone.
Moreover, the unique Strayton engine 102 provides many benefits in both open and closed systems, such as increased Brayton cycle 104 efficiency due to a higher turbine inlet temperature achieved via conductive cooling of the turbine from the embedded acoustic Stirling cycle 120. Brayton cycle 104 efficiency is further increased because the embedded acoustic Stirling cycle 120 provides for higher thermal recuperation with thermal transfer from the turbine 108 to the compressor 106 exhaust. In addition, the overall system efficiency is higher because of the reciprocal thermoacoustic topping and bottoming cycles of the Brayton cycle engine 104 and Stirling cycle engine 120. Furthermore, the heat transfer provided by the embedded acoustic Stirling cycle 120 allows the size of heat exchangers to be reduced. Moreover, thermoacoustic cooling provided by the embedded Stirling cycle 120 can be used to refrigerate the power generators 140, 142, bearings 130, and electronics which may be included in the system.
Additional benefits are realized through use of the example Strayton engine 102 in a closed cycle. For instance, separation of the heat source 136 from the turbine inlet fluid enables the use of a nuclear, solar, or combustible heat sources and further protects turbine blades from combustion products, reactivity, and creep. In addition, the use of higher-pressure working fluids achieves higher specific power at any altitude. Furthermore, bearings 130 can be pressurized gas bearings that support high-speed, no-maintenance shafts (e.g., hollow rotating shaft 110) which reduces the overall mass of the turbomachinery and generator. Additionally, higher temperature turbine blades can be used which otherwise could not be used in a closed system due to limited blade cooling options and refractory coating limitations.
Moreover, significant performance gains are realized due to the following unique features of the Strayton engine 102. First, the ability to cool the turbine blades conductively with the embedded thermodynamic Stirling cycle 120 enables operating the Brayton cycle 104 at a higher compression ratio and hence a higher efficiency. Second, the waste heat from cooling the turbine blades and rejected heat exhaust from the turbine 108 are used to power the Stirling engine 120 embedded within the hollow rotating shaft 110 (thereby acting as a bottoming cycle). Third, the rejected heat from the embedded Stirling engine 120 is used to heat the compressed Brayton working fluid (thereby acting as a recuperator and a topping cycle for the Brayton engine 104) and as such, the Brayton engine 104 and embedded Stirling engine 120 mutually serve as topping and bottoming cycles at the same time for maximum system efficiency. Fourth, by closing the entire system into a hermetically sealed unit, the working fluid of the Brayton and Stirling cycles 104, 120 can be pressurized to increase the specific power, resulting in a reduction of the turbine diameter to 4 inches or less at a megawatt scale, making the system a highly effective conductive heat transfer component for both cooling of the turbine 108 and heating of the compressor 106 outlet. Fifth, normally a closed Brayton cycle requires a very large recuperator that dominates the mass of the entire system, but the embedded Stirling cycle 120 naturally provides recuperation when it acoustically transfers the waste heat from the turbine end to the compressor end. As such, a smaller recuperator 144 can be used. Sixth, no gearbox is required because the rotational speed of the hollow rotating shaft 110 can be perfectly matched with the required generator speeds (due to the sealed working fluid and pressure tuning thereof). Seventh, the sealed system is perfectly quiet. Eighth, relaxed tolerances can be used because the dual topping/bottoming cycle synergy reduces the need for separate high efficiency components (one cycle's loss is the other cycle's gain), thereby reducing manufacturing costs. Ninth, the hermetically sealed Brayton and Stirling cycles 104, 120 enable the use of inert working fluids (typically noble gases) to eliminate corrosion. Tenth, the noble gas working fluids enables higher operating temperatures because they don't corrode like super-critical CO2 at temperatures greater than 923K. Moreover, the noble gas working fluids are more compatible with higher temperature refractory turbine blades, and when combined with the embedded conductive cooling of the Stirling cycle 120, turbine 108 inlet temperatures of greater than 1500K are potentially possible resulting in even higher efficiency. Eleventh, the super-critical CO2 heat rejection constraint (critical point temperature of about 310K) requires large heat exchangers, but noble gases can reject at higher temperatures, which is useful for heat exchanger mass rejection in aeronautical and space applications. Twelfth, the example Strayton engine 102 has natural momentum cancelling and a compact size enabled by eliminating an external recuperator and corresponding plumbing. Thirteenth, the example Strayton engine 102 is heat source agnostic, which enables zero-emission or sustainable fuels to be used for aircraft and nuclear sources in terrestrial and space applications. Fourteenth, the inert working fluid does not require the very high pressures required by super-critical CO2 (i.e., 2 MPa vs. 25 MPa), thereby reducing system mass. Fifteenth, the entire system is hermetically sealed with no moving external seals. Sixteenth, the pressurized working fluid enables long life gas bearings 130 that are non-contact, rotating, oscillating, and that require no lubrication.
These unique benefits and performance gains are further realized by combining multiple of the above-described Strayton cycles together in staged system 200 as shown in
It should be understood that each Strayton engine 202a-202d includes components similar to the at least one Strayton engine 102 described above and illustrated in
In particular, with reference to
As shown in
For example, during operation of the four Strayton engines 202a-202d in
In some embodiments, each the four Strayton engines 202a-202d can generate about 2.5 MW of power. As such, the quad configuration of the four Strayton engines 202a-202d can generate a total of about 10 MW of power. However, these levels of power generation are only examples, and it should be understood that each of the four Strayton engines 202a-202d individually or in the quad configuration can operate at lower power levels as desired.
In some embodiments, the staged system 200 having the quad configuration of Strayton engines 202a-202d in
It should be understood that the multi-level stacked system 300 shown in
Moving from left to right in
The intercooling and reheating levels 302, 306 provide intercooling and reheating for the Brayton cycle components of the Strayton engines having the quad configuration in the middle level 304. In this regard, both the intercooling and reheating levels 302, 306 are similarly arranged in a quad configuration. A single recuperator 308 can thus be centrally located with respect to each of the bottom intercooling level 302, the quad configured Strayton engine middle level 304, and the top reheating level 306. Each level 302, 304, and 306, along with recuperator 308, are fluidically interconnected via plumbing 310.
Additional details of the bottom intercooling level 302 and the top reheating level 306 will now be discussed with reference to
It is noted that the bottom intercooling level heat exchangers 316a-316d provide intercooling for the corresponding Brayton cycle components (e.g., compressors 206a-206d from
Each of the bottom intercooling level heat exchangers 316a-316d and top reheating level heat exchangers 318a-318d are similarly constructed. Thus, in
The four acoustic bottom intercooling level heat exchangers 316a-316d (and the four acoustic top reheating level heat exchangers 318a-318d) are arranged in a quad configuration wherein the heat exchangers are placed ¼ wavelength apart to form a self-amplifying loop 328. In other words, each acoustic bottom intercooling level heat exchangers 316a-316d (and each acoustic top reheating level heat exchangers 318a-318d) are placed acoustically 90 degrees apart, such that the distance the acoustic wave travels in the hollow tube is 25% of the total acoustic wavelength. The total length of the acoustic hollow tubing 330 (and hollow tubing 332) is equal to one wavelength of the acoustic wave in the Stirling cycle. The acoustic energy in the loop 328 can be used to generate electricity with a bi-directional turbine generator (not shown) disposed within hollow tubing 330 (and hollow tubing 332) and adjacent to one side of each acoustic heat exchanger 316a-316d (and one side of each acoustic heat exchanger 318a-318d). More particularly, the bi-directional turbine generators are generally disposed adjacent to the side of each acoustic heat exchanger 316a-316d (and each acoustic heat exchanger 318a-318d) where the hot side heat exchangers 324a-324d are disposed.
As discussed above, each of the bottom intercooling level 302, the middle Strayton cycle level 304, and the top reheating level 306 include four Stirling cycle engines which are placed 90 degrees apart in a quad configuration to form a loop within the respective hollow tubes 330, 230, and 332. More particularly, the respective regenerators in each level 302, 304, and 306 are placed 90 degrees apart. The total perimeter length of each quad hollow tubing 330, 230, and 332 is equal to one wavelength of the acoustic wave traversing through the hollow tubing 330, 230, and 332. So with a 90-degree separation, it should be understood that the acoustic wave has traveled 25% of this total wavelength. The wavelength is a function of the frequency and wave speed. The frequency is chosen (about 60 Hz in some embodiments) and the wave speed is a function of the temperature and working fluid used. Thus, for example, assuming a wave speed of 300 m/s and a frequency of 60 Hz, the total wavelength would be 5 m. The distance between each Stirling regenerator in this case would be 25% of 5 m or 5/4 m, which is the distance the sound wave travels in the hollow tubes 330, 230, and 332 for this example.
Turning now to
As briefly described above, intercooling is provided for each compressor 206a-206d of the four Strayton engines 202a-202d in the middle level 304 and reheating is provided for each turbine 208a-208d of the four Strayton engines 202a-202d in the middle level 304. In
The intercooling is provided by the bottom intercooling level 302. In this regard, an inlet side of the compressor 206c is fluidically connected to the intercooling heat exchanger 316b of the immediately preceding stage and an outlet side of the compressor 206c is fluidically connected to the intercooling heat exchanger 316c of the corresponding stage which is disposed below the compressor 206c. The reheating is provided by the top reheating level 306. In this regard, an inlet side of the turbine 208b is fluidically connected to the corresponding hot heat exchanger 340b disposed behind the turbine 208b and an outlet side of the turbine 208b is fluidically connected to the hot heat exchanger 340c of the immediately subsequent stage. It should be understood that while the connections for intercooling and reheating discussed above are directed to two of the four Strayton stages, the remaining two Strayton stages are connected in a substantially similar manner.
Moreover, in some embodiments, the multi-level stacked system 300 is a closed system that can be coupled with a separate propulsion generating hydrogen combustion system to provide zero-emission electric power (discussed in further detail below). In this regard, additional components are included with the multi-level stacked system 300 to provide the zero-emission electric power. These components include hot heat exchangers 340b, 340c and steam mixers 342b, 342c. Both the hot heat exchangers 340b, 340c and steam mixers 342b, 342c are fluidically connected to the combustors 336b, 336c, respectively. It is noted that through the use of combustors 336b, 336c, the combustion exhaust can be separated from the turbines of the middle level 304. Steam mixers 342b, 342c are further connected to the recuperator 308. In addition, the hot heat exchangers 340b, 340c are fluidically connected to the turbines 208b, 208c and to the reheating heat exchangers 318b, 318c. It should be understood that while the multi-level stacked system 300 of
With reference to
Turning now to
Referring now to
In this manner, the separation of the multi-level stacked system 300 from the combustion system 400 enables both pre- and post-emission control for achieving zero green-house gas emissions. Post-emission control can be achieved since the combustion exhaust is not used for propulsion. Moreover, the separation of power generation by the multi-level stacked system 300 from electric motor propulsion by the hydrogen combustion system 400 allows the use of contra-rotating fan configurations. As a result, the thermodynamic and propulsive efficiency are simultaneously improved and greenhouse gas emissions are eliminated.
In the embodiment illustrated in
Turning now to
The previously described closed configurations can also be converted to an open cycle where the working fluid is atmospheric air instead of a pressurized inert working fluid. Such an open cycle is schematically illustrated in
Ranges can be expressed herein as from “about” one particular value, and/or to “about” another particular value. When such a range is expressed, another embodiment includes from the one particular value and/or to the other particular value. Similarly, when values are expressed as approximations, by use of the antecedent “about,” it will be understood that the particular value forms another embodiment. It will be further understood that the endpoints of each of the ranges are significant both in relation to the other endpoint, and independently of the other endpoint.
Directional terms as used herein—for example up, down, right, left, front, back, top, bottom—are made only with reference to the figures as drawn and are not intended to imply absolute orientation.
Unless otherwise expressly stated, it is in no way intended that any method set forth herein be construed as requiring that its steps be performed in a specific order, nor that with any apparatus specific orientations be required. Accordingly, where a method claim does not actually recite an order to be followed by its steps, or that any apparatus claim does not actually recite an order or orientation to individual components, or it is not otherwise specifically stated in the claims or description that the steps are to be limited to a specific order, or that a specific order or orientation to components of an apparatus is not recited, it is in no way intended that an order or orientation be inferred, in any respect. This holds for any possible non-express basis for interpretation, including: matters of logic with respect to arrangement of steps, operational flow, order of components, or orientation of components; plain meaning derived from grammatical organization or punctuation, and; the number or type of embodiments described in the specification.
As used herein, the singular forms “a,” “an” and “the” include plural referents unless the context clearly dictates otherwise. Thus, for example, reference to “a” component includes aspects having two or more such components, unless the context clearly indicates otherwise.
While particular embodiments have been illustrated and described herein, it should be understood that various other changes and modifications may be made without departing from the scope of the claimed subject matter. Moreover, although various aspects of the claimed subject matter have been described herein, such aspects need not be utilized in combination. It is therefore intended that the appended claims cover all such changes and modifications that are within the scope of the claimed subject matter.
This application claims priority to and the benefit of the following U.S. Provisional Patent Application Ser. No. 63/364,294, filed May 6, 2022 and entitled “NO MAINTENANCE, LIGHT-WEIGHT, HIGH-EFFICIENCY, CLOSED STRAYTON CYCLE POWER GENERATOR FOR THE CHALLENGING 50 kW TO 500 kW APPLICATIONS.” The application listed above is hereby incorporated by reference in its entirety.
Number | Name | Date | Kind |
---|---|---|---|
4199945 | Finkelstein | Apr 1980 | A |
5456076 | Zornes | Oct 1995 | A |
9664181 | Steiner | May 2017 | B2 |
10495355 | Fukaya | Dec 2019 | B2 |
10507934 | Dyson, Jr. | Dec 2019 | B1 |
20130092350 | N. | Apr 2013 | A1 |
20180363564 | Geneste | Dec 2018 | A1 |
Number | Date | Country | |
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63364294 | May 2022 | US |