Method for Liquid Air and Gas Energy Storage
20190063265 ยท 2019-02-28
Assignee
Inventors
Cpc classification
F01L15/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02B41/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2270/0581
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J1/004
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2265/07
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J1/0012
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J2210/62
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2221/031
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2265/066
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Y02T10/12
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
F17C2227/0309
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01K27/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J1/0251
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J2230/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J1/0092
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02B29/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C2265/05
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J1/0224
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
H02J15/006
ELECTRICITY
F17C9/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01D15/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J1/0222
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25J2230/30
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
F01K27/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F17C9/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
H02J15/00
ELECTRICITY
F02B29/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02B41/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F01D15/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Abstract
A method for liquid air and gas energy storage (LAGES) which integrates the processes of liquid air energy storage (LAES) and regasification of liquefied natural gas (LNG) at the import terminal through the exchange of thermal energy between the streams of air and natural gas (NG) in their gaseous and liquid states and includes harnessing the LNG as an intermediate heat carrier between the air streams being regasified and liquefied, recovering a compression heat from air liquefier for LNG regasification and utilizing a cold thermal energy of liquid air being regasified for reliquefaction of a part of send-out NG stream with its return to LNG terminal.
Claims
1. A method for liquid air and gas energy storage (LAGES) comprising in combination: pumping the liquefied natural gas (LNG) from the tanks of LNG Storage and Regasification (LNGSR) terminal into a co-located Liquid Air Energy Storage (LAES) system for continuous regasifying the LNG in the said system and final injecting the regasified LNG into a transmission pipeline; interchanging a waste thermal energy between the LNG being regasified and the process air being continuously liquefied in the LAES system; consuming a required power from the grid and/or other energy source for production of the liquid air with its storing only in the periods of low demand for energy in the grid; on-demand discharging the said LAES system with generation of the on-peak power delivered into grid through consuming both a stored and directly produced liquid air at a rate exceeding a rate of its direct production; and wherein the improvement comprises in combination: pumping the whole amount of LNG destined for regasification and its delivering into LAES system at the first low pressure and first low temperature during the LAES system discharging; using a minor part of cold thermal energy of discharged liquid air for deep cooling the said delivered LNG down to the second low temperature, which is below the first one; controlled dividing the deeply cooled LNG stream into two parts, first of which is further pumped at the second high pressure and regasified in the LAES system during its discharging; storing the second part of deeply cooled LNG at a pressure not exceeding the first low one and at a temperature not exceeding the second low one; pumping the stored second part of deeply cooled LNG at the second high pressure and its regasifying in the LAES system during its charging only; using most of the cold thermal energy of discharged liquid air for reliquefying a part of highly pressurized NG extracting from the outlet of LAES system; and depressurizing and recycling a reliquefied NG into the tanks of LNGSR terminal, resulting in enhancement of LAES power output at the given LNGSR terminal send-out capacity.
2. A method as in claim 1, wherein a relationship between the mass flow-rates of a said LNG stream being regasified in the LAES system and a said air stream being liquefied in the LAES system is maintained in the range of (1.05-1.15):1, whereas a share of NG being reliquefied in the LAES system is provided in the range of 15-35% of the LNG being regasified in this system.
3. A method as in claims 1 and 2, wherein charging the LAES system includes the following steps: pressurizing the feed air stream in intercooled compressor set up to an intermediate cycle pressure; aftercooling and drying the pressurized feed air stream with its freeing from the atmospheric CO.sub.2 contaminants; pressurizing the recirculating boil-off air stream in the uncooled compressor set up to said intermediate cycle pressure; forming a process air stream as the mixture of the pressurized feed and recirculating boil-off air streams with following pressurizing the process air stream in two-stage intercooled compressor set up to top cycle pressure; deep cooling the process air stream by the LNG stream, resulting in liquefaction of the process air stream and regasification of the LNG stream; following reducing a temperature of the liquefied process air by the stream of recirculating boil-off air; final cooling and depressurizing the liquefied process air in the liquid air expander, resulting in formation of deeply cooled two-phase process air stream escaping the said expander at the lowest cycle temperature and lowest cycle pressure close to its atmospheric value; separating the liquid and boil-off phases of process air with recirculation of boil-off air phase; and storing a liquid air phase during off-peak hours or its direct use in the discharging the LAES system for production of on-demand power.
4. A method as in claims 1-3, wherein compression heat extracted from the pressurized feed and process air streams is recovered for superheating the regasified LNG stream up to a minimal temperature required for its injection into a transmission pipeline, for which purpose the water or water-glycol cooling medium transferring a compression heat from pressurized feed and process air to regasified LNG circulates in a closed loop and provides a temperature of cooled air at the inlet of intercooled compressor stages not exceeding 10 C.
5. A method as in claims 1 and 2, wherein discharging the LAES system includes the following steps: pumping the consumed liquid air delivered directly from a said process air separator and from the LAES storage tank up to a top discharge pressure; heating a consumed liquid air, resulting from recovering a part of its cold thermal energy for said deep cooling the whole of delivered LNG down to the second low temperature; further heating and regasifying a consumed liquid air, resulting from recovering another part of its cold thermal energy for said reliquefying a part of send-out NG extracting from the outlet of LAES system; final heating the regasified consumed air by a stream of exhaust gases escaping the LAES system; expanding the regasified consumed air down to an intermediate pressure required for supercharging the downstream installed reciprocating gas engine with the combustion air, accompanied by production of the expansion power delivered into grid; cooling the partially expanded consumed air down to an intermediate temperature required for supercharging the downstream installed reciprocating gas engine with the combustion air; using the partially expanded and cooled consumed air for combustion of fuel in the downstream installed reciprocating gas engine; operating the said engine with production of a power delivered into grid; releasing the exhaust gases from the said engine at the enhanced pressure and temperature; expanding the exhaust gases down to a pressure close to its atmospheric value, accompanied by production of the expansion power delivered into grid; recovering a waste hot thermal energy of expanded exhaust gases for the said final heating the regasified consumed air; and releasing the cooled exhaust gases into atmosphere.
6. A method as in claims 1 and 5, wherein a temperature of exhaust gases before their said expansion is increased through their heating in the duct burner with consumption of a required fuel.
7. A method as in claims 1 and 3, wherein the full or a part of power required for production of liquid air in the LAES system is delivered by the grid-connected power expanders, installed at the pressure reduction stations of the NG transmission pipelines and converting a gas pressure drop potential into useful energy.
8. A method as in claim 1, which is used for provision of the base-load operation of the LAES system with its charge and discharge coincident in time, for which purpose the whole amount of liquid air continuously produced with use of charge power is instantly directed for a said deep cooling of LNG and its regasification, as well as for production of the discharge power, whereas the whole amount of deeply cooled LNG is instantly pumped up to a high pressure and subjected to regasification in the LAES system.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0020] Embodiments will hereinafter be described in detail below with reference to the accompanying drawings, wherein lie reference numerals represent like elements. The accompanying drawings have not necessarily been drawn to scale. Where applicable, some features may not be illustrated to assist in the description of underlying features.
[0021]
[0022]
[0023]
[0024]
DETAILED DESCRIPTION OF THE INVENTION
[0025] The practical realization of the proposed method for liquid air and gas energy storage (LAGES) may be performed through the integration between the LNG storage and regasification (LNGSR) terminal and liquid air energy storage (LAES) system. At such LAGES facility the interchanging of a waste thermal energy between the LNG being regasified and partially reliquefied and the process air being liquefied and regasified provide a drastic increase in performance of the LAES system and LNGSR terminal.
[0026] The general principles of the LAGES operation in energy storage mode are illustrated with the
[0027] Production of liquid air is performed continuously during both charge and discharge of the LAES system in its CH train. For this purpose the train is supplied with fresh air 12 and electricity 13 from the grid 14. The energy intensity of air liquefaction is significantly reduced, resulting from the said heat exchange between the process air stream being liquefied and LNG stream being regasified in the regasifier 6. In so doing a mass flow-rate relationship between these two streams should be maintained in the range of (1.05-1.15):1. The resultant liquid air product is delivered through control valve 15 into tank 16 for storage during off-peak hours or may be instantly used together with the previously accumulated liquid air from the tank 16 for production of on-demand power during on-peak hours. For these purposes the combined liquid air stream is delivered by high pressure pump 17 into LNG deep cooler 3, wherein a minor part of cold thermal energy of this air is transferred to the LNG stream being cooled. The liquid air escapes the LNG cooler 3 at a somewhat increased temperature and is delivered into liquid air regasifier 18, wherein most of its cold thermal energy is recovered for reliquefying a part of highly pressurized NG extracting from the outlet of CH train. The resultant regasified and highly-pressurized air is directed to DCH train, which is also supplied with NG fuel 19. The on-demand power 20 produced by the DCH train is delivered into grid 14, whereas the LAES exhaust gases 21 are removed to atmosphere. A pressure of NG reliquefied in the liquid air regasifier 18 is reduced in the liquid gas expander 22, after which the reliquefied NG may be returned into storage tank 2 of LNGSR terminal or used for loading the trucks 24 and ship bunkering. In so doing, a share of the highly-pressurized regasified NG directed to reliquefaction may be maintained in the range of 15-35% of total amount of LNG regasified in the LAES system.
[0028] The general principles of charge (CH) train operation during the LAES discharge and charge are illustrated with the
[0029] The fresh air 11 is continuously pressurized by the intercooled compressor 12 up to an intermediate pressure and aftercooled in air cooler 13 with following drying and freeing from the atmospheric CO.sub.2 contaminants in adsorber 14. In its turn a boil-off air is pressurized by the uncooled compressor 15 up to the same pressure. The process air, as the mixture of the fresh and boil-off air streams, is pressurized by the intercooled compressor 16 from an intermediate up to a top cycle pressure, at which it is delivered into air liquefier/NG regasifier 7. A power required for driving all the compressors is delivered from the grid during off-peak hours and from the DCH train of the LAES system during on-peak hours. In the device 7 a heat exchange between the high-pressure process air being liquefied and high-pressure LNG stream being regasified is performed. Through recovery of compression heat in the CH train, a temperature of NG stream escaping the device 7 in gaseous state via pipe 17 is further increased in NG heater 18 up to a level required for injection of NG into gas network. For these purposes the CH train is equipped with the closed cooling system, including the intercoolers of the air compressors 12 and 16, aftercooler 13, balance heat exchanger 19, NG heater 18 and pump 20, providing the circulation of water or water-glycol mixture through all the equipment. A temperature of NG injected into gas network may be maintained at a level of 5-15 C. with simultaneous provision of the air temperature at the inlet of all stages of intercooled compressors at a level not exceeding 10 C.
[0030] The high-pressure liquefied process air escaping the device 7 is further cooled in heat exchanger 21 by a stream of boil-off air and depressurized in the liquid air expander 22 with final liquid air cooling down to a bottom cycle temperature. The two-phase air stream at the expander outlet is divided in the air separator 23 into two streams: boil-off air and liquid air. The boil-off air stream is recirculated through heat exchanger 21 to inlet of compressor 15, whereas the liquid air stream is delivered into the liquid air storage 24 during off-peak hours or bypasses the storage 24 via pipe 25 during on-peak hours. During on-peak hours the mixture of two liquid air streams (from pipe 25 and from storage 24) is pumped by the high-pressure pump 26 through LNG deep cooler 4 and delivered via pipe 27 to DCH train. A heat transfer between the low-pressure LNG stream and high-pressure liquid air stream in the cooler 4 is performed without changes in phase of both streams and leads to cooling the LNG by approximately 10-15 C. and heating the liquid air by approximately 20-30 C. A deep cooling of LNG provides its sufficiently low temperature at the inlet of device 7 that a high process air liquefaction ratio may be achieved in the CH train. A storage of the deeply cooled LNG between the LAES discharge and charge may be optionally performed in the service tank 9 under low pressure provided by the LNG pump 1. In this case the installation and operation of liquid air expander 8 and low pressure LNG pump 10 are not required.
[0031] The general principles of discharge (DCH) train operation during the LAES discharge are illustrated with the
[0032] The regasified liquid air escaping the device 32 as a high-pressure air is superheated in the recuperator 36 by LAES exhaust and partially expanded in the HP expander 37 down to a pressure required for supercharging the reciprocating engine 38 by combustion air. A gaseous fuel delivered into this engine via pipe 39 is converted here into useful power and a stream of exhaust gases 37 escaping the engine at the enhanced pressure and temperature. This temperature may be optionally increased through combustion of an additional fuel in the duct burner 40. The following expansion of exhaust gases in the low-pressure expander 42 down to atmospheric pressure is accompanied by reducing their outlet temperature, which however is sufficient to provide a said superheating of the high-pressure air in the recuperator 36. The finally cooled exhaust gases 43 are removed into atmosphere. The pioneering use of pressurized supplementary firing in the exhaust of DCH train leads to an increase in temperature of exhaust and air streams at the inlet of expanders 42 and 37 and to corresponding increase in their power outputs. These outputs add up to 50% of the LAES facility discharge output. Another one-half facility output provides the reciprocating gas engine 38. It should be equipped with intercooler 43 of combustion air, if duct burner 40 is installed.
[0033] The invented method may be also applied to operation of the LAGES facility in base-load mode as shown in the
[0034] During operation of the LAGES facility in base-load regime the low-pressure LNG is continuously (24 h/d) sent to the deep cooler 3 and a control valve 4 directs the entire deeply cooled LNG stream through a high-pressure pump 5 to CH train 6 for its regasification. In its turn, production of liquid air is performed also on 24 h/d basis and a control valve 15 instantly directs the produced liquid air through a high-pressure pump 17 to the DCH train. Here it is firstly used in the device 18 for reliquefaction of a part of NG delivered via pipe 11 from CH train outlet and then for generation of discharged power in power block 31. By this means the storages of deeply cooled LNG and liquid air are taken out of service in this regime of LAGES operation.
INDUSTRIAL APPLICABILITY
[0035] The developed method for the Liquid Air and Gas Energy Storage (LAGES) is an unique integration between the processes in Liquid Air Energy Storage (LAES) system and LNG Storage and Regasification (LNGSR) terminal. At a sacrifice of exchanging the waste energy flows between two facilities a need for any vaporizers, sea water and/or fuel commonly used to vaporize LNG at the terminal could be fully obviated simultaneously with a drastic reduction in losses during energy converting at the LAES facility. A recasted round-trip efficiency of such energy storage could exceed 180% with a capability for co-production of re-gasified NG and up to 75-95 MW of peaking power per each MTPA of terminal sent-out capacity. The world's first use of the reciprocating engine during discharging the LAES facility makes possible not only to halve an amount of liquid air required for on-peak production of a given power, but also to highly profitably and simply recover an exhaust thermal energy of such engine. In addition, a waste cold thermal energy of the discharged air may be used for re-liquefying a part of send-out NG at a rate of 16-33% of send-out terminal capacity. The reliquefied NG may be used for loading the trucks and ship bunkering or returned into storage tanks for a corresponding increase in total amount of electrical energy (in MWh) which may be produced at a given terminal send-out capacity.
[0036] The performances of LAGES facility using the proposed method of operation are tabulated below. The calculation of these performances has been performed for the case of a possible integration between the LNGSR terminal having 0.43 MTPA of capacity and the LAES system with installed 33 MW of peaking power output. At such LAGES facility the LNG regasification and production of liquid air in the charge (CH) train of the LAES system is performed continuously 24 h per day and on condition that relationship between the flow-rates of LNG (pure methane) and charging air streams is equal to 1.1:1. The discharge of LAES system is run on a daily basis during 12 on-peak hours, for which purpose the liquid air produced at that instant and during off-peak hours is used.
[0037] In so doing, the low pressure of LNG stream and the high pressure of resulting NG stream are set at the levels of 6 and 80 barA correspondingly, whereas a top cycle pressure of process air stream and a pressure of pumped discharged air stream are set at a level of 67 barA and 140 barA correspondingly. Amount of fuel combusted in the duct burner of the discharge (DCH) train of LAES system provides the admissible temperatures of gaseous streams at the inlet of turbomachinery used: 540 C. for discharged air at the inlet of the modified steam turbine being used as HP expander and 760 C. for exhaust gases at the inlet of power turbine being used as LP expander. Finally, a DCH train comprises a set of two reciprocating gas engines, being charged with combustion air from the CH train at a pressure of 4 barA. The DCH train of LAES system provides simple and effective harnessing the potential and thermal energy of their exhaust gases escaping the engines at a pressure of 3.5 barA and a temperature of 570 C.
[0038] A power required for operation of the CH train during off-peak hours is delivered from the grid, whereas during on-peak hours it is extracted from the gross DCH train output, resulting in corresponding decrease in net discharged power delivered into grid. Taking into account the chosen identical durations of the off-peak and on-peak hours, the grid round-trip efficiency (RTE) of the LAGES system may by determined from a simple division of its net discharge power by the charge one.
[0039] The gross discharge power produced by the HP and LP expanders and reciprocating engines is the sum of a power produced by the discharged air delivered from CH train to DCH one and an extra power, produced with help of fuel self-consumed by the engines and in the duct burner of the DCH train. If this fuel would be alternatively consumed by a much used simple cycle peaking gas turbine, a grid power equivalent of the consumed fuel could be equal to a fuel thermal equivalent multiplied by average fuel-to-power conversion efficiency at the peaking gas turbine plant. By this means net actual (recasted) discharge power of LAGES facility may be determined by subtraction of a grid power equivalent of fuel self-consumed at this facility from its net discharge power output. In its turn, a recasted RTE value for the developed LAGES facility is determined by division of its net recasted discharge power by charge one. The main data of the LAGES facility operated in the energy storage regime are presented below in the Table 1.
TABLE-US-00001 LNG PROCESSING DATA 1 Time-period of LNG delivery and deep cooling h/d 12 2 Mass flow-rate of LNG delivered kg/s 33 3 Low pressure of LNG delivered barA 6 4 Temperature of LP LNG delivered C. 158.8 5 Temperature of HP deeply cooled LNG C. 170.4 6 LNG service tank for 12 h storage (P = 1.5 bar, T = 173 C.) m{circumflex over ()}3 1,584 7 Time-period of LNG re-gasification in the LAES system h/d 24 8 Mass flow-rate of the whole of re-gasified LNG kg/s 16.5 9 Pressure of re-gasified LNG barA 79.5 10 Temperature of re-gasified LNG C. 15 11 Time-period of NG re-liquefaction in the LAES system h/d 12 12 Minimum mass flow-rate of re-liquefied NG kg/s 5.5 13 Maximum mass flow-rate of re-liquefied NG kg/s 11.0 14 Pressure of re-liquefied NG barA 1.4 15 Temperature of re-liquefied NG C. 159.1 16 Maximum NG send-out capacity MTPA 0.428 17 Minimum re-liquefying capacity MTPA 0.085 18 Minimum NG send-out capacity MTPA 0.342 19 Maximum re-liquefying capacity MTPA 0.171 LAES CHARGE (CH) PROCESS DATA 20 Time-period of LAES charge with grid power consumption h/d 12 21 Process air flow-rate kg/s 19.3 22 Liquid air (LAIR) production rate kg/s 15.1 23 Air pressure at feed air compressor outlet barA 8.4 24 Air temperature at the intercoolers outlet C. 10 25 Air pressure at process air compressor outlet barA 67.5 26 Air liquefaction ratio % 78.2 27 Charge (CH) power consumption MWE 9.2 28 LAIR tank for 12 h storage (P = 1.05 barA, T = 194.2 C.) m{circumflex over ()}3 746 29 LNG re-gasified-to-AIR liquefied ratio kg/kg 1.09 30 LAIR pressure at the outlet of HP pump barA 140.5 31 LAIR temperatures at outlet of HP pump/LNG deep cooler C. 189/161 LAES DISCHARGE (DCH) PROCESS DATA 32 Daily time-period of the LAES discharge h/d 12 33 LAIR consumption rate kg/s 30.2 34 Gross DCH power output with fuel consumption MWe 41.4 35 Net DCH power with fuel consumption MWe 32.2 36 Mass flow-rate of NG self-consumed kg/s 1.012 37 Annual amount of NG self-consumed MTPA 0.0157 38 NG self-consumption as share of net SOC % 3.7 39 Thermal input with fuel self-consumed MWth 49.2 40 DCH power w/o fuel consumption MWe 6.4 41 Fuel-to-extra power conversion efficiency % 71 SPECIFIC LAGES DATA 42 Specific CH energy input kWhit LAIR 169 43 Specific gross DCH energy output kWhit LAIR 381 44 Specific CH power relative to max SOC MWe/MTPA 21.5 45 Specific net DCH power relative to max SOC MWe/MTPA 75.2 46 Specific net DCH power relative to min SOC MWe/MTPA 94.2 GRID and RECASTED RTE OF ENERGY STORAGE 47 Grid RTE of the LAES facility % 350 48 Assumed average grid fuel-to-power conversion efficiency % 33 49 Grid power equivalent to fuel self-consumed MWe 16.2 50 Net recasted DCH power produced MWe 16.0 51 Recasted RTE of the LAES facility % 174
[0040] According to the invented method, the LAGES facility described above may be operated in base-load regime. For analysis of this option it is assumed that the LNGSR terminal described above is a part of a national gas transmission and distribution system, including also import of pipeline gas, underground NG storages and a number of the pressure reduction stations. At least three of these PR stations having a NG flow-rate of 75,000 NmA3/h each should be equipped with the NG expanders which are recovering the energy of expansion of NG from 80 down to 20 barA for production of electrical energy, transmitted through electrical grid to the LAGES facility. Here the delivered energy is used for driving the compressors of the CH train.
[0041] The LNG is continuously (24 h/d) delivered through deep cooler into this train and subjected to regasification through heat exchange with process air being liquefied. Two-thirds of regasified LNG is directed to NG main pipeline, whereas one-third is directed to DCH train for reliquefaction. The produced liquid air is instantly used together with fuel in the DCH train for production of discharged power. By this means, the LAGES operation in base-load regime obviates a need for usage of liquid air and deeply cooled LNG storages.
[0042] Below two alternatives of this technical solutions are considered. In the alternative A recovery of waste heat from the co-located industrial or power generation facilities for preheating the NG before its expansion is performed, making possible to produce a power by the expanders at the PR stations without any fuel consumption. In the alternative B preheating the NG at the PR stations is performed with use of a required fuel. The main data of the LAGES facility operated in the base-load regime are presented below in the Table 2. They testify that alternative A provides much higher fuel-to-power conversion efficiency of the LAGES facility.
TABLE-US-00002 Alt. A Alt. B LNG PROCESSING DATA 1 Time-period of LNG delivery and deep cooling, h/d 24 24 2 Mass flow-rate of LNG delivered, kg/s 16.5 16.5 3 Low pressure of LNG delivered, barA 6 6 4 Temperature of LP LNG delivered, C. 158.8 158.8 5 Temperature of HP deeply cooled LNG, C. 170.4 170.4 6 Time-period of LNG re-gasification in the LAES system, h/d 24 24 7 Mass flow-rate of the whole of re-gasified LNG, kg/s 16.5 16.5 8 Pressure of re-gasified LNG, barA 79.5 79.5 9 Temperature of re-gasified LNG, C. 15 15 10 Time-period of NG re-liquefaction in the LAES system, h/d 24 24 11 Mass flow-rate of re-liquefied NG, kg/s 5.5 5.5 12 Pressure of re-liquefied NG, barA 1.4 1.4 13 Temperature of re-liquefied NG, C. 159.1 159.1 14 NG send-out capacity, MTPA 0.342 0.342 15 Re-liquefying capacity, MTPA 0.171 0.171 LIQUID AIR PRODUCTION DATA 16 Time-period of LAIR production with power consumption, h/d 24 24 17 Process air flow-rate, kg/s 19.3 19.3 18 Liquid air (LAIR) production rate, kg/s 15.1 15.1 19 Air pressure at feed air compressor outlet, barA 8.4 8.4 20 Air temperature at the intercoolers outlet, C. 10 10 21 Air pressure at process air compressor outlet, barA 67.5 67.5 22 Air liquefaction ratio, % 78.2 78.2 23 Power consumption by CH train, MWe 9.2 9.2 24 LAIR temperature at the CH train outlet, C. 194.2 194.2 25 LNG re-gasified-to-AIR liquefied ratio, kg/kg 1.09 1.09 26 LAIR pressure at the outlet of HP pump, barA 140.5 140.5 27 LAIR temperatures at outlet of HP pump/deep cooler, C. 189/161 189/161 DATA OF EXPANDER SETS AT PR STATIONS 28 A number of expander sets, set 3 3 29 NG flow-rate through one expander, kg/s//Nm{circumflex over ()}3/h 16.5//75,000 16.5//75,000 30 NG pressure at expander inlet/outlet, barA 80//20 80//20 31 NG temperature before preheater, at expander inlet/outlet, C. 15/103/14 15/103/14 32 Mass flow-rate of NG self-consumed by one PR station, kg/s 0 0.081 33 A share of NG self-consumption, % 0 0.49 34 Thermal input with fuel at one PR station, MWth 0 3.93 35 Power output of one expander, MWe 3.07 3.07 LAES DISCHARGE (DCH) PROCESS DATA 36 Daily time-period of the LAES discharge, h/d 24 24 37 LAIR consumption rate, kg/s 15.1 15.1 38 DCH power output, MWe 20.7 20.7 39 Mass flow-rate of NG self-consumed in DCH train, kg/s 0.506 0.506 40 Thermal input with fuel self-consumed in DCH train, MWth 24.6 24.6 41 Annual NG self-consumption, MTPA 0.0157 0.0157 42 A share of LNG self-consumption, % 3.1 3.1 LAGES EFFICIENCY DATA 43 Total thermal input with fuel consumed, MWth 24.6 36.4 44 Total power output, MWe 20.7 20.7 45 LAGES fuel-to-power conversion efficiency, % 84.1 56.9
[0043] It should be noted that the term comprising does not exclude other elements or steps and a or an do not exclude a plurality. It should also be noted that reference signs in the claims should not apparent to one of skill in the art that many changes and modifications can be effected to the above embodiments while remaining within the spirit and scope of the present invention. For example, the invented method may be applied to design and operation of the near-shore Floating Storage and Regasification Units (FSRU) connected with the national electric and natural gas networks.