CROSS-REFERENCE TO RELATED APPLICATIONS
TECHNICAL FIELD
[0002] The present invention disclosed herein relates to a natural gas liquefaction apparatus,
and more particularly, to a natural gas liquefaction apparatus for liquefying natural
gas through a plurality of cycles using different refrigerants.
BACKGROUND ART
[0003] In general, natural gas is transported in a gas state through land or marine gas
piping, or is stored in an LNG transport ship in a state of liquefied natural gas
(LNG) and transported.
[0004] At this point, natural gas is obtained by being cooled to an ultra low temperature
and has a volume reduced to about 1/600 of that of gas-state natural gas, and is therefore
very suitable for long distance marine transportation.
[0005] In addition, conventionally used liquefaction methods for natural gas have been performed
by allowing the natural gas to pass through one or more heat exchangers so as to be
cooled.
[0007] However, the technology disclosed in the patent has a limitation in that it is difficult
to adjust process variables because cycles are each configured in series in its entirety,
and the limitation greatly decreases process efficiency.
[0008] Consequently, a method for solving the limitation is demanded.
DISCLOSURE OF THE INVENTION
TECHNICAL PROBLEM
[0009] The present invention is devised to solve the abovementioned limitation of conventional
art, and has the object of providing a natural gas liquefaction apparatus which facilitates
the adjustment of process variables and is capable of maximizing heat exchange efficiency.
[0010] The object of the present invention is not limited to the aforesaid, but other objects
not described herein will be clearly understood by those skilled in the art from descriptions
below.
TECHNICAL SOLUTION
[0011] To achieve the aforementioned object, a natural gas liquefaction apparatuses according
to the present invention includes: a cryogenic heat exchanger through which natural
gas passes through and is liquefied into LNG through heat exchange with a first refrigerant
and a second refrigerant; a first refrigerant cycle through which the first refrigerant
circulates, which has some paths passing through the cryogenic heat exchanger to perform
heat exchange, and which has a path of the first refrigerant divided into a plurality
of paths after performing heat exchange at the cryogenic heat exchanger and performs
expansion and pre-compression of the first refrigerant; and a second refrigerant cycle
through which the second refrigerant circulates and which has some paths passing though
the cryogenic heat exchanger.
[0012] The first refrigerant cycle may include: a first refrigerant first compression part
provided upstream of the cryogenic heat exchanger and configured to compress the first
refrigerant to a high pressure; a first refrigerant first turbo expander including
a first refrigerant first expansion part provided downstream of the cryogenic heat
exchanger and configured to expand the first flow among the two divided flows of the
first refrigerant having passed through the cryogenic heat exchanger, and a first
refrigerant first pre-compression part configured to pre-compress the first refrigerant
which has been expanded by the first refrigerant first expansion part and have passed
through the cryogenic heat exchanger again; and a first refrigerant second turbo expander
including a first refrigerant second expansion part provided downstream of the cryogenic
heat exchanger and configured to expand the second flow among the two divided flows
of the first refrigerant having passed through the cryogenic heat exchanger, and a
first refrigerant second pre-compression part configured to pre-compress the first
refrigerant which has been expanded by the first refrigerant second expansion part
and have passed through the cryogenic heat exchanger again.
[0013] In addition, the first refrigerant cycle may include: a first refrigerant first compression
part provided upstream of the cryogenic heat exchanger and configured to compress
the first refrigerant to a high pressure; a first refrigerant first turbo expander
including a first refrigerant first expansion part provided downstream of the cryogenic
heat exchanger and configured to expand the first flow among the three divided flows
of the first refrigerant having passed through the cryogenic heat exchanger, and a
first refrigerant first pre-compression part configured to pre-compress the first
refrigerant which has been expanded by the first refrigerant first expansion part
and has passed through the cryogenic heat exchanger again; a first refrigerant second
turbo expander including a first refrigerant second expansion part provided downstream
of the cryogenic heat exchanger and configured to expand the second flow among the
three divided flows of the first refrigerant having passed through the cryogenic heat
exchanger, and a first refrigerant second pre-compression part configured to pre-compress
the first refrigerant which has been expanded by the first refrigerant second expansion
part and has passed through the cryogenic heat exchanger again; and a first refrigerant
third turbo expander including a first refrigerant third expansion part provided downstream
of the cryogenic heat exchanger and configured to expand the third flow among the
three divided flows of the first refrigerant having passed through the cryogenic heat
exchanger, and a first refrigerant third pre-compression part configured to pre-compress
the first refrigerant which has been expanded by the first refrigerant third expansion
part and has passed through the cryogenic heat exchanger again.
[0014] In addition, the first refrigerant first compression part may be provided in plurality.
[0015] In addition, the second refrigerant cycle may include a second refrigerant compression
part provided upstream of the cryogenic heat exchanger and configured to compress
the second refrigerant to a high pressure; and a second refrigerant turbo expander
including a second refrigerant expansion part provided downstream of the cryogenic
heat exchanger and configured to expand the second refrigerant having passed through
the cryogenic heat exchanger, and a second refrigerant pre-compression part configured
to pre-compress the second refrigerant which has been expanded by the second refrigerant
expansion part and has passed through the cryogenic heat exchanger again.
ADVANTAGEOUS EFFECTS
[0016] The natural gas liquefaction apparatus of the present invention for solving the abovementioned
limitation has the following effects.
[0017] First, there is a merit in that a portion of the first refrigerant cycle divides
the flow of the first refrigerant so that expansion and pre-compression for each flow
of the first refrigerant may be separately performed, and thus process variables are
easily adjusted.
[0018] Secondly, there is a merit in that due to excellent heat exchange efficiency, the
yield can be increased and energy may be saved.
[0019] Thirdly, there is a merit in that the flow rate of the second refrigerant can be
reduced compared to that in conventional arts.
[0020] Effects to be obtained by the present invention are not limited to the aforesaid,
but other effects not described herein will be clearly understood by those skilled
in the art from descriptions below.
BRIEF DESCRIPTION OF THE DRAWINGS
[0021]
FIG. 1 is a view illustrating the configuration of a natural gas liquefaction apparatus
according to a first embodiment of the present invention.
FIG. 2 is a graph illustrating a composite curve of a conventional natural gas liquefaction
apparatus.
FIG. 3 is a view illustrating a composite curve of a natural gas liquefaction apparatus
according to the first embodiment of the present invention.
FIG. 4 is a view illustrating the configuration of a natural gas liquefaction apparatus
according to a second embodiment of the present invention.
MODE FOR CARRYING OUT THE INVENTION
[0022] Hereinafter, preferable embodiments of the present invention with which the purpose
of the present invention may specifically be achieved will be described with reference
to the accompanying drawings. In describing the embodiments, like names and reference
symbols are used for the same elements, and the additional description thereon will
not be provided.
[0023] FIG. 1 is a view illustrating the configuration of a natural gas liquefaction apparatus
according to a first embodiment of the present invention.
[0024] As illustrated in FIG.1, a natural gas liquefaction apparatus according to a first
embodiment of the present invention includes an ultra low temperature heat exchange
10, a first refrigerant cycle 100, and a second refrigerant cycle 200.
[0025] The cryogenic heat exchanger 10 allows natural gas passing therethrough to be liquefied
into LNG by the heat exchange with the first refrigerant circulating in first refrigerant
cycle 100 and the second refrigerant cycle 200 circulating in the second refrigerant
cycle 200.
[0026] At this point, in case of the present embodiment, methane serves as the first refrigerant
and nitrogen serves as the second refrigerant. However, embodiments are not limited
to the present embodiment, other refrigerants may of course be used as the first and
second refrigerants.
[0027] In addition, as described above, the first refrigerant circulates through the first
refrigerant cycle 100, some paths of which perform heat exchange via the cryogenic
heat exchanger 10.
[0028] At this point, after performing the heat exchange at the cryogenic heat exchanger
10, the path of the first refrigerant cycle 100 is divided into a plurality of paths
so that expansion and pre-compression of the first refrigerant may be performed. That
is, the first refrigerant cycle 100 has a parallel structure because the path of the
first refrigerant is divided after passing through the cryogenic heat exchanger 10.
[0029] In particular, in the present embodiment, the first refrigerant cycle 100 includes
a first refrigerant compression part 110, a first turbo expander 120, and a second
turbo expander 130.
[0030] The first refrigerant first compression part 110 is provided upstream of the cryogenic
heat exchanger 10 in the entire first refrigerant cycle 100, and compresses the first
refrigerant to a high pressure (for example, about 50-60 barg). In case of the present
embodiment, the first refrigerant first compression part 110 is provided as a plurality
of compression parts 111 and 112.
[0031] In addition, the first turbo expander 120 includes a first refrigerant first expansion
part 121 and a first refrigerant first pre-compression part 122.
[0032] The first refrigerant first expansion part 121 is provided downstream of the cryogenic
heat exchanger 10 in the entire first refrigerant cycle 100, and expands a first flow
which is a portion of the two divided flows of the first refrigerant after passing
through the cryogenic heat exchanger 10.
[0033] By means of the first expansion part 121, the first flow of the first refrigerant
may be expanded to, for example, about 10-12 barg. The expanded first flow of the
first refrigerant may be cooled to, for example, about -55°C to about -75°C. The expanded
and cooled first flow of the first refrigerant by the first refrigerant first expansion
part 121 circulates to the cryogenic heat exchanger 10 side to perform heat exchange.
[0034] The first flow of the first refrigerant flowing into the cryogenic heat exchanger
10 from the first refrigerant first expansion part 121 may be configured to pass through
a warm heat exchange region 16 (upstream region of inner region of the heat exchanger
10 with respect to the flow of natural gas) inside the cryogenic heat exchanger 10.
[0035] The first refrigerant first pre-compression part 122 is also provided downstream
of the cryogenic heat exchanger 10 in the entire first refrigerant cycle 100. The
first refrigerant first pre-compression part 122 and the first refrigerant first expansion
part 121 may operate linked with each other.
[0036] The first refrigerant first pre-compression part 122 pre-compresses, for example
to about 20-25 barg, the first flow of the first refrigerant, which have been expanded
by the first refrigerant first expansion part 121 and have passed through the cryogenic
heat exchanger 10 again, and then supplies the first flow to the first refrigerant
first compression part 110 described above.
[0037] In addition, the second turbo expander 130 includes a first refrigerant second expansion
part 131 and a first refrigerant second pre-compression part 132.
[0038] The first refrigerant second expansion part 131 is provided downstream of the cryogenic
heat exchanger 10 in the entire first refrigerant cycle 100, and expands a second
flow which is a portion of the two divided flows of the first refrigerant after passing
through the cryogenic heat exchanger 10.
[0039] The first refrigerant first expansion part 121 and the first refrigerant second expansion
part 131 are configured to sequentially receive the first flow and the second flow,
which flow into the cryogenic heat exchanger 10 via the same refrigerant line from
the first refrigerant first compression part 110 and which are heat-exchanged inside
the cryogenic heat exchanger 10.
[0040] By means of the second expansion part 131, the second flow of the first refrigerant
may be expanded to, for example, about 15-20 barg. The expanded second flow of the
first refrigerant may be cooled to, for example, about -90°C to about -115°C. The
second flow of the first refrigerant expanded and cooled by the first refrigerant
first expansion part 131 circulates to the cryogenic heat exchanger 10 side to perform
heat exchange.
[0041] The second flow of the first refrigerant flowing into the cryogenic heat exchanger
10 from the first refrigerant second expansion part 131 may be configured to sequentially
pass through an intermediate heat exchange region 14 (midstream region of the inner
region of the heat exchanger 10 with respect to the flow of natural gas) and a warm
heat exchange region 16 inside the cryogenic heat exchanger 10.
[0042] The first refrigerant second pre-compression part 132 is also provided downstream
of the cryogenic heat exchanger 10 in the entire first refrigerant cycle 100. The
first refrigerant second pre-compression part 132 and the first refrigerant second
expansion part 131 may operate linked with each other.
[0043] The first refrigerant second pre-compression part 132 pre-compresses, for example
to about 20-25 barg, the second flow of the first refrigerant, which have been expanded
by the first refrigerant second expansion part 131 and have passed through the cryogenic
heat exchanger 10 again, and then supplies the second flow to the first refrigerant
first compression part 110 described above.
[0044] The first flow of the first refrigerant pre-compressed by the first refrigerant first
pre-compression part 122 and the second flow of the first refrigerant second pre-compression
part 132 may be mixed in a mixing pipe and transferred to the first refrigerant first
compression part 110.
[0045] In the embodiment, the pressure of the first refrigerant discharged from the first
refrigerant first pre-compression part 122 and the pressure of the first refrigerant
discharged from the first refrigerant second pre-compression part 132 may be mixed
at the same pressure, and then the mixed flow is allowed to flow into the first refrigerant
first compression part 110. Thus, the compression efficiency of the first refrigerant
may be enhanced.
[0046] As described above, in the present embodiment, the first refrigerant compressed at
the first refrigerant first compression part 110 is divided into two flows and circulate
through mutually different paths, and thus, there is a merit in that not only process
variables may easily be adjusted, but also the heat exchange efficiency is very excellent.
[0047] In addition, in the present embodiment, the first turbo expander 120 and the second
turbo expander 130 cools the first refrigerant to mutually different temperatures,
and the flow rate is configured such that about 25-45% is divided to the side of relatively
high process temperature and about 55-75% is divided to the side of relatively low
temperature.
[0048] As such, the first refrigerant with divided flows are introduced into the cryogenic
heat exchanger 10 and a pre-cooling (from about -55 °C to -75°C, to about 30°C to
45°C) and a partial liquefaction (from about -90 °C to -115°C, to about 30°C to 45°C)
may be separated and efficiently performed.
[0049] For example, the first turbo expander 120 may adjust the temperature difference between
the first refrigerant and a fluid in a warm region corresponding to -65 °C to -30°C
with the first flow rate of the first refrigerant to adjust the process of the pre-cooling.
[0050] The second turbo expander 130 may adjust the temperature difference between the first
refrigerant and a fluid in an intermediate region corresponding to -110 °C to -65°C
with the second flow rate of the first refrigerant to adjust the process of the liquefaction
(partial liquefaction).
[0051] Meanwhile, as described above, the second refrigerant circulates through the second
refrigerant cycle 200, some paths of which perform heat exchange via the cryogenic
heat exchanger 10.
[0052] In the present embodiment, the second refrigeration cycle 200 includes a second refrigerant
compression part 210 and the second refrigerant turbo expander 220.
[0053] The second refrigerant compression part 210 is provided upstream of the cryogenic
heat exchanger 10 in the entire second refrigerant cycle 200, and compresses the second
refrigerant to a high pressure (for example, about 50-60 barg).
[0054] In addition, the second refrigerant turbo expander 220 includes a second refrigerant
expansion part 221 and a second refrigerant pre-compression part 222.
[0055] The second refrigerant expansion part 221 is provided downstream of the cryogenic
heat exchanger 10 in the entire second refrigerant cycle 200, is in charge of a remaining
liquefaction process (from about -165 °C to -150°C, to about 30°C to 45°C), and expands
the second refrigerant having passed through the cryogenic heat exchanger 10.
[0056] The second refrigerant may be expanded to about 12-18 barg by the second refrigerant
expansion part 221. The flow of the expanded second refrigerant may be cooled to about
-150 °C to -165°C. The flow of the second refrigerant expanded and cooled by the second
refrigerant expansion part 221 circulates to the cryogenic heat exchanger 10 side
to perform heat exchange. Here, the second refrigerant is in charge of a process of
a cold loop (from -165 °C to -150°C, to 30 °C to 45°C including an ultra cold section
(-165°C to -110°C) in which heat exchange may not be performed with the first refrigerant.
[0057] The flow of the second refrigerant flowing into the cryogenic heat exchanger 10 from
the second refrigerant expansion part 221 may be configured to sequentially pass through,
in the cryogenic heat exchanger 10, a cold heat exchange region 12 (downstream region
inside the heat exchanger 10 with respect to the flow of natural gas), an intermediate
heat exchange region 14 (midstream region of the inner region of the heat exchanger
10 with respect to the flow of natural gas) and a warm heat exchange region 16.
[0058] The second refrigerant pre-compression part 222 is also provided downstream of the
cryogenic heat exchanger 10 in the entire second refrigerant cycle 200, and pre-compresses
the second refrigerant, having passed through the cryogenic heat exchanger 10 again,
to about 15-20 barg, for example.
[0059] The entirety of the pre-cooling, liquefaction, and subcooling which are liquefaction
process of a fluid may be adjusted by the first turbo expander 120, the second turbo
expander 130 and the second refrigerant turbo expander 220.
[0060] As described above, the present invention has an additional merit in that the flow
rate of the second refrigerant of the second refrigerant cycle 200 may be reduced
compared to that in the conventional art through an efficient process of the first
refrigerant cycle 100.
[0061] FIG. 2 is a graph illustrating a composite curve of a related natural gas liquefaction
apparatus, and FIG. 3 is a view illustrating a composite curve of a natural gas liquefaction
apparatus according to the first embodiment of the present invention. Here, x-axes
of the graphs illustrated in FIGS. 2 and 3 indicate heat flow transferred in a heat
exchanger through the heat amount of each of the turbo expanders and the compression
parts, and y-axes indicates temperatures.
[0062] In addition, the hot composite of natural gas located on the upper side is depicted
in a solid line and the cold composite of the refrigerant located on the lower side
is depicted in a dotted line.
[0063] First, examining the composite curve illustrated in the graph of FIG. 2, it may be
confirmed that the temperature difference between the hot composite as natural gas
and the cold composite as the refrigerant is large in a range of about -40°C to about
-100ºC, and thus, it may be found that the area formed between the hot composite and
the cold composite is larger than that of the cold region.
[0064] This is because the first refrigerant cycle and the second refrigerant cycle are
entirely formed in series and has only one adjustable inflection point and thus there
is a limit in optimizing a system.
[0065] Conversely, examining the composite curve illustrated in the graph of FIG. 3, it
may be confirmed that the temperature difference between the hot composite as natural
gas and the cold composite as the refrigerant is large in a range of about -40°C to
about -100°C, and thus, the area formed between the hot composite and the cold composite
may be minimized.
[0066] This is because the first refrigerant cycle is formed, unlike that in the conventional
art, in series as a pre-cooling section (30 °C to about -65°C) and a partial liquefaction
(30°C to about -110°C), and a plurality of adjustable inflection points are present.
[0067] A natural gas liquefaction apparatus of the present invention has a first refrigerant
cycle composed of a warm loop and an intermediate loop, and a second refrigerant cycle
composed of a cold loop. In FIG. 1, the warm loop is illustrated in dotted lines,
the intermediate loop is illustrated in alternate long and short dash lines, and the
cold loop is illustrated in alternate long and two short dash lines.
[0068] Each loop is operated in various temperature ranges considering the composite curve.
For example, the intermediate loop through which the first refrigerant circulates
is cooled to about -90°C to -115°C and may be operated until reaching about 25°C to
45°C, the warm loop through which the first refrigerant circulates is cooled to about
-55°C to - 75°C and may be operated until reaching about 25°C to 45°C, and the cold
loop through which the first refrigerant circulates is cooled to about -150°C to -165°C
and may be operated until reaching about 25°C to 45°C.
[0069] Changes in the amounts or ratios of the first refrigerant and the second refrigerant
which circulate through respective loops may substantially affect the composite curve.
More specifically, a change in the second flow rate of the first refrigerant circulating
through the intermediate loop may substantially affect a liquefaction region between
about -115°C to -90°C. In addition, a change in the first flow rate circulating through
the warm loop may mainly have influence at about -90°C or higher.
[0070] As such, according to the natural gas liquefaction apparatus of the present invention,
by adjusting the first and second flow rates of the first refrigerant and the flow
rate of the second refrigerant, and adjusting the temperatures of the respective loops,
the difference between the composite curves of the fluid (natural gas) and the refrigerants
may effectively be reduced in the temperature sections mainly dealt with the respective
loops.
[0071] In addition, the efficiency of a liquefaction process of a fluid may be improved
by reducing the energy consumed for liquefying the fluid by enhancing the compression
efficiency of the refrigerant and effectively cooling the fluid with a simple process.
[0072] The log mean temperature differences (LMTDs) illustrated in FIGS. 2 and 3 are log
mean temperature differences between the hot composite of natural gas and the cold
composite of the refrigerant. The LMTD, with which the entire heat exchange process
inside a heat exchange is analyzed by a mean temperature, is a value representing
the temperature difference between the natural gas and the refrigerant. When ΔT1 is
the difference between the inlet side temperature of natural gas and the outlet side
temperature of a refrigerant in a heat exchanger, and ΔT2 is the difference between
the outlet side temperature of the natural gas and the inlet side temperature of the
refrigerant in a heat exchanger, the LMTD may be calculated as the value of [(ΔT1-ΔT2)/{(lnΔT1)-(lnΔT2)}].
[0073] Referring to FIGS. 2 and 3, when comparing the LMTDs of the composite curves of actual
two processes, it may be found that the difference between the hot composite of the
natural gas and the cold composite of the refrigerant is about 4.309°C and is smaller
in the present embodiment than about 4.685°C in a conventional device, and this means
that the cooling efficiency becomes better.
[0074] In addition, in the present embodiment, unlike in conventional arts, since a cooling
process of at least -110°C is efficiently performed in the first refrigerant cycle,
the flow rate of the second refrigerant required in the second refrigerant cycle is
reduced, and thus, unlike the conventional arts, there is a merit in that sufficient
pressurization may be performed only with a single second refrigerant compression
part and the number of apparatuses may also be reduced.
[0075] In FIGS. 2 and 3, the portions depicted by shadow represent a portion of the pre-cooling
process of natural gas and liquefaction/partial liquefaction process. Comparing with
FIG. 2, according to the embodiment of the present invention, it may be confirmed
that the difference between the composite curve of the natural gas and the composite
curve of the refrigerant in the pre-cooling process is reduced in the liquefaction/partial
liquefaction processes (portions depicted by shadow in FIG. 3).
[0076] This is because the first refrigerant cycle is formed in parallel as the pre-cooling
section (about 30°C to -65°C) and the partial liquefaction section (about 30°C to
- 110°C), so that the pre-cooling section (about 30°C to -65°C) may be adjusted by
the first flow rate of the first refrigerant, and the partial liquefaction section
(about 30°C to -110°C) may be adjusted by the second flow rate of the first refrigerant,
and a plurality of adjustable inflection points are present in the pre-cooling section
(about 30°C to -65°C) and the partial liquefaction section (about 30°C to -110°C),
and the pre-cooling and partial liquefaction processes may be separated and efficiently
performed.
[0077] That is, according to the embodiment of the present invention, the heat exchange
(subcooling process) between the natural gas and the refrigerant in the ultra cold
section (about -165°C to -110°C) may be adjusted by the second refrigerant cycle in
which the second refrigerant circulates through the cold loop, the heat exchange (liquefaction/partial
liquefaction process) between the natural gas and the refrigerant in the intermediate
section (about -110°C to -65°C) may be adjusted by the first refrigerant cycle in
which the second flow of the first refrigerant circulates through the intermediate
loop, and the heat exchange (pre-cooling process) between the natural gas and the
refrigerant in the warm section (about -65°C to -30°C) may be adjusted by the first
refrigerant cycle in which the first flow of the first refrigerant circulates through
the warm loop
[0078] Thus, according to the embodiment of the present invention, the first flow rate of
the first refrigerant circulating through the warm loop, the second flow rate of the
first refrigerant circulating through the intermediate loop, and the flow rate of
the second refrigerant circulating through the cold loop are each adjusted, so that
the temperature differences between the fluid and the refrigerants for each loop is
adjusted, and the distance between the composite curves of the fluid (natural gas)
and the refrigerants may effectively reduced in the temperature section mainly dealt
with by each loop.
[0079] In addition, the pressure of the first refrigerant discharged from the first refrigerant
first pre-compression part 122 and the pressure of the first refrigerant discharged
from the first refrigerant second pre-compression part 132 may be mixed at the same
pressure, and then the mixed flow is allowed to flow into the first refrigerant first
compression part 110. Thus, the compression efficiency of the refrigerant may be enhanced.
That is, according to the embodiment of the present invention, the efficiency of a
liquefaction process of a fluid may be improved by reducing the energy consumed for
liquefying the fluid by enhancing the compression efficiency of the refrigerant and
effectively cooling the fluid with a simple process.
[0080] In Table 1 provided below, the yields and energy efficiencies of the natural gas
liquefaction apparatuses according to a conventional art and the present embodiment
are compared.
[Table 1]
|
Conventional art |
Present embodiment |
Compressor Duty [MW] |
40.0 |
40.0 |
LNG Production [MTPA] |
1.005 |
1.183 |
Efficiency [kW/(ton/day)] |
14.42 |
12.23 |
[0081] Examining Table 1 above, the production was performed on the basis of available capacity
of about 40.0 MW, and it may be confirmed that the present embodiment may increase
the yield as much as about 17.8% from about 1.005 MTPA to 1.183 MTPA in the conventional
art.
[0082] In addition, it may be confirmed that energy is reduced to about 12.23 kW from about
14.42 kW of energy consumed for LNG production of about 1 ton/day, and thus about
17.8 % of energy may be saved.
[0083] FIG. 4 is a view illustrating the configuration of a natural gas liquefaction apparatus
according to a second embodiment of the present invention.
[0084] In the second embodiment of the present invention illustrated in FIG. 4, the entirety
of components is configured in the same manner as the first embodiment. However, the
present embodiment is different from the abovementioned first embodiment in that the
flow of a first refrigerant having passed through a cryogenic heat exchanger 10 is
divided into three flows in the first refrigerant cycle 100.
[0085] Accordingly, in the present embodiment, a first flow among the three divided flows
of the first refrigerant is supplied to a first refrigerant first turbo expander 120
side, and the second flow among the three divided flows of the first refrigerant is
supplied to a first refrigerant second turbo expander 130 side.
[0086] In addition, in the present embodiment, a first refrigerant third turbo expander
140 is further provided, and a third flow among the three divided flows of the first
refrigerant is supplied to the first refrigerant third turbo expander 140 side.
[0087] In addition, the first refrigerant third turbo expander 140 may include: a first
refrigerant third expansion part 141 which expands the third flow among the three
divided flows of the first refrigerant; and a first refrigerant third pre-compression
part 142 which pre-compresses the first refrigerant which has been expanded by the
first refrigerant third expansion part 141 and has passed through again the cryogenic
heat exchanger 10.
[0088] As such, it may be found that in the present invention, the flow of the first refrigerant
may be divided into a plurality of paths more than two divided paths.
[0089] So far, preferable embodiments of the present invention have been described, and
it would be obvious to those skilled in the art that the present invention may be
implemented in other specific s\forms without departing from the spirit and scope
of the invention aside from the abovementioned embodiments. Therefore, embodiments
described above should not be construed as limitative but illustrative, and thus,
the present invention is not limited to the above description, and may also be modified
within the scope of claims and equivalent scope thereto.