Liquefaction apparatus

Information

  • Patent Grant
  • 6250244
  • Patent Number
    6,250,244
  • Date Filed
    Wednesday, August 23, 2000
    24 years ago
  • Date Issued
    Tuesday, June 26, 2001
    23 years ago
Abstract
A support structure that is either floatable or otherwise adapted to be disposed in an offshore location at least partially above sea level. A natural gas liquefaction system is located on or in the support structure and has a series of heat exchangers for cooling the natural gas in a countercurrent heat exchange relationship with a refrigerant. One or more compressors compress the refrigerant which is divided into two separate streams. Each stream is fed to a liquid expansion turbine where it is isentropically expanded. The expanded streams of refrigerant are then fed to the cool end of one of the heat exchangers.
Description




BACKGROUND OF THE INVENTION




1. Field of the Invention




This invention relates to a liquefaction apparatus, and more particularly relates to an offshore apparatus for liquefying natural gas.




2. Description of the Related Art




Natural gas is obtained from gas, gas/condensate and oil fields occurring in nature, and generally comprises a mixture of compounds, the most predominant of which is methane. Usually, natural gas contains at least 95% methane and other low boiling hydrocarbon (although it may contain less); the remainder of the composition comprises mainly nitrogen and carbon dioxide. The precise composition varies widely, and may include a variety of other impurities including hydrogen sulphide and mercury.




Natural gas may be “lean” gas or “rich” gas. These terms do not have a precise meaning, but it is generally understood in the art that a lean gas will tend to have less higher hydrocarbons than a rich gas. Thus, a lean gas may contain little or no propane, butane or pentane, whereas a rich gas would contain at least one of these materials.




Since natural gas is a mixture of gases, it liquifies over a range of temperatures; when liquefied, natural gas is called “LNG” (liquefied natural gas). Typically, natural gas compositions will liquefy, at atmospheric pressure, in the temperature range −165° C. to −155° C. The critical temperature of natural gas is about −90° C. to −80° C., which means that in practice it cannot be liquefied purely by the application of pressure it must be also be cooled below the critical temperature.




Natural gas is often liquefied before being transported to its point of end use. Liquefaction enables the volume of natural gas to be reduced by a factor of about 600. The capital costs, and running costs, of the apparatus required to liquefy the natural gas is very high, but not as high as the cost of transporting unliquefied natural gas.




The liquefaction of natural gas can be carried out by cooling the gas in countercurrent heat exchange relationship with a gaseous refrigerant, rather than with the liquid refrigerants used in conventional liquefaction methods, such as the cascade or propane-precooled mixed refrigerant processes. At least part of the refrigerant is passed through a refrigeration cycle which involves at least one compression step and at least one expansion step. Before the compression step, the refrigerant is usually at ambient temperature (ie the temperature of the surrounding atmosphere). During the compression step, the refrigerant is compressed to a high pressure, and is warmed by the compression process. The compressed refrigerant is then cooled with the ambient air, or with water if there is a water supply available, to return the refrigerant back to ambient temperature. The refrigerant is then expanded in order to cool it further. There are basically two methods of achieving the expansion. One method involves a throttling process, which may take place through a J-T valve (Joule-Thomson valve), wherein the refrigerant is expanded substantially isenthalpically. The other method involves a substantially isentropic expansion, which may take place through a nozzle, or, more usually, through an expander or turbine. The substantially isentropic expansion of the refrigerant is known in the art as “work expansion”. When the refrigerant is expanded through a turbine, work may be recovered from the turbine: this work can be used to contribute to the energy required to compress the refrigerant.




It is generally recognised that work expansion is more efficient than throttling (a greater temperature drop can be achieved for the same pressure reduction), but the equipment is more expensive. As a result most processes usually use only work expansion, or a mixture of work expansion and throttling.




When natural gas of a particular composition is cooled at a constant pressure, then for any given temperature of the gas there will be a particular value for the rate of change of enthalpy (Q) of the gas. The temperature (T) can be plotted against Q to produce a “cooling curve” for natural gas. The cooling curve is highly dependent upon pressure: if the pressure is below the critical pressure, then the T/Q cooling curve is highly irregular, ie, it contains several portions of different gradient, including a portion of zero, or close to zero, gradient. With increases in pressure, particularly above the critical pressure, the T/Q cooling curve tends towards a straight line.




Reference is now made to

FIG. 1

, which is a graph of temperature vs. rate of change of enthalpy for the cooling of natural gas below and above critical pressure. The curve A, which is for the cooling of natural gas below critical pressure, will be considered in more detail. The curve A has a characteristic shape, which can be divided into a number of regions. Region


1


has a constant gradient and represents the sensible cooling of the gas. Region


2


has a decreasing gradient and is below the dew point temperature of the gas as heavier components begin to condense. Region


3


corresponds to the bulk liquefaction of the gas and has the lowest gradient in the curve: the curve in this portion is almost horizontal. Region


4


has an increasing gradient and is above the bubble point temperature of the liquid as the lightest components are condensed. Region


5


is below the bubble point temperature and is of a constant gradient, which is greater than the gradient of regions


3


and


4


. Region


5


corresponds to the sensible cooling of the liquid; this is known as the “sub-cooling” region.




Reference is now made to

FIG. 2

of the drawings, which is a graph of T/Q showing the combined cooling curve for natural gas and nitrogen, for a natural gas pressure of about 5.5 MPa. The graph also shows the warming curve for nitrogen over the same temperature range. This graph is representative of a liquefaction system in which natural gas is cooled in a series of heat exchangers by a simple nitrogen expander cycle. The nitrogen refrigerant exiting the series of heat exchangers is compressed, cooled with ambient air, cooled to about −152° C. by work expansion, then fed to the cold end of the series of heat exchangers. The nitrogen refrigerant is precooled, before work expansion, by being passed through at least one heat exchanger at the warm end of the series of heat exchangers; thus, the cooling curve is a combined natural gas/nitrogen cooling curve.




The gradient of the cooling and warming curves at any particular point in

FIG. 2

is dT/dQ. It is well known in the liquefaction field that the most efficient process is one which, for any given value of Q, the corresponding temperature on the cooling curve of the natural gas is as close as possible to the corresponding temperature on the warming curve of the refrigerant. This has the implication that dT/dQ for the cooling curve of the natural gas is as close as possible to dT/dQ for the warming curve of the refrigerant. However, for any given Q, the closer the temperature of the natural gas and the refrigerant, the higher the surface area needed for the heat exchanger. Thus, there has to be a certain trade off between minimising the temperature difference, and minimising the heat exchanger surface area. For this reason, it is generally preferred that for any given Q, the temperature of the natural gas is at least 2° C. higher than that of the refrigerant.




In

FIG. 2

, the nitrogen warming curve is approximately a single straight line (ie, it has constant gradient). This is representative of a single stage refrigeration cycle, wherein the all the refrigerant nitrogen is cooled by work expansion to a low temperature of about −160° C. to −140° C., and is then passed in countercurrent heat exchange relationship with the natural gas. It is clear that at most parts of the T/Q curve there is a large temperature difference between the natural gas and the nitrogen refrigerant, and this indicates that the heat exchange is highly inefficient.




It is also known that the gradient of the warming curve of the refrigerant can be altered by changing the flow rate of the refrigerant through the heat exchangers: specifically, the gradient can be increased by decreasing the refrigerant flow rate. In the system shown in

FIG. 2

it is not possible to decrease the nitrogen flow rate, because the increase in gradient will cause the nitrogen warming curve to intersect with the natural gas cooling curve. An intersection of the two curves is indicative of a temperature “pinch” or “cross-over” in the heat exchanger between the nitrogen and the natural gas, and under this condition it is impossible for the process to work.




However, if the nitrogen flow is split into two streams it is possible to make the nitrogen warming curve change from a single straight line into two intersecting straight line portions of different gradient. An example of such a process is disclosed in U.S. Pat. No. 3,677,019. This specification discloses a process in which the compressed refrigerant is split into at least two portions, and each portion is cooled by work expansion. Each work expanded portion is fed to a separate heat exchanger for cooling the gas to be liquefied. This causes the refrigerant warming curve to comprise at least two straight line portions of different gradient. This aids in the matching of the warming and cooling curves and improves the efficiency of the process. This specification was published over twenty years ago, and the process disclosed therein is inefficient by modern standards.




In U.S. Pat. No. 4,638,639 there is disclosed a process for liquefying a permanent gas stream, which also involves splitting the refrigerant stream into at least two portions in order to match the cooling curve of the gas to be liquefied with the warming curve of the refrigerant. The outlet of all the expanders in this process is at a pressure above about 1 MPa. The specification suggests that such high pressures increase the specific heat of the refrigerant, thereby improving the efficiency of the refrigerant cycle. In order to realise an efficiency improvement it is necessary for the refrigerant to be at, or near, its saturation point at the outlet of one of the expanders, because the specific heat is higher near to saturation. If the refrigerant is at the saturation point, then under these conditions there will be some liquid in the refrigerant that is fed to the heat exchangers. This leads to additional expense, because either the heat exchanger needs to be modified in order to handle a two-phase refrigerant, or the refrigerant needs to be separated into liquid and gaseous phases before being fed to the heat exchanger.




U.S. Pat. No. 4,638,639 is primarily concerned with processes in which the refrigerant comprises a portion of the gas to be liquefied, ie the refrigerant is the same as the gas to be liquefied. The specification is particularly concerned with a system in which nitrogen is liquefied using a nitrogen refrigerant. The specification does not specifically disclose a process in which natural gas is cooled by nitrogen, nor would it be expected to be useful in such a process, because all modern large-scale processes for liquefying natural gas use a mixed refrigerant cooling cycle. Furthermore, in U.S. Pat. No. 4,638,639 the gas being liquefied is cooled to a temperature just below its critical temperature. A series of three J-T valves are provided to sub-cool the gas being liquefied.




The earliest refrigerant cycle used for the liquefaction of natural gas was the cascade process. Natural gas can be cooled in the cascade process by successive cooling with, for example, propane, ethylene and methane refrigerants. The mixed refrigerant cycle, which was developed later, involves the circulation of a multi component refrigerant stream, usually after precooling to −30° C. with propane. The nature of the mixed refrigerant cycle is such that the heat exchangers in the process must routinely handle the flow of a two phase refrigerant. This requires the use of large, specialised heat exchangers. The mixed refrigerant cycle is the most thermodynamically efficient of the previously known natural gas liquefaction processes: it enables the warming curve of the refrigerant to be closely matched to the cooling curve of the natural gas over a wide temperature range. Examples of mixed refrigerant processes are disclosed in U.S. Pat. Nos. 3,763,658 and 4,586,942, and in European Paten No 87,086.




One of the reasons for the widespread use of the mixed refrigerant cycle in the cooling of natural gas is the efficiency of that process. The installation of a typical mixed refrigerant liquefaction plant for natural gas would cost upward of $US 1,000,000,000, but the high cost can be justified by the efficiency gains. In order to be cost effective through economy of scale the mixed refrigerant plants typically need to be able to produce at least 3 million tonnes of LNG per annum.




The size and complexity of mixed refrigerants liquefaction plants is such that, to date, they have all been constructed, and located, on land. Due to the size of natural gas liquefaction plants, and the requirement for deep water harbours, they cannot always be located near to the natural gas fields. Gas from the natural gas fields is usually transported to the liquefaction plant by pipeline. In the case of offshore natural gas fields, there are severe practical limitations on the maximum length of the pipeline. This means that offshore natural gas fields that are more than about 200 miles from land are seldom developed.




BRIEF SUMMARY OF THE INVENTION




According to one aspect of the present invention there is provided an offshore apparatus for liquefying natural gas, comprising a support structure which is either floatable or is otherwise adapted to be disposed in an offshore location at least partially above sea level, and natural gas liquefaction means disposed on or in the support structure, the natural gas liquefaction means comprising a series of heat exchangers for cooling the natural gas in countercurrent heat exchange relationship with a refrigerant, compression means for compressing the refrigerant, and expansion means for isentropically expanding at least two separate streams of the compressed refrigerant, wherein said expanded streams of refrigerant communicate with a cool end of a respective one of the heat exchangers.




The support structure may be a fixed structure, ie a structure that is fixed to the seabed, and is supported by the seabed. Preferred forms of fixed structure include a steel jacket support structure and a gravity base support structure.




Alternatively, the support structure may be a floating structure, ie a structure that floats above the seabed. In this embodiment, the support structure is preferable a flatable vessel having a steel or concrete hull, such as a ship or a barge.




In one preferred embodiment, the support structure is a floating production storage and off-loading unit (FPSO).




Pretreatment means is usually provided for pretreating the natural gas before it is delivered to the liquefaction means. The pretreatment means may include separation stages for removing impurities, such as condensate, carbon dioxide and produced water.




The natural gas liquefaction apparatus may be provided in combination with storage means for receiving and storing the natural gas after it has been liquefied. The storage means may be provided on or in the support structure. Alternatively, the storage means may be provided on a separate support structure, which is either floatable or otherwise adapted to be disposed in an offshore location at least partially above sea level; the separate support structure may be of the same type as, or of a different type to, the support structure for the liquefaction means. It is particularly preferred that the support structure is a ship, and that the liquefaction means and the storage means are provided on said ship.




In a preferred embodiment, the support structure comprises two spaced gravity bases, and a platform bridging said gravity bases, wherein said storage means comprises a storage tank provided on or in at least one of said gravity bases, and wherein the liquefaction means is provided on or in said bridging platform.




Means can be provided for connecting said apparatus to a subsea well, whereby the natural gas can be delivered to the liquefaction means at a pressure above 5.5 MPa, said pressure being derived directly or indirectly from the pressure in the subsea well. To facilitate this, the apparatus according to the invention can be located sufficiently close to the natural gas producing formation that the pressure of the natural gas in the series of heat exchangers can be provided substantially entirely by the pressure inherent in the natural gas producing formation. In certain gas fields, some of the gas may be recompressed for re-injection, and therefore may be available at a high pressure if passed through one or more compression stages of the re-injection apparatus before being passed to the liquefaction means.




According to another aspect of the invention there is provided natural gas liquefaction apparatus, for offshore installation, comprising: natural gas liquefaction means having (i) a series of heat exchangers for cooling the natural gas in countercurrent heat exchange relationship with a refrigerant, (ii) compression means for compressing the refrigerant, and (iii) expansion means for isentropically expanding at least two separate streams of the compressed refrigerant, wherein said expanded streams of refrigerant communicate with a cool end of a respective one of the heat exchangers; and a support frame carrying the components of the liquefaction means as a single unit for transportation to, and installation at, the offshore location.




Preferably, the liquefaction means further comprises cooling means for cooling the refrigerant after it has been compressed and before it is isentropically expanded, said cooling means comprising a heat exchanger, a liquid coolant and a refrigeration unit for cooling the coolant to a temperature between −10° C. and 20° C., wherein the compressed refrigerant is cooled in said heat exchanger in countercurrent relationship with said coolant.




The expansion means may comprise a work expander disposed in each of said compressed refrigerant streams, and the compression means may comprise at least one compressor.




The compression means preferably comprises a first compressor adapted to compress the refrigerant to an intermediate pressure, and a second compressor adapted to compress the refrigerant to a higher pressure. The second compressor is desirably operatively connected to the refrigerant expander means, whereby substantially all the work required to compress the refrigerant from the intermediate pressure to the higher pressure is provided by the expansion means. In one construction the expansion means comprises two turbo expanders, and the second compressor comprises two compressors each operatively connected to a respective one of the turbo expanders. In another construction the refrigerant expander means comprises two turbo expanders, and the second compressor comprises a single compressor operatively connected to both the turbo expanders by means of a common shaft. An aftercooler is generally provided for cooling the compressed refrigerant from the second compression means.




The first compressor may comprise a single compressor with an aftercooler for cooling the compressed refrigerant, but it is preferred that the first compressor comprises a series of at least two compressors with an intercooler between each compressor of the series, and an aftercooler after the last compressor of the series.




The series of heat exchangers preferably comprises an initial heat exchanger, an intermediate heat exchanger and a final heat exchanger, and the natural gas is passed sequentially through the initial, the intermediate and the final heat exchangers in order to cool it to successively cooler temperatures; refrigerant in a first of said refrigerant streams is delivered to the final heat exchanger, and refrigerant in a second of said refrigerant streams is delivered to the intermediate heat exchanger.




The refrigerant may be cooled in the initial heat exchanger after being compressed, but before being isentropically expanded, and the refrigerant in said first refrigerant stream may be cooled in the intermediate heat exchanger after being cooled in the initial heat exchanger, but before being isentropically expanded.




The apparatus is preferably operated such that the final heat exchanger receives refrigerant from the first refrigerant stream, and the relative flowrates of the first and second refrigerant streams are such that the warming curve for the refrigerant comprises a plurality of segments of different gradient, the refrigerant is warmed in said final heat exchanger to a temperature below −80° C., and the coolest refrigerant temperature and the flowrate of refrigerant in said first refrigerant stream are such that a part of the refrigerant warming curve relating to the final heat exchanger is at all times within 1 to 10° C., preferably 1 to 5° C., of the corresponding part of the cooling curve for the natural gas.




It will usually be most efficient to operate the heat exchangers such that the temperature difference between the natural gas cooling curve and the corresponding part of the refrigerant warming curve is between 1° C. and 5° C. Typically this temperature difference will be above 2° C., because smaller temperature differences require larger, more expensive, heat exchangers, and there is a greater risk that a temperature pinch will be inadvertently created in the heat exchanger. However, in circumstances where there is a surplus of energy available, it can be sensible to operate with temperature differences above 5° C., and perhaps as high as 10° C.: this enables the size of the heat exchangers to be reduced, thereby saving capital costs.




The apparatus is preferably operated such that the coolest refrigerant temperature is no greater than −130° C., whereby the natural gas is sub-cooled substantially in said series of heat exchangers. Most preferably, the coolest refrigerant temperature is in the range −140° C. to −160° C.




The liquefaction means may further comprise a gas turbine for generating power for the compression means. The gas turbine preferably comprises an aero-derivative gas turbine; this is advantageous because it has a smaller size and weight than the alternative industrial type gas turbines commonly used in onshore LNG plants. In addition, the aero-derivative turbine has high thermal efficiency, and it is easy to maintain due to its light weight components. The number and rating of the turbines depends upon the amount of LNG that it is desired to produce; for example, to produce about 2 million tonnes LNG/annum would require two aero-derivative turbines each rated at about 40 MW.




It is preferred that the liquefaction means further comprises a second series (or “train”) of heat exchangers, said second series of heat exchangers being arranged in parallel with said first series of heat exchangers, and a separate refrigerant compression means and refrigerant expansion means for each series of heat exchangers. At least some of the or each series of heat exchangers and pipework connected thereto are preferably disposed within a single, common heat insulating housing—this is known as a “cold box”, and it usually contains pearlite or rock wool. When there is more than one heat exchanger train, it is preferred that each heat exchanger train is disposed in its own cold box.




The liquefaction means may further comprise natural gas expansion means adapted to receive and expand sub-cooled natural gas from the series of the heat exchangers; the expansion means serves to expand the sub-cooled natural gas to a sub-critical pressure, thereby simultaneously cooling and liquefying the natural gas. The expansion means may be substantially isenthalpic expansion means, such as a J-T valve, or substantially isentropic expansion means, such as a liquid or hydraulic turbine expander. When the expansion means comprises a liquid or hydraulic turbine expander, or other work-producing expansion means, it is preferred that an electrical generator is provided. The generator is arranged to convert the work produced by the expansion means into electrical energy.




The liquefaction means may further comprise a flash vessel adapted to receive expanded natural gas from the natural gas expansion means. In practice the expanded natural gas comprises a two phase mixture of liquid and gas. The flash vessel is provided with a fuel gas exit, through which natural gas comprising mainly methane and a lesser amount of nitrogen is taken, and a LNG exit through which LNG is taken. It is preferable that the flash vessel is provided in the form of a fractionating column having a reboiler which comprises a heat exchanger arranged to warm a liquid stream, taken from the column, in countercurrent heat exchange relationship with natural gas exiting said series of heat exchangers. A fuel gas compressor means can be provided to compress the fuel gas to a suitable pressure for use in a gas turbine, after the gas is warmed in a heat exchanger. The flash vessel is preferably disposed within the cold box. It is desirable that the gas turbine is powered by fuel gas derived from the fuel gas exit of the flash vessel: by means of this arrangement, all the work required to compress the refrigerant is provided to the first compressor means, and this work is entirely provided by fuel gas created by the liquefaction process.




There are a number of suitable embodiments for the heat exchangers in the series. Aluminum plate-fin heat exchangers can only be manufactured up to a certain size and a number of individual cores must be manifolded together in parallel to handle the flowrates involved in the process and apparatus of the present invention. The single phase nature of the refrigerant makes it possible for these cores to be manifolded together relatively easily, without the difficulties encountered with two phase systems. However, aluminium plate-fin heat exchangers are constrained by the fact that the allowable design pressure decreases with increasing core size: in order to maintain the number of cores to a practical limit, the natural gas pressure should be below about 5.5 MPa. If higher pressures are desired, then it is preferred to use a spiral wound heat exchanger, a PCHE (printed circuit heat exchanger) or spool wound heat exchanger. Each heat exchanger in the series may comprise a plurality of heat exchanger cores in parallel. Each heat exchanger in the series may comprise more than one heat exchanger. In the preferred arrangement, the heat exchangers in the series are integrated into a single unit with appropriate inlet and outlet conduits.




It is possible for the natural gas to be cooled by the refrigerant in further intermediate heat exchangers arranged upstream of the final heat exchanger. However, it is preferred to use only one intermediate heat exchanger, because this reduces the complexity of the equipment, and makes it possible to achieve lower pressure drops across the heat exchanger train.




Whilst it is preferred that the refrigerant is divided into two streams, because this is the arrangement uses the least space, it is possible to divide the refrigerant into three, four or more streams. Each stream may be isentropically expanded in parallel with the other streams. It is also possible for one or more of the isentropic expansion steps to be carried out in stages using a series of isentropic expanders.




It is preferred that the refrigerant comprises at least 50 mol % nitrogen, more preferably at least 80 mol % nitrogen, and most preferably substantially 100 mol % nitrogen. Nitrogen has a substantially linear warming curve over the temperature range −160° C. to 20° C. In one preferred embodiment the refrigerant comprises nitrogen and up to 10 vol %, preferably 5-10 vol %, methane.




The refrigerant is ideally provided in a closed loop refrigerant cycle. The refrigerant could be, but need not be, taken from the stream of natural gas to be liquefied. Make-up refrigerant can be provided from a refrigerant source external to the refrigerant cycle.




The apparatus according to the invention is preferably operated in accordance with a process described in our copending PCT application of even date entitled “Liquefaction Process”. According to this process there is provided a natural gas liquefaction process comprising passing natural gas through a series of heat exchangers in countercurrent relationship with a gaseous refrigerant circulated through a work expansion cycle, said work expansion cycle comprising compressing the refrigerant, dividing and cooling the refrigerant to produce at least first and second cooled refrigerant streams, substantially isentropically expanding the first refrigerant stream to a coolest refrigerant temperature, substantially isentropically expanding the second refrigerant stream to an intermediate refrigerant temperature warmer than said coolest refrigerant temperature, and delivering the refrigerant in the first and second refrigerant streams to a respective heat exchanger for cooling the natural gas through corresponding temperature ranges, wherein the refrigerant in the first stream is isentropically expanded to a pressure at least 10 times greater than, and usually more than 10 times greater than, the total pressure drop of the first refrigerant stream across said series of heat exchangers, said pressure being in the range 1.2 to 2.5 MPa.




Preferably, the refrigerant is compressed to a pressure in the range 5.5 to 10 MPa. It is preferred that the first stream is isentropically expanded to a pressure in the range 1.5 to 2.5 MPa. The refrigerant in the first stream is preferably isentropically expanded to a pressure at least 20 times greater than the total pressure drop of the first refrigerant stream across said series of heat exchangers. It is possible to operate the process such that the first stream is isentropically expanded to a pressure at least 100 times greater than the total pressure drop of the first refrigerant stream across said series of heat exchangers. However, for most practical installations the refrigerant in the first stream will be isentropically expanded to a pressure not more than 50 times greater than the total pressure drop of the first refrigerant stream across said series of heat exchangers.




In one particularly desirable embodiment the refrigerant is compressed to a pressure in the range 7.5 to 9.0 MPa, the refrigerant in the first refrigerant stream is expanded to a pressure in the range 1.7 to 2.0 MPa, and the refrigerant in the first stream is isentropically expanded to a pressure in the range 15 to 20 times the total pressure drop of the first refrigerant stream across said series of heat exchangers.




The process is usually operated such that the temperature of each refrigerant stream after each isentropic expansion is greater than 1-2° C. above the saturation temperature of the refrigerant. Under these conditions, the refrigerant is well into the single phase, and is not close to saturation, there will be substantially no liquid in the isoentropically expanded refrigerant portions. However, there may be circumstances when it is desirable to operate the process such that a small amount of liquid is formed during expansion. For example, if the refrigerant comprises nitrogen with up to 10 vol % methane, preferably 5-10 vol % methane, then the process will be most efficient if some liquid is allowed to form during expansion.




The ratio of the pressure of the refrigerant, immediately prior to the isentropic expansion, to the pressure of the refrigerant, immediately after the isentropic expansion, is preferably in the range 3:1 to 6:1, more preferably 3:1 to 5:1.




In practice the best value for the intermediate refrigerant temperature depends upon the composition of the natural gas, and its pressure. However, in general the optimum value for the intermediate refrigerant temperature will be in the range −85° C. to −110° C.




The apparatus according to the invention can be used to produce LNG on a commercial scale, typically 0.5 to 2.5 million tonnes of LNG per annum. In an offshore natural gas liquefaction apparatus comprising two heat exchanger trains each in a cold box, it is possible to produce around 3 million tonnes/annum of LNG. The heat exchanger trains, including power generators and other associated equipment can be fitted on a single platform of about 35 m by 70 m, having a weight around 9000 tonnes. This size is small enough for the liquefaction means to be installed on an offshore production platform or a floating production and storage vessel.




The use of the present invention to liquefy gas at an offshore location has a number of advantages. The equipment is simple, particularly compared with the mixed refrigerant cycle; the refrigerant can be non-flammable; a relatively small amount of space is required; and the invention can be operated entirely with known, readily available equipment.











BRIEF DESCRIPTION OF THE DRAWINGS




Reference is now made to the accompanying drawings in which:





FIG. 1

is a graph of temperature vs. rate of change of enthalpy showing the cooling curve of natural gas above and below critical pressure;





FIG. 2

is a graph of temperature vs. rate of change of enthalpy showing the combined cooling curve for natural gas and nitrogen, and the warming curve for nitrogen, in a simple expander process;





FIG. 3

is a schematic diagram showing one embodiment of apparatus for the process according to the present invention;





FIG. 4

is a graph of temperature vs. rate of change of enthalpy showing the combined cooling curve for natural gas and nitrogen, and the warming curve for nitrogen for the process illustrated in

FIG. 3

, when the natural gas has a lean gas composition and the natural gas pressure is about 5.5 MPa;





FIG. 5

is a graph of temperature vs. rate of change of enthalpy showing the combined cooling curve for natural gas and nitrogen, and the warming curve for nitrogen for the process illustrated in

FIG. 3

, when the natural gas has a rich gas composition and the natural gas pressure is about 5.5 MPa;





FIG. 6

is a schematic diagram of another embodiment of apparatus for the process according to the present invention;





FIG. 7

is a graph of temperature vs. rate of change of enthalpy showing the combined cooling curve for natural gas and nitrogen, and the warming curve for nitrogen for the process illustrated in

FIG. 6

, in which the natural gas has a lean gas composition and the natural gas pressure is about 5.5 MPa;





FIG. 8

is a graph of temperature vs. rate of change of enthalpy showing the combined cooling curve for natural gas and nitrogen, and the warming curve for nitrogen for the process illustrated in

FIG. 6

, in which the natural gas has a rich gas composition and the natural gas pressure is about 7.7 MPa;





FIG. 9

is a graph of temperature vs. rate of change of enthalpy showing the combined cooling curve for natural gas and nitrogen, and the warming curve for nitrogen for the process illustrated in

FIG. 6

, in which the natural gas has a rich gas composition and the natural gas pressure is about 8.3 MPa;





FIG. 10

is a schematic diagram of one embodiment of a natural gas liquefaction apparatus according to the present invention;





FIG. 11

is a schematic diagram of another embodiment of a natural gas liquefaction apparatus according to the present invention;





FIG. 12

is a schematic diagram of another embodiment of a natural gas liquefaction apparatus according to the present invention;





FIG. 13

is a schematic diagram of one embodiment of a part of the apparatus shown in

FIGS. 10

to


12


; and





FIG. 14

is a schematic diagram of another embodiment of a part of the apparatus shown in

FIGS. 10

to


12


.











DETAILED DESCRIPTION OF THE INVENTION





FIGS. 1 and 2

have already been discussed above. Referring to

FIG. 3

, an apparatus for liquefying natural gas is shown. Lean natural gas, at a pressure of about 5.5 MPa, is fed from a pre-treatment plant (not shown) to conduit


1


. The natural gas is conduit


1


comprises 5.7 mol % nitrogen, 94.1 mol % methane and 0.2 mol % ethane. Various pre-treatment arrangements are known in the art and the exact configuration depends on the composition of the natural gas recovered from the ground, including the level of undesirable contaminants. Typically the pre-treatment plant would remove carbon dioxide, water, sulphur compounds, mercury contaminants and heavy hydrocarbons.




The natural gas in conduit


1


is fed to heat exchanger


66


, where it is cooled to 10° C. with chilled water. The exchanger


66


could be provided as part of the pre-treatment plant. In particular, the exchanger could be provided upstream of a water removal unit of the pre-treatment plant, in order to allow condensation and separation of the water contained in the natural gas, and to minimise the size of equipment.




The natural gas exiting the heat exchanger


66


is fed to conduit


2


from where it is passed to the warm end of a series of heat exchangers comprising an initial heat exchanger


50


, two intermediate heat exchangers


51


and


52


, and a final heat exchanger


53


. The series of heat exchangers


50


to


53


serves to cool the natural gas to a temperature sufficiently low that it can be liquefied when flashed to a pressure (usually about atmospheric pressure) below the critical pressure of the natural gas.




The natural gas in conduit


2


, at a temperature of about 10° C., is first fed to the warm end of the heat exchanger


50


. The natural gas is cooled in heat exchanger


50


to −23.9° C., and is passed from the cool end of the exchanger


50


to a conduit


3


. The natural gas in conduit


3


is fed to the warm end of the exchanger


51


, in which it is cooled to a temperature of −79.5° C. The natural gas exits the cool end of the exchanger


51


into a conduit


4


, from which it is fed to the warm end of the exchanger


52


. The exchanger


52


cools the natural gas to a temperature of −102° C., and natural gas exits the cool end of exchanger


52


into a conduit


5


. The natural gas in conduit


5


is fed to the warm end of exchanger


53


, in which it is cooled to a temperature of −146° C. The natural gas exits the cool end of the exchanger


53


into a conduit


6


.




The natural gas in conduit


6


is fed to the warm end of a heat exchanger


54


, in which it is cooled to a temperature of about −158° C., and it exits the cool end of the exchanger


54


into a conduit


7


. The natural gas in conduit


7


, which is still at supercritical pressure, is fed to a liquid expansion turbine


56


in which the natural gas is substantially isentropically expanded to a pressure of about 150 kPa. In the turbine


56


the natural gas is liquefied, and is reduced in temperature to about −166° C. The turbine


56


drives an electrical generator G to recover the work as electrical power.




The fluid exiting the turbine


56


is fed to a conduit


8


. This fluid is predominantly liquid natural gas, with some natural gas in the gaseous state. The fluid in conduit


8


is fed to the top of a fractionating column


57


. The natural gas feed in column


1


contains about 6 mol % of nitrogen: the fractionating column


57


serves to strip this nitrogen from the LNG. The stripping process is assisted by using the exchanger


54


to provide reboil heat transferred from the natural gas in conduit


6


. LNG is fed from the column


57


to conduit


67


, through which the LNG is fed to the cool end of the exchanger


54


. The exchanger


54


warms the LNG to a temperature of about −160° C.; the LNG exits the warm end of the exchanger


54


into conduit


68


, through which it is fed back to the column


57


.




Stripped nitrogen gas is fed from the top end of the column


57


to the conduit


9


. The conduit


9


also contains a large percentage of methane gas, which is also stripped in the column


57


. The gas in conduit


9


, which is at a temperature of −166.8° C. and a pressure of 120 kPa, is fed to the cool end of a heat exchanger


55


, in which the gas is warmed to a temperature of about 7° C. The warmed gas is fed from the warm end of the exchanger


55


to a conduit


10


, from which it is fed to a fuel gas compressor (not shown). The methane fed through the conduit


10


is used to provide the bulk of the fuel gas requirements of the liquefaction plant.




LNG is fed from the bottom of the column


57


to a conduit


11


and then to a pump


58


. The pump


58


pumps the LNG into a conduit


12


and on to a LNG storage tank (see FIGS.


10


and


11


). The LNG in conduit


12


is at a temperature of −160.2° C. and a pressure of 170 KPa.




The nitrogen refrigeration cycle which cools the natural gas to a temperature at which it can liquefy will now be described. Nitrogen refrigerant is discharged from the warm end of the exchanger


50


into a conduit


32


. The nitrogen in conduit


32


is at a temperature of 7.9° C. and a pressure of 1.14 MPa. The nitrogen is fed to a multistage compressor unit


59


, which comprises at least two compressors


69


and


70


, with at least one intercooler


71


, and an aftercooler


72


. The compressors


69


and


70


are driven by a gas turbine


73


. The cooling in the intercooler


71


and the aftercooler


72


is provided to return the nitrogen to ambient temperatures. The operation of the compressor unit


59


consumes almost all of the power required by the nitrogen refrigeration cycle. The gas turbine


73


can be driven by the fuel gas derived from conduit


10


.




The compressed nitrogen is fed from the compressor unit


59


to a conduit


33


at a pressure of 3.34 MPa and a temperature of 30° C. The conduit


33


leads to two conduits


34


and


35


between which the nitrogen from the conduit


33


is split according to the power absorbed by the compressor. The nitrogen in the conduit


34


is fed to a compressor


62


in which it is compressed to a pressure of about 5.6 MPa, and is then fed from the compressor


62


to a conduit


36


. The nitrogen in the conduit


35


is fed to a compressor


63


in which it is compressed to a pressure of about 5.6 MPa, and is then fed from the compressor


63


to a conduit


37


. The nitrogen in both the conduits


36


and


37


is fed to a conduit


38


and then to an aftercooler


64


, where it is cooled to 30° C. The nitrogen is fed from the aftercooler


64


through a conduit


39


to a heat exchanger


65


in which it is cooled to a temperature of about 10° C. by chilled water. The cooled nitrogen is fed from the exchanger


65


to a conduit


40


, which leads to two conduits


20


and


41


; the pressure in conduit


40


is 5.5 MPa. The nitrogen flowing through the conduit


40


is split between the conduits


20


and


41


: about 2 mol % of the nitrogen in conduit


40


flows through the conduit


41


.




The nitrogen flowing through the conduit


41


is fed to the warm end of the heat exchanger


55


, where it is cooled to a temperature of about −122.7° C. The cooled nitrogen is fed from the cool end of the exchanger


55


to a conduit


42


. The conduit


20


is connected to the warm end of the heat exchanger


50


, whereby the nitrogen is fed to the warm end of the heat exchanger


50


. The nitrogen from conduit


20


is pre-cooled to −23.9° C. in the heat exchanger


50


, and is fed from the cool end of the heat exchanger


50


to a conduit


21


.




The conduit


21


leads to two conduits


22


and


23


. The nitrogen flowing through the conduit


21


is split between the conduits


22


and


23


: about 37 mol % of the total nitrogen flowing through the conduit


21


is fed to the conduit


23


. The nitrogen in the conduit


22


is fed to a turbo expander


60


, in which it is work expanded to a pressure of 1.18 MPa and a temperature of −105.5° C. The expanded nitrogen exits from the expander


60


into a conduit


28


.




The nitrogen in the conduit


23


is fed to the warm end of the heat exchanger


51


, in which it is cooled to a temperature of −79.6° C. The nitrogen exits the cool end of the exchanger


51


into a conduit


24


, which is connected to a conduit


25


. The conduit


42


is also connected to the conduit


25


, so that the cooled nitrogen from the heat exchangers


51


and


55


is all fed to the conduit


25


. The nitrogen in conduit


25


, which is at a temperature of −83.1° C., is fed to a turbo expander


61


in which it is work expanded to a pressure of 1.2 MPa and a coolest nitrogen temperature of −148° C. The expanded nitrogen exits from the expander


61


into a conduit


26


.




The turbo expander


60


is arranged to drive the compressor


62


, and the turbo expander


61


is arranged to drive the compressor


63


. In this way the majority of the work produced by the expanders


60


and


61


can be recovered. In a modification the compressors


62


and


63


can be replaced with a single compressor that is connected to the conduits


33


and


38


. This single compressor can be arranged to be driven by the turbo expanders


60


and


61


, for example by being connected to a common shaft.




The nitrogen in the conduit


26


is fed to the cool end of the exchanger


53


to cool the natural gas fed to the exchanger


53


from the conduit


5


by countercurrent heat exchange. In the heat exchanger


53


the nitrogen is warmed to an intermediate nitrogen temperature of −105.5° C. The warmed nitrogen exits the warm end of the exchanger


53


into a conduit


27


, which is connected to a conduit


29


. The conduit


28


is also connected to the conduit


29


, whereby the nitrogen from the warm end of the heat exchanger


53


is recombined with the nitrogen from the turbo expander


60


.




The nitrogen in the conduit


29


, which comprises 100% of the total refrigerant flow, is fed to the cool end of the heat exchanger


52


. The nitrogen from the conduit


29


serves to cool the natural gas fed to the exchanger


52


from the conduit


4


by countercurrent heat exchange. The nitrogen flowing through the exchanger


52


is warmed by the natural gas to a temperature of −83.2° C., and exits from the exchanger


52


into a conduit


30


.




The nitrogen is fed from the conduit


30


to the cool end of the heat exchanger


51


, in which it serves to cool the natural gas fed to the exchanger


51


from the conduit


3


, and serves to cool the nitrogen refrigerant fed to the exchanger


51


from the conduit


23


, by countercurrent heat exchange. The nitrogen fed to the heat exchanger


51


from the conduit


30


is warmed to about −40° C., and exits the exchanger


51


into a conduit


31


.




The nitrogen is fed from the conduit


31


to the cool end of the heat exchanger


50


, in which it serves to cool the natural gas fed to the exchanger


50


from the conduit


2


, and serves to cool the nitrogen refrigerant fed to the exchanger


50


from the conduit


20


, by countercurrent heat exchange. The nitrogen fed to the heat exchanger


50


from the conduit


31


is warmed to 7.9° C., and exits the exchanger


50


into the conduit


32


.




Reference is now made to

FIG. 4

, which is a temperature-enthalpy graph representing the process of

FIG. 3

, in which the natural gas has the lean composition described above. The graph shows a combined cooling curve for the natural gas and the nitrogen refrigerant and a warming curve for the nitrogen refrigerant.




The cooling curve has a plurality of regions identified as


4


-


1


,


4


-


2


,


4


-


3


and


4


-


4


. The region


4


-


1


corresponds to cooling in the heat exchanger


50


: the gradient in this region is less than what would be the gradient of the cooling curve of natural gas alone over this region; in other words, the presence of the nitrogen refrigerant in the exchanger


50


lowers the gradient in this region. The region


4


-


2


corresponds to cooling in the heat exchanger


51


. The gradient is steeper here, due to the removal of part of the nitrogen refrigerant in conduit


22


; the slope of the curve in region


4


-


2


is closer to the natural gas cooling curve than in region


4


-


1


. The region


4


-


3


corresponds to cooling in the heat exchanger


52


. The gradient here represents the natural gas cooling curve only, because there is no refrigerant being cooled in the heat exchanger


52


. This part of the curve represents the region over which liquefaction would take place if the pressure of the natural gas were below the critical pressure. The critical temperature is within the temperature range of region


4


-


3


. The region


4


-


4


corresponds to cooling in the heat exchanger


53


. The gradient is steepest in region


4


-


4


and represents the sub-cooling of the natural gas. If the natural gas were just below the critical pressure in this region, then it would be a liquid.




The warming curve has two regions identified as


4


-


5


and


4


-


6


: the region


4


-


5


corresponds to refrigerant warming in the heat exchanger


53


; and the region


4


-


6


corresponds to refrigerant warming in the heat exchangers


50


,


51


and


52


. The gradient of the warming curve in region


4


-


5


is greater than the gradient in the region


4


-


6


: this is due to the smaller mass flow rate of nitrogen in the heat exchanger


53


compared with the mass flow rate in the heat exchangers


50


,


51


and


52


. A point


4


-


7


represents the nitrogen temperature in the conduit


26


as it enters the cool end of the heat exchanger


53


. A point


4


-


8


represents the nitrogen temperature in the conduit


32


as it exits the warm end of the heat exchanger


50


. The points


4


-


7


and


4


-


8


set the end points of the nitrogen warming curve.




The regions


4


-


5


and


4


-


6


intersect at a point


4


-


9


, which represents the nitrogen at the nitrogen intermediate temperature as it exits the heat exchanger


53


. It is highly advantageous that the point


4


-


9


is set as warm as possible within the constraints of the system. The nitrogen represented by the point


4


-


7


should be 1° C. to 5° C. cooler than the temperature of the natural gas exiting the heat exchanger


53


into the conduit


6


, and the nitrogen represented by the point


4


-


9


should be 1° C. to 10° C. cooler than the temperature of the natural gas entering the heat exchanger


53


from the conduit


5


; these conditions are necessary to obtain a close match between the natural gas cooling curve and the nitrogen warming curve over the regions


4


-


4


and


4


-


5


. The temperature of the nitrogen represented by the point


4


-


9


should be below the critical temperature of the natural gas; this condition is also necessary to obtain a very close match between the natural gas cooling curve and the nitrogen warming curve over the regions


4


-


4


and


4


-


5


. Finally, the temperature of then nitrogen represented by the point


4


-


9


needs to be low enough that the straight line region between the point


4


-


9


and


4


-


8


does not intersect the natural gas/nitrogen cooling curve in the regions


4


-


1


,


4


-


2


or


4


-


3


. A point


4


-


10


on the nitrogen warming curve and


4


-


11


on the natural gas/nitrogen cooling curve represents the point of closest approach between the natural gas/nitrogen cooling curve and the nitrogen warming curve. An intersection of the two curves at the point


4


-


10


and


4


-


11


(or anywhere else) represents a temperature pinch in the heat exchangers. In practice, the point


4


-


9


should be chosen so that there is a 1° C. to 10° C. temperature difference between the natural gas/nitrogen being cooled at the point


4


-


11


and the nitrogen being warmed at the point


4


-


10


.




The specific process parameters are heavily dependent upon the natural gas composition. The description in relation to

FIGS. 3 and 4

was for a lean gas composition. The process could be used with a rich gas composition, comprising, for example, 4.1 mol % nitrogen, 83.9 mol % methane, 8.7 mol % ethane, 2.8 mol % propane and 0.5 mol % butane. Using such a composition, assuming a feed pressure in conduit


1


of about 5.5 MPa and a natural gas temperature in conduit


2


of 10° C., the pressures in the process are substantially the same as those described above with reference to the lean gas example. However, some of the temperatures are different.




The natural gas emerging from heat exchanger


50


to conduit


3


is at −14° C., the natural gas emerging from heat exchanger


51


to conduit


4


is at −81.1° C., the natural gas emerging from heat exchanger


52


to conduit


5


is at −95.0° C., and the natural gas emerging from heat exchanger


53


to conduit


6


is at −146° C.




As in the

FIG. 3

embodiment, about 2.5 mol % of the total nitrogen flowing through the conduit


40


flows through the conduit


41


, while the rest flows through the conduit


20


. The nitrogen flowing through the conduit


41


emerges from the heat exchanger


155


into the conduit


42


at a temperature of about −105° C. The nitrogen in the conduit


22


is divided between the conduits


22


and


23


: about 33 mol % flows through the conduit


23


and about 67 mol % flows through the conduit


22


. The nitrogen refrigerant exiting the heat exchanger


50


to the conduit


21


is at −14° C. and the nitrogen refrigerant exiting the heat exchanger


51


to the conduit


24


is at −81.1° C. After mixing the nitrogen from the conduit


24


with the nitrogen from the conduit


42


, the nitrogen in the conduit


25


is at a temperature of −83.0° C. The nitrogen refrigerant from the conduit


22


is expanded in the turbo expander


60


to a temperature of 31 98.5° C., while the nitrogen refrigerant from the conduit


25


is expanded in the turbo expander


61


to a temperature of −148° C.




The nitrogen refrigerant exits from the heat exchanger


53


to the conduit


27


at −98.5° C., is combined with the refrigerant from the conduit


28


, is passed through the heat exchanger


52


, and exits from the heat exchanger


52


to the conduit


30


at a temperature of −92.1° C. Subsequently, the nitrogen refrigerant exits from the heat exchanger


51


to the conduit


31


at a temperature of about −24.4° C.




The temperature of the nitrogen exiting from the top of the column


57


to the conduit


9


is −164.1° C., and the temperature of the LNG product in conduit


12


is −158.4° C.





FIG. 5

is similar to

FIG. 4

, and shows a temperature-enthalpy graph representing the process of

FIG. 3

, where the natural gas has the rich composition described above. The graph shows a combined cooling curve for the natural gas and the nitrogen refrigerant and a warming curve for the nitrogen refrigerant. The cooling and warming curves have a plurality of regions identified as


5


-


1


to


5


-


6


, which correspond to regions


4


-


1


to


4


-


6


respectively of

FIG. 4

, and have a plurality of temperature points


5


-


7


to


5


-


11


, which correspond to regions


4


-


7


to


4


-


11


respectively of FIG.


4


. The description above, relating the

FIG. 4

, also applies to

FIG. 5

, with the exception that in

FIG. 5

, the natural gas critical temperature is in the region


5


-


2


, rather than


5


-


3


.




Referring now to

FIG. 6

, another embodiment of an apparatus for the present invention is shown. The

FIG. 6

embodiment bears many similarities to the

FIG. 3

embodiment, and the reference numerals given to the parts in

FIG. 6

are exactly 100 higher than the equivalent parts in the

FIG. 3

embodiment. The embodiment shown in

FIG. 6

is preferred to the embodiment shown in

FIG. 3

, because fewer heat exchangers are required.




Lean natural gas is fed from a pre-treatment plant (not shown) to conduit


101


. The natural gas in conduit


101


comprises 5.7 mol % nitrogen, 94.1 mol % methane and 0.2 mol % ethane, and is at a pressure of about 5.5 MPa. As discussed above, various pre-treatment arrangements are known in the art and the exact configuration depends on the composition of the natural gas recovered from the ground, including the level of undesirable contaminants. Typically the pre-treatment plant would remove carbon dioxide, water, sulphur compounds, mercury contaminants and heavy hydrocarbons.




The natural gas in conduit


101


is fed to heat exchanger


166


, where it is cooled to 10° C. with chilled water. The exchanger


166


could be provided as part of the pre-treatment plant. In particular, the exchanger could be provided upstream of a water removal unit of the pre-treatment plant, in order to allow condensation and separation of the water contained in the natural gas, and to minimise the size of equipment.




The natural gas exiting the heat exchanger


166


is fed to conduit


102


from where it is passed to the warm end of a series of heat exchangers


150


,


151


and


153


. The series of heat exchangers


150


to


153


cool the natural gas to a temperature sufficiently low that it can be liquefied when flashed to a pressure (usually about atmospheric pressure) below the critical pressure of the natural gas. It will be noted that in the embodiment of

FIG. 6

there is no heat exchanger equivalent to the heat exchanger


52


of FIG.


3


.




The natural gas in conduit


102


, at a temperature of about 10° C., is first fed to the warm end of the heat exchanger


150


. The natural gas is cooled in heat exchanger


150


to −41.7° C., and is passed from the cool end of the exchanger


150


to a conduit


103


. The natural gas in conduit


103


is fed to the warm end of the exchanger


151


, in which it is cooled to a temperature of about −98.2° C. The natural gas exits the cool end of the exchanger


151


into a conduit


104


, from which it is fed to the warm end of the exchanger


153


, in which it is cooled to a temperature of −146° C. The natural gas exits the cool end of the exchanger


153


into a conduit


106


.




The natural gas in conduit


106


is fed to the warm end of a heat exchanger


154


, in which it is cooled to a temperature of about −158° C., and it exits the cool end of the exchanger


154


into a conduit


107


. The natural gas in conduit


107


, which is still at supercritical pressure, is fed to a liquid expansion turbine


156


in which the natural gas is substantially isentropically expanded to a pressure of about 150 kPa. In the turbine


56


the natural gas is liquefied, and is reduced in temperature to about −167° C. The turbine


156


drives an electrical generator G′ to recover the work as electrical power.




The fluid exiting the turbine


156


is fed to a conduit


108


. This fluid is predominantly liquid natural gas, with some natural gas in the gaseous state. The fluid in conduit


108


is fed to the top of a fractionating column


157


. The natural gas feed in conduit


1


contains about 6 mol % of nitrogen: the fractionating column


57


serves to strip the nitrogen from the LNG. The stripping process is assisted by using the exchanger


154


to provide reboil heat transferred from the natural gas in conduit


106


. LNG is fed from the column


157


to conduit


167


, from where the LNG is fed to the cool end of the exchanger


154


. The exchanger


154


warms the LNG to a temperature of about −160° C.; the LNG exits the warm end of the exchanger


154


into a conduit


168


, through which it is fed back to the column


157


.




Stripped nitrogen gas is fed from the top end of the column


157


to the conduit


109


. The conduit


109


also contains a large percentage of methane gas, which is also stripped in the column


57


. The gas in conduit


109


, which is at a temperature of −166.8° C. and pressure of 120 kPa, is fed to the cool end of a heat exchanger


155


, in which the gas is warmed to a temperature of about 7° C. The warmed gas is fed from the warm end of the exchanger


105


to a conduit


110


, from which it is fed to a fuel gas compressor (not shown). The methane fed through the conduit


110


is used to provide the bulk of the fuel gas requirements of the liquefaction plant.




LNG is fed from the bottom of the column


157


to a conduit


111


and then to a pump


158


. The pump


158


pumps the LNG into a conduit


112


and on to a LNG storage tank (see FIGS.


10


and


11


).




The nitrogen refrigeration cycle which cools the natural gas to a temperature at which it can liquefy will now be described. Nitrogen refrigerant is discharged from the warm end of the exchanger


150


into a conduit


132


. The nitrogen in conduit


132


is at a temperature of about 7.9° C. and a pressure of 1.66 MPa. The nitrogen is fed to a multistage compressor unit


159


, which comprises at least two compressors


169


and


170


, with at least one intercooler


171


, and an aftercooler


172


. The compressors


169


and


170


are driven by a gas turbine


173


. The cooling in the intercooler


171


and the aftercooler


172


is provided to return the nitrogen to ambient temperatures. The operation of the compressor unit


159


consumes almost all of the power required by the nitrogen refrigeration cycle. The gas turbine


173


can be driven by the fuel gas derived from conduit


110


.




The compressed nitrogen is fed from the compressor unit


159


to a conduit


133


at a pressure of 3.79 MPa. The conduit


133


leads to two conduits


134


and


135


between which the nitrogen from the conduit


133


is split according to the power absorbed by the compressor. The nitrogen in the conduit


134


is fed to a compressor


162


in which it is compressed to a pressure of about 5.5 MPa, and is then fed from the compressor


162


to conduit a


136


. The nitrogen in the conduit


135


is fed to a compressor


163


in which it is compressed to a pressure of about 5.5 MPa, and is then fed from the compressor


163


to conduit a


137


. The nitrogen in both the conduits


136


and


137


is fed to a conduit


138


and then to an aftercooler


164


, where it is cooled back to ambient temperatures. The nitrogen is fed from the aftercooler


164


through a conduit


139


to a heat exchanger


165


in which it is cooled to a temperature of 10° C. by chilled water. The cooled nitrogen is fed from the exchanger


165


to a conduit


140


, which leads to two conduits


120


and


141


. The nitrogen flowing through the conduit


140


is split between the conduits


120


and


141


: about 2 mol % of the nitrogen in conduit


140


flows through the conduit


121


.




The nitrogen flowing through the conduit


141


is fed to the warm end of the heat exchanger


155


, where it is cooled to a temperature of about −123° C. The cooled nitrogen is fed from the cool end of the exchanger


155


to a conduit


142


. The conduit


120


is connected to the warm end of the heat exchanger


150


, whereby the nitrogen is fed to the warm end of the heat exchanger


150


. The nitrogen from conduit


120


is pre-cooled to −41.7° C. in the heat exchanger


150


, and is fed from the cool end of the heat exchanger


150


to a conduit


121


.




The conduit


121


leads to two conduits


122


and


123


. The nitrogen flowing through the conduit


121


is split between the conduits


122


and


123


: about 26 mol % of the total nitrogen flowing through the conduit


121


is fed to the conduit


123


. The nitrogen in the conduit


122


is fed to a turbo expander


160


, in which it is work expanded to a pressure of 1.73 MPa and a temperature of −102.5° C. The expanded nitrogen exits from the expander


160


into a conduit


128


.




The nitrogen in the conduit


123


is fed to the warm end of the heat exchanger


151


, in which it is cooled to a temperature of about −98.2° C. The nitrogen exits the cool end of the exchanger


151


into a conduit


124


, which is connected to a conduit


125


. The conduit


42


is also connected to the conduit


125


, so that the cooled nitrogen from the heat exchangers


151


and


155


is all fed to the conduit


125


. The nitrogen in conduit


125


, which is at a temperature of −100.3° C., is fed to a turbo expander


161


in which it is work expanded to a pressure of 1.76 MPa and a coolest nitrogen temperature of about −148° C. The expanded nitrogen exits from the expander


161


into a conduit


126


.




The turbo expander


160


is arranged to drive the compressor


162


, and the turbo expander


161


is arranged to drive the compressor


163


. In this way the majority of the work produced by the expanders


160


and


161


can be recovered. In a modification the compressors


162


and


163


can be replaced with a single compressor that is connected to the conduits


133


and


138


. This single compressor can be arranged to be driven by the turbo expanders


160


and


161


, for example by being connected to a common shaft.




The nitrogen in the conduit


126


is fed to the cool end of the exchanger


153


to cool the natural gas fed to the exchanger


153


from the conduit


104


by countercurrent heat exchange. In the heat exchanger


153


the nitrogen is warmed to an intermediate nitrogen temperature of −102.5° C. The warmed nitrogen exits the warm end of the exchanger


153


into a conduit


127


, which is connected to a conduit


129


. The conduit


128


is also connected to the conduit


129


, whereby the nitrogen from the warm end of the heat exchanger


153


is recombined with the nitrogen from the turbo expander


160


.




The nitrogen is fed from the conduit


129


to the cool end of the heat exchanger


151


, in which it serves to cool the natural gas fed to the exchanger


151


from the conduit


103


, and serves to cool and nitrogen refrigerant fed to the exchanger


151


from the conduit


123


, by countercurrent heat exchange. The nitrogen fed to the heat exchanger


151


from the conduit


129


is warmed to about −57.9° C., and exits the exchanger


151


into a conduit


131


.




The nitrogen is fed from the conduit


131


to the cool end of the heat exchanger


150


, in which it serves to cool the natural gas fed to the exchanger


150


from the conduit


102


, and serves to cool the nitrogen refrigerant fed to the exchanger


150


from the conduit


120


, by countercurrent heat exchange. The nitrogen fed to the heat exchanger


150


from the conduit


131


is warmed to 7.9° C., and exits the exchanger


150


into the conduit


132


.





FIG. 7

is similar to

FIG. 4

, and shows a temperature-enthalpy graph representing the process of

FIG. 6

, where the natural gas has the lean composition described above. The graph shows a combined cooling curve for the natural gas and the nitrogen refrigerant and a warming curve for the nitrogen refrigerant.




The cooling curve has a plurality of regions identified as


7


-


1


,


7


-


2


and


7


-


4


. The region


7


-


1


corresponds to cooling in the heat exchanger


150


: the gradient in this region is less than what would be the gradient of the cooling curve of natural gas alone over the region; in other words, the presence of the nitrogen refrigerant in the exchanger


150


lowers the gradient in this region. The region


7


-


2


corresponds to cooling in the heat exchanger


151


. The gradient is steeper here, due to the removal of part of the nitrogen refrigerant in conduit


122


; the slope of the curve in region


7


-


2


is closer to the natural gas cooling curve than in region


7


-


1


. This part of the curve also represents the region over which liquefaction would take place if the pressure of the natural gas were below the critical pressure: the critical temperature is within the temperature range of region


7


-


2


. The region


7


-


4


corresponds to cooling in the heat exchanger


153


. The gradient is steepest in region


7


-


4


and represents the sub-cooling of the natural gas. Note that there is no region


7


-


3


in

FIG. 7

, because there is no heat exchanger


152


.




The nitrogen warming curve has two regions identified as


7


-


5


and


7


-


6


: the region


7


-


5


corresponds to refrigerant warming in the heat exchanger


153


; and the region


7


-


6


corresponds to refrigerant warming in the heat exchangers


150


and


151


. The gradient of the warming curve in region


7


-


5


is greater than the gradient in the region


7


-


6


: this is due to the smaller mass flow rate of nitrogen in the heat exchanger


153


compared with the mass flow rate in the heat exchangers


150


and


151


. A point


7


-


7


represents the nitrogen temperature in the conduit


126


as it enters the cool end of the heat exchanger


153


. A point


7


-


8


represents the nitrogen temperature in the conduit


132


as it exits the warm end of the heat exchanger


150


. The points


7


-


7


and


7


-


8


set the end points of the nitrogen warming curve.




The regions


7


-


5


and


7


-


6


intersect at a point


7


-


9


, which represents the nitrogen at the nitrogen intermediate temperature as it exits the heat exchanger


153


. It is highly advantageous that the point


7


-


9


is set as warm as possible within the constraints of the system. The nitrogen represented by the point


7


-


7


should be 1° C. to 5° C. cooler than the temperature of the natural gas exiting the heat exchanger


153


into the conduit


106


, and the nitrogen represented by the point


7


-


9


should be 1° C. to 10° C. cooler than the temperature of the natural gas entering the heat exchanger


153


from the conduit


105


; these conditions are necessary to obtain a very close match between the natural gas cooling curve and the nitrogen warming curve over the regions


7


-


4


and


7


-


5


. The temperature of the nitrogen represented by the point


8


.


9


should be below the critical temperature of the natural gas: this condition is also necessary to obtain a very close match between the natural gas cooling curve and the nitrogen warming curve over the regions


7


-


4


and


7


-


5


. Finally, the temperature of the nitrogen represented by the point


7


-


9


needs to be low enough that the straight line region between the point


7


-


9


and


7


-


8


does not intersect the natural gas/nitrogen cooling curve in the regions


7


-


1


or


7


-


2


. A point


7


-


10


on the nitrogen warming curve and


7


-


11


on the natural gas/nitrogen cooling curve represents the point of closest approach between the natural gas/nitrogen cooling curve and the nitrogen warming curve. An intersection of the two curves at the point


7


-


10


and


7


-


11


(or anywhere else) represents a temperature pinch in the heat exchangers. In practice, the point


7


-


9


should be chosen so that there is a 1° C. temperature difference between the natural gas/nitrogen being cooled at the point


7


-


11


and the nitrogen being warmed at the point


7


-


10


.




The process of

FIG. 6

will now be considered for a rich gas composition, comprising 4.1 mol % nitrogen, 83.9 mol % methane, 8.7 mol % ethane, 2.8 mol % propane and 0.5 mol % butane, using a natural gas feed pressure in conduit


1


of about 7.6 MPa and a natural gas temperature in conduit


102


of 10° C.




Under these new conditions, the natural gas would exit from the heat exchanger


150


into the conduit


103


at a temperature of −8.0° C., the natural gas would exit from the heat exchanger


151


into the conduit


104


at a temperature of −87° C., and the natural gas would exit from the heat exchanger


153


into the conduit


106


at a temperature of −146° C.




The nitrogen refrigerant exiting from the heat exchanger into the conduit


132


is at a temperature of 7.9° C. and a pressure of 2.31 MPa. The nitrogen refrigerant is compressed in the compressor unit


159


to a pressure of 6.08 MPa, and is then further compressed in the compressors


162


and


163


to a pressure of about 10 MPa.




The nitrogen refrigerant in the conduit


140


is at a temperature of 10.0° C., as a result of the cooling in the aftercooler


164


and the heat exchanger


165


. About 2.2 mol % of the nitrogen flowing through the conduit


140


flows through the conduit


141


, while the remainder flows through the conduit


120


. The nitrogen flowing through the conduit


141


is reduced in temperature to about −108° C. in the heat exchanger


155


.




The nitrogen refrigerant exiting the heat exchanger


150


into the conduit


121


it at a temperature of −8° C. About 25 mol % of the nitrogen in the conduit


121


flows through the conduit


123


, while the remaining 75 mol % flows through the conduit


122


. The nitrogen flowing through the conduit


123


emerges from the heat exchanger


151


at a temperature of −87° C., from where it flows into the conduit


125


along with the nitrogen from the conduit


142


: the temperature of the nitrogen in the conduit


125


is −88.7° C. The nitrogen flowing through the conduit


122


is expanded in the turbo expander


160


to a pressure of 2.39 MPa and a temperature of −90.5° C., and the nitrogen flowing through the conduit


125


is expanded in the turbo expander


161


to a pressure of 2.42 MPa and a temperature of −148° C.




The nitrogen refrigerant emerging from the heat exchanger


153


into the conduit


127


is at a temperature of −90.5° C., and the nitrogen refrigerant emerging from the heat exchanger


151


into the conduit


131


is at a temperature of about −18° C.





FIG. 8

is similar to

FIG. 7

, and shows a temperature-enthalpy graph representing the process of

FIG. 6

, where the natural gas has the rich composition described above, and is supplied at a pressure of about 7.6 MPa. The graph shows a combined cooling curve for the natural gas and the nitrogen refrigerant and a warming curve for the nitrogen refrigerant. The cooling and warming curves have a plurality of regions


8


-


1


to


8


-


6


, which correspond to regions


7


-


1


to


7


-


6


respectively of

FIG. 7

, and have a plurality of temperature points


8


-


7


to


8


-


11


, which correspond to temperature points


7


-


7


to


7


-


11


respectively of FIG.


7


. The description above, relating to

FIG. 7

, also applies to FIG.


8


.




The process of

FIG. 6

will now be considered for a rich gas composition, comprising 4.1 mol % nitrogen, 84.1 mol % methane, 8.5 mol % ethane, 2.6 mol % propane and 0.7 mol % butane, using a natural gas feed pressure in conduit


1


of about 8.25 MPa and a natural gas temperature in conduit


102


of 10° C. There is one slight modification to the process described above with respect to FIG.


6


: boil-off gas from LNG storage tanks is combined with the top product from column


157


in conduit


109


, and the combined contents of the conduit


109


are fed to the heat exchanger


155


.




Under these new conditions, the natural gas would exit from the heat exchanger


151


into the conduit


104


at a temperature of −86.2° C., and would exit from the heat exchanger


153


into the conduit


106


at a temperature of −148.3° C.




The nitrogen refrigerant exiting from the heat exchanger into the conduit


132


is at a temperature of 3.0° C. and a pressure of 1.77 MPa. The nitrogen refrigerant is compressed in the compressor unit


159


to a pressure of 4.97 MPa, and is then further compressed in the compressors


162


and


163


to a pressure of about 8.3 MPa.




The nitrogen refrigerant in the conduit


140


is at a temperature of 10.0° C., as a result of the cooling in the aftercooler


164


and the heat exchanger


165


. About 1.7 mol % of the nitrogen flowing through the conduit


140


flows through the conduit


141


, while the remainder flows through the conduit


120


. The nitrogen flowing through the conduit


141


is reduced in temperature to about −143° C. in the heat exchanger


155


.




The nitrogen refrigerant exiting the heat exchanger


150


into the conduit


121


is at a temperature of −7° C. About 31 mol % of the nitrogen in the conduit


121


flows through the conduit


123


, while the remaining 69 mol % flows through the conduit


122


. The nitrogen flowing through the conduit


123


emerges from the heat exchanger


151


at a temperature of −86.2° C., from where it flows into the conduit


125


along with the nitrogen from the conduit


142


; the temperature of the nitrogen in the conduit


125


is −89.3° C. The nitrogen flowing through the conduit


122


is expanded in the turbo expander


160


to a pressure of 1.84 MPa and a temperature of −93.2° C., and the nitrogen flowing through the conduit


125


is expanded in the turbo expander


161


to a pressure of 1.87 MPa and a temperature of −152.2° C.




The nitrogen refrigerant emerging from the heat exchanger


153


into the conduit


127


is at a temperature of −93.2° C.





FIG. 9

is similar to

FIG. 7

, and shows a temperature-enthalpy graph representing the process of

FIG. 6

, where the natural gas has the rich composition described above, and is supplied at a pressure of about 8.25 MPa. The graph shows a combined cooling curve for the natural gas and the nitrogen refrigerant and a warming curve for the nitrogen refrigerant. The cooling and warming curves have a plurality of regions


9


-


1


to


9


-


6


, which correspond to regions


7


-


1


to


7


-


6


respectively of

FIG. 7

, and have a plurality of temperature points


9


-


7


to


9


-


11


, which correspond to temperature points


7


-


7


to


7


-


11


respectively of FIG.


7


. The description above, relating to

FIG. 7

, also applies to FIG.


9


.




In

FIG. 9

the minimum temperature difference between the two curves is 3.9° C., while in

FIGS. 4

,


5


,


7


and


8


, the minimum temperature difference is 2° C.




Referring to

FIG. 10

an embodiment of an apparatus for producing LNG is generally designated


500


. The apparatus comprises a floating platform in the form of a ship


501


, which carries a natural gas liquefaction plant


502


and LNG storage tanks


503


. The LNG is fed from the plant


502


to the storage tanks


503


via a conduit


504


. The natural gas is supplied to the plant


502


via a pipeline


505


, which extends to a natural gas rig


506


, and via a riser and manifold arrangement


510


, which extends from the ship


501


to the pipeline


505


. It is possible for the natural gas to be supplied from a plurality of said gas rigs


506


. A pre-treatment plant (not shown) may be provided for the natural gas, before it is fed to the plant


502


. The pre-treatment plant may be provided on the rig


506


, on a separate unit (not shown) or on the ship


501


.




The ship


501


also includes accommodation


507


, mooring lines


508


, and means


509


for supplying LNG from the storage tanks


503


to an LNG carrier (not shown).




Referring to

FIG. 11

another embodiment of an apparatus for producing LNG is generally designated


600


. The apparatus comprises platform


601


, which is supported above the water level


607


by legs


609


, a natural gas liquefaction plant


602


and an LNG storage tank


603


. The LNG is fed from the plant


602


to the storage tank


603


via a conduit


604


. The storage tank


603


is supported by a concrete gravity base


610


, which rests on seabed


608


. The natural gas is supplied to the plant


602


via a pipeline


605


, which communicates with a natural gas rig


606


. It is possible for the natural gas to be supplied from a plurality of said gas rigs


606


. A pre-treatment plant (not shown) may be provided for the natural gas, before it is fed to the plant


602


. The pre-treatment plant may be provided on the rig


606


, on a separate unit (not shown), on the platform


601


or on the gravity base


610


. Means


611


is provided for supplying LNG from the storage tanks


603


to a LNG carrier (not shown). In a modification the apparatus


600


could be provided on the rig


606


.





FIG. 12

shows a modification of the LNG apparatus


600


shown in FIG.


11


. In

FIG. 12

the modified LNG apparatus is generally designated


600


′ and comprises two spaced concrete gravity bases


610


′, which rest on the seabed


608


′, so that they project above the water level


607


′. A liquefaction plant


602


′ is provided on a platform


601


′, which rests on the gravity bases


610


′ and bridges the gap between the gravity bases


610


′. An LNG storage tank


603


′ is provided on each of the gravity bases


610


′.




The platform


601


′ can be installed by supporting it on a barge (not shown): floating the barge into the gap between the gravity bases


610


′ so that the platform


601


′ projects over the upper surface of each gravity base


610


′; lowering the barge so that the platform


601


′ rests on the gravity bases


610


′; and finally floating the barge out of the gap between the gravity bases


610


′.




Referring to

FIG. 13

, the natural gas liquefaction plants


502


,


602


and


602


′ of

FIGS. 10

to


12


are shown in more detail. In general, the components of the plant shown in

FIG. 13

are similar to the components shown in

FIGS. 3 and 6

. Natural gas is supplied to conduit


450


of the plant at high pressure, which may be supercritical; the natural gas may have been pre-treated to remove contaminants using conventional processes. The natural gas in conduit


450


is fed to a heat exchanger


401


in which it is cooled with chilled water supplied from a chilled water refrigeration unit


415


. The heat exchanger


401


may, instead, be incorporated in the pretreatment process. The heat exchanger


401


may be a conventional shell and tube heat exchanger, or any other type of heat exchanger suitable for cooling natural gas with chilled water, including a PCHE.




The cooled natural gas exits from the heat exchanger


401


to a conduit


451


, through which it is fed to a cold box


402


, where the gas is progressively cooled to a low temperature in a series of heat exchangers (not shown) within the box


402


. The heat exchanger arrangement in the cold box


402


may be the same as the arrangement of heat exchangers


50


,


51


,


52


and


53


shown in

FIG. 3

, or may be the same as the arrangement of heat exchangers


150


,


151


and


153


shown in FIG.


6


. The type of heat exchangers used depends on the pressure at which the natural gas is supplied. If the pressure is below about 5.5 MPa, then each heat exchanger comprises a number of aluminium plate heat exchangers manifolded in series. If the pressure is above about 5.5 MPa, then each heat exchanger comprises, for example, a spiral wound heat exchanger, a PCHE or a spool wound heat exchanger. However, when a spiral wound heat exchanger is used, the embodiment shown in

FIG. 14

is more appropriate. The cold box


402


is filled with pearlite or rock wool to provide insulation.




The are many advantages to using a the cold box


402


. First, it enables the majority of the cold equipment and piping to be contained within a single space that requires a much smaller plot area than if the equipment and piping were installed separately. The quantity of external insulation required is much less than if the equipment and piping were installed separately, and this reduces the cost and time of installation and future maintenance. In addition, the number of flanges required for connections of piping and equipment is reduced, because all the connections within the box are fully welded—this reduces the possibility of leaks from cold flange during normal operation and during cool-down and warm-up operations. The entire cold box installation can be constructed in a controlled industrial location and can be delivered to the construction site fully leak tested, dry and ready for commissioning—this would otherwise have to be done on the individual bits of equipment and piping in the field in remote locations and under less than ideal conditions. The cold box steel shell and insulation provides protection from the salt air environment in an offshore location, and affords a measure of fire protection for the equipment containing the hydrocarbon inventory. It should be noted that, when spiral wound heat exchangers are used, the first and intermediate exchanger bundles may both be included in a single vertical exchanger shell and may be installed separately to the cold box. In this case, the spiral wound heat exchanger is externally insulated and the cold box containing the remaining cold exchangers and vessel is significantly smaller.




The sub-cooled natural gas is withdrawn from the cold box


402


, at its lowest temperature of about −158° C., into a conduit


452


, through which it is fed to a liquid or hydraulic turbine expander disposed within a suction vessel


413


in which the sub-cooled natural gas is work expanded to a low pressure (which is sub-critical), with a concomitant reduction in temperature and the formation of LNG. The work generated in the liquid or hydraulic turbine expander in the suction vessel


413


is used to turn an electrical generator; the electrical generator is also housed within the suction vessel


413


. It is possible for the liquid or hydraulic turbine expander and the suction vessel


413


to be replaced with a throttle valve: this will simplify the equipment, saving on capital costs and space, but there will be a small loss in process efficiency.




The LNG exits the liquid or hydraulic turbine expander in the suction vessel


413


into a conduit


453


, which is fed back into the cold box


402


to a nitrogen stripper located within the cold box


402


. The nitrogen stripper within the cold box


402


may be the same as the nitrogen stripper


57


in

FIG. 3

, or the nitrogen stripper


157


in FIG.


6


. The cold flash gas from the top of the nitrogen stripper is then reheated in another heat exchanger in the cold box


402


, which may be the same as the heat exchanger


55


shown in

FIG. 3

, or the heat exchanger


155


shown in FIG.


6


. The reheated flash gash exits the cold box


402


into a conduit


454


, which is equivalent to the conduit


10


of

FIG. 3

, or the conduit


110


of FIG.


6


. The reheated flash gas in the conduit


454


is fed to a compressor unit


414


in which it is compressed to the required fuel gas system pressure. Cooling is provided in the compressor unit


414


by cooling water, which enters the unit


414


via conduit


455


and leaves the unit


414


via conduit


456


. The compressed fuel gas exits the compressor unit


414


into a conduit


457


. The compressor unit


414


may be an integrally geared multistage centrifugal compressor driven by an electric motor and complete with integral intercoolers and aftercoolers. Alternatively, the unit


414


may be an API specification centrifugal compressor with several compressor cases driven by an electric motor or a small gas turbine. The power requirements for the unit


414


may be provided by part of the fuel gas produced therein.




The LNG product exits the nitrogen stripper into a conduit


458


, through which it is fed to a submerged pump


412


. The submerged pump


412


pumps the LNG into a conduit


459


, through which it is fed to storage tanks (see

FIGS. 10

or


11


).




The refrigeration of the natural gas in the cold box


402


is provided by a nitrogen refrigeration cycle, the components of which will now be described. Nitrogen refrigerant exits the cold box


402


into conduit


460


, having been warmed to ambient temperatures by countercurrent heat exchange with the natural gas. The nitrogen in the conduit


460


is fed to a first stage compressor


405


where it is compressed to high pressure. The compressed nitrogen exits the compressor


405


into a conduit


461


, through which it is fed to an intercooler


462


, where the nitrogen is cooled with cooling water. The compressed nitrogen exits the intercooler


462


into a conduit


463


through which it is fed to a second stage compressor


406


, where it is compressed to an even higher pressure. The compressed nitrogen exits the compressor


406


into a conduit


464


, through which it is fed to an aftercooler


465


, where the nitrogen is cooled with cooling water. The compressors


405


and


406


may be multi wheel API type compressors; alternatively, axial flow compressors may be used if the suction pressure is low enough and/or the circulation rate is high enough. The compressors


405


and


406


may be provided in the form of a single compressor.




The compressors


405


and


406


are driven by a gas turbine


403


. The gas turbine


403


is an aero-derivative type of gas turbine because of its smaller size and weight compared to the alternative industrial type gas turbines commonly used in onshore LNG plants. The temperature of the ambient air locations where the plant is located is often high, and this can substantially reduce the site rating of gas turbine


403


. This problem can be solved by cooling the gas turbine inlet air with chilled water in a heat exchanger


404


. The turbine air is taken in through an inlet manifold


467


of the turbine


403


, in which the heat exchanger


404


is disposed. The chilled water can be provided from the unit


15


.




The high pressure nitrogen refrigerant exits the aftercooler


465


into a conduit


466


, from which the flow is subsequently divided between conduits


470


and


471


. The nitrogen flowing through the conduit


470


is fed to the compressor side of the expander/compressor unit


408


, while the nitrogen flowing through the conduit


471


is fed to the compressor side of the expander/compressor unit


409


. The compressed nitrogen exits the units


408


and


409


into conduits


472


and


473


respectively at an even higher, supercritical, pressure. The nitrogen flowing through the conduits


472


and


473


is recombined in a conduit


474


, through which it is fed to an aftercooler


410


, where it is cooled with cooling water. The nitrogen refrigerant exits the aftercooler


410


into a conduit


475


, through which it is fed to a heat exchanger


411


, where it is further cooled by countercurrent heat exchange with chilled water provided by the unit


15


. The heat exchangers


462


,


465


,


410


and


411


are all stainless steel PCHE exchangers; a closed circuit of fresh water is used for cooling in exchangers


462


,


465


and


410


. Alternatively, direct seawater cooling may be used for these exchangers, if suitable materials of construction are employed.




The nitrogen refrigerant exits the heat exchanger


411


into a conduit


476


, through which it is fed to the cold box


402


, where it is pre-cooled in the series of heat exchangers in a similar manner to that shown in

FIG. 3

or

FIG. 6. A

portion of the pre-cooled nitrogen (50-80 mol % of the total nitrogen flow) is withdrawn from the cold box


402


into a conduit


477


, through which it is fed to the turbo expander end of the expander/compressor unit


409


. The nitrogen in the expander compressor unit


409


is expanded to a lower pressure, with concomitant temperature drop. The work produced during this expansion stage is used to drive the compressor end of the expander/compressor unit


409


. The expander nitrogen exits the turbo expander of the expander/compressor unit into a conduit


478


.




Another portion of the pre-cooled nitrogen (20-50 mol % of the total nitrogen flow) is withdrawn from the cold box


402


into a conduit


479


, through which it is fed to the turbo expander end of the expander/compressor unit


408


; the nitrogen withdrawn into the conduit


479


has been cooled to a lower temperature than that withdrawn through the conduit


478


. The nitrogen in the expander compressor unit


408


is expanded to a lower pressure, with concomitant temperature drop. The work produced during this expansion stage is used to drive the compressor end of the expander/compressor unit


408


. The expanded nitrogen exits the turbo expander of the expander/compressor unit into a conduit


480


.




The nitrogen in the conduits


478


and


480


is fed back to the series of heat exchanger within the cold box


402


, and serves to cool the natural gas entering the cold box


402


via the conduit


451


and to pre-cool the nitrogen entering the cold box


402


via the conduit


476


. The nitrogen flowing in the conduits


478


and


480


may follow the same path as the nitrogen in conduits


28


and


26


respectively in

FIG. 3

, or as the nitrogen in conduits


128


and


126


respectively in FIG.


6


. As explained above, the warmed nitrogen is subsequently withdrawn from the cold box


402


via the conduit


460


.




The expander/compressor units


408


and


409


may be conventional radial flow expander units. If desired the expander of expander/compressor unit


409


may be replaced by two expander units in parallel or in series. All the expander/compressor units


408


/


409


may be installed on a single skid to save on plot area and interconnecting pipework; they may also have a common lube oil skid, thereby saving further in plot area and cost. Another possibility is to connect the expanders to a single compressor or a multi-stage compressor, this would avoid the need to split the nitrogen flow into conduits


470


and


471


.




The chilled water refrigeration unit


415


comprises one or more standard, commercially available units, which can use refrigerants such as Freon, propane, ammonia, etc. The chilled water is circulated to the heat exchangers


401


,


404


and


411


in a closed circuit by centrifugal pumps (not shown). This unit has the advantage that it requires only a small inventory of refrigerant, and takes up very little space.




The cooling water system is also a closed circuit system—it uses fresh water to allow the use of PCHE exchangers. The PCHE heat exchangers have the advantage that they are considerably smaller and cheaper than the conventional shell and tube heat exchangers normally used for this type of system.




The nitrogen refrigeration system is a closed circuit system containing an initial inventory of dry nitrogen gas. This nitrogen must be replenished during normal operation, due to small losses of refrigerant from the circuit. These losses are caused by, for example, leaks to atmosphere from compressor seals and pipework flanges etc. A small amount of nitrogen is continuously added to the refrigeration system by nitrogen make-up unit (not shown), in order to compensate for the leakages. The nitrogen is extracted from the instrument air system on the plant. The make-up unit may be a commercially available unit, which can be of the membrane type or the pressure swing absorption type.





FIG. 14

shows another embodiment of the apparatus shown in FIG.


13


. Many of the parts illustrated in

FIG. 14

are identical to the parts illustrated in FIG.


13


—like parts have been designated with like reference numerals. The differences are as follows:




The embodiment shown in

FIG. 14

uses a series of heat exchangers in the form of a spiral wound heat exchanger (also known as a coil wound heat exchanger)


480


in place of the series of heat exchangers located within the cold box


402


in the apparatus shown in FIG.


13


. The heat exchanger


480


is provided with its own thermal insulation, so there is no need to locate it within a cold box. Cooled natural gas at supercritical pressure is withdrawn from the heat exchanger


480


via a conduit


482


, and is fed to a nitrogen stripper located within a cold box


484


. The nitrogen stripper within the cold box


484


may be the same as the nitrogen stripper


57


or


157


.




The five refrigeration cycles described above, and shown in

FIGS. 4

,


5


,


7


,


8


and


9


, were simulated in order to make comparisons between the relative performance.




The first cycle, as illustrated in

FIG. 4

, used lean gas at a pressure of 5.5 MPa cooled with refrigerant at 1.2 MPa. The total power requirement was found to be 17.1 kW/tonne natural gas produced/day.




The second cycle, as illustrated in

FIG. 5

, used rich gas at a pressure of 5.5 MPa cooled with refrigerant at 1.2 MPa. The total power requirement was found to be 15.0 kW/tonne natural gas produced/day.




The third cycle, as illustrated in

FIG. 7

, used lean gas at a pressure of 5.5 MPa cooled with refrigerant at 1.7 MPa. The total power requirement was found to be 17.4 kW/tonne natural gas produced/day. However, although the power requirement was higher than the first and second cycle, the increased pressure allows the heat exchanger sizes to be reduced.




The fourth cycle, as illustrated in

FIG. 8

, used rich gas at a pressure of 7.6 MPa cooled with refrigerant at 2.4 MPa. The total power requirement was found to be 13.0 kW/tonne natural gas produced/day.




The fifth cycle, as illustrated in

FIG. 9

, used rich gas at a pressure of 8.25 MPa cooled with refrigerant at 1.8 MPa. The total power requirement was found to be 14.6 kW/tonne natural gas produced/day.




For comparison, the power requirement of a conventional propane pre-cooled mixed refrigerant cycle would be in the range 13 to 14 kW/tonne natural gas produced/day, and the power requirement of the simple nitrogen refrigeration cycle shown in

FIG. 2

is about 27 kW/tonne natural gas produced/day. This shows that the process of the present invention is much more efficient than the simple refrigeration cycle.




Whilst certain embodiments of the invention have been described herein, it will be appreciated that the invention may be modified.




For the avoidance of doubt, the term “comprising” as used in this specification means “includes”.



Claims
  • 1. An offshore apparatus for liquefying natural gas, comprising:a support structure which is either floatable or is otherwise adapted to be disposed in an offshore location at least partially above sea level, and natural gas liquefaction means disposed on or in the support structure, the natural gas liquefaction means comprising a series of heat exchangers for cooling the natural gas in countercurrent heat exchange relationship with a refrigerant, compression means for compressing the refrigerant, expansion means for isentropically expanding at least two separate streams of the compressed refrigerant, wherein said expanded streams of refrigerant communicate with a cool end of a respective one of the heat exchangers, a flash vessel for separating the natural gas cooled by said series of heat exchangers into a liquid phase stream and a gaseous phase stream, the gaseous phase stream being arranged in countercurrent head exchange relationship with part of the refrigerant by means, and wherein the flash vessel and at least some of the or each series of heat exchangers and pipework connected thereto are disposed within a single, common heat insulating housing.
  • 2. The apparatus of claim 1, wherein:the support structure is a fixed support structure.
  • 3. The apparatus of claim 2, wherein:the fixed support structure includes a steel jacket or a concrete gravity base.
  • 4. The apparatus of claim 1, wherein:the support structure is a floating support structure.
  • 5. The apparatus of claim 4, wherein:the support structure is a waterborne vessel having a steel or concrete hull.
  • 6. The apparatus of claim 4, wherein:the support structure is a floating production storage and off-loading unit.
  • 7. The apparatus of claim 1, further comprising:pretreatment means for pretreating the natural gas befor eit is delivered to the liquefaction means.
  • 8. The apparatus of claim 1, further comprising:storage means for storing liquefied natural gas produced by the liquefaction means.
  • 9. The apparatus of claim 8, wherein:the support structure comprises two spaced gravity bases, and a platform bridging said gravity bases, wherein said storage means comprises a storage tank provided on or in at least one of said gravity bases, and wherein the liquefaction means is provided on or in said bridging platform.
  • 10. The apparatus of claim 1, further comprising:means for connecting said apparatus to a subsea well, whereby the natural gas can be delivered to the liquefication means at a pressure above 5.5 Mpa, said pressure being derived directly or indirectly from the pressure in the subsea well.
  • 11. A natural gas apparatus, for offshore installation, comprising:natural gas liquefaction means comprising a series of heat exchangers for cooling the natural gas in countercurrent heat exchange relationship with a refrigerant, compression means for compressing the refrigerant, expansion means for isentropically expanding at least two separate streams of the compressed refrigerant, wherein said expanded streams fo refrigerant communicate with a cool end of a respective one of the heat exchangers into a liquid phase stream and a gaseous phase stream, the gaseous phase stream being arranged in countercurrent heat exchange relationship with part of the refrigerant by means, and wherein the flash vessel and at least some of the or each series of heat exchangers and pipework connected thereto are disposed within a single, common heat insulating housing; and a support frame carrying the components of the liquefaction means as a single unit for transportation to, and installation at, the offshore location.
  • 12. The apparatus of claim 11, wherein:the liquefaction means further comprises cooling means for cooling the refrigerant after it has been compressed and before it is isentropically expanded, said cooling means comprising a heat exchanger, a liquid coolant and a refrigerant unit for cooling the coolant to a temperature between −10° C. and 20° C., wherein the compressed refrigerant is cooled in said heat exchanger in countercurrent relationship with said coolant.
  • 13. The apparatus of claim 1, wherein:the expansion means comprises a work expander disposed in each of said compressed refrigerant streams, and the compression means comprising at least one compressor.
  • 14. The apparatus of claim 1, wherein:the series of heat exchangers comprises an initial heat exchanger, an intermediate heat exchanger and a final heat exchanger, and the natural gas is passed sequentially through the initial, the intermediate and the final heat exchangers in order to cool it to successively cooler temperatures, and wherein refrigerant in a first of said refrigerant streams is delivered to the final heat exchanger, and a refrigerant in a second of said refrigerant stream is delivered to the intermediate heat exchanger.
  • 15. The apparatus of claim 14, wherein:said refrigerant is cooled in the initial heat exchanger after being compressed, but before being isentropically expanded, and wherein the refrigerant in said first refrigerant stream is cooled in the intermediate heat exchanger after being cooled in the initial heat exchanger, but before being isentropically expanded.
  • 16. The apparatus of claim 15, wherein the final heat exchanger receives refrigerant from the first refrigerant stream, the relative flowrates of the first and second refrigerant streams are such that the warming curve for the refrigerant comprises a plurality of segments of different gradient, the refrigerant is warmed in said final heat exchanger to a temperature below −80° C., and the coolest refrigerant temperature and the flowrate of refrigerant in said first refrigerant stream are such that a part of the refrigerant warming curve relating to the final heat exchanger is at all times with 1 to 10° C. of the corresponding part of the cooling curve for the natural gas.
  • 17. The apparatus of claim 16, wherein:coolest refrigerant temperature and the flowrate of refrigerant in said first refrigerant stream is such that the part of the refrigerant warming curve relating to the final heat exchanger is at all times within 1 to 5° C. of the corresponding part of the cooling curve for the natural gas.
  • 18. The apparatus of claim 17, wherein:the liquefaction means further comprises a gas turbine for generating power for the compression means.
  • 19. The apparatus of claim 18, wherein:the gas turbine comprises an aero-derivative gas turbine.
  • 20. The apparatus of claim 19, wherein:the liquefaction means further comprises a second series of heat exchangers, said second series of heat exchangers being arranged in parallel with said first series of heat exchangers, and a separate refrigerant compression means and refrigerant expansion means for each series of heat exchangers.
  • 21. The apparatus of claim 20, wherein:said series of heat exchangers comprises an aluminum plate heat exchanger, a spool wound heat exchanger, a spiral would heat exchanger, a printed circuit heat exchanger, or a combination of two or more thereof.
  • 22. The apparatus of claim 21, wherein:the refrigerant contains at least 50% vol. nitrogen.
  • 23. The apparatus of claim 22, wherein:the refrigerant contains substantially 100% vol. nitrogen.
Priority Claims (4)
Number Date Country Kind
9520303 Oct 1995 GB
9520348 Oct 1995 GB
9520349 Oct 1995 GB
9520356 Oct 1995 GB
CROSS-REFERENCES TO RELATED APPLICATIONS

This application is a continuation application of parent application Ser. No. 09/051,210, filed Jul. 13, 1998 which was derived from PCT International application no. PCT/GB96/02434, filed Oct. 4, 1996.

US Referenced Citations (7)
Number Name Date Kind
3677019 Olszewski Jul 1972
3763658 Gaumer, Jr. et al. Oct 1973
3766583 Phelps Oct 1973
4217848 Meyer-Haake Aug 1980
4586942 Gauthier May 1986
4638639 Marshall et al. Jan 1987
4846862 Cook Jul 1989
Foreign Referenced Citations (1)
Number Date Country
3200958 Jul 1983 DE
Continuations (1)
Number Date Country
Parent 09/051210 US
Child 09/644233 US