The present invention is applied to the energy field, in particular it integrates power production technologies and storage technologies.
It is known that electrical energy production and network stability rely on a variety of sources and technologies, first and foremost including thermal fuel power plants of various nature, nuclear, hydroelectric, wind, solar power plants, etc.
Peculiar aspects of each of these sources are mainly:
Each of the aspects mentioned above corresponds to a constraint in the possibility of exploiting the energy source at issue; indeed:
Based on these three aspects, the energy sources and the related exploitation technologies can be classified into:
The rigidity and discontinuity of the energy sources are responsible for a misalignment between supply and demand and the consequent instability of the electrical power network, overloaded with energy which is impossible to be utilized by a small demand at certain times and others in which it is not sufficiently supplied.
The issue of emissions, on the other hand, is increasingly driving the replacement of thermo-electric combustion technologies with sources having a lower environmental impact, mainly solar and wind, which aggravate the problem of instability of the electrical power network because of their discontinuity.
Nowadays, the strategy to make the network stable consists of covering the demand peaks by means of hydroelectric and turbogas power plants which, by virtue of higher flexibility and less inertia in load variations, are particularly suitable for this purpose.
However, hydroelectric technology is mature and little space remains for its further diffusion, while turbogas power plants are responsible for the emission of large amounts of greenhouse gases.
Research has so far followed separate tracks, studying storage systems for solar and wind energy on the one hand and CO2 sequestration systems for thermal fuel power plants on the other.
One of the most promising storage technologies is the production of liquid air from the excess of electrical energy, to then obtain power therefrom during demand peaks.
This technology is called LAES, standing for Liquid Air Energy Storage, and is shown in
During storage, a LAES plant exploits the energy from renewable sources to produce liquid air, while in use it obtains power from the previously-stored liquid air.
The energy can be conveniently recovered from the liquid air either through the use of a thermal machine operating between the ambient temperature and the evaporation temperature of the liquid air, which is used as a heat sink or through the following process (
The recent technologies in the area of carbon dioxide sequestration are based on combustion in an artificial atmosphere, mainly composed of carbon dioxide and oxygen, which for this reason is referred to as oxy-combustion.
In order to accomplish the oxy-combustion, oxygen from the atmosphere must be separated from nitrogen by means of a very energy-intensive process known in the art.
Known energy production systems by means of oxy-combustion are the Graz cycle and the Allam cycle.
The operation of an oxy-combustion turbogas power plant according to the Graz cycle is diagrammatically shown in
The production process of O2 fed to the combustor is known in the art, and cryogenic air distillation is typically employed for large amounts.
Therefore, the Graz cycle comprises a Rankine steam cycle, which implies the release of large amounts of heat at low temperature, thus compromising the heat recovery efficiency.
A solution to this problem is offered by the Allam cycle, in which the elimination of the Rankine cycle is suggested.
As shown in the diagram in
The process of producing 02 fed to the combustor belongs to the prior art, and cryogenic air distillation is typically employed for large amounts.
The oxy-combustion process is configured as an energy production system, possibly to be used to cover network demand peaks but is not an energy storage system per se.
Furthermore, this system also greatly suffers from the operations of separating oxygen from nitrogen and liquefying a portion of the CO2, which results in an efficiency reduction from a theoretical 58% of a combined cycle, without CO2 sequestration, to 35%.
Furthermore, the Rankine steam cycle for recovering heat from exhaust fumes is limited in efficiency by the significant condensation heat of water, as noted by the inventors of the Allam cycle, in addition to requiring a long series of operations to condition the water and dispose of the additives injected into the latter.
Furthermore, the CO2 obtained from the process is either gaseous, as in the case of the Graz cycle, or liquid, only at high pressure, therefore an additional treatment is needed for it to be stored.
LAES technology requires a significant energy expenditure for the production of liquid air estimated at 0.45 kW/kg, which strongly limits the amount of recoverable energy: the efficiency of a LAES system demonstrated to date is about 15%.
Prior document EP 0 831 205 describes the generation of a gas in a combustor from a fluid containing carbon and/or hydrogen and/or oxygen and from a gas containing at least hydrogen, thus obtaining a fluid which is expanded to produce electrical energy and then fed to a carbon dioxide recovery system.
Prior document DE 103 30 859 describes a semi-closed CO2 cycle for the production of electrical energy, in which a compressor compresses the circulating gas, which is then fed to a turbine after passing through a combustion chamber, in which a boiler for heat recovery is present; the residual heat contained in the expanded exhaust gases is used to generate steam and/or hot water.
Prior document KR 102 048 844 describes a liquefied air regasification system comprising a carbon dioxide scavenging apparatus, where such an apparatus is inserted into a commercial power plant to separate and remove environmental contaminants from the exhaust gases, and a liquefied air regasification apparatus in order to increase the efficiency of environmental contaminant separation and removal while producing additional electrical energy.
The inventors of the present patent application have surprisingly found that oxy-combustion technologies can be synergistically integrated with liquid air energy storage (LAES) technologies, by means of a highly efficient process, which allows obviating the problem of fluctuations in the demand and production of electrical energy, and thus providing a stabilizing effect of the electrical power network, further promoting the use of renewable energy.
According to a first object, the present invention describes a process for producing power by using a high-pressure gas turbine, and liquefying one or more gases, which employs a first and a second working fluid.
In a second object, the present invention describes a variant of the process, in which a medium-pressure gas turbine is employed.
In a third object, the present invention describes a variant of the process, in which a low-pressure gas turbine is employed.
According to further objects of the invention, each process is described according to a first embodiment, in which said liquefaction comprises a step of direct heat exchange between said gas and said second working fluid, while in a second embodiment, said liquefaction comprises a step of indirect heat exchange between said gas and said second working fluid.
According to a first object of the invention, a process for producing power and liquefying one or more gases is described.
In particular, such a method comprises the steps of:
For the purposes of the present invention, step 1) can be achieved by the combustion of an appropriate fuel F at high pressure in an atmosphere of CO2 and O2.
In step 2), the power generated by the expander, represented by a gas turbine, can be converted into electrical and/or mechanical energy according to techniques known in the field.
For the purposes of the present invention, such a power can be converted into electrical energy by using a high-pressure gas turbine.
In particular, a high-pressure gas turbine operates at pressures of about 100-900 barg.
For the purposes of the present invention, in step 3), inside the heat recovery unit WHRU, the cooling of the expanded exhaust gas 2 is obtained by virtue of the heat exchange with a first working fluid.
More in particular, the cooling may be achieved by means of one or a plurality of successive heat exchange steps with said first working fluid.
According to a preferred aspect of the invention, after each heat exchange step, and irrespective of the other steps, said first working fluid may be expanded in a respective step of expansion.
Therefore, according to the present invention, each step of heat exchange may occur with said first working fluid in unexpanded form or in expanded form after one or more successive steps of heating and possible respective expansion.
For the purposes of the present invention, in particular, said steps of heat exchange are first implemented with said first working fluid in an expanded form after one or more steps of expansion, irrespective of the number of steps of heat exchange and possible expansion and then with said first working fluid in an unexpanded form.
Since said first working fluid is heated after each step of heat exchange, the successive steps of heat exchange involve a first working fluid flow which is more and more heated, as well as possibly more expanded.
In an embodiment of the invention, said step 3) comprises: a first, a second, a third, and a fourth heat exchange between said expanded exhaust gas 2 and said first working fluid, as will be described in greater detail below.
For the purposes of the present invention, said first working fluid is liquid air.
As for step 4), the separation between CO2 and condensed water vapor is achieved in the first separator S1 according to techniques known in the art.
As for step 5) of recycling the portion of condensed water vapor 4′ separated in the first separator S1 to the combustor COMB, this is conducted after pumping by means of a first pump P1, thus obtaining a high-pressure flow 4″.
For the purposes of the present invention, before being sent to the combustor COMB, said high-pressure condensed water vapor flow 4″ can be subjected to one or a plurality of steps of heat exchange with the expanded exhaust gas 2 inside the heat recovery unit WHRU, thus obtaining a high-pressure heated water vapor flow 4″.
As for step 8), the yet further dehydration of the further dehydrated exhaust gas 8 is conducted in order to obtain a CO2 flow with a water content of less than 500 ppm and preferably less than 50 ppm.
The flow obtained from step 8) is a flow of exhaust gas 9 mainly composed of CO2, being composed of CO2 at least in 90% molar amount.
In particular, such a step 8) is conducted according to techniques known in the field.
For the purposes of the present invention, the step 9) of liquefying the CO2 includes using both the first working fluid and the second working fluid.
For the purposes of the present invention, said second working fluid is liquid oxygen; for example, said second working fluid flow is liquid oxygen having a purity over 90% and preferably over 95%.
In particular, said step 9) comprises a heat exchange between said exhaust gas 9 mainly composed of CO2 and said first and second working fluids.
A liquid CO2 flow is thus obtained from step 9), which for the purposes of the present patent application can also be referred to as pure CO2; indeed, such a flow comprises only traces of other components, such as oxygen, nitrogen, and argon.
According to a first embodiment of the invention, said heat exchange with the first and second working fluids is direct.
Anticipating a second embodiment of the invention, described below, the heat exchange between said flow of exhaust gas 9 mainly composed of CO2 with the first and second working fluids is indirect.
As described above, in a first embodiment, the liquefaction of CO2 in step 9) is conducted by direct heat exchange between said flow of exhaust gas 9 mainly composed of CO2 and said first and second working fluids.
In particular, said step 9) is conducted inside a liquefaction unit LU.
For the purposes of the present invention, step 9) can comprise the sub-steps of:
In an aspect of the invention, the step 9a) includes cooling the flow 9 mainly composed of CO2 to a temperature between the triple point of CO2 and −40° C.
In an aspect of the invention, steps 9c) and 9d) are optional.
In another aspect of the invention, steps 9c) and 9d), if conducted, can be repeated multiple times, if required and justified by the need to achieve an effective CO2 separation and an acceptable plant complexity.
In particular, the colling steps 9a) and 9c) are preferably conducted in the same exchangers of the CO2 liquefaction unit LUTE.
In step 9d), the gas flow 17 released into the atmosphere mainly consists of oxygen, argon, nitrogen, and non-separated CO2.
A liquid CO2 flow 11 and partially heated first and second working fluids are thus obtained from step 9).
After the heat exchange of step 9), the second working fluid, which is oxygen, is then sent to the combustor COMB for step 1).
As for the liquid CO2 flow 11, this is removed from the system and possibly stored according to the most appropriate methods.
A portion of said liquefied CO2 flow 12 is instead recycled to the combustor COMB, after pumping by means of a second pump P2, thus obtaining a high-pressure liquid CO2 flow 13 (or a recycling CO2 portion).
For the purposes of the present invention, before being sent to the combustor COMB, said portion 13 of high-pressure CO2 is used in the step 6) of cooling the partially dehydrated exhaust gas 5 in the first exchanger TE1, thus obtaining a high-pressure heated CO2 portion 13′.
After this step, the high-pressure CO2 portion 13′ is used in the step 3) of cooling the expanded exhaust gas 2 inside the heat recovery unit WHRU, as described in greater detail below.
As indicated above, the step 3) of heat exchange in the heat recovery unit WHRU between the expanded exhaust gas 2 and the first working fluid comprises either one or a plurality of steps.
According to an embodiment of the invention, said step 3) comprises a first (step 3a), a second (step 3b), a third (step 3c), and a fourth (step 3d) heat exchange.
Indeed, as shown for example in
Such a flow of the first high-pressure working fluid 31 is employed for cooling the flow 9 mainly composed of CO2 inside the second exchanger LUTE, thus obtaining a heated flow of the first working fluid 32; such a flow 32 is then employed in the step 3) of cooling the expanded exhaust gas 2.
In particular, according to an embodiment of the invention, a first heat exchange 3a) is implemented with the expanded exhaust gas 2, thus obtaining a flow of the partially heated first working fluid 33.
Such a flow of the first partially heated working fluid 33 is employed in a second step of heat exchange 3b) with the expanded exhaust gas 2, thus obtaining a flow of the first further heated working fluid 34, which is then expanded in a second expander EX2.
The further heated and expanded flow 35 thus obtained is employed in a third step of heat exchange 3c) with the expanded exhaust gas 2, thus obtaining a flow of the first even more heated working fluid 36, which is then expanded in a third expander EX3 thus obtaining an even more heated and expanded flow 37.
Such a flow of the first further heated and expanded working fluid 37 performs a fourth step of heat exchange 3d) with the expanded exhaust gas 2, thus obtaining a flow of the first working fluid 38 in gaseous phase, which is then expanded in a fourth expander EX4.
The expanded working flow 39 in gaseous phase thus obtained is then released into the atmosphere or employed for other purposes.
For example, it can be employed for the regeneration of molecular sieves possibly employed in the dehydration of the incoming air for the liquid air or oxygen production operations, thus contributing to a greater integration between electrical energy storage and production technologies.
According to the above description, further heat exchanges may be conducted within the heat recovery unit WHRU.
In particular, such further heat exchanges involve:
In particular, the high-pressure condensed flow 4″ is employed in a fifth step of further cooling the expanded exhaust gas 2.
As for the recycling CO2 portion 13′, this is employed in one or a plurality of further heat exchanges with the expanded exhaust gas flow 2.
In particular, such heat exchanges are conducted in counterflow, and therefore the expanded exhaust gas flow 2 will conduct heat exchanges with a less and less cold portion 13′ of heated recycling CO2.
According to an embodiment of the present invention, said portion 13′ of CO2 is employed in a sixth heat exchange, thus obtaining a flow of further heated CO2 13″, and in a seventh heat exchange with the expanded exhaust gas 2 inside the heat recovery unit WHRU, thus obtaining a flow of even more heated CO2 13′″.
Therefore, according to an embodiment of the present invention, the expanded exhaust gas 2 is subjected, in the heat recovery unit (WHRU), to the following steps of cooling:
More in particular, the expanded exhaust gas 2 can be sequentially subjected to the following cooling steps:
For the purposes of the present invention, each of the above steps may be repeated or may be optional.
For the purposes of the present invention, the two working fluids are produced in a preceding step according to methods known in the art, e.g., in an air separation unit (ASU) and in an air liquefaction unit, to be then stored in appropriate tanks, possibly at a pressure above atmospheric pressure.
As described above, in the step 9) of CO2 liquefaction, a second working fluid is employed in addition to the first working fluid.
In particular, said second working fluid, once produced in an air liquefaction unit, is stored in an appropriate tank ST2, possibly at a higher pressure than atmospheric pressure.
A flow of said second working fluid 40 is drawn from the tank ST2 and pumped at high pressure by a fourth pump P4, thus obtaining a flow 41 of the second high-pressure working fluid which is sent to the exchanger of the liquefaction unit LUTE for step 9a).
More in particular, the oxygen can be pumped at a slightly higher pressure than that of the combustor, while the liquid air is pumped at an even higher pressure, e.g., at a pressure up to 300 barg and preferably at a pressure of about 20-300 barg.
After the heat exchange, the flow 42 of the second heated working fluid thus obtained is sent to the combustor COMB for step 1).
According to an alternative embodiment of the present invention, for example depicted in
Indeed, said heat exchange is mediated by a refrigerant vector fluid RF.
For the purposes of the present invention, said refrigerant vector fluid RF is chosen from the group comprising: CF4, argon, R32, R41, R125, etc.
In particular, said step 9′) is conducted inside a liquefaction unit LU.
For the purposes of the present invention, step 9′) can comprise the sub-steps of:
9′0) obtaining, by cooling in a second exchanger LUTE, a cooled flow 50 of a refrigerant vector fluid RF by heat exchange with the pumped flow of the first working fluid 31 and the pumped flow of the second working fluid 41,
For the purposes of the present invention, the flow 9 mainly composed of CO2 of step 9′a) is the CO2 flow obtained from step 8).
In an aspect of the invention, the step 9′a) of CO2 liquefaction includes cooling it to a temperature between the triple point of CO2 and −40° C.
In an aspect of the invention, steps 9′c) and 9′d) are optional.
According to another aspect of the invention, steps 9′c) and 9′d), if conducted, can be repeated multiple times, if required and justified by the need to achieve an effective CO2 separation and an acceptable plant complexity.
In particular, step 9′a) and step 9′c) are conducted in the same refrigerant bath RB.
In step 9′d), the gas flow 17 released into the atmosphere mainly consists of oxygen, argon, nitrogen, and the non-separated CO2.
As for the heated refrigerant fluid flow 51 obtained after the step 9′) of heat exchange with the flow 9 mainly composed of CO2, this is subjected to compression in a second compressor C2 and then cooled in step 9′0).
According to a second object, the invention describes a variant of the process described above.
In particular, as shown in
For the purposes of the present invention, the embodiment described above comprises the use of medium-pressure gas turbines which operate at pressures of about 35-100 barg.
Advantageously, such a process configuration thus allows the use of machines with established and commercially widely available technology.
According to an aspect of the present invention, such a configuration may provide for the step 9) of CO2 liquefaction to be conducted by direct heat exchange between the CO2 flow and the first and second heat exchange/cooling fluids, as described above.
In another aspect of the present invention, such a configuration may provide for the step 9) of CO2 liquefaction to be a step 9′) conducted by indirect heat exchange, by using a refrigerant vector fluid RF, between the CO2 flow and the first and second heat exchange/cooling fluids, as described above.
According to the present invention, a variant of the above process is described.
In particular, as depicted in
For the purposes of the present invention, the embodiment described above comprises the use of low-pressure gas turbines which operate up to about 35 barg.
Advantageously, such a process configuration thus allows the use of machines with established and commercially widely available technology.
According to an aspect of the present invention, depicted for example in
In another aspect of the present invention, depicted for example in
Examples of embodiments according to the above description are diagrammatically depicted in the figures.
In particular, the diagram in
The diagram in
In particular, the diagram in
The diagram in
In particular, the diagram in
The diagram in
From the description provided above, the advantages offered by the present invention will be apparent to a person skilled in the art.
From the plant engineering point of view, the described process allows eliminating the Rankine cycle for the recovery of heat from the exhaust turbine fumes and simplifying the plant, especially if the Rankine cycle uses water as an engine fluid.
Furthermore, the process is particularly suitable for off-shore applications.
According to the integration of an oxy-combustion plant for energy production with a LAES storage, the present invention allows creating a synergy between a system for storing electrical energy, which is in excess of demand at certain times, and a system for producing electrical energy to be fed into the network during periods of increased demand.
In particular, the synergy is demonstrated in the higher efficiency than the efficiency offered by the simple sum of the individual technologies.
One of the most obvious advantages is the possibility of leveling and stabilizing the network, i.e., making its production continuous and aligning the supply with the demand for electrical energy.
By virtue of the stabilizing effect of the electrical power network, the system of the invention promotes further use of renewable energy.
Therefore, this combination allows overcoming the known problems in the industry, while ensuring zero environmental impact.
The integration of oxy-combustion and liquid air energy storage (LAES) technologies results in an energy production battery which combines the merits of both technologies and uses the resulting synergies to eliminate/improve important technical aspects of both.
A particular merit of the present invention is that it achieves an efficiency, with respect to the fuel (calculated based on the LHV), of about 80%, which is particularly high compared to conventional oxy-fuel combustion layouts.
With respect to fuel use, compared to traditional oxy-combustion layouts, the process described increases the life of non-renewable resources, extending the time available for the energy transition.
Number | Date | Country | Kind |
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102020000023167 | Oct 2020 | IT | national |
Filing Document | Filing Date | Country | Kind |
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PCT/IB2021/058984 | 9/30/2021 | WO |