RECOMPRESSED TRANSCRITICAL CYCLE WITH VAPORIZATION IN CRYOGENIC OR LOW-TEMPERATURE APPLICATIONS, AND/OR WITH COOLANT FLUID
20220186884 · 2022-06-16
Inventors
- Massimiliano SBARSI (San Donato Milanese (Milano), IT)
- Lucio AURILIO (San Donato Milanese (Milano), IT)
- Anton Marco FANTOLINI (San Donato Milanese (Milano), IT)
- Salvatore DE RINALDIS (San Donato Milanese (Milano), IT)
Cpc classification
F17C2223/033
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2227/0323
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01K7/32
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C9/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2260/046
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F22B3/08
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2227/0327
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01K19/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2223/0161
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2265/05
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2227/0135
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01K25/103
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C5/06
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2227/0362
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
Abstract
A process for regasifying a fluid and generating electrical energy includes subjecting an operating fluid to 1) pumping, the pumping step including a low pressure pumping step 1a) and a high pressure pumping step 1b), 2) heating in a recuperator to obtain a heated flow, the heating step including a low temperature heat recovery step 2a) and a high temperature heat recovery step 2b), 3) further heating through a high temperature source to obtain a further heated flow, 4) expanding in a turbine, with generation of electrical energy to obtain an expanded flow, 5) cooling by heat exchange to obtain a cooled flow, and 6) condensing the flow of the operating fluid and regasifying the fluid. After low pressure pumping, a portion of the flow of the operating fluid is subjected to recompression to obtain a flow combined with the flow of the operating fluid obtained from step 2a).
Claims
1. A process for regasifying a fluid and generating electrical energy, said process comprising subjecting a flow of an operating fluid to the following steps: 1) pumping, said pumping step comprising a low pressure pumping step 1a) and a high pressure pumping step 1b), 2) heating in a recuperator, thus obtaining a heated flow, said heating step comprising a low temperature heat recovery step 2a) and a high temperature heat recovery step 2b), 3) further heating through a high temperature source, thus obtaining a further heated flow, 4) expanding in a turbine, with generation of electrical energy, thus obtaining an expanded flow, 5) cooling in a heat recuperator by heat exchange, in a step 5a) with the flow of step 2b), and in a step 5b) with the flow of step 2a), thus obtaining a cooled flow, and 6) condensing said flow of said operating fluid and regasifying said fluid, wherein after the low pressure pumping step, a portion of the flow of said operating fluid to a recompression step, thus obtaining a flow which is combined with the flow of the operating fluid obtained from step 2a).
2. The process of claim 1, wherein said recompression step is preceded by a vaporization step I).
3. The process of claim 2, wherein said vaporization step is carried out by a low temperature heat source.
4. The process of claim 1, wherein step 3) is carried out by a high temperature heat source.
5. The process of claim 1, wherein an expansion step is carried out after step 5) and prior to step 6).
6. The process of claim 1, wherein step 6) is carried out by heat exchange with said fluid to be regasified.
7. The process of claim 1, wherein step 6) is carried out by heat exchange by an intermediate fluid which acquires heat in step 6) and releases heat to said fluid to be regasified.
8. The process of claim 1, wherein a step of superheating said fluid to be regasified is carried out after step 6).
9. The process of claim 8, wherein said superheating step is carried out by a low temperature heat source.
10. A liquefied natural gas (LNG) regasification line comprising a regasification section, wherein step 6) of a process for regasifying a fluid and generating electrical energy, said process comprising subjecting a flow of an operating fluid to the following steps: 1) pumping, said pumping step comprising a low pressure pumping step 1a) and a high pressure pumping step 1 b), 2) heating in a recuperator, thus obtaining a heated flow, said heating step comprising a low temperature heat recovery step 2a) and a high temperature heat recovery step 2b), 3) further heating through a high temperature source, thus obtaining a further heated flow, 4) expanding in a turbine, with generation of electrical energy, thus obtaining an expanded flow, 5) cooling in a heat recuperator by heat exchange, in a step 5a) with the flow of step 2b), and in a step 5b) with the flow of step 2a), thus obtaining a cooled flow, and 6) condensing said flow of said operating fluid and regasifying said fluid, wherein after the low pressure pumping step, a portion of the flow of said operating fluid to a recompression step, thus obtaining a flow which is combined with the flow of the operating fluid obtained from step 2a), is carried out inside said regasification section.
11. A liquefied natural gas (LNG) regasification plant comprising one or more regasification lines according to claim 10.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0039]
[0040]
[0041]
[0042]
[0043]
DETAILED DESCRIPTION OF THE INVENTION
[0044] The present invention is particularly described in relation to regasifying liquefied natural gas (LNG), but it is equally applicable for regasifying or vaporizing other liquefied fluids stored at low temperatures (lower than about 0° C.) or at cryogenic temperatures (lower than −45° C.)
[0045] For example, the present invention is applied for regasifying a liquefied gas selected from the group which comprises, for example: air, nitrogen, commercially available hydrocarbon compounds such as alkanes, including for example propane and butane, or alkenes, including for example ethylene and propylene.
[0046] The terms “evaporation” and “vaporization”, which are applicable to LNG, are to be intended as synonyms in the following description.
[0047] Moreover, “liquefied natural gas”, later also referred to as “liquefied gas”, in the present description means a liquid obtained from natural gas after suitable refining and dehydrating processes and next cooling and condensation steps.
[0048] More generally, “liquefied gas” in the present description means a fluid having a mainly liquid component.
[0049] Moreover, the term “low temperature heat source” in the present description means for example: ambient air, seawater, low temperature solar thermal, exhaust heat of a low temperature thermodynamic cycle, low temperature process and/or machinery heat recovery.
[0050] A low temperature source generally operates at temperatures, which are lower than 180° C., preferably lower than 120° C.
[0051] The term “high temperature heat source” instead means for example: high temperature thermal solar, exhaust heat of a high temperature thermodynamic cycle, exhaust gas of a gas turbine or internal combustion engine, high temperature process and/or machinery heat recovery.
[0052] A high temperature source generally operates at temperatures, which are higher than 180° C., preferably higher than 300° C., and even more preferably higher than 400° C. and beyond.
[0053] For the purposes of the present invention, it may be provided that the same low or high temperature heat source feeds several heating systems.
[0054] In the continuation of the description, the term “seawater” refers not only to seawater conveniently processed to remove sediments and conveniently pumped (for example at about 2 bar), but more generally, environmental water obtained from rivers, canals, wells, natural basins such as lakes, etc. and artificial basins.
[0055] For the purposes of the present invention, the operating fluid is CO.sub.2.
[0056] For the purposes of the present invention, an intermediate operating fluid is a fluid capable of carrying out a heat transfer from one cycle to another.
[0057] Such an intermediate operating fluid may perform for example a heat transfer from a first power cycle (to which reference may be made as a topping cycle) and to a second power cycle (to which reference may be made as a bottoming cycle).
[0058] In one aspect of the invention, the bottoming cycle is a power cycle equal to the topping cycle.
[0059] In a preferred aspect, the intermediate operating fluid is different from the operating fluid of the topping cycle.
[0060] For the purposes of the present invention, an operating fluid is involved which is different from CO.sub.2 and preferably is a gas or a gas mixture selected from the group comprising: hydrocarbons, nitrogen, CO.sub.2 and coolants.
[0061] According to a first object, the present invention describes a process for regasifying a fluid to be regasified and for generating electrical energy.
[0062] As described above, such a fluid to be regasified preferably is LNG.
[0063] In a particular aspect of the present invention, the process comprises the employment of an operating fluid, which preferably is CO.sub.2.
[0064] More in detail, the process comprises subjecting an operating fluid to the steps of:
[0065] 1) pumping,
[0066] 2) heating in a recuperator, thus obtaining a heated flow,
[0067] 3) heating through a high temperature source, thus obtaining a further heated flow,
[0068] 4) expanding in a turbine, with generation of electrical energy (through a generator), thus obtaining an expanded flow,
[0069] 5) cooling in a recuperator, thus obtaining a cooled flow,
[0070] 6) condensing said operating fluid flow.
[0071] For the purposes of the present invention, step 1) comprises a low pressure pumping sub-step 1a) and a high pressure pumping step 1b).
[0072] Step 1a) increases the pressure up to about 30 to 60 bar.
[0073] Step 1b) increases the pressure beyond about 150 bar.
[0074] More specifically, after the low pressure pumping step 1a), a portion of the flow of said operating fluid is subjected to a recompression step.
[0075] The recompression increases the pressure up to about 150 bar.
[0076] In a preferred aspect, said flow is subjected to a vaporization step I) prior to recompression.
[0077] With regards to step 2), said step comprises a low temperature heat recovery step 2a) (LTR) and a high temperature heat recovery step 2b) (HTR).
[0078] In particular, step 2a) increases the temperature up to about 200° C.
[0079] The flow of the operating fluid obtained after the recompression is then combined with the flow of the operating fluid obtained from step 2a) to be subjected to step 2b).
[0080] According to the present invention, the operating fluid is CO.sub.2 and such an expansion step 4) is therefore a transcritical expansion step.
[0081] For the purposes of the present invention, step 5) is carried out in the same recuperator as step 2); indeed, the heat exchange of step 5) is carried out with the flow of steps 2b) (high temperature recovery or step 5a)) and 2a) (low temperature recovery or step 5b), respectively, and allows a cooled flow to be obtained.
[0082] As described above, the operating fluid may be CO.sub.2; alternatively, an operating fluid may be employed mainly consisting of CO.sub.2 with the addition of hydrocarbon/additive mixtures, which allow this fluid to be liquefied at higher temperatures than the ambient temperature or to the one of the available cold fluid.
[0083] According to a first aspect of the invention schematized in
[0084] In one aspect of the present invention, the above-described vaporization step I) may be carried out by employing a low temperature heat source, as defined above.
[0085] In another aspect of the present invention, the heating step 3) may be carried out by employing a high temperature heat source, as defined above.
[0086] According to another aspect of the present invention, the fluid to be regasified may be subjected to a superheating step after step 6).
[0087] In particular, said superheating step may be carried out by employing a low temperature heat source.
[0088] For the purposes of the present invention, the flow of operating fluid employed in steps from 1) to 6) of the described process is the flow of operating fluid obtained after the condensation step 6), thereby configuring a cycle.
[0089] According to a second embodiment of the present invention depicted in
[0090] In a preferred aspect of the present invention, the operating fluid is CO.sub.2 and therefore such a further expansion step is a subcritical expansion step.
[0091] According to an alternative embodiment of the present invention depicted in
[0092] More specifically, such an indirect exchange occurs by means of an intermediate operating fluid, as described above.
[0093] Such an intermediate operating fluid circulates within a cycle, referred to as a bottoming cycle.
[0094] More in detail, said bottoming cycle comprises a first exchanger COND1 (which corresponds to the condenser of step 6) and which is the condenser of the topping cycle), inside of which the heat exchange is carried out between the operating fluid and said intermediate operating fluid which is thus heated, and a second exchanger COND2, inside of which the heat exchange is carried out between the intermediate operating fluid and the fluid to be regasified, to which heat is yielded.
[0095] For the purposes of the present invention, the vaporization step I) carried out prior to recompression, the heating step 3) and the possible superheating step of the fluid to be regasified are carried out by employing heat sources as described above.
[0096] In one aspect of the present invention depicted for example in
[0097] Such a configuration, which may equally be applied also in the presence of a bottoming cycle
[0098] According to a further aspect of the present invention not depicted in the drawings, the turbine may actuate the low pressure pump and/or the high pressure pump.
[0099] For the purposes of the present invention, the described process may further comprise a step of regulating the circulating mass flow of CO.sub.2 in the cycle, wherein the CO.sub.2 is kept at the liquid state (also by virtue of the frigories provided by the cold source, and pressurized).
[0100] For this purpose, the plant may comprise a CO.sub.2 storage tank.
[0101] Such adjustment advantageously allows the power of the cycle to be regulated.
[0102] According to a second object of the present invention, there is described a regasifying line for a fluid, preferably the liquefied natural gas (LNG) which allows generating electrical energy by means of the above-described process.
[0103] The term “regasifying line” means that independent and replicable portion of the plant that includes the structures, the equipment, the machinery and the systems for regasifying a given flow of the liquefied natural gas (LNG).
[0104] In particular, such structures, equipment, machinery and systems originate from the tank (TANK) in which the LNG is stored, and comprise cryogenic pumps, possibly low and high pressure pumps and a BOG compressor, which may be common to several regasifying lines, and a regasification section, and end with the regasified LNG introduction point into the distribution network of the gas itself.
[0105] For the purposes of the present invention, the regasification section is the condenser wherein step 6) of condensing the operating fluid and regasifying the fluid to be regasified occurs, according to the above-described process.
Alternatively, a regasifying line of the present invention may be provided in energy bypass configuration with respect to a traditional technology of an existing plant.
As shown in
[0106] According to an alternative embodiment of the present invention, the power cycle described may be integrated with a conventional technology of SCV type. Here, a coil containing condensing CO.sub.2 or a suitable fluid (such as, for example water-glycol) which exchanges heat with the condensing CO.sub.2 heats the vaporization bath.
The layouts proposed may also be applied for making plants for regasifying technical gas (such as, for example hydrogen, air, nitrogen or other gas) or plants with low or cryogenic temperature fluid storages, also for cryogenic depots or storages.
When an export of electrical energy is not provided, to balance out the electric and heat loads, the power cycle may operate on a fraction of the LNG, regasifying the remaining fraction of LNG, with other systems and/or employing the surplus of electric power to feed air heating technologies.
In an alternative configuration, the CO.sub.2 fraction which is not employed for regasifying LNG may be employed for achieving a cooling/liquefaction of the air by utilizing also a part of the electric power generated by the cycle itself, if required; thereby, in addition to obtaining a liquid air storage, nitrogen and oxygen may be obtained, and the latter may be employed to achieve a CO.sub.2 cycle with internal oxy-combustion technologies.
The values indicated in the following section refer to a reference regasifying plant by way of explanation, but are in any case valid if considered as specific/unitary value.
Moreover, the results obtained in terms of extractible net electric power and thermodynamic efficiency of the cycle refer to a pressure of 100 to 250 or 150 to 350 bar and beyond A, and at a temperature of about 350° C. to 550° C. or 450° C. to 650° C., up to 700° C. and beyond, at the transcritical expansion turbine input, where applicable.
The diagram in
CO.SUB.2 .Circuit
[0107] The variation with respect to the diagram of the background art in
Then, it is not separated but is entirely sent to the condenser (COND 1), condensing at a lower pressure with respect to the diagram in
Indeed, the fluid is sent to a low pressure pump (LP-P) where it is pumped at a pressure between 30 and 60 bar (7), in any case corresponding to the evaporation temperature in (11). The fluid is output from the low pressure pump divided into two flows. The first flow (14) is sent into a high pressure pump (HP-P) and is pumped at a pressure higher than 150 bar (8), then it is sent to the heat exchanger (LTR) where it is preheated at a maximum temperature of about 200° C. (9). The second flow (13) is vaporized by the ambient heat to a variable ambient temperature between 0° C. and 30° C. through an air cooler (AMB VAP or LTR2) (11) and then is sent to the recompressor (R-COMPR) to be compressed at a higher pressure than 150 bar (12). This flow output from the recompressor is combined with the one (9) from the first heat exchanger (LTR) and is sent to the second heat exchanger (HTR) (10) to be further superheated (1).
The main results are: a net electric power up to 21.4 MWe, thermodynamic performance up to 62.2% (not considering the ambient heat in AMB VAP/LTR2), employing a total circulating CO.sub.2 of 294.6 t/h.
LNG Circuit
[0108] 123.61 t/h of LNG are drawn at the temperature of −156.6° C. and at a pressure of 90.5 bar A (100). Then, the LNG receives heat in COND 1 (24.34 MWt), reaching the temperature of 2.5° C. (101).
If the employment of a seawater circuit is provided (optional for the vaporization of the CO.sub.2, not depicted in the drawings), an (optional) seawater circuit may be integrated in the CO.sub.2 cycle to provide the heat duty required at AMB VAP to vaporize the CO.sub.2.
With reference to the above-described case, 1828.44 t/h of seawater at the temperature of 30° C. and at atmospheric pressure are drawn at the seawater intake and pumped at the pressure of about 2 bar A by means of a pump. The flow is then fed to the CO.sub.2 AMB VAP (10.61 MWt) vaporizer, where it is cooled by 5° C. and discharged into the sea, thus allowing the vaporization of the CO.sub.2 at a pressure of 45.01 bar and a corresponding temperature of 10° C. (11) on the other side of the exchanger AMB VAP.
The main results in terms of net electric power and thermodynamic performance are entirely similar to those obtained in the above-described case, less the power required for pumping the seawater.
The same reference diagram in
The circuit is the same, but the LNG is not entirely regasified, i.e. up to a temperature of 2.5° C., by means of the condensation of the power cycle. Indeed, the remaining portion is regasified through an ambient means, which may be seawater. Moreover, it is employed for the vaporization of the CO.sub.2 in AMB VAP (also described in the option indicated in the above-indicated case).
CO.SUB.2 .Circuit
[0109] With respect to the diagram in
LNG Circuit
[0110] The output temperature of the natural gas (LNG regasification) is lower given that it is heated with the CO.sub.2 cycle through the same condenser (COND 1) with a variable temperature reached between −55° C. and 0° C. (101). Therefore, a further superheating fluid is required to heat the natural gas at the required temperature, included between 0 and 10° C. (in the particular case, of 2.5° C.). For this purpose, the natural gas is sent into an ambient air cooler or into an optional seawater circuit (102).
With respect to the above-described circuit (diagram 3A without the dotted section), the LNG is not entirely vaporized up to the temperature of 2.5° C. through the heat exchange with the CO.sub.2 in COND1. The following description is consistent with the balance indicated above.
123.61 t/h of LNG are drawn at the temperature of −156.6° C. and at a pressure of 90.5 bar A (100). Then the LNG receives heat (17.4 MWt) if, as indicated above, the pressure CO.sub.2 circuit side to the flow (6) is equal to 8.318 bar in COND1 up to reaching a temperature of −46° C. (101). The remaining part of the vaporization, which is dependent on the preceding heat exchange in COND1, is completed in the heater SH where the LNG receives heat from the seawater circulating in a dedicated circuit and reaches a temperature of 2.5° C. (102).
Seawater Circuit (not Depicted in the Drawings)
[0111] A seawater circuit is installed to provide, downstream of COND1, the remaining heat required for the vaporization of the LNG up to 2.5° C. Moreover, it may (optionally) be integrated in the CO.sub.2 cycle to provide the heat duty required to vaporize the CO.sub.2 in AMB VAP and it requires being integrated.
With reference to the actual above-described case, 2681.39 t/h of seawater at the temperature of 30° C. and at an atmospheric pressure are drawn at the seawater intake and pumped at the pressure of about 2 bar A by means of a pump. Of this flow, a part, i.e. 1485.31 t/h, of seawater are (optionally) fed to the vaporizer AMB VAP (8.62 MWt) where they are cooled by 5° C., thus allowing the vaporization of the CO.sub.2 at a pressure of 45.01 and a corresponding temperature of 10° C. (11) on the other side of the exchanger AMB VAP. The remaining flow, i.e. 1196.08 t/h of seawater, instead is fed to the heater SH (6.94 MWt) where it is cooled by 5° C., thus allowing the vaporization of the LNG from the temperature obtained at the output of COND1 up to reaching a temperature of 2.5° C., not obtained with the condenser COND1 alone. It therefore is mixed with the flow output from AMB VAP and is discharged into the sea at the temperature of 25° C.
Alternatively, as shown in diagram 2B, the cycle in
It is worth noting the reference diagram in
CO.SUB.2 .Circuit
[0112] The diagram provides for the operating fluid at the output of the heat exchangers (HTR and LTR, where the fluid is desuperheated (5)) to be further expanded in SC-EXP (15) prior to being fed to COND1.
[0113] The advantages offered by the present invention are apparent to a person skilled in the art from the description above.
[0114] Considering the conventional regasification technologies, the main advantages of the solution appear to be: [0115] reduction of the consumption of fuel gas with respect to the SCV technology, the advantage expressed in terms of Fuel Gas Saving (FGS)=(Gas cycle consumption−SCV or ORV consumption)/SCV or ORV consumption [%] up to 60% (30%) with energy surplus availability; [0116] reduction of the CO.sub.2 emissions up to 60% (30%), (proportionately to the reduction of the fuel gas consumption, with respect to a conventional SCV and ORV technology); [0117] generating electrical energy may be employed to meet the plant needs and for exporting the same; [0118] specific technical problems are avoided or significantly reduced both for the above-mentioned ORV and for SCV; [0119] all the advantages associated with the employment of carbon dioxide as operating fluid can be utilized: low freezing point, stability.
[0120] Moreover, more in detail, the following was positively noted: [0121] the availability of a cold well, represented by the LNG or other technical gas to be regasified or by a storage at low or cryogenic temperatures, which allows the CO.sub.2 to be liquefied at different pressures, thus obtaining (Brayton-Rankine) transcritical CO.sub.2 power generating cycles, with significantly greater efficiency than the CO.sub.2 (supercritical) Brayton cycles; [0122] the employment of a pump for compressing the condensed CO.sub.2 allows a reduction of the power required by the cycle and of the plant cost to be obtained with respect to the employment of the primary compressor required in the supercritical CO.sub.2 Brayton cycles; [0123] engineering simplicity, especially for retrofitting existing plants, the CO.sub.2 power cycle may be integrated in a conventional SCV technology, as described above; [0124] the possibility of including a CO.sub.2 storage tank (not depicted in the drawings) allows regulating the power of the cycle by regulating the circulating mass flow in the cycle, where the CO.sub.2 is kept in the liquid state also by virtue of the frigories provided by the cold source, and pressurized: this allows a given operating flexibility to be obtained also in the startup and stop steps and in potential emergency scenarios; and it simplifies designing the storage tank, which may operate at lower pressures and with smaller volumes.
[0125] More specifically, with respect to the CO.sub.2 transcritical power generating cycles, the following advantages can be recognized: [0126] the CO.sub.2 transcritical power generating cycles allow the expansion from high pressures in supercritical step to low pressures in subcritical step, under condition of condensing the CO.sub.2 at low temperatures, using the LNG or a fluid with adequate thermal level as cold well, by means of one or more expansion turbines, utilizing the specific high work of the fluid at high pressures: by allowing an increased expansion ratio of the turbines, this generates sufficient power to feed the utilities of the LNG regasification plant or also a surplus of electric power generated available to feed possible external utilities; [0127] the optimization of the transcritical CO.sub.2 cycle allows an increased share of frigories available during the LNG vaporization to be used and drastically reduces the consumption of energy required to regasify the LNG.
[0128] With reference to the drawings in
[0131] With reference to the drawings in
[0133] Overall, the cascade power generating cycles may be combined so as to best utilize the features and constraints thereof to the advantage of regasifying the LNG, thus improving the employment of the frigories (vaporization curve). Although they have increased engineering complexity, they allow the overall plant efficiency to be improved.
[0134] In the case of a CO.sub.2 topping cycle and a bottoming cycle with fluid different from CO.sub.2 as described above: [0135] the condensation of the CO.sub.2 is carried out by means of the vaporization of the fluid in the bottoming cycle which occurs at temperatures which are compatible with the solidification of the CO.sub.2 and which condenses, recuperating the LNG frigories with a more efficient LNG vaporization curve and the possibility of recuperating all the frigories available in the LNG; [0136] the addition of the topping cycle allows the extraction of increased power with respect to the system with only bottoming cycle and the possibility of best utilizing the available heat sources, especially if at high temperature, thus allowing the recuperation of this heat to be distributed between the two cycles; in particular, the range of condensation temperatures of the CO.sub.2 (between the triple point at −56.56° C. and the critical temperature of +30.98° C.) allows a bottoming cycle with organic fluid to be coupled in an optimal manner to one of the innovative CO.sub.2 cycles proposed in this paper and to optimize the pressure jumps in the two-cycle turbines.
[0137] Moreover, the CO.sub.2 topping cycle is a supercritical/transcritical cycle with recuperator and recompressor, therefore the energy available at high temperature is utilized well in a high efficiency topping cycle, instead designating the energy at lower temperatures (the one discharged from the top cycle) to the ORC bottoming cycle. The two cascade cycles (CO.sub.2 topping cycle and ORC bottoming cycle) are optimized with the heat inputs in the temperature ranges appropriate thereto, with benefits to the overall efficiency and simplification in designing the turbomachinery.
[0138] All the embodiments of the invention may operate in configuration both of energy bypass at a conventional regasifying technology for an existing plant (as shown in