Mechanical/electrical power generation system
11255223 · 2022-02-22
Assignee
Inventors
Cpc classification
F02C3/34
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01K7/32
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01K25/103
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01K23/08
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02C1/007
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02C1/105
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02C1/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
F01K23/08
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01K7/32
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02C1/00
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02C3/34
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02C1/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Abstract
Power is produced by operating first and second nested cycles utilising CO.sub.2 as working fluid without mixing of working fluid between the nested cycles. The first cycle comprises a semi-open loop operating under low pressure conditions in which CO.sub.2 is sub-critical. The second cycle comprises a closed loop operating under higher pressure conditions in which CO.sub.2 is supercritical. The first cycle operates in a Brayton cycle including oxycombustion of hydrocarbons, preferably LNG, in a combustion chamber under low pressure conditions, expansion for power production to provide a first power source, cooling in a recuperator, compression, reheating by counter-current passage via the recuperator, and return of working fluid heated by the recuperator back to the combustion chamber. Water and excess CO.sub.2 resulting from the oxycombustion step are separated from the first cycle. The first cycle serves as a source of heat for the second cycle by gas/gas heat exchange in a gas/gas heat exchanger which results in cooling of the products of combustion and circulating working fluid in the first cycle and heating of working fluid in the second cycle. The second cycle is operated in a Brayton cycle including heating of working fluid in the second cycle by the gas/gas heat exchanger, expansion for power generation to provide a second power source, cooling in two-stages by first and second recuperator steps, compression, reheating by counter-current passage via the first recuperator step, and return of working fluid heated by the first recuperator step back to the gas/gas heat exchanger. Working fluid in the first cycle following the compression step is heated by working fluid in the second cycle by counter-current passage via the second recuperator step.
Claims
1. A power production method comprising operating first and second nested cycles utilising CO.sub.2 as working fluid without mixing of working fluid between the nested cycles, the first cycle comprising a semi-open loop operating under low pressure conditions in which CO.sub.2 is sub-critical, and the second cycle comprising a closed loop operating under higher pressure conditions in which CO.sub.2 is supercritical; the first cycle operating in a Brayton cycle including oxycombustion of hydrocarbons in a combustion chamber under low pressure conditions, expansion for power production to provide a first power source, cooling in a recuperator, compression, reheating by counter-current passage via said recuperator, and return of working fluid heated by the recuperator back to the combustion chamber; water and excess CO.sub.2 resulting from said oxycombustion being separated from the first cycle; the first cycle serving as a source of heat for the second cycle by gas/gas heat exchange in a gas/gas heat exchanger which results in cooling of the circulating working fluid including products of combustion in the first cycle and heating of working fluid in said second cycle; the second cycle operating in a Brayton cycle including heating of working fluid in the second cycle by said gas/gas heat exchanger, expansion for power generation to provide a second power source, cooling in two-stages by first and second recuperator steps, compression, reheating by counter-current passage via the first recuperator step, and return of working fluid heated by the first recuperator step back to the gas/gas heat exchanger; and working fluid in the first cycle following said compression step in said first cycle, being heated by working fluid in the second cycle by counter-current passage via the second recuperator step.
2. The method according to claim 1, wherein said step of cooling of the working fluid including products of combustion in said first cycle occurs prior to said expansion step in said first cycle.
3. The method according to claim 2, wherein said expansion step in said first cycle is performed by a single first turbine, and wherein said gas/gas heat exchanger is positioned upstream of the first turbine in said first cycle.
4. The method according to claim 1, wherein said expansion step in said first cycle occurs prior to said step of cooling of the working fluid including products of combustion.
5. The method according to claim 1, wherein said expansion step in said first cycle is performed by a plurality of first turbines, at least one of which is positioned upstream of the gas/gas heat exchanger.
6. The method according to claim 1, further comprising further cooling the working fluid including products of combustion in said first cycle that has already been cooled in said recuperator in a cooler condenser, and wherein water is separated from said first cycle by separating condensed water from the remaining gaseous working fluid after cooling in said cooler condenser and before said compression step in said first cycle.
7. The method according to claim 6, wherein the hydrocarbon fuel for said first cycle consists of substantially pure methane, and wherein, following further purification, said separated condensed water provides a source of potable water.
8. The method according to claim 1, wherein the maximum temperature of the working fluid in the second cycle is no greater than 800° C., and the maximum pressure in the second cycle is no greater than 400 bar.
9. The method according to claim 8, wherein the maximum temperature of the working fluid in the second cycle is between 700° C. and 800° C. and the maximum pressure in the second cycle is between 200 and 400 bar.
10. The method according to claim 1, wherein the maximum pressure in the first cycle is no greater than 30 bar.
11. The method according to claim 10, wherein the maximum pressure in the first cycle is between 20 and 30 bar.
12. The method according to claim 1, wherein excess CO.sub.2 is removed from the first cycle after the compression step for storage or sequestration.
13. An apparatus adapted to provide mechanical/electrical power in first and second nested cycles utilising CO.sub.2 as working fluid without mixing of working fluid between the nested cycles, the first cycle operating under low pressure conditions in which CO.sub.2 is sub-critical, and the second cycle operating under higher pressure conditions in which CO.sub.2 is supercritical; the apparatus comprising: a first apparatus coupled to provide the first cycle and including a combustion chamber adapted to burn hydrocarbons in oxygen under low pressure conditions, at least one first turbine adapted to expand the working fluid including products of combustion to provide a first power source, a first recuperator for cooling expanded fluid from the at least one first turbine, a first compressor, first fluid couplings for returning working fluid from the first compressor to the combustion chamber via counter-current passage through said first recuperator, and separators for removing water and excess CO.sub.2 from the first cycle; a gas/gas heat exchanger adapted to cool the working fluid including products of combustion in said first cycle, and adapted to serve as a source of heat for the second cycle by gas/gas heat exchange with said working fluid including products of combustion in the first cycle; and a second apparatus coupled to the gas/gas heat exchanger to provide the second cycle and including a second turbine adapted to expand heated second cycle working fluid from the gas/gas heat exchanger to provide a second power source, a two-stage recuperator apparatus for cooling expanded working fluid from the second turbine in a first stage recuperator and subsequently in a second stage recuperator, a second compressor receiving working fluid from the two-stage recuperator apparatus, and second fluid couplings for returning working fluid in said second cycle from the second compressor to the gas/gas heat exchanger via counter-current flow through the first stage recuperator thereby to be heated; and the first fluid couplings being coupled to the second stage recuperator to heat working fluid in the first cycle prior to further heating thereof in the first recuperator.
14. The apparatus according to claim 13, wherein said first apparatus comprises a single first turbine, and the gas/gas heat exchanger is positioned upstream of the first turbine.
15. The apparatus according to claim 13, wherein said first apparatus comprises a single first turbine, and the gas/gas heat exchanger is positioned downstream of the first turbine.
16. The apparatus according to claim 13, wherein said first apparatus comprises a plurality of first turbines, at least one of which is positioned upstream of the gas/gas heat exchanger.
17. The apparatus according to claim 13, wherein a cooler condenser is coupled to the first recuperator to receive the working fluid including products of combustion therefrom in said first cycle before passing said working fluid with products of combustion and condensed water to said separators.
18. A self-contained power system adapted for use in a marine vessel and comprising the apparatus according to claim 13, wherein one of the first and second power sources is adapted to provide mechanical drive to propel the vessel and the other is adapted to provide electricity for the vessel.
19. The self-contained power system according to claim 18, further comprising a treatment apparatus adapted to treat the separated water to provide a source of potable water for the vessel.
20. A self-contained power system adapted for use in an isolated oil or gas well drilling facility and comprising the apparatus according to claim 13, wherein one of the first and second power sources is adapted to provide mechanical drive to propel a drill and the other is adapted to provide electricity for the facility.
21. The self-contained power system according to claim 20, further comprising a treatment apparatus for treating the separated water to provide a source of potable water for the facility.
22. A self-contained power system adapted for use in an isolated oil or gas production facility and comprising the apparatus according to claim 13, further comprising a treatment apparatus for treating the separated water to provide a source of potable water for the facility, and an injection means adapted to inject the removed excess CO.sub.2 into the ground for enhanced oil or gas recovery or for CO.sub.2 sequestration.
23. A chemical or petrochemical plant or refinery, provided with an integrated self-contained power system comprising the apparatus according to claim 13, wherein the removed excess CO.sub.2 from the apparatus serves as a CO.sub.2 source for process use or for sequestration, the separated water from the apparatus serves as a water source for process use or being treatable to provide a source of potable water for the plant or refinery, and excess heat from the apparatus serves as a source of heat for process use.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) Reference will now be made to the accompanying drawings, by way of example only, in which:
(2)
(3)
(4)
(5)
DESCRIPTION OF PREFERRED EMBODIMENTS
(6) Power generation systems of the kind schematically illustrated in
(7) Typical figures for temperature and pressure given below are derived from NIST (National Institute of Standards and Technology) and validated using process modeling and computer simulations.
(8) Referring to
CH.sub.4+2O.sub.2═CO.sub.2+2H.sub.2O
The use of oxygen, rather than air, and the use of LNG as fuel provide clean and complete combustion to CO.sub.2 and water with minimal production of undesirable NO.sub.x and SO.sub.x pollutants. The combustion requires the significant quantities of CO.sub.2 provided by recirculation of the working fluid in the first cycle to cool the flame temperature so that combustion is conducted within the conventional bounds of existing materials and technology. Such use of CO.sub.2 in sub-critical low pressure combustion, typically at 20-30 bar, means that commercially available combustion chambers using generally available materials may be employed. The working fluid and products of combustion typically exit the combustion chamber at 20-30 bar and 800-1200° C. This high temperature low pressure gas passes in the first cycle to a gas/gas heat exchanger 12 which is also included in a second high pressure cycle discussed below. It should be noted that there is no mixing between working fluid in the two cycles.
(9) Approximately 70% of the heat content of the combustion gases is transferred to high pressure working fluid in the second cycle through heat exchanger 12. Low pressure working fluid in the first cycle exiting the heat exchanger 12 passes to a low pressure expander in the form of first turbine 13 and is still at a relatively high temperature of 500-900° C. (more preferably 500-750° C.) with sufficient energy to allow the first turbine 13 to extract a useful quantity of power.
(10) Alternatively, the turbine 13 could be positioned before the heat exchanger 12, or there may be a plurality of first turbines 13 which may operate in parallel, or serially, and at least one of which may be positioned before the heat exchanger 12. Arrangements in which the or a turbine 13 is positioned upstream of the heat exchanger 12 are less preferred, as such turbine would need to be specially constructed from alloys capable of withstanding the high temperatures of gases directly from the combustion chamber and/or would require blade cooling.
(11) In the illustrated embodiment, fluid from the first turbine is first cooled by a first recuperator 14 which transfers heat to recirculating CO.sub.2 passing back to the combustion chamber 10, and then by a cooler 15, typically to a temperature of 20-60° C. so that water condenses into liquid water which is separated in separator 16, from which separator produced water is removed by water pump 17 to provide a treatable source for a potable water supply. The remaining CO.sub.2 gas, typically at 10 bar and 20-60° C., passes to first compressor 18 where it is compressed to 20-30 bar and 110-130° C., passes through an after cooler 19 where it is cooled to 20-60° C. before being reheated, firstly to 120-140° C. in a second stage 20 of a two-stage recuperator 21 included in the high pressure second cycle and discussed below, and then in first recuperator 14 as mentioned above, from which it emerges at 20-30 bar and 400-600° C. before passing in recirculation to combustion chamber 10. Excess CO.sub.2 is withdrawn from the first cycle at 22 downstream of the first compressor 18 and after cooler 19.
(12) Practical embodiments of first turbine 13 and first compressor 18 may be relatively compact and lightweight as compared with typical gas or steam turbines or large diesel engines. For example a range of turbomachinery rotors are available from equipment manufacturers that currently supply high pressure gas compressors which can attain the pressures from 10-30 bar to 400 bar envisaged in practical embodiments of the present process and also mechanical drive steam turbines that are built to withstand 150 bar and 600° C. Suitable such equipment is listed in Compression Technology Sourcing Supplement, published March 2017 by Diesel & Gas Turbine Publications, Waukesha, Wis. 53186-1873, United States of America. Conventional industrial heavy duty gas turbines are designed and manufactured to higher temperatures than envisaged in the present process but the pressures are limited to 30 bar, namely pressures of the order of the maximum pressures envisaged in the first low pressure cycle in practical embodiments of the present process.
(13) The second cycle uses CO.sub.2 as working fluid in an essentially closed cycle at high pressure at which the CO.sub.2 is in a supercritical state. At the critical pressure of 73 bar and a temperature of 35° C. CO.sub.2 becomes super dense and behaves more like a liquid than a gas, and requires greatly reduced compression power. Supercritical CO.sub.2 above this temperature and pressure has a very high density and specific heat more like a liquid than a gas. As explained above, the combustion products in the first cycle serve as heat source for the second cycle at gas/gas heat exchanger 12 from which the supercritical CO.sub.2 emerges at 200-400 bar and 700-800° C., passing to second turbine 23. Because the second cycle operates under high pressure conditions in which the CO.sub.2 is supercritical, the bulk of the power produced in the system as a whole is generated by expansion in second turbine 23. The working fluid emerges from second turbine 23 at 80 bar and 500-600° C., and is cooled in two-stage recuperator 21 and a further cooler 24 before passing via a KO drum 25, to condense any liquid droplets that might be present, to second compressor 26. The two stage recuperator 21 includes a first stage 27 in which working fluid in the second cycle returning to the gas/gas heat exchanger 12 is heated, emerging at 200-400 bar and 500-600° C., having been heated by expanded working fluid from the second turbine 23. Working fluid from second turbine 23 emerges from the first stage 27 of the recuperator at 80 bar and 130-150° C. and is further cooled to 70-80° C. in the second stage 20 of the recuperator, where heat is transferred to low pressure working fluid in the first cycle passing from the first compressor 18 back towards the combustion chamber 10, as explained above. Cooler 24 further reduces the working fluid in the second cycle to a temperature of 40° C. at 80 bar.
(14) The system described lends itself to variation for specific needs. For example, for ship propulsion systems, the high pressure gas flow from the gas/gas heat exchanger can be split into two streams passing to parallel expander turbines. One may be used to generate electrical power by running at constant speed. The other may be run at varying speeds to drive the ship propulsion system.
(15) The proposed compressors are small and compact and may suitably be of the centrifugal type. In view of this, it will be seen that the respective compressors of
(16) Provision is made at 30 and 31 respectively to fill the first low pressure cycle and the second high pressure cycle with dry CO.sub.2 at start up.
(17) As the maximum temperature of working fluid in the second cycle in the
(18) Embodiments of the nested first and second CO.sub.2 cycles described above can achieve net efficiencies of over 40%, which is higher than for conventional steam or gas turbine systems while being much lighter and occupying significantly less space than conventional steam or gas turbine power generation systems. Moreover, they can do so without needing to rely upon the extreme temperatures and pressures necessary for the Allam cycle to achieve its claimed efficiencies, as a result of which proven and readily available materials and readily available components can be employed.
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(20) The small weight and space requirements for practical embodiments of our system that can produce 50 MW of power by clean combustion without emissions and at a net efficiency of around 40% make the system especially suitable for powering marine vessels or for use on isolated oil or gas platforms. The turbomachinery required for the high pressure cycle in a practical embodiment of 50 MW power system in accordance with the present teachings may be very compact by virtue of employing supercritical CO.sub.2 and so may have a bulk no greater than that of a conventional cargo container. That required for the low pressure cycle would be greater, but with suitable design and optimisation of equipment, considerable saving in weight and space overall may be achieved by practical embodiments of power system of the kind described herein, as compared with conventional steam turbines used to power container ships and bulk oil or LNG bulk carriers. Such savings may be utilised to increase the payload carried, making operation more profitable. On an isolated oil or gas platform, space is always at a premium.